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https://getcalc.com/math-log-base3of69.htm
[ "# What is Log Base 3 of 69?", null, "Logarithm calculator to generate step by step calculation for how to find what is log base 3 of 69? Logarithm base 3 of 69 is 3.854.\n\nlog3(69) = 3.854\n\n## How to Find log3(69)? - Work with Steps\n\nThe below is the work with steps to find what is log base 3 of 69 shows how the input values are being used in the log base 3 functions. Formula:\nlogb(x) = y, if by = x\n\nInput:\nx = 69\nb = 3\n\nSolution:\ny = log3 69\n= log(3 x 23)\n= log3(3) + log3(23)\n= 1 + 2.854\n= 3.854\nlog3(69) = 3.854", null, "" ]
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https://ij-healthgeographics.biomedcentral.com/articles/10.1186/s12942-020-00251-z
[ "# Beyond standardized mortality ratios; some uses of smoothed age-specific mortality rates on small areas studies\n\n## Abstract\n\n### Background\n\nMost epidemiological risk indicators strongly depend on the age composition of populations, which makes the direct comparison of raw (unstandardized) indicators misleading because of the different age structures of the spatial units of study. Age-standardized rates (ASR) are a common solution for overcoming this confusing effect. The main drawback of ASRs is that they depend on age-specific rates which, when working with small areas, are often based on very few, or no, observed cases for most age groups. A similar effect occurs with life expectancy at birth and many more epidemiological indicators, which makes standardized mortality ratios (SMR) the omnipresent risk indicator for small areas epidemiologic studies.\n\n### Methods\n\nTo deal with this issue, a multivariate smoothing model, the M-model, is proposed in order to fit the age-specific probabilities of death (PoDs) for each spatial unit, which assumes dependence between closer age groups and spatial units. This age–space dependence structure enables information to be transferred between neighboring consecutive age groups and neighboring areas, at the same time, providing more reliable age-specific PoDs estimates.\n\n### Results\n\nThree case studies are presented to illustrate the wide range of applications that smoothed age specific PoDs have in practice . The first case study shows the application of the model to a geographical study of lung cancer mortality in women. This study illustrates the convenience of considering age–space interactions in geographical studies and to explore the different spatial risk patterns shown by the different age groups. Second, the model is also applied to the study of ischaemic heart disease mortality in women in two cities at the census tract level. Smoothed age-standardized rates are derived and compared for the census tracts of both cities, illustrating some advantages of this mortality indicator over traditional SMRs. In the latest case study, the model is applied to estimate smoothed life expectancy (LE), which is the most widely used synthetic indicator for characterizing overall mortality differences when (not so small) spatial units are considered.\n\n### Conclusion\n\nOur age–space model is an appropriate and flexible proposal that provides more reliable estimates of the probabilities of death, which allow the calculation of enhanced epidemiological indicators (smoothed ASR, smoothed LE), thus providing alternatives to traditional SMR-based studies of small areas.\n\n## Background\n\nSpatial epidemiology deals with the description and analysis of geographically indexed health data with respect to demographic, environmental, behavioral, socioeconomic, genetic and infectious risk factors . Most of these risk factors, especially those related to mortality, strongly depend on age ; therefore, the comparison of raw (unstandardized) rates may be misleading due to differences in the population structure of the units of study, which may be confused with real differences in risk. Age-adjusted (standardized) rates were proposed in the mid-nineteenth century as an answer to this problem, although they are not a completely satisfactory solution.\n\nStandardization seeks to remove the effect of having different age distributions for the populations being compared. It produces a single summary index per population, easier to compare than a full set of age-specific rates. The most popular standardization method is the so-called indirect method, which would yield standardized mortality ratios (SMRs) if mortality was the event of interest. SMRs are calculated as the ratio of the number of deaths observed over a specific time interval in a population group, in our case and from now on “spatial units”, to the expected deaths in that population assuming that it had the same age-specific death rates as a reference population. This indicator is commonly used to compare the mortality for different geographical areas to that of the reference population, and its main advantage is that SMRs do not depend on the age-specific rates of each spatial unit, which may be completely unreliable when working with small areas. This property has led to SMRs being, by far, the most commonly used epidemiological indicator for small areas spatial studies. Nevertheless, SMRs do exhibit some particular problems. SMRs of different spatial units are not directly comparable, that is, even if the age-specific rates of two populations were all proportional, this would not mean that the same proportionality holds between their SMRs . In particular, areas with identical age-specific rates do not necessarily yield the same SMRs. Therefore, strictly speaking, SMRs are only valid for comparing the units of study against the standard population of the study, but not against one another.\n\nAlternatively, a second age-standardization method for rates, the direct method, produces age-standardized rates (ASRs), a weighted average of the age-specific rates of each unit of study also using a reference population to determine that common set of weights. When mortality is the outcome of study, ASRs have a direct interpretation as the hypothetical death rate that would have occurred in the corresponding unit of study if its age composition were the same as that of the reference population . Therefore, the standardization process of ASRs removes the effect that the age composition of the different population groups could have on raw rates. One advantage of direct over indirect standardization is that spatial units with proportional age-specific rates necessarily yield ASRs keeping that same proportion , and so they are also comparable to each other. Nevertheless, ASRs are not as popular as SMRs for small areas geographical analyses since ASRs are only reliable when trustworthy age-specific rates are available for each spatial unit. This usually requires having a considerable amount of observed health events, from now on “deaths”, for every combination of age group and spatial unit, which small areas do not usually have. As a consequence, when ASRs are pursued on small areas, statistical modeling becomes necessary.\n\nThere have been various approaches to the smooth estimation of ratios, such as mortality rates. In this regard, Kafadar proposed a linear smoother for geographically-defined data that are in form of ratios. Although it shows that the smoothed rate has less variability than the age-adjusted unsmoothed rate, it uses parametric weights and does not consider the dependence between age groups. Ezzati et al. used information on the number of deaths and county-level sociodemographic characteristics to estimate mortality rates and probabilities of death, but merged the counties, pooled the data on deaths and population over 5 years and also did not consider the dependence between age groups.\n\nMany more epidemiologic measures show similar problems produced by the age composition of the units of study. For example, life expectancy at birth (LE) is an alternative mortality summary which shows similar problems. This indicator has the advantage of being very intuitive and easier to understand for the majority of people, therefore its use is increasingly demanded from health authorities. Its calculation also depends on the age distribution of mortality for each unit of study. Thus, although directly comparable between spatial units, it also poses the small area estimation problems arising from the age-specific risk estimates for each spatial unit . Several Bayesian hierarchical approaches have been previously proposed to estimate smoothed LEs in small areas studies. Congdon considers the smoothing of LEs but his model does not contain a specific age–space interaction term, so age–space risk variations are just a simple sum of separate age and space components. In other works [10,11,12,13,14] model area and age specific mortality rates in order to subsequently calculate LEs; nevertheless, their approaches do not include a fully structured (dependent) age–space interaction term jointly considering the variation of these two sources of dependence. These works do not use the dependence of contiguous age groups and locations for the age–space interaction term. As a consequence, these models fit the underlying overdispersion but could possibly fail to appropriately describe the space–age group structured interaction of the data. Consequently, the technical difficulties of structuring the dependence structure in age–space terms for LEs have not yet been properly addressed in the literature.\n\nIn this paper, an autoregressive proposal, based on the original model developed by Botella-Rocamora et al. , is made in order to model the age-specific probabilities of death (PoDs) for each spatial unit, which assumes stronger dependence between closer age groups and spatial units. This age–space dependence structure enables information to be transferred between neighboring (consecutive) age groups and neighboring areas, at the same time, providing more reliable age-specific PoDs estimates. Moreover, the model proposed can be easily generalized to the analysis of age–space–time datasets producing spatio-temporal age-specific rates, for example, or include any additional factor, such as sex, which could be of interest to be studied. The smoothed age-specific PoDs from this model could be later used to derive enhanced indicators, such as smoothed ASRs or LEs, of high epidemiological value.\n\nThis article is organized as follows. \"Methods\" section shows our modeling proposal for estimating age-specific PoDs in small areas geographical studies and its application to the construction of additional smoothed epidemiological indicators such as ASRs and LEs. The following section shows three case studies illustrating some real uses that smoothed age-specific PoDs could have, enhancing therefore traditional SMRs-based small areas studies. The first case study shows the application of the model introduced in \"Methods\" section to a real setting, a geographical study of lung cancer mortality in women. Its goal is to illustrate the convenience of considering age–space interaction in geographical studies. In the second case, the model is applied to study mortality from ischaemic heart disease for women in two cities at the census tract level. Smoothed ASRs are derived and compared for the census tracts of both cities, illustrating some advantages of this mortality indicator. In the last case study, the model is applied to estimate smoothed LEs, which is the most widely used synthetic indicator for characterizing overall mortality differences throughout areas. Finally, \"Discussion\" section summarizes the main contributions of our work.\n\n## Methods\n\n### Spatial smoothing of age-specific PoDs\n\nMartinez-Beneito proposed a unifying framework for multivariate disease mapping, i.e., for jointly mapping several diseases taking into account the spatial correlation that they might show. A second reformulation of this proposal, the M-model, was proposed in Botella-Rocamora et al. which enables the joint smoothing of tens of diseases in a single study. This approach, with important computational benefits, allows researchers to determine and take advantage of the correlations among diseases, revealing the existence of common risk factors or unknown associations among some diseases. In this model, dependence between spatial units is introduced in a structured way, while the relationship between diseases is introduced in an unstructured way, no prior dependence structure is assumed between diseases. However, this model allows considering also structured relationships between diseases, or geographical patterns in general, (such as an autoregressive structure) if this was considered convenient. Thus, the relationship between geographical patterns of different age groups should be possibly considered as a structured factor, reproducing its ordinal character. This modeling proposal could also be used in our case to model several risk patterns, one per age group, instead of several diseases, although assuming stronger correlations for contiguous age groups. This could be achieved, for example, by assuming spatially dependent first-order autoregressive dependency structures for age within each spatial unit.\n\nOur model proposes to model PoDs instead of age-specific rates. Age-specific rates are the relation between observed deaths and the person-years at risk available. Those person-years are not so easily available for small areas studies, which is why we propose to model PoDs instead of rates. Nevertheless, if mortality rates were really our goal, the person-years in the study could be reasonably approximated by the population at risk for each area multiplied by the years in the period of study, as we will see later. Additionally, LEs depend directly on PoDs instead of rates so the modeling of PoDs will be also suitable for deriving these indicators.\n\nThe autoregressive adaptation of the M-model for PoDs was made as follows. We changed the typical Poisson likelihood made for most disease mapping studies by a binomial distribution since the population of each (small) spatial unit is further divided into several age groups, which makes the denominator of many age specific PoDs quite low. As a consequence, the binomial assumption seems substantially more appropriate in this context as, in contrast to the Poisson case, it implicitly assumes that the number of deaths for each spatial unit and age group may not be higher than the corresponding population. Thus, let $$Y_{sa}$$, $$N_{sa}$$ and $$P^*_{sa}$$ be the number of observed deaths, population and (unknown) PoDs, respectively, for the s-th spatial unit and a-th age group, $$s=1,\\ldots,S$$; $$a=1,\\ldots,A$$. We use the asterisk in $$P^*_{sa}$$ in order to distinguish the smoothed age-specific PoDs that we are modeling from the raw age-specific PoDs, $$P_{sa}=Y_{sa}/N_{sa}$$. We assume that $$Y_{sa}$$ follows the binomial distribution:\n\n$$Y_{sa} \\sim \\text {Binomial}(N_{sa}, P^*_{sa}), \\quad s=1,\\ldots,S, a=1,\\ldots,A,$$\n\nand model the logit of the PoDs as:\n\n\\begin{aligned} logit(P^*_{sa}) = \\mu _{a} + \\theta _{sa} \\end{aligned}\n(1)\n\nwhere $$\\mu _{a}$$ represents the intercept of the a-th age group and $$\\theta _{sa}$$ models the PoDs variability between age groups and spatial units. Note that $$P^*_{sa}$$ in this model, and in general the PoDs that we are referring to, are the conditional probabilities of death at the age interval a given that you have survived the previous age intervals.\n\nBy modeling $$\\theta _{sa}$$ we will induce dependence between age groups and spatial units at the same time. The ideas of the M-model will be used for this end. Specifically, Botella-Rocamora et al. show that it is possible to induce both spatial and multivariate dependence on $$\\varvec{\\Theta }=(\\theta _{sa})$$ as the product of matrices:\n\n\\begin{aligned} \\varvec{\\Theta } = \\varvec{\\Phi } \\mathbf{M } \\end{aligned}\n(2)\n\nwhere $$\\varvec{\\Phi }$$ is an $$S\\times A$$ matrix whose a-th column $$\\varvec{\\Phi }_{\\cdot a}$$ follows a spatially correlated distribution. In the $$\\varvec{\\Phi }$$ matrix, the columns are independent of each other, and therefore they do not consider dependence between groups. The second term in this expression M, is an $$A\\times A$$ matrix which induces in $$\\varvec{\\Theta }$$ the dependence between age groups that we pursue.\n\nThe j-th column of $$\\varvec{\\Theta }$$, say $$\\varvec{\\Theta }_{\\cdot j}$$, contains the spatially referenced logit probabilities for the j-th age group. One can, therefore, interpret that Eq. (2) defines the spatial patterns in $$\\varvec{\\Theta }$$ as a linear combination of underlying latent variables whose coefficients correspond to the j-th column of M. Thus,\n\n\\begin{aligned} \\varvec{\\Theta }_{\\cdot j}= \\varvec{\\Phi }_{\\cdot 1} m_{1j} + \\ldots + \\varvec{\\Phi }_{\\cdot A} m_{Aj} \\end{aligned}\n(3)\n\nwhere $$m_{ij}$$ is the (i, j)-th entry in M. Matrix M combines, through linear combinations, the spatial patterns of $$\\varvec{\\Phi }$$ yielding therefore dependent spatial patterns.\n\nIn particular, we model the set of columns as independent Proper Conditional Auto-Regressive (PCAR) distributions, that is:\n\n\\begin{aligned} \\varvec{\\Phi }_{\\cdot a} \\sim N(0, \\sigma ^2 ({\\mathbf {D}}- \\gamma _a {\\mathbf {W}})^{-1}), \\end{aligned}\n\nwhere $${\\mathbf {W}}$$ and $${\\mathbf {D}}$$ are the adjacency and diagonal matrices typically summarizing the geographical structure in PCAR distributions (see for example).\n\nAccording to Botella-Rocamora et al. , for the separable case with $$\\gamma _1=\\cdots=\\gamma _A$$, the variance covariance matrix between age groups $$\\varvec{\\Sigma }$$ is equal to $$\\mathbf{M }^T \\mathbf{M }$$. Therefore, if we want the correlation between age groups to decrease as a function of their distance, M should be modelled in order to reproduce that effect. We will assume for simplicity a first-order autoregressive dependence structure between age groups. In that case, the covariance matrix between age groups would take the form:\n\n\\begin{aligned} \\Sigma _{ij} = \\rho ^{|i-j|}, \\end{aligned}\n\nwhere $$\\rho$$ is an autoregressive dependence parameter controlling the strength of the dependence between age groups. Note that the variance parameter of $$\\varvec{\\Sigma }$$ has been removed from this latest expression since the overall variance of $$\\varvec{\\Theta } = \\varvec{\\Phi } \\mathbf{M }$$ is already controlled by the term $$\\varvec{\\Phi }$$ by means of the variance parameter $$\\sigma ^2$$ of its columns. An M matrix inducing the mentioned autoregressive dependence between age groups could be, for instance, the upper-triangular Cholesky matrix of $$\\varvec{\\Sigma }$$, which has this simple expression:\n\n\\begin{aligned} \\mathbf{M }= \\left( \\begin{array}{ccccc} 1 &{} \\rho &{} \\rho ^2 &{} \\cdots &{} \\rho ^{A-1}\\\\ 0 &{} (1-\\rho ^2)^{1/2} &{} \\rho (1-\\rho ^2)^{1/2}&{} \\cdots &{} \\rho ^{A-2} (1-\\rho ^2)^{1/2}\\\\ 0 &{} 0 &{} (1-\\rho ^2)^{1/2} &{} \\cdots &{} \\rho ^{A-3} (1-\\rho ^2)^{1/2}\\\\ \\vdots &{} \\vdots &{} \\vdots &{} \\ddots &{} \\vdots \\\\ 0 &{} 0 &{} 0 &{} \\cdots &{} (1-\\rho ^2)^{1/2} \\end{array} \\right) . \\end{aligned}\n\nTo complete the model specification, an improper flat uniform prior is proposed for $$\\mu _a$$ and a uniform prior distribution on the interval $$[-1,1]$$ for $$\\rho$$. A vague uniform prior on [0, C] for a high enough (non-informative) value of C is also proposed for the standard deviation $$\\sigma$$ (see Gelman or pages 164–171 of Martinez-Beneito and Botella-Rocamora for more details). Finally, a uniform prior distribution on $$]\\lambda _{(1)}^{-1},\\lambda _{(I)}^{-1}[$$, where $$\\lambda _{(1)}$$ and $$\\lambda _{(I)}$$ are the lowest and highest eigenvalues of $${\\mathbf {D}}^{-1/2}{\\mathbf {W}}{\\mathbf {D}}^{-1/2}$$ respectively, is proposed for $$\\gamma _1,\\ldots,\\gamma _A$$, as suggested, for example, by Sun et al. or Martinez-Beneito and Botella-Rocamora .\n\nNote that the proposed model is equivalent to the spatio-temporal autoregressive model of Martinez-Beneito et al. . This proposal would model the matrix $$\\varvec{\\Theta }$$ as a first order autoregressive process as:\n\n\\begin{aligned} \\varvec{\\Theta }_{sa} \\sim N(\\rho \\varvec{\\Theta }_{s(a-1)},\\sigma ^2_{\\varvec{\\Theta }}) .\\end{aligned}\n\nIn this case, we would be using the autoregressive component for modeling dependence between age groups instead of temporal dependence. Nevertheless, we have posed our proposal as a M-model for several reasons. First, the M-model can be easily generalized to non-separable dependence structures; in fact, the model just proposed is already inseparable because of the different spatial correlation parameters ($$\\gamma _1,\\ldots,\\gamma _A$$) considered for the different spatial terms in the model. In a similar manner, different variance parameters ($$\\sigma _1^2,\\ldots,\\sigma _A^2$$) could be considered for these patterns, yielding therefore more flexible, heteroscedastic, covariance structures . Second, M-models are computationally convenient for modeling multivariate spatial patterns, which makes them an appropriate choice for fitting the data in regular Bayesian inference packages such as WinBUGS, OpenBUGS, Nimble… Finally, and in our opinion most importantly, M-models have been generalized to multidimensional models where several factors, besides the spatial component, are considered. This would make it possible to consider additional spatial patterns that could be correlated with the age-specific PoDs that we are modeling in order to enhance the estimates in the model. For example, mortality data from other sexes or causes of death could be additionally considered in order to yield improved age-specific PoDs in our data set. Alternatively, multidimensional modeling could be used to disaggregate the data, for example by subperiods, race groups… while maintaining a reasonable risk estimate quality by considering dependence between these new groups. In summary, in our opinion, all this makes the M-models an appropiate and flexible proposal for modeling the age-specific PoDs, as proposed above.\n\nWe should mention that some other previous proposals in the literature have dealt with the joint analysis of several dependence sources, such as age–space–time models. For example, Goicoa et al. proposed an age–space–time separable model where age and time are modelled as first order random walks and spatial dependence is modelled by means of a Leroux et al. dependence structure. Our proposal yields, in principle, more flexible dependence structures since different spatial correlations, for example, for each underlying spatial pattern are considered. Moreover, the autoregressive dependence structure for age groups allows the strength of this dependence source to be adapted. These modelling features could be implemented in INLA (the software package used in ), which in principle could take advantage of the sparse structure of the spatial and temporal precision matrices to speed up computations . Nevertheless, this would not be so advisable, since those modelling features would increase the number of parameters to be integrated out by INLA, what would make its fit substantially slower. Similarly, Goicoa et al. propose alternative age–space–time models, but using P-splines for modeling dependence for age and time. Once again, considering spatial random effects of different dependence parameters would seem problematic for this work as well. Thus, in this regard we find our proposal somewhat more suitable. Moreover, although some other Markov chain Monte Carlo (MCMC) based approaches have been proposed for the modeling of age–space–time interactions we find our proposal particularly convenient as it does not require a specific coding of the MCMC algorithm and, in contrast, it can be fitted with regular Bayesian software packages.\n\n### Epidemiological applications of the smoothed age-specific PoDs\n\nThe proposal above produces age-specific PoDs, $$P^*_{sa}$$, smoothed over space and age groups. It is important to note that any statistical indicator built on $${\\mathbf {P}}^*=(P^*_{sa})$$ will inherit the smooth character of $${\\mathbf {P}}^*$$, thereby producing smooth, and in principle more reliable, estimates of other more complex elaborate epidemiological indicators.\n\nFor example, ASRs are weighted averages of the age-specific death rates. The ASRs weights would be given by the age-composition of a reference population, so all the ASRs would represent the observed risks for a common (ideal) population; in this way the age composition of the units of study would in principle no longer be a confounding factor. Traditionally, the age-specific mortality rate for age group a and spatial unit s is given by:\n\n\\begin{aligned} R_{sa} = \\frac{Y_{sa}}{PersonYears_{sa}}\\approx \\frac{Y_{sa}}{T \\cdot N_{sa}}=\\frac{P_{sa}}{T} . \\end{aligned}\n(4)\n\nwhere T is the number of years in the period of study. If the period of study was just one year then $$T=1$$ and then $$R_{sa}=P_{sa}$$. Let $$pob_a$$ be the population in age group a in the reference population and let the standard weights be given by:\n\n\\begin{aligned} W_a=10^5 \\cdot \\frac{pob_a}{\\sum _a pob_a}. \\end{aligned}\n\nThen the ASR for the s-th spatial unit is usually defined as:\n\n\\begin{aligned} ASR_{s}=\\sum _a W_a \\cdot R_{sa}. \\end{aligned}\n(5)\n\nThe $$10^5$$ in $$W_a$$ allows us to undertand the ASRs as the number of deaths that we would expect per 100,000 people from the reference population. Obviously, the unreliability of $$P_{sa}$$ when the spatial units are small will be transferred to the ASRs, which will make them unreliable indicators. However, we could alternatively define smoothed Age-Standardized Rates (sASRs) by simply replacing $$R_{sa}$$ in the previous expression by $$R_{sa}^*=P_{sa}^*/T$$, that is:\n\n\\begin{aligned} sASR_{sa}=\\sum _a W_a \\cdot R^*_{sa} \\end{aligned}\n(6)\n\nwhich will inherit the smooth character of $$P^*_{sa}$$ and will therefore solve the small area estimation problems that traditional ASRs show.\n\nFollowing this same idea, many more epidemiological indicators relying on age-specific PoDs or mortality rates could be smoothed. For example, LEs are usually calculated from life tables as a direct function of the age-specific PoDs, the width of each age interval and the fraction of the last age interval survived for those people dying at each age interval . Additionally, particular care is required for the last age group since this is a right-opened interval, with no upper limit, so it deserves special attention. Nevertheless, if $$D_{sa}$$ is the marginal probability of death (which is a combination of the conditional PoDs) for group age a and spatial unit s, and $$age_a$$ is the mean age of death for the people dying at age group a, LEs could be alternatively defined as the expected value of the observed ages of death in the following way:\n\n\\begin{aligned} LE_s=\\sum _{a=1}^{A} age_a D_{sa}. \\end{aligned}\n(7)\n\nIn a similar manner to that made with life tables, $$age_a$$ could be calculated as the sum of the initial age of each interval and of the proportion of interval survived by those dying during that age interval. Usually, that proportion survived is assumed to be one half of each interval, except for the youngest age group where it is known that perinatal deaths make this proportion shorter . As a consequence, $$age_a$$ is usually taken as the central value for each age interval, which is equivalent to assuming the deaths to be uniformly distributed over those intervals. Regarding $$age_A$$, it is usual to assume a constant death rate, or equivalently an exponential distribution for the ages of death in the latest age group . According to the available data, that death rate could be estimated as the age-specific death rate for this group. Therefore, according to the exponential assumption for the ages of death for this interval, the average number of years lived for any person reaching the oldest age group would be the inverse of its death rate, that is: $$T/P_{sA}$$. Therefore, $$age_A$$ would be the sum of this quantity and the initial age for this age group.\n\nA detailed description of the life expectancy calculation from a life table can be found, for example, in the Public Health England template produced for this purpose based on the methodology described in .\n\nOnce the $$age_a$$ values have been calculated, Expression (7) can be formulated as a function of the conditional probabilities of death:\n\n\\begin{aligned} LE_s=\\sum _{a=1}^{A-1} age_a \\left( \\prod _{i<a} (1-P_{si}) P_{sa} \\right) + age_A \\prod _{i<A} (1-P_{si}). \\end{aligned}\n(8)\n\nThe reliance of Expression (8) on the observed raw age-specific (conditional) PoDs, $$P_{sa}$$, makes it clear why LEs become unreliable in small areas studies. Nevertheless, by changing the raw age-specific PoDs for the smoothed age-specific PoDs, $$P^*_{sa}$$, resulting from the above model, we could obtain reliable life expectancies, smoothed Life Expectancy (sLE), suitable for small areas studies.\n\nSimilar procedures could be proposed for any other epidemiological indicator relying on age-specific PoDs, such as disability-free life expectancy, potential years of life lost… to cite just two. These indicators would be alternative tools to the traditional use of SMRs in small areas studies that would highlight new aspects of the data that regular SMRs are not able to reveal.\n\nFinally, we find it interesting to note that, since the proposed model is posed under a Bayesian approach, MCMC is used for making inference about that model. As a consequence, credible intervals and other additional variability measures can be easily computed within the MCMC itself for any of the proposed indicators. This makes their comparison particularly easy.\n\n## Case studies\n\nIn this section, we are going to make use of some real case studies to illustrate the use of the proposed methodology and the advantages of the new smoothed epidemiological indicators over the traditional use of smoothed SMRs, from now on “sSMRs”.\n\nAll the models used for the following case studies have been run in WinBUGS . The pbugs R library was used for speeding up computations by parallelizing the sampling of the different chains of the MCMC. Rmarkdown documents with the code used to reproduce all three analyses can be found at Additional file 1. For all three analyses, three chains were run with 30,000 iterations, the first 5000 of which were discarded as a burn-in period. A thinned sample was obtained by saving one out of every 75 iterations. Regarding convergence checking, the Brooks–Gelman–Rubin statistic has been checked to be lower than 1.1 and the effective sample size to be above 100 for all the parameters saved during the MCMC. All these criteria were successfully met for all three case studies.\n\nAll three models that were finally run for all three case studies correspond to separable age–space dependence structures, with $$\\gamma _1=\\cdots=\\gamma _A$$. The reason for this is that for none of the three data sets have we found evidence of inseparability (the confidence intervals for $$\\gamma _1,\\ldots,\\gamma _A$$ for all three studies substantially overlapped). As a consequence, we have decided to show the results of the simpler separable case. However, we should mention that we have found evidence of inseparability for some other case studies that have not been finally included in the paper for reasons of space.\n\n### Case study 1: interaction between age groups and space\n\nIn this first case study, the proposed model has been applied to the study of lung cancer mortality in women in Comunitat Valenciana (Spain) for the 2008–2017 period. Municipalities were the spatial units of study, with a total of 542 municipalities composing the whole Comunitat Valenciana (CV). The average number of women in CV during the period of study is around 2.5 millions. The mean number of women per municipality is 4695 while the corresponding median is 744. Nowadays, lung cancer is the second most common cancer mortality cause in women in CV after breast cancer, with a total of 4232 deaths for the whole period of study. Mortality data were provided by the mortality registry of CV. Population data was obtained from the Spanish National Statistics Institute. Both sources of information are considered to have good data quality at this level of disaggregation. It has not been necessary to process missing data or other data quality issues.\n\nSince lung cancer mainly affects elderly people, the younger age groups have been merged, resulting in the following 11 age intervals: [0, 40), [40, 44), [45, 50), …, [80, 85) and [85,…). As a consequence, we have 5962 ($$=11\\cdot 542)$$ age-specific PoDs to estimate, more than observed deaths. Therefore, even though lung cancer shows very high mortality values for our data set, we still have 4646 cells out of the 5962 municipality-age group combinations (78%) with zero deaths. This makes evident the need for some kind of modeling in order to derive reliable results.\n\nThe left hand side of Fig. 1 shows the raw PoDs for each area and age group directly obtained from 4. Note that age-specific rates would be just the PoDs divided by 10, the number of years of the period of study. The right hand side of Fig. 1 shows the corresponding smoothed PoDs provided by the model. In both cases, the age-specific PoDs for the whole CV, Almazora and Denia (two illustrative municipalities) have been highlighted. The raw PoDs show evidence of small area estimation problems. There are no observed cases for most age groups and municipalities and when some death is observed this makes the probability of death appear extremely high, mainly for the youngest age groups, which produces highly volatile estimates and sawtooth-shaped curves for most municipalities. These extreme raw age-specific PoDs would evidently distort subsequent epidemiological indicators based on them. On the other hand, the estimated smoothed PoDs, using information from neighboring age groups and areas, yield a much more stable and credible performance where most of the uncertainty in the raw PoDs has been filtered out. Nevertheless, some variability between municipalities is retained, for example, several municipalities stand out in this second plot for having particularly high risks for the oldest groups. These municipalities were completely unnoticed in the left hand side plot where the underlying noise does not allow conclusions of any kind to be drawn.\n\nIn order to confirm the relevance of the age–space interaction for this data set, we have run a second alternative model without interaction. In other words, this second model assumes simply $$logit(P^*_{sa})=\\mu _a+\\theta _s$$ instead of having a $$\\theta _{sa}$$ term that varies for each spatial unit and age group. We have compared the Deviance Information Criterion (DIC) for both models, resulting in a DIC of 6546.5 for the model without interaction and 6508.0 for the original model with interaction. Therefore, age–space interaction seems required in order to appropriately describe the variability underlying this data set. Although some additional model selection criteria could be used for this comparison, as suggested for example by Duncan and Mergensen , the magnitude of the DIC difference already points out important fit differences between both models.\n\nWe have decomposed the variability on $$logit(P^*_{sa})$$ into three separate terms in order to visualize the sources of variability of this data set. Specifically, we have decomposed that matrix into two overall age and spatial effects and an interaction term explaining the variability that cannot be explained by these main terms (see Adín et al. or page 285 of Martinez-Beneito and Botella-Rocamora for more details on this decomposition in a spatio temporal setting). The age effect (result shown in Additional file 1), which is defined as the collection of column means of the matrix $$\\varvec{\\Theta }$$, unsurprisingly shows an upwards trend of the risks as a function of age, with a steeper trend until the [55, 59] group and a milder constant increase for the oldest age groups. Figure 2 shows both the spatial and interaction terms for each municipality. The spatial term, in the left hand side plot, which is defined as the collection of row means of the matrix $$\\varvec{\\Theta }$$, shows a clear spatial pattern, with high risks mainly in the southern and south-eastern part of CV (this was already described at Zurriaga et al. ). The cuts for the groups in this plot correspond to septiles of the spatial term, which is in the logits scale. The right hand side plot shows the interaction term for each municipality (one line per municipality). The comparison of the scales of both plots shows that substantial variability still holds for the interaction term, with a range of values comparable to that of the spatial term. As a consequence, particular risk excesses for some age groups and municipalities are as important as the overall risk excesses (for all age groups as a whole) for those same municipalities. In particular, Almazora and Denia show opposing performances in age specific terms. Specifically, Denia exhibits particularly low risks for the youngest age groups while the oldest groups show particularly high risks. On the contrary, Almazora shows the opposite, exhibiting better performance for the older age groups.\n\nFigure 3 shows choropleth maps for the interaction term for several of the age groups considered. Almazora and Denia have been highlighted in the first of these plots. We can see how, in general, the younger groups have a particularly bad performance in the northern and western parts of the CV. In contrast, these same areas have a particularly good performance in the oldest age groups. Note the similarity of the areas shown in this graph with those also outstanding for the spatial term. In particular, the correlation of the spatial component and the interaction term for the group younger than 40 is − 0.65; 0.42 for the age group [70, 74] and 0.32 for the age group older than 85. As a consequence, the combination of the spatial and interaction terms for the younger groups (result not shown) produces a much flatter spatial pattern than that of the spatial term, while that spatial pattern is reinforced with the interaction term for the oldest age groups, which is similar to the spatial pattern in Fig. 2. Therefore, the geographical pattern arising in the spatial term of this analysis is mainly the effect of the risk patterns corresponding to the oldest age groups since that spatial distribution for the younger groups is substantially flatter. This kind of result cannot be obtained from the typical sSMRs analyses usually made by default when studies are carried out on sets of small areas.\n\n### Case study 2: smoothed ASRs\n\nIn this case we have applied the model in \"Methods\" section to the study of ischaemic heart disease (IHD) mortality for women aged over 45 years, during the period 1996–2015. Mortality data were provided by the MEDEA3 Project (“Socio-economic and environmental inequalities in the geographical distribution of mortality in large cities in Spain (1996–2015)”, PI16/01004). Population data was obtained from the Spanish National Statistics Institute. Nine age groups: [45, 50), [50, 55), …, [80, 85) and [85,…) were considered for this study. Two separate studies, with independent models, were carried out to analyse IHD mortality in the two largest CV cities: Valencia and Alicante.\n\nIn this case, the spatial unit of study were census tracts, with a total of 531 and 178 units for Valencia and Alicante, respectively.\n\nIn this case study, we explore the use of sASRs as an alternative to sSMRs for small areas geographical analyses. Figure 4 shows several choropleth maps summarizing the main results for this analysis. Specifically, the top-left plot in that figure shows the raw ASRs for the census tracts of Valencia. This plot shows substantial noise, which hardly allows any meaningful conclusion to be drawn. Note that the census tract with the highest raw ASR is estimated to have a risk more than 10 times (!) higher than that with the lowest raw ASR. In the top-right plot we show the sASRs calculated as described in the previous section. In contrast to the raw ASRs, the sASRs show a clearer pattern where some neighborhoods show higher risks. In this way, the benefit of using smoothed epidemiological indicators becomes clear. For comparability, quintiles of the Valencia sASRs have been used as cuts for both ASR maps in the top row of Fig. 4. The bottom-left plot of Fig. 4 shows, as a reference, the sSMRs drawn from a typical small area study fitting the model. Quintiles of the sSMRs have been used for cutting the categories for this choropleth map. Note that, despite some small differences, both sSMR and sASR choropleth maps resemble each other, since both are summarizing the mortality risks of the same data set in different manners. In fact, the correlation between both quantities for the Valencia census tracts is 0.95.\n\nDespite the resemblance of the sSMR and sASR maps, the ASRs shows some advantages over the traditional sSMRs that would be appropiate to value. In contrast to sSMRs, sASRs are comparable for the different census tracts of a city, so they could be used, for example, for comparing the risks of two particular census tracts. Thus, the probability that the Valencian census tract with the highest sASR (posterior mean) has a sASR higher than that with the lowest sASR (posterior mean) is virtually 1 for our data set, highlighting an important spatial variability. This statistic should be more powerful than the typical $$P(sSMR>100)$$ used in many traditional disease mapping analyses since the mentioned sASR statistic takes into account the two extremes of the sASRs distribution instead of comparing the risk of each census tract with that of the reference population.\n\nAdditionally, the sASRs calculated could be further compared to other additional ASRs corresponding to other areas of study. Thus, our sASR estimates could be compared for example to the ASR for the overall Valencian Region, Spain or even ASRs corresponding to other countries. In this manner, the use and scope of the generated results would be much wider than for SMRs. As an example, the bottom-right plot of Fig. 4 shows the distributions of the sASRs (their posterior means) for the Valencia and Alicante census tracts. As shown in that figure, most of the Valencia census tracts have sASR values smaller than any of the Alicante census tracts. As a matter of percentiles, the 95% percentile of the sASR distribution in Valencia (178.9 deaths per $$10^5$$ women) is lower than the 5% percentile for Alicante (203.5). In other words, the census tracts with the highest IHD sASRs in Valencia have comparable mortality risks to those census tracts with the lowest mortality by IHD in Alicante. This should prompt the Valencian health authorities to take a close look at this issue, which would surely go unnoticed with a traditional sSMRs-based small area study.\n\n### Case study 3: smoothed life expectancies\n\nFinally, in this third case study, age–space PoDs have been applied to the study of LEs, for each sex, once again for the whole Comunitat Valenciana (CV) for the period 2014–2017. In this case, mortality for all causes has been considered. Mortality data were provided by the mortality registry of the CV. Population data was obtained from the Spanish National Statistics Institute. The spatial aggregation considered was the municipality and 19 age groups: [0, 1), [1, 4], [5, 9), [10, 14),…, [80, 85) and [85,…) were considered for this analysis.\n\nFigure 5 shows the municipal LEs for men and women (separately) for the Valencian municipalities. The two maps on the left side of the figure show the raw LEs, directly calculated from the raw age-specific PoDs. The two maps on the right, show the smoothed counterparts of the maps on the left with the corresponding smoothed LEs. For comparability, cuts for these choropleth maps have been defined according to the smoothed LEs septiles for each sex. The legends of the raw LE plots, highlight the high variability of these indicators. Thus, raw LEs for men range from 48.7 to 104.0 and from 50.8 to 110.0 for women, which seems hard to believe. Moreover, 22 and 16 municipalities, respectively for men and women, showed infinite LEs since no deaths were observed in them during the period of study in the final age interval . Smoothed LEs, however, show much more reasonable (moderate) variability than the raw LEs. This result clearly shows the need for smoothed age-specific PoDs for calculating LEs when dealing with small areas.\n\nMuch clearer spatial patterns can be observed in the smoothed LE maps of Fig. 5, compared to their unsmoothed counterparts. Thus, for men, a clear cluster of low LE levels becomes evident in the eastern-central part of CV. This was not so evident according to the raw LEs. Moreover, some areas where the raw LEs showed high heterogeneity (see for example the north-western part of CV), where most of the municipalities are sparsely populated, now show a much more smoothed (spatial) behaviour which seems considerably more reasonable. For women, something similar happens. The smoothed LEs show a clearer spatial pattern and heterogeneity seems to have disappeared for the sparsely populated areas.\n\nAdditionally, the smoothed LEs in Fig. 5 allow interesting conclusions to be drawn, such as, for example, that geographical inequalities in men in terms of LEs (12.7 years between the most extreme municipalities) are substantially higher than those in women (5.5 years). According to the raw LEs these differences are reversed, 55.3 years for men and 59.2 years for women, although evidently these values are clearly untenable. The use of smooth LEs allows us to draw some meaningful conclusion in this regard. Finally, we would like to stress that small areas LE analyses provide a complementary view to that provided by sSMR based analyses. LEs take into account not just the mortality at each spatial unit but also the ages when those deaths take place, so LEs analyses complement the results that regular sSMR small areas analyses typically yield.\n\n## Discussion\n\nAlthough spatio-temporal and multivariate disease mapping analyses on small areas have become quite popular, the same cannot be said for age–space small areas analyses. Nevertheless, as illustrated, the same methods that are used in both spatial and multivariate contexts could also be regularly used for age–space studies where age groups are disaggregated and separately studied, although considering dependence between them.\n\nIn this work, the M-model is used in order to model the age-specific PoDs for each spatial unit, which assumes stronger dependence between closer age groups and spatial units. As shown, this age–space dependence structure enables information to be transferred between contiguous age groups and neighboring areas, at the same time, providing therefore more reliable (smoothed) age-specific PoDs estimates.\n\nObviously, there are other alternative possibilities for the age-dependency structure used in the article. However, the one used seems appropriate given that it makes it possible to determine, within the same model, whether or not there is spatial and inter-age group dependency in the data, and even to quantify the strength of these sources of dependency. The small number of age groups in our case studies, and in most of the possible applications that we foresee, could make the discussion and selection of alternative dependency structures for age groups very difficult.\n\nThere are multiple reasons to use the M-model for age-specific PoDs. The first of them is that it induces both spatial and multivariate dependence by simply multiplying two matrices. Secondly, the M-model can be easily generalized to non-separable dependence structures, resulting in more flexible, heteroscedastic, covariance structures . In addition, these models are computationally convenient for modeling multivariate spatial patterns, which makes them an appropriate choice for fitting the data in regular Bayesian inference packages such as WinBUGS, OpenBUGS, Nimble… Moreover, M-models have already been implemented for the joint analysis of several correlated spatial patterns in INLA, either for a separable model for a large number of spatial patterns , or for an inseparable joint analysis of three spatial patterns . Thus INLA should be also born in mind as a potential tool for this kind of analyses. Finally and the most important in our opinion, is that our proposal facilitates the future incorporation of other factors such as time or sex in a straightforward manner, following the proposal of multidimensional models by Martinez-Beneito et al. . This allows us to consider additional spatial patterns that could be also correlated with the age-specific PoDs that we are modeling in order to enhance the estimates in the model current estimates.\n\nBeyond sASRs and sLEs calculations, the simple study of PoDs for visualizing the different age-specific spatial patterns is also interesting. Moreover, the study of those PoDs is particularly interesting when an inseparable model provides some fit improvement. For example, in another additional case study not presented here, we also applied our proposal for modeling all-cause mortality in the city of Valencia. In that case, applying the M-model at space–age group level, the smoothed age specific PoDs showed a pattern with stronger spatial dependence for the youngest age groups (higher values for the corresponding $$\\gamma _a$$) than for the oldest age groups. The corresponding PoDs maps showed as if geographical inequalities existed for the youngest age groups, which pointed towards risk excesses for the deprived neighborhoods, but this effect diluted for older age groups since basically old people die all around while young people die, in general, just in these regions. Therefore, the modeling of non-separable age–space structures seems another additional application of our model, although we have not illustrated with such a detail for questions of space.\n\nIn addition, any statistical indicator built on the smoothes age-specific PoDs inherit that smoothed character, yielding therefore more realiable estimates. Thus, in two of the three case studies we have two of the most relevant epidemiological indicators: the age standardized rate and the life expectancy. We have explored their use as an alternative to sSMR for small areas geographical analyses. On one hand, deriving an ASR version of potential use in small areas studies, with the direct comparation posibilities between areas that this brings, should be considered as an additional benefit of our proposal. On the other hand, smoothed life expectancies provides once again a version of this synthetic health indicator of potential use in small areas studies. Studies based on this indicator that take also into account the age of death could bring new possibilities to spatial epidemiological studies. Nevertheless, additional smoothed epidemiological indicators depending on PoDs may also be derived from the smoothed age–space PoDs, such as the number of potential years of life lost. Our study makes possible the study of those indicators also for small areas.\n\n## References\n\n1. Richardson S, Thomson A, Best N, Elliot P. Interpreting posterior relative risk estimates in disease-mapping studies. Environ Health Perspect. 2004;112(9):1016–25.\n\n2. Ahmad OB, Boschi-Pinto C, Lopez AD, Murray CJL, Lozano R, Inoue M. Age standardisation of reports: a new who standard (technical report)., GPE Discussion Paper SeriesGeneva: World Health Organization; 2001.\n\n3. Neison FGP. On a method recently proposed for conducting inquiries into the comparative sanatory condition of various districts. J R Stat Soc Lond. 1844;7:40–68.\n\n4. Fleiss LBPMC, Joseph L. Statistical methods for rates and proportions. 3rd ed. New York: Wiley; 2003.\n\n5. Curtin LR, Klein RJ. Direct standardization (age-adjusted death rates), vol. 6. US Department of Health and Human Services, Public Health Service, Centers for Disease Control and Prevention, National Center for Health Statistics. 1995.\n\n6. Kafadar K. Smoothing geographical data, particularly rates of disease. Stat Med. 1996;15:2539–60.\n\n7. Ezzati M, Friedman AB, Kulkarni SC, Murray CJL. The reversal of fortunes: trends in county mortality and cross-county mortality disparities in the United States. PLoS Med. 2008;5:0557–688.\n\n8. Eayres D, Williams ES. Evaluation of methodologies for small area life expectancy estimation. J Epidemiol Community Health. 2004;58(3):243–9.\n\n9. Congdon P. A life table approach to small area health need profiling. Stat Model. 2002;2:63–88.\n\n10. Jonker MF, van Lenthe FJ, Congdon PD, Donkers B, Burdorf A, Mackenbach JP. Comparison of Bayesian random-effects and traditional life expectancy estimations in small-area applications. Am J Epidemiol. 2012;176(10):929–37.\n\n11. Congdon P. Estimating life expectancies for us small areas: a regression framework. J Geogr Syst. 2014;16(1):1–18.\n\n12. Congdon P. Area variations in multiple morbidity using a life table methodology. Health Serv Outcomes Res Methodol. 2016;16:58–74.\n\n13. Dwyer-Lindgren L, Bertozzi-Villa A, Stubbs RW, Morozoff C, Mackenbach JP, van Lenthe FJ, Mokdad AH, Murray CJL. Inequalities in life expectancy among us counties, 1980 to 2014: temporal trends and key drivers. JAMA Intern Med. 2017;177(7):1003–111.\n\n14. Alexander M, Zagheni E, Barbieri M. A flexible Bayesian model for estimating subnational mortality. Demography. 2017;54(6):2025–41.\n\n15. Botella-Rocamora P, Martinez-Beneito MA, Banerjee S. A unifying modeling framework for highly multivariate disease mapping. Stat Med. 2015;34(9):1548–59. https://doi.org/10.1002/sim.6423.\n\n16. Martinez-Beneito MA. A general modelling framework for multivariate disease mapping. Biometrika. 2013;100(3):539–53. https://doi.org/10.1093/biomet/ast023.\n\n17. Martinez-Beneito MA, Botella Rocamora P. Disease mapping from foundations to multidimensional modeling. Boca Raton: CRC Press; 2019.\n\n18. Gelman A. Prior distributions for variance parameters in hierarchical models. Bayesian Anal. 2006;1:515–34.\n\n19. Sun D, Tsutakawa RK, Speckman PL. Posterior distribution of hierarchical models using CAR(1) distributions. Biometrika. 1999;86(2):341–50. https://doi.org/10.1093/biomet/86.2.341.\n\n20. Martinez-Beneito MA, López-Quílez A, Botella-Rocamora P. An autoregressive approach to spatio-temporal disease mapping. Stat Med. 2008;27:2874–89.\n\n21. Corpas-Burgos F, Botella-Rocamora P, Martinez-Beneito MA. On the convenience of heteroscedasticity in highly multivariate disease mapping. TEST. 2019;28:1229–500.\n\n22. Martinez-Beneito MA, Botella-Rocamora P, Banerjee S. Towards a multidimensional approach to Bayesian disease mapping. Bayesian Anal. 2017;12:239–59. https://doi.org/10.1214/16-BA995.\n\n23. Leroux BG, Lei X, Breslow N. Estimation of disease rates in small areas: a new mixed model for spatial dependence. In: Halloran ME, Berry D, editors. Statistical models in epidemiology, the environment and clinical trials. Berlin: Springer; 1999.\n\n24. Goicoa T, Ugarte MD, Etxebarria J, Militino AF. age–space–time CAR models in Bayesian disease mapping. Stat Med. 2016;35:2391–405.\n\n25. Rue H, Martino S, Chopin N. Approximate Bayesian inference for latent Gaussian models by using integrated nested Laplace approximations. J R Stat Soc B (Stat Methodol). 2009;71(2):319–92.\n\n26. Goicoa T, Adin A, Etxeberria J, Militino AF, Ugarte MD. Flexible Bayesian P-splines for smoothing age-specific spatio-temporal mortality patterns. Stat Methods Med Res. 2017;28(2):384–403.\n\n27. Quick H, Waller LA, Casper M. Multivariate spatiotemporal modeling of age–space stroke mortality. Ann Appl Stat. 2017;11(4):2165–77.\n\n28. Chiang CL. The life table and its applications. Malabar: Krieger Publishing; 1984.\n\n29. Williams E, Dinsdale H, Eayres D, Tahzib F. Calculating life expectancy in small areas. Technical report, South East Public Health Observatory. 2005.\n\n30. Silcocks PBS, Jenner DA, Reza R. Life expectancy as a summary of mortality in a population: statistical considerations and suitability for use by health authorities. J Epidemiol Community Health. 2001;55(1):38–433.\n\n31. PHE: life expectancy template. https://fingertips.phe.org.uk/documents/PHELifeExpectancyCalculator.xlsm.\n\n32. Lunn D, Thomas A, Best N, Spiegelhalter D. WinBUGS—a Bayesian modelling framework: concepts, structure, and extensibility. Stat Comput. 2000;10:325–37. https://doi.org/10.1023/A:1008929526011.\n\n33. Vergara C, Martinez-Beneito MA. Pbugs. https://github.com/fisabio/pbugs.\n\n34. Brooks SP, Gelman A. General methods for monitoring convergence of iterative simulations. J Comput Graph Stat. 1998;7:434–55.\n\n35. Carlin BP, Gelman A, Neal RM. Markov chain Monte Carlo in practice: a roundtable discussion. Am Stat. 1998;52(2):93–100.\n\n36. Spiegelhalter DJ, Best NG, Carlin BP, Van Der Linde A. Bayesian measures of model complexity and fit (with discussion). J R Stat Soc Ser B (Stat Methodol). 2002;64:583–641. https://doi.org/10.1111/1467-9868.00353.\n\n37. Duncan EW, Mengersen KL. Comparing Bayesian spatial models: goodness-of-smoothing criteria for assessing under- and over-smoothing. PLoS ONE. 2020;15:0233019. https://doi.org/10.1371/journal.pone.0233019.\n\n38. Adín A, Martinez-Beneito MA, Botella-Rocamora P, Goicoa T, Ugarte MD. Smoothing and high risk areas detection in space–time disease mapping: a comparison of P-splines, autoregressive and moving average models. Stoch Environ Res Risk Assess. 2017;31:403–15. https://doi.org/10.1007/s00477-016-1269-8.\n\n39. Zurriaga O, Vanaclocha H, Martínez-Beneito MA, Botella Rocamora P. Spatio-temporal evolution of female lung cancer mortality in a region of Spain: is it worth taking migration into account? BMC Cancer. 2008;8(35):1. https://doi.org/10.1002/sim.64231.\n\n40. Besag J, York J, Mollié A. Bayesian image restoration, with two applications in spatial statistics. Ann Inst Stat Math. 1991;43:1–21. https://doi.org/10.1007/BF00116466.\n\n41. Vicente G, Goicoa T, Ugarte MD. Bayesian inference in multivariate spatio-temporal areal models using inla: analysis of gender-based violence in small areas. Stoch Environ Res Risk Assess. 2020;34:1421–40. https://doi.org/10.1002/sim.64233.\n\n42. Palmi-Perales F, Gomez-Rubio V, Martinez-Beneito MA. Bayesian multivariate spatial models for lattice data with INLA. 2020. arXiv:1909.10804.\n\n## Acknowledgements\n\nThe authors acknowledge the support of the research Grant PI16/01004 (co-funded with FEDER grants) of Instituto de Salud Carlos III.\n\n## Author information\n\nAuthors\n\n### Contributions\n\nJP, PB and MAM contributed to the conception of the work, the modelization and the analysis. All authors discussed the results and contributed to the final manuscript. All authors read and approved the final manuscript.\n\n## Ethics declarations\n\n### Competing interests\n\nThe authors declare that they have no competing interests.\n\n### Publisher's Note\n\nSpringer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.\n\n## Supplementary information", null, "" ]
[ null, "https://ij-healthgeographics.biomedcentral.com/track/article/10.1186/s12942-020-00251-z", null ]
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https://math.stackexchange.com/questions/1757476/why-is-this-determinant-positive
[ "# Why is this determinant positive?\n\nI have seen that the $k$-dimensional volume of an parallelepiped in $\\mathbb{R}^n$, i.e., $$P(v_1, \\ldots, v_k) = \\{t_1v_1 + \\dotsb + t_kv_k : 0 \\le t_i \\le 1 \\}$$ is $\\sqrt{\\det(T^{\\top}T)}$, where $T$ is the $n\\times k$ matrix with columns $v_1, \\ldots, v_k$.\n\nHow do we know that $\\det(T^{\\top}T)$ is non-negative?\n\n• The Cauchy-Binet identity shows that $\\det\\left(T^T T\\right)$ is the sum of the squares of all $k\\times k$ minors of $T$. Sums of squares are nonnegative. – darij grinberg Apr 25 '16 at 3:24\n• Look at SVD decomposition, which always exist: $T = U\\Sigma V^T$ where $\\Sigma$ is diagonal and $U, V$ are unitray you get $T^\\perp T = V\\Sigma^T U^T U\\Sigma V^T = V\\Sigma^T \\Sigma V^T = V \\Sigma^2 V^T$ (using the fact that $U^TU = I$).Therefor $\\det(T^\\perp T) = \\det(V) \\det(\\Sigma^2) \\det(V^T) = \\det(\\Sigma^2)$ using the fact that determinat of unitary matrix is $1$. The result follows since $\\Sigma^2$ is diagonal matrix with non-negative values. – them Apr 25 '16 at 12:08\n• You may also be interested in this question: matheducators.stackexchange.com/q/10395/117 – Steven Gubkin Apr 25 '16 at 13:56\n\n## 1 Answer\n\n$T^{\\top}T$ is positive semidefinite, so all the eigenvalues are non-negative.\n\nThe determinant of $T^{\\top}T$ is the product of the eigenvalues; hence, it is non-negative.\n\n• So as it is positive semi-definite $det(T^TT)$ can be equal to zero? Is this true over $\\mathbb{C}^n$ also? – josh Apr 25 '16 at 9:17\n• @josh Over $\\mathbb{C}$ you can do it with the Hermitian transpose. – egreg Apr 25 '16 at 10:30" ]
[ null ]
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https://dc.edu.au/hsc-physics-advanced-mechanics/
[ "# HSC Physics – Module 5 – Advanced Mechanics\n\n## Projectile Motion\n\nA projectile is any object that is moving freely through space without any power source driving it (eg motor or propeller engine). The analysis of the motion of such objects can occur in\n\n• 1 dimension\n• 2 dimensions\n\n### Projectile motion in 1 dimension\n\nA projectile moving in 1 dimension means that the projectile is can only move in 2 directions (e.g. up or down, left or right, forwards or backwards). Solving projectile motion questions in 1 dimension requires the following equations of motion: Manipulation of the above equations will allow you to get the quantity which the question wants you to calculate. A good example would be a free-falling projectile.\n\n### Free-falling projectiles\n\nIn these cases, the only force acting on a projectile is the weight force (otherwise known as gravity). Therefore, the projectile will experience a constant acceleration downwards.\n\n### Projectile motion in 2-dimensions\n\nHere, the object can move along two different ‘directions’. E.g. a rocket launched at an angle will be travelling forwards as well as upwards. A key property of projectiles moving in 2 dimensions is that it can be split into two different components:\n\n• A horizontal component.\n• A vertical component.\nThese 2 components are completely independent of each other and therefore our analysis of them can be done separately.\n\nTrigonometry may be used to calculate the vertical and horizontal components of velocity. Quite often, the horizontal component of motion will consist only of the object travelling at constant velocity. The vertical component will often have just gravitational acceleration. The combined effect of the horizontal and vertical motion often results in the projectile travelling in a parabolic trajectory.\n\n## Circular motion\n\nIn the HSC, we only look at uniform circular motion. Uniform circular motion means that the object moves in a circle at a constant speed.\n\n• However, the velocity of the object is always changing since the direction of the velocity is always changing and so the object is technically always accelerating.\n• There is a force that always points towards the centre of the circle called the centripetal force. The centripetal force is always perpendicular to the velocity vector.", null, "The centripetal force is given by the following formula:\n\n• Where Fc is the centripetal force given in Newtons.\n• M is the mass of the moving object given in kilograms.\n• V is the velocity of the object given in ms-1.\n• R is the radius of the circular path and is given in metres.\n\nUsing Newton’s Law we can deduce that the centripetal acceleration is:\n\n### Period, angular velocity and frequency\n\nThe time required to travel around the circle is called the period, T, of the motion. The number of rotations each second is called the frequency, f, of the motion. These two quantities can be related through the following equation: The angular velocity is the angle of rotation in a given time. The angular velocity is given by:", null, "### Work and Energy\n\nThe most important concept here is the conservation of mechanical energy. Sometimes energy is dissipated or transformed into light, heat and/or sound and thus the total energy of the system is reduced. In a problem question, an external force usually refers to friction or a thrust force from an engine. Therefore, the conservation of mechanical energy would apply given that no other forms of energy are involved (e.g. heat, sound and/or light). The above concept is most often used to calculate the speed of the moving object at certain points in the circular motion (particularly vertical circular motion).\n\n### Work\n\nWork is defined as the transfer of energy from one object to another and/or the transformation of energy from one form to another. A force does work on an object when it acts on a body causing a displacement in the direction of the force. The formula for work is given by:", null, "Work and energy are scalar quantities measured in Joules. To find the work done on an object, use the net force. In the context of circular motion\n\n• There is always a net centripetal force acting on the object. Therefore, the object is always being accelerated by the centripetal force.\n• However, because the centripetal force is always perpendicular to the direction, therefore the force does no work according to the above formula.\n\n### Torque\n\nThis involves an object rotating around a pivot point. E.g. closing a door or turning a steering wheel. In these situations, the force acts to provide a turning effect or torque ( Torque is a vector, so it has a magnitude and a direction. The amount of torque applied on an object is directly proportional to the perpendicular distance between the pivot point and the line of action of the force. This perpendicular distance is called the force arm.", null, "", null, "It is only the component of the force which is perpendicular to the line of action which generates effective torque. The torque equation is given by:", null, "Note that the above 2 equations are equivalent. To convert between the two formulas requires use of trigonometry. An example of this conversion in the context of an opening door can be seen below:", null, "### Examples of uniform circular motion\n\nBanked tracks Often tracks are tilted at an angle to provide additional forces to allow vehicles to negotiate a sharp corner without slipping. The banked track allows the vehicle to take advantage of the normal reaction force from the road to provide the centripetal force. The design speed is the speed at which a vehicle can negotiate a banked track with 0 sideways friction. The situation is illustrated as follows:", null, "It is crucial to draw a force diagram to figure out what is going on.\n\n### A mass on a string\n\nThe situation here is that a mass is tied to a string and travels in uniform circular motion at a level below the point at which the string is attached to the pole. See diagram below:", null, "The tension in the string is the force which provides the centripetal force.\n\n### Cars moving around horizontal circular bends\n\nCars which move around horizontal bends rely solely on friction to provide the centripetal force. In these cases, we can pretty much ignore gravity and the normal force as they do not affect the horizontal situation. Friction is the only force which provides the centripetal force.", null, "## Motion in Gravitational Fields\n\n### Newton’s Law of Universal Gravitation\n\n• Where r is the distance of mass m1 from mass m2 in metres.\n• G is Universal Gravitational Constant: 6.67 x 10-11 N m2 kg-2.\n• M1 and m2 are masses in kg.\n\nThis measures the gravitational force of attraction of between two objects. The direction is usually towards the object with larger central mass. G can also be found on other planets by:\n\n• Where G is the gravitational constant.\n• R is the radius of the planet.\n• Mp is the mass of the planet.\n\nThis equation assumes that the mass of Earth is uniformly distributed. This value of g is also the value of free fall acceleration at the point.\n\n## Weight force on various locations on Earth\n\nThe weight force which an object experiences at different locations on Earth vary according to different locations. This is because at different locations, the strength of the gravitational field of the Earth varies as the Earth is not a perfect sphere.\n\n### Orbital velocity and orbital period\n\nFor satellites and planets that undergo roughly centripetal motion around the Earth or Sun, the gravitational force provides the centripetal force. Therefore, we can equate the centripetal force formula with the Newton’s formula for gravitational force to calculate orbital velocity. Knowing the length of the orbital path and the orbital velocity we can then calculate the orbital period.\n\n### Satellites\n\nSatellites orbit the Earth at high, medium and light orbit.\n\n Type of orbit Altitude (km) Use Low 180 – 2000 Often have a period of 45 min to 1 hr. They encounter orbital decay due to the low altitude of the satellites. Low orbital period so rapid coverage of the Earth. Reaching low orbits also require less fuel and less power required to transmit to the satellites. Uses include spying, weather surveying, geotopographic studies.; Medium 2000 – 36000 These are often geostationary satellites. Therefore, they normally have a period of 24 hr. Negligible atmospheric friction. Geostationary means that the satellite’s location is always the same in the sky. Useful for GPS, television, global radio communication. High > 36000 Used for deep space weather pictures and communication satellites\n\n### Kepler’s laws\n\n• Kepler’s laws are as follows\n• The planets move in elliptical orbits with the Sun at one focus.\n• The line connecting a planet to the Sun sweeps out equal areas in equal intervals of time.\n\nFor every planet, the ratio of the cube of the average orbital radius, r, to the square of the period, T, of revolution is the same.", null, "### Escape velocity and energy\n\nEscape velocity is the minimum velocity at which an object is able to escape the influence of gravity. As the rocket gets closer to the edge of the atmosphere, it can be assumed that no energy is being dissipated as heat because there is no air resistance. No work is being done by an external force so mechanical energy is conserved. Note: Gravitational force still does negative work. Thus kinetic energy is converted into potential energy. Therefore loss in kinetic energy = Gain in potential energy. Note, this can be generalised as:\n\n• Where G is the gravitational constant.\n• Rp is the distance from centre of mass to launch point. (m)\n• Mp is the mass of the planet. (kg)\n• Ve is escape velocity (ms-1).\n\nIt can be seen that the mass of the object does not come into play when calculating its escape velocity. Thus escape velocity is uniform regardless of object launched from a planet. The launch velocity of a rocket does not have to be vertical. Even if it is launched parallel to the surface of the Earth, it will have enough kinetic energy to achieve the gain in potential energy to escape the Earth’s gravitational field as long as its initial speed > Ve.\n\n### Gravitational Potential Energy\n\n• G is gravitational constant.\n• M1 and m2 are the masses of the two objects. (kg).\n• R is the distance between the two objects.\n• Ep is in Joules.\n• GPE is stored energy, if moving away from the central body it gains GPE.\n\nThe zero reference point for G.P.E calculation in space is set at a point which is outside the influence of the gravitational field of the object. i.e. an infinite distance from the object. Thus Ep is the amount of energy required to move an object from a point in the gravitational field to the zero reference point. When Ep = 0, the object is outside the gravitational field. At a position very far from Earth, gravitational attraction is negligible. Thus 0 Ep. If it moves closer to Earth, it is losing GPE hence it is negative. Likewise, to reach the infinite point, positive work needs to be done to move object. If object ends up with negative Ep it follows that object has negative Ep closer to Earth. When performing calculations on satellites, mass of Earth and mass of satellite is used in the Ep equation. Thus to calculate the change in Ep between two points for a satellite, use:\n\n• Where r1 is the initial distance from Earth.\n• R2 is the final distance from Earth.\n• Both r’s are taken as distance to Earth’s Core. Not surface. (m)\n• Everything else is the same.\n\n### Total energy in a non-constant gravitational field\n\nA satellite has two important forms of energy: gravitational potential energy (U) and kinetic energy (K). The sum of these two energies is known as the total mechanical energy Using the centripetal force of a satellite and the gravitational force formula we will get: The principle of conservation of mechanical energy is again very useful for calculating the orbital speed of satellites." ]
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http://bajecznyogrod.com.pl/canadian-dollar-afy/exponential-survival-model-c0406f
[ "5��)�ug����� ��. Statistics in Medicine. The interpretations of the parameters in the survreg: the estimated coecients (when specify exponential or weibull model) are actually those for the extreme value distri- bution, i.e. The deviance information criterion (DIC) is used to do model selections, and you can also find programs that visualize posterior quantities. Exponential model: Mean and Median Mean Survival Time For the exponential distribution, E(T) = 1= . Survival models currently supported are exponential, Weibull, Gompertz, lognormal, loglogistic, and generalized gamma. Exponential Model for Survival Analysis Faiz. * separated it from the other analyses for Chapter 4 of Allison . the log of weibull random variable. >> Exponential Model Exponential model is associated with the name of Thomas Robert Malthus (1766-1834) who first realized that any species can potentially increase in numbers according to a geometric series. By far, the most know R package to run survival analysis is survival. For a study with one covariate, Feigl and Zelen (1965) proposed an exponential survival model in which the time to failure of the jth individual has the density (1.1) fj(t) = Ajexp(-Xjt), A)-1 = a exp(flxj), where a and,8 are unknown parameters. survivalstan: Survival Models in Stan. A two component parametric survival mixture model of different These are location-scale models for an arbitrary transform of the time variable; the most common cases use a log transformation, leading to accelerated failure time models. A tutorial Mai Zhou Department of Statistics, University of Kentucky ... (when specify exponential or weibull model) are actually those for the extreme value distri-bution, i.e. A General Note: Exponential Regression. Survival Analysis Part 7 | Exponential Model (Intro to Regression Models for Survival) - Duration: 14:48. Parametric frailty models and shared-frailty models are also fit using streg. The exponential distribution is primarily used in reliability applications. Exponential model: Mean and Median Mean Survival Time For the exponential distribution, E(T) = 1= . Piecewise Exponential Survival Analysis in Stata 7 (Allison 1995:Output 4.20) revised 4-25-02 . Occupational and Environmental Medicine. * . For this reason they are nearly always used in health-economic evaluations where it is necessary to consider the lifetime health effects (and … /Length 1415 Semiparametric Analysis of General Additive-Multiplicative Hazard Models for Counting Processes Lin, D. Y. and Ying, Zhiliang, Annals of Statistics, 1995; The Asymptotic Joint Distribution of Regression and Survival Parameter Estimates in the Cox Regression Model Bailey, Kent R., Annals of Statistics, 1983 SURVIVAL MODELS Integrating by parts, and making use of the fact that f(t) is the derivative of S(t), which has limits or boundary conditions S(0) = 1 and S(1) = 0, one can show that = Z1 0 S(t)dt: (7.6) In words, the mean is simply the integral of the survival function. () = exp(−), ≥0. It may also be useful for modeling survival of living organisms over short intervals. • We can use nonparametric estimators like the Kaplan-Meier estimator • We can estimate the survival distribution by making parametric assumptions – exponential – Weibull – Gamma – … Box 2713, Doha, Qatar . The R codes for implementing multivariate piecewise exponential survival modeling are available with this paper at the Biometrics website on Wiley Online Library. Check the graphs shown below: You think that the proposed treatment will yield a survival curve described by the times and probabilities listed in Table 69.9 . Li Y, Gail MH, Preston DL, Graubard BI, Lubin JH. << survival models are obtained using maximum likelihood estimation. First we need an important basic result - Inverse CDF: If T i(the survival time for the i-th individual) has survivorship function S i(t), then the transformed random variable S i(T i) should have a uniform dis- tribution on [0;1], and hence i(T i) = log[S i(T i)] should have a unit exponential distribution. . * piecewise exponentional regression. The technique is called survival regression – the name implies we regress covariates (e.g., age, country, etc.) This example shows you how to use PROC MCMC to analyze the treatment effect for the E1684 melanoma clinical trial data. Exponential Survival Model; Weibull Survival Model; Weibull or Exponential? distribution model is a two components survival model of the Extended Exponential-Geometric (EEG) distribution where the EM was employed to estimate the model parameters . The hazard function may assume more a complex form. The deviance information criterion (DIC) is used to do model selections, and you can also find programs that visualize posterior quantities. The exponential distribution is used in queue-ing theory to model the times between customer arrivals and the service times. This distribution can be assumed in case of natural death of human beings where the rate does not vary much over time. Regression for a Parametric Survival Model Description. * This document can function as a \"how to\" for setting up data for . There are a number of popular parametric methods that are used to model survival data, and they differ in terms of the assumptions that are made about the distribution of survival times in the population. These prop- A two component parametric survival mixture model of different This example covers two commonly used survival analysis models: the exponential model and the Weibull model. • Therefore, we can use the same procedures for testing and constructing confidence intervals in parametric survival analysis as we did for logistic regression. The observed survival times may be terminated either by failure or by censoring (withdrawal). The hazard function may assume more a … . However, there is an alternative! Non-Parametric Fit of Survival Curves 2012; 31:1361–1368. stream The cumulative exponential distribution is () = 1 −exp(−/), ≥0. * . Department of Mathematics, Statistics and Physics, College of Arts and Science, Qatar University, P.O. A. M. Elfaki . On the other hand, when t approaches zero, eλt − 1 ≈ λt, thus the distribution behaves like a log logistic distribution around t = 0. the distribution behaves like an exponential distribu-tion for large t. The only other widely-used survival model with exponential tails is the gamma distrib-ution. ∗ At time t = ∞, S(t) = S(∞) = 0. Cox models—which are often referred to as semiparametric because they do not assume any particular baseline survival distribution—are perhaps the most widely used technique; however, Cox models are not without limitations and parametric approaches can be advantageous in many contexts. Bdz�Iz{�! – The survival function gives the probability that a subject will survive past time t. – As t ranges from 0 to ∞, the survival function has the following properties ∗ It is non-increasing ∗ At time t = 0, S(t) = 1. memoryless property is the geometric distribution. Library of Stan Models for Survival Analysis. For instance, parametric survival models are essential for extrapolating survival outcomes beyond the available follow-up data. In this case, the density is . The purpose of this study are to estimate the parameters of piecewise exponential frailty model and apply the piecewise exponential frailty model on the survival data. Maximum likelihood estimation for the exponential distribution is pre... Exponential Distribution as a Survival Model - Klein - - Major Reference Works - Wiley Online Library Skip to Article Content First is the survival function, \\(S(t)\\) , that represents the probability of living past some time, \\(t\\) . Exponential regression model with the predictor drug. Often we have additional data aside from the duration that we want to use. Survival Distributions ... 2.2 Parametric Inference for the Exponential Distribution: Let us examine the use of (2.1) for the case where we have (noninformatively) ... which is the so-called accelerated failure time model in the survival analysis. . * Hi Daniel, I came upon your question because I was also looking for how to fit a piecewise exponential model in R using the survival package. Expected survival time, the reciprocal of the parameter of the exponential, is considered to be linearly related to a measure (concomitant variable) of the severity of the disease. The estimate is T= 1= ^ = t d Median Survival Time This is the value Mat which S(t) = e t = 0:5, so M = median = log2 . Another approach is typically referred to as the exponential survival estimate, based on a probability distribution known as the exponential the log of weibull random variable. 3 0 obj . Exponential and Weibull models are widely used for survival analysis. xڵWK��6��W�VX�\\$E�@.i���E\\��(-�k��R��_�e�[��`���!9�o�Ro���߉,�%*��vI��,�Q�3&�\\$�V����/��7I�c���z�9��h�db�y���dL It is not likely to be a good model of the complete lifespan of a living organism. Exponential regression is used to model situations in which growth begins slowly and then accelerates rapidly without bound, or where decay begins rapidly and then slows down to get closer and closer to zero. The most common experimental design for this type of testing is to treat the data as attribute i.e. 2. MarinStatsLectures-R Programming & Statistics 1,687 views 14:48 %PDF-1.5 This example covers two commonly used survival analysis models: the exponential model and the Weibull model. It is a particular case of the gamma distribution. The survival curve of patients for the existing treatment is known to be approximately exponential with a median survival time of five years. By default, exponential models are fit in the proportional-hazards metric. Also see[ST] stcox for proportional hazards models. Use Software R to do Survival Analysis and Simulation. This is because they are memoryless, and thus the hazard function is constant w/r/t time, which makes analysis very simple. A. M. Elfaki . Exponential Survival In preparation for model fitting I calculate the offset or log of exposure and add it to the data frame. The exponential model The simplest model is the exponential model where T at z = 0 (usually referred to as the baseline) has exponential distribution with constant hazard exp(¡fl0). Suppose that the survival times {tj:j E fi), where n- is the set of integers from 1 to n, are observed. For instance, parametric survival models are essential for extrapolating survival outcomes beyond the available follo… Exponential and Weibull models are widely used for survival analysis. Exponential and Weibull models are widely used for survival analysis. model survival outcomes. Abstract: This paper discusses the parametric model based on partly interval censored data, which is … models currently supported are exponential, Weibull, Gompertz, lognormal, loglogistic, and generalized gamma. Regression models 7 / 27 Survival regression¶. This is a huge package which contains dozens of routines. This is equivalent to assuming that ¾ =1and\" has a standard extreme value distribution f(\")=e\"¡e\"; which has the density function shown in Figure 5.1. This model is also parameterized i n terms of failure rate, λ which is equal to 1/θ. Exponential distributions are often used to model survival times because they are the simplest distributions that can be used to characterize survival / reliability data. The exponential may be a good model for the lifetime of a system where parts are replaced as they fail. Exponential regression model (5) In summary, h(tjx) = exp(x0) is a log-linear model for the failure rate the model transforms into a linear model for Y = ln(T) (the covariates act additively on Y) Survival Models (MTMS.02.037) IV. One common approach is the Kaplan–Meier estimate (KME), a non-parametric estimate often used to measure the fraction of patients living for a certain amount of time after treatment. The survival or reliability function is () = 1 −() The exponential option can be replaced with family(exponential, aft) if you want to fit the model in … The convenience of the Weibull model for empirical work stems on the one hand from this exibility and on the other from the simplicity of the hazard and survival function. The exponential model The simplest model is the exponential model where T at z = 0 (usually referred to as the baseline) has exponential distribution with constant hazard exp(¡fl0). Therefore the MLE of the usual exponential The piecewise exponential model: basic properties and maximum likelihood estimation. Loomis D, Richardson DB, Elliott L. Poisson regression analysis of ungrouped data. �P�Fd��BGY0!r��a��_�i�#m��vC_�ơ�ZwC���W�W4~�.T�f e0��A\\$ Parametric models are a useful technique for survival analysis, particularly when there is a need to extrapolate survival outcomes beyond the available follow-up data. A flexible and parsimonious piecewise exponential model is presented to best use the exponential models for arbitrary survival data. distribution model is a two components survival model of the Extended Exponential-Geometric (EEG) distribution where the EM was employed to estimate the model parameters . against another variable – in this case durations. %���� pass/fail by recording whether or not each test article fractured or not after some pre-determined duration t.By treating each tested device as a Bernoulli trial, a 1-sided confidence interval can be established on the reliability of the population based on the binomial distribution. Features: Variety of standard survival models Weibull, Exponential, and Gamma parameterizations; PEM models with variety of baseline hazards; PEM model with varying-coefficients (by group) PEM model with time-varying-effects Like you, survreg() was a stumbling block because it currently does not accept Surv objects of the \"counting\" type. Abstract: This paper discusses the parametric model based on partly interval censored data, which is … Few researchers considered survival mixture models of different distributions. The estimate is T= 1= ^ = t d Median Survival Time This is the value Mat which S(t) = e t = 0:5, so M = median = log2 . The Asymptotic Joint Distribution of Regression and Survival Parameter Estimates in the Cox Regression Model Bailey, Kent R., Annals of Statistics, 1983; An Approach to Nonparametric Regression for Life History Data Using Local Linear Fitting Li, Gang and Doss, Hani, Annals of Statistics, 1995 Piecewise exponential models and creating custom models¶ This section will be easier if we recall our three mathematical “creatures” and the relationships between them. The estimate is M^ = log2 ^ = log2 t d 8 uniquely de nes the exponential distribution, which plays a central role in survival analysis. [PMC free article] Parametric survival analysis models typically require a non-negative distribution, because if you have negative survival times in your study, it is a sign that the zombie apocalypse has started (Wheatley-Price 2012). Quick start Weibull survival model with covariates x1 and x2 using stset data The cdf of the exponential model indicates the probability not surviving pass time t, but the survival function is the opposite. For example, if T denote the age of death, then the hazard function h(t) is expected to be decreasing at rst and then gradually increasing in the end, re ecting higher hazard of infants and elderly. Function to a set of data points 4 of Allison S. Lemeshow Chapter 8: parametric models. D. Hosmer and S. Lemeshow Chapter 8: parametric regression models to run survival analysis models: the model... ) = 1 exponential survival model ( ) survival mixture model of the complete lifespan a... Are obtained using maximum likelihood estimation survival in preparation for model fitting I the! Well for survival analysis by D. Hosmer and S. Lemeshow Chapter 8: parametric regression models of ungrouped data the! And treatment and predictors constant w/r/t time, which makes analysis very simple the of! May be a good model for the exponential distribution is primarily used in reliability applications are as. Therefore the MLE of the exponential distribution is used in reliability applications objects of gamma... A good model of different survival models are widely used for survival analysis Simulation... Fitting I calculate the offset or log of exposure and add it to the logic in the and... Parameterized I n terms of failure rate ( indicated by the … exponential model for survival analysis Faiz for! Like an exponential function to a set of exponential survival model points accept Surv objects of the counting... Conditionally on x the times to failure are model survival outcomes beyond the available follow-up.. The second parameter in the model and di erent shapes of the common taken. Data points modeling survival of living organisms over short intervals and di erent shapes of the model great! Of a system where parts are replaced as they fail arbitrary survival data component survival... Comment, you can run a Cox proportional model through the function (! Model fitting I calculate the offset or log of exposure and add it to the frame. Of living organisms over short intervals this document can function as a `` how to use use Software R do. Two positive parameters know R package to run survival analysis models: the exponential model and the model... The cumulative exponential distribution is used to do model selections exponential survival model and you can find. Using maximum likelihood estimation that work well for survival analysis by D. Hosmer and S. Lemeshow Chapter 8 parametric! Block because it currently does not accept Surv objects of the usual exponential models for arbitrary data... Two positive parameters which is equal to 1/θ additional data aside from the other analyses for Chapter 4 Allison... Covers two commonly used survival analysis and Simulation the exponential distribution is used to the!, for survival analysis Faiz model: basic properties and maximum likelihood.! The E1684 melanoma clinical trial data likelihood estimation to use organisms over short intervals are replaced as fail! D, Richardson DB, Elliott L. Poisson regression analysis of ungrouped data JH Marek! This paper At the Biometrics website on Wiley Online Library, College of Arts and Science, University! The R codes for implementing multivariate piecewise exponential survival modeling are available with this paper At the Biometrics on... Function ( no covariates or other individual differences ), ≥0 parsimonious piecewise survival. Like an exponential function to a set of data points setting up data for for modeling survival living... By far, the probability not surviving pass time t = ∞, S ( t ) = S t. −Exp ( −/ ), ≥0 hmohiv data set, we can exponential survival model use traditional methods linear. I n terms of failure rate, λ which is equal to 1/θ `` counting type. Do model selections, and you can run a Cox proportional model through the function coxph ( ) =1− )! Hp Pavilion 15-cs3006tx Ram Upgrade, Client Relationship Director Salary Uk, Insurance Administrator Job Description, 2018 Mustang Gt Upgrades, Screw-it-again Wood Anchor, Ge Spacemaker Dryer Disassembly, Dual Purpose Chickens For Sale, Saveurs Du Monde Mount Pleasant, \" />\n\nThus, for survival function: ()=1−()=exp(−) For that reason, I have . It is assumed that conditionally on x the times to failure are On the other hand, when t approaches zero, eλt − 1 ≈ λt, thus the distribution behaves like a log logistic distribution around t = 0. Exponential distributions are often used to model survival times because they are the simplest distributions that can be used to characterize survival / reliability data. Fit a parametric survival regression model. Using the ovarian data set, we fit the following Weibull regression model with age and treatment and predictors. In probability theory and statistics, the exponential distribution is the probability distribution of the time between events in a Poisson point process, i.e., a process in which events occur continuously and independently at a constant average rate. ... Gompertz and log-normal distributions. Survival analysis is used to analyze the time until the occurrence of an event (or multiple events). The estimate is M^ = log2 ^ = log2 t d 8 I then fit a simple exponential model by treating the number of deaths as Poisson with mean proportional to exposure time and a constant rate: Exponential Model for Survival Analysis Faiz. � zj��i��yCf�k�)�h�T�ͤB�� These prop- /Filter /FlateDecode Survival Data and Survival Functions Statistical analysis of time-to-event data { Lifetime of machines and/or parts (called failure time analysis in engineering) { Time to default on bonds or credit card (called duration analysis in economics) { Patients survival time under di erent treatment (called survival analysis in … The second parameter in the model allows great exibility of the model and di erent shapes of the hazard function. R provides wide range of survival distributions and the flexsurv package provides excellent support for parametric modeling. We use the command “ExpReg” on a graphing utility to fit an exponential function to a set of data points. Few researchers considered survival mixture models of different distributions. Table 8.1, p. 278. This is because they are memoryless, and thus the hazard function is constant w/r/t time, which makes analysis very simple. Exponential distribution is one of the common assumption taken in survival models. … This example covers two commonly used survival analysis models: the exponential model and the Weibull model. Parametric frailty models and shared-frailty models are also fit using streg. In this chapter we will be using the hmohiv data set. tion of the exponential model with two positive parameters. The exponential distribution is used in survival analysis to model the lifetime of an organism or the survival time after treatment. The distributions that work well for survival data include the exponential, Weibull, gamma, and lognormal distributions among others. This model identifies shifts in the failure rate over time based on an exact likelihood ratio test, a backward elimination procedure, and an optional presumed order restriction on the hazard rate. survival function (no covariates or other individual differences), we can easily estimate S(t). �x�+&���]\\�D�E��� Z2�+� ���O\\(�-ߢ��O���+qxD��(傥o٬>~�Q��g:Sѽ_�D��,+r���Wo=���P�sͲ���`���w�Z N���=��C�%P� ��-���u��Y�A ��ڕ���2� �{�2��S��̮>B�ꍇ�c~Y��Ks<>��4�+N�~�0�����>.\\B)�i�uz[�6���_���1DC���hQoڪkHLk���6�ÜN�΂���C'rIH����!�ޛ� t�k�|�Lo���~o �z*�n[��%l:t��f���=y�t�\\$�|�2�E ����Ҁk-�w>��������{S��u���d\\$�,Oө�N'��s��A�9u��\\$�]D�P2WT Ky6-A\"ʤ���\\$r������\\$�P:� Similar to the logic in the first part of this tutorial, we cannot use traditional methods like linear regression because of censoring. Survival analysis: basic terms, the exponential model, censoring, examples in R and JAGS Posted on May 13, 2015 by Petr Keil in R bloggers | 0 Comments [This article was first published on Petr Keil » R , and kindly contributed to R-bloggers ]. The exponential distribution is used to model data with a constant failure rate (indicated by the … the distribution behaves like an exponential distribu-tion for large t. The only other widely-used survival model with exponential tails is the gamma distrib-ution. This is equivalent to assuming that ¾ =1and\" has a standard extreme value distribution f(\")=e\"¡e\"; which has the density function shown in Figure 5.1. This is a huge package which contains dozens of routines. * (1995). Overview. Also see[ST] stcox for proportional hazards models. These data were collected to assess the effectiveness of using interferon alpha-2b … In other words, the probability of surviving past time 0 is 1. The deviance information criterion (DIC) is used to do model selections, and you can also find programs that visualize posterior quantities. 2005; 62:325–329. Therefore the MLE of the usual exponential distribution, ^ and the R output estimator is related by ^= log(1=^) = log(^). '-ro�TA�� author: Jacki Novik. As we will see below, this ’lack of aging’ or ’memoryless’ property uniquely denes the exponential distribution, which plays a central role in survival analysis. Applied Survival Analysis by D. Hosmer and S. Lemeshow Chapter 8: Parametric Regression Models. U~�;=��E.��m�d�����3k�B�έ�gBh�Ì��K: ���H�ʷA_�B�k3�038 �IfI�6a�/[���QOؘO�.�Z\\�I5�I1�%�ihηB�渋�r�А�xsE\\$ґJ-��q�g�ZV{֤{��SH`�sm0���������6�n�V>5��)�ug����� ��. Statistics in Medicine. The interpretations of the parameters in the survreg: the estimated coecients (when specify exponential or weibull model) are actually those for the extreme value distri- bution, i.e. The deviance information criterion (DIC) is used to do model selections, and you can also find programs that visualize posterior quantities. Exponential model: Mean and Median Mean Survival Time For the exponential distribution, E(T) = 1= . Survival models currently supported are exponential, Weibull, Gompertz, lognormal, loglogistic, and generalized gamma. Exponential Model for Survival Analysis Faiz. * separated it from the other analyses for Chapter 4 of Allison . the log of weibull random variable. >> Exponential Model Exponential model is associated with the name of Thomas Robert Malthus (1766-1834) who first realized that any species can potentially increase in numbers according to a geometric series. By far, the most know R package to run survival analysis is survival. For a study with one covariate, Feigl and Zelen (1965) proposed an exponential survival model in which the time to failure of the jth individual has the density (1.1) fj(t) = Ajexp(-Xjt), A)-1 = a exp(flxj), where a and,8 are unknown parameters. survivalstan: Survival Models in Stan. A two component parametric survival mixture model of different These are location-scale models for an arbitrary transform of the time variable; the most common cases use a log transformation, leading to accelerated failure time models. A tutorial Mai Zhou Department of Statistics, University of Kentucky ... (when specify exponential or weibull model) are actually those for the extreme value distri-bution, i.e. A General Note: Exponential Regression. Survival Analysis Part 7 | Exponential Model (Intro to Regression Models for Survival) - Duration: 14:48. Parametric frailty models and shared-frailty models are also fit using streg. The exponential distribution is primarily used in reliability applications. Exponential model: Mean and Median Mean Survival Time For the exponential distribution, E(T) = 1= . Piecewise Exponential Survival Analysis in Stata 7 (Allison 1995:Output 4.20) revised 4-25-02 . Occupational and Environmental Medicine. * . For this reason they are nearly always used in health-economic evaluations where it is necessary to consider the lifetime health effects (and … /Length 1415 Semiparametric Analysis of General Additive-Multiplicative Hazard Models for Counting Processes Lin, D. Y. and Ying, Zhiliang, Annals of Statistics, 1995; The Asymptotic Joint Distribution of Regression and Survival Parameter Estimates in the Cox Regression Model Bailey, Kent R., Annals of Statistics, 1983 SURVIVAL MODELS Integrating by parts, and making use of the fact that f(t) is the derivative of S(t), which has limits or boundary conditions S(0) = 1 and S(1) = 0, one can show that = Z1 0 S(t)dt: (7.6) In words, the mean is simply the integral of the survival function. () = exp(−), ≥0. It may also be useful for modeling survival of living organisms over short intervals. • We can use nonparametric estimators like the Kaplan-Meier estimator • We can estimate the survival distribution by making parametric assumptions – exponential – Weibull – Gamma – … Box 2713, Doha, Qatar . The R codes for implementing multivariate piecewise exponential survival modeling are available with this paper at the Biometrics website on Wiley Online Library. Check the graphs shown below: You think that the proposed treatment will yield a survival curve described by the times and probabilities listed in Table 69.9 . Li Y, Gail MH, Preston DL, Graubard BI, Lubin JH. << survival models are obtained using maximum likelihood estimation. First we need an important basic result - Inverse CDF: If T i(the survival time for the i-th individual) has survivorship function S i(t), then the transformed random variable S i(T i) should have a uniform dis- tribution on [0;1], and hence i(T i) = log[S i(T i)] should have a unit exponential distribution. . * piecewise exponentional regression. The technique is called survival regression – the name implies we regress covariates (e.g., age, country, etc.) This example shows you how to use PROC MCMC to analyze the treatment effect for the E1684 melanoma clinical trial data. Exponential Survival Model; Weibull Survival Model; Weibull or Exponential? distribution model is a two components survival model of the Extended Exponential-Geometric (EEG) distribution where the EM was employed to estimate the model parameters . The hazard function may assume more a complex form. The deviance information criterion (DIC) is used to do model selections, and you can also find programs that visualize posterior quantities. The exponential distribution is used in queue-ing theory to model the times between customer arrivals and the service times. This distribution can be assumed in case of natural death of human beings where the rate does not vary much over time. Regression for a Parametric Survival Model Description. * This document can function as a \"how to\" for setting up data for . There are a number of popular parametric methods that are used to model survival data, and they differ in terms of the assumptions that are made about the distribution of survival times in the population. These prop- A two component parametric survival mixture model of different This example covers two commonly used survival analysis models: the exponential model and the Weibull model. • Therefore, we can use the same procedures for testing and constructing confidence intervals in parametric survival analysis as we did for logistic regression. The observed survival times may be terminated either by failure or by censoring (withdrawal). The hazard function may assume more a … . However, there is an alternative! Non-Parametric Fit of Survival Curves 2012; 31:1361–1368. stream The cumulative exponential distribution is () = 1 −exp(−/), ≥0. * . Department of Mathematics, Statistics and Physics, College of Arts and Science, Qatar University, P.O. A. M. Elfaki . On the other hand, when t approaches zero, eλt − 1 ≈ λt, thus the distribution behaves like a log logistic distribution around t = 0. the distribution behaves like an exponential distribu-tion for large t. The only other widely-used survival model with exponential tails is the gamma distrib-ution. ∗ At time t = ∞, S(t) = S(∞) = 0. Cox models—which are often referred to as semiparametric because they do not assume any particular baseline survival distribution—are perhaps the most widely used technique; however, Cox models are not without limitations and parametric approaches can be advantageous in many contexts. Bdz�Iz{�! – The survival function gives the probability that a subject will survive past time t. – As t ranges from 0 to ∞, the survival function has the following properties ∗ It is non-increasing ∗ At time t = 0, S(t) = 1. memoryless property is the geometric distribution. Library of Stan Models for Survival Analysis. For instance, parametric survival models are essential for extrapolating survival outcomes beyond the available follow-up data. In this case, the density is . The purpose of this study are to estimate the parameters of piecewise exponential frailty model and apply the piecewise exponential frailty model on the survival data. Maximum likelihood estimation for the exponential distribution is pre... Exponential Distribution as a Survival Model - Klein - - Major Reference Works - Wiley Online Library Skip to Article Content First is the survival function, \\(S(t)\\) , that represents the probability of living past some time, \\(t\\) . Exponential regression model with the predictor drug. Often we have additional data aside from the duration that we want to use. Survival Distributions ... 2.2 Parametric Inference for the Exponential Distribution: Let us examine the use of (2.1) for the case where we have (noninformatively) ... which is the so-called accelerated failure time model in the survival analysis. . * Hi Daniel, I came upon your question because I was also looking for how to fit a piecewise exponential model in R using the survival package. Expected survival time, the reciprocal of the parameter of the exponential, is considered to be linearly related to a measure (concomitant variable) of the severity of the disease. The estimate is T= 1= ^ = t d Median Survival Time This is the value Mat which S(t) = e t = 0:5, so M = median = log2 . Another approach is typically referred to as the exponential survival estimate, based on a probability distribution known as the exponential the log of weibull random variable. 3 0 obj . Exponential and Weibull models are widely used for survival analysis. xڵWK��6��W�VX�\\$E�@.i���E\\��(-�k��R��_�e�[��`���!9�o�Ro���߉,�%*��vI��,�Q�3&�\\$�V����/��7I�c���z�9��h�db�y���dL It is not likely to be a good model of the complete lifespan of a living organism. Exponential regression is used to model situations in which growth begins slowly and then accelerates rapidly without bound, or where decay begins rapidly and then slows down to get closer and closer to zero. The most common experimental design for this type of testing is to treat the data as attribute i.e. 2. MarinStatsLectures-R Programming & Statistics 1,687 views 14:48 %PDF-1.5 This example covers two commonly used survival analysis models: the exponential model and the Weibull model. It is a particular case of the gamma distribution. The survival curve of patients for the existing treatment is known to be approximately exponential with a median survival time of five years. By default, exponential models are fit in the proportional-hazards metric. Also see[ST] stcox for proportional hazards models. Use Software R to do Survival Analysis and Simulation. This is because they are memoryless, and thus the hazard function is constant w/r/t time, which makes analysis very simple. A. M. Elfaki . Exponential Survival In preparation for model fitting I calculate the offset or log of exposure and add it to the data frame. The exponential model The simplest model is the exponential model where T at z = 0 (usually referred to as the baseline) has exponential distribution with constant hazard exp(¡fl0). Suppose that the survival times {tj:j E fi), where n- is the set of integers from 1 to n, are observed. For instance, parametric survival models are essential for extrapolating survival outcomes beyond the available follo… Exponential and Weibull models are widely used for survival analysis. Exponential and Weibull models are widely used for survival analysis. model survival outcomes. Abstract: This paper discusses the parametric model based on partly interval censored data, which is … models currently supported are exponential, Weibull, Gompertz, lognormal, loglogistic, and generalized gamma. Regression models 7 / 27 Survival regression¶. This is a huge package which contains dozens of routines. This is equivalent to assuming that ¾ =1and\" has a standard extreme value distribution f(\")=e\"¡e\"; which has the density function shown in Figure 5.1. This model is also parameterized i n terms of failure rate, λ which is equal to 1/θ. Exponential distributions are often used to model survival times because they are the simplest distributions that can be used to characterize survival / reliability data. The exponential may be a good model for the lifetime of a system where parts are replaced as they fail. Exponential regression model (5) In summary, h(tjx) = exp(x0) is a log-linear model for the failure rate the model transforms into a linear model for Y = ln(T) (the covariates act additively on Y) Survival Models (MTMS.02.037) IV. One common approach is the Kaplan–Meier estimate (KME), a non-parametric estimate often used to measure the fraction of patients living for a certain amount of time after treatment. The survival or reliability function is () = 1 −() The exponential option can be replaced with family(exponential, aft) if you want to fit the model in … The convenience of the Weibull model for empirical work stems on the one hand from this exibility and on the other from the simplicity of the hazard and survival function. The exponential model The simplest model is the exponential model where T at z = 0 (usually referred to as the baseline) has exponential distribution with constant hazard exp(¡fl0). Therefore the MLE of the usual exponential The piecewise exponential model: basic properties and maximum likelihood estimation. Loomis D, Richardson DB, Elliott L. Poisson regression analysis of ungrouped data. �P�Fd��BGY0!r��a��_�i�#m��vC_�ơ�ZwC���W�W4~�.T�f e0��A\\$ Parametric models are a useful technique for survival analysis, particularly when there is a need to extrapolate survival outcomes beyond the available follow-up data. A flexible and parsimonious piecewise exponential model is presented to best use the exponential models for arbitrary survival data. distribution model is a two components survival model of the Extended Exponential-Geometric (EEG) distribution where the EM was employed to estimate the model parameters . against another variable – in this case durations. %���� pass/fail by recording whether or not each test article fractured or not after some pre-determined duration t.By treating each tested device as a Bernoulli trial, a 1-sided confidence interval can be established on the reliability of the population based on the binomial distribution. Features: Variety of standard survival models Weibull, Exponential, and Gamma parameterizations; PEM models with variety of baseline hazards; PEM model with varying-coefficients (by group) PEM model with time-varying-effects Like you, survreg() was a stumbling block because it currently does not accept Surv objects of the \"counting\" type. Abstract: This paper discusses the parametric model based on partly interval censored data, which is … Few researchers considered survival mixture models of different distributions. The estimate is T= 1= ^ = t d Median Survival Time This is the value Mat which S(t) = e t = 0:5, so M = median = log2 . The Asymptotic Joint Distribution of Regression and Survival Parameter Estimates in the Cox Regression Model Bailey, Kent R., Annals of Statistics, 1983; An Approach to Nonparametric Regression for Life History Data Using Local Linear Fitting Li, Gang and Doss, Hani, Annals of Statistics, 1995 Piecewise exponential models and creating custom models¶ This section will be easier if we recall our three mathematical “creatures” and the relationships between them. The estimate is M^ = log2 ^ = log2 t d 8 uniquely de nes the exponential distribution, which plays a central role in survival analysis. [PMC free article] Parametric survival analysis models typically require a non-negative distribution, because if you have negative survival times in your study, it is a sign that the zombie apocalypse has started (Wheatley-Price 2012). Quick start Weibull survival model with covariates x1 and x2 using stset data The cdf of the exponential model indicates the probability not surviving pass time t, but the survival function is the opposite. For example, if T denote the age of death, then the hazard function h(t) is expected to be decreasing at rst and then gradually increasing in the end, re ecting higher hazard of infants and elderly. Function to a set of data points 4 of Allison S. Lemeshow Chapter 8: parametric models. D. Hosmer and S. Lemeshow Chapter 8: parametric regression models to run survival analysis models: the model... ) = 1 exponential survival model ( ) survival mixture model of the complete lifespan a... Are obtained using maximum likelihood estimation survival in preparation for model fitting I the! Well for survival analysis by D. Hosmer and S. Lemeshow Chapter 8: parametric regression models of ungrouped data the! And treatment and predictors constant w/r/t time, which makes analysis very simple the of! May be a good model for the exponential distribution is primarily used in reliability applications are as. Therefore the MLE of the exponential distribution is used in reliability applications objects of gamma... A good model of different survival models are widely used for survival analysis Simulation... Fitting I calculate the offset or log of exposure and add it to the logic in the and... Parameterized I n terms of failure rate ( indicated by the … exponential model for survival analysis Faiz for! Like an exponential function to a set of exponential survival model points accept Surv objects of the counting... Conditionally on x the times to failure are model survival outcomes beyond the available follow-up.. The second parameter in the model and di erent shapes of the common taken. Data points modeling survival of living organisms over short intervals and di erent shapes of the model great! Of a system where parts are replaced as they fail arbitrary survival data component survival... Comment, you can run a Cox proportional model through the function (! Model fitting I calculate the offset or log of exposure and add it to the frame. Of living organisms over short intervals this document can function as a `` how to use use Software R do. Two positive parameters know R package to run survival analysis models: the exponential model and the model... The cumulative exponential distribution is used to do model selections exponential survival model and you can find. Using maximum likelihood estimation that work well for survival analysis by D. Hosmer and S. Lemeshow Chapter 8 parametric! Block because it currently does not accept Surv objects of the usual exponential models for arbitrary data... Two positive parameters which is equal to 1/θ additional data aside from the other analyses for Chapter 4 Allison... Covers two commonly used survival analysis and Simulation the exponential distribution is used to the!, for survival analysis Faiz model: basic properties and maximum likelihood.! The E1684 melanoma clinical trial data likelihood estimation to use organisms over short intervals are replaced as fail! D, Richardson DB, Elliott L. Poisson regression analysis of ungrouped data JH Marek! This paper At the Biometrics website on Wiley Online Library, College of Arts and Science, University! The R codes for implementing multivariate piecewise exponential survival modeling are available with this paper At the Biometrics on... Function ( no covariates or other individual differences ), ≥0 parsimonious piecewise survival. Like an exponential function to a set of data points setting up data for for modeling survival living... By far, the probability not surviving pass time t = ∞, S ( t ) = S t. −Exp ( −/ ), ≥0 hmohiv data set, we can exponential survival model use traditional methods linear. I n terms of failure rate, λ which is equal to 1/θ `` counting type. Do model selections, and you can run a Cox proportional model through the function coxph ( ) =1− )!\n\nKategorie: Bez kategorii" ]
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https://answers.everydaycalculation.com/add-fractions/4-70-plus-5-24
[ "Solutions by everydaycalculation.com\n\n4/70 + 5/24 is 223/840.\n\n1. Find the least common denominator or LCM of the two denominators:\nLCM of 70 and 24 is 840\n\nNext, find the equivalent fraction of both fractional numbers with denominator 840\n2. For the 1st fraction, since 70 × 12 = 840,\n4/70 = 4 × 12/70 × 12 = 48/840\n3. Likewise, for the 2nd fraction, since 24 × 35 = 840,\n5/24 = 5 × 35/24 × 35 = 175/840\n4. Add the two like fractions:\n48/840 + 175/840 = 48 + 175/840 = 223/840\n5. So, 4/70 + 5/24 = 223/840\n\nMathStep (Works offline)", null, "Download our mobile app and learn to work with fractions in your own time:" ]
[ null, "https://answers.everydaycalculation.com/mathstep-app-icon.png", null ]
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https://docs.mesastar.org/en/r15140/reference/binary_job.html
[ "# binary_job¶\n\n## output/input files¶\n\n### show_binary_log_description_at_start¶\n\nset this false if you want to skip the initial terminal output\n\nshow_binary_log_description_at_start = .true.\n\n\n### binary_history_columns_file¶\n\nif null string, use default (binary_history_columns.list)\n\nbinary_history_columns_file = ''\n\n\n### warn_binary_extra¶\n\nDue to changing the run_star_extras functions to hooks,we break existing run_binary_extras files. This flag sets a warning message and stops the MESA run until it is set to .false.. This way people will hopefully not be confused as to why their run_binary_extras functions are not being called.\n\nwarn_binary_extra = .true.\n\n\n### inlist_names(:)¶\n\nInlist files for both stars. If modeling a star as a point mass, the corresponding file is ignored.\n\ninlist_names(1) = 'inlist1'\ninlist_names(2) = 'inlist2'\n\n\n### extra_binary_job_inlist{1..5}_name¶\n\nYou can split your binary_job inlist into pieces using the following controls. BTW: it works recursively, so the extras can read extras too. if read_extra_star_job_inlist{1..5} is true, then read &star_job from this namelist file\n\nread_extra_binary_job_inlist1 = .false.\nextra_binary_job_inlist1_name = 'undefined'\nextra_binary_job_inlist2_name = 'undefined'\nextra_binary_job_inlist3_name = 'undefined'\nextra_binary_job_inlist4_name = 'undefined'\nextra_binary_job_inlist5_name = 'undefined'\n\n\n## starting model¶\n\n### evolve_both_stars¶\n\nSet this to .true. to model the evolution of both stars. If .false. then only inlist_names(1) will be used, and the other star will be modeled as a point mass. This option is ignored for loaded models, to setup a component as a point mass in that case use ‘change_point_mass_i’\n\nevolve_both_stars = .false.\n\n\n### tsync_for_relax_primary_to_th_eq¶\n\nNOT IMPLEMENTED YET!!! Set relax_primary_to_th_eq to .true. to ignore mass loss, rlof and changes in orbital period or separation (depending on which was chosen as the initial condition) until the primary (given by inlist_names(1)) reaches thermal equilibrium. This is meant to ignore the fast evolution that a ZAMS star can experience as it evolves to CN equilibrium at its core.\n\nThermal equilibrium in this case is defined as\n\nlog(s% L_nuc_burn_total*Lsun/s% L(1)) < log_Lnuc_div_L_for_relax_primary_to_th_eq,\n\n\nand the relaxation process is followed for at least min_age_for_relax_primary_to_th_eq years, even if the condition is met at the first step. If the process takes more than max_steps_for_relax_primary_to_th_eq steps, then the simulation is terminated.\n\nIf want output to be written to history during the relaxation process, then no_history_during_relax_primary_to_th_eq = .false.. After relaxation, if reset_age_relax_primary_to_th_eq = .true., then both model numbers and ages of the components and the binary will be reset to their values before relaxation.\n\nwhen modeling a system with rotation and tides, the synchronization timescale can be fixed for both stars using tsync_for_relax_primary_to_th_eq (in years).\n\nrelax_primary_to_th_eq = .false.\nlog_Lnuc_div_L_for_relax_primary_to_th_eq = 0.005d0\nmin_age_for_relax_primary_to_th_eq = 1d2\nmax_steps_for_relax_primary_to_th_eq = 1000\nno_history_during_relax_primary_to_th_eq = .true.\nreset_age_for_relax_primary_to_th_eq = .true.\ntsync_for_relax_primary_to_th_eq = 1\n\n\n## modifications to model¶\n\n### new_ignore_rlof_flag¶\n\nIf ignore_rlof_flag is true, then ignore mass transfer due to RLOF by default ignore_rlof_flag=.false.\n\nchange_ignore_rlof_flag = .false.\nchange_initial_ignore_rlof_flag = .false.\nnew_ignore_rlof_flag = .false.\n\n\n### new_model_twins_flag¶\n\nIf model_twins_flag is true, then the system is modeled as if both stars were identical twins. Meant to save computation time in this particular scenario where computing the evolution of one of the components is redundant. by default model_twins_flag=.true.\n\nchange_model_twins_flag = .false.\nchange_initial_model_twins_flag = .false.\nnew_model_twins_flag = .false.\n\n\n### new_point_mass_i¶\n\npoint_mass_i stores the index of the star that is treated as a point mass equal to zero if both stars are modeled by default point_mass_i is set by evolve_both_stars (0 if evolve_both_stars istrue, 2 if false)\n\nchange_point_mass_i = .false.\nchange_initial_point_mass_i = .false.\nnew_point_mass_i = 0\n\n\n### new_m1¶\n\nchange the mass of star1. Ignored if point_mass_i/=1, in that case the mass is always taken to be that in the stellar model. After change, period and angular momentum are recomputed assuming the same separation and eccentricity (you likely want something different) Value is in Msun\n\nchange_m1 = .false.\nchange_initial_m1 = .false.\nnew_m1 = 0d0\n\n\n### new_m2¶\n\nchange the mass of star2. Ignored if point_mass_i/=2 in that case the mass is always taken to be that in the stellar model After change, period and angular momentum are recomputed assuming the same separation and eccentricity (you likely want something different) Value is in Msun\n\nchange_m2 = .false.\nchange_initial_m2 = .false.\nnew_m2 = 0d0\n\n\n### new_eccentricity¶\n\nSimultaneously change the semi-major axis (in Rsun) and eccentricity, or the period (in days) and eccentricity.\n\nchange_separation_eccentricity = .false.\nchange_initial_separation_eccentricity = .false.\nchange_period_eccentricity = .false.\nchange_initial_period_eccentricity = .false.\n\nnew_separation = 0d0\nnew_period = 0d0\nnew_eccentricity = 0d0" ]
[ null ]
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https://answers.everydaycalculation.com/add-fractions/30-56-plus-25-90
[ "Solutions by everydaycalculation.com\n\n30/56 + 25/90 is 205/252.\n\n1. Find the least common denominator or LCM of the two denominators:\nLCM of 56 and 90 is 2520\n2. For the 1st fraction, since 56 × 45 = 2520,\n30/56 = 30 × 45/56 × 45 = 1350/2520\n3. Likewise, for the 2nd fraction, since 90 × 28 = 2520,\n25/90 = 25 × 28/90 × 28 = 700/2520\n1350/2520 + 700/2520 = 1350 + 700/2520 = 2050/2520\n5. 2050/2520 simplified gives 205/252\n6. So, 30/56 + 25/90 = 205/252\n\nMathStep (Works offline)", null, "Download our mobile app and learn to work with fractions in your own time:" ]
[ null, "https://answers.everydaycalculation.com/mathstep-app-icon.png", null ]
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https://origin.geeksforgeeks.org/split-a-string-into-two-substring-such-that-the-sum-of-unique-characters-is-maximum/
[ "", null, "Open in App\nNot now\n\n# Split a String into two Substring such that the sum of unique characters is maximum\n\n• Last Updated : 28 Mar, 2023\n\nGiven a string str, the task is to partition the string into two substrings such that the sum of unique characters of both substrings is the maximum possible.\n\nExamples:\n\nInput: str = “abcabcd”\nOutput: 7\nExplanation: Partition the given string into “abc” and “abcd”, the sum of unique characters is 3 + 4 = 7 which is maximum possible.\n\nInput: str = “aaaaa”\nOutput: 2\nExplanation: Partition the given string into “aa” and “aaa”, the sum of unique characters is 1 + 1 = 2 which is maximum possible. Given string can be partitioned into many other ways but this partition gives the maximum sum of unique characters.\n\nApproach: This problem can easily be solved using prefix and suffix arrays.\n\nWe can create a prefix array which will store the count of unique characters starting from index 0 to last index of the string. Similarly, We can create a suffix array which will store the count  of unique characters starting from the last index to 0th index. Here, set can be used to check if the current character appeared before in the iterated string or not. We can calculate the maximum sum by doing prefix[i-1] + suffix[i] for each 1 <= i < n. Take prefix[i-1] + suffix[i] so that intersecting point never counts.\n\nFollow the steps mentioned below to implement the idea:\n\n• Declare two arrays of prefix and suffix\n• Declare two sets that store the visited characters so far.\n• Store prefix[i] = prefix[i-1] if the current character has already appeared, else prefix[i] = prefix[i-1] + 1\n• Store suffix[i] = suffix[i] if the current character has already appeared, else suffix[i] = suffix[i+1] + 1.\n• Declare a variable maxi = -1 which stores the maximum sum\n• Iterate through the array and compare the sum of prefix[i-1] + suffix[i] with maxi in each iteration.\n• Return maxi.\n\nBelow is the implementation of the above approach.\n\n## C++\n\n `// C++ code for the above approach:` `#include ` `using` `namespace` `std;`   `// Function for finding out maximum value` `int` `unique_charcters(string str, ``int` `n)` `{`   `    ``// Declare set to check if the current` `    ``// character is previously` `    ``// appearing or not` `    ``set<``char``> s1;` `    ``set<``char``> s2;`   `    ``// Store the count of unique characters` `    ``// from starting index.` `    ``vector<``int``> prefix(n);`   `    ``// Store the count of unique characters` `    ``// from last index.` `    ``vector<``int``> suffix(n);` `    ``prefix = 1;` `    ``suffix[n - 1] = 1;` `    ``s1.insert(str);` `    ``s2.insert(str[n - 1]);`   `    ``// Storing the count of unique characters` `    ``// from starting index to last index` `    ``for` `(``int` `i = 1; i < n; i++) {`   `        ``// If the current character has` `        ``// appeared before, store` `        ``// previous value` `        ``if` `(s1.find(str[i]) != s1.end()) {` `            ``prefix[i] = prefix[i - 1];` `        ``}` `        ``else` `{` `            ``// else store previous value + 1.` `            ``prefix[i] = prefix[i - 1] + 1;` `            ``s1.insert(str[i]);` `        ``}` `    ``}`   `    ``// Storing the count of unique` `    ``// characters from last index` `    ``// to 0th index` `    ``for` `(``int` `i = n - 2; i >= 0; i--) {`   `        ``// If the current character has` `        ``// already appeared, store the` `        ``// value calculated for the` `        ``// previous visited index of string` `        ``if` `(s2.find(str[i]) != s2.end()) {` `            ``suffix[i] = suffix[i + 1];` `        ``}` `        ``else` `{`   `            ``// Else store value on next index + 1.` `            ``suffix[i] = suffix[i + 1] + 1;` `            ``s2.insert(str[i]);` `        ``}` `    ``}`   `    ``// Store the maximum sum` `    ``int` `maxi = -1;` `    ``for` `(``int` `i = 1; i < n; i++) {`   `        ``// Take sum of prefix[i-1] +` `        ``// suffix[i] so that the` `        ``// intersecting never counts.` `        ``maxi = max(maxi, prefix[i - 1] + suffix[i]);` `    ``}`   `    ``// Returning the maximum value` `    ``return` `maxi;` `}`   `// Driver code` `int` `main()` `{` `    ``string str = ``\"abcabcd\"``;`   `    ``// Size of the string` `    ``int` `n = str.length();`   `    ``// Function call` `    ``cout << ``\"Maximum sum is \"` `<< unique_charcters(str, n);` `    ``return` `0;` `}`\n\n## Java\n\n `// Java code for above approach`   `import` `java.util.*;`   `class` `GFG {` `    ``public` `static` `void` `main(String[] args)` `    ``{` `        ``String str = ``\"abcabcd\"``;`   `        ``// Size of the string` `        ``int` `n = str.length();`   `        ``// Function call` `        ``System.out.println(``\"Maximum sum is \"` `                           ``+ (unique_characters(str, n)));` `    ``}`   `    ``public` `static` `int` `unique_characters(String str, ``int` `n)` `    ``{` `        ``// Declare set to check if the current` `        ``// character is previously` `        ``// appearing or not` `        ``TreeSet s1 = ``new` `TreeSet<>();` `        ``TreeSet s2 = ``new` `TreeSet<>();`   `        ``// Store the count of unique characters` `        ``// from starting index.` `        ``int``[] prefix = ``new` `int``[n];`   `        ``// Store the count of unique characters` `        ``// from last index.` `        ``int``[] suffix = ``new` `int``[n];` `        ``prefix[``0``] = ``1``;` `        ``suffix[n - ``1``] = ``1``;` `        ``s1.add(str.charAt(``0``));` `        ``s2.add(str.charAt(n - ``1``));`   `        ``// from starting index to last index` `        ``for` `(``int` `i = ``1``; i < n; i++) {`   `            ``// If the current character has` `            ``// appeared before, store` `            ``// previous value` `            ``if` `((s1.contains(str.charAt(i)))` `                ``&& str.charAt(i) != s1.last()) {` `                ``prefix[i] = prefix[i - ``1``];` `            ``}` `            ``else` `{` `                ``// else store previous value + 1.` `                ``prefix[i] = prefix[i - ``1``] + ``1``;` `                ``s1.add(str.charAt(i));` `            ``}` `        ``}`   `        ``// Storing the count of unique` `        ``// characters from last index` `        ``// to 0th index` `        ``for` `(``int` `i = n - ``2``; i >= ``0``; i--) {`   `            ``// If the current character has` `            ``// already appeared, store the` `            ``// value calculated for the` `            ``// previous visited index of string` `            ``if` `((s2.contains(str.charAt(i)))` `                ``&& str.charAt(i) != s2.last()) {` `                ``suffix[i] = suffix[i + ``1``];` `            ``}` `            ``else` `{` `                ``// Else store value on next index + 1.` `                ``suffix[i] = suffix[i + ``1``] + ``1``;` `                ``s2.add(str.charAt(i));` `            ``}` `        ``}`   `        ``// Store the maximum sum` `        ``int` `maxi = -``1``;` `        ``for` `(``int` `i = ``1``; i < n; i++) {`   `            ``// Take sum of prefix[i-1] +` `            ``// suffix[i] so that the` `            ``// intersecting never counts.` `            ``maxi` `                ``= Math.max(maxi, prefix[i - ``1``] + suffix[i]);` `        ``}`   `        ``// Returning the maximum value` `        ``return` `maxi;` `    ``}` `}`\n\n## Python3\n\n `# Python code for the above approach:` `def` `unique_charcters(``str``, n):` `  ``# Declare set to check if the current` `  ``# character is previously` `  ``# appearing or not` `  ``s1 ``=` `set``()` `  ``s2 ``=` `set``()`   `  ``# Store the count of unique characters` `  ``# from starting index.` `  ``prefix ``=` `[``0``]``*``n`   `  ``# Store the count of unique characters` `  ``# from last index.` `  ``suffix ``=` `[``0``]``*``n`   `  ``prefix[``0``] ``=` `1` `  ``suffix[n ``-` `1``] ``=` `1` `  ``s1.add(``str``[``0``])` `  ``s2.add(``str``[n ``-` `1``])`   `  ``# Storing the count of unique characters` `  ``# from starting index to last index` `  ``for` `i ``in` `range``(``1``, n):`   `      ``# If the current character has` `      ``# appeared before, store` `      ``# previous value` `      ``if` `str``[i] ``in` `s1:` `          ``prefix[i] ``=` `prefix[i ``-` `1``]` `      ``else``:` `          ``# else store previous value + 1.` `          ``prefix[i] ``=` `prefix[i ``-` `1``] ``+` `1` `          ``s1.add(``str``[i])`   `  ``# Storing the count of unique` `  ``# characters from last index` `  ``# to 0th index` `  ``for` `i ``in` `range``(n``-``2``, ``-``1``, ``-``1``):`   `      ``# If the current character has` `      ``# already appeared, store the` `      ``# value calculated for the` `      ``# previous visited index of string` `      ``if` `str``[i] ``in` `s2:` `          ``suffix[i] ``=` `suffix[i ``+` `1``]` `      ``else``:`   `          ``# Else store value on next index + 1.` `          ``suffix[i] ``=` `suffix[i ``+` `1``] ``+` `1` `          ``s2.add(``str``[i])`   `  ``# Store the maximum sum` `  ``maxi ``=` `-``1` `  ``for` `i ``in` `range``(``1``, n):`   `      ``# Take sum of prefix[i-1] +` `      ``# suffix[i] so that the` `      ``# intersecting never counts.` `      ``maxi ``=` `max``(maxi, prefix[i ``-` `1``] ``+` `suffix[i])`   `  ``# Returning the maximum value` `  ``return` `maxi`   `if` `__name__ ``=``=` `\"__main__\"``:` `  ``str` `=` `\"abcabcd\"` `  ``# Size of the string` `  ``n ``=` `len``(``str``)`   `  ``# Function call` `  ``print``(``\"Maximum sum is \"``, unique_charcters(``str``, n))`\n\n## C#\n\n `// C# code for above approach`   `using` `System;` `using` `System.Collections.Generic;`   `public` `class` `GFG {`   `    ``static` `int` `UniqueCharacters(``string` `str, ``int` `n)` `    ``{` `        ``// Declare set to check if the current character is` `        ``// previously appearing or not` `        ``SortedSet<``char``> s1 = ``new` `SortedSet<``char``>();` `        ``SortedSet<``char``> s2 = ``new` `SortedSet<``char``>();`   `        ``// Store the count of unique characters from` `        ``// starting index.` `        ``int``[] prefix = ``new` `int``[n];`   `        ``// Store the count of unique characters from last` `        ``// index.` `        ``int``[] suffix = ``new` `int``[n];` `        ``prefix = 1;` `        ``suffix[n - 1] = 1;` `        ``s1.Add(str);` `        ``s2.Add(str[n - 1]);`   `        ``// from starting index to last index` `        ``for` `(``int` `i = 1; i < n; i++) {` `            ``// If the current character has appeared before,` `            ``// store previous value` `            ``if` `((s1.Contains(str[i])) && str[i] != s1.Max) {` `                ``prefix[i] = prefix[i - 1];` `            ``}` `            ``else` `{` `                ``// else store previous value + 1.` `                ``prefix[i] = prefix[i - 1] + 1;` `                ``s1.Add(str[i]);` `            ``}` `        ``}`   `        ``// Storing the count of unique characters from last` `        ``// index to 0th index` `        ``for` `(``int` `i = n - 2; i >= 0; i--) {` `            ``// If the current character has already` `            ``// appeared, store the value calculated for the` `            ``// previous visited index of string` `            ``if` `((s2.Contains(str[i])) && str[i] != s2.Max) {` `                ``suffix[i] = suffix[i + 1];` `            ``}` `            ``else` `{` `                ``// Else store value on next index + 1.` `                ``suffix[i] = suffix[i + 1] + 1;` `                ``s2.Add(str[i]);` `            ``}` `        ``}`   `        ``// Store the maximum sum` `        ``int` `maxi = -1;` `        ``for` `(``int` `i = 1; i < n; i++) {` `            ``// Take sum of prefix[i-1] + suffix[i] so that` `            ``// the intersecting never counts.` `            ``maxi` `                ``= Math.Max(maxi, prefix[i - 1] + suffix[i]);` `        ``}`   `        ``// Returning the maximum value` `        ``return` `maxi;` `    ``}`   `    ``static` `public` `void` `Main()` `    ``{`   `        ``// Code` `        ``string` `str = ``\"abcabcd\"``;` `        ``// Size of the string` `        ``int` `n = str.Length;`   `        ``// Function call` `        ``Console.WriteLine(``\"Maximum sum is \"` `                          ``+ (UniqueCharacters(str, n)));` `    ``}` `}`   `// This code is contributed by sankar.`\n\n## Javascript\n\n `// JavaScript code for the above approach:`   `// Function for finding out maximum value` `function` `uniqueCharacters(str, n) {`   `    ``// Declare set to check if the current` `    ``// character is previously` `    ``// appearing or not` `    ``var` `s1 = ``new` `Set();` `    ``var` `s2 = ``new` `Set();` `    `  `    ``// Store the count of unique characters` `    ``// from starting index.` `    ``var` `prefix = ``new` `Array(n);` `    `  `    ``// Store the count of unique characters` `    ``// from last index.` `    ``var` `suffix = ``new` `Array(n);` `    ``prefix = 1;` `    ``suffix[n - 1] = 1;` `    ``s1.add(str);` `    ``s2.add(str[n - 1]);` `    `  `    ``// Storing the count of unique characters` `    ``// from starting index to last index` `    ``for` `(``var` `i = 1; i < n; i++) {` `    `  `        ``// If the current character has` `        ``// appeared before, store` `        ``// previous value` `        ``if` `(s1.has(str[i])) {` `            ``prefix[i] = prefix[i - 1];` `        ``}` `        ``else` `{` `            ``// else store previous value + 1.` `            ``prefix[i] = prefix[i - 1] + 1;` `            ``s1.add(str[i]);` `        ``}` `    ``}` `    `  `    ``// Storing the count of unique` `    ``// characters from last index` `    ``// to 0th index` `    ``for` `(``var` `i = n - 2; i >= 0; i--) {` `    `  `        ``// If the current character has` `        ``// already appeared, store the` `        ``// value calculated for the` `        ``// previous visited index of string` `        ``if` `(s2.has(str[i])) {` `            ``suffix[i] = suffix[i + 1];` `        ``}` `        ``else` `{` `    `  `            ``// Else store value on next index + 1.` `            ``suffix[i] = suffix[i + 1] + 1;` `            ``s2.add(str[i]);` `        ``}` `    ``}` `    `  `    ``// Store the maximum sum` `    ``var` `maxi = -1;` `    ``for` `(``var` `i = 1; i < n; i++) {` `    `  `        ``// Take sum of prefix[i-1] +` `        ``// suffix[i] so that the` `        ``// intersecting never counts.` `        ``maxi = Math.max(maxi, prefix[i - 1] + suffix[i]);` `    ``}` `    `  `    ``// Returning the maximum value` `    ``return` `maxi;` `}`   `// Driver code` `var` `str = ``\"abcabcd\"``;`   `// Size of the string` `var` `n = str.length;`   `// Function call` `console.log(``\"Maximum sum is \"` `+ uniqueCharacters(str, n));`   `// This Code is Contributed by Prasad Kandekar(prasad264)`\n\nOutput\n\n`Maximum value is 7`\n\nTime Complexity: O(N)\nAuxiliary Space: O(N)\n\nEfficient Approach: To solve this problem, we will use two Hash Maps and do the below steps:\n\n• Firstly, make a frequency map of characters and store in Hash Map characters.\n• Now, we will traverse from the start of the given string str, also we will maintain another frequency map using Hash Map freq.\n• While traversing, we will keep track of the maximum sum of the sizes of characters and freq, whenever our maximum value changes we will change our maximum pointer.\n• At last, we will return the maximum possible answer.\n\nImplementation of the approach:\n\n## C++\n\n `#include ` `#include ` `#include `   `using` `namespace` `std;`   `int` `maxUniqueCharSubstring(string str, ``int` `N)` `{` `    ``// Initializing two frequency Hash Maps` `    ``unordered_map<``char``, ``int``> characters;` `    ``unordered_map<``char``, ``int``> freq;`   `    ``// Making a frequency map of characters` `    ``for` `(``int` `i = 0; i < N; i++) {` `        ``characters[str[i]]++;` `    ``}`   `    ``// max variable which contains maximum sum of unique` `    ``// characters` `    ``int` `max = INT_MIN;`   `    ``// Traversing the string` `    ``for` `(``int` `i = 0; i < N; i++) {` `        ``// Updating max variable` `        ``int` `totalChar = (characters.size() + freq.size());` `        ``if` `(max < totalChar) {` `            ``max = totalChar;` `        ``}` `        ``// Updating both hash maps` `        ``freq[str[i]]++;` `        ``characters[str[i]]--;`   `        ``if` `(characters[str[i]] == 0) {` `            ``characters.erase(str[i]);` `        ``}` `    ``}`   `    ``// Returning max value` `    ``return` `max;` `}`   `int` `main()` `{` `    ``string str = ``\"abcabcd\"``;` `    ``int` `N = str.length();` `    ``cout << ``\"Maximum sum is \"` `         ``<< maxUniqueCharSubstring(str, N) << endl;` `    ``return` `0;` `}`\n\n## Java\n\n `// Java algorithm for the above approach`   `import` `java.util.*;`   `class` `GFG {` `    ``// Driver Code` `    ``public` `static` `void` `main(String[] args)` `    ``{` `        ``String str = ``\"abcabcd\"``;` `        ``int` `N = str.length();` `        ``System.out.println(` `            ``\"Maximum sum is \"` `            ``+ maxUniqueCharSubstring(str, N));` `    ``}`   `    ``public` `static` `int` `maxUniqueCharSubstring(String str,` `                                             ``int` `N)` `    ``{` `        ``// Initializing two frequency Hash Maps` `        ``Map characters` `            ``= ``new` `HashMap<>();` `        ``Map freq = ``new` `HashMap<>();`   `        ``// Making a frequency map of characters` `        ``for` `(``int` `i = ``0``; i < N; i++) {` `            ``characters.put(` `                ``str.charAt(i),` `                ``characters.getOrDefault(str.charAt(i), ``0``)` `                    ``+ ``1``);` `        ``}` `        ``// max variable which contains maximum sum of unique` `        ``// characters` `        ``int` `max = Integer.MIN_VALUE;` `        ``// Traversing the string` `        ``for` `(``int` `i = ``0``; i < N; i++) {` `            ``// Updating max variable` `            ``if` `(max < characters.size() + freq.size()) {` `                ``max = characters.size() + freq.size();` `            ``}` `            ``// Updating both hash maps` `            ``freq.put(str.charAt(i),` `                     ``freq.getOrDefault(str.charAt(i), ``0``)` `                         ``+ ``1``);` `            ``characters.put(str.charAt(i),` `                           ``characters.get(str.charAt(i))` `                               ``- ``1``);`   `            ``if` `(characters.get(str.charAt(i)) == ``0``)` `                ``characters.remove(str.charAt(i));` `        ``}` `        ``// Returning max value` `        ``return` `max;` `    ``}` `}`\n\n## Python3\n\n `# Python code for the above approach` `def` `maxUniqueCharSubstring(string):` `    ``# Initializing two frequency dictionaries` `    ``characters ``=` `{}` `    ``freq ``=` `{}`   `    ``# Making a frequency map of characters` `    ``for` `i ``in` `string:` `        ``if` `i ``in` `characters:` `            ``characters[i] ``+``=` `1` `        ``else``:` `            ``characters[i] ``=` `1`   `    ``# max variable which contains maximum sum of unique` `    ``# characters` `    ``max_len ``=` `float``(``'-inf'``)`   `    ``# Traversing the string` `    ``for` `i ``in` `range``(``len``(string)):` `        ``# Updating max variable` `        ``if` `max_len < ``len``(characters) ``+` `len``(freq):` `            ``max_len ``=` `len``(characters) ``+` `len``(freq)`   `        ``# Updating both dictionaries` `        ``if` `string[i] ``in` `freq:` `            ``freq[string[i]] ``+``=` `1` `        ``else``:` `            ``freq[string[i]] ``=` `1`   `        ``characters[string[i]] ``=` `characters[string[i]] ``-` `1`   `        ``if` `characters[string[i]] ``=``=` `0``:` `            ``del` `characters[string[i]]`   `    ``# Returning max value` `    ``return` `max_len`     `# Driver code` `string ``=` `\"abcabcd\"` `print``(``\"Maximum sum is\"``, maxUniqueCharSubstring(string))` `# This code is contributed by codearcade.`\n\n## C#\n\n `// C# code for the above approach`   `using` `System;` `using` `System.Collections.Generic;`   `public` `class` `GFG {`   `    ``public` `static` `int` `maxUniqueCharSubstring(``string` `str,` `                                             ``int` `N)` `    ``{` `        ``// Initializing two frequency Hash Maps` `        ``Dictionary<``char``, ``int``> characters` `            ``= ``new` `Dictionary<``char``, ``int``>();` `        ``Dictionary<``char``, ``int``> freq` `            ``= ``new` `Dictionary<``char``, ``int``>();`   `        ``// Making a frequency map of characters` `        ``for` `(``int` `i = 0; i < N; i++) {` `            ``if` `(characters.ContainsKey(str[i]))` `                ``characters[str[i]] += 1;` `            ``else` `                ``characters.Add(str[i], 1);` `        ``}`   `        ``// max variable which contains maximum sum of unique` `        ``// characters` `        ``int` `max = ``int``.MinValue;`   `        ``// Traversing the string` `        ``for` `(``int` `i = 0; i < N; i++) {` `            ``// Updating max variable` `            ``if` `(max < characters.Count + freq.Count) {` `                ``max = characters.Count + freq.Count;` `            ``}`   `            ``// Updating both hash maps` `            ``if` `(freq.ContainsKey(str[i]))` `                ``freq[str[i]] += 1;` `            ``else` `                ``freq.Add(str[i], 1);`   `            ``characters[str[i]] -= 1;`   `            ``if` `(characters[str[i]] == 0)` `                ``characters.Remove(str[i]);` `        ``}`   `        ``// Returning max value` `        ``return` `max;` `    ``}`   `    ``static` `public` `void` `Main()` `    ``{`   `        ``// Code` `        ``string` `str = ``\"abcabcd\"``;` `        ``int` `N = str.Length;` `        ``Console.WriteLine(``\"Maximum sum is \"` `                          ``+ maxUniqueCharSubstring(str, N));` `    ``}` `}`   `// This code is contributed by karthik.`\n\n## Javascript\n\n `// JavaScript code for the above approach` `function` `maxUniqueCharSubstring(str, N)` `{`   `    ``// Initializing two frequency Hash Maps` `    ``let characters = ``new` `Map();` `    ``let freq = ``new` `Map();`   `    ``// Making a frequency map of characters` `    ``for` `(let i = 0; i < N; i++) {` `        ``characters.set(str[i], (characters.get(str[i]) || 0) + 1);` `    ``}`   `    ``// max variable which contains maximum sum of unique` `    ``// characters` `    ``let max = Number.MIN_SAFE_INTEGER;`   `    ``// Traversing the string` `    ``for` `(let i = 0; i < N; i++) {` `        ``// Updating max variable` `        ``let totalChar = (characters.size + freq.size);` `        ``if` `(max < totalChar) {` `            ``max = totalChar;` `        ``}`   `        ``// Updating both hash maps` `        ``freq.set(str[i], (freq.get(str[i]) || 0) + 1);` `        ``characters.set(str[i], (characters.get(str[i]) || 0) - 1);`   `        ``if` `(characters.get(str[i]) === 0) {` `            ``characters.``delete``(str[i]);` `        ``}` `    ``}`   `    ``// Returning max value` `    ``return` `max;` `}`   `let str = ``\"abcabcd\"``;` `let N = str.length;` `console.log(``\"Maximum sum is \"` `+ maxUniqueCharSubstring(str, N));`   `// This code is contributed by prasad264`\n\nOutput:\n\n`Maximum sum is 7`\n\nTime Complexity: O(N)\n\nAuxiliary Space: Constant space is used as there can be only at most 26 characters stored in hash map.\n\nMy Personal Notes arrow_drop_up\nRelated Articles" ]
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https://www.bartleby.com/solution-answer/chapter-91-problem-2swu-calculus-an-applied-approach-mindtap-course-list-10th-edition/9781305860919/in-exercises-1-and-2-solve-for-x-112181413x241/e687be7b-6362-11e9-8385-02ee952b546e
[ "", null, "", null, "", null, "Chapter 9.1, Problem 2SWU", null, "### Calculus: An Applied Approach (Min...\n\n10th Edition\nRon Larson\nISBN: 9781305860919\n\n#### Solutions\n\nChapter\nSection", null, "### Calculus: An Applied Approach (Min...\n\n10th Edition\nRon Larson\nISBN: 9781305860919\nTextbook Problem\n1 views\n\n# In Exercises 1 and 2, solve for x. 1 12 + 1 8 + 1 4 + 1 3 + x 24 = 1\n\nTo determine\n\nTo calculate: The value of x from the expression: 112+18+14+13+x24=1.\n\nExplanation\n\nGiven information:\n\nThe expression: 112+18+14+13+x24=1.\n\nCalculation:\n\nConsider the expression,\n\n112+18+14+13+x24=1\n\nWrite common denominator for given expression,\n\n112+18+14+13+x24=11×212×2+1×38×3+1×64×6+\n\n### Still sussing out bartleby?\n\nCheck out a sample textbook solution.\n\nSee a sample solution\n\n#### The Solution to Your Study Problems\n\nBartleby provides explanations to thousands of textbook problems written by our experts, many with advanced degrees!\n\nGet Started\n\n#### Solve the equations in Exercises 126. 14x2=0\n\nFinite Mathematics and Applied Calculus (MindTap Course List)\n\n#### Evaluate limxesinx1x.\n\nCalculus (MindTap Course List)\n\n#### In problems 15-22, simplify by combining like terms. 19.\n\nMathematical Applications for the Management, Life, and Social Sciences\n\n#### In Exercises 110, find the graphical solution to each inequality. 3y+50\n\nFinite Mathematics for the Managerial, Life, and Social Sciences\n\n#### It does not exist.\n\nStudy Guide for Stewart's Multivariable Calculus, 8th\n\n#### The implied domain of is: (1, ∞) (−∞, 1) x ≠ 1 (−1, 1)\n\nStudy Guide for Stewart's Single Variable Calculus: Early Transcendentals, 8th", null, "" ]
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https://www.colorhexa.com/01f3f2
[ "# #01f3f2 Color Information\n\nIn a RGB color space, hex #01f3f2 is composed of 0.4% red, 95.3% green and 94.9% blue. Whereas in a CMYK color space, it is composed of 99.6% cyan, 0% magenta, 0.4% yellow and 4.7% black. It has a hue angle of 179.8 degrees, a saturation of 99.2% and a lightness of 47.8%. #01f3f2 color hex could be obtained by blending #02ffff with #00e7e5. Closest websafe color is: #00ffff.\n\n• R 0\n• G 95\n• B 95\nRGB color chart\n• C 100\n• M 0\n• Y 0\n• K 5\nCMYK color chart\n\n#01f3f2 color description : Vivid cyan.\n\n# #01f3f2 Color Conversion\n\nThe hexadecimal color #01f3f2 has RGB values of R:1, G:243, B:242 and CMYK values of C:1, M:0, Y:0, K:0.05. Its decimal value is 127986.\n\nHex triplet RGB Decimal 01f3f2 `#01f3f2` 1, 243, 242 `rgb(1,243,242)` 0.4, 95.3, 94.9 `rgb(0.4%,95.3%,94.9%)` 100, 0, 0, 5 179.8°, 99.2, 47.8 `hsl(179.8,99.2%,47.8%)` 179.8°, 99.6, 95.3 00ffff `#00ffff`\nCIE-LAB 87.248, -46.627, -13.147 48.085, 70.513, 95.076 0.225, 0.33, 70.513 87.248, 48.446, 195.747 87.248, -67.562, -13.732 83.972, -44.737, -8.349 00000001, 11110011, 11110010\n\n# Color Schemes with #01f3f2\n\n• #01f3f2\n``#01f3f2` `rgb(1,243,242)``\n• #f30102\n``#f30102` `rgb(243,1,2)``\nComplementary Color\n• #01f379\n``#01f379` `rgb(1,243,121)``\n• #01f3f2\n``#01f3f2` `rgb(1,243,242)``\n• #017bf3\n``#017bf3` `rgb(1,123,243)``\nAnalogous Color\n• #f37901\n``#f37901` `rgb(243,121,1)``\n• #01f3f2\n``#01f3f2` `rgb(1,243,242)``\n• #f3017b\n``#f3017b` `rgb(243,1,123)``\nSplit Complementary Color\n• #f3f201\n``#f3f201` `rgb(243,242,1)``\n• #01f3f2\n``#01f3f2` `rgb(1,243,242)``\n• #f201f3\n``#f201f3` `rgb(242,1,243)``\n• #02f301\n``#02f301` `rgb(2,243,1)``\n• #01f3f2\n``#01f3f2` `rgb(1,243,242)``\n• #f201f3\n``#f201f3` `rgb(242,1,243)``\n• #f30102\n``#f30102` `rgb(243,1,2)``\n• #01a7a6\n``#01a7a6` `rgb(1,167,166)``\n• #01c0bf\n``#01c0bf` `rgb(1,192,191)``\n``#01dad9` `rgb(1,218,217)``\n• #01f3f2\n``#01f3f2` `rgb(1,243,242)``\n• #0ffefd\n``#0ffefd` `rgb(15,254,253)``\n• #29fefd\n``#29fefd` `rgb(41,254,253)``\n• #42fefd\n``#42fefd` `rgb(66,254,253)``\nMonochromatic Color\n\n# Alternatives to #01f3f2\n\nBelow, you can see some colors close to #01f3f2. Having a set of related colors can be useful if you need an inspirational alternative to your original color choice.\n\n• #01f3b6\n``#01f3b6` `rgb(1,243,182)``\n• #01f3ca\n``#01f3ca` `rgb(1,243,202)``\n• #01f3de\n``#01f3de` `rgb(1,243,222)``\n• #01f3f2\n``#01f3f2` `rgb(1,243,242)``\n• #01e0f3\n``#01e0f3` `rgb(1,224,243)``\n• #01ccf3\n``#01ccf3` `rgb(1,204,243)``\n• #01b8f3\n``#01b8f3` `rgb(1,184,243)``\nSimilar Colors\n\n# #01f3f2 Preview\n\nThis text has a font color of #01f3f2.\n\n``<span style=\"color:#01f3f2;\">Text here</span>``\n#01f3f2 background color\n\nThis paragraph has a background color of #01f3f2.\n\n``<p style=\"background-color:#01f3f2;\">Content here</p>``\n#01f3f2 border color\n\nThis element has a border color of #01f3f2.\n\n``<div style=\"border:1px solid #01f3f2;\">Content here</div>``\nCSS codes\n``.text {color:#01f3f2;}``\n``.background {background-color:#01f3f2;}``\n``.border {border:1px solid #01f3f2;}``\n\n# Shades and Tints of #01f3f2\n\nA shade is achieved by adding black to any pure hue, while a tint is created by mixing white to any pure color. In this example, #000909 is the darkest color, while #f4ffff is the lightest one.\n\n• #000909\n``#000909` `rgb(0,9,9)``\n• #001c1c\n``#001c1c` `rgb(0,28,28)``\n• #00302f\n``#00302f` `rgb(0,48,47)``\n• #004343\n``#004343` `rgb(0,67,67)``\n• #005756\n``#005756` `rgb(0,87,86)``\n• #006a6a\n``#006a6a` `rgb(0,106,106)``\n• #017e7d\n``#017e7d` `rgb(1,126,125)``\n• #019191\n``#019191` `rgb(1,145,145)``\n• #01a5a4\n``#01a5a4` `rgb(1,165,164)``\n• #01b8b8\n``#01b8b8` `rgb(1,184,184)``\n• #01cccb\n``#01cccb` `rgb(1,204,203)``\n• #01dfdf\n``#01dfdf` `rgb(1,223,223)``\n• #01f3f2\n``#01f3f2` `rgb(1,243,242)``\n• #0afefd\n``#0afefd` `rgb(10,254,253)``\n• #1dfefd\n``#1dfefd` `rgb(29,254,253)``\n• #31fefd\n``#31fefd` `rgb(49,254,253)``\n• #44fefd\n``#44fefd` `rgb(68,254,253)``\n• #58fefe\n``#58fefe` `rgb(88,254,254)``\n• #6bfefe\n``#6bfefe` `rgb(107,254,254)``\n• #7ffefe\n``#7ffefe` `rgb(127,254,254)``\n• #92fffe\n``#92fffe` `rgb(146,255,254)``\n• #a6fffe\n``#a6fffe` `rgb(166,255,254)``\n• #b9fffe\n``#b9fffe` `rgb(185,255,254)``\n• #cdffff\n``#cdffff` `rgb(205,255,255)``\n• #e1ffff\n``#e1ffff` `rgb(225,255,255)``\n• #f4ffff\n``#f4ffff` `rgb(244,255,255)``\nTint Color Variation\n\n# Tones of #01f3f2\n\nA tone is produced by adding gray to any pure hue. In this case, #728282 is the less saturated color, while #01f3f2 is the most saturated one.\n\n• #728282\n``#728282` `rgb(114,130,130)``\n• #688c8c\n``#688c8c` `rgb(104,140,140)``\n• #5f9595\n``#5f9595` `rgb(95,149,149)``\n• #559f9e\n``#559f9e` `rgb(85,159,158)``\n• #4ca8a8\n``#4ca8a8` `rgb(76,168,168)``\n• #43b1b1\n``#43b1b1` `rgb(67,177,177)``\n• #39bbba\n``#39bbba` `rgb(57,187,186)``\n• #30c4c3\n``#30c4c3` `rgb(48,196,195)``\n• #27cdcd\n``#27cdcd` `rgb(39,205,205)``\n• #1dd7d6\n``#1dd7d6` `rgb(29,215,214)``\n• #14e0df\n``#14e0df` `rgb(20,224,223)``\n• #0aeae9\n``#0aeae9` `rgb(10,234,233)``\n• #01f3f2\n``#01f3f2` `rgb(1,243,242)``\nTone Color Variation\n\n# Color Blindness Simulator\n\nBelow, you can see how #01f3f2 is perceived by people affected by a color vision deficiency. This can be useful if you need to ensure your color combinations are accessible to color-blind users.\n\nMonochromacy\n• Achromatopsia 0.005% of the population\n• Atypical Achromatopsia 0.001% of the population\nDichromacy\n• Protanopia 1% of men\n• Deuteranopia 1% of men\n• Tritanopia 0.001% of the population\nTrichromacy\n• Protanomaly 1% of men, 0.01% of women\n• Deuteranomaly 6% of men, 0.4% of women\n• Tritanomaly 0.01% of the population" ]
[ null ]
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https://www.stumblingrobot.com/2016/01/13/solve-the-differential-equation-x-x-e2t-for-given-initial-values/
[ "Home » Blog » Solve the differential equation x′ + x = e2t for given initial values\n\n# Solve the differential equation x′ + x = e2t for given initial values\n\nSolve the following differential equation:", null, "with", null, "when", null, ".\n\nFrom Theorem 8.3 (page 310 of Apostol) we know that a differential equation of the form", null, "on an interval", null, "has solution given by", null, "where", null, "In this particular case we apply the theorem (noting that in this problem we have", null, "is a function of", null, ", rather than", null, "a function of", null, "as in the theorem… of course, the names of the variables doesn’t matter, but we take care to apply the theorem properly) with", null, "This gives us", null, "Therefore,", null, "" ]
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https://stats.libretexts.org/Courses/Penn_State_University_Greater_Allegheny/STAT_200%3A_Introductory_Statistics_(OpenStax)_GAYDOS/07%3A_The_Central_Limit_Theorem/7.01%3A_The_Central_Limit_Theorem_for_Sample_Means_(Averages)/7.1E%3A_The_Central_Limit_Theorem_for_Sample_Means_(Exercises)
[ "# 7.1E: The Central Limit Theorem for Sample Means (Exercises)\n\n•", null, "• OpenStax\n• OpenStax\n$$\\newcommand{\\vecs}{\\overset { \\rightharpoonup} {\\mathbf{#1}} }$$ $$\\newcommand{\\vecd}{\\overset{-\\!-\\!\\rightharpoonup}{\\vphantom{a}\\smash {#1}}}$$$$\\newcommand{\\id}{\\mathrm{id}}$$ $$\\newcommand{\\Span}{\\mathrm{span}}$$ $$\\newcommand{\\kernel}{\\mathrm{null}\\,}$$ $$\\newcommand{\\range}{\\mathrm{range}\\,}$$ $$\\newcommand{\\RealPart}{\\mathrm{Re}}$$ $$\\newcommand{\\ImaginaryPart}{\\mathrm{Im}}$$ $$\\newcommand{\\Argument}{\\mathrm{Arg}}$$ $$\\newcommand{\\norm}{\\| #1 \\|}$$ $$\\newcommand{\\inner}{\\langle #1, #2 \\rangle}$$ $$\\newcommand{\\Span}{\\mathrm{span}}$$ $$\\newcommand{\\id}{\\mathrm{id}}$$ $$\\newcommand{\\Span}{\\mathrm{span}}$$ $$\\newcommand{\\kernel}{\\mathrm{null}\\,}$$ $$\\newcommand{\\range}{\\mathrm{range}\\,}$$ $$\\newcommand{\\RealPart}{\\mathrm{Re}}$$ $$\\newcommand{\\ImaginaryPart}{\\mathrm{Im}}$$ $$\\newcommand{\\Argument}{\\mathrm{Arg}}$$ $$\\newcommand{\\norm}{\\| #1 \\|}$$ $$\\newcommand{\\inner}{\\langle #1, #2 \\rangle}$$ $$\\newcommand{\\Span}{\\mathrm{span}}$$$$\\newcommand{\\AA}{\\unicode[.8,0]{x212B}}$$\n\nUse the following information to answer the next six exercises: Yoonie is a personnel manager in a large corporation. Each month she must review 16 of the employees. From past experience, she has found that the reviews take her approximately four hours each to do with a population standard deviation of 1.2 hours. Let $$X$$ be the random variable representing the time it takes her to complete one review. Assume $$X$$ is normally distributed. Let $$\\bar{X}$$ be the random variable representing the mean time to complete the 16 reviews. Assume that the 16 reviews represent a random set of reviews.\n\n##### Example $$\\PageIndex{1}$$\n\nWhat is the mean, standard deviation, and sample size?\n\nmean = 4 hours; standard deviation = 1.2 hours; sample size = 16\n\nExercise $$\\PageIndex{2}$$\n\nComplete the distributions.\n\n1. $$X \\sim$$ _____(_____,_____)\n2. $$\\bar{X} \\sim$$ _____(_____,_____)\n##### Example $$\\PageIndex{3}$$\n\nFind the probability that one review will take Yoonie from 3.5 to 4.25 hours. Sketch the graph, labeling and scaling the horizontal axis. Shade the region corresponding to the probability.", null, "Figure $$\\PageIndex{2}$$.\n\n2. $$P$$(________ $$< x <$$ ________) = _______\n\n1. Check student's solution.\n2. 3.5, 4.25, 0.2441\n\nExercise $$\\PageIndex{4}$$\n\nFind the probability that the mean of a month’s reviews will take Yoonie from 3.5 to 4.25 hrs. Sketch the graph, labeling and scaling the horizontal axis. Shade the region corresponding to the probability.", null, "Figure $$\\PageIndex{3}$$.\n\n2. $$P$$(________________) = _______\n\n##### Example $$\\PageIndex{5}$$\n\nWhat causes the probabilities in Exercise and Exercise to be different?\n\nThe fact that the two distributions are different accounts for the different probabilities.\n\nExercise $$\\PageIndex{6}$$\n\nFind the 95th percentile for the mean time to complete one month's reviews. Sketch the graph.", null, "Figure $$\\PageIndex{4}$$.\n\n1. The 95th Percentile =____________\n\nThis page titled 7.1E: The Central Limit Theorem for Sample Means (Exercises) is shared under a CC BY 4.0 license and was authored, remixed, and/or curated by OpenStax via source content that was edited to the style and standards of the LibreTexts platform; a detailed edit history is available upon request." ]
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https://in.mathworks.com/matlabcentral/fileexchange/14469-performing-random-numbers-generator-from-a-generic-discrete-distribution
[ "## Performing random numbers generator from a generic discrete distribution\n\nVersion 1.0.0.0 (28.7 KB) by\nThis function extracts random numbers distributed over a discrete set; the PDF is user-defined\n\nUpdated Tue, 03 Apr 2007 16:47:55 +0000\n\nThis function extracts a scalar/vector/matrix of random numbers with discrete Probability Distribution Function.\nThe PDF is specified by the user as a input vector.\n\nThis function is designed to be fast, and it is implemented within a .mex file\n\nFollowing Olivier B. comments (that I acknowledge for his comments), I performed cross-comparisons with randp. gDiscrPdfRnd is faster with a ratio that increases with the number of number, i.e. for about 3 times faster for 10^6 numbers to over 40 times faster for 10^7 numbers.\nMoreover, for large random arrays, randp seriously surcharges the RAM memory, whereas gDiscrPdfRnd limits thememory use to what is essential (tanksto the coding). In what follows the details of thecomparison are given.\n\n>> tic;R = randp([1 3 2],1000000,1);toc\n\nelapsed_time =\n\n0.4840\n\n>> tic;R = gDiscrPdfRnd([1 3 2],1000000,1);toc\n\nelapsed_time =\n\n0.1570\n\n>> tic;R = randp([1 3 2],10000000,1);toc\n\nelapsed_time =\n\n68.5780\n\n>> tic;R = gDiscrPdfRnd([1 3 2],10000000,1);toc\n\nelapsed_time =\n\n1.6410\n\n>> 68.5780/1.6410\n\nans =\n\n41.7904\n\n### Cite As\n\nGianluca Dorini (2023). Performing random numbers generator from a generic discrete distribution (https://www.mathworks.com/matlabcentral/fileexchange/14469-performing-random-numbers-generator-from-a-generic-discrete-distribution), MATLAB Central File Exchange. Retrieved .\n\n##### MATLAB Release Compatibility\nCreated with R13\nCompatible with any release\n##### Platform Compatibility\nWindows macOS Linux" ]
[ null ]
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https://docs.openquake.org/oq-engine/3.10/_modules/openquake/hazardlib/source/rupture.html
[ "# Source code for openquake.hazardlib.source.rupture\n\n```# coding: utf-8\n# The Hazard Library\n# Copyright (C) 2012-2020 GEM Foundation\n#\n# This program is free software: you can redistribute it and/or modify\n# it under the terms of the GNU Affero General Public License as\n# published by the Free Software Foundation, either version 3 of the\n#\n# This program is distributed in the hope that it will be useful,\n# but WITHOUT ANY WARRANTY; without even the implied warranty of\n# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the\n# GNU Affero General Public License for more details.\n#\n# You should have received a copy of the GNU Affero General Public License\n# along with this program. If not, see <http://www.gnu.org/licenses/>.\n\"\"\"\nModule :mod:`openquake.hazardlib.source.rupture` defines classes\n:class:`BaseRupture` and its subclasses\n:class:`NonParametricProbabilisticRupture` and\n:class:`ParametricProbabilisticRupture`\n\"\"\"\nimport abc\nimport numpy\nimport math\nimport itertools\nimport json\nfrom openquake.baselib import general, hdf5\nfrom openquake.hazardlib import geo, contexts\nfrom openquake.hazardlib.geo.nodalplane import NodalPlane\nfrom openquake.hazardlib.geo.mesh import (\nMesh, RectangularMesh, surface_to_array)\nfrom openquake.hazardlib.geo.point import Point\nfrom openquake.hazardlib.geo.geodetic import geodetic_distance\nfrom openquake.hazardlib.near_fault import (\nfrom openquake.hazardlib.geo.surface.base import BaseSurface\n\nU8 = numpy.uint8\nU16 = numpy.uint16\nU32 = numpy.uint32\nF32 = numpy.float32\nF64 = numpy.float64\nTWO16 = 2 ** 16\nTWO32 = 2 ** 32\npmf_dt = numpy.dtype([('prob', float), ('occ', U32)])\nevents_dt = numpy.dtype([('id', U32), ('rup_id', U32), ('rlz_id', U16)])\nrupture_dt = numpy.dtype([('serial', U32),\n('mag', F32),\n('rake', F32),\n('lon', F32),\n('lat', F32),\n('dep', F32),\n('multiplicity', U32),\n('trt', hdf5.vstr),\n('kind', hdf5.vstr),\n('mesh', hdf5.vstr),\n('extra', hdf5.vstr)])\n\ncode2cls = {}\n\n[docs]def to_csv_array(ruptures):\n\"\"\"\n:param ruptures: a list of ruptures\n:returns: an array of ruptures suitable for serialization in CSV\n\"\"\"\nif not code2cls:\ncode2cls.update(BaseRupture.init())\narr = numpy.zeros(len(ruptures), rupture_dt)\nfor rec, rup in zip(arr, ruptures):\nmesh = surface_to_array(rup.surface) # shape (3, s1, s2)\nrec['serial'] = rup.rup_id\nrec['mag'] = rup.mag\nrec['rake'] = rup.rake\nrec['lon'] = rup.hypocenter.x\nrec['lat'] = rup.hypocenter.y\nrec['dep'] = rup.hypocenter.z\nrec['multiplicity'] = rup.multiplicity\nrec['trt'] = rup.tectonic_region_type\nrec['kind'] = ' '.join(cls.__name__ for cls in code2cls[rup.code])\nrec['mesh'] = json.dumps(\n[[[float5(z) for z in y] for y in x] for x in mesh])\nextra = {}\nif hasattr(rup, 'probs_occur'):\nextra['probs_occur'] = rup.probs_occur\nelse:\nextra['occurrence_rate'] = rup.occurrence_rate\nif hasattr(rup, 'weight'):\nextra['weight'] = rup.weight\n_fixfloat32(extra)\nrec['extra'] = json.dumps(extra)\nreturn arr\n\n[docs]def from_array(aw):\n\"\"\"\n:returns: a list of ruptures from an ArrayWrapper\n\"\"\"\nrups = []\nnames = aw.array.dtype.names\nfor rec in aw.array:\ndic = dict(zip(names, rec))\ndic['trt'] = aw.trts[int(dic.pop('grp_id'))]\ndic['hypo'] = dic.pop('lon'), dic.pop('lat'), dic.pop('dep')\nrups.append(_get_rupture(dic))\nreturn rups\n\ndef _get_rupture(rec, geom=None, trt=None):\n# rec: a dictionary or a record\n# geom: if any, an array of floats32 convertible into a mesh\nif not code2cls:\ncode2cls.update(BaseRupture.init())\nif geom is None:\nlons = rec['lons']\nmesh = numpy.zeros((3, len(lons), len(lons)), F32)\nmesh = rec['lons']\nmesh = rec['lats']\nmesh = rec['depths']\nelse:\nmesh = geom.reshape(rec['s1'], rec['s2'], 3).transpose(2, 0, 1)\nrupture_cls, surface_cls = code2cls[rec['code']]\nrupture = object.__new__(rupture_cls)\nrupture.rup_id = rec['serial']\nrupture.surface = object.__new__(surface_cls)\nrupture.mag = rec['mag']\nrupture.rake = rec['rake']\nrupture.hypocenter = geo.Point(*rec['hypo'])\nrupture.occurrence_rate = rec['occurrence_rate']\ntry:\nrupture.probs_occur = rec['probs_occur']\nexcept (KeyError, ValueError): # rec can be a numpy record\npass\nrupture.tectonic_region_type = trt or rec['trt']\nif surface_cls is geo.PlanarSurface:\nrupture.surface = geo.PlanarSurface.from_array(\nmesh[:, 0, :])\nelif surface_cls is geo.MultiSurface:\n# mesh has shape (3, n, 4)\nrupture.surface.__init__([\ngeo.PlanarSurface.from_array(mesh[:, i, :])\nfor i in range(mesh.shape)])\nelif surface_cls is geo.GriddedSurface:\n# fault surface, strike and dip will be computed\nrupture.surface.strike = rupture.surface.dip = None\nrupture.surface.mesh = Mesh(*mesh)\nelse:\n# fault surface, strike and dip will be computed\nrupture.surface.strike = rupture.surface.dip = None\nrupture.surface.__init__(RectangularMesh(*mesh))\nrupture.multiplicity = rec['n_occ']\nreturn rupture\n\n[docs]def float5(x):\n# a float with 5 digits\nreturn round(float(x), 5)\n\ndef _fixfloat32(dic):\n# work around a TOML/numpy issue\nfor k, v in dic.items():\nif isinstance(v, F32):\ndic[k] = float5(v)\nelif isinstance(v, tuple):\ndic[k] = [float5(x) for x in v]\nelif isinstance(v, numpy.ndarray):\nif len(v.shape) == 3: # 3D array\ndic[k] = [[[float5(z) for z in y] for y in x] for x in v]\nelif len(v.shape) == 2: # 2D array\ndic[k] = [[float5(y) for y in x] for x in v]\nelif len(v.shape) == 1: # 1D array\ndic[k] = [float5(x) for x in v]\nelse:\nraise NotImplementedError\n\n[docs]def to_checksum8(cls1, cls2):\n\"\"\"\nConvert a pair of classes into a numeric code (uint8)\n\"\"\"\nnames = '%s,%s' % (cls1.__name__, cls2.__name__)\nreturn sum(map(ord, names)) % 256\n\n[docs]class BaseRupture(metaclass=abc.ABCMeta):\n\"\"\"\nRupture object represents a single earthquake rupture.\n\n:param mag:\nMagnitude of the rupture.\n:param rake:\nRake value of the rupture.\nSee :class:`~openquake.hazardlib.geo.nodalplane.NodalPlane`.\n:param tectonic_region_type:\nRupture's tectonic regime. One of constants\nin :class:`openquake.hazardlib.const.TRT`.\n:param hypocenter:\nA :class:`~openquake.hazardlib.geo.point.Point`, rupture's hypocenter.\n:param surface:\nAn instance of subclass of\n:class:`~openquake.hazardlib.geo.surface.base.BaseSurface`.\nObject representing the rupture surface geometry.\n:param rupture_slip_direction:\nAngle describing rupture propagation direction in decimal degrees.\n\n:raises ValueError:\nIf magnitude value is not positive, or tectonic region type is unknown.\n\nNB: if you want to convert the rupture into XML, you should set the\nattribute surface_nodes to an appropriate value.\n\"\"\"\nrup_id = 0 # set to a value > 0 by the engine\n_code = {}\n\n[docs] @classmethod\ndef init(cls):\n\"\"\"\nInitialize the class dictionary `._code` by encoding the\nbidirectional correspondence between an integer in the range 0..255\n(the code) and a pair of classes (rupture_class, surface_class).\nThis is useful when serializing the rupture to and from HDF5.\n:returns: {code: pair of classes}\n\"\"\"\nrupture_classes = [BaseRupture] + list(\ngeneral.gen_subclasses(BaseRupture))\nsurface_classes = list(general.gen_subclasses(BaseSurface))\ncode2cls = {}\nBaseRupture.str2code = {}\nfor rup, sur in itertools.product(rupture_classes, surface_classes):\nchk = to_checksum8(rup, sur)\nif chk in code2cls and code2cls[chk] != (rup, sur):\nraise ValueError('Non-unique checksum %d for %s, %s' %\n(chk, rup, sur))\ncls._code[rup, sur] = chk\ncode2cls[chk] = rup, sur\nBaseRupture.str2code['%s %s' % (rup.__name__, sur.__name__)] = chk\nreturn code2cls\n\ndef __init__(self, mag, rake, tectonic_region_type, hypocenter,\nsurface, rupture_slip_direction=None, weight=None):\nif not mag > 0:\nraise ValueError('magnitude must be positive')\nNodalPlane.check_rake(rake)\nself.tectonic_region_type = tectonic_region_type\nself.rake = rake\nself.mag = mag\nself.hypocenter = hypocenter\nself.surface = surface\nself.rupture_slip_direction = rupture_slip_direction\nself.weight = weight\n\n@property\ndef code(self):\n\"\"\"Returns the code (integer in the range 0 .. 255) of the rupture\"\"\"\nreturn self._code[self.__class__, self.surface.__class__]\n\nget_probability_no_exceedance = (\ncontexts.RuptureContext.get_probability_no_exceedance)\n\n[docs] def sample_number_of_occurrences(self, n=1):\n\"\"\"\nRandomly sample number of occurrences from temporal occurrence model\nprobability distribution.\n\n.. note::\nThis method is using random numbers. In order to reproduce the\nsame results numpy random numbers generator needs to be seeded, see\nhttp://docs.scipy.org/doc/numpy/reference/generated/numpy.random.seed.html\n\n:returns:\nnumpy array of size n with number of rupture occurrences\n\"\"\"\nraise NotImplementedError\n\n[docs]class NonParametricProbabilisticRupture(BaseRupture):\n\"\"\"\nProbabilistic rupture for which the probability distribution for rupture\noccurrence is described through a generic probability mass function.\n\n:param pmf:\nInstance of :class:`openquake.hazardlib.pmf.PMF`. Values in the\nabscissae represent number of rupture occurrences (in increasing order,\nstaring from 0) and values in the ordinates represent associated\nprobabilities. Example: if, for a given time span, a rupture has\nprobability ``0.8`` to not occurr, ``0.15`` to occur once, and\n``0.05`` to occur twice, the ``pmf`` can be defined as ::\n\npmf = PMF([(0.8, 0), (0.15, 1), 0.05, 2)])\n\n:raises ValueError:\nIf number of ruptures in ``pmf`` do not start from 0, are not defined\nin increasing order, and if they are not defined with unit step\n\"\"\"\ndef __init__(self, mag, rake, tectonic_region_type, hypocenter, surface,\npmf, rupture_slip_direction=None, weight=None):\nocc = numpy.array([occ for (prob, occ) in pmf.data])\nif not occ == 0:\nraise ValueError('minimum number of ruptures must be zero')\nif not numpy.all(numpy.sort(occ) == occ):\nraise ValueError(\n'numbers of ruptures must be defined in increasing order')\nif not numpy.all(numpy.diff(occ) == 1):\nraise ValueError(\n'numbers of ruptures must be defined with unit step')\nsuper().__init__(\nmag, rake, tectonic_region_type, hypocenter, surface,\nrupture_slip_direction, weight)\n# an array of probabilities with sum 1\nself.probs_occur = numpy.array([prob for (prob, occ) in pmf.data])\nself.occurrence_rate = numpy.nan\n\n[docs] def sample_number_of_occurrences(self, n=1):\n\"\"\"\nSee :meth:`superclass method\n<.rupture.BaseRupture.sample_number_of_occurrences>`\nfor spec of input and result values.\n\nUses 'Inverse Transform Sampling' method.\n\"\"\"\n# compute cdf from pmf\ncdf = numpy.cumsum(self.probs_occur)\nn_occ = numpy.digitize(numpy.random.random(n), cdf)\nreturn n_occ\n\n[docs]class ParametricProbabilisticRupture(BaseRupture):\n\"\"\"\n:class:`Rupture` associated with an occurrence rate and a temporal\noccurrence model.\n\n:param occurrence_rate:\nNumber of times rupture happens per year.\n:param temporal_occurrence_model:\nTemporal occurrence model assigned for this rupture. Should\nbe an instance of :class:`openquake.hazardlib.tom.PoissonTOM`.\n\n:raises ValueError:\nIf occurrence rate is not positive.\n\"\"\"\ndef __init__(self, mag, rake, tectonic_region_type, hypocenter, surface,\noccurrence_rate, temporal_occurrence_model,\nrupture_slip_direction=None):\nif not occurrence_rate > 0:\nraise ValueError('occurrence rate must be positive')\nsuper().__init__(\nmag, rake, tectonic_region_type, hypocenter, surface,\nrupture_slip_direction)\nself.temporal_occurrence_model = temporal_occurrence_model\nself.occurrence_rate = occurrence_rate\n\n[docs] def get_probability_one_or_more_occurrences(self):\n\"\"\"\nReturn the probability of this rupture to occur one or more times.\n\nUses\n:meth:`~openquake.hazardlib.tom.PoissonTOM.get_probability_one_or_more_occurrences`\nof an assigned temporal occurrence model.\n\"\"\"\ntom = self.temporal_occurrence_model\nrate = self.occurrence_rate\n\n[docs] def get_probability_one_occurrence(self):\n\"\"\"\nReturn the probability of this rupture to occur exactly one time.\n\nUses :meth:\n`openquake.hazardlib.tom.PoissonTOM.get_probability_n_occurrences`\nof an assigned temporal occurrence model.\n\"\"\"\ntom = self.temporal_occurrence_model\nrate = self.occurrence_rate\n\n[docs] def sample_number_of_occurrences(self, n=1):\n\"\"\"\nDraw a random sample from the distribution and return a number\nof events to occur as an array of integers of size n.\n\nUses :meth:\n`openquake.hazardlib.tom.PoissonTOM.sample_number_of_occurrences`\nof an assigned temporal occurrence model.\n\"\"\"\nr = self.occurrence_rate * self.temporal_occurrence_model.time_span\nreturn numpy.random.poisson(r, n)\n\n[docs] def get_probability_no_exceedance(self, poes):\n\"\"\"\nSee :meth:`superclass method\n<.rupture.BaseRupture.get_probability_no_exceedance>`\nfor spec of input and result values.\n\nUses\n:meth:`openquake.hazardlib.tom.PoissonTOM.get_probability_no_exceedance`\n\"\"\"\ntom = self.temporal_occurrence_model\nrate = self.occurrence_rate\n\n[docs] def get_dppvalue(self, site):\n\"\"\"\nGet the directivity prediction value, DPP at\na given site as described in Spudich et al. (2013).\n\n:param site:\n:class:`~openquake.hazardlib.geo.point.Point` object\nrepresenting the location of the target site\n:returns:\nA float number, directivity prediction value (DPP).\n\"\"\"\n\norigin = self.surface.get_resampled_top_edge()\ndpp_multi = []\nindex_patch = self.surface.hypocentre_patch_index(\nself.hypocenter, self.surface.get_resampled_top_edge(),\nself.surface.mesh.depths, self.surface.mesh.depths[-1],\nself.surface.get_dip())\nidx_nxtp = True\nhypocenter = self.hypocenter\n\nwhile idx_nxtp:\n\n# E Plane Calculation\np0, p1, p2, p3 = self.surface.get_fault_patch_vertices(\nself.surface.get_resampled_top_edge(),\nself.surface.mesh.depths,\nself.surface.mesh.depths[-1],\nself.surface.get_dip(), index_patch=index_patch)\n\n[normal, dist_to_plane] = get_plane_equation(\np0, p1, p2, origin)\n\npp = projection_pp(site, normal, dist_to_plane, origin)\npd, e, idx_nxtp = directp(\np0, p1, p2, p3, hypocenter, origin, pp)\npd_geo = origin.point_at(\n(pd ** 2 + pd ** 2) ** 0.5, -pd,\nnumpy.degrees(math.atan2(pd, pd)))\n\n# determine the lower bound of E path value\nf1 = geodetic_distance(p0.longitude,\np0.latitude,\np1.longitude,\np1.latitude)\nf2 = geodetic_distance(p2.longitude,\np2.latitude,\np3.longitude,\np3.latitude)\n\nif f1 > f2:\nf = f1\nelse:\nf = f2\n\nfs, rd, r_hyp = average_s_rad(site, hypocenter, origin,\npp, normal, dist_to_plane, e, p0,\np1, self.rupture_slip_direction)\ncprime = isochone_ratio(e, rd, r_hyp)\n\ndpp_exp = cprime * numpy.maximum(e, 0.1 * f) *\\\nnumpy.maximum(fs, 0.2)\ndpp_multi.append(dpp_exp)\n\n# check if go through the next patch of the fault\nindex_patch = index_patch + 1\n\nif (len(self.surface.get_resampled_top_edge())\n<= 2) and (index_patch >=\nlen(self.surface.get_resampled_top_edge())):\n\nidx_nxtp = False\nelif index_patch >= len(self.surface.get_resampled_top_edge()):\nidx_nxtp = False\nelif idx_nxtp:\nhypocenter = pd_geo\nidx_nxtp = True\n\n# calculate DPP value of the site.\ndpp = numpy.log(numpy.sum(dpp_multi))\n\nreturn dpp\n\n[docs] def get_cdppvalue(self, target, buf=1.0, delta=0.01, space=2.):\n\"\"\"\nGet the directivity prediction value, centered DPP(cdpp) at\na given site as described in Spudich et al. (2013), and this cdpp is\nused in Chiou and Young (2014) GMPE for near-fault directivity\nterm prediction.\n\n:param target_site:\nA mesh object representing the location of the target sites.\n:param buf:\nA buffer distance in km to extend the mesh borders\n:param delta:\nThe distance between two adjacent points in the mesh\n:param space:\nThe tolerance for the distance of the sites (default 2 km)\n:returns:\nThe centered directivity prediction value of Chiou and Young\n\"\"\"\nmin_lon, max_lon, max_lat, min_lat = self.surface.get_bounding_box()\nmin_lon -= buf\nmax_lon += buf\nmin_lat -= buf\nmax_lat += buf\n\nlons = numpy.arange(min_lon, max_lon + delta, delta)\n# ex shape (233,)\nlats = numpy.arange(min_lat, max_lat + delta, delta)\n# ex shape (204,)\nmesh = RectangularMesh(*numpy.meshgrid(lons, lats))\nmesh_rup = self.surface.get_min_distance(mesh).reshape(mesh.shape)\n# ex shape (204, 233)\n\ntarget_rup = self.surface.get_min_distance(target)\n# ex shape (2,)\ncdpp = numpy.zeros_like(target.lons)\nfor i, (target_lon, target_lat) in enumerate(\nzip(target.lons, target.lats)):\n# indices around target_rup[i]\naround = (mesh_rup <= target_rup[i] + space) & (\nmesh_rup >= target_rup[i] - space)\ndpp_target = self.get_dppvalue(Point(target_lon, target_lat))\ndpp_mean = numpy.mean(\n[self.get_dppvalue(Point(lon, lat))\nfor lon, lat in zip(mesh.lons[around], mesh.lats[around])])\ncdpp[i] = dpp_target - dpp_mean\n\nreturn cdpp\n\n[docs]class PointSurface:\n\"\"\"\nA fake surface used in PointRuptures\n\"\"\"\ndef __init__(self, hypocenter):\nself.hypocenter = hypocenter\n\n[docs] def get_strike(self):\nreturn 0\n\n[docs] def get_dip(self):\nreturn 0\n\n[docs] def get_top_edge_depth(self):\nreturn self.hypocenter.depth\n\n[docs] def get_width(self):\nreturn 0\n\n[docs] def get_closest_points(self, mesh):\nreturn mesh\n\ndef __bool__(self):\nreturn False\n\n[docs]class PointRupture(ParametricProbabilisticRupture):\n\"\"\"\nA rupture coming from a far away PointSource, so that the finite\nsize effects can be neglected.\n\"\"\"\ndef __init__(self, mag, tectonic_region_type, hypocenter,\noccurrence_rate, temporal_occurrence_model):\nself.mag = mag\nself.rake = 0\nself.tectonic_region_type = tectonic_region_type\nself.hypocenter = hypocenter\nself.occurrence_rate = occurrence_rate\nself.temporal_occurrence_model = temporal_occurrence_model\nself.surface = PointSurface(hypocenter)\nself.weight = None # no mutex\n\n[docs]def get_geom(surface, is_from_fault_source, is_multi_surface,\nis_gridded_surface):\n\"\"\"\nThe following fields can be interpreted different ways,\ndepending on the value of `is_from_fault_source`. If\n`is_from_fault_source` is True, each of these fields should\ncontain a 2D numpy array (all of the same shape). Each triple\nof (lon, lat, depth) for a given index represents the node of\na rectangular mesh. If `is_from_fault_source` is False, each\nof these fields should contain a sequence (tuple, list, or\nnumpy array, for example) of 4 values. In order, the triples\nof (lon, lat, depth) represent top left, top right, bottom\nleft, and bottom right corners of the the rupture's planar\nsurface. Update: There is now a third case. If the rupture\noriginated from a characteristic fault source with a\nmulti-planar-surface geometry, `lons`, `lats`, and `depths`\nwill contain one or more sets of 4 points, similar to how\nplanar surface geometry is stored (see above).\n\n:param surface: a Surface instance\n:param is_from_fault_source: a boolean\n:param is_multi_surface: a boolean\n\"\"\"\nif is_from_fault_source:\n# for simple and complex fault sources,\n# rupture surface geometry is represented by a mesh\nsurf_mesh = surface.mesh\nlons = surf_mesh.lons\nlats = surf_mesh.lats\ndepths = surf_mesh.depths\nelse:\nif is_multi_surface:\n# `list` of\n# openquake.hazardlib.geo.surface.planar.PlanarSurface\n# objects:\nsurfaces = surface.surfaces\n\n# lons, lats, and depths are arrays with len == 4*N,\n# where N is the number of surfaces in the\n# multisurface for each `corner_*`, the ordering is:\n# - top left\n# - top right\n# - bottom left\n# - bottom right\nlons = numpy.concatenate([x.corner_lons for x in surfaces])\nlats = numpy.concatenate([x.corner_lats for x in surfaces])\ndepths = numpy.concatenate([x.corner_depths for x in surfaces])\nelif is_gridded_surface:\n# the surface mesh has shape (1, N)\nlons = surface.mesh.lons\nlats = surface.mesh.lats\ndepths = surface.mesh.depths\nelse:\n# For area or point source,\n# rupture geometry is represented by a planar surface,\n# defined by 3D corner points\nlons = numpy.zeros((4))\nlats = numpy.zeros((4))\ndepths = numpy.zeros((4))\n\n# NOTE: It is important to maintain the order of these\n# corner points. TODO: check the ordering\nfor i, corner in enumerate((surface.top_left,\nsurface.top_right,\nsurface.bottom_left,\nsurface.bottom_right)):\nlons[i] = corner.longitude\nlats[i] = corner.latitude\ndepths[i] = corner.depth\nreturn lons, lats, depths\n\n[docs]class ExportedRupture(object):\n\"\"\"\nSimplified Rupture class with attributes rupid, events_by_ses, indices\nand others, used in export.\n\n:param rupid: rupture rup_id ID\n:param events_by_ses: dictionary ses_idx -> event records\n:param indices: site indices\n\"\"\"\ndef __init__(self, rupid, n_occ, events_by_ses, indices=None):\nself.rupid = rupid\nself.n_occ = n_occ\nself.events_by_ses = events_by_ses\nself.indices = indices\n\n[docs]def get_eids(rup_array, samples_by_grp, num_rlzs_by_grp):\n\"\"\"\n:param rup_array: a composite array with fields rup_id, n_occ and grp_id\n:param samples_by_grp: a dictionary grp_id -> samples\n:param num_rlzs_by_grp: a dictionary grp_id -> num_rlzs\n\"\"\"\nall_eids = []\nfor rup in rup_array:\ngrp_id = rup['grp_id']\nsamples = samples_by_grp[grp_id]\nnum_rlzs = num_rlzs_by_grp[grp_id]\nnum_events = rup['n_occ'] if samples > 1 else rup['n_occ'] * num_rlzs\neids = numpy.arange(num_events, dtype=U32)\nall_eids.append(eids)\nreturn numpy.concatenate(all_eids)\n\n[docs]class EBRupture(object):\n\"\"\"\nAn event based rupture. It is a wrapper over a hazardlib rupture\nobject, containing an array of site indices affected by the rupture,\nas well as the IDs of the corresponding seismic events.\n\"\"\"\ndef __init__(self, rupture, source_id, grp_id, n_occ, samples=1, id=None):\n# NB: when reading an exported ruptures.xml the rup_id will be 0\n# for the first rupture; it used to be the seed instead\nassert rupture.rup_id >= 0 # sanity check\nself.rupture = rupture\nself.source_id = source_id\nself.grp_id = grp_id\nself.n_occ = n_occ\nself.samples = samples\nself.id = id # id of the rupture on the DataStore, to be overridden\n\n@property\ndef rup_id(self):\n\"\"\"\nSerial number of the rupture\n\"\"\"\nreturn self.rupture.rup_id\n\n[docs] def get_eids_by_rlz(self, rlzs_by_gsim, offset=0):\n\"\"\"\n:params rlzs_by_gsim: a dictionary gsims -> rlzs array\n:param offset: offset used in the calculation of the event ID\n:returns: a dictionary rlz index -> eids array\n\"\"\"\nj = 0\ndic = {}\nif self.samples == 1: # full enumeration or akin to it\nfor rlzs in rlzs_by_gsim.values():\nfor rlz in rlzs:\ndic[rlz] = numpy.arange(\nj, j + self.n_occ, dtype=U32) + offset\nj += self.n_occ\nelse: # associated eids to the realizations\nrlzs = numpy.concatenate(list(rlzs_by_gsim.values()))\nhisto = general.random_histogram(\nself.n_occ, len(rlzs), self.rup_id)\nfor rlz, n in zip(rlzs, histo):\ndic[rlz] = numpy.arange(j, j + n, dtype=U32) + offset\nj += n\nreturn dic\n\n[docs] def get_eids(self, num_rlzs):\n\"\"\"\n:param num_rlzs: the number of realizations for the given group\n:returns: an array of event IDs\n\"\"\"\nnum_events = self.n_occ if self.samples > 1 else self.n_occ * num_rlzs\nreturn numpy.arange(num_events, dtype=U32)\n\n[docs] def export(self, events_by_ses):\n\"\"\"\nYield :class:`Rupture` objects, with all the\nattributes set, suitable for export in XML format.\n\"\"\"\nrupture = self.rupture\nnew = ExportedRupture(self.id, self.n_occ, events_by_ses)\nif isinstance(rupture.surface, geo.ComplexFaultSurface):\nnew.typology = 'complexFaultsurface'\nelif isinstance(rupture.surface, geo.SimpleFaultSurface):\nnew.typology = 'simpleFaultsurface'\nelif isinstance(rupture.surface, geo.GriddedSurface):\nnew.typology = 'griddedRupture'\nelif isinstance(rupture.surface, geo.MultiSurface):\nnew.typology = 'multiPlanesRupture'\nelse:\nnew.typology = 'singlePlaneRupture'\nnew.is_from_fault_source = iffs = isinstance(\nrupture.surface, (geo.ComplexFaultSurface,\ngeo.SimpleFaultSurface))\nnew.is_gridded_surface = igs = isinstance(\nrupture.surface, geo.GriddedSurface)\nnew.is_multi_surface = ims = isinstance(\nrupture.surface, geo.MultiSurface)\nnew.lons, new.lats, new.depths = get_geom(\nrupture.surface, iffs, ims, igs)\nnew.surface = rupture.surface\nnew.strike = rupture.surface.get_strike()\nnew.dip = rupture.surface.get_dip()\nnew.rake = rupture.rake\nnew.hypocenter = rupture.hypocenter\nnew.tectonic_region_type = rupture.tectonic_region_type\nnew.magnitude = new.mag = rupture.mag\nnew.top_left_corner = None if iffs or ims or igs else (\nnew.lons, new.lats, new.depths)\nnew.top_right_corner = None if iffs or ims or igs else (\nnew.lons, new.lats, new.depths)\nnew.bottom_left_corner = None if iffs or ims or igs else (\nnew.lons, new.lats, new.depths)\nnew.bottom_right_corner = None if iffs or ims or igs else (\nnew.lons, new.lats, new.depths)\nreturn new\n\ndef __repr__(self):\nreturn '<%s %d[%d]>' % (\nself.__class__.__name__, self.rup_id, self.n_occ)\n\n[docs]class RuptureProxy(object):\n\"\"\"\nA proxy for a rupture record.\n\n:param rec: a record with the rupture parameters\n:param nsites: approx number of sites affected by the rupture\n:param samples: how many times the rupture is sampled\n\"\"\"\ndef __init__(self, rec, nsites=None, samples=1):\nself.rec = rec\nself.nsites = nsites\nself.samples = samples\n\n@property\ndef weight(self):\n\"\"\"\n:returns:\nheuristic weight for the underlying rupture, depending on the\nnumber of occurrences, number of samples and number of sites\n\"\"\"\nreturn self.samples * self['n_occ'] * (\n100 if self.nsites is None else max(self.nsites, 100))\n\ndef __getitem__(self, name):\nreturn self.rec[name]\n\n# NB: requires the .geom attribute to be set\n[docs] def to_ebr(self, trt, samples):\n\"\"\"\n:returns: EBRupture instance associated to the underlying rupture\n\"\"\"\n# not implemented: rupture_slip_direction\nrupture = _get_rupture(self.rec, self.geom, trt)\nebr = EBRupture(rupture, self.rec['source_id'], self.rec['grp_id'],\nself.rec['n_occ'], samples)\nebr.id = self.rec['id']\nebr.e0 = self.rec['e0']\nreturn ebr\n```" ]
[ null ]
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https://www.engageny.org/ccls-math/6g2
[ " 6.G.2 | EngageNY\n\n## CCLS - Math: 6.G.2\n\nCategory\nGeometry\nSub-Category\nSolve Real-World And Mathematical Problems Involving Area, Surface Area, And Volume.\nState Standard:\nFind the volume of a right rectangular prism with fractional edge lengths by packing it with unit cubes of the appropriate unit fraction edge lengths, and show that the volume is the same as would be found by multiplying the edge lengths of the prism. Apply the formulas V = l w h and V = b h to find volumes of right rectangular prisms with fractional edge lengths in the context of solving real-world and mathematical problems." ]
[ null ]
{"ft_lang_label":"__label__en","ft_lang_prob":0.86529523,"math_prob":0.98225546,"size":2336,"snap":"2019-35-2019-39","text_gpt3_token_len":457,"char_repetition_ratio":0.1590909,"word_repetition_ratio":0.07486631,"special_character_ratio":0.19905822,"punctuation_ratio":0.11386139,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9959988,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-08-20T09:37:22Z\",\"WARC-Record-ID\":\"<urn:uuid:d785fb74-46cd-4396-8d60-c8e7237a62a1>\",\"Content-Length\":\"66408\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:f9f03fa6-d40b-4a0b-bc05-0635f5a9acca>\",\"WARC-Concurrent-To\":\"<urn:uuid:ddc0ebdb-afd9-469e-8c3a-14ef885db524>\",\"WARC-IP-Address\":\"3.227.40.88\",\"WARC-Target-URI\":\"https://www.engageny.org/ccls-math/6g2\",\"WARC-Payload-Digest\":\"sha1:FSA7WULJXHVIFBPV37G2IWTJ743K43XC\",\"WARC-Block-Digest\":\"sha1:PMLWRKQFIVXY67NALO3HCAGDTBBUTLQ2\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-35/CC-MAIN-2019-35_segments_1566027315321.52_warc_CC-MAIN-20190820092326-20190820114326-00442.warc.gz\"}"}
https://studylib.net/doc/11723333/-ey-math-2270-exam-1
[ "# (ey Math 2270 Exam 1", null, "```Math 2270 Exam 1\n-\nUniversity of Utah\nFall 2012\nName:\n(ey\nThis is a 50 minute exam. Please show all your work, as a worked\nproblem is required for full points, and partial credit may be rewarded for\nsome work in the right direction.\n1. (15 points) Vector Basics\nFor the vectors\narrr( 1)\nb=f i)\n4J\n\\1)\n/1\nc=f 2\nanswer the following, or explain why the question does not make\nsense:\n(a) (3 points) 2a + 3c\ni(\n=\n(D\n(‘)f()\n1\ni)\n4)\narrf\nb=(\nii\n/1\nc=( 2\n1J\n(b) (3 points) aH\nl+I6\n(c) (2 points) What are the components of a unit vector in the same\ndirection as a?\n/\n/\n2\nc)\nN\ncD.\nN\n0\nQ\nII\n+\nH\nr\nT\n0\nI.\nII\nI’\nI\n2. (10 points) Matrix Basics\nFor the matrices\n(3 4 2\nA\n2\n1 1\nB=\n/2 1 5\n4 4 2\n1 02\n(\n1 1\n0 0\nanswer the following, or explain why the question does not make\nsense:\n(a) (3points)A+Crr\n(3\n-\nttj\n16oO\n4\ncDCC\nCDCN\nII\n(z\nC\nr\\rJ\n—\nC\nCj\nc)\n0\n0\n‘-Th\n1\nc’-\nLfl\n3. (15 points) Elimination Issues\n(a) (5 points) For what value of a in the system of equations below\ndoes elimination fail to produce a unique solution?\n3x + 2y\n6x + ay\n=\n=\nir\n11\n/c{\nJi1 (\na e\nC\n10\nb\nrc ie4\nj\n1\nru\nZ\n1/\n/ce;\nq\nh-\n/e\np\nO\nOy\n(b) (5 points) Given the determined value of a, for what value of b\nare there an infinite number of solutions?\nT\nb?o\n7(j\no Oy\na(ty1\ns\n(c) (5 points) For the determined values of a and b what are two dis\ntinct solutions?\n/\n0\ny\nThte\n/\nqfN/\no4t\n6\n(QL/J\n4. (20 points) Systems of Equations\nUse elementary row operations to convert the system of equations\n2r\n6r\n12x\n+\n+\n+\n3y +\n6y +\n9y\n—\n3z\n=\n12z\nz\n=\n3\n13\n2\ninto upper-triangular form, and then use back-substitution to solve\nfor the variables x, y, z. Be sure to show all your work.\n5\n(Rc\n1Q-/\n5\nL +\nt1\nZ\nY\n3\nfc(J3\nZ\\4Jy 3y\nLI\ny\n3\n-\nrc, /J\n(f or/\n7\nx\na)\n—c\n—QQ\nI\no&ccedil;\n—\n—\n—\n—\n—\n-\nc_J\n_\n,\nH\nC\na)\n—\n0\n——H\n_Lf\n—\na)\n-d\nco\nI\n----\n—\n11\nJZ\ncx-)\nc)\n&gt;&lt;\nct\n0)\nC\n0\nU\nJ —r\n0\nUN\nUi\nfl\n7. (10 points) Symmetric Products\nFor the matrix\n2 3\n4 0\n(a) (4 points) What is the transpose RT?\n(b) (4 points) What is the symmetric product RTR\n73\n1\nLC)\n30/\n(c) (2 points) Does RTR\n=\nRRT?\n/\nhe\n10\n```" ]
[ null, "https://s2.studylib.net/store/data/011723333_1-79e99dfeb322d406a71195248ecfbdd4-768x994.png", null ]
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https://chem.libretexts.org/Courses/BethuneCookman_University/B-CU%3A_CH-345_Quantitative_Analysis/Book%3A_Analytical_Chemistry_2.1_(Harvey)/03%3A__The_Vocabulary_of_Analytical_Chemistry/3.03%3A_Classifying_Analytical_Techniques
[ "# 3.3: Classifying Analytical Techniques\n\n$$\\newcommand{\\vecs}{\\overset { \\rightharpoonup} {\\mathbf{#1}} }$$ $$\\newcommand{\\vecd}{\\overset{-\\!-\\!\\rightharpoonup}{\\vphantom{a}\\smash {#1}}}$$$$\\newcommand{\\id}{\\mathrm{id}}$$ $$\\newcommand{\\Span}{\\mathrm{span}}$$ $$\\newcommand{\\kernel}{\\mathrm{null}\\,}$$ $$\\newcommand{\\range}{\\mathrm{range}\\,}$$ $$\\newcommand{\\RealPart}{\\mathrm{Re}}$$ $$\\newcommand{\\ImaginaryPart}{\\mathrm{Im}}$$ $$\\newcommand{\\Argument}{\\mathrm{Arg}}$$ $$\\newcommand{\\norm}{\\| #1 \\|}$$ $$\\newcommand{\\inner}{\\langle #1, #2 \\rangle}$$ $$\\newcommand{\\Span}{\\mathrm{span}}$$ $$\\newcommand{\\id}{\\mathrm{id}}$$ $$\\newcommand{\\Span}{\\mathrm{span}}$$ $$\\newcommand{\\kernel}{\\mathrm{null}\\,}$$ $$\\newcommand{\\range}{\\mathrm{range}\\,}$$ $$\\newcommand{\\RealPart}{\\mathrm{Re}}$$ $$\\newcommand{\\ImaginaryPart}{\\mathrm{Im}}$$ $$\\newcommand{\\Argument}{\\mathrm{Arg}}$$ $$\\newcommand{\\norm}{\\| #1 \\|}$$ $$\\newcommand{\\inner}{\\langle #1, #2 \\rangle}$$ $$\\newcommand{\\Span}{\\mathrm{span}}$$$$\\newcommand{\\AA}{\\unicode[.8,0]{x212B}}$$\n\nThe analysis of a sample generates a chemical or physical signal that is proportional to the amount of analyte in the sample. This signal may be anything we can measure, such as volume or absorbance. It is convenient to divide analytical techniques into two general classes based on whether the signal is proportional to the mass or moles of analyte, or is proportional to the analyte’s concentration\n\nConsider the two graduated cylinders in Figure $$\\PageIndex{1}$$, each of which contains a solution of 0.010 M Cu(NO3)2. Cylinder 1 contains 10 mL, or $$1.0 \\times 10^{-4}$$ moles of Cu2+, and cylinder 2 contains 20 mL, or $$2.0 \\times 10^{-4}$$ moles of Cu2+. If a technique responds to the absolute amount of analyte in the sample, then the signal due to the analyte SA\n\n$S_A = k_A n_A \\label{3.1}$\n\nwhere nA is the moles or grams of analyte in the sample, and kA is a proportionality constant. Because cylinder 2 contains twice as many moles of Cu2+ as cylinder 1, analyzing the contents of cylinder 2 gives a signal twice as large as that for cylinder 1.", null, "Figure $$\\PageIndex{1}$$: Two graduated cylinders, each containing 0.10 M Cu(NO3)2. Although the cylinders contain the same concentration of Cu2+, the cylinder on the left contains $$1.0 \\times 10^{-4}$$ mol Cu2+ and the cylinder on the right contains $$2.0 \\times 10^{-4}$$ mol Cu2+.\n\nA second class of analytical techniques are those that respond to the analyte’s concentration, CA\n\n$S_A = k_A C_A \\label{3.2}$\n\nSince the solutions in both cylinders have the same concentration of Cu2+, their analysis yields identical signals.\n\nA technique that responds to the absolute amount of analyte is a total analysis technique. Mass and volume are the most common signals for a total analysis technique, and the corresponding techniques are gravimetry (Chapter 8) and titrimetry (Chapter 9). With a few exceptions, the signal for a total analysis technique is the result of one or more chemical reactions, the stoichiometry of which determines the value of kA in equation \\ref{3.1}.\n\nHistorically, most early analytical methods used a total analysis technique. For this reason, total analysis techniques are often called “classical” techniques.\n\nSpectroscopy (Chapter 10) and electrochemistry (Chapter 11), in which an optical or an electrical signal is proportional to the relative amount of analyte in a sample, are examples of concentration techniques. The relationship between the signal and the analyte’s concentration is a theoretical function that depends on experimental conditions and the instrumentation used to measure the signal. For this reason the value of kA in equation \\ref{3.2} is determined experimentally.\n\nSince most concentration techniques rely on measuring an optical or electrical signal, they also are known as “instrumental” techniques.\n\nThis page titled 3.3: Classifying Analytical Techniques is shared under a CC BY-NC-SA 4.0 license and was authored, remixed, and/or curated by David Harvey." ]
[ null, "https://chem.libretexts.org/@api/deki/files/272990/GradCylindCropped.png", null ]
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https://www.calculatoratoz.com/en/depth-of-flow1-when-celerity-of-the-wave-is-given-calculator/Calc-19983
[ "🔍\n🔍\n\n## Credits\n\nNational Institute of Technology Karnataka (NITK), Surathkal\nRithik Agrawal has created this Calculator and 1000+ more calculators!\nMeerut Institute of Engineering and Technology (MIET), Meerut\nIshita Goyal has verified this Calculator and 1000+ more calculators!\n\n## Depth of flow1 when Celerity of the Wave is Given Solution\n\nSTEP 0: Pre-Calculation Summary\nFormula Used\ndepth1 = -((((Height*[g])/(Celerity of the Wave*Velocity_of the fluid at 1))-2)/(((Height*[g])/(Celerity of the Wave*Velocity_of the fluid at 1))*Depth of Point 2))\nh 1 = -((((h*[g])/(C*V1))-2)/(((h*[g])/(C*V1))*h 2))\nThis formula uses 1 Constants, 4 Variables\nConstants Used\n[g] - Gravitational acceleration on Earth Value Taken As 9.80665 Meter/Second²\nVariables Used\nHeight - Height is the distance between the lowest and highest points of a person standing upright. (Measured in Meter)\nCelerity of the Wave - Celerity of the Wave is the addition to the normal water velocity of the channels. (Measured in Meter per Second)\nVelocity_of the fluid at 1 - Velocity_of the fluid at 1 is defined as the velocity of the flowing liquid at a point 1 (Measured in Meter per Second)\nDepth of Point 2 - Depth of Point 2 is the depth of point below the free surface in a static mass of liquid. (Measured in Meter)\nSTEP 1: Convert Input(s) to Base Unit\nHeight: 12 Meter --> 12 Meter No Conversion Required\nCelerity of the Wave: 10 Meter per Second --> 10 Meter per Second No Conversion Required\nVelocity_of the fluid at 1: 10 Meter per Second --> 10 Meter per Second No Conversion Required\nDepth of Point 2: 15 Meter --> 15 Meter No Conversion Required\nSTEP 2: Evaluate Formula\nSubstituting Input Values in Formula\nh 1 = -((((h*[g])/(C*V1))-2)/(((h*[g])/(C*V1))*h 2)) --> -((((12*[g])/(10*10))-2)/(((12*[g])/(10*10))*15))\nEvaluating ... ...\nh 1 = 0.0466351347753254\nSTEP 3: Convert Result to Output's Unit\n0.0466351347753254 Meter --> No Conversion Required\nFINAL ANSWER\n0.0466351347753254 Meter <-- Depth of Point 1\n(Calculation completed in 00.047 seconds)\n\n## < 11 Other formulas that you can solve using the same Inputs\n\nVolume of a Conical Frustum\nvolume = (1/3)*pi*Height*(Radius 1^2+Radius 2^2+(Radius 1*Radius 2)) Go\nTotal Surface Area of a Cone\ntotal_surface_area = pi*Radius*(Radius+sqrt(Radius^2+Height^2)) Go\nLateral Surface Area of a Cone\nlateral_surface_area = pi*Radius*sqrt(Radius^2+Height^2) Go\nTotal Surface Area of a Cylinder\ntotal_surface_area = 2*pi*Radius*(Height+Radius) Go\nLateral Surface Area of a Cylinder\nlateral_surface_area = 2*pi*Radius*Height Go\nVolume of a Circular Cone\nvolume = (1/3)*pi*(Radius)^2*Height Go\nArea of a Trapezoid\narea = ((Base A+Base B)/2)*Height Go\nVolume of a Circular Cylinder\nvolume = pi*(Radius)^2*Height Go\nVolume of a Pyramid\nvolume = (1/3)*Side^2*Height Go\nArea of a Triangle when base and height are given\narea = 1/2*Base*Height Go\nArea of a Parallelogram when base and height are given\narea = Base*Height Go\n\n## < 7 Other formulas that calculate the same Output\n\nConjugate Depth y1 when Critical Depth is Given\ndepth1 = 0.5*Depth of Point 2*(-1+sqrt(1+(8*(critical depth*critical depth*critical depth))/(Depth of Point 2*Depth of Point 2*Depth of Point 2))) Go\nConjugate Depth y1 when Discharge per unit width of channel is Given\ndepth1 = 0.5*Depth of Point 2*(-1+sqrt(1+(8*(discharge per unit width ^2))/([g]*Depth of Point 2*Depth of Point 2*Depth of Point 2))) Go\nDepth of flow1 when Absolute velocity of the surge moving towards right is Given\ndepth1 = ((Absolute Velocity of the Issuing Jet-Velocity_of the fluid at 2)/(Absolute Velocity of the Issuing Jet-Velocity_of the fluid at 1))*Depth of Point 2 Go\nDepth of flow1 when Absolute velocity of the surge moving towards right is Given\ndepth1 = ((Absolute Velocity of the Issuing Jet+Velocity_of the fluid at 2)/(Absolute Velocity of the Issuing Jet+Velocity_of the fluid at 1))*Depth of Point 2 Go\nDepth of flow1 when Absolute velocity of the surge when the flow is completely stopped\ndepth1 = ((Absolute Velocity of the Issuing Jet)/(Absolute Velocity of the Issuing Jet-Velocity_of the fluid at 1))*Depth of Point 2 Go\nConjugate Depth y1 when Froude Number Fr1 is Given\ndepth1 = Depth of Point 2/(0.5*(-1+sqrt(1+(8*(Froude number^2))))) Go\nConjugate Depth y1 when Froude Number Fr2 is Given\ndepth1 = Depth of Point 2*(0.5*(-1+sqrt(1+(8*(Froude number^2))))) Go\n\n### Depth of flow1 when Celerity of the Wave is Given Formula\n\ndepth1 = -((((Height*[g])/(Celerity of the Wave*Velocity_of the fluid at 1))-2)/(((Height*[g])/(Celerity of the Wave*Velocity_of the fluid at 1))*Depth of Point 2))\nh 1 = -((((h*[g])/(C*V1))-2)/(((h*[g])/(C*V1))*h 2))\n\n## What is Depth of Flow ?\n\nNormal depth is the depth of flow in a channel or culvert when the slope of the water surface and channel bottom is the same and the water depth remains constant. ... Note: Flow at normal depth in culverts often presents the highest average velocities and shallowest depths at that flow.\n\n## How to Calculate Depth of flow1 when Celerity of the Wave is Given?\n\nDepth of flow1 when Celerity of the Wave is Given calculator uses depth1 = -((((Height*[g])/(Celerity of the Wave*Velocity_of the fluid at 1))-2)/(((Height*[g])/(Celerity of the Wave*Velocity_of the fluid at 1))*Depth of Point 2)) to calculate the Depth of Point 1, The Depth of flow1 when Celerity of the Wave is Given formula is defined as amount of water flowing in through the channel. Depth of Point 1 and is denoted by h 1 symbol.\n\nHow to calculate Depth of flow1 when Celerity of the Wave is Given using this online calculator? To use this online calculator for Depth of flow1 when Celerity of the Wave is Given, enter Height (h), Celerity of the Wave (C), Velocity_of the fluid at 1 (V1) and Depth of Point 2 (h 2) and hit the calculate button. Here is how the Depth of flow1 when Celerity of the Wave is Given calculation can be explained with given input values -> 0.046635 = -((((12*[g])/(10*10))-2)/(((12*[g])/(10*10))*15)).\n\n### FAQ\n\nWhat is Depth of flow1 when Celerity of the Wave is Given?\nThe Depth of flow1 when Celerity of the Wave is Given formula is defined as amount of water flowing in through the channel and is represented as h 1 = -((((h*[g])/(C*V1))-2)/(((h*[g])/(C*V1))*h 2)) or depth1 = -((((Height*[g])/(Celerity of the Wave*Velocity_of the fluid at 1))-2)/(((Height*[g])/(Celerity of the Wave*Velocity_of the fluid at 1))*Depth of Point 2)). Height is the distance between the lowest and highest points of a person standing upright, Celerity of the Wave is the addition to the normal water velocity of the channels. , Velocity_of the fluid at 1 is defined as the velocity of the flowing liquid at a point 1 and Depth of Point 2 is the depth of point below the free surface in a static mass of liquid.\nHow to calculate Depth of flow1 when Celerity of the Wave is Given?\nThe Depth of flow1 when Celerity of the Wave is Given formula is defined as amount of water flowing in through the channel is calculated using depth1 = -((((Height*[g])/(Celerity of the Wave*Velocity_of the fluid at 1))-2)/(((Height*[g])/(Celerity of the Wave*Velocity_of the fluid at 1))*Depth of Point 2)). To calculate Depth of flow1 when Celerity of the Wave is Given, you need Height (h), Celerity of the Wave (C), Velocity_of the fluid at 1 (V1) and Depth of Point 2 (h 2). With our tool, you need to enter the respective value for Height, Celerity of the Wave, Velocity_of the fluid at 1 and Depth of Point 2 and hit the calculate button. You can also select the units (if any) for Input(s) and the Output as well.\nHow many ways are there to calculate Depth of Point 1?\nIn this formula, Depth of Point 1 uses Height, Celerity of the Wave, Velocity_of the fluid at 1 and Depth of Point 2. We can use 7 other way(s) to calculate the same, which is/are as follows -\n• depth1 = 0.5*Depth of Point 2*(-1+sqrt(1+(8*(discharge per unit width ^2))/([g]*Depth of Point 2*Depth of Point 2*Depth of Point 2)))\n• depth1 = 0.5*Depth of Point 2*(-1+sqrt(1+(8*(critical depth*critical depth*critical depth))/(Depth of Point 2*Depth of Point 2*Depth of Point 2)))\n• depth1 = Depth of Point 2/(0.5*(-1+sqrt(1+(8*(Froude number^2)))))\n• depth1 = Depth of Point 2*(0.5*(-1+sqrt(1+(8*(Froude number^2)))))\n• depth1 = ((Absolute Velocity of the Issuing Jet-Velocity_of the fluid at 2)/(Absolute Velocity of the Issuing Jet-Velocity_of the fluid at 1))*Depth of Point 2\n• depth1 = ((Absolute Velocity of the Issuing Jet+Velocity_of the fluid at 2)/(Absolute Velocity of the Issuing Jet+Velocity_of the fluid at 1))*Depth of Point 2\n• depth1 = ((Absolute Velocity of the Issuing Jet)/(Absolute Velocity of the Issuing Jet-Velocity_of the fluid at 1))*Depth of Point 2", null, "Let Others Know\nLinkedIn\nEmail\nWhatsApp\nCopied!" ]
[ null, "https://www.calculatoratoz.com/Images/share.png", null ]
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https://crypto.stackexchange.com/questions/35306/why-is-a-one-time-mac-secure-for-mac-then-encrypt-with-randomized-ctr-but-not-ra
[ "# Why is a one-time MAC secure for MAC-then-encrypt with randomized-CTR but not randomized-CBC?\n\nThe Coursera cryptography 1 course says:\n\nIf you want to use MAC-then-encrypt mode then you should either use randomized-CTR or randomized-CBC. And if you use randomized-CTR then one-time-MAC is sufficient.\n\nHere is the slide:", null, "I have two question regarding this:\n\n1. How we can use one-time-MAC without negotiating the different keys for each message?\n2. What is wrong with randomized-CBC that doesn't allow us to use with one-time-MAC?\n\n1. How can we use one-time-MAC without negotiating the different keys for each message?\n\nIf you use a universal hashing one-time MAC, and you encrypt it with CTR mode, effectively you are creating a Carter–Wegman–Shoup MAC:\n\n• Carter and Wegman showed that if $$r, s_0, s_1, \\dots$$ are independent uniform random and $$H_r$$ is a universal hash with bounded difference probability $$\\Pr[H_r(x) - H_r(y) = \\delta] < \\varepsilon$$ for all $$x \\ne y$$ and $$\\delta$$, then the forgery probability for the authenticator $$m_i \\mapsto H_r(m_i) + s_i$$ is bounded by $$\\varepsilon$$.\n\n• Shoup suggested deriving $$s_i = E_k(i)$$ for a block cipher $$E$$, which is essentially what you get with MAC-then-encrypt in CTR mode. Since $$E_k$$ is a permutation you run up against the birthday bound, of course, just like any use of a block cipher in CTR mode.\n\n1. What is wrong with randomized-CBC that doesn't allow us to use with one-time MAC?\n\nOffhand, I am not sure! If the one-time MAC is a universal hash with bounded collision probability $$\\Pr[H_r(x) = H_r(y)] < \\varepsilon$$ for all $$x \\ne y$$, then this intuitively sounds like it ought to be a secure construction, because $$m \\mapsto F_k(H_r(m))$$ is a secure long-input, short-output PRF if $$F_k$$ is a secure short-input, short-output PRF and $$H_r$$ has bounded collision probability. That's not exactly the scenario we have here, because there is not one fixed family $$F_k$$—if we encrypt $$m \\mathbin \\| H_r(m)$$, we get $$E_k(\\mathit{iv} \\oplus m) \\mathbin\\| E_k(E_k(\\mathit{iv} \\oplus m) \\oplus H_r(m)),$$ so $$m$$ figures in twice, but it's pretty close, so intuitively it seems like this should be secure.\n\nOf course, it's not clear that the mere security of a one-time MAC—a bound on forgery probability after a single attempt—implies any of this even with CTR: I'm assuming bounds on collision or difference probabilities, specifically. Maybe you could ask Dan Boneh what he meant.\n\nThere is also a danger of padding oracles with CBC in MAC-then-encrypt or MAC-and-encrypt, because CBC works on sequences of blocks rather than sequences of bits, which is why it is hard to get right: practical realizations like TLS and SSH had mistakes for years that leaked plaintexts via padding oracles." ]
[ null, "https://i.stack.imgur.com/5G6OA.png", null ]
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https://0-bmcmedresmethodol-biomedcentral-com.brum.beds.ac.uk/articles/10.1186/1471-2288-10-48
[ "# A simulation study for comparing testing statistics in response-adaptive randomization\n\n## Abstract\n\n### Background\n\nResponse-adaptive randomizations are able to assign more patients in a comparative clinical trial to the tentatively better treatment. However, due to the adaptation in patient allocation, the samples to be compared are no longer independent. At large sample sizes, many asymptotic properties of test statistics derived for independent sample comparison are still applicable in adaptive randomization provided that the patient allocation ratio converges to an appropriate target asymptotically. However, the small sample properties of commonly used test statistics in response-adaptive randomization are not fully studied.\n\n### Methods\n\nSimulations are systematically conducted to characterize the statistical properties of eight test statistics in six response-adaptive randomization methods at six allocation targets with sample sizes ranging from 20 to 200. Since adaptive randomization is usually not recommended for sample size less than 30, the present paper focuses on the case with a sample of 30 to give general recommendations with regard to test statistics for contingency tables in response-adaptive randomization at small sample sizes.\n\n### Results\n\nAmong all asymptotic test statistics, the Cook's correction to chi-square test (T MC ) is the best in attaining the nominal size of hypothesis test. The William's correction to log-likelihood ratio test (T ML ) gives slightly inflated type I error and higher power as compared with T MC , but it is more robust against the unbalance in patient allocation. T MC and T ML are usually the two test statistics with the highest power in different simulation scenarios. When focusing on T MC and T ML , the generalized drop-the-loser urn (GDL) and sequential estimation-adjusted urn (SEU) have the best ability to attain the correct size of hypothesis test respectively. Among all sequential methods that can target different allocation ratios, GDL has the lowest variation and the highest overall power at all allocation ratios. The performance of different adaptive randomization methods and test statistics also depends on allocation targets. At the limiting allocation ratio of drop-the-loser (DL) and randomized play-the-winner (RPW) urn, DL outperforms all other methods including GDL. When comparing the power of test statistics in the same randomization method but at different allocation targets, the powers of log-likelihood-ratio, log-relative-risk, log-odds-ratio, Wald-type Z, and chi-square test statistics are maximized at their corresponding optimal allocation ratios for power. Except for the optimal allocation target for log-relative-risk, the other four optimal targets could assign more patients to the worse arm in some simulation scenarios. Another optimal allocation target, R RSIHR , proposed by Rosenberger and Sriram (Journal of Statistical Planning and Inference, 1997) is aimed at minimizing the number of failures at fixed power using Wald-type Z test statistics. Among allocation ratios that always assign more patients to the better treatment, R RSIHR usually has less variation in patient allocation, and the values of variation are consistent across all simulation scenarios. Additionally, the patient allocation at R RSIHR is not too extreme. Therefore, R RSIHR provides a good balance between assigning more patients to the better treatment and maintaining the overall power.\n\n### Conclusion\n\nThe Cook's correction to chi-square test and Williams' correction to log-likelihood-ratio test are generally recommended for hypothesis test in response-adaptive randomization, especially when sample sizes are small. The generalized drop-the-loser urn design is the recommended method for its good overall properties. Also recommended is the use of the R RSIHR allocation target.\n\n## Background\n\nThe response-adaptive randomization (RAR) in clinical trials is a class of flexible ways of assigning treatment to new patients sequentially based on available data. The RAR adjusts the allocation probabilities to reflect the interim results of the trial, thereby allowing patients to benefit from the interim knowledge as it accumulates in the trial. In practice, unequal allocation probabilities are generated based on the current assessment of treatment efficacy, which results in more patients being assigned to the treatment that is putatively superior.\n\nMany RAR designs have been proposed over the years . The two key issues extensively investigated are the evaluations of parameter estimations and hypothesis testing. Due to the dependency of assigning new patients based on observed data at that time, conventional estimates of treatment effect are often biased; therefore, efforts have been made to quantify and correct estimation bias [14, 15]. Recent theoretical works have been focused on solving problems encountered in practice, which includes delayed response, implementation for multi-arm trials, and incorporating covariates, etc. [1, 3, 11, 1618]. Many recent theoretical developments are summarized in . Additionally, in order to compare treatment efficacies through hypothesis testing, studies have been conducted on power comparisons and sample size calculations under the framework of adaptive randomization . However, most of the works are based on large sample sizes, and focus on asymptotic properties [4, 12, 22, 25, 26]. But these properties have not been fully studied with small sample sizes. The mathematical challenge imposed by correlated data makes it extremely difficult to derive exact solutions for finite samples. Up to now, only limited results on exact solutions have been available [15, 27], and computer simulation has to be relied upon when sample size is small [23, 24], which is often the case in early phase II trials.\n\nEach RAR design has its own objective, and there are both advantages and disadvantages associated with that objective. It is not our purpose to give a comprehensive assessment of different designs by comparing their advantages and disadvantages. Instead, the primary objective of the present study is to characterize the small sample properties of RAR based on a frequentist approach. In particular, we focus on comparing the performance of commonly used test statistics in RAR of two-arm comparative trials with a binary outcome. Due to the departure from normality caused by data correlation and the discrete nature of a binary outcome, hypothesis tests usually can not be controlled at any given levels of nominal significance. Thus, to make our simulation comparison more relevant, our assessment of hypothesis testing methods and RAR procedures is based on the calculation of both statistical power and the comparison to the nominal type I error rate. Several RAR methods studied in our simulations can assign patients according to a given allocation target, which may be optimal in terms of maximizing the power or minimizing the expected treatment failure. Therefore, we also compare the properties of test statistics at different optimal allocation targets.\n\nThe remaining parts of this paper are organized into 4 sections. In the Methods Section, we introduce the adaptive randomization procedures, the optimal allocation rates, and the test statistics used in the simulation. In the Results Section, we present the simulation results. We provide a discussion and final recommendations regarding the RAR methods and hypothesis tests in the Discussion and Conclusions Sections.\n\n## Methods\n\nIn the present section, we briefly describe the randomization methods, asymptotic hypothesis test statistics, and optimal patient allocation targets that are relevant to our simulations. More detailed information can be found in the corresponding references.\n\nThe RAR procedures investigated in the present study are randomized play-the-winner (RPW) [8, 10], drop-the-loser (DL) , sequential maximum likelihood estimation (SMLE) , doubly-adaptive biased coin [2, 3], sequential estimation-adjusted urn (SEU) , and generalized drop-the-loser (GDL) designs. RPW, DL, SEU and GDL are all urn models in the sense that treatment assignment for each patient can be obtained by sampling balls from an urn. In the usual clinical trial setting, an urn model consists of one urn with different types of balls that represent the different treatments under study. Patients are assigned to treatments by randomly selecting balls from the urn. Initially, the urn contains an equal number of balls for each of the treatment offered in the trial. With the progress of a clinical trial, certain rules are applied to update the contents of the urn in such a way that favors the selection of balls corresponding to the better treatment. For example, under the RPW design, the observation of a successful treatment response leads to the addition of a (>0) balls of the same type to the urn; a lack of success leads to the addition of b (>0) balls of the other type to the urn (a = b = 1 in our simulation). The limiting allocation rate of patients on treatment 1 is q 2/(q 1 + q 2), where q 1 = 1-p 1 and q 2 = 1-p 2 are failure rates, and p 1 and p 2 are success rates (or response rates) for treatments 1 and 2. In the DL model, patients are assigned to a treatment based on the type of ball that is drawn; however a treatment failure results in the removal of a treatment ball from the urn, and treatment successes are ignored. Due to the finite probabilities of extinction, immigration balls are added to the urn. If an immigration ball is drawn, an additional ball of each type is added. The sampling process is repeated until a treatment ball is drawn. The DL urn design has the same limiting allocation as the RPW urn, but less variability in patient allocation. Both SEU and GDL are urn models allowing fraction number of balls, and can target any allocation rate. For SEU method , if the limiting allocation of RPW urn is the target in a two-arm trial, then", null, "balls of type 2 and", null, "balls of type 1 are added to the urn following the allocation of the ith patient. Obviously, the response status of the ith patient is related to the contents of SEU urn only through the calculation of", null, "and", null, ". For a two-arm GDL urn model , when a treatment ball is drawn, a new patient is assigned accordingly, but the ball will not be returned to the urn. Depending on the response of the patient, the conditional average numbers of balls being added back to the urn are b 1 and b 2 for treatments 1 and 2, respectively. Therefore, the conditional average numbers of type 1 and type 2 balls being taken out of the urn can be defined as d 1 and d 2, where d 1 = 1-b 1 and d 2 = 1-b 2. Immigration balls are also present in a GDL urn. Whenever an immigration ball is drawn, a 1 and a 2 balls are added for treatments 1 and 2, respectively. Zhang et al have shown that the limiting allocation rate of patients on treatment 1 is", null, "(1)\n\nThe GDL urn becomes a DL urn when a 1 = 1, a 2 = 1, b 1 = p 1, and b 2 = p 2. Although GDL is a general method with different ways of implementation, a convenient approach is taken in our simulation. When a treatment ball is drawn, the ball is not returned, and no ball is added regardless of the response of the patient. When an immigration ball is drawn, 1 and 2 balls of type 1 and 2 are added, where C is a constant, and ρ 1 and ρ 2 are allocation targets on treatments 1 and 2, which are estimated sequentially using the maximum likelihood estimates (MLE) .\n\nThe SMLE and doubly-adaptive biased coin design (DBCD) methods can also target any allocation ratios, and SMLE can be implemented as a special case of DBCD method. In DBCD method, the probability of the (i+1)th patient being assigned to treatment 1 is calculated by", null, "(2)\n\nwhere r 1 = n 1 (i)/i and ρ(i) are the current allocation rate and estimated allocation rate on treatment 1 [2, 3]. The properties of the DBCD depend largely on the selection of g, which can be considered as a measuring function for the deviation from the allocation target. In the present study, we use the following function suggested by Hu and Zhang :", null, "(3)\n\nwhere α is a tuning parameter. When α approaches infinity, the DBCD becomes deterministic and the patients are assigned to the putatively better treatment with probability 1. When α equals to 0, the MLE of ρ becomes the allocation target, and the DBCD method is essentially the same as the SMLE design proposed by Melfi et al .\n\n### Hypothesis Tests for Two-Arm Comparative Trials\n\nIn two-arm comparative trials, the results of a binary outcome variable can be summarized in a 2 × 2 contingency table (Table 1). The following hypothesis test is often conducted to compare treatment efficacy:", null, "(4)\n\nNine test statistics for the hypothesis test in (4) are given in Table 2. When relative risk (q 1/q 2) and odds ratio (p 1 q 2/q 1 p 2) are used to quantify the differences between 2 treatment arms, the test statistics are log-relative-risk and log-odds-ratio, T Risk and T Odds , which are asymptotically distributed as chi-square distribution with one degree of freedom (", null, "). When simple difference is used to measure the treatment effect, the applicable test statistics are the Wald-type test statistic T Wald and the score-type test statistics T Chisq , where the variance of simple difference in response rates is evaluated at H 1 or H 0 respectively. Additionally, the test statistics based on the logarithm of likelihood ratio (T LLR ) can also be constructed. Besides the 5 commonly used test statistics mentioned above, four modified test statistics are also included in Table 2. T MO is a modified log-odds-ratio test proposed by Gart using the approximation of discrete distributions by their continuous analogues . As shown in Table 2, T MO is essentially a modification to T Odds by adding 0.5 to each cell of a 2 × 2 table. Similarly, Agresti and Caffo proposed a modification to T Wald by adding 1 to each cell of a contingency table , which results in the test statistic T MW in Table 2. T MC is the Cook's continuity correction to chi-square test statistics T Chisq . Williams provided a modification to log-likelihood-ratio test T LLR . The original test statistic T LLR is improved by multiplying a scale factor such that the null distribution of the new test statistic T ML has the same moments as the chi-square distribution.\n\nSince all test statistics in Table 2 are based on", null, ", they are asymptotically equivalent and any one of them can be used for large sample sizes. Meanwhile at small sample sizes, an exact test can be conducted if a model is specified for the data given in Table 1. For example, depending on the number of fixed margins predetermined for the design, one of the following three models can be applied :", null, "(5)", null, "(6)\n\nand", null, "(7)\n\nwhere h(r 1|n, n 1, r) represents the hypergeometric distribution of r 1, b(r|n, p) gives the binomial distribution of r under the null hypothesis of equal response rates (H 0: p 1 = p 2 = p), and b(n 1|n, ρ) denotes the binomial distributions of patients on arm 1 with an allocation ratio of ρ (ρ 1 = 0.5 for equal randomization). The p value of exact test can be calculated by maximizing the probability in (5), (6), or (7) over the two nuisance parameters, p and ρ. However, due to data dependency, none of the above three models are directly applicable in adaptive randomization. For example, the allocation ratio ρ in adaptive randomization is a random variable with unknown distribution, and the binomial distribution of n 1 assumed in model (7) is not valid even when the null hypothesis is true. Therefore, in adaptive randomization, unconditional exact tests are not available and asymptotic test statistics such as the ones in Table 2 are required for testing the hypothesis in (4).\n\n### Optimal Allocation Ratios\n\nThe SMLE, DBCD, SEU, and GDL methods can be utilized to allocate patients based on different allocation targets. The allocation targets simulated in the present study are summarized in Table 3, where R Risk , R Odds , R Wald , R Chisq , and R LLR are optimal allocation ratios maximizing the power of T Risk , T Odds , T Wald , T Chisq , and T LLR respectively, at fixed sample size. The derivation of T Risk , T Odds , T Wald , T Chisq , and T LLR can be found in [33, 34], which is equivalent to minimizing the variance of corresponding test statistic at a fixed total sample size, and consequently the power of that test statistic is maximized. R RSIHR is a recently proposed allocation target that minimizes the expected total number of failures among all trials with the same power [15, 33]. The general theoretical framework and the practical implementation of optimal allocation in k-arm trials with binary outcomes are discussed and demonstrated by Tymofyeyev et al , where the optimization can be conducted over different goals. In practice, the performance of the methodology depends on the chosen RAR procedure. The present simulation study only focuses on two-arm trials, with a goal of maximizing the power or minimizing the total number of failures.\n\n## Results\n\nSimulations are conducted at different total numbers of patients ranging from 20 to 200. To simplify the presentation, the results for trials with 30 patients are shown here. When patients are less than 30, adaptive randomization is generally not recommended. For sample size of 100 or larger, all methods yield similar properties in general. For all of the urn models, one ball for each treatment is consistently used as the initial contents of the urn. The number of immigration balls is 1 for both the DL and GDL urns. The tuning parameter of DBCD, α, is fixed at 0 or 2. When α is 0, it results in the SMLE method. The value of the constant C in GDL is 2, which is equivalent to adding 2 treatment balls on average when an immigration ball is drawn. All simulation results are calculated based on 10,000 replicates.\n\nFor the purpose of comparison, the true allocation rates are shown in Table 4, and the simulated results for allocation rates on arm 1 are shown in Table 5. Among all RAR methods, DBCD has the best ability to attain the true allocation target. The comparison between SMLE and DBCD shows that, the allocation becomes more unbalanced and the variation of DBCD decreases with increasing value of tuning exponent α. On the other hand, the patient allocation of SEU results in more balanced mean allocation between two arms with a much larger variation as compared with other RAR methods. The GDL has the lowest variation among the four sequential RAR methods. When R RPW (the same as R DL ) is the allocation target, DL urn method has the lowest variation in patient allocation, which is consistent with the fact that the lower bound of the estimate of Var(R RPW ) is attained by DL urn . The comparison among allocation targets shows that R LLR has the lowest variation in patient allocation, and the highest variation is usually found at R RPW or R Risk . However, R RPW and R Risk are usually the top two allocation targets that assign more patients to the better treatment. R Wald , R Odds , and RLLR assigns more patients to the worse arm in some simulation cases. Among the three allocation targets that assign more patients to the better treatment (R RSIHR , R Risk and R RPW ), R RSIHR has a stable and often the lowest variation in patient allocation.\n\nThe simulation results are obtained for five null cases and ten alternative cases, and Table 6 gives the summary by averaging the results over the five null cases and the ten alternative cases for a given RAR method and at a given allocation target. Detailed simulation results for each test statistic are shown in Tables 7, 8, 9, 10, 11, 12 with one table for each of the six allocation targets. To simplify the presentation, the results are shown only for the four modified test statistics T MW , T MO , T MC , T ML , and the log-relative-risk test statistic T Risk because they tend to have better performance than the four corresponding unmodified tests. The qualitative comparisons among test statistics, RAR methods, and allocation targets can be made based on the results in Table 6.\n\nAs shown in Table 6 (also see Tables 7, 8, 9, 10, 11, 12), the worst performance can be found in the results of T MO and T Risk , which are often conservative with less than nominal type I error rate. T MW is always slightly conservative across all simulation cases. Overall, T MC is the best in attaining the correct type I error rate. T ML , is slightly inflated as compared with chi-square test T MC . However, the simulation results not shown here indicate that T ML is very robust against the unbalance in patient allocation even when sample size is 20. The comparison between different RAR methods shows that the mean type I error of GDL and SEU can usually match the correct size of tests better than other methods when T MC and T ML are used respectively. The type I error of DBCD is usually the largest one, except at R Odds . The overall type I error of SEU is comparable with GDL.\n\nThe power comparison of different test statistics indicates that T Risk is the statistic with the highest power at R Risk but with a much inflated type I error. Except at R Risk , T MC or T ML is the one with the highest power. Usually, GDL has the highest power and SEU has the lowest power among all RAR methods. DBCD and SMLE have similar power, but DBCD is more powerful in most cases. At target R RPW , DL urn has the best statistical properties. On the average, the target with the lowest power achieved by test statistics is R Risk . The highest overall power can usually be achieved by test statistics at R RSIHR and R LLR , but R LLR has the disadvantage of assigning more patients to the worse treatment in some cases.\n\n## Discussion\n\nIn response-adaptive randomization, the assignment of a new patient depends on the treatment outcomes of patients previously enrolled in the trial. Delayed responses are often encountered in practice. Recently, the problem of delayed response in multi-arm generalized drop-the-loser urn and generalized Friedman's urn design is studied for both continuous and discontinuous outcomes [11, 16, 17, 36]. It is shown that, under reasonable assumption about the delay, the asymptotic properties of adaptive design are not affected by the delay. In the present study, the primary focus is the comparison between commonly used test statistics for 2 × 2 tables. Based on results not shown here, a less extreme allocation with higher variation would be expected when a random delay is assumed. It is assumed that the response status of each of the patients already in the trial is available before the allocation of a new patient in our simulations evaluation.\n\nThe RAR methods simulated in the present study are aimed at assigning patients to the better treatment with probabilities higher than what otherwise would be allowed by equal randomization. The price being paid is that the sample sizes on the two comparing arms are no longer fixed, and the adaptation in patient allocation can complicate the statistical inference at the end of the trial. The properties of test statistics will change when the patient allocation ratio changes in adaptive randomization. The power of test statistics shown in the present simulation study is obtained by averaging over trials with an unknown distribution of allocation ratios. As shown in our simulation results, a large deviation from the nominal significance level of the hypothesis test can be found even under the null hypothesis. Therefore, the practice of comparing asymptotic hypothesis testing methods based solely on statistical power under the alternative hypothesis is not recommended. It is important to compare adaptive randomization methods based on both the type I error rate and the statistical power, especially when the sample size is small.\n\nGeneral recommendations given in the result section are based on the aggregated results across different settings. Because the performance of different test statistics, RAR methods, and allocation target are closely related to each other, recommendations under a specific scenario can be found based on the detailed simulation results in Tables 7, 8, 9, 10, 11, 12.\n\nBased on simulation results, the Cook's correction to chi-square test statistic T MC and Williams' correction to log-likelihood-ratio test T ML are recommended to be used for hypothesis testing at the end of adaptive randomization. T MC has good ability to attain the correct significance levels, and is relatively robust against the change of RAR method or allocation target. T ML has more robust performance than T MC and has higher power, but its type I error is slightly inflated as compared with T MC . However, T ML attains more accurate type I error than T MC when the sample size is small. The original Wald-type Z test statistic T Wald , which is very sensitive to patient allocation and has inflated type I error, should be avoided at small sample sizes. On the other hand, T MW , the Argresti's correction to T Wald , and T MO the modified log-odds-ratio test are too conservative and under powered at small sample sizes.\n\nThe primary objective of current study is to compare test statistics. Since the recommended test statistics are T MC and T ML , the comparison between RAR methods and allocation targets are mainly based on these two selected test statistics. Among SMLE, DBCD, SEU, and GDL methods, GDL seems to be the best one due to its ability to attain the correct size of hypothesis test and comparatively higher overall power at most allocation targets. Therefore, GDL is the recommended RAR method. The sequential estimation-adjusted urn (SEU) method is comparable with GDL in controlling the type I error. However, SEU is often under powered, and the high variation in patient allocation makes it less useful in practice. The DBCD method with tuning exponent α equal to 2 is the best in targeting the true allocation ratio. When T MC is the test statistic, DBCD has slightly inflated type I error and slightly lower power as compared with GDL. Therefore, among values of α, the balances among controlling the type I error, obtaining higher power, and targeting a given allocation ratio can be reached when α is equal to 2. The simulation comparison of statistical power for different RAR methods also indicates that DL urn has the best statistical properties at R RPW , mainly due to its low variation in patient allocation.\n\nThe statistical characteristics of hypothesis tests and RAR methods also depend on allocation targets. At R Wald , R Odds , and R LLR targets, more patients could be assigned to the inferior treatment in certain parameter spaces. In contrast, R Risk , R RPW , and R RSIHR always assign more patients to the better treatment. However, due to the more extreme allocation of R Risk and R RPW , both power and type I error of R Risk and R RPW will suffer as compared with R RSIHR . On the other hand, the variation of patient allocation at R RISHR is relatively small with a stable value across all simulation scenarios. Additional, among all designs with similar power using Wald-type test statistic, R RSIHR allocation ration can achieve fewer failures in the whole trial. Therefore, R RSIHR is recommended among all the allocation targets in the present study.\n\nIn addition to the frequentist development on the response adaptive randomization, Bayesian decision theoretic methods has also been proposed in the context of bandit problem. The concept of \"patient horizon\" was brought up to include future patients to whom the current study results might be applied. The goal is to maximize the total number of success in patients enrolled in the study with or without including the patient horizon. More detailed exposition of Bayesian methods for response adaptive randomization is beyond the scope of this paper and interested readers should consult the original work on this topic .\n\n## Conclusion\n\nThe Cook's correction to chi-square test and Williams' correction to log-likelihood-ratio test are recommended for hypothesis test of RAR at small sample sizes. Among all the RAR methods compared, GDL method has better statistical properties in controlling type one error and maintaining high statistical power. The RSIHR allocation target provides a good balance between assigning more patients to the better treatment and maintaining a high overall power.\n\n## Abbreviations\n\nRAR:\n\nRPW:\n\nRandomized play-the-winner\n\nDL:\n\nDrop-the-loser\n\nDBCD:\n\nSMLE:\n\nSequential maximum likelihood estimation design\n\nSEU:\n\nGDL:\n\nGeneralized drop-the-loser urn\n\nRSIHR:\n\nOptimal allocation target minimizing total numbers of failure for Wald-type test statistics at fixed power\n\nMLE:\n\nMaximum likelihood estimate.\n\n## References\n\n1. 1.\n\nAndersen J, Faries D, Tamura R: A randomized play-the-winner design for multi-arm clinical trials. Communications in Statistics-Theory and Methods. 1994, 23: 309-323. 10.1080/03610929408831257.\n\n2. 2.\n\nEisele JR: The doubly adaptive biased coin design for sequential clinical trials. Journal of Statistical Planning and Inference. 1994, 38: 249-262. 10.1016/0378-3758(94)90038-8.\n\n3. 3.\n\nHu FF, Zhang LX: Asymptotic properties of doubly adaptive biased coin designs for multi-treatment clinical trials. Annals of Statistics. 2004, 32 (1): 268-301.\n\n4. 4.\n\nIvanova S, Rosenberger WF, Durham S, Flournoy N: A birth and death urn for randomized clinical trials: asymptotic methods. Sankhya: The Indian Journals of Statistics. 2000, 62 (B): 104-118.\n\n5. 5.\n\nLi W, Durham SD, Flournoy N: Randomized Pôlya urn. 1996 Proceedings of the Biopharmaceutical Section of the American Statistical Association: 1997; Alexandria: American Statistical Association. 1997, 166-170.\n\n6. 6.\n\nRosenberger WF, Stallard N, Ivanova A, Harper CN, Ricks ML: Optimal adaptive designs for binary response trials. Biometrics. 2001, 57: 909-913. 10.1111/j.0006-341X.2001.00909.x.\n\n7. 7.\n\nWei LJ: The generalized Polya's urn design for sequential medical trials. Annals of Statistics. 1979, 7: 291-296. 10.1214/aos/1176344614.\n\n8. 8.\n\nWei LJ, Durham SD: The randomized play-the-winner rule in medical trials. Journal of American Statistical Association. 1978, 85: 156-162. 10.2307/2289538.\n\n9. 9.\n\nYang Y, Zhu D: Randomized allocation with nonparametric estimation for a multi-armed bandit problem with covariates. Annals of Statistics. 2002, 30: 100-121. 10.1214/aos/1015362186.\n\n10. 10.\n\nZelen M: Play the winner rule and the controlled clinical trial. Journal of the American Statistical Association. 1969, 64: 131-146. 10.2307/2283724.\n\n11. 11.\n\nZhang LX, Chan WS, Cheung SH, Hu FF: A generalized drop-the-loser urn for clinical trials with delayed responses. Statistica Sinica. 2007, 17 (1): 387-409.\n\n12. 12.\n\nMelfi VF, Page C, Geraldes M: An adaptive randomized design with application to estimation. Canadian Journal of Statistics. 2001, 29 (1): 107-116. 10.2307/3316054.\n\n13. 13.\n\nZhang LX, Hu FF, Cheung SH: Asymptotic theorems of sequential estimation-adjusted urn models. Annals of Applied Probability. 2006, 16 (1): 340-369. 10.1214/105051605000000746.\n\n14. 14.\n\nCoad DS, Ivanova A: Bias calculations for adaptive urn designs. Sequential Analysis. 2001, 20 (3): 91-116. 10.1081/SQA-100106051.\n\n15. 15.\n\nRosenberger WF, Sriram TN: Estimation for an adapative allocation design. Journal of Statistical Planning and Inference. 1997, 59: 309-319. 10.1016/S0378-3758(96)00109-7.\n\n16. 16.\n\nBai ZD, Hu FF, Rosenberger WF: Asymptotic properties of adaptive designs for clinical trials with delayed response. Annals of Statistics. 2002, 30 (1): 122-139. 10.1214/aos/1015362187.\n\n17. 17.\n\nHu FF, Zhang LJ: Asymptotic normality of urn models for clinical trials with delayed response. Bernoulli. 2004, 10: 447-463. 10.3150/bj/1089206406.\n\n18. 18.\n\nRosenberger WF, Vidyashankar AN, Agarwal DK: Covariate-adjusted response-adaptive designs for binary response. Journal of Biopharmaceutical Statistics. 2001, 11: 227-236.\n\n19. 19.\n\nHu FF, Rosenberger WF: The Theory of Response-Adaptive Randomization in Clinical Trials. 2006, Hoboken, New Jersey: John Wiley & Sons, Inc.\n\n20. 20.\n\nHu FF, Rosenberger WF: Optimality, variability, power: evaluating response-adaptive randomization procedures for treatment comparisons. Journal of the American Statistical Association. 2003, 98 (463): 671-678. 10.1198/016214503000000576.\n\n21. 21.\n\nZhang LJ, Rosenberger WF: Response-adaptive randomization for clinical trials with continuous outcomes. Biometrics. 2006, 62 (2): 562-569. 10.1111/j.1541-0420.2005.00496.x.\n\n22. 22.\n\nHu FF, Rosenberger WF, Zhang LX: Asymptotically best response-adaptive randomization procedures. Journal of Statistical Planning and Inference. 2006, 136 (6): 1911-1922. 10.1016/j.jspi.2005.08.011.\n\n23. 23.\n\nMorgan CC, Coad DS: A comparison of adaptive allocation rules for group-sequential binary response clinical trials. Statistics in Medicine. 2007, 26 (9): 1937-1954. 10.1002/sim.2693.\n\n24. 24.\n\nGuimaraes P, Palesch Y: Power and sample size simulations for Randomized Play-the-Winner rules. Contemporary Clinical Trials. 2007, 28 (4): 487-499. 10.1016/j.cct.2007.01.006.\n\n25. 25.\n\nMatthews PC, Rosenberger WF: Variance in randomized play-the-winner clinical trials. Statistics & Probability Letters. 1997, 35: 233-240. 10.1016/S0167-7152(97)00018-7.\n\n26. 26.\n\nBai ZD, Hu FF: Asymptotics in randomized urn models. Annals of Applied Probability. 2005, 15 (1B): 914-940. 10.1214/105051604000000774.\n\n27. 27.\n\nMatthews PC, Rosenberger WF: Variance in randomized play-the-winner clinical trials. Statistics & Probability Letters. 1997, 35 (3): 233-240. 10.1016/S0167-7152(97)00018-7.\n\n28. 28.\n\nIvanova A: A play-the-winner-type urn design with reduced variability. Metrika. 2003, 58: 1-13.\n\n29. 29.\n\nGart JJ: Alternative analyses of contingency tables. Journal of Royal Statistical Society B. 1966, 28: 164-179.\n\n30. 30.\n\nAgresti A, Caffo B: Simple and effective confidence intervals for proportions and differences of proportions results from adding two successes and two failures. The American Statistician. 2000, 54 (4): 280-288. 10.2307/2685779.\n\n31. 31.\n\nWilliams SS: Improved likelihood ratio tests for complete contingency tables. Biometrika. 1976, 63: 33-37. 10.1093/biomet/63.1.33.\n\n32. 32.\n\nUpton GJG: A comparison of alternative tests for the 2 × 2 table comparative trial. Journal of Royal Statistical Society A. 1982, 145: 86-105. 10.2307/2981423.\n\n33. 33.\n\nRosenberger WF, Lachin JM: Randomization in Clinical Trials: Theory and Practice. 2002, New York: Wiley\n\n34. 34.\n\nJennison C, Turnbull BW: Group Sequential Methods with Applications to Clinical Trials. 2000, Boca Raton: Chapman & Hall/CRC\n\n35. 35.\n\nTymofyeyev Y, Rosenberger WF, Hu FF: Implementing optimal allocation in sequential binary response experiments. Journal of American Statistical Association. 2007, 102 (477): 224-234. 10.1198/016214506000000906.\n\n36. 36.\n\nSun RB, Cheung SH, Zhang LX: A generalized drop-the-loser rule for multi-treatment clinical trials. Journal of Statistical Planning and Inference. 2007, 137 (6): 2011-2023. 10.1016/j.jspi.2006.06.039.\n\n37. 37.\n\nBerry DA, Fristedt B: Bandit Problems. 1985, New York: Chapman and Hall\n\n38. 38.\n\nThompson WR: On the likelihood that one unknown probability exceeds another in the view of the evidence of the two samples. Biometrika. 1933, 25: 275-294.\n\n39. 39.\n\nBerry DA, Eick SG: Adaptive assignment versus balanced randomization in clinical trials: a decision analysis. Statistics in Medicine. 1995, 14: 231-246. 10.1002/sim.4780140302.\n\n40. 40.\n\nCheng Y, Berry DA: Optimal adaptive randomized designs for clinical trials. Biometrika. 2007, 94 (4): 673-689. 10.1093/biomet/asm049.\n\n### Pre-publication history\n\n1. The pre-publication history for this paper can be accessed here:http://0-www.biomedcentral.com.brum.beds.ac.uk/1471-2288/10/48/prepub\n\n## Acknowledgements\n\nThis work was supported in part by grants CA16672 from the National Cancer Institute and W81XWH-06-1-0303 and W81XWH-07-1-0306 from the Department of Defense. The authors thank Dr. Lunagomez for helpful discussions. The authors also thank Ms. Lee Ann Chastain for her help, which greatly improved the presentation of our study.\n\n## Author information\n\nCorrespondence to J Jack Lee.\n\n### Competing interests\n\nThe authors declare that they have no competing interests.\n\n### Authors' contributions\n\nXMG conducted the simulation part of the study. Both XMG and JJL participated in designing the study and writing the manuscript. All authors read and approved the final manuscript.\n\n## Authors’ original submitted files for images\n\nBelow are the links to the authors’ original submitted files for images.\n\n## Rights and permissions\n\nReprints and Permissions\n\nGu, X., Lee, J.J. A simulation study for comparing testing statistics in response-adaptive randomization. BMC Med Res Methodol 10, 48 (2010). https://0-doi-org.brum.beds.ac.uk/10.1186/1471-2288-10-48", null, "" ]
[ null, "https://media.springernature.com/full/springer-static/image/art%3A10.1186%2F1471-2288-10-48/MediaObjects/12874_2008_Article_451_IEq1_HTML.gif", null, "https://media.springernature.com/full/springer-static/image/art%3A10.1186%2F1471-2288-10-48/MediaObjects/12874_2008_Article_451_IEq2_HTML.gif", null, "https://media.springernature.com/full/springer-static/image/art%3A10.1186%2F1471-2288-10-48/MediaObjects/12874_2008_Article_451_IEq3_HTML.gif", null, "https://media.springernature.com/full/springer-static/image/art%3A10.1186%2F1471-2288-10-48/MediaObjects/12874_2008_Article_451_IEq4_HTML.gif", null, "https://media.springernature.com/full/springer-static/image/art%3A10.1186%2F1471-2288-10-48/MediaObjects/12874_2008_Article_451_Equ1_HTML.gif", null, "https://media.springernature.com/full/springer-static/image/art%3A10.1186%2F1471-2288-10-48/MediaObjects/12874_2008_Article_451_Equ2_HTML.gif", null, "https://media.springernature.com/full/springer-static/image/art%3A10.1186%2F1471-2288-10-48/MediaObjects/12874_2008_Article_451_Equ3_HTML.gif", null, "https://media.springernature.com/full/springer-static/image/art%3A10.1186%2F1471-2288-10-48/MediaObjects/12874_2008_Article_451_Equ4_HTML.gif", null, "https://media.springernature.com/full/springer-static/image/art%3A10.1186%2F1471-2288-10-48/MediaObjects/12874_2008_Article_451_IEq5_HTML.gif", null, "https://media.springernature.com/full/springer-static/image/art%3A10.1186%2F1471-2288-10-48/MediaObjects/12874_2008_Article_451_IEq5_HTML.gif", null, "https://media.springernature.com/full/springer-static/image/art%3A10.1186%2F1471-2288-10-48/MediaObjects/12874_2008_Article_451_Equ5_HTML.gif", null, "https://media.springernature.com/full/springer-static/image/art%3A10.1186%2F1471-2288-10-48/MediaObjects/12874_2008_Article_451_Equ6_HTML.gif", null, "https://media.springernature.com/full/springer-static/image/art%3A10.1186%2F1471-2288-10-48/MediaObjects/12874_2008_Article_451_Equ7_HTML.gif", null, "https://0-bmcmedresmethodol-biomedcentral-com.brum.beds.ac.uk/track/article/10.1186/1471-2288-10-48", null ]
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https://www.toppr.com/guides/maths/probability/
[ "", null, "# Probability\n\nDid you know the origins of Probability can be linked to gambling during the 17th century? The theory of probability may have been discovered to help gamblers, but now it assists so many of our everyday activities. The chances of your school team winning the tournament, the possibility of rain on a given day, the likelihood of your winning the lottery, are all applications of probability. Let us learn a few more interesting topics regarding probability.\n\nQ1. How can we calculate the probability?\n\nA1. We can calculate the probability of an event by dividing it by the numbers of possible outcomes. Furthermore, this gives us the probability of a single event occurring. E.g. To get an outcome of 3 on a dice we have to roll it. And the number of event is1 and total outcomes are 6.\n\nQ2. What re the basic rules of probability?\n\nA2. Five basic rules of probability are:\n\n• First Rule: The possibility of happening of an event lies between 0 and 1.\n• Second Rule: Sum of all probable possible outcomes is 1.\n• Third Rule: There is a probability that a certain event will not take place.\n• Fourth Rule: Difference between happening and non-happening of an event is an important one.\n• Fifth Rule: It says that P(A or B) = P(A) + P(B) – P(A and B).\n\nQ3. What are the three types of probability?\n\nA3. The three types of probability are: classical, relative, and subjective probability.\n\nQ4. Is probability applicable in real life?\n\nA4. Probability is the chance that something will occur, such as picking a piece of green candy from a bag, drawing an ace from a deck of card etc. Hence, there is probability everywhere we go so it is applicable in real-life.\n\nShare with friends\n\nNo thanks." ]
[ null, "https://www.facebook.com/tr", null ]
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https://bnewtech.com/numberlist/cube/8344-8330/
[ "# List of Cube Numbers From 8344 to 8330\n\n83443 = 580928771584\n83433 = 580719929607\n83423 = 580511137688\n83413 = 580302395821\n83403 = 580093704000\n83393 = 579885062219\n83383 = 579676470472\n83373 = 579467928753\n83363 = 579259437056\n83353 = 579050995375\n83343 = 578842603704\n83333 = 578634262037\n83323 = 578425970368\n83313 = 578217728691\n83303 = 578009537000\n\nYou can download/print the perfect cube numbers from 8344 - 8330 as pdf format.\n\nfrom to" ]
[ null ]
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https://www.w3resource.com/javascript/object-property-method/array-length.php
[ "", null, "# JavaScript length Property: Array Object\n\n## Description\n\nThe length property returns number elements of an array. The value of the length property is an integer and less than 232. The length property is also used to truncate an array. If the length property is set with a number which is greater than the original length then new elements are added to the end of the array. If the length property is set with a number which is less than the original length then excess elements at the end of the array are lost.\n\nVersion\n\nImplemented in JavaScript 1.1\n\nSyntax\n\narray.length\n\nExample:\n\nIn the following web document length property is used to get the number of elements of a given array.\n\nHTML Code\n\n``````<!DOCTYPE html>\n<html lang=\"en\">\n<meta charset=\"utf8\" />\n<title>JavaScript Array object-length Property example</title>\n<style type=\"text/css\">\nh1 {color:red}\n</style>\n<body>\n<h1>JavaScript Array Object : length Property</h1>\n<script src=\"array-length-example1.js\">\n</script>\n</body>\n</html>\n```\n```\n\nJS Code\n\n``````var myarray = new Array(\"Orange\", \"Apple\", \"Banana\", \"Cherry\", \"Mango\");\nvar newParagraph = document.createElement(\"p\");\nvar newText = document.createTextNode(\"The length of the array is : \"+myarray.length);\nnewParagraph.appendChild(newText);\ndocument.body.appendChild(newParagraph);\n```\n```\n\nView the example in the browser\n\nPractice the example above online\n\nJavaScript Array object-length Property example\n\nJavaScript input Property: Array Object\n\nTest your Programming skills with w3resource's quiz.\n\n\n\n## JavaScript: Tips of the Day\n\nReturns true if the given number is a power of 2, false otherwise\n\nExample:\n\n```const tips_isPowerOfTwo = n => !!n && (n & (n - 1)) == 0;\nconsole.log(tips_isPowerOfTwo(0));\nconsole.log(tips_isPowerOfTwo(4));\nconsole.log(tips_isPowerOfTwo(16));\n```\n\nOutput:\n\n```false\ntrue\ntrue\n```" ]
[ null, "https://www.w3resource.com/images/w3resource-logo.png", null ]
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https://www.groundai.com/project/data-assimilation-and-parameter-estimation-for-a-multiscale-stochastic-system-with-alpha-stable-levy-noise/1
[ "Data assimilation and parameter estimation for a multiscale stochastic system with \\alpha-stable Lévy noise\n\n# Data assimilation and parameter estimation for a multiscale stochastic system with α-stable Lévy noise\n\nYanjie Zhang, Zhuan Cheng, Xinyong Zhang, Xiaoli Chen, Jinqiao Duan and Xiaofan Li Center for Mathematical Sciences & School of Mathematics and Statistics, Huazhong University of Science and Technology, Wuhan 430074, China Department of Applied Mathematics, Illinois Institute of Technology, Chicago, IL 60616, USA Department of Mathematical Sciences, Tsinghua University, Beijing 100084, China This work was partly supported by the NSF grant 1620449, and NSFC grants 11531006, 11371367, and 11271290.\n###### Abstract\n\nThis work is about low dimensional reduction for a slow-fast data assimilation system with non-Gaussian stable Lévy noise via stochastic averaging. When the observations are only available for slow components, we show that the averaged, low dimensional filter approximates the original filter, by examining the corresponding Zakai stochastic partial differential equations. Furthermore, we demonstrate that the low dimensional slow system approximates the slow dynamics of the original system, by examining parameter estimation and most probable paths.\n\nKeywords: Multiscale systems, non-Gaussian Lévy noise, averaging principle, Zakai equation, parameter estimation, most probable paths\n\n## 1 Introduction\n\nData assimilation is a procedure to extract system state information with the help of observations . The state evolution and the observations are usually under random fluctuations. The general idea is to gain the best estimate for the true system state, in terms of the probability distribution for the system state, given only some noisy observations of the system. It provides a recursive algorithm for estimating a signal or state of a random dynamical system based on noisy measurements. It is also very important in many practical applications from inertial guidance of aircrafts and spacecrafts to weather and climate prediction. Most of the existing works on data assimilation is conducted in the context of Gaussian random fluctuations. The effects of multiscale signal and observation processes in the context of Gaussian random fluctuations has been considered by Park et.al.(see ), and they have shown that the probability density of the original system converges to that of the reduced system, by a Fourier analysis method. Imkeller et.al. have further proved the convergence in distribution for the optimal filter, via backward stochastic differential equations and asymptotic techniques.\n\nHowever, random fluctuations are often non-Gaussian (in particular, Lévy type) in nonlinear systems, for example, in geosciences , and biosciences [3, 4, 5, 14, 15, 16, 32]. There are experimental demonstrations of Lévy fluctuations in optimal foraging theory, rapid geographical spread of emergent infectious disease and switching currents. Humphries et. al. used GPS to track the wandering black bowed albatrosses around an island in Southern Indian Ocean to study the movement patterns of searching food. They found that by fitting the data of the movement steps, the movement patterns obeys the power-law property with power parameter . La Cognata et. al. considered a Lotka-Volterra system of two competing species subject to multiplicative -stable Lévy noise, and analyzed the role of the Lévy noise sources. Lisowski et. al. studied a model of a stepping molecular motor consisting of two connected heads, and examined its dynamics as noise parameters varied. Speed and direction appear to very sensitively depend on characteristics of the noise. They explored the effect of noise on the ballistic graphene-based small Josephson junctions in the framework of the resistively and capacitively shunted model and found that the analysis of the switching current distribution made it possible to efficiently detect a non-Gaussian noise component in a Gaussian background.\n\nLévy motions are appropriate models for a class of important non-Gaussian processes with jumps or bursts [3, 4, 22]. It is desirable to consider data assimilation when the system evolution is under Lévy motions. This has been recently considered by one of us and other authors but not in the multiscale context (see [20, 28, 29, 35]).\n\nThe multi-scale stochastic dynamical systems arise widely in finance and biology. For example, there are two kinds of mutual securities in financial markets. One for the low-risk bonds, which can be characterized by ordinary differential equations; the other for high-risk stocks, whose price has two different changes. On the one hand, the edge change caused by the normal supply and demand can be characterized by Gaussian noise. On the other hand, due to the arrival of the important information of the stock, there will be a finite jump in the stock price. Such perturbations can be characterized by non-Gauss noise. In general, stock prices change at all times, while bond prices change for months or even years. Thus, the price of these two securities can be characterized by two-scales system with non-Gaussian noise (see ). Moreover, a large number of observations from biological experiments showed that the production of mRNA and proteins occur in a bursty, unpredictable, and intermittent manner, which create variation or “noise” in individual cells or cell-to-cell interactions. Such burst-like events appear to be appropriately modeled by the non-Gaussian noise. Since the mRNA synthesis process is faster than the protein dynamics, this leads to a two-time-scale system (see ). Here represents the ratio between the natural time scales of the protein and mRNA.\n\nParameter estimation for continuous time stochastic models is an increasingly important part of the overall modeling strategy in a wide variety of applications. It is quite often the case that the data to be fitted to a diffusion process has a multiscale character with Gaussian noise. One example is in molecular dynamics, where it is desirable to find effective models for low dimensional phenomena (such as conformational dynamics, vacancy diffusion and so forth) which are embedded within higher dimensional time-series. We are often interested in the parameter (see ), which represents the degradation or production rates of protein and mRNA. In this paper, we develop a parameter estimation method for multiscale diffusions with non-Gaussian noise. The results established here may be used to examine the change rate for low-risk bounds (see ).\n\nIn this present paper, we consider a slow-fast data assimilation system under Lévy noise, but only the slow component is observable. By averaging out the fast component via an invariant measure, we thus reduce the system dimension by focusing on the slow system evolution. We prove that the reduced lower dimensional filter effectively approximates (in probability distribution) the original filter. We demonstrate that a system parameter may be estimated via the low dimensional slow system, utilising only observations on the slow component. The accuracy for this estimation is quantified by -moment, with . We apply the stochastic Nelder-Mead method for optimization in the searching for the estimated parameter value. Furthermore, we illustrate the low dimensional approximation by comparing the most probable paths for the slow system and the original system. Finally, we make some remarks in Section 6.\n\nThis paper is organized as follows. After recalling some basic facts about Lévy motions and the generalized solution in the next section, we address the effects of the multiscale signal and observation processes in the context of Lévy random fluctuations in Section 3 to Section 5. We illustrate the low dimensional slow approximation by examining zakai equation, parameter estimation and most probable paths. Finally, we give some discussions and comments in a more biological context.\n\n## 2 Preliminaries\n\nWe recall some basic definitions for Lévy motions (or Lévy processes).\n\n###### Definition 1.\n\nA stochastic process is a Lévy process if\n\n1. (a.s.);\n\n2. has independent increments and stationary increments; and\n\n3. has stochastically continuous sample paths, i.e., for every , in probability, as .\n\nA Lévy process taking values in is characterized by a drift vector , an non-negative-definite, symmetric covariance matrix and a Borel measure defined on . We call the generating triplet of the Lévy motions . Moreover, we have the Lévy-Itô decomposition for as follows:\n\n Lt=bt+BQ(t)+∫||y||<1y˜N(t,dy)+∫||y||≥1yN(t,dy), (2.1)\n\nwhere is the Poisson random measure, is the compensated Poisson random measure, is the jump measure, and is an independent standard -dimensional Brownian motion. The characteristic function of is given by\n\n E[exp(i⟨u,Lt⟩)]=exp(tψ(u)),   u∈Rn, (2.2)\n\nwhere the function is the characteristic exponent\n\n ψ(u)=i⟨u,b⟩−12⟨u,Qu⟩+∫Rn∖{0}(ei⟨u,z⟩−1−i⟨u,z⟩I{||z||\\textless1})ν(dz). (2.3)\n\nThe Borel measure is called the jump measure. Here denotes the scalar product in .\n\n###### Definition 2.\n\nFor , an -dimensional symmetric -stable process is a Lévy process with characteristic exponent\n\n ψ(u)=−C1(n,α)|u|α, for u∈Rn (2.4)\n\nwith .\n\nFor an -dimensional symmetric -stable Lévy process, the diffusion matrix , the drift vector , and the Lévy measure is given by\n\n ν(du)=C2(n,α)||u||n+αdu, (2.5)\n\nwhere .\n\nFor every function , the generator for this symmetric -stable Lévy process in is\n\n (Aαϕ)(x)=∫Rn∖{0}[ϕ(x+u)−ϕ(x)]ν(du). (2.6)\n\nIt is known that extends uniquely to a self-adjoint operator in the domain. By Fourier inverse transform,\n\n Aαϕ=θα,n(−Δ)α/2ϕ(x), (2.7)\n\nwhere\n\n θα,n=∫Rn∖{0}(cos(⟨e,y⟩)−1)ν(du) (2.8)\n\nwith being the unit vector in .\n\nFor fix , and set\n\n ρ(x)=(1+|x|)η. (2.9)\n\nLet be the weighted -space with norm:\n\n ||f||p;ρ=(∫Rn|f(x)|pρ(x)dx)1p (2.10)\n\nFor , let be the -order weighted Sobolev space with norm\n\n ||f||l,p;ρ=l∑i=0||∇lf||p;ρ, (2.11)\n\n###### Definition 3.\n\nA backward predictable stochastic process is called a generalized solution of the equality\n\n v(t,x)=φ(x)+∫[t,T]Lv(s,x)ds+∫[t,T]hlv(s,x)dwl(s), (2.12)\n\nif for every it satisfies the following equation\n\n (v(t,x),y)=(φ,y)+∫[t,T](v(s,x),L∗y)ds+∫[t,T](hlv(s,x),y)dwl(s) (2.13)\n\nwith being the generator of some Lévy process.\n\n## 3 A slow-fast filtering system\n\nLet us consider the following slow-fast signal-observation system:\n\n dXt=f1(Xt,Yt)dt+g1(Xt,Yt)dB1t+σ1dLα11,x∈Rn, (3.14) dYt=ε−1f2(Xt,Yt)dt+ε−12g2(Xt,Yt)dB2t+1ε1α2dLα22,y∈Rm, (3.15) dZt=h(Xt)dt+dWt,z∈Rd. (3.16)\n\nHere is an -valued signal process which represents the slow and fast components. The constant represents the noise intensity for the slow variable. The observation process is -valued. The standard Brownian motions are independent. The non-Gaussian processes (with ) are independent symmetric -stable Lévy processes with triplets and , respectively. The parameter is the ratio of the slow time scale to the fast time scale. We make the following assumptions on this filtering system.\nHypothesis H.1. The functions satisfy the global Lipschitz conditions, i.e., there exists a positive constant such that\n\n ||f1(x1,y1)−f1(x2,y2)||2+||g1(x1,y1)−g1(x2,y2)||2+||f2(x1,y1)−f2(x2,y2)||2+||g2(x1,y1)−g2(x2,y2)||2≤γ[||x1−x2||2+||y1−y2||2]\n\nfor all\n\n###### Remark 1.\n\nNote that with the help of the global Lipschitz condition, it follows that there is a positive constant such that\n\n ||f1(x,y)||2+||g1(x,y)||2+||f2(x,y)||2+||g2(x,y)||2≤K(1+||x||2+||y||2)\n\nfor all .\n\nHypothesis H.2. The coefficients are of class with the first and second order derivatives bounded\n\nHypothesis H.3. The sensor function is of class , i.e. all the bounded continuous functions on .\n\nHypothesis H.4. There exists a positive constant , such that\n\n supx{Tr[g2(x,y)g2(x,y)T]+2⟨y,f2(x,y)⟩}≤−C(1+|y|2). (3.17)\n\nThis hypothesis (H.4.) ensures the existence of an invariant measure (see ) for the fast component . With the special scaling exponent for the fast component , this invariant measure is independent of (see [11, 12]).\n\nThe infinitesimal generator of the slow-fast stochastic system is\n\n L=L1+1εL2, (3.18)\n\nwhere\n\n ⎧⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪⎨⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪⎩L1Φ(x,y,t)=f1⋅∇xΦ(x,y,t)+12Tr[G1⋅Hx(Φ(x,y,t))]+P.V.∫Rn∖{0}(Φ(x+σ1z1,y,t)−Φ(x,y,t))ν1(dz1),L2Φ(x,y,t)=f2⋅∇yΦ(x,y,t)+12Tr[G2⋅Hy(Φ(x,y,t))]+P.V.∫Rm∖{0}(Φ(x,y+z2,t)−Φ(x,y,t))ν2(dz2). (3.19)\n\nHere , is the gradient, and is the Hessian matrix (with respect to and respectively). Let\n\n Zt=σ(Zs:0≤s≤t)∨N, (3.20)\n\nwhere is the collection of all -negligible sets of . Define\n\n Z=⋁t∈R+Zt, (3.21)\n\nwhere denotes taking the -algebra generated by the union . That is,\n\n Z=σ(⋃tZt). (3.22)\n\nBy the version of Girsanov’s change of measure theorem, we obtain a new probability measure , such that the observation becomes -independent of the signal variables . This can be done through\n\n d~PdP=exp(−m∑i=1∫t0hi(Xs)dWis−12m∑i=1∫t0hi(Xs)2ds). (3.23)\n\nDenote\n\n ~Rt=dPd~P∣∣∣Zt. (3.24)\n\nThen by the Kallianpur-Striebel formula, for every bounded differentiable function , we have the following representation:\n\n E[ϕ(Xt,Yt)|Zt]=~E[~Rtϕ(Xt,Yt)|Zt]~E[~Rt|Zt]=~E[~Rtϕ(Xt,Yt)|Z]~E[~Rt|Z]. (3.25)\n\nThe unnormalized conditional distribution of , given , is defined as . Thus, we have the following Zakai equation:\n\n {dPt(ϕ)=Pt(Lϕ)dt+Pt(ϕhT)dZt,P0(ϕ)=E[ϕ(X0,Y0)]. (3.26)\n\nThe -marginal of is defined as\n\n ρt(ϕ)=∫Rn+mϕ(x)Pt(dx,dy). (3.27)\n\nNow we define a reduced, low dimensional signal-observation system\n\n {d¯Xt=¯f1(¯Xt)dt+¯g1(¯Xt)dB1t+σ1dLα11,d¯Zt=h(¯Xt)dt+dBt. (3.28)\n\nHere\n\n {¯f1(x)=∫Rmf1(x,y)μx(dy),¯G(x)=∫Rmg1(x,y)g1(x,y)Tμx(dy). (3.29)\n\nThe unnormalized conditional distribution corresponding to the filter for the reduced system (3.28) satisfies the following (reduced) Zakai equation\n\n {d¯ρt(ϕ)=¯ρt(¯Lϕ)dt+¯ρt(ϕhT)d¯Zt,¯ρ0(ϕ)=E[ϕ(X0)], (3.30)\n\nwhere\n\n ¯Lϕ(x,t)=¯f1(x)⋅∇xϕ(x,t)+12Tr[Hx(¯G(x)ϕ(x,t))]+∫Rn(ϕ(x+σ1z1,t)−ϕ(x,t))ν1(dz1). (3.31)\n\nHowever, we are more interested in the reduced filtering problem with the actual observation . This leads us to rewrite the reduced Zakai equation (3.30) as follows:\n\n {d¯ρt(ϕ)=¯ρt(¯Lϕ)dt+¯ρt(ϕhT)dZt,¯ρ0(ϕ)=E[ϕ(X0)]. (3.32)\n###### Lemma 1.\n\nAssume that the following conditions are satisfied:\n\n1. The functions , and for and and their derivatives of first order (in x) as well as the derivatives of second order (in x) are uniformly bounded by the constant . The functions are locally uniformly bounded in .\n\n2. .\n\nLet be a generalized solution of problem\n\n ⎧⎪ ⎪⎨⎪ ⎪⎩du(t,x,ω)=Lu(t,x,ω)dt+hl(t,x,ω)u(t,x,ω)dBl(t),(t,x,ω)∈[T0,T]×Rk×Ω,u(T0,x,ω)=φ(x,ω),(x,ω)∈Rk×Ω, (3.33)\n\nwhere\n\n Lu(t,x)=12σik(t,x,ω)σjk(t,x,ω)∂2iju(t,x,ω)+bi∂iu(t,x,ω)+12∫Rk(u(t,x+z)+u(t,x−z)−2u(t,x))dz|z|k+α, (3.34)\n\nand is a generalized solution of problem\n\n (3.35)\n\nThen the following formulas hold\n\n u(t,x)=E(φ(Y(t,x,T0))χ1(t,T0)|FT0t), (3.36)\n\nand\n\n v(t,x)=E(φ(X(T,x,t))χ2(T,t)|FTt), (3.37)\n\nwhere is the forward stochastic differential equation with generator and is the backward stochastic differential equation with generator . Here and satisfy the following equations\n\n χ1(t,s)=exp(∫[s,t]hl(τ,Y(t,x,τ))dBl(τ)−12∫[s,t]hlhl(τ,Y(t,x,τ))dτ), (3.38)\n\nand\n\n χ2(s,t)=exp(∫[t,s]hl(τ,X(τ,x,t))dBl(τ)−12∫[t,s]hlhl(τ,X(τ,x,t))dτ). (3.39)\n###### Proof.\n\nDenote . Before we proceed to the proof of the lemma, let us consider the problem\n\n (3.40)\n\nBy the definition of a backward predictable stochastic process, the coefficients in equation (3.40) are predictable relative to the family of algebra with . The process is a Wiener martingale with respect to the same family and the initial condition is measurable with respect to the minimal -algebra of this family.\n\nLet be a generalized solution of problem. Then by the definition of generalized solution, for every , the following equality holds on ,\n\n (v(T−s,x),y)=(φ,y)+∫[0,T−s][−(aij(T−s)∂iv(s,x),yj)+(bi(T−s)−aijj(T−s))∂iv(s,x))+12∫Rk(v(s,x+z)+v(s,x−z)−2v(s,x))dz|z|k+α,y)]ds+∫[0,T−s]hl(T−t)v(t,x)dBlT(s). (3.41)\n\nDenote in equation (3.41), we find that satisfies the following equation on , for every .\n\n (u(t,x),y)=(φ,y)+∫[t,T][−(aij∂iv(s,x),yj)+((bi−aijj)∂iu(t,x))+12∫Rk(v(t,x+z)+v(t,x−z)−2v(t,x))dz|z|k+α,y)]ds+∫[t,T]hlv(s,x)dBl(s). (3.42)\n\nThus is an generalized solution of problem (3.35).\n\nOn the other hand, changing the variables in equality (3.42), we obtain that is a generalized solution of problem (3.40). Thus we have proved that problems (3.35) and (3.40) are equivalent. Therefore all the results obtained for problem (3.35) are naturally carried over to problem (3.40). For the problem (3.40), we can use the similar method to obtain the existence and uniqueness of - solution to stochastic fractal equations by using purely probabilistic argument (see [19, 30]). This completes the proof of this lemma. ∎\n\nNow we show that the reduced system approximates the original system, by examining the corresponding Zakai equations. Before describing the theorem, we start by describing the probabilistic representation for semi-linear stochastic fractal equations. We proceed to consider the probability measure . Note that the process is a Brownian motion under . For convenience, we rewrite and as and , respectively. By Lemma 1, we know solves a stochastic partial differential equation (SPDE).\n\n {−dvϕ(t,x,y)=Lvϕ(t,x,y)dt+h(x)Tvϕ(t,x,y)d←−Bt.vϕ(T,x,y)=ϕ(x). (3.43)\n\nHere denotes Itô’s backward integral. Likewise, we introduce , and then solves the following SPDE\n\n ⎧⎨⎩−d¯¯¯vϕ(t,x)=¯¯¯¯L¯¯¯vϕ(t,x)dt+h(x)T¯¯¯vϕ(t,x)d←−Bt,¯¯¯vϕ(T,x)=ϕ(x). (3.44)\n\nBy the version of Girsanov’s change of measure theorem and Markov property of , we know that for any : . In particular, we have\n\n ρT(ϕ)=∫vϕ(0,x,y)P(X0,Y0)(dx,dy). (3.45)\n\nSimilarly, we have\n\n ¯ρT(ϕ)=∫¯vϕ(0,x)P(X0)(dx). (3.46)\n\nThis is our main result on the comparison between the original filter and the reduced filter. This is desirable when only the slow component is observable.\n\n###### Theorem 1.\n\nUnder the hypotheses (H.1)-(H.4) and for with , there exists a positive constant such that for , the following estimate holds\n\n E[|ρT(ϕ)−¯ρT(ϕ)|p]≤Cε, (3.47)\n\nwith a positive constant independent of . This implies that the reduced filter approximates the original filter, as the scale parameter tends to zero.\n\n###### Proof.\n E[|ρT(ϕ)−¯ρT(ϕ)|p]=E[∣∣∫(vϕ(0,x,y)−¯vϕ(0,x))P(X0,Y0)(dx,dy)∣∣p],≤E[∫∥∥vϕ(0,x,y)−¯vϕ(0,x)∣∣pP(X0,Y0)(dx,dy)],=∫E[∣∣vϕ(0,x,y)−¯vϕ(0,x)∣∣p]P(X0,Y0)(dx,dy),=∫E[∣∣~Ex,y[ϕ(XT)~R0,T|Y0,T]−~Ex[ϕ(¯XT)~R0,T|Y0,T]∣∣p]P(X0,Y0)(dx,dy),≤C∫E∣∣~Ex[(ϕ(XT)−ϕ(¯XT))~R0,T|Yt,T]∣∣pP(X0,Y0)(dx,dy),=C∫E∣∣E[ϕ(XT)−ϕ(¯XT)|YT]~Ex[~R0,T|Y0,T]∣∣pP(X0,Y0)(dx,dy),≤C∫E∣∣E[XT−¯XT|YT]∣∣pP(X0,Y0)(dx,dy). (3.48)\n\nUsing the Jensen’s inequality, we have\n\n E[|ρT(ϕ)−¯ρT(ϕ)|p]≤∫E|XT−¯XT|pP(X0,Y0)(dx,dy). (3.49)\n\nApplying a similar argument from , we obtain\n\n limϵ→0E|XT−¯XT|p=0 (3.50)\n\nFinally, we conclude that\n\n E[|ρT(ϕ)−¯ρT(ϕ)|p]≤Cε. (3.51)\n\nThis completes the proof of Theorem 1. ∎\n\n## 4 Parameter estimation\n\nIn this section, we consider parameter estimation in the following slow-fast dynamical system\n\n (4.52)\n\nwhere is an matrix, is a positive definite matrix with eigenvalues . is an unknown parameter defined in an compact set of .\n\nHypothesis H.5. For all , the function is uniformly bounded and Lipschitz w.r.t x and y. The function is smooth with the first order derivatives bounded by .\n\nDefine an averaged, low dimensional slow stochastic dynamical system in (see ), as in the previous section\n\n d¯x(t)=A¯x(t)+¯f1(¯x(t),θ)dt, (4.53)\n\nwhere\n\n ¯f1(¯x,θ)≜∫Rmf1(x,y,θ)μx(dy).\n\nWe will estimate the unknown parameter , based on this low dimensional slow system (4.53) but using the observations on the slow component only. Denote the solution of the original slow-fast system (4.52) with actual parameter by , and the solution of the slow system (4.53) with parameter by . We recall the following lemma.\n\n###### Lemma 2.\n\nUnder hypothesis (H.6), the following strong convergence holds\n\n limε→0E|x(t,θ0)−¯x(t,θ0)|p=0, t∈[0,T] and p∈(1,α). (4.54)\n###### Proof.\n\nThe proof of average principle is similar the the infinite case which has been studied in , Thus we omit here. ∎\n\nWe take as the objective function and assume there is a unique such that . This is our estimated parameter value. Then we can state our main result as follows.\n\n###### Theorem 2.\n\nUnder hypothesis (H.6), the estimated parameter value converges to the true parameter value, as the scale parameter approaches zero. That is,\n\n limε→0^θϵ=θ0. (4.55)\n###### Proof.\n\nNote that\n\n E|¯x(t,θ0)−¯x(t,^θε)|p≤C(E|x(t,θ0)−¯x(t,θ0)|p+E|x(t,θ0)−¯x(t,^θε)|p), (4.56)\n\nfor some positive constant . Integrating both sides with respect to time, we get\n\n ∫T0E|¯x(t,θ0)−¯x(t,^θε)|pdt≤C(F(θ0)+F(^θε))≤2CF(θ0). (4.57)\n\nWe calculate the difference between and to obtain\n\n ˙¯x(t,θ0)−˙¯x(t,^θε)=A[¯x(t,θ0)−¯x(t,^θε)]+[¯f1(¯x(t,θ0),θ0)−¯f1(¯x(t,^θε),^θε)].\n\nBy the variation of constant formula, we have\n\n ¯x(t,θ0)−¯x(t,^θε)=∫t0eA(t−s)[¯f1(¯x(s,θ0),θ0)−¯f1(¯x(s,^θε),^θε)]ds.\n\nUsing the mean value theorem, we obtain\n\n ¯x(t,θ0)−¯x(t,^θε)=(θ0−^θε)∫t0eA(t−s)∇θ¯f1(¯x(s,θ′),θ′)ds, (4.58)\n\nfor some with . Denote\n\n G(θ′)=∫T0∣∣∣∫t0eA(t−s)∇θ¯f" ]
[ null ]
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https://excelchamps.com/formulas/starts-with/
[ "# Check IF a Cell Value Starts with a Text or a Number (Formula in Excel)\n\nLast Updated: November 21, 2023\n\n- Written by Puneet\n\nIn Excel, while working with data there might be a situation when you need to check if the value in a cell starts with a particular text or if the starting part of that value is a number or not.  In this tutorial, we will learn to write a formula to text both conditions.\n\n## IF a Cell Value Starts with a Particular Text\n\nIn the following example, you need to check if the starting three characters of the cell are equal to LXI. For this, you need to use the IF and LEFT.\n\nYou can use the below steps to write this formula:\n\n1. First, enter the IF function in a cell.\n2. After that, enter the LEFT function in the first argument of the IF, and refer to the cell A2 where you have the value, in the second argument, use 3 for the num_digit.\n3. Next, use the equal sign and enter the value (using double quotation marks) that you want to test.\n4. Now, in the second argument, enter “Yes”.\n5. And in the third argument, enter “No”.\n6. In the end, enter closing parentheses and hit enter to get the result.\n\nAs you can see below, for all the values where we have the value “LXI” at the start of the value, it returns Yes, else No.\n\n``=IF(LEFT(A2,3)=\"LXI\",\"Yes\",\"No\")``\n\nUse the below formula if you want to count the number of cells which starts with a particular value.\n\n``=SUMPRODUCT(--(LEFT(A2:A10,3)=\"LXI\"))``\n\n``=IF(ISNUMBER(VALUE(LEFT(A2,2))), \"Yes\",\"No\")``" ]
[ null ]
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https://kb.kutu66.com/c/post_2805358
[ "# c - 根据点旋转一个对象\n\n0 0\n``````\nO\nposition 2\n\nO Y\nobject ( x,y,z )\nposition 1\n\n``````\n\n``````\nglPushMAtrix ()\nglTranslatef ( -x, -y, -z ) ;\nglRotatef ( Q, 1.0f, 0.0f, 0.0f );\n\nglCylinder (/*argument*/)\nglPopMatriX ()\n\n``````\n\n0 0\n\n``````\nglTranslatef(-x, -y, -z);\nglRotatef(Q, 1.0, 0.0, 0.0);\nglTranslatef(x, y, z);\n//draw the object\n\n``````\n\n``````\naxis = vec(center_of_rotation - initial_position, center_of_rotation - final_position)\n\n``````\n\n``````\nfloat X1;//initial position\nfloat X2;//final position\nfloat O;//orign of rotation\n\nfloat OX1; OX1 = X1 - O; OX1 = X1 - O; OX1 = X1 - O;\nfloat OX2; OX2 = X2 - O; OX2 = X2 - O; OX2 = X2 - O;\n\nfloat axis;//vector product OX1 and OX2\naxis = OX1*OX2-OX1*OX2;\naxis = OX1*OX2-OX1*OX2;\naxis = OX1*OX2-OX1*OX2;\n\n``````" ]
[ null ]
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https://www.hanspub.org/journal/PaperInformation.aspx?PaperID=34651
[ "# 红外线透镜穿透率量测技术Measurement Technology of Transmittance of Infrared Optical System\n\nDOI: 10.12677/OE.2020.101003, PDF, HTML, XML, 下载: 194  浏览: 1,101\n\nAbstract: Infrared optical system is used in 8~12 μm range of infrared spectrum, which cannot be seen by human eyes, and the transmittance measurement method of visible optical system cannot be used, and the transmittance of infrared optical system was difficult to measure. At present, FTIR spec-trometer is used to measure transmittance of infrared optical system, which is very expensive and expensive to maintain. In this study, the transmittance of infrared optical system is measured by integrating the infrared sensing circuit and the smart infrared collimating beam. The measurement system consists of 2 mm diameter infrared collimating beam, thermopile sensor, OP amplifier, A/D IC and microprocessor. The thermopile converts the thermal radiation into analog electronic signal, and amplifies by OP amplifier, converted into digital by A/D IC, processed by 8051 microprocessor and displayed by LCD. The specifications of the lens to be tested are: focal length 19 mm, the f-number f/1.1 and the material of the lens was made by the black diamond. The test result of transmittance of the lens was 89%.\n\n1. 前言\n\n2. 基本原理 \n\n$\\text{TE:}\\gamma \\perp =\\frac{\\mathrm{cos}\\theta -\\sqrt{{n}^{2}-{\\mathrm{sin}}^{2}\\theta }}{\\mathrm{cos}\\theta +\\sqrt{{n}^{2}-{\\mathrm{sin}}^{2}\\theta }}=-\\frac{\\mathrm{sin}\\left({\\theta }_{i}-{\\theta }_{t}\\right)}{\\mathrm{sin}\\left({\\theta }_{i}+{\\theta }_{t}\\right)}$ (1)\n\n$\\text{TE:}\\gamma \\parallel =\\frac{{n}^{2}\\mathrm{cos}\\theta -\\sqrt{{n}^{2}-{\\mathrm{sin}}^{2}\\theta }}{{n}^{2}\\mathrm{cos}\\theta +\\sqrt{{n}^{2}-{\\mathrm{sin}}^{2}\\theta }}=-\\frac{\\mathrm{tan}\\left({\\theta }_{i}-{\\theta }_{t}\\right)}{\\mathrm{tan}\\left({\\theta }_{i}+{\\theta }_{t}\\right)}$ (2)\n\n$\\text{TE:}t\\perp =\\frac{2\\mathrm{cos}\\theta }{\\mathrm{cos}\\theta +\\sqrt{{n}^{2}-{\\mathrm{sin}}^{2}\\theta }}=\\frac{2\\mathrm{sin}{\\theta }_{t}\\mathrm{cos}{\\theta }_{i}}{\\mathrm{sin}\\left({\\theta }_{i}+{\\theta }_{t}\\right)}$ (3)", null, "(4)\n\n${R}_{s}={r}_{s}{r}_{s}^{\\varnothing },\\text{\\hspace{0.17em}}{R}_{p}={r}_{p}{r}_{p}^{\\varnothing }$ (5)\n\n${|{r}_{s}|}^{2}+{|{t}_{s}|}^{2}=1,\\text{\\hspace{0.17em}}{|{r}_{p}|}^{2}+{|{t}_{p}|}^{2}=1$ (6)\n\n${R}_{s,normal}={R}_{p,normal}=\\left[\\frac{n-{n}^{\\prime }}{n+{n}^{\\prime }}\\right]$ (7)", null, "Figure 1. Refraction and refraction at an interface between two media\n\n3. 系统架构", null, "Figure 2. Measurement system block diagram", null, "(a)", null, "(b)\n\nFigure 3. (a) Thin film infrared source and parabolic mirror; (b) IR source modulation curve", null, "Figure 4. Thermopile sensors", null, "Table 1. Optical electrical characteristics", null, "Figure 5. Output and input curve\n\n1) IR Source脉冲电路", null, "Figure 6. System structure", null, "Figure 7. PWM modulations", null, "Figure 8. IR source circuit\n\n2) Thermopile的讯号放大\n\nThermopile的讯号输出大约只有数十μV~数mV左右,为了后续A/D数据撷取,必须进行高倍数的讯号放大。且因制程及材质的关系其内部阻抗也相当大,约在数十KΩ左右且变化很大,因此放大器的选择即是一项重要的工作。要选用适合的放大器,首先要考虑组件的特性。Thermopile的输出为一直流电压准位且压降微弱,只有数十μV~数mV左右,故选用的放大器带宽并不是我们在意的项目,必须特别注意的是VOS (Offset Voltage)这项参数。过大的VOS将会使电压输出失真,因此我们必须选用低VOS的运算放大器。另外VOS的温度飘移(Offset Drift)也应尽量选择低的参数值,以增加整个放大电路的稳定性。总和以上要点,我们选用了MAXIM的MAX4238,MAX4238的VOS在室温下的典型值只有0.1 μV,即使最大值也只有2 μV,且其VOS温度飘移为10 nV/℃。另外,MAX4238的增益带宽积(GBWP)也高达1 MHZ,在高倍数放大下也不至于失真,各规格特性均可完全符合我们的需求。\n\nThermopile的结构上约有数50~150 KΩ的内阻,且非定值,不同组件间的内阻差异也很大,为了排除Thermopile内部阻抗的影响,放大器电路设计上必须使用具有高输入阻抗的放大型式。非反向放大器即具有高输入阻抗的特性,此类型放大器输入阻抗一般可有数十MΩ~数百MΩ的等级。", null, "Figure 9. Thermopile preamplifier circuit\n\n$fc=\\frac{1}{2\\text{π}RC}=\\frac{1}{2\\text{π}×10\\text{k}×1\\text{μ}}=15.9\\text{\\hspace{0.17em}}\\text{Hz}$ (8)", null, "Figure 10. Thermopile preamplifier circuit\n\nMCP3302是一个SPI (Serial Peripheral Interface)串行接口的13bit SAR型模拟/数字转换器(A/D Converter),可依需求使用4通道单端输入或2通道差动输入,电源电压使用5 V时,取样频率(sampling rate)可以达到100 KHZ,量测误差最大为±1 LSB INL (MCP3302-B)或±2 LSB INL (MCP3302-C)。\n\nMCP3302使用上必须遵循其制定的SPI命令格式来对其进行转换与读取的动作。MCP3302的串行接口有三个入接脚,一个讯号输出接脚,其通讯格式里为一个启始位之后接着4个命令位,此4个位指定了MCP3302的动作模式,分别为1 bit的单端/差动选择位(Single/Diff)和3 bits的channel选择位(D2~D0)。", null, "Figure 11. ADC signal acquisition interface circuit\n\n4) 单芯片89C51处理器\n\n5) 红外线检测装置实体", null, "(a)", null, "(b)", null, "(c)\n\nFigure 12. (a) System hardware diagram; (b) IR Source pulse circuit; (c) Thermopile measurement circuit\n\n4. 实验方法与结果\n\n1) 测试物品:红外镜组焦距19 mm,其光圈f/1.1,光学材料为黑钻石硫属化物玻璃(Black Diamond™ chalcogenide glass),其光学特性如表2所列。黑钻石硫属化物玻璃如AMTIR-1,IG6,BD2,GASIR-1及GE等其穿透率光谱范围0.7~20.0 μm如图13所示 。图14所示为红外线镜组外观图。\n\n2) 精密镜片夹具:要求垂直度与平行度。\n\n3) 红外光学系统穿透率量测系统。\n\n4) 实验方法\n\na. 确认红外光学系统穿透率量测系统在最佳运作状况。\n\nb. Alignment红外准直光束与Thermopile在同一水平面及同一光轴,使Thermopile输出信号最大。\n\nc. 将红外镜组置于红外光学系统穿透率量测系统装置中。\n\nd. 调整红外镜组垂直于远红外准直光束,平移Thermopile,使Thermopile接受到穿透信号最大。确认Thermopile接受到最大信号之后,进行穿透率量测。\n\ne. 改变红外光源强弱,量取不同穿透信号。\n\nf. 进行红外镜组穿透率分析。", null, "Figure 13. Transmittance spectrum of the chalcogenide glass", null, "Table 2. Optical characteristics of infrared lens", null, "Figure 14. Infrared lens\n\n5) 红外镜组穿透率(T)的量测结果", null, "Table 3. Test data of transmittance", null, "Figure 15. Statistical curve of test data\n\n5. 结论", null, "Table 4. Comparison of this method with FTIR spectrometer detection\n\n Hecht, E. (2016) Optics. 5th Edition, Addison-Wesley Longman, Inc., Reading. Smith, W.J. (1992) Modern Lens Design. McGraw Hill, New York. Index of /wp-content/uploads/Linear/IRSources. https://www.boselec.com/wp-content/uploads/Linear/IRSources PerkinElmer Optoelectronics, Inc. (2003) “TPS 334—Thermopile Detector” Datasheet. Wolfe, W.L., Kruse, P.W. and Bass, I.M. (1995) “Thermal detectors” in Handbook of Optics. McGraw-Hill, New York. https://www.hamamatsu.com/resources/pdf/ssd/e07_handbook_Thermal_detectors, Chp. 7, pp. 3-7. Nam, M., Washer, J. and Oh, J. (2015) Breaking the Mold: Overcoming Manufacturing Challenges of Chal-cogenide Glass Optics. https://www.photonics.com/Articles/Breaking_the_Mold_Overcoming_Manufacturing/a57309" ]
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http://www.abuildersengineer.com/2014/07/
[ "## Wednesday, July 16, 2014\n\n### SHEAR STRESS IN STEEL BEAM\n\nThis beam, supporting a column point load of 96 k over a door, is a composite beam consisting of a wide-flange base beam with 8x½ in plates welded to top and bottom flanges. The beam is analyzed with and without  plates.  As shown before, for steel beams shear stress is assumed to be resisted by the web only, computed as fv  = V/Av.  The base beam is a W10x49 [10 in (254 mm) nominal depth, 49 lbs/ft (6.77 kg/m) DL] with a moment of inertia Ixx= 272 in^4 (11322 cm^4).  Shear in the welds connecting the plates to the beam is found using the shear flow formula q = VQ/(I).\n\n1  Beam of L= 6 ft (1.83 m) span with P = 96 k point load\n2  Composite wide-flange beam W10x49 with 8x½ inch stiffener plates\n\nShear force V = P/2 = 96/2          V = 48 k\nBending moment M = 48(3)         M = 144 k’\n\nWide-flange beam\n\nSince the beam would fail in bending, a composite beam is used.\n\nComposite beam\n\nSince the shear force remains unchanged, the web shear stress is still ok.\n\nShear flow q in welded plate connection\n\nSince there are two welds, each resists half the total shear flow\n\nNote: in this steel beam, bending is stress is more critical than shear stress; this is typical for steel beams, except very short ones.\n\n## Monday, July 7, 2014\n\n### SHEAR STRESS IN WOOD I-BEAM\n\nSince this is not a rectangular beam, shear stress must be computed by the general shear formula.  The maximum shear stress at the neutral axis as well as shear stress at the intersection between flange and web (shear plane As) will be computed.  The latter gives the shear stress in the glued connection.  To compare shear- and bending stress the latter is also computed.\n\nBeam of L= 10 ft length, with uniform load w= 280plf (W = 2800 lbs)\nCross-section of wood I-beam\n\nFor the formula v= VQ/(Ib) we must find the moment of inertia of the entire cross-section. We could use the parallel axis theorem of Appendix A.  However, due to symmetry, a simplified formula is possible, finding the moment of inertia for the overall dimensions as rectangular beam minus that for two rectangles on both sides of the web.\n\nNote c= 10/2 = 5 (half the beam depth due to symmetry)\n\nStatic moment Q of flange about the neutral axis:\n\nShear stress at flange/web intersection:\n\nStatic moment Q of flange plus upper half of web about the neutral axis\n\nMaximum shear stress at neutral axis:\n\nNote: Maximum shear stress reaches almost the allowable stress limit, but bending stress is well below allowable bending stress because the beam is very short.  We can try at what span the beam approaches allowable stress, assuming L= 30 ft, using the same total load W = 2800 lbs to keep shear stress constant:\n\nAt 30 ft span bending stress is just over the allowable stress of 1450 psi.  This shows that in short beams shear governs, but in long beams bending or deflection governs.\n\n## Wednesday, July 2, 2014\n\n### SHEAR STRESS IN WOOD AND STEEL BEAMS\n\nBased on the forgoing general derivation of shear stress, the formulas for shear stress in rectangular wood beams and flanged steel beams is derived here.  The maximum stress in those beams is customarily defined as fv instead of v in the general shear formula.\n\nShear at neutral axis of rectangular beam (maximum stress),\nNote: this is the same formula derived for maximum shear stress before\n\nShear stress at the bottom of rectangular beam.  Note that y= 0 since the centroid of the area above the shear plane (bottom) coincides with the neutral axis of the entire section. Thus Q= Ay = (bd/2) 0 = 0, hence\n\nv = V 0/(I b) = 0 = fv, thus\nfv = 0\n\nNote: this confirms an intuitive interpretation that suggests zero stress since no fibers below the beam could resist shear\n\n3  Shear stress at top of rectangular beam.  Note A = 0b = 0 since the depth of the shear area above the top of the beam is zero.  Thus\n\nQ = Ay = 0 d/2 = 0, hence v = V 0/(I b) = 0 = fv, thus\nfv = 0\n\nNote: this, too, confirms an intuitive interpretation that suggests zero stress since no fibers above the beam top could resist shear.\n\n4\nShear stress distribution over a rectangular section is parabolic as implied by the formula Q=b(d^2)/8 derived above.\n\n5  Shear stress in a steel beam is minimal in the flanges and parabolic over the web.\n\nThe formula v = VQ/(I b) results in a small stress in the flanges since the width b of flanges is much greater than the web thickness.  However, for convenience, shear  stress in steel beams is computed as “average” by the simplified formula:" ]
[ null ]
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https://mathematica.stackexchange.com/questions/105079/plotting-eigenvalues-with-devoted-level-coloring
[ "# plotting eigenvalues with devoted level coloring\n\nI am about to plot eigenvalues of a matrix versus varyingj's.\n\nHma[j_Integer] = {{0.1*j^2, 0, 0, 0.2*j, 0}, {0, 0.1*j, 0, 0.2*j^3,\n0}, {0, 0.1*j, 0, 0, 0.2*j}, {0.1*j^2, 0, 0, 0, 0.2*j}, {0, 0,\n0.1*j, 0.2*j, 0}};\nListPlot[data]", null, "I am trying to have a plot with specified color as I manually showed above. (higher eigenvalues (first ones) with a same color (for example Red above), seconds with same color (and different from the first ones for example Yellow))\n\nFor the data in the question, the following also works.\n\nListPlot[Transpose[Split[data, First[#1] === First[#2] &]],\nPlotStyle -> {Blue, Green, Purple, Orange, Red}]", null, "This, of course, assumes that data already is ordered by size. If not, use\n\nListPlot[SortBy[Transpose[Split[data, First[#1] === First[#2] &]], Last],\nPlotStyle -> {Blue, Green, Purple, Orange, Red}]\n\n\nAnd, if larger markers (or other such presentation changes) are desired, use\n\nListPlot[SortBy[Transpose[Split[data, First[#1] === First[#2] &]], Last],\nPlotStyle -> ({#, PointSize[Large]} & /@ {Blue, Green, Purple, Orange, Red})]", null, "Note that the Green points are scarcely visible, because they approximately coincide with the Purple points.\n\n n=5;", null, "" ]
[ null, "https://i.stack.imgur.com/e0KzR.png", null, "https://i.stack.imgur.com/zyRYF.png", null, "https://i.stack.imgur.com/xZYf0.png", null, "https://i.stack.imgur.com/XpwZf.jpg", null ]
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https://m.wxwm.cc/nansheng/shanggan/
[ "• 琴弦低声唱离别。\n\n• 再美的曾经、我只能回忆\n\n• 硪卟數蒵丗庎\n\n• _⺌詮劇終.﹎"\n\n• 风゛化了我们的回忆\n\n• 只剩下背影\n\n• 柠檬太酸i\n\n• 她求我滚i\n\n• 无伴人\n\n• ξ 回不去的苍白\n\n• 一个人高傲的独活\n\n• 无言以对 ζ\n\n• 若终要失去、不如放开\n\n• 惹尘埃是非\n\n• 花醉花思泪\n\n• 胭脂 ※\n\n• 凄惨的回忆"\n\n• 呼吸时,心都会痛。\n\n• 原来爱情这么难\n\n• 深夜在被窝里偷哭\n\n• 你凭什么不打扰我\n\n• 任这空虚沸腾\n\n• 锁心,锁\n\n• 筋疲力尽的追逐,只是徒劳\n\n• 爱人别走\n\n• 输不起的感情\n\n• 空寂\n\n• oo-┈→凉心℡~\n\n• 都叫兽别走i\n\n• 再见、亲爱的\n\n• 承载着曾经。\n\n• ┗從未拥冇、談何矢佉┓\n\n• ﹎ゞ没有信任的爱情\u0007/╱°\n\n• 夜盲症\n\n• 壹朵薔薇花\n\n• 苦撑\n\n• 划伤了心_ジ\n\n• 选择放手\n\n• 听海的哭泣\n\n• ╰天使的伤\n\n• 冷态度i\n\n• 孤独是世界绝症!\n\n• 傷、待續\n\n• 习惯了∥与影子的对话﹌\n\n• 笑着、说再见\n\n• 弦断心凉繁华逝\n\n• 独活\n\n• 费劲心思爱过\n\n• 没有未来。\n\n• ︶ㄣ x1n痛の兹味\n\n• ~隐隐的伤感 /\n\n• 情到深处竟是离别i\n\n• 不狸不气的。爱你\n\n• ﹌你给的诺言、都记得″\n\n• 婲開、終須落\n\n• 有一种想念叫避而不见@\n\n• 是你让我学会熬、\n\n• 心碎见蓝天\n\n• 那悲傷、凋落\n\n• 〆雨滴落丶浅似留殇\n\n• 天堂の劇終℡\n\n• 繁华里的沧桑ぢ\n\n• ζ眼泪在失落\n\n• 带泪怎笑.\n\n• 笑着流泪、我学不会じ\n\n• 最终的最终、终究是戏\n\n• 我没变、只是你厌倦了\n\n• 欲言又止的难受\n\n• 残阳照、墨痕\n\n• 看见你心都碎了\n\n• 在給我Ⅰ丶勇气\n\n• 你萌化了我的心i\n\n• 一切只是我希望i\n\n• 想念、是会【致命】的痛\n\n• [ 不如初 ]\n\n• 强势控局\n\n• 读书凶铃!\n\n• 別ㄋ、那纏綿\n\n• ▲黑色瞳孔丶满带伤痛\n\n• 〆青春献给了课桌\n\n• 一次性抹掉春冬\n\n• 。- ‘梦毁千百次’.\n\n• 回忆像章鱼扑上来\n\n• 眼泪替我卸妆\n\n• 等你归\n\n• 转圈圈\n\n• 笑出的泪 =\n\n• 心酸不已。\n\n• 纠结、回忆的痛\n\n• 一个人的承诺\n\n• 宁做不懂是是非非的孩子\n\n• 深秋、知涼\n\n• 我深知我不配\n\n• 一秒的安慰、\n\n• 他說的愛過是錯過…\n\n• 々 被你所伤\n\n• 心里住了个不可能的人i\n\n• 花露水。防蚊の\n\n• 红丶╮A\n\n• 容我爱你可好\n\n• 说㈠半旳爱\n\n• 执手曲已凉i\n\n• 无法诠释的永恒\n\n• 回来好么\n\n• 相爱太早,不能终老。\n\n• 伱给的爱 太牵强\n\n• 伴君悲歌\n\n• 孤独解酒\n\n• ╯遗失的繁华\n\n• シ独守空城づ\n\n• 血溅了白纱。\n\n• 一曲断肠i\n\n• The city of the sky\n\n• 你的爱、太虚伪。\n\n• 莪的悲伤 仍在继续\n\n• 旧心酸。\n\n• ︶ㄣ鈊痛|戀 落泪\n\n• 没有你\n\n• 一个人的浪漫/*\n\n• 疯狂的丶丿石头\n\n• 和寂寞有染 ∥\n\n• 他故事中的我、\n\n• 何时秋风悲画扇\n\n• 糖果控、\n\n• ︶心痛的玩笑\n\n• 本是古典 何须时尚\n\n• 你名毁她命\n\n• 回不到从前@\n\n• 时间能让我忘了你吗\n\n• 美人性情\n\n• 悲痛\n\n• 微笑要带着眼泪才耐看づ\n\n• 多余的⌒温柔\n\n• 爲何離開↘莪\n\n• 想哭无泪\n\n• 认命扮矮人\n\n• 沧桑的岁月浮华了谁\n\n• 逼着放弃最痛苦\n\n• 那时年少,\n\n• 柠檬落泪都是酸;\n\n• 爱情的旋律\n\n• 刺心谎言,\n\n• 真相背后的残忍\n\n• 爱上夜的黑、迷失了我的爱\n\n• 心痛像条线\n\n• *﹏無心不心痛〆\n\n• 凄寒半世留殇铭\n\n• 荒废过的心存有你\n\n• 我忘不掉你!\n\n• 有些歌,听得沉醉了\n\n• ㄨ_花叹、\n\n• 情话再多、只是一种敷衍\n\n• 作业变成蝴蝶飞走了@\n\n• 爱情已剧终\n\n• 我与影子孤独终老\n\n• 你不过是个过客而已@\n\n• ち潮货↙总裁\n\n• ——摇摆世界\n\n• 安徒生的谎言、\n\n• 离你我心不碎\n\n• 矫情不是我的范#\n\n• 不爱,滚i\n\n• 放肆演绎青春i\n\n• 吃货总比痴货好!\n\n• 骑着蜗牛,拽天下ㄟ\n\n• 爱的分界线。\n\n• 回忆太细\n\n• 初衷的味道\n\n• 拥抱漏风\n\n• 思念埋在发间\n\n• 半分笑——〆\n\n• 一万种快乐\n\n• 梦好沉\n\n• 几度温柔,\n\n• 笑脸是悲伤的面纱.\n\n• 厌情症°\n\n• 醋,是一种爱i\n\n• 墨香染城\n\n• 玉砌似画染\n\n• 旧夏浅入梦°\n\n• 想赢就别喊停。\n\n• 对伱微笑╮纯属伱很可笑\n\n• 旧街凉风°\n\n• 撑起一片天\n\n• 倾听心跳de旋律\n\n• 若爱、请深爱。\n\n• 时间把苦熬成甜\n\n• 不合脚的鞋再美也不要\n\n• 阳光总在风雨后\n\n• 我若不努力,谁给我未来\n\n• 安于得失、淡于成败\n\n• 曾经的你早已不复存在\n\n• 深情在睫,孤意在眉\n\n• 浅嗄ゞ写卟完的温柔\n\n• 关于爱情只字不提\n\n• 江南烟雨〆相思醉つ\n\n• 花静幽然\n\n• 许你三千笔墨画我绝世倾城\n\n• 我像谁°\n\n• 多情人\n\n• 海屿荒\n\n• 后来呢\n\n• 顾与我i\n\n• 攻你心i\n\n• 陪你闹i\n\n• 久伴我i\n\n• 我会暖i\n\n• 一抹高傲旳笑。\n\n• 走开、暧昧\n\n• 钻石般耀眼\n\n• 完美洒脱\n\n• 膜拜的对象≈\n\n• 快乐是选择\n\n• 高调。转身\n\n• 不期待.再重来\n\n• 无所谓的魅惑\n\n• 释放シ生命的光华\n\n• 兄弟是拿心来对待的\n\n• 脉搏跳动着高傲ヅ\n\n• 非买品ю\n\n• 演绎つ只属于我们的未来\n\n• 尘缘而已。\n\n• 分了、我来合。\n\n• 止步爱情°\n\n• ——活出自己的精彩.℡\n\n• 美男子\n\n• 微笑面对未来\n\n• 光彩夺目的高傲\n\n• 耀眼的光芒\n\n• 晋豫达人\n\n• 拒绝翻版.\n\n• 丶限量版帅仔\n\n• 爱就一辈子\n\n• 漫天游ゝ\n\n• 亲吻ωǒ资本\n\n• 继续丿辉煌、\n\n• 〞将军っ\n\n• 淡淡的优雅\n\n• ∝耀出彩\n\n• ╰ 笑看人生\n\n• 你好优秀!\n\n• 炫丽德青春、\n\n• 活出高姿态、\n\n• 炫彩死神\n\n• 、信者得爱\n\n• 玉衡逍龙.+\n\n• 青春爱无赦 *\n\n• ワ逆转结局\n\n• 梦的怒放╮\n\n• 永不退缩\n\n• 活着便精采°\n\n• 受大气,成大器i\n\n• 男心凉\n\n• ╰︶ 男爵\n\n• 那个位置,叫做刻骨铭心\n\n• 时间把苦熬成甜\n\n• 别吵赢道理却输了感情\n\n• 给时间时间,让过去过去\n\n• 想赢就别喊停\n\n• 梦想不只是梦与想\n\n• 笑脸赢人脉\n\n• 一边得到一边失去\n\n• 我若不努力,谁给我未来\n\n• 安于得失、淡于成败\n\n• 把每天当末日来过\n\n• 柠檬不该羡慕西瓜的甜\n\n• 你若盛开、蝴蝶自来\n\n• 不要活给别人看\n\n• 若无过客丶何来人生\n\n• 每一天都是限量版\n\n• 挫折是化了妆的祝福\n\n• 成熟不在于年龄而在于经历\n\n• 得之坦然、失之淡然\n\n• 心是晴朗的人生就没有雨天\n\n• 不努力,拿什么说明天\n\n• 密码里隐藏着秘密\n\n• 珍惜〆眼前的幸福╮\n\n• 至少我还有梦\n\n• 欲戴王冠必承其重\n\n• 不忘初心方得终始\n\n• 孤独是成长的必修课\n\n• 今天不走明天要跑\n\n• 因为知足,所以幸福\n\n• 念你情深\n\n• 人生如梦、梦如烟\n\n• 相爱就爱,别怕阻碍\n\n• 北岛旅客\n\n• 一夕意相左\n\n• 旧光影里的格子少年\n\n• 陪笑\n\n• 跪下喊爷!\n\n• 吻妳是不想失去妳\n\n• 一步踏尽一树白\n\n• 你知道我长短\n\n• 执念于你\n\n• 赠你深爱与久伴\n\n• 醉挽清风丶已成空\n\n• 念念相忘\n\n• 心不大只有你\n\n• 纤纤公子\n\n• 独手毁天下\n\n• 年轻不拽世界何以精彩\n\n• 风雨都扛过\n\n• 劳资最烦起名了\n\n• 酷似你爹\n\n• 命里不缺狗,你要走就走\n\n• 星战@\n\n• 将神@\n\n• 龙将@\n\n• 邪恶%\n\n• 新仙剑\n\n• 大将军\n\n• 夜店之王\n\n• 斗破乾坤\n\n• 坦克世界\n\n• 修真世界\n\n• 傲视天地\n\n• 光辉终结\n\n• 现代战争\n\n• 卡通农场\n\n• 公子泺尘\n\n• 神将三国\n\n• 王者天下\n\n• 橘萝卜蹲@\n\n• 苍空的蓝耀\n\n• 旋风小陀螺\n\n• 秋风追猎者\n\n• 迷你大城市\n\n• 噬血魅影@\n\n• 暴君与猫@\n\n• 战神将军@\n\n• 柔媚——妖瞳\n\n• 夏眠i\n\n• 乱斗堂\n\n• 弑鬼神\n\n• 战无极\n\n• 天下白\n\n• 苏伯陵\n\n• 安如山\n\n• 刺情°\n\n• 微生墨\n\n• 霸剑皇侯\n\n• 似梦似幻\n\n• 很傻、很固执\n\n• 卖萌的小行家\n\n• 阳光男孩\n\n• yí銗、镎命嫒ぐ\n\n• 劳资独宠一方\n\n• 。赫颜\n\n• 酷似你爹\n\n• 渣爷!\n\n• 小屁孩先森^\n\n• £霸王↘爷战神三\n\n• 爷ワ゛给钮淡定\n\n• 行星美男\n\n• 謌践踏爱綪\n\n• 欠你的幸福\n\n• 三好不良少年°\n\n• 竹·小马‖儒\n\n• 无处话凄凉\n\n• 滁ㄋ故亊涐一兂所冇\n\n• 烈酒配孤独\n\n• 渺远的断云□\n\n• ’楠軕蒗児ヽ\n\n• 又被自己帅到了\n\n• 荒世独拥\n\n• 任性男神\n\n• 苍苍迟暮\n\n• 静守己心,看淡浮华\n\n• 胖次超人\n\n• 跑到坟场去吓鬼\n\n• 久挽不留\n\n• 劳资独宠一方\n\n• 荒笹独拥\n\n• 怨风离愁人\n\n• 孤骨\n\n• 濄徃谩谩说\n\n• 承诺早已泛黄\n\n• 廻忆里菂馀温\n\n• 风月瘦如刀,催人老\n\n• 无处寄笺\n\n• 情话至深\n\n• 旅人泪\n\n• 一句爱的晚安语\n\n• ←狱邪魂断ぐ\n\n• 竖起中指操起生活\n\n• 阳光宅男\n\n• ——鲭风痴鵟//\n\n• 无能\n\n• 时间煮雨是他的倾诉\n\n• 清尊素影\n\n• 长愿相随\n\n• 再闹硪憱垱众亲祢\n\n• 拿命珍惜她\n\n• 为你我受冷风吹\n\n• 孤独是我妻\n\n• 谁会发光我就灭谁的光\n\n• 我曾经掏空了心\n\n• 人前给面子,人后扇耳光\n\n• 猎鹿人\n\n• 风度翩翩°\n\n• 龙爷无敌°\n\n• 那一季、那点伤\n\n• Mr°骚年ぃ\n\n• 陷阱里的王子\n\n• い 第 一 先 生 が\n\n• 跳梁小丑\n\n• 蜀国犀利哥\n\n• 老师、她亲硪\n\n• 怪咖男渣!\n\n• 岁月枯荣\n\n• ╰嘞蚗儅哖\n\n• 未来家庭主男。\n\n• 挑眉少年°\n\n• 英雄♀奶油♂\n\n• \親愛dé咾婆ゞ |\n\n• 坏男孩\n\n• 苏三大爷\n\n• 喜旧之人——\n\n• 爵士少年.﹌‖\n\n• 上学穿拖鞋是汉子@\n\n• 餦街舊魜灬\n\n• 丿灬哥的范儿丶\n\n• 小小少爷i\n\n• 少年未老心已凉√\n\n• 亦枫\n\n• 孤男寡旅\n\n• 辣条先森i\n\n• 老纳曾是一朵花i\n\n• 哥贱到你烦\n\n• 零帝\n\n• 胡渣硬男。\n\n• 指尖星光在流浪\n\n• 仮蒎の尐夥姅\n\n• 萌漢紙\n\n• 仯年丕變杺ヽ\n\n• 瑷俄dê請呼χí←\n\n• 做你的男人。\n\n• 小萌男!\n\n• 学弟°\n\n• 我是Bb哥\n\n• 傲视群雄\n\n• 暮然回首脖子疼\n\n• ヤrú菓méi姷ài簻\n\n• ←栢褩缃厭oО\n\n• 沬粜遈沬箌粜\n\n• 璐蒤鎐遠、匢朢初吢\n\n• tū嘫鋒悧の徊yì…\n\n• 风扑进怀\n\n• 旧事甚歉\n\n• 无尽空虚\n\n• 贱是一种态度\n\n• 單裑等鱫\n\n• ⺷壹筆縴連ず\n\n• zhí戳xīn扉//\n\n• 爱人想离我怎挽\n\n• 剑起苍穹云归处\n\n• ╰嘞蚗儅哖\n\n• ◇喰種,蠶飠吣靈\n\n• 殺手\n\n• ﹎.茵为她值得⺌\n\n• 酒醉夜未阑\n\n• 痴心错付\n\n• ﹏風流∨成癮Ο\n\n• ╰→嗳棏呔遲ㄞ\n\n• 练习拥抱\n\n• 泡面君ˇ\n\n• 两包辣条约吗\n\n• 独酌陈酿\n\n• 各走各路〃\n\n• 也许,我只是一个过客\n\n• 你是我在青春里辗转的歌\n\n• 三千青丝散\n\n• 只為ㄋ遇見你\n\n• 活着别让心遭罪\n\n• 丢了薇笑ヽ嗱什麼伪装\n\n• 幸福加载中…\n\n• 总有一个人先走\n\n• 说爱太烫嘴ァ\n\n• 想你的时候*落泪忧伤\n\n• 心动心痛丶\n\n• 冗长梦毁\n\n• 你可知道我的梦i\n\n• 好了伤疤忘了痛\n\n• ″ 葬你身边\n\n• 比纸薄的情ゝ\n\n• 情缘隔世\n\n• 私の心は撩乱\n\n• 还在等\n\n• 一句分手,都是泡沫\n\n• 人心真脏@\n\n• 忧伤倒数≈\n\n• - 對ai情禁言。、\n\n• 哭到失控\n\n• 爱是泡沫。\n\n• 死撑着装坚强\n\n• 男神离我好远@\n\n• 柠檬太酸i\n\n• 海伤°\n\n• 执著心却凉ι\n\n• 离北°\n\n• 那一抹忧伤。\n\n• 哪有胖子不忧伤丶\n\n• 该笑吗.\n\n• 远离碍i\n\n• 够狠心i\n\n• 知心碍人i\n\n• 放不下你是我活该\n\n• 太揪心\n\n• 他心无我!\n\n• 一千零一句谎言\n\n• 怪我冷i\n\n• 我该拿什么换回你,\n\n• 爱情谷底\n\n• 他不会回来了。\n\n• 我已开始怀念\n\n• 今年夏天我们就散了。\n\n• 我算什么@\n\n• 童话破灭。\n\n• 一个人失忆\n\n• 我本冷情怎暖你心i\n\n• 救赎@\n\n• 抱歉我无梦赠你\n\n• 灰白色充斥记忆i\n\n• 想说的话压在心底——.\n\n• 〆﹏落日般的忧伤\n\n• 追爱成忆i\n\n• 太熟悉了会陌生°\n\n• 郁闷中……\n\n• ℡ 晴天有点孤单、\n\n• 寂寞的心。\n\n• 半城繁華半城傷づ\n\n• 一个人的孤单情歌。\n\n• 离心愁i\n\n• 感情已褪色\n\n• 殇城似觞\n\n• 回忆那么疼!\n\n• 时间把回忆埋了\n\n• 回忆再美、也带着伤\n\n• 梦醒人走茶凉↘\n\n• 痛而不言i\n\n• 会好的i\n\n• 人心不可猜透@\n\n• 眼中的忧伤如同仓皇的落日\n\n• 微笑、掩盖悲伤\n\n• 眼里的寂寞。\n\n• 梦散了i\n\n• 用微笑掩盖痛\n\n• 三千弱水化作眼泪!\n\n• 抓不紧 i\n\n• 我会怕i\n\n• 左眼会陪右眼哭i\n\n• 殘留的温柔@\n\n• 分手理由ヾ\n\n• 心瞎,\n\n• 孤伴i\n\n• 盐不及泪咸 i\n\n• 不曾拥有你i\n\n• 低凋、进行曲\n\n• 笑、淡化了那伤\n\n• 我年轻丶心不定\n\n• の),茈娚孓\n\n• ㄗs銱児啷当\n\n• 风蓅Иé尙\n\n• /.赱私娚孒o.\n\n• メ霸气爷ャ\n\n• 尐样贼≯坏\n\n• →伤你无鈊^-\n\n• 對伱啲依賴\n\n• 为幸福向前冲\n\n• 丶柔情小男人\n\n• 温习你的温柔.\n\n• 連椄 ф簖╮\n\n• 情在⒈夜之间﹏\n\n• 霸道D温柔\n\n• 心照不宣\n\n• 贩卖幸福。\n\n• 丢不掉的思念\n\n• 不稀罕你的爱\n\n• 念念不忘︶——\n\n• 无力的,微笑\n\n• 哥、寂寞成伤\n\n• 無法回頭 、\n\n• 午夜,醉情歌\n\n• 斩碎星空\n\n• 單身リ天涯\n\n• 一切从头。\n\n• ╭冷眼旁观\n\n• 坦白\n\n• 怡然自得。\n\n• 哼着情歌、享受寂寞\n\n• 无声无息。安之若素╮\n\n• 站在高岗\n\n• 暴雨的洗礼\n\n• 你只是道听途说 つ\n\n• 做人要有风范\n\n• 〆岁月成『风』\n\n• ¢ 无可替代的友谊﹌\n\n• 我们性格不合\n\n• 用眼角去看中国人" ]
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https://www.managementtutors.com/Recent_Question/37331/RESEARCH-SCHOOL-OF-FINANCE-ACTUARIAL-STUDIESAND-STATISTICSINTRODUCTORY
[ "Recent Question/Assignment\n\nRESEARCH SCHOOL OF FINANCE, ACTUARIAL STUDIES\nAND STATISTICS\nINTRODUCTORY MATHEMATICAL STATISTICS PRINCIPLES OF MATHEMATICAL STATISTICS\n(STAT2001/6039)\nAssignment 1 (2018 Semester 1)\nYour solutions to this assignment should be placed in the appropriate box in the RSFAS School foyer by the due time and date (as provided in the Course Outline and on Wattle). Attach a cover sheet (as provided on Wattle) which has your ANU ID number. The assignment is out of 100 and is worth 10% of your overall course mark.\nProblem 1 (Total 20 marks)\nSuppose that P AB( ) = 0.1, P(B ? =C) 1 and P B( - =A) P A( ? =B) 2 (P A- B). Find P AB P AC P ABC P A P( )+ ()- ()- ( )+ ( )B -PC P ABC( )- ( ), or determine the range of possible values for this quantity if it cannot be calculated as a single number.\nProblem 2 (Total 30 marks)\nHomer and Marge play a game by taking turns rolling a standard six-sided die, starting with Homer, until there occurs a sequence of k or more 4s immediately followed by a 5 or 6 (e.g. 45, 245 or 5446, if k = 1). The last person to roll wins the game. (E.g., if k = 2, then each of the sequences 446, 64445 and 465443445 results in Homer winning.) Find the probability that Homer wins, for each k = 0, 1, 2, 3 and 99.\nProblem 3 (Total 50 marks)\nA stack of ten cards has four hearts (which are red), three diamonds (which are red), two spades (which are black) and one club (which is black). Four cards are sampled from the stack, randomly and without replacement, and placed in a box. Then one card is randomly selected from the box. If that card is a heart then all of the other three cards in the box are burnt. Otherwise, two cards are sampled, randomly and without replacement, from the other three cards in the box, and then these two cards are burnt. Find the probability that exactly k red cards are burnt, for each possible value of k.\nPage 1 of 1" ]
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https://jutge.org/problems/P70756_en
[ "# Partitions P70756\n\nStatement", null, "html\n\nWrite a program that, given n different words s1, …, sn and a number p, prints all the ways to share the words between p subsets.\n\nInput\n\nInput consists of a natural number n > 0, followed by s1, …, sn, followed by a natural number p > 0.\n\nOutput\n\nPrint all the ways to share the words between p subsets. The elements of each set must appear in the same order than in the input. Print an empty line after each partition.\n\nObservation\n\nStrictly speaking, a partition cannot have empty subsets, but we forget about that restriction in this exercise.\n\nYou can print the solutions to this exercise in any order.\n\nPublic test cases\n• Input\n\n```2\nhello bye\n2\n```\n\nOutput\n\n```subset 1: {hello,bye}\nsubset 2: {}\n\nsubset 1: {hello}\nsubset 2: {bye}\n\nsubset 1: {bye}\nsubset 2: {hello}\n\nsubset 1: {}\nsubset 2: {hello,bye}\n\n```\n• Information\nAuthor" ]
[ null, "https://jutge.org/problems/P70756_en/png", null ]
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https://www.1onepsilon.com/single-post/2018/04/27/Can-the-truth-be-tabulated
[ "© 2016 by One on Epsilon PTY LTD\n\n# Can the truth be tabulated?\n\nApril 26, 2018\n\nHow often during the day do you think about what is true or what is false? What does it mean for a statement to be true? Are some statements more true than others? Think about the last time someone asked you a question. When you responded, was there a clear distinction between a true answer and a false answer?\n\nIn regular day to day communication, often the issue of true vs. false can become quite a grey area. What about truth in mathematics? In mathematical logic, statements are taken as either true or false. In this post, we consider some examples of circumstances where this thinking can lead to a contradiction. Enter the paradox.\n\nA paradox can mean many things in mathematics. Sometimes it refers to a result that is counter-intuitive or unexpected. Other times it refers to a situation that results in an incorrect conclusion because of a subtle error or incorrect assumption made somewhere along the way.\n\nHere, we would like to explore a well-known paradox that occurs in the context of mathematical logic known as Curry’s Paradox. Before we delve into Curry’s Paradox, let's consider a simpler logical paradox.\n\nConsider the following statement:\n\nThis sentence is false.\n\nThink about this for a moment. If the sentence is actually false, as it claims to be, then the sentence must be true. Alternatively, if the sentence is true, then the sentence must be false! Hang on, we’re going in circles here! This statement is an example of a logical paradox, that is, a statement that is inconsistent with logic. The paradox arises due to the statement referring to the value of its own truth.\n\nIn using the word logic here, we mean that every statement is either true or false, but it cannot be both true and false. Furthermore, if a statement is not true, then it is false, and vice versa.\n\nIn order to carefully examine and understand Curry’s Paradox, let’s first explore compound statements. A compound statement is one that is made up of two or more statements. Here is an example of a compound statement:\n\nIt is raining or the kids are playing outside.\n\nWe can use brackets to separate out the distinct statements.\n\n(It is raining) or (the kids are playing outside).\n\nLet’s set A to represent the statement “it is raining” and B to represent the statement “the kids are playing outside.” Our sentence is then:\n\nA or B.\n\nOne way to analyze a compound statement is by using a truth table. This is a table that keeps a record of all possibilities of the truth-value of each statement. These values are used to determine the value of the compound statement.\n\nThere are two possible values for statement A, true or false. There are two possible values of statement B, true or false. The compound statement, \"A or B\" uses the Boolean operator OR. We can think of it as, \"When A and/or B is true, this statement is true.\" Here is the truth table for \"A or B\":\n\nNote that the compound statement \"A or B\" is only false if A and B are both false.\n\nTwo statements are logically equivalent if their truth tables are the same. It might seem strange at first, but another way of conveying the meaning of that original sentence is the following logical conditional statement:\n\nIf (not A) then B\n\nLet’s look at this a bit more closely. If “not A” (the hypothesis) is true, then the entire statement can only be true if B (the conclusion) is also true.\n\nWe must be very clear to take the statement at face value and not interpret anything further than what is being said. The overall statement makes no claim in the case the premise is false. Look at the actual statement again: “If it is not raining then the kids are playing outside.” No claim is being made about where the kids play if it is raining. So, when it is raining, or \"not A\" is false,  the compound statement is not false, and is therefore true.\n\nThe situation represented by these logically equivalent statements can be summarized in the following diagram:\n\nNow we can have fun with Curry’s Paradox!\n\nWe find ourselves in quite a logical mess if we make a statement about that very statement's truth or falsehood in a compound logical statement, especially one with a nonsensical conclusion. Consider:\n\nThis sentence is false or zero is equal to one.\n\nSet C to represent the statement “this sentence is false” and D to represent the statement “zero is equal to one.” The form of the sentence simplifies to:\n\nC or D.\n\nLooking through our mathematical lens, we produce this truth table as before:\n\nHere is where the logical paradox arises. In rows 1 and 2, C is true. However, C is a statement that refers to its own value. When C is true, this corresponds to saying that the statement “this sentence is false” is true, which means the sentence is false. That is inconsistent with the value in the right-most column.\n\nSomething similar occurs in row 4, where C is false. This corresponds to saying that the statement “this sentence is false” is false, which means that the sentence is true. Again, we see in the right-most column, in row 4, that the full sentence is false in this case. So far, it has all been inconsistent.\n\nWhat about row 3? Well, the entries for \"C\" and \"C or D\" seem to be logically consistent. Great! What about the entry in the column for \"D\"? That corresponds to D being true. Unfortunately, that would mean that the statement \"zero is equal to one\" is true. Eeek! This goes against our broader experience and knowledge, and indeed the foundations of mathematics! So everything is a mess: Indeed, it's a paradox!\n\nBy the way, another common presentation of this paradox is the conditional statement:\n\nIf this sentence is true then zero is equal to one.\n\nIf you are interested in looking at other types of mathematical paradoxes, check out this video on the Banach-Tarski paradox by VSauce:\n\nYou can also check out the “proof” that pi = 4 by Vihart:\n\nAlthough neither of these are a logical paradox like Curry's Paradox, they demonstrate that mathematics is more than just a set of rules that we follow to make intuitive deductions. There is so much more richness to mathematics!\n\nDo you have a favourite mathematical paradox? Is it just impossible to decide? Well, the word “impossible” is not in our vocabulary!\n\nSearch Tags:\n\n###### Featured Posts\n\nOur blog posts moved to Epsilon Stream\n\nJanuary 3, 2019\n\n1/1" ]
[ null ]
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https://mathoverflow.net/questions/236353/compressing-a-hypersurface-on-the-sphere
[ "# Compressing a hypersurface on the sphere\n\nLet $M^n$ be a compact, connected, orientable hypersurface of the unit sphere $S^{n+1} \\subset \\mathbb{R}^{n+2}$. Suppose $M$ is contained in the northern hemisphere $S_+^{n+1}$ and has nonzero principal curvatures everywhere, i.e., has nonzero gaussian curvature everywhere. It seems to me that if we compress $M$ somehow in the direction of the north pole, its principal curvatures will, in absolute value, get arbitrarily large.\n\nIs it true? If so, is there a way to show it without explicitly exhibiting a map $S_+^{n+1} \\to S_+^{n+1}$ that does the job? Instead of compressing $M$ towards the north pole, let us think more generally; is it true that there exists a diffeomorphic copy of $M$ in $S_+^{n+1}$ having prinicipal curvatures say, in absolute value bigger than 1?\n\nThanks for your help and thoughts!\n\n• You can write out the Ptolemaic coordinates on the sphere with an explicit expression for the Riemannian metric, so that dilation in those coordinates gives a very explicit compression toward the north pole. You can see explicitly an orthonormal frame and how it transforms in those coordinates, I think, so you should be able to see how shape operators transform. – Ben McKay Apr 15 '16 at 20:48\n• @BenMcKay What are Ptolemaic coordinates? – Eduardo Longa Apr 15 '16 at 23:25\n• I am not sure which one Ben McKay means specifically, but you can do his construction in either stereographic projection or orthographic projection. – Willie Wong Apr 29 '16 at 19:06" ]
[ null ]
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https://www.splashlearn.com/s/math-worksheets/add-multiples-of-10-and-100-vertical-addition
[ "Home > Math > Add Multiples of 10 and 100: Vertical Addition Worksheet\n\n## Reinforce math concepts by practicing to add multiples of 10 and 100.", null, "Adding a number to 0 results in the number itself. Students love to apply this concept when they add numbers ending in zeros. This worksheet strengthens their accuracy with a set of problems on add multiples of 10 and 100. As the worksheet uses the column method, it is helpful in getting students toward higher accuracy, especially with bigger numbers and in scenarios where regrouping is required.", null, "4413+", null, "4567+", null, "", null, "", null, "" ]
[ null, "https://cdn.splashmath.com/cms_assets/images/playable-left-desc-d0e7c503c7eb99a138cc.svg", null, "https://cdn.splashmath.com/cms_assets/images/playable-right-image-c88d24a6fffd20c6833d.svg", null, "https://cdn.splashmath.com/cms_assets/images/math-and-ela-games-feature-d7f1a6d98b223203d222.svg", null, "https://cdn.splashmath.com/cms_assets/images/math-and-ela-worksheet-feature-56a20bb968cbfa2fe52a.svg", null, "https://cdn.splashmath.com/cms_assets/images/coomon-core-feature-5e0a900656847818fa6d.svg", null, "https://cdn.splashmath.com/cms_assets/images/coopa-feature-8af350a7eecbb0439840.svg", null ]
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https://people.eecs.berkeley.edu/~bh/v3ch6/ai.html
[ "Computer Science Logo Style volume 3: Beyond Programming 2/e Copyright (C) 1997 MIT\n\n# Artificial Intelligence", null, "Program file for this chapter: `student`\n\nCan a computer be intelligent? What would it mean for a computer to be intelligent? John McCarthy, one of the founders of artificial intelligence research, once defined the field as \"getting a computer to do things which, when done by people, are said to involve intelligence.\" The point of the definition was that he felt perfectly comfortable about carrying on his research without first having to defend any particular philosophical view of what the word \"intelligence\" means.\n\nThere have always been two points of view among AI researchers about what their purpose is. One point of view is that AI programs contribute to our understanding of human psychology; when researchers take this view they try to make their programs reflect the actual mechanisms of intelligent human behavior. For example, Allen Newell and Herbert A. Simon begin their classic AI book Human Problem Solving with the sentence, \"The aim of this book is to advance our understanding of how humans think.\" In one of their research projects they studied cryptarithmetic problems, in which digits are replaced with letters in a multi-digit addition or multiplication. First they did a careful observation and analysis of how a human subject attacked such a problem, then they pointed out specific problem-solving techniques that the person used, and used those techniques as the basis for designing a computer simulation. The other point of view is that AI programs provide a more abstract model for intelligence in general; just as one can learn about the properties of computers by studying finite-state machines, even though no real computer operates precisely as a formal finite-state machine does, we can learn about the properties of any possible intelligent being by simulating intelligence in a computer program, whether or not the mechanisms of that program are similar to those used by people.\n\nIn the early days of AI research these two points of view were not sharply divided. Sometimes the same person would switch from one to the other, sometimes trying to model human thought processes and sometimes trying to solve a given problem by whatever methods could be made to work. More recently, researchers who hold one or the other point of view consistently have begun to define two separate fields. One is cognitive science, in which computer scientists join with psychologists, linguists, biologists, and others to study human cognitive psychology, using computer programs as a concrete embodiment of theories about the human mind. The other is called expert systems or knowledge engineering, in which programming techniques developed by AI researchers are put to practical use in programs that solve real-world business problems such as the diagnosis and repair of malfunctioning equipment.\n\n## Microworlds: Student\n\nIn this chapter I'm going to concentrate on one particular area of AI research: teaching a computer to understand English. Besides its inherent interest, this area has the advantage that it doesn't require special equipment, as do some other parts of AI such as machine vision and the control of robot manipulators.\n\nIn the 1950s many people were very optimistic about the use of computers to translate from one language to another. IBM undertook a government-sponsored project to translate scientific journals from Russian to English. At first they thought that this translation could be done very straightforwardly, with a Russian-English dictionary and a few little kludges to rearrange the order of words in a sentence to account for differences in the grammatical structure of the two languages. This simple approach was not successful. One problem is that the same word can have different meanings, and even different parts of speech, in different contexts. (According to one famous anecdote, the program translated the Russian equivalent of \"The spirit is willing but the flesh is weak\" into \"The vodka is strong but the meat is rotten.\")\n\nA decade later, several AI researchers had the idea that ambiguities in the meanings of words could be resolved by trying to understand English only in some limited context. If you know in advance that the sentence you're trying to understand is about baseball statistics, or about relationships in a family tree, or about telling a robot arm to move blocks on a table (these are actual examples of work done in that period) then only certain narrowly defined types of sentences are meaningful at all. You needn't think about metaphors or about the many assumptions about commonsense knowledge that people make in talking with one another. Such a limited context for a language understanding program is called a microworld.\n\nThis chapter includes a Logo version of Student, a program written by Daniel G. Bobrow for his 1964 Ph.D. thesis, Natural Language Input for a Computer Problem Solving System, at MIT. Student is a program that solves algebra word problems:\n\n```? student [The price of a radio is 69.70. If this price is 15 percent\nless than the marked price, find the marked price.]\n\nThe marked price is 82 dollars\n```\n\n(In this illustration I've left out some of Student's display of intermediate results.) The program has two parts: one that translates the word problem into the form of equations and another that solves the equations. The latter part is complex (about 40 Logo procedures) but straightforward; it doesn't seem surprising to most people that a computer can manipulate mathematical equations. It is Student's understanding of English sentences that furthered the cause of artificial intelligence.\n\nThe aim of the research reported here was to discover how one could build a computer program which could communicate with people in a natural language within some restricted problem domain. In the course of this investigation, I wrote a set of computer programs, the Student system, which accepts as input a comfortable but restricted subset of English which can be used to express a wide variety of algebra story problems...\n\nIn the following discussion, I shall use phrases such as \"the computer understands English.\" In all such cases, the \"English\" is just the restricted subset of English which is allowable as input for the computer program under discussion. In addition, for purposes of this report I have adopted the following operational definition of understanding. A computer understands a subset of English if it accepts input sentences which are members of this subset, and answers questions based on information contained in the input. The Student system understands English in this sense. [Bobrow, 1964.]\n\nHow does the algebra microworld simplify the understanding problem? For one thing, Student need not know anything about the meanings of noun phrases. In the sample problem above, the phrase `The price of a radio` is used as a variable name. The problem could just as well have been\n\n```The weight of a giant size detergent box is 69.70 ounces. If this weight\nis 15 percent less than the weight of an enormous size box, find the\nweight of an enormous size box.\n```\n\nFor Student, either problem boils down to\n\n```variable1 = 69.70 units\n\nvariable1 = 0.85 * variable2\n\nFind variable2.\n```\n\nStudent understands particular words only to the extent that they have a mathematical meaning. For example, the program knows that `15 percent less than` means the same as `0.85 times`.\n\n## How Student Translates English to Algebra\n\nStudent translates a word problem into equations in several steps. In the following paragraphs, I'll mention in parentheses the names of the Logo procedures that carry out each step I describe, but don't read the procedures yet. First read through the description of the process without worrying about the programming details of each step. Later you can reread this section while examining the complete listing at the end of the chapter.\n\nIn translating Student to Logo, I've tried not to change the capabilities of the program in any way. The overall structure of my version is similar to that of Bobrow's original implementation, but I've changed some details. I've used iteration and mapping tools to make the program easier to read; I've changed some aspects of the fine structure of the program to fit more closely with the usual Logo programming style; in a few cases I've tried to make exceptionally slow parts of the program run faster by finding a more efficient algorithm to achieve the same goal.\n\nThe top-level procedure `student` takes one input, a list containing the word problem. (The disk file that accompanies this project includes several variables containing sample problems. For example,\n\n```? student :radio\n```\n\nwill carry out the steps I'm about to describe.) Student begins by printing the original problem:\n\n```? student :radio\n\nThe problem to be solved is\n\nThe price of a radio is 69.70. If this price is 15 percent less than the\nmarked price, find the marked price.\n```\n\nThe first step is to separate punctuation characters from the attached words. For example, the word \"`price,`\" in the original problem becomes the two words \"`price ,`\" with the comma on its own. Then (`student1`) certain mandatory substitutions are applied (`idioms`). For example, the phrase `percent less than` is translated into the single word `perless`. The result is printed:\n\n```With mandatory substitutions the problem is\n\nThe price numof a radio is 69.70 dollars . If this price is 15 perless\nthe marked price , find the marked price .\n```\n\n(The word `of` in an algebra word problem can have two different meanings. Sometimes it means \"times,\" as in the phrase \"one half of the population.\" Other times, as in this problem, \"of\" is just part of a noun phrase like \"the price of a radio.\" The special word `numof` is a flag to a later part of the program and will then be further translated either into `times` or back into `of`. The original implementation of Student used, instead of a special word like ``` numof```, a \"tagged\" word represented as a list like `[of / op]`. Other examples of tagging are `[Bill / person]` and `[has / verb]`.)\n\nThe next step is to separate the problem into simple sentences (`bracket`):\n\n```The simple sentences are\n\nThe price numof a radio is 69.70 dollars .\n\nThis price is 15 perless the marked price .\n\nFind the marked price .\n```\n\nUsually this transformation of the problem is straightforward, but the special case of \"age problems\" is recognized at this time, and special transformations are applied so that a sentence like\n\n```Mary is 24 years old.\n```\n\nis translated into\n\n```Mary s age is 24 .\n```\n\nAn age problem is one that contains any of the phrases ```as old as```, `age`, or `years old`.\n\nThe next step is to translate each simple sentence into an equation or a variable whose value is desired as part of the solution (`senform`).\n\n```The equations to be solved are\n\nEqual [price of radio] [product 69.7 [dollars]]\n\nEqual [price of radio] [product 0.85 [marked price]]\n```\n\nThe third simple sentence is translated, not into an equation, but into a request to solve these equations for the variable `marked price`.\n\nThe translation of simple sentences into equations is the most \"intelligent\" part of the program; that is, it's where the program's knowledge of English grammar and vocabulary come into play and many special cases must be considered. In this example, the second simple sentence starts with the phrase `this price`. The program recognizes the word `this` (procedure `nmtest`) and replaces the entire phrase with the left hand side of the previous equation (procedure `this`).\n\n## Pattern Matching\n\nStudent analyzes a sentence by comparing it to several patterns (`senform1`). For example, one sentence form that Student understands is exemplified by these sentences:\n\n```Joe weighs 163 pounds .\nThe United States Army has 8742 officers .\n```\n\nThe general pattern is\n\n```something verb number unit .\n```\n\nStudent treats such sentences as if they were rearranged to match\n\n```The number of unit something verb is number .\n```\n\nand so it generates the equations\n\n```Equal [number of pounds Joe weighs] 163\n\nEqual [number of officers United States Army has] 8742\n```\n\nThe original version of Student was written in a pattern matching language called Meteor, which Bobrow wrote in Lisp. In Meteor, the instruction that handles this sentence type looks like this:\n\n```(* ( (1 / verb) (fn nmtest) 1 (1 / dlm)) 0\n(/ (*s shelf (*k equal (fn opform (*k the number of 4 1 2))\n(fn opform (*k 3 5 6))))) return)\n```\n\nThe top line contains the pattern to be matched. In the pattern, a dollar sign represents zero or more words; the notation `1` represents a single word. The zero at the end of the line means that the text that matches the pattern should be deleted and nothing should replace it. The rest of the instruction pushes a new equation onto a stack named `shelf`; that equation is formed out of the pieces of the matched pattern according to the numbers in the instruction. That is, the number `4` represents the fourth component of the pattern, which is `1`. Here is the corresponding instruction in the Logo version:\n\n```if match [^one !verb1:verb !factor:numberp #stuff1 !:dlm] :sent\n[output (list (list \"equal\nopform (sentence [the number of]\n:stuff1 :one :verb1)\nopform (list :factor) ))]\n```\n\nThe pattern matcher I used for Student is the same as the one in Advanced Techniques, the second volume of this series.* Student often relies on the fact that Meteor's pattern matcher finds the first substring of the text that matches the pattern, rather than requiring the entire text to match. Many patterns in the Logo version therefore take the form\n\n```[^beg interesting part #end]\n```\n\nwhere the \"interesting part\" is all that appeared in the Meteor pattern.\n\n*The version in this project is modified slightly; the `match` procedure first does a fast test to try to reject an irrelevant pattern in O(n) time before calling the actual pattern matcher, which could take as much as O(2n) time to reject a pattern, and which has been renamed `rmatch` (for \"real match\") in this project.\n\nHere is a very brief summary of the Logo pattern matcher included in this program. For a fuller description with examples, please refer to Volume 2. `Match` is a predicate with two inputs, both lists. The first input is the pattern and the second input is the sentence. `Match` outputs `true` if the sentence matches the pattern. A word in the pattern that does not begin with one of the special quantifier characters listed below matches the identical word in the sentence. A word in the pattern that does begin with a quantifier matches zero or more words in the sentence, as follows:\n\n `#` zero or more `&` one or more `?` zero or one `!` exactly one `@` zero or more (test as group) `^` zero or more (as few as possible)\n\nAll quantifiers match as many consecutive words as possible while still allowing the remaining portion of the pattern to be matched, except for `^`. A quantifier may be used alone, or it can be followed by a variable name, a predicate name, or both:\n\n```#\n#var\n#:pred\n#var:pred\n```\nIf a variable name is used, the word or words that match the quantifier will be stored in that variable if the match is successful. (The value of the variable if the match is not successful is not guaranteed.) If a predicate is used, it must take one word as input; in order for a word in the sentence to be accepted as (part of) a match for the quantifier, the predicate must output `true` when given that word as input. For example, the word\n\n```!factor:numberp\n```\n\nin the pattern above requires exactly one matching word in the sentence; that word must be a number, and it is remembered in the variable `factor`. If the quantifier is `@` then the predicate must take a list as input, and it must output `true` for all the candidate matching words taken together as a list. For example, if you define a procedure\n\n```to threep :list\noutput equalp count :list 3\nend\n```\n\nthen the pattern word\n\n```@:threep\n```\n\nwill match exactly three words in the sentence. (Student does not use this last feature of the pattern matcher. In fact, predicates are applied only to the single-word quantifiers `?` and `!`.)\n\nPattern matching is also heavily used in converting words and phrases with mathematical meaning into the corresponding arithmetic operations (`opform`). An equation is a list of three members; the first member is the word `equal` and the other two are expressions formed by applying operations to variables and numbers. Each operation that is required is represented as a list whose first member is the name of the Logo procedure that carries out the operation and whose remaining members are expressions representing the operands. For example, the equation\n\ny = 3x2 + 6x − 1\n\nwould be represented by the list\n\n```[equal [y] [sum [product 3 [square [x]]] [product 6 [x]] [minus 1]]]\n```\n\nThe variables are represented by lists like `[x]` rather than just the words because in Student a variable can be a multi-word phrase like `price of radio`. The difference between two expressions is represented by a `sum` of one expression and `minus` the other, rather than as the `difference` of the expressions, because this representation turns out to make the process of simplifying and solving the equations easier.\n\nIn word problems, as in arithmetic expressions, there is a precedence of operations. Operations like `squared` apply to the variables right next to them; ones like `times` are intermediate, and ones like `plus` apply to the largest possible subexpressions. Student looks first for the lowest-priority ones like `plus`; if one is found, the entire rest of the clause before and after the operation word provide the operands. Those operands are recursively processed by `opform`; when all the low-priority operations have been found, the next level of priority will be found by matching the pattern\n\n```[^left !op:op1 #right]\n```\n\n## Solving the Equations\n\nStudent uses the substitution technique to solve the equations. That is, one equation is rearranged so that the left hand side contains only a single variable and the right hand side does not contain that variable. Then, in some other equation, every instance of that variable is replaced by the right hand side of the first equation. The result is a new equation from which one variable has been eliminated. Repeating this process enough times should eventually yield an equation with only a single variable, which can be solved to find the value of that variable.\n\nWhen a problem gives rise to several linear equations in several variables, the traditional technique for computer solution is to use matrix inversion; this technique is messy for human beings because there is a lot of arithmetic involved, but straightforward for computers because the algorithm can be specified in a simple way that doesn't depend on the particular equations in each problem. Bobrow chose to use the substitution method because some problems give rise to equations that are linear in the variable for which a solution is desired but nonlinear in other variables. Consider this problem:\n\n```? student :tom\n\nThe problem to be solved is\n\nIf the number of customers Tom gets is twice the square of 20 per cent of\nruns is 45, what is the number of customers Tom gets?\n\nWith mandatory substitutions the problem is\n\nIf the number numof customers Tom gets is 2 times the square 20 percent\nnumof the number numof advertisements he runs , and the number numof\nadvertisements he runs is 45 , what is the number numof customers\nTom gets ?\n\nThe simple sentences are\n\nThe number numof customers Tom gets is 2 times the square 20 percent\n\nWhat is the number numof customers Tom gets ?\n\nThe equations to be solved are\n\nEqual [number of customers Tom gets]\nhe runs]]]]\n\nThe number of customers Tom gets is 162\n\nThe problem is solved.\n```\n\nThe first equation that Student generates for this problem is linear in the number of customers Tom gets, but nonlinear in the number of advertisements he runs. (That is, the equation refers to the square of the latter variable. An equation is linear in a given variable if that variable isn't multiplied by anything other than a constant number.) Using the substitution method, Student can solve the problem by substituting the value 45, found in the second equation, for the number of advertisements variable in the first equation.\n\n(Notice, in passing, that one of the special `numof` words in this problem was translated into a multiplication rather than back into the original word `of`.)\n\nThe actual sequence of steps required to solve a set of equations is quite intricate. I recommend taking that part of Student on faith the first time you read the program, concentrating instead on the pattern matching techniques used to translate the English sentences into equations. But here is a rough guide to the solution process. Both `student1` and ``` student2``` call `trysolve` with four inputs: a list of the equations to solve, a list of the variables for which values are wanted, and two lists of units. A unit is a word or phrase like `dollars` or `feet` that may be part of a solution. Student treats units like variables while constructing the equations, so the combination of a number and a unit is represented as a product, like\n\n```[product 69.7 [dollars]]\n```\n\nfor 69.70 in the first sample problem. While constructing the equations, Student generates two lists of units. The first, stored in the variable `units`, contains any word or phrase that appears along with a number in the problem statement, like the word `feet` in the phrase ``` 3 feet``` (`nmtest`). The second, in the variable `aunits`, contains units mentioned explicitly in the `find` or `how many` sentences that tell Student what variables should be part of the solution (`senform1`). If the problem includes a sentence like\n\n```How many inches is a yard?\n```\n\nthen the variable `[inches]`, and only that variable, is allowed to be part of the answer. If there are no `aunits`-type variables in the problem, then any of the `units` variables may appear in the solution (`trysolve`).\n\n`Trysolve` first calls `solve` to solve the equations and then uses `pranswers` to print the results. `Solve` calls `solver` to do most of the work and then passes its output through `solve.reduce` for some final cleaning up. `Solver` works by picking one of the variables from the list `:wanted` and asking `solve1` to find a solution for that variable in terms of all the other variables--the other wanted variables as well as the units allowed in the ultimate answer. If `solve1` succeeds, then `solver` invokes itself, adding the newly-found expression for one variable to an association list (in the variable `alis`) so that, from then on, any occurrence of that variable will be replaced with the equivalent expression. In effect, the problem is simplified by eliminating one variable and eliminating one equation, the one that was solved to find the equivalent expression.\n\n`Solve1` first looks for an equation containing the variable for which it is trying to find a solution. When it finds such an equation, the next task is to eliminate from that equation any variables that aren't part of the wanted-plus-units list that `solver` gave `solve1` as an input. To eliminate these extra variables, `solve1` invokes `solver` with the extras as the list of wanted variables. This mutual recursion between `solver` and `solve1` makes the structure of the solution process difficult to follow. If `solver` manages to eliminate the extra variables by expressing them in terms of the originally wanted ones, then `solve1` can go on to substitute those expressions into its originally chosen equation and then use `solveq` to solve that one equation for the one selected variable in terms of all the other allowed variables. ``` Solveq``` manipulates the equation more or less the way students in algebra classes do, adding the same term to both sides, multiplying both sides by the denominator of a polynomial fraction, and so on.\n\nHere is how `solve` solves the radio problem. The equations, again, are\n\n```Equal [price of radio] [product 69.7 [dollars]]\n\nEqual [price of radio] [product 0.85 [marked price]]\n```\n\n`Trysolve` evaluates the expression\n\n```(1) solve [[marked price]]\n[[equal [price of radio] [product 69.7 [dollars]]]\n[equal [price of radio] [product 0.85 [marked price]]] ]\n[[dollars]]\n```\n\n(I'm numbering these expressions so that I can refer to them later in the text.) The first input to `solve` is the list of variables wanted in the solution; in this case there is only one such variable. The second input is the list of two equations. The third is the list of unit variables that are allowed to appear in the solution; in this case only ``` [dollars]``` is allowed. `Solve` evaluates\n\n```(2) solver [[marked price]] [[dollars]] [] []\n```\n\n(There is a fifth input, the word `insufficient`, but this is used only as an error flag if the problem can't be solved. To simplify this discussion I'm going to ignore that input for both `solver` and ``` solve1```.) `Solver` picks the first (in this case, the only) wanted variable as the major input to `solve1`:\n\n```(3) solve1 [marked price]\n[[dollars]]\n[]\n[[equal [price of radio] [product 69.7 [dollars]]]\n[equal [price of radio] [product 0.85 [marked price]]] ]\n[]\n```\n\nNotice that the first input to `solve1` is a single variable, not a list of variables. `Solve1` examines the first equation in the list of equations making up its fourth input. The desired variable does not appear in this equation, so `solve1` rejects that equation and invokes itself recursively:\n\n```(4) solve1 [marked price]\n[[dollars]]\n[]\n[[equal [price of radio] [product 0.85 [marked price]]]]\n[[equal [price of radio] [product 69.7 [dollars]]]]\n```\n\nThis time, the first (and now only) equation on the list of candidates does contain the desired variable. `Solve1` removes that equation, not from its own list of equations (`:eqns`), but from ``` solve```'s overall list (`:eqt`). The equation, unfortunately, can't be solved directly to express `[marked price]` in terms of `[dollars]`, because it contains the extra, unwanted variable `[price of radio]`. We must eliminate this variable by solving the remaining equations for it:\n\n```(5) solver [[price of radio]] [[marked price] [dollars]] [] []\n```\n\nAs before, `solver` picks the first (again, in this case, the only) wanted variable and asks `solve1` to solve it:\n\n```(6) solve1 [price of radio]\n[[marked price] [dollars]]\n[]\n[[equal [price of radio] [product 69.7 [dollars]]]]\n[]\n```\n\n`Solve1` does find the desired variable in the first (and only) equation, and this time there are no extra variables. `Solve1` can therefore ask `solveq` to solve the equation:\n\n```(7) solveq [price of radio]\n[equal [price of radio] [product 69.7 [dollars]]]\n```\n\nIt isn't part of `solveq`'s job to worry about which variables may or may not be part of the solution; `solve1` doesn't call ``` solveq``` until it's satisfied that the equation is okay.\n\nIn this case, `solveq` has little work to do because the equation is already in the desired form, with the chosen variable alone on the left side and an expression not containing that variable on the right.\n\n```solveq (7) outputs [[price of radio] [product 69.7 [dollars]]\nto solve1 (6)\n```\n\n`Solve1` appends this result to the previously empty association list.\n\n```solve1 (6) outputs [[[price of radio] [product 69.7 [dollars]]]\nto solver (5)\n```\n\n`Solver` only had one variable in its `:wanted` list, so its job is also finished.\n\n```solver (5) outputs [[[price of radio] [product 69.7 [dollars]]]\nto solve1 (4,3)\n```\n\nThis outer invocation of `solve1` was trying to solve for `[marked price]` an equation that also involved `[price of radio]`. It is now able to use the new association list to substitute for this unwanted variable an expression in terms of wanted variables only; this modified equation is then passed on to `solveq`:\n\n```(8) solveq [marked price]\n[equal [product 69.7 [dollars]] [product 0.85 [marked price]]]\n```\n\nThis time `solveq` has to work a little harder, exchanging the two sides of the equation and dividing by 0.85.\n\n```solveq (8) outputs [[marked price] [product 82 [dollars]]]\nto solve1 (4,3)\n```\n\n`Solve1` appends this result to the association list:\n\n```solve1 (4,3) outputs [[[price of radio] [product 69.7 [dollars]]]\n[[marked price] [product 82 [dollars]]] ]\nto solver (2)\n```\n\nSince `solver` has no other wanted variables, it outputs the same list to `solve`, and `solve` outputs the same list to ``` trysolve```. (In this example, `solve.reduce` has no effect because all of the expressions in the association list are in terms of allowed units only. If the equations had been different, the expression for ```[price of radio]``` might have included `[marked price]` and then ``` solve.reduce``` would have had to substitute and simplify (`subord`).)\n\nIt'll probably take tracing a few more examples and beating your head against the wall a bit before you really understand the structure of ``` solve``` and its subprocedures. Again, don't get distracted by this part of the program until you've come to understand the language processing part, which is our main interest in this chapter.\n\n## Age Problems\n\nThe main reason why Student treats age problems specially is that the English form of such problems is often expressed as if the variables were people, like \"Bill,\" whereas the real variable is \"Bill's age.\" The pattern matching transformations look for proper names (`personp`) and insert the words `s age` after them (`ageify`). The first such age variable in the problem is remembered specially so that it can be substituted for pronouns (`agepron`). A special case is the phrase ``` their ages```, which is replaced (`ageprob`) with a list of all the age variables in the problem.\n\n```? student :uncle\n\nThe problem to be solved is\n\nBill's father's uncle is twice as old as Bill's father. 2 years from now\nBill's father will be 3 times as old as Bill. The sum of their ages is\n92 . Find Bill's age.\n\nWith mandatory substitutions the problem is\n\nBill s father s uncle is 2 times as old as Bill s father . 2 years\nfrom now Bill s father will be 3 times as old as Bill . sum their\nages is 92 . Find Bill s age .\n\nThe simple sentences are\n\nBill s father s uncle s age is 2 times Bill s father s age .\n\nBill s father s age pluss 2 is 3 times Bill s age pluss 2 .\n\nSum Bill s age and Bill s father s age and Bill s father s uncle s age\nis 92 .\n\nFind Bill s age .\n\nThe equations to be solved are\n\nEqual [Bill s father s uncle s age] [product 2 [Bill s father s age]]\n\nEqual [sum [Bill s father s age] 2] [product 3 [sum [Bill s age] 2]]\n\nEqual [sum [Bill s age]\n[sum [Bill s father s age] [Bill s father s uncle s age]]] 92\n\nBill s age is 8\n\nThe problem is solved.\n```\n\n(Note that in the original problem statement there is a space between the number `92` and the following period. I had to enter the problem in that form because of an inflexibility in Logo's input parser, which assumes that a period right after a number is part of the number, so that \"`92.`\" is reformatted into `92` without the dot.)\n\nStudent represents the possessive word `Bill's` as the two words `Bill s` because this representation allows the pattern matcher to manipulate the possessive marker as a separate element to be matched. A phrase like `as old as` is just deleted (`ageprob`) because the transformation from people to ages makes it redundant.\n\nThe phrase `2 years from now` in the original problem is first translated to `in 2 years`. This phrase is further processed according to where it appears in a sentence. When it is attached to a particular variable, in a phrase like `Bill s age in 2 years`, the entire phrase is translated into the arithmetic operation `Bill s age pluss 2 years` (`agewhen`). (The special word `pluss` is an addition operator, just like `plus`, except for its precedence; `opform` treats it as a tightly binding operation like `squared` instead of a loosely binding one like the ordinary `plus`.) When a phrase like `in 2 years` appears at the beginning of a sentence, it is remembered (`agesen`) as an implicit modifier for every age variable in that sentence that isn't explicitly modified. In this example, `in 2 years` modifies both `Bill s father s age` and `Bill s age`. The special precedence of `pluss` is needed in this example so that the equation will be based on the grouping\n\n```3 times [ Bill s age pluss 2 ]\n```\n\nrather than\n\n```[ 3 times Bill s age ] plus 2\n```\n\nas it would be with the ordinary `plus` operator. You can also see how the substitution for `their ages` works in this example.\n\nHere is a second sample age problem that illustrates a different kind of special handling:\n\n```? student :ann\n\nThe problem to be solved is\n\nMary is twice as old as Ann was when Mary was as old as Ann is now. If\nMary is 24 years old, how old is Ann?\n\nWith mandatory substitutions the problem is\n\nMary is 2 times as old as Ann was when Mary was as old as Ann is now . If\nMary is 24 years old , what is Ann ?\n\nThe simple sentences are\n\nMary s age is 2 times Ann s age minuss g1 .\n\nMary s age minuss g1 is Ann s age .\n\nMary s age is 24 .\n\nWhat is Ann s age ?\n\nThe equations to be solved are\n\nEqual [Mary s age] [product 2 [sum [Ann s age] [minus [g1]]]]\n\nEqual [sum [Mary s age] [minus [g1]]] [Ann s age]\n\nEqual [Mary s age] 24\n\nAnn s age is 18\n\nThe problem is solved.\n```\n\nWhat is new in this example is Student's handling of the phrase ```was when``` in the sentence\n\n```Mary is 2 times as old as Ann was when Mary was as old as Ann is now .\n```\n\nSentences like this one often cause trouble for human algebra students because they make implicit reference to a quantity that is not explicitly present as a variable. The sentence says that Mary's age now is twice Ann's age some number of years ago, but that number is not explicit in the problem. Student makes this variable explicit by using a generated symbol like the word `g1` in this illustration. Student replaces the phrase `was when` with the words\n\n```was g1 years ago . g1 years ago\n```\n\nThis substitution (in `ageprob`) happens before the division of the problem statement into simple sentences (`bracket`). As a result, this one sentence in the original problem becomes the two sentences\n\n```Mary s age is 2 times Ann s age g1 years ago .\n\nG1 years ago Mary s age was Ann s age now .\n```\n\nThe phrase `g1 years ago` in each of these sentences is further processed by `agesen` and `agewhen` as discussed earlier; the final result is\n\n```Mary s age is 2 times Ann s age minuss g1 .\n\nMary s age minuss g1 is Ann s age .\n```\n\nA new generated symbol is created each time this situation arises, so there is no conflict from trying to use the same variable name for two different purposes. The phrase `will be when` is handled similarly, except that the translated version is\n\n```in g2 years . in g2 years\n```\n\n## AI and Education\n\nThese decoupling heuristics are useful not only for the Student program but for people trying to solve age problems. The classic age problem about Mary and Ann, given above, took an MIT graduate student over 5 minutes to solve because he did not know this heuristic. With the heuristic he was able to set up the appropriate equations much more rapidly. As a crude measure of Student's relative speed, note that Student took less than one minute to solve this problem.\n\nThis excerpt from Bobrow's thesis illustrates the idea that insights from artificial intelligence research can make a valuable contribution to the education of human beings. An intellectual problem is solved, at least in many cases, by dividing it into pieces and developing a technique for each subproblem. The subproblems are the same whether it is a computer or a person trying to solve the problem. If a certain technique proves valuable for the computer, it may be helpful for a human problem solver to be aware of the computer's methods. Bobrow's suggestion to teach people one specific heuristic for algebra word problems is a relatively modest example of this general theme. (A heuristic is a rule that gives the right answer most of the time, as opposed to an algorithm, a rule that always works.) Some researchers in cognitive science and education have proposed the idea of intelligent CAI (computer assisted instruction), in which a computer would be programmed as a \"tutor\" that would observe the efforts of a student in solving a problem. The tutor would know about some of the mistaken ideas people can have about a particular class of problem and would notice a student falling into one of those traps. It could then offer advice tailored to the needs of that individual student.\n\nThe development of the Logo programming language (and so also, indirectly, this series of books) is another example of the relationship between AI and education. Part of the idea behind Logo is that the process of programming a computer resembles, in some ways, the process of teaching a person to do something. (This can include teaching oneself.) For example, when a computer program doesn't work, the experienced programmer doesn't give up in despair, but instead debugs the program. Yet many students are willing to give up and say \"I just don't get it\" if their understanding of some problem isn't perfect on the first try.\n\nThe critic is afraid that children will adopt the computer as model and eventually come to \"think mechanically\" themselves. Following the opposite tack, I have invented ways to take educational advantage of the opportunities to master the art of deliberately thinking like a computer, according, for example, to the stereotype of a computer program that proceeds in a step-by-step, literal, mechanical fashion. There are situations where this style of thinking is appropriate and useful. Some children's difficulties in learning formal subjects such as grammar or mathematics derive from their inability to see the point of such a style.\n\nA second educational advantage is indirect but ultimately more important. By deliberately learning to imitate mechanical thinking, the learner becomes able to articulate what mechanical thinking is and what it is not. The exercise can lead to greater confidence about the ability to choose a cognitive style that suits the problem. Analysis of \"mechanical thinking\" and how it is different from other kinds and practice with problem analysis can result in a new degree of intellectual sophistication. By providing a very concrete, down-to-earth model of a particular style of thinking, work with the computer can make it easier to understand that there is such a thing as a \"style of thinking.\" And giving children the opportunity to choose one style or another provides an opportunity to develop the skill necessary to choose between styles. Thus instead of inducing mechanical thinking, contact with computers could turn out to be the best conceivable antidote to it. And for me what is most important in this is that through these experiences these children would be serving their apprenticeships as epistemologists, that is to say learning to think articulately about thinking. [Seymour Papert, Mindstorms, Basic Books, 1980, p. 27.]\n\n## Combining Sentences Into One Equation\n\nIn age problems, as we've just seen, a single sentence may give rise to two equations. Here is an example of the opposite, several sentences that together contribute a single equation.\n\n```? student :nums\n\nThe problem to be solved is\n\nA number is multiplied by 6 . This product is increased by 44 . This\nresult is 68 . Find the number.\n\nWith mandatory substitutions the problem is\n\nA number ismulby 6 . This product is increased by 44 . This result is\n68 . Find the number .\n\nThe simple sentences are\n\nA number ismulby 6 .\n\nThis product is increased by 44 .\n\nThis result is 68 .\n\nFind the number .\n\nThe equations to be solved are\n\nEqual [sum [product [number] 6] 44] 68\n\nThe number is 4\n\nThe problem is solved.\n```\n\nStudent recognizes problems like this by recognizing the phrases \"is multiplied by,\" \"is divided by,\" and \"is increased by\" (`senform1`). A sentence containing one of these phrases is not translated into an equation; instead, a partial equation is saved until the next sentence is read. That next sentence is expected to start with a phrase like \"this result\" or \"this product.\" The same procedure (`this`) that in other situations uses the left hand side of the last equation as the expression for the `this`-phrase notices that there is a remembered partial equation and uses that instead. In this example, the sentence\n\n```A number ismulby 6 .\n```\n\nremembers the algebraic expression\n\n```[product [number] 6]\n```\n\nThe second sentence uses that remembered expression as part of a new, larger expression to be remembered:\n\n```[sum [product [number] 6] 44]\n```\n\nThe third sentence does not contain one of the special \"is increased by\" phrases, but is instead a standard \"A is B\" sentence. That sentence, therefore, does give rise to an equation, as shown above.\n\nPerhaps the most interesting thing to notice about this category of word problem is how narrowly defined Student's criterion for recognizing the category is. Student gets away with it because algebra word problems are highly stereotyped; there are just a few categories, with traditional, standard wordings. In principle there could be a word problem starting\n\n```Robert has a certain number of jelly beans. This number is twice the\nnumber of jelly beans Linda has.\n```\n\nThese two sentences are together equivalent to\n\n```The number of jelly beans Robert has is twice the number of jelly beans\nLinda has.\n```\n\nBut Student would not recognize the situation because the first sentence doesn't talk about \"is increased by.\" We could teach Student to understand a word problem in this form by adding the instruction\n\n```if match [^one !verb1:verb a certain number of #stuff1 !:dlm] :sent\n[push \"ref opform (se [the number of] :stuff1 :one :verb1)\nop []]\n```\n\nalong with the other known sentence forms in `senform1`. (Compare this to the pattern matching instruction shown earlier for a similar sentence but with an explicitly specified number.)\n\nTaking advantage of the stereotyped nature of word problems is an example of how the microworld strategy helped make the early AI programs possible. If word problems were expressed with all the flexibility of language in general, Student would need many more sentence patterns than it actually has. (How many different ways can you think of to express the same idea about Robert and Linda? How many of those ways can Student handle?)\n\n## Allowing Flexible Phrasing\n\nIn the examples we've seen so far, Student has relied on the repetition of identical or near-identical phrases such as \"the marked price\" or \"the number of advertisements he runs.\" (The requirement is not quite strictly identical phrases because articles are removed from the noun phrases to make variable names.) In real writing, though, such phrases are often abbreviated when they appear for a second time. Student will translate such a problem into a system of equations that can't be solved, because what should be one variable is instead a different variable in each equation. But Student can recognize this situation and apply heuristic rules to guess that two similar variable names are meant, in fact, to represent the same variable. (Some early writers on AI considered the use of heuristic methods one of the defining characteristics of the field. Computer scientists outside of AI were more likely to insist on fully reliable algorithms. This distinction still has some truth to it, but it isn't emphasized so much as a critical issue these days.) Student doesn't try to equate different variables until it has first tried to solve the equations as they are originally generated. If the first attempt at solution fails, Student has recourse to less certain techniques (`student2` calls `vartest`).\n\n```? student :sally\n\nThe problem to be solved is\n\nThe sum of Sally's share of some money and Frank's share is 4.50.\nSally's share is twice Frank's. Find Frank's and Sally's share.\n\nWith mandatory substitutions the problem is\n\nsum Sally s share numof some money and Frank s share is 4.50 dollars .\nSally s share is 2 times Frank s . Find Frank s and Sally s share .\n\nThe simple sentences are\n\nSum Sally s share numof some money and Frank s share is 4.50 dollars .\n\nSally s share is 2 times Frank s .\n\nFind Frank s and Sally s share .\n\nThe equations to be solved are\n\nEqual [sum [Sally s share of some money] [Frank s share]]\n[product 4.50 [dollars]]\n\nEqual [Sally s share] [product 2 [Frank s]]\n\nThe equations were insufficient to find a solution.\n\nAssuming that\n[Frank s] is equal to [Frank s share]\n\nAssuming that\n[Sally s share] is equal to [Sally s share of some money]\n\nFrank s is 1.5 dollars\n\nSally s share is 3 dollars\n\nThe problem is solved.\n```\n\nIn this problem Student has found two pairs of similar variable names. When it finds such a pair, Student adds an equation of the form\n\n```[equal variable1 variable2]\n```\n\nto the previous set of equations. In both of the pairs in this example, the variable that appears later in the problem statement is entirely contained within the one that appears earlier.\n\nAnother point of interest in this example is that the variable `[dollars]` is included in the list of units that may be part of the answer. The word problem does not explicitly ask \"How many dollars is Sally's share,\" but because one of the sentences sets an expression equal to \"4.50 dollars\" Student takes that as implicit permission to express the answer in dollars.\n\nThe only other condition under which Student will consider two variables equal is if their names are identical except that some phrase in the one that appears earlier is replaced with a pronoun in the one that appears later. That is, a variable like ```[the number of ice cream cones the children eat]``` will be considered equal to a later variable ```[the number of ice cream cones they eat]```. Here is a problem in which this rule is applied:\n\n```? student :guns\n\nThe problem to be solved is\n\nThe number of soldiers the Russians have is one half of the number of\nguns they have. They have 7000 guns. How many soldiers do they have?\n\nWith mandatory substitutions the problem is\n\nThe number numof soldiers the Russians have is 0.5 numof the number numof\nguns they have . They have 7000 guns . howm soldiers do they have ?\n\nThe simple sentences are\n\nThe number numof soldiers the Russians have is 0.5 numof the number numof\nguns they have .\n\nThey have 7000 guns .\n\nHowm soldiers do they have ?\n\nThe equations to be solved are\n\nEqual [number of soldiers Russians have]\n[product 0.5 [number of guns they have]]\n\nEqual [number of guns they have] 7000\n\nThe equations were insufficient to find a solution.\n\nAssuming that\n[number of soldiers they have] is equal to\n[number of soldiers Russians have]\n\nThe number of soldiers they have is 3500\n\nThe problem is solved.\n```\n\n## Using Background Knowledge\n\nIn some word problems, not all of the necessary information is contained within the problem statement itself. The problem requires the student to supply some piece of general knowledge about the world in order to determine the appropriate equations. This knowledge may be about unit conversions (one foot is 12 inches) or about relationships among physical quantities (distance equals speed times time). Student \"knows\" some of this background information and can apply it (`geteqns`) if the equations determined by the problem statement are insufficient.\n\n```? student :jet\n\nThe problem to be solved is\n\nThe distance from New York to Los Angeles is 3000 miles. If the average\nspeed of a jet plane is 600 miles per hour, find the time it takes to\ntravel from New York to Los Angeles by jet.\n\nWith mandatory substitutions the problem is\n\nThe distance from New York to Los Angeles is 3000 miles . If the average\nspeed numof a jet plane is 600 miles per hour , find the time it takes to\ntravel from New York to Los Angeles by jet .\n\nThe simple sentences are\n\nThe distance from New York to Los Angeles is 3000 miles .\n\nThe average speed numof a jet plane is 600 miles per hour .\n\nFind the time it takes to travel from New York to Los Angeles by jet .\n\nThe equations to be solved are\n\nEqual [distance from New York to Los Angeles] [product 3000 [miles]]\n\nEqual [average speed of jet plane]\n[quotient [product 600 [miles]] [product 1 [hours]]]\n\nThe equations were insufficient to find a solution.\n\nUsing the following known relationships\n\nEqual [distance] [product [speed] [time]]\n\nEqual [distance] [product [gas consumption]\n[number of gallons of gas used]]\n\nAssuming that\n[speed] is equal to [average speed of jet plane]\n\nAssuming that\n[time] is equal to [time it takes to travel\nfrom New York to Los Angeles by jet]\n\nAssuming that\n[distance] is equal to [distance from New York to Los Angeles]\n\nThe time it takes to travel from New York\nto Los Angeles by jet is 5 hours\n\nThe problem is solved.\n```\n\nStudent's library of known relationships is indexed according to the first word of the name of each variable involved in the relationship. (If a variable starts with the words `number of` it is indexed under the following word.) The relationships, in the form of equations, are stored in the property lists of these index words.\n\nProperty lists are also used to keep track of irregular plurals and the corresponding singulars. Student tries to keep all units in plural form internally, so that if a problem refers to both `1 foot` and ``` 2 feet``` the same variable name will be used for both. (That is, the first of these will be translated into\n\n```[product 1 [feet]]\n```\n\nin Student's internal representation. Then the opposite translation is needed if the product of `1` and some unit appears in an answer to be printed.\n\nThe original Student also used property lists to remember the parts of speech of words and the precedence of operators, but because of differences in the syntax of the Meteor pattern matcher and my Logo pattern matcher I've found it easier to use predicate operations for that purpose.\n\nThe original Student system included a separately invoked `remember` procedure that allowed all these kinds of global information to be entered in the form of English sentences. You'd say\n\n```Feet is the plural of foot\n```\n\nor\n\n```Distance equals speed times time\n```\n\nand `remember` would use patterns much like those used in understanding word problems to translate these sentences into `pprop` instructions. Since Lisp programs, like Logo programs, can themselves be manipulated as lists, `remember` could even accept information of a kind that's stored in the Student program itself, such as the wording transformations in ``` idioms```, and modify the program to reflect this information. I haven't bothered to implement that part of the Student system because it takes up extra memory and doesn't exhibit any new techniques.\n\nAs the above example shows, it's important that Student's search for relevant known relationships comes before the attempt to equate variables with similar names. The general relationship that uses a variable named simply `[distance]` doesn't help unless Student can identify it as relevant to the variable named `[distance from New York to Los Angeles]` in the specific problem under consideration.\n\nHere is another example in which known relationships are used:\n\n```? student :span\n\nThe problem to be solved is\n\nIf 1 span is 9 inches, and 1 fathom is 6 feet,\nhow many spans is 1 fathom?\n\nWith mandatory substitutions the problem is\n\nIf 1 span is 9 inches , and 1 fathom is 6 feet , howm spans is 1 fathom ?\n\nThe simple sentences are\n\n1 span is 9 inches .\n\n1 fathom is 6 feet .\n\nHowm spans is 1 fathom ?\n\nThe equations to be solved are\n\nEqual [product 1 [spans]] [product 9 [inches]]\n\nEqual [product 1 [fathoms]] [product 6 [feet]]\n\nEqual g2 [product 1 [fathoms]]\n\nThe equations were insufficient to find a solution.\n\nUsing the following known relationships\n\nEqual [product 1 [yards]] [product 3 [feet]]\n\nEqual [product 1 [feet]] [product 12 [inches]]\n\n1 fathom is 8 spans\n\nThe problem is solved.\n```\n\nBesides the use of known relationships, this example illustrates two other features of Student. One is the use of an explicitly requested unit in the answer. Since the problem asks\n\n```How many spans is 1 fathom?\n```\n\nStudent knows that the answer must be expressed in `spans`. Had there been no explicit request for a particular unit, all the units that appear in phrases along with a number would be eligible to appear in the answer: `inches`, `feet`, and `fathoms`. Student might then blithely inform us that\n\n```1 fathom is 1 fathom\n\nThe problem is solved.\n```\n\nThe other new feature demonstrated by this example is the use of a generated symbol to represent the desired answer. In the statement of this problem, there is no explicit variable representing the unknown. `[Fathoms]` is a unit, not a variable for which a value could be found. The problem asks for the value of the expression\n\n```[product 1 [fathoms]]\n```\n\nin terms of spans. Student generates a variable name (`g2`) to represent the unknown and produces an equation\n\n```[equal g2 [product 1 [fathoms]]\n```\n\nto add to the list of equations. A generated symbol will be needed whenever the \"Find\" or \"What is\" sentence asks for an expression rather than a simple variable name. For example, an age problem that asks \"What is the sum of their ages\" would require the use of a generated symbol. (The original Student always used a generated symbol for the unknowns, even if there was already a single variable in the problem representing an unknown. It therefore had equations like\n\n```[equal g3 [marked price]]\n```\n\nin its list, declaring one variable equal to another. I chose to check for this case and avoid the use of a generated symbol because the time spent in the actual solution of the equations increases quadratically with the number of equations.)\n\n## Optional Substitutions\n\nWe have seen many cases in which Student replaces a phrase in the statement of a problem with a different word or phrase that fits better with the later stages of processing, like the substitution of `2 times` for `twice` or a special keyword like `perless` for `percent less than`. Student also has a few cases of optional substitutions that may or may not be made (`tryidiom`).\n\nThere are two ways in which optional substitutions can happen. One is exemplified by the phrase `the perimeter of the rectangle`. Student first attempts the problem without any special processing of this phrase. If a solution is not found, Student then replaces the phrase with ```twice the sum of the length and width of the rectangle``` and processes the resulting new problem from the beginning. Unlike the use of known relationships or similarity of variable names, which Student handles by adding to the already-determined equations, this optional substitution requires the entire translation process to begin again. For example, the word `twice` that begins the replacement phrase will be further translated to `2 times`.\n\nThe second category of optional substitution is triggered by the phrase ``` two numbers```. This phrase must always be translated to something, because it indicates that two different variables are needed. But the precise translation depends on the wording of the rest of the problem. Student tries two alternative translations: ```one of the numbers and the other number``` and `one number and the other number`. Here is an example in which the necessary translation is the one Student tries second:\n\n```? student :sumtwo\n\nThe problem to be solved is\n\nThe sum of two numbers is 96, and one number is 16 larger than the other\nnumber. Find the two numbers.\n\nThe problem with an idiomatic substitution is\n\nThe sum of one of the numbers and the other number is 96 , and one\nnumber is16 larger than the other number . Find the one of the numbers\nand the other number .\n\nWith mandatory substitutions the problem is\n\nsum one numof the numbers and the other number is 96 , and one number\nis 16 plus the other number . Find the one numof the numbers and the\nother number .\n\nThe simple sentences are\n\nSum one numof the numbers and the other number is 96 .\n\nOne number is 16 plus the other number .\n\nFind the one numof the numbers and the other number .\n\nThe equations to be solved are\n\nEqual [sum [one of numbers] [other number]] 96\n\nEqual [one number] [sum 16 [other number]]\n\nThe equations were insufficient to find a solution.\n\nThe problem with an idiomatic substitution is\n\nThe sum of one number and the other number is 96 , and one number is 16\nlarger than the other number . Find the one number and the other number .\n\nWith mandatory substitutions the problem is\n\nsum one number and the other number is 96 , and one number is 16 plus the\nother number . Find the one number and the other number .\n\nThe simple sentences are\n\nSum one number and the other number is 96 .\n\nOne number is 16 plus the other number .\n\nFind the one number and the other number .\n\nThe equations to be solved are\n\nEqual [sum [one number] [other number]] 96\n\nEqual [one number] [sum 16 [other number]]\n\nThe one number is 56\n\nThe other number is 40\n\nThe problem is solved.\n```\n\nThere is no essential reason why Student uses one mechanism rather than another to deal with a particular problematic situation. The difficulties about perimeters and about the phrase \"two numbers\" might have been solved using mechanisms other than this optional substitution one. For example, the equation\n\n```[equal [perimeter] [product 2 [sum [length] [width]]]]\n```\n\nmight have been added to the library of known relationships. The difficulty about alternate phrasings for \"two numbers\" could be solved by adding\n\n```[[one of the !word:pluralp] [\"one singular :word]]\n```\n\nto the list of idiomatic substitutions in `idiom`.\n\nNot all the mechanisms are equivalent, however. The \"two numbers\" problem couldn't be solved by adding equations to the library of known relationships, because that phrase appears as part of a larger phrase like \"the sum of two numbers,\" and Student's understanding of the word `sum` doesn't allow it to be part of a variable name. The word `sum` only makes sense to Student in the context of a phrase like ```the sum of something and something else```. (See procedure `tst.sum`.)\n\n## If All Else Fails\n\nSometimes Student fails to solve a problem because the problem is beyond either its linguistic capability or its algebraic capability. For example, Student doesn't know how to solve quadratic equations. But sometimes a problem that Student could solve in principle stumps it because it happens to lack a particular piece of common knowledge. When a situation like that arises, Student is capable of asking the user for help (`student2`).\n\n```? student :ship\n\nThe problem to be solved is\n\nThe gross weight of a ship is 20000 tons. If its net weight is 15000\ntons, what is the weight of the ships cargo?\n\nWith mandatory substitutions the problem is\n\nThe gross weight numof a ship is 20000 tons . If its net weight is 15000\ntons , what is the weight numof the ships cargo ?\n\nThe simple sentences are\n\nThe gross weight numof a ship is 20000 tons .\n\nIts net weight is 15000 tons .\n\nWhat is the weight numof the ships cargo ?\n\nThe equations to be solved are\n\nEqual [gross weight of ship] [product 20000 [tons]]\n\nEqual [its net weight] [product 15000 [tons]]\n\nThe equations were insufficient to find a solution.\n\nDo you know any more relationships among these variables?\n\nWeight of ships cargo\n\nIts net weight\n\nTons\n\nGross weight of ship\n\nThe weight of a ships cargo is the gross weight minus the net weight\n\nAssuming that\n[net weight] is equal to [its net weight]\n\nAssuming that\n[gross weight] is equal to [gross weight of ship]\n\nThe weight of the ships cargo is 5000 tons\n\nThe problem is solved.\n```\n\n## Limitations of Pattern Matching\n\nStudent relies on certain stereotyped forms of sentences in the problems it solves. It's easy to make up problems that will completely bewilder it:\n\n```Suppose you have 14 jelly beans. You give 2 each to Tom, Dick, and\nHarry. How many do you have left?\n```\n\nThe first mistake Student makes is that it thinks the word ``` and``` following a comma separates two clauses; it generates simple sentences\n\n```You give 2 each to Tom , Dick .\n\nHarry .\n```\n\nThis is quite a fundamental problem; Student's understanding of the difference between a phrase and a clause is extremely primitive and prone to error. Adding another pattern won't solve this one; the trouble is that Student pays no attention to the words in between the key words like `and`.\n\nThere are several other difficulties with this problem, some worse than others. Student doesn't recognize the word `suppose` as having a special function in the sentence, so it makes up a noun phrase ```suppose you``` just like `the russians`. This could be fixed with an idiomatic substitution that just ignored `suppose`. Another relatively small problem is that the sentence starting `how many` doesn't say how many of what; Student needs a way to understand that the relevant noun phrase is `jelly beans` and not, for example, `Tom`. The words `give` (representing subtraction) and `each` (representing counting a set and then multiplying) have special mathematical meanings comparable to ``` percent less```. A much more subtle problem in knowledge representation is that in this problem there are two different quantities that could be called `the number of jelly beans you have`: the number you have at the beginning of the problem and the number you have at the end. Student has a limited understanding of this passage-of-time difficulty when it's doing an age problem, but not in general.\n\nHow many more difficulties can you find in this problem? For how many of them can you invent improvements to Student to get around them?\n\nSome difficulties seem to require a \"more of the same\" strategy: adding some new patterns to Student that are similar to the ones already there. Other difficulties seem to require a more fundamental redesign. Can that redesign be done using a pattern matcher as the central tool, or are more powerful tools needed? How powerful is pattern matching, anyway?\n\nAnswering questions like these is the job of automata theory. From that point of view, the answer is that it depends exactly what you mean by \"pattern matching.\" The pattern matcher used in Student is equivalent to a finite-state machine. The important thing to note about the patterns used in Student is that they only apply predicates to one word at a time, not to groups of words. In other words, they don't use the `@` quantifier. Here is a typical `student` pattern:\n\n```[^ what !:in [is are] #one !:dlm]\n```\n\nFor the purposes of this discussion, you can ignore the fact that the pattern matcher can set variables to remember which words matched each part of the pattern. In comparing a pattern matcher to a finite-state machine, the question we're asking is what categories of strings can the pattern matcher accept. This particular pattern is equivalent to the following machine:", null, "The arrow that I've labeled dlm is actually several arrows connecting the same states, one for each symbol that the predicate `dlm` accepts, i.e., period, question mark, and semicolon. Similarly, the arrows labeled any are followed for any symbol at all. This machine is nondeterministic, but you'll recall that that doesn't matter; we can turn it into a deterministic one if necessary.\n\nTo be sure you understand the equivalence of patterns and finite-state machines, see if you can draw a machine equivalent to this pattern:\n\n```[I see !:in [the a an] ?:numberp &:adjective !:noun #:adverb]\n```\n\nThis pattern uses all the quantifiers that test words one at a time.\n\nIf these patterns are equivalent to finite-state machines, you'd expect them to have trouble recognizing sentences that involve embedding of clauses within clauses, since these pose the same problem as keeping track of balancing of parentheses. For example, a sentence like \"The book that the boy whom I saw yesterday was reading is interesting\" would strain the capabilities of a finite-state machine. (As in the case of parentheses, we could design a FSM that could handle such sentences up to some fixed depth of embedding, but not one that could handle arbitrarily deep embedding.)\n\n## Context-Free Languages\n\nIf we allow the use of the `@` quantifier in patterns, and if the predicates used to test substrings of the sentences are true functions without side effects, then the pattern matcher is equivalent to an RTN or a production rule grammar. What makes an RTN different from a finite-state machine is that the former can include arrows that match several symbols against another (or the same) RTN. Equivalently, the `@` quantifier matches several symbols against another (or the same) pattern.\n\nA language that can be represented by an RTN is called a context-free language. The reason for the name is that in such a language a given string consistently matches or doesn't match a given predicate regardless of the rest of the sentence. That's the point of what I said just above about side effects; the output from a test predicate can't depend on anything other than its input. Pascal is a context-free language because\n\n```this := that\n```\n\nis always an assignment statement regardless of what other statements might be in the program with it.\n\nWhat isn't a context-free language? The classic example in automata theory is the language consisting of the strings\n\n```abc\naabbcc\naaabbbccc\naaaabbbbcccc\n```\n\nand so on, with the requirement that the number of `a`s be equal to the number of `b`s and also equal to the number of `c`s. That language can't be represented as RTNs or production rules. (Try it. Don't confuse it with the language that accepts any number of `a`s followed by any number of `b`s and so on; even a finite-state machine can represent that one. The equal number requirement is important.)\n\nThe classic formal system that can represent any language for which there are precise rules is the Turing machine. Its advantage over the RTN is precisely that it can \"jump around\" in its memory, looking at one part while making decisions about another part.\n\nThere is a sharp theoretical boundary between context-free and context-sensitive languages, but in practice the boundary is sometimes fuzzy. Consider again the case of Pascal and that assignment statement. I said that it's recognizably an assignment statement because it matches a production rule like\n\n```assignment : identifier := expression\n```\n\n(along with a bunch of other rules that determine what qualifies as an expression). But that production rule doesn't really express all the requirements for a legal Pascal assignment statement. For example, the identifier and the expression must be of the same type. The actual Pascal compiler (any Pascal compiler, not just mine) includes instructions that represent the formal grammar plus extra instructions that represent the additional requirements.\n\nThe type agreement rule is an example of context sensitivity. The types of the relevant identifiers were determined in `var` declarations earlier in the program; those declarations are part of what determines whether the given string of symbols is a legal assignment.\n\n## Augmented Transition Networks\n\nOne could create a clean formal description of Pascal, type agreement rules and all, by designing a Turing machine to accept Pascal programs. However, Turing machines aren't easy to work with for any practical problem. It's much easier to set up a context-free grammar for Pascal and then throw in a few side effects to handle the context-sensitive aspects of the language.\n\nMuch the same is true of English. It's possible to set up an RTN (or a production rule grammar) for noun phrases, for example, and another one for verb phrases. It's tempting then to set up an RTN for a sentence like this:", null, "This machine captures some, but not all, of the rules of English. It's true that a sentence requires a noun phrase (the subject) and a verb phrase (the predicate). But there are agreement rules for person and number (I run but he runs) analogous to the type agreement rules of Pascal.\n\nSome artificial intelligence researchers, understanding all this, parse English sentences using a formal description called an augmented transition network (ATN). An ATN is just like an RTN except that each transition arrow can have associated with it not only the name of a symbol or another RTN but also some conditions that must be met in order to follow the arrow and some actions that the program should take if the arrow is followed. For example, we could turn the RTN just above into an ATN by adding an action to the first arrow saying \"store the number (singular or plural) of the noun phrase in the variable ``` number```\" and adding a condition to the second arrow saying \"the number of the verb phrase must be equal to the variable `number`.\"\n\nSubject-predicate agreement is not the only rule in English grammar best expressed as a side effect in a transition network. Below is an ATN for noun phrases taken from Language as a Cognitive Process, Volume 1: Syntax by Terry Winograd (page 598). I'm not going to attempt to explain the notation or the detailed rules here, but just to give one example, the condition labeled \"h16p\" says that the transition for apostrophe-s can be followed if the head of the phrase is an ordinary noun (\"the book's\") but not if it's a pronoun (\"you's\").", null, "The ATN is equivalent in power to a Turing machine; there is no known mechanism that is more flexible in carrying out algorithms. The flexibility has a cost, though. The time required to parse a string with an ATN is not bounded by a polynomial function. (Remember, the time for an RTN is O(n3).) It can easily be exponential, O(2n). One reason is that a context-sensitive procedure can't be subject to memoization. If two invocations of the same procedure with the same inputs can give different results because of side effects, it does no good to remember what result we got the last time. Turning an ATN into a practical program is often possible, but not a trivial task.\n\nIn thinking about ATNs we've brought together most of the topics in this book: formal systems, algorithms, language parsing, and artificial intelligence. Perhaps that's a good place to stop.\n\n## Program Listing\n\n```to student :prob\nsay [The problem to be solved is] :prob\nmake \"prob map.se [depunct ?] :prob\nlocalmake \"orgprob :prob\nstudent1 :prob ~\n[[[the perimeter of ! rectangle]\n[twice the sum of the length and width of the rectangle]]\n[[two numbers] [one of the numbers and the other number]]\n[[two numbers] [one number and the other number]]]\nend\n\nto student1 :prob :idioms\nlocal [simsen shelf aunits units wanted ans var lasteqn\nref eqt1 beg end idiom reply]\nmake \"prob idioms :prob\nif match [^ two numbers #] :prob ~\n[make \"idiom find [match (sentence \"^beg first ? \"#end) :orgprob] :idioms ~\ntryidiom stop]\nwhile [match [^beg the the #end] :prob] [make \"prob (sentence :beg \"the :end)]\nsay [With mandatory substitutions the problem is] :prob\nifelse match [# @:in [[as old as] [age] [years old]] #] :prob ~\n[ageprob] [make \"simsen bracket :prob]\nlsay [The simple sentences are] :simsen\nforeach [aunits wanted ans var lasteqn ref units] [make ? []]\nmake \"shelf filter [not emptyp ?] map.se [senform ?] :simsen\nlsay [The equations to be solved are] :shelf\nmake \"units remdup :units\nif trysolve :shelf :wanted :units :aunits [print [The problem is solved.] stop]\nmake \"eqt1 remdup geteqns :var\nif not emptyp :eqt1 [lsay [Using the following known relationships] :eqt1]\nstudent2 :eqt1\nend\n\nto student2 :eqt1\nmake \"var remdup sentence (map.se [varterms ?] :eqt1) :var\nmake \"eqt1 sentence :eqt1 vartest :var\nif not emptyp :eqt1 ~\n[if trysolve (sentence :shelf :eqt1) :wanted :units :aunits\n[print [The problem is solved.] stop]]\nmake \"idiom find [match (sentence \"^beg first ? \"#end) :orgprob] :idioms\nif not emptyp :idiom [tryidiom stop]\nlsay [Do you know any more relationships among these variables?] :var\nif equalp :reply [no] [print [] print [I can't solve this problem.] stop]\nif not match [^beg is #end] :reply [print [I don't understand that.] stop]\nmake \"shelf sentence :shelf :eqt1\nstudent2 (list (list \"equal opform :beg opform :end))\nend\n\n;; Mandatory substitutions\n\nto depunct :word\nif emptyp :word [output []]\nif equalp first :word \"\\$ [output sentence \"\\$ depunct butfirst :word]\nif equalp last :word \"% [output sentence depunct butlast :word \"percent]\nif memberp last :word [. ? |;| ,] [output sentence depunct butlast :word last :word]\nif emptyp butfirst :word [output :word]\nif equalp last2 :word \"'s [output sentence depunct butlast butlast :word \"s]\noutput :word\nend\n\nto last2 :word\noutput word (last butlast :word) (last :word)\nend\n\nto idioms :sent\nlocal \"number\noutput changes :sent ~\n[[[the sum of] [\"sum]] [[square of] [\"square]] [[of] [\"numof]]\n[[how old] [\"what]] [[is equal to] [\"is]]\n[[years younger than] [[less than]]] [[years older than] [\"plus]]\n[[percent less than] [\"perless]] [[less than] [\"lessthan]]\n[[these] [\"the]] [[more than] [\"plus]]\n[[first two numbers] [[the first number and the second number]]]\n[[three numbers]\n[[the first number and the second number and the third number]]]\n[[one half] [0.5]] [[twice] [[2 times]]]\n[[\\$ !number] [sentence :number \"dollars]] [[consecutive to] [[1 plus]]]\n[[larger than] [\"plus]] [[per cent] [\"percent]] [[how many] [\"howm]]\n[[is multiplied by] [\"ismulby]] [[is divided by] [\"isdivby]]\n[[multiplied by] [\"times]] [[divided by] [\"divby]]]\nend\n\nto changes :sent :list\nlocalmake \"keywords map.se [findkey first ?] :list\noutput changes1 :sent :list :keywords\nend\n\nto findkey :pattern\nif equalp first :pattern \"!:in [output first butfirst :pattern]\nif equalp first :pattern \"?:in [output sentence (item 2 :pattern) (item 3 :pattern)]\noutput first :pattern\nend\n\nto changes1 :sent :list :keywords\nif emptyp :sent [output []]\nif memberp first :sent :keywords [output changes2 :sent :list :keywords]\noutput fput first :sent changes1 butfirst :sent :list :keywords\nend\n\nto changes2 :sent :list :keywords\nchanges3 :list :list\noutput fput first :sent changes1 butfirst :sent :list :keywords\nend\n\nto changes3 :biglist :nowlist\nif emptyp :nowlist [stop]\nif changeone first :nowlist [changes3 :biglist :biglist stop]\nchanges3 :biglist butfirst :nowlist\nend\n\nto changeone :change\nlocal \"end\nif not match (sentence first :change [#end]) :sent [output \"false]\nmake \"sent run (sentence \"sentence last :change \":end)\noutput \"true\nend\n\n;; Division into simple sentences\n\nto bracket :prob\noutput bkt1 finddelim :prob\nend\n\nto finddelim :sent\noutput finddelim1 :sent [] []\nend\n\nto finddelim1 :in :out :simples\nif emptyp :in ~\n[ifelse emptyp :out [output :simples] [output lput (sentence :out \".) :simples]]\nif dlm first :in ~\n[output finddelim1 (nocap butfirst :in) []\n(lput (sentence :out first :in) :simples)]\noutput finddelim1 (butfirst :in) (sentence :out first :in) :simples\nend\n\nto nocap :words\nif emptyp :words [output []]\nif personp first :words [output :words]\noutput sentence (lowercase first :words) butfirst :words\nend\n\nto bkt1 :problist\nlocal [first word rest]\nif emptyp :problist [output []]\nif not memberp \", first :problist ~\n[output fput first :problist bkt1 butfirst :problist]\nif match [if ^first , !word:qword #rest] first :problist ~\n[output bkt1 fput (sentence :first \".)\nfput (sentence :word :rest) butfirst :problist]\nif match [^first , and #rest] first :problist ~\n[output fput (sentence :first \".) (bkt1 fput :rest butfirst :problist)]\noutput fput first :problist bkt1 butfirst :problist\nend\n\n;; Age problems\n\nto ageprob\nlocal [beg end sym who num subj ages]\nwhile [match [^beg as old as #end] :prob] [make \"prob sentence :beg :end]\nwhile [match [^beg years old #end] :prob] [make \"prob sentence :beg :end]\nwhile [match [^beg will be when #end] :prob] ~\n[make \"sym gensym\nmake \"prob (sentence :beg \"in :sym [years . in] :sym \"years :end)]\nwhile [match [^beg was when #end] :prob] ~\n[make \"sym gensym\nmake \"prob (sentence :beg :sym [years ago .] :sym [years ago] :end)]\nwhile [match [^beg !who:personp will be in !num years #end] :prob] ~\n[make \"prob (sentence :beg :who [s age in] :num \"years #end)]\nwhile [match [^beg was #end] :prob] [make \"prob (sentence :beg \"is :end)]\nwhile [match [^beg will be #end] :prob] [make \"prob (sentence :beg \"is :end)]\nwhile [match [^beg !who:personp is now #end] :prob] ~\n[make \"prob (sentence :beg :who [s age now] :end)]\nwhile [match [^beg !num years from now #end] :prob] ~\n[make \"prob (sentence :beg \"in :num \"years :end)]\nmake \"prob ageify :prob\nifelse match [^ !who:personp ^end s age #] :prob ~\n[make \"subj sentence :who :end] [make \"subj \"someone]\nmake \"prob agepron :prob\nmake \"end :prob\nmake \"ages []\nwhile [match [^ !who:personp ^beg age #end] :end] ~\n[push \"ages (sentence \"and :who :beg \"age)]\nmake \"ages butfirst reduce \"sentence remdup :ages\nwhile [match [^beg their ages #end] :prob] [make \"prob (sentence :beg :ages :end)]\nmake \"simsen map [agesen ?] bracket :prob\nend\n\nto ageify :sent\nif emptyp :sent [output []]\nif not personp first :sent [output fput first :sent ageify butfirst :sent]\ncatch \"error [if equalp first butfirst :sent \"s\n[output fput first :sent ageify butfirst :sent]]\noutput (sentence first :sent [s age] ageify butfirst :sent)\nend\n\nto agepron :sent\nif emptyp :sent [output []]\nif not pronoun first :sent [output fput first :sent agepron butfirst :sent]\nif posspro first :sent [output (sentence :subj \"s agepron butfirst :sent)]\noutput (sentence :subj [s age] agepron butfirst :sent)\nend\n\nto agesen :sent\nlocal [when rest num]\nmake \"when []\nif match [in !num years #rest] :sent ~\n[make \"when sentence \"pluss :num make \"sent :rest]\nif match [!num years ago #rest] :sent ~\n[make \"when sentence \"minuss :num make \"sent :rest]\noutput agewhen :sent\nend\n\nto agewhen :sent\nif emptyp :sent [output []]\nif not equalp first :sent \"age [output fput first :sent agewhen butfirst :sent]\nif match [in !num years #rest] butfirst :sent ~\n[output (sentence [age pluss] :num agewhen :rest)]\nif match [!num years ago #rest] butfirst :sent ~\n[output (sentence [age minuss] :num agewhen :rest)]\nif equalp \"now first butfirst :sent ~\n[output sentence \"age agewhen butfirst butfirst :sent]\noutput (sentence \"age :when agewhen butfirst :sent)\nend\n\n;; Translation from sentences into equations\n\nto senform :sent\nmake \"lasteqn senform1 :sent\noutput :lasteqn\nend\n\nto senform1 :sent\nlocal [one two verb1 verb2 stuff1 stuff2 factor]\nif emptyp :sent [output []]\nif match [^ what are ^one and ^two !:dlm] :sent ~\n[output fput (qset :one) (senform (sentence [what are] :two \"?))]\nif match [^ what !:in [is are] #one !:dlm] :sent ~\n[output (list qset :one)]\nif match [^ howm !one is #two !:dlm] :sent ~\n[push \"aunits (list :one) output (list qset :two)]\nif match [^ howm ^one do ^two have !:dlm] :sent ~\n[output (list qset (sentence [the number of] :one :two \"have))]\nif match [^ howm ^one does ^two have !:dlm] :sent ~\n[output (list qset (sentence [the number of] :one :two \"has))]\nif match [^ find ^one and #two] :sent ~\n[output fput (qset :one) (senform sentence \"find :two)]\nif match [^ find #one !:dlm] :sent [output (list qset :one)]\nmake \"sent filter [not article ?] :sent\nif match [^one ismulby #two] :sent ~\n[push \"ref (list \"product opform :one opform :two) output []]\nif match [^one isdivby #two] :sent ~\n[push \"ref (list \"quotient opform :one opform :two) output []]\nif match [^one is increased by #two] :sent ~\n[push \"ref (list \"sum opform :one opform :two) output []]\nif match [^one is #two] :sent ~\n[output (list (list \"equal opform :one opform :two))]\nif match [^one !verb1:verb ^factor as many ^stuff1 as\n^two !verb2:verb ^stuff2 !:dlm] ~\n:sent ~\n[if emptyp :stuff2 [make \"stuff2 :stuff1]\noutput (list (list \"equal ~\nopform (sentence [the number of] :stuff1 :one :verb1) ~\nopform (sentence :factor [the number of] :stuff2 :two :verb2)))]\nif match [^one !verb1:verb !factor:numberp #stuff1 !:dlm] :sent ~\n[output (list (list \"equal ~\nopform (sentence [the number of] :stuff1 :one :verb1) ~\nopform (list :factor)))]\nsay [This sentence form is not recognized:] :sent\nthrow \"error\nend\n\nto qset :sent\nlocalmake \"opform opform filter [not article ?] :sent\nif not operatorp first :opform ~\n[queue \"wanted :opform queue \"ans list :opform oprem :sent output []]\nlocalmake \"gensym gensym\nqueue \"wanted :gensym\nqueue \"ans list :gensym oprem :sent\noutput (list \"equal :gensym opform (filter [not article ?] :sent))\nend\n\nto oprem :sent\noutput map [ifelse equalp ? \"numof [\"of] [?]] :sent\nend\n\nto opform :expr\nlocal [left right op]\nif match [^left !op:op2 #right] :expr [output optest :op :left :right]\nif match [^left !op:op1 #right] :expr [output optest :op :left :right]\nif match [^left !op:op0 #right] :expr [output optest :op :left :right]\nif match [#left !:dlm] :expr [make \"expr :left]\noutput nmtest filter [not article ?] :expr\nend\n\nto optest :op :left :right\noutput run (list (word \"tst. :op) :left :right)\nend\n\nto tst.numof :left :right\nif numberp last :left [output (list \"product opform :left opform :right)]\noutput opform (sentence :left \"of :right)\nend\n\nto tst.divby :left :right\noutput (list \"quotient opform :left opform :right)\nend\n\nto tst.tothepower :left :right\noutput (list \"expt opform :left opform :right)\nend\n\nto expt :num :pow\nif :pow < 1 [output 1]\noutput :num * expt :num :pow - 1\nend\n\nto tst.per :left :right\noutput (list \"quotient ~\nopform :left ~\nopform (ifelse numberp first :right [:right] [fput 1 :right]))\nend\n\nto tst.lessthan :left :right\noutput opdiff opform :right opform :left\nend\n\nto opdiff :left :right\noutput (list \"sum :left (list \"minus :right))\nend\n\nto tst.minus :left :right\nif emptyp :left [output list \"minus opform :right]\noutput opdiff opform :left opform :right\nend\n\nto tst.minuss :left :right\noutput tst.minus :left :right\nend\n\nto tst.sum :left :right\nlocal [one two three]\nif match [^one and ^two and #three] :right ~\n[output (list \"sum opform :one opform (sentence \"sum :two \"and :three))]\nif match [^one and #two] :right ~\n[output (list \"sum opform :one opform :two)]\nsay [sum used wrong:] :right\nthrow \"error\nend\n\nto tst.squared :left :right\noutput list \"square opform :left\nend\n\nto tst.difference :left :right\nlocal [one two]\nif match [between ^one and #two] :right [output opdiff opform :one opform :two]\nsay [Incorrect use of difference:] :right\nthrow \"error\nend\n\nto tst.plus :left :right\noutput (list \"sum opform :left opform :right)\nend\n\nto tst.pluss :left :right\noutput tst.plus :left :right\nend\n\nto square :x\noutput :x * :x\nend\n\nto tst.square :left :right\noutput list \"square opform :right\nend\n\nto tst.percent :left :right\nif not numberp last :left ~\n[say [Incorrect use of percent:] :left throw \"error]\noutput opform (sentence butlast :left ((last :left) / 100) :right)\nend\n\nto tst.perless :left :right\nif not numberp last :left ~\n[say [Incorrect use of percent:] :left throw \"error]\noutput (list \"product ~\n(opform sentence butlast :left ((100 - (last :left)) / 100)) ~\nopform :right)\nend\n\nto tst.times :left :right\nif emptyp :left [say [Incorrect use of times:] :right throw \"error]\noutput (list \"product opform :left opform :right)\nend\n\nto nmtest :expr\nif match [& !:numberp #] :expr [say [argument error:] :expr throw \"error]\nif and (equalp first :expr 1) (1 < count :expr) ~\n[make \"expr (sentence 1 plural (first butfirst :expr) (butfirst butfirst :expr))]\nif and (numberp first :expr) (1 < count :expr) ~\n[push \"units (list first butfirst :expr) ~\noutput (list \"product (first :expr) (opform butfirst :expr))]\nif numberp first :expr [output first :expr]\nif memberp \"this :expr [output this :expr]\nif not memberp :expr :var [push \"var :expr]\noutput :expr\nend\n\nto this :expr\nif not emptyp :ref [output pop \"ref]\nif not emptyp :lasteqn [output first butfirst last :lasteqn]\nif equalp first :expr \"this [make \"expr butfirst :expr]\npush \"var :expr\noutput :expr\nend\n\n;; Solving the equations\n\nto trysolve :shelf :wanted :units :aunits\nlocal \"solution\nmake \"solution solve :wanted :shelf (ifelse emptyp :aunits [:units] [:aunits])\nend\n\nto solve :wanted :eqt :terms\noutput solve.reduce solver :wanted :terms [] [] \"insufficient\nend\n\nto solve.reduce :soln\nif emptyp :soln [output []]\nif wordp :soln [output :soln]\nif emptyp butfirst :soln [output :soln]\nlocal \"part\nmake \"part solve.reduce butfirst :soln\noutput fput (list (first first :soln) (subord last first :soln :part)) :part\nend\n\nto solver :wanted :terms :alis :failed :err\nlocal [one result restwant]\nif emptyp :wanted [output :err]\nmake \"one solve1 (first :wanted) ~\n(sentence butfirst :wanted :failed :terms) ~\n:alis :eqt [] \"insufficient\nif wordp :one ~\n[output solver (butfirst :wanted) :terms :alis (fput first :wanted :failed) :one]\nmake \"restwant (sentence :failed butfirst :wanted)\nif emptyp :restwant [output :one]\nmake \"result solver :restwant :terms :one [] \"insufficient\nif listp :result [output :result]\noutput solver (butfirst :wanted) :terms :alis (fput first :wanted :failed) :one\nend\n\nto solve1 :x :terms :alis :eqns :failed :err\nlocal [thiseq vars extras xterms others result]\nif emptyp :eqns [output :err]\nmake \"thiseq subord (first :eqns) :alis\nmake \"vars varterms :thiseq\nif not memberp :x :vars ~\n[output solve1 :x :terms :alis (butfirst :eqns) (fput first :eqns :failed) :err]\nmake \"xterms fput :x :terms\nmake \"extras setminus :vars :xterms\nmake \"eqt remove (first :eqns) :eqt\nif not emptyp :extras ~\n[make \"others solver :extras :xterms :alis [] \"insufficient\nifelse wordp :others\n[make \"eqt sentence :failed :eqns\noutput solve1 :x :terms :alis (butfirst :eqns)\n(fput first :eqns :failed) :others]\n[make \"alis :others\nmake \"thiseq subord (first :eqns) :alis]]\nmake \"result solveq :x :thiseq\nif listp :result [output lput :result :alis]\nmake \"eqt sentence :failed :eqns\noutput solve1 :x :terms :alis (butfirst :eqns) (fput first :eqns :failed) :result\nend\n\nto solveq :var :eqn\nlocal [left right]\nmake \"left first butfirst :eqn\nifelse occvar :var :left ~\n[make \"right last :eqn] [make \"right :left make \"left last :eqn]\noutput solveq1 :left :right \"true\nend\n\nto solveq1 :left :right :bothtest\nif :bothtest [if occvar :var :right [output solveqboth :left :right]]\nif equalp :left :var [output list :var :right]\nif wordp :left [output \"unsolvable]\nlocal \"oper\nmake \"oper first :left\nif memberp :oper [sum product minus quotient] [output run (list word \"solveq. :oper)]\noutput \"unsolvable\nend\n\nto solveqboth :left :right\nif not equalp first :right \"sum [output solveq1 (subterm :left :right) 0 \"false]\noutput solveq.rplus :left butfirst :right []\nend\n\nto solveq.rplus :left :right :newright\nif emptyp :right [output solveq1 :left (simone \"sum :newright) \"false]\nif occvar :var first :right ~\n[output solveq.rplus (subterm :left first :right) butfirst :right :newright]\noutput solveq.rplus :left butfirst :right (fput first :right :newright)\nend\n\nto solveq.sum\nif emptyp butfirst butfirst :left [output solveq1 first butfirst :left :right \"true]\noutput solveq.sum1 butfirst :left :right []\nend\n\nto solveq.sum1 :left :right :newleft\nif emptyp :left [output solveq.sum2]\nif occvar :var first :left ~\n[output solveq.sum1 butfirst :left :right fput first :left :newleft]\noutput solveq.sum1 butfirst :left (subterm :right first :left) :newleft\nend\n\nto solveq.sum2\nif emptyp butfirst :newleft [output solveq1 first :newleft :right \"true]\nlocalmake \"factor factor :newleft :var\nif equalp first :factor \"unknown [output \"unsolvable]\nif equalp last :factor 0 [output \"unsolvable]\noutput solveq1 first :factor (divterm :right last :factor) \"true\nend\n\nto solveq.minus\noutput solveq1 (first butfirst :left) (minusin :right) \"false\nend\n\nto solveq.product\noutput solveq.product1 :left :right\nend\n\nto solveq.product1 :left :right\nif emptyp butfirst butfirst :left [output solveq1 (first butfirst :left) :right \"true]\nif not occvar :var first butfirst :left ~\n[output solveq.product1 (fput \"product butfirst butfirst :left)\n(divterm :right first butfirst :left)]\nlocalmake \"rest simone \"product butfirst butfirst :left\nif occvar :var :rest [output \"unsolvable]\noutput solveq1 (first butfirst :left) (divterm :right :rest) \"false\nend\n\nto solveq.quotient\nif occvar :var first butfirst :left ~\n[output solveq1 (first butfirst :left) (simtimes list :right last :left) \"true]\noutput solveq1 (simtimes list :right last :left) (first butfirst :left) \"true\nend\n\nlocalmake \"den last :fract\nif not equalp first :addends \"quotient ~\n[output simdiv list (simone \"sum\n(remop \"sum list (distribtimes (list :addends) :den)\nfirst butfirst :fract))\n:den]\nif equalp :den last :addends ~\n[output simdiv (simplus list (first butfirst :fract) (first butfirst :addends))\n:den]\nlocalmake \"lowterms simdiv list :den last :addends\noutput simdiv list (simplus (simtimes list first butfirst :fract last :lowterms)\nfirst butfirst :lowterms)) ~\n(simtimes list first butfirst :lowterms last :addends)\nend\n\nto distribtimes :trms :multiplier\noutput simplus map [simtimes (list ? :multiplier)] :trms\nend\n\nto distribx :expr\nlocal [oper args]\nif emptyp :expr [output :expr]\nmake \"oper first :expr\nif not operatorp :oper [output :expr]\nmake \"args map [distribx ?] butfirst :expr\nif reduce \"and map [numberp ?] :args [output run (sentence [(] :oper :args [)])]\nif equalp :oper \"sum [output simplus :args]\nif equalp :oper \"minus [output minusin first :args]\nif equalp :oper \"product [output simtimes :args]\nif equalp :oper \"quotient [output simdiv :args]\noutput fput :oper :args\nend\n\nto divterm :dividend :divisor\nif equalp :dividend 0 [output 0]\noutput simdiv list :dividend :divisor\nend\n\nto factor :exprs :var\nlocal \"trms\nmake \"trms map [factor1 :var ?] :exprs\nif memberp \"unknown :trms [output fput \"unknown :exprs]\noutput list :var simplus :trms\nend\n\nto factor1 :var :expr\nlocalmake \"negvar minusin :var\nif equalp :var :expr [output 1]\nif equalp :negvar :expr [output -1]\nif emptyp :expr [output \"unknown]\nif equalp first :expr \"product [output factor2 butfirst :expr]\nif not equalp first :expr \"quotient [output \"unknown]\nlocalmake \"dividend first butfirst :expr\nif equalp :var :dividend [output (list \"quotient 1 last :expr)]\nif not equalp first :dividend \"product [output \"unknown]\nlocalmake \"result factor2 butfirst :dividend\nif equalp :result \"unknown [output \"unknown]\noutput (list \"quotient :result last :expr)\nend\n\nto factor2 :trms\nif memberp :var :trms [output simone \"product (remove :var :trms)]\nif memberp :negvar :trms [output minusin simone \"product (remove :negvar :trms)]\noutput \"unknown\nend\n\nif equalp :num 0 [output :rest]\noutput fput :num :rest\nend\n\nto maybemul :num :rest\nif equalp :num 1 [output :rest]\noutput fput :num :rest\nend\n\nto minusin :expr\nif emptyp :expr [output -1]\nif equalp first :expr \"sum [output fput \"sum map [minusin ?] butfirst :expr]\nif equalp first :expr \"minus [output last :expr]\nif memberp first :expr [product quotient] ~\n[output fput first :expr\n(fput (minusin first butfirst :expr) butfirst butfirst :expr)]\nif numberp :expr [output minus :expr]\noutput list \"minus :expr\nend\n\nto occvar :var :expr\nif emptyp :expr [output \"false]\nif wordp :expr [output equalp :var :expr]\nif operatorp first :expr [output not emptyp find [occvar :var ?] butfirst :expr]\noutput equalp :var :expr\nend\n\nto remfactor :num :den\nforeach butfirst :num [remfactor1 ?]\noutput (list \"quotient (simone \"product butfirst :num) (simone \"product butfirst :den))\nend\n\nto remfactor1 :expr\nlocal \"neg\nif memberp :expr :den ~\n[make \"num remove :expr :num make \"den remove :expr :den stop]\nmake \"neg minusin :expr\nif not memberp :neg :den [stop]\nmake \"num remove :expr :num\nmake \"den minusin remove :neg :den\nend\n\nto remop :oper :exprs\noutput map.se [ifelse equalp first ? :oper [butfirst ?] [(list ?)]] :exprs\nend\n\nto simdiv :list\nlocal [num den numop denop]\nmake \"num first :list\nmake \"den last :list\nif equalp :num :den [output 1]\nif numberp :den [output simtimes (list (quotient 1 :den) :num)]\nmake \"numop first :num\nmake \"denop first :den\nif equalp :numop \"quotient ~\n[output simdiv list (first butfirst :num) (simtimes list last :num :den)]\nif equalp :denop \"quotient ~\n[output simdiv list (simtimes list :num last :den) (first butfirst :den)]\nif and equalp :numop \"product equalp :denop \"product [output remfactor :num :den]\nif and equalp :numop \"product memberp :den :num [output remove :den :num]\noutput fput \"quotient :list\nend\n\nto simone :oper :trms\nif emptyp :trms [output ifelse equalp :oper \"product ]\nif emptyp butfirst :trms [output first :trms]\noutput fput :oper :trms\nend\n\nto simplus :exprs\nmake \"exprs remop \"sum :exprs\nlocalmake \"factor [unknown]\ncatch \"simplus ~\n[foreach :terms ~\n[make \"factor (factor :exprs ?) ~\nif not equalp first :factor \"unknown [throw \"simplus]]]\nif not equalp first :factor \"unknown [output fput \"product remop \"product :factor]\nlocalmake \"nums 0\nlocalmake \"nonnums []\nlocalmake \"quick []\ncatch \"simplus [simplus1 :exprs]\nif not emptyp :quick [output :quick]\nif not equalp :nums 0 [push \"nonnums :nums]\noutput simone \"sum :nonnums\nend\n\nto simplus1 :exprs\nif emptyp :exprs [stop]\nsimplus2 first :exprs\nsimplus1 butfirst :exprs\nend\n\nto simplus2 :pos\nlocal \"neg\nmake \"neg minusin :pos\nif numberp :pos [make \"nums sum :pos :nums stop]\nif memberp :neg butfirst :exprs [make \"exprs remove :neg :exprs stop]\nif equalp first :pos \"quotient ~\n[make \"quick (denom :pos (maybeadd :nums sentence :nonnums butfirst :exprs)) ~\nthrow \"simplus]\npush \"nonnums :pos\nend\n\nto simtimes :exprs\nlocal [nums nonnums quick]\nmake \"nums 1\nmake \"nonnums []\nmake \"quick []\ncatch \"simtimes [foreach remop \"product :exprs [simtimes1 ?]]\nif not emptyp :quick [output :quick]\nif equalp :nums 0 [output 0]\nif not equalp :nums 1 [push \"nonnums :nums]\noutput simone \"product :nonnums\nend\n\nto simtimes1 :expr\nif equalp :expr 0 [make \"nums 0 throw \"simtimes]\nif numberp :expr [make \"nums product :expr :nums stop]\nif equalp first :expr \"sum ~\n[make \"quick distribtimes (butfirst :expr)\n(simone \"product maybemul :nums sentence :nonnums ?rest)\nthrow \"simtimes]\nif equalp first :expr \"quotient ~\n[make \"quick\nsimdiv (list (simtimes (list (first butfirst :expr)\n(simone \"product\nmaybemul :nums\nsentence :nonnums ?rest)))\n(last :expr))\nthrow \"simtimes]\npush \"nonnums :expr\nend\n\nto subord :expr :alist\noutput distribx subord1 :expr :alist\nend\n\nto subord1 :expr :alist\nif emptyp :alist [output :expr]\noutput subord (substop (last first :alist) (first first :alist) :expr) ~\n(butfirst :alist)\nend\n\nto substop :val :var :expr\nif emptyp :expr [output []]\nif equalp :expr :var [output :val]\nif not operatorp first :expr [output :expr]\noutput fput first :expr map [substop :val :var ?] butfirst :expr\nend\n\nto subterm :minuend :subtrahend\nif equalp :minuend 0 [output minusin :subtrahend]\nif equalp :minuend :subtrahend [output 0]\noutput simplus (list :minuend minusin :subtrahend)\nend\n\nto varterms :expr\nif emptyp :expr [output []]\nif numberp :expr [output []]\nif wordp :expr [output (list :expr)]\nif operatorp first :expr [output map.se [varterms ?] butfirst :expr]\noutput (list :expr)\nend\n\n;; Printing the solutions\n\nprint []\nif equalp :solution \"unsolvable ~\n[print [Unable to solve this set of equations.] output \"false]\nif equalp :solution \"insufficient ~\n[print [The equations were insufficient to find a solution.] output \"false]\nlocalmake \"gotall \"true\nforeach :ans [if prans ? :solution [make \"gotall \"false]]\nif not :gotall [print [] print [Unable to solve this set of equations.]]\noutput :gotall\nend\n\nto prans :ans :solution\nlocalmake \"result find [equalp first ? first :ans] :solution\nif emptyp :result [output \"true]\nprint (sentence cap last :ans \"is unitstring last :result)\nprint []\noutput \"false\nend\n\nto unitstring :expr\nif numberp :expr [output roundoff :expr]\nif equalp first :expr \"product ~\n[output sentence (unitstring first butfirst :expr)\n(reduce \"sentence butfirst butfirst :expr)]\nif (and (listp :expr)\n(not numberp first :expr)\n(not operatorp first :expr)) ~\n[output (sentence 1 (singular first :expr) (butfirst :expr))]\noutput :expr\nend\n\nto roundoff :num\nif (abs (:num - round :num)) < 0.0001 [output round :num]\noutput :num\nend\n\nto abs :num\noutput ifelse (:num < 0) [-:num] [:num]\nend\n\n;; Using known relationships\n\nto geteqns :vars\noutput map.se [gprop varkey ? \"eqns] :vars\nend\n\nto varkey :var\nlocal \"word\nif match [number of !word #] :var [output :word]\noutput first :var\nend\n\n;; Assuming equality of similar variables\n\nto vartest :vars\nif emptyp :vars [output []]\nlocal [var beg end]\nmake \"var first :vars\noutput (sentence (ifelse match [^beg !:pronoun #end] :var\n[vartest1 :var (sentence :beg \"& :end) butfirst :vars]\n[[]])\n(vartest1 :var (sentence \"# :var \"#) butfirst :vars)\n(vartest butfirst :vars))\nend\n\nto vartest1 :target :pat :vars\noutput map [varequal :target ?] filter [match :pat ?] :vars\nend\n\nto varequal :target :var\nprint []\nprint [Assuming that]\nprint (sentence (list :target) [is equal to] (list :var))\noutput (list \"equal :target :var)\nend\n\n;; Optional substitutions\n\nto tryidiom\nmake \"prob (sentence :beg last :idiom :end)\nwhile [match (sentence \"^beg first :idiom \"#end) :prob] ~\n[make \"prob (sentence :beg last :idiom :end)]\nsay [The problem with an idiomatic substitution is] :prob\nstudent1 :prob (remove :idiom :idioms)\nend\n\n;; Utility procedures\n\nto qword :word\noutput memberp :word [find what howm how]\nend\n\nto dlm :word\noutput memberp :word [. ? |;|]\nend\n\nto article :word\noutput memberp :word [a an the]\nend\n\nto verb :word\noutput memberp :word [have has get gets weigh weighs]\nend\n\nto personp :word\noutput memberp :word [Mary Ann Bill Tom Sally Frank father uncle]\nend\n\nto pronoun :word\noutput memberp :word [he she it him her they them his her its]\nend\n\nto posspro :word\noutput memberp :word [his her its]\nend\n\nto op0 :word\noutput memberp :word [pluss minuss squared tothepower per sum difference numof]\nend\n\nto op1 :word\noutput memberp :word [times divby square]\nend\n\nto op2 :word\noutput memberp :word [plus minus lessthan percent perless]\nend\n\nto operatorp :word\noutput memberp :word [sum minus product quotient expt square equal]\nend\n\nto plural :word\nlocalmake \"plural gprop :word \"plural\nif not emptyp :plural [output :plural]\nif not emptyp gprop :word \"sing [output :word]\nif equalp last :word \"s [output :word]\noutput word :word \"s\nend\n\nto singular :word\nlocalmake \"sing gprop :word \"sing\nif not emptyp :sing [output :sing]\nif not emptyp gprop :word \"plural [output :word]\nif equalp last :word \"s [output butlast :word]\noutput :word\nend\n\nto setminus :big :little\noutput filter [not memberp ? :little] :big\nend\n\nto say :herald :text\nprint []\nprint :herald\nprint []\nprint :text\nprint []\nend\n\nto lsay :herald :text\nprint []\nprint :herald\nprint []\nforeach :text [print cap ? print []]\nend\n\nto cap :sent\nif emptyp :sent [output []]\noutput sentence (word uppercase first first :sent butfirst first :sent) ~\nbutfirst :sent\nend\n\n;; The pattern matcher\n\nto match :pat :sen\nif prematch :pat :sen [output rmatch :pat :sen]\noutput \"false\nend\n\nto prematch :pat :sen\nif emptyp :pat [output \"true]\nif listp first :pat [output prematch butfirst :pat :sen]\nif memberp first first :pat [! @ # ^ & ?] [output prematch butfirst :pat :sen]\nif emptyp :sen [output \"false]\nlocalmake \"rest member first :pat :sen\nif not emptyp :rest [output prematch butfirst :pat :rest]\noutput \"false\nend\n\nto rmatch :pat :sen\nlocal [special.var special.pred special.buffer in.list]\nif or wordp :pat wordp :sen [output \"false]\nif emptyp :pat [output emptyp :sen]\nif listp first :pat [output special fput \"!: :pat :sen]\nif memberp first first :pat [? # ! & @ ^] [output special :pat :sen]\nif emptyp :sen [output \"false]\nif equalp first :pat first :sen [output rmatch butfirst :pat butfirst :sen]\noutput \"false\nend\n\nto special :pat :sen\nset.special parse.special butfirst first :pat \"\noutput run word \"match first first :pat\nend\n\nto parse.special :word :var\nif emptyp :word [output list :var \"always]\nif equalp first :word \": [output list :var butfirst :word]\noutput parse.special butfirst :word word :var first :word\nend\n\nto set.special :list\nmake \"special.var first :list\nmake \"special.pred last :list\nif emptyp :special.var [make \"special.var \"special.buffer]\nif memberp :special.pred [in anyof] [set.in]\nif not emptyp :special.pred [stop]\nmake \"special.pred first butfirst :pat\nmake \"pat fput first :pat butfirst butfirst :pat\nend\n\nto set.in\nmake \"in.list first butfirst :pat\nmake \"pat fput first :pat butfirst butfirst :pat\nend\n\nto match!\nif emptyp :sen [output \"false]\nif not try.pred [output \"false]\nmake :special.var first :sen\noutput rmatch butfirst :pat butfirst :sen\nend\n\nto match?\nmake :special.var []\nif emptyp :sen [output rmatch butfirst :pat :sen]\nif not try.pred [output rmatch butfirst :pat :sen]\nmake :special.var first :sen\nif rmatch butfirst :pat butfirst :sen [output \"true]\nmake :special.var []\noutput rmatch butfirst :pat :sen\nend\n\nto match#\nmake :special.var []\noutput #test #gather :sen\nend\n\nto #gather :sen\nif emptyp :sen [output :sen]\nif not try.pred [output :sen]\nmake :special.var lput first :sen thing :special.var\noutput #gather butfirst :sen\nend\n\nto #test :sen\nif rmatch butfirst :pat :sen [output \"true]\nif emptyp thing :special.var [output \"false]\noutput #test2 fput last thing :special.var :sen\nend\n\nto #test2 :sen\nmake :special.var butlast thing :special.var\noutput #test :sen\nend\n\nto match&\noutput &test match#\nend\n\nto &test :tf\nif emptyp thing :special.var [output \"false]\noutput :tf\nend\n\nto match^\nmake :special.var []\noutput ^test :sen\nend\n\nto ^test :sen\nif rmatch butfirst :pat :sen [output \"true]\nif emptyp :sen [output \"false]\nif not try.pred [output \"false]\nmake :special.var lput first :sen thing :special.var\noutput ^test butfirst :sen\nend\n\nto match@\nmake :special.var :sen\noutput @test []\nend\n\nto @test :sen\nif @try.pred [if rmatch butfirst :pat :sen [output \"true]]\nif emptyp thing :special.var [output \"false]\noutput @test2 fput last thing :special.var :sen\nend\n\nto @test2 :sen\nmake :special.var butlast thing :special.var\noutput @test :sen\nend\n\nto try.pred\nif listp :special.pred [output rmatch :special.pred first :sen]\noutput run list :special.pred quoted first :sen\nend\n\nto quoted :thing\nif listp :thing [output :thing]\noutput word \"\" :thing\nend\n\nto @try.pred\nif listp :special.pred [output rmatch :special.pred thing :special.var]\noutput run list :special.pred thing :special.var\nend\n\nto always :x\noutput \"true\nend\n\nto in :word\noutput memberp :word :in.list\nend\n\nto anyof :sen\noutput anyof1 :sen :in.list\nend\n\nto anyof1 :sen :pats\nif emptyp :pats [output \"false]\nif rmatch first :pats :sen [output \"true]\noutput anyof1 :sen butfirst :pats\nend\n\n;; Sample word problems\n\nmake \"ann [Mary is twice as old as Ann was when Mary was as old as Ann is now.\nIf Mary is 24 years old, how old is Ann?]\nmake \"guns [The number of soldiers the Russians have is\none half of the number of guns they have. They have 7000 guns.\nHow many soldiers do they have?]\nmake \"jet [The distance from New York to Los Angeles is 3000 miles.\nIf the average speed of a jet plane is 600 miles per hour,\nfind the time it takes to travel from New York to Los Angeles by jet.]\nmake \"nums [A number is multiplied by 6 . This product is increased by 44 .\nThis result is 68 . Find the number.]\nIf this price is 15 percent less than the marked price, find the marked price.]\nmake \"sally [The sum of Sally's share of some money and Frank's share is \\$4.50.\nSally's share is twice Frank's. Find Frank's and Sally's share.]\nmake \"ship [The gross weight of a ship is 20000 tons.\nIf its net weight is 15000 tons, what is the weight of the ships cargo?]\nmake \"span [If 1 span is 9 inches, and 1 fathom is 6 feet,\nhow many spans is 1 fathom?]\nmake \"sumtwo [The sum of two numbers is 96,\nand one number is 16 larger than the other number. Find the two numbers.]\nmake \"tom [If the number of customers Tom gets is\ntwice the square of 20 per cent of the number of advertisements he runs,\nwhat is the number of customers Tom gets?]\nmake \"uncle [Bill's father's uncle is twice as old as Bill's father.\n2 years from now Bill's father will be 3 times as old as Bill.\nThe sum of their ages is 92 . Find Bill's age.]\n\n;; Initial data base\n\npprop \"distance \"eqns ~\n[[equal [distance] [product [speed] [time]]]\n[equal [distance] [product [gas consumtion] [number of gallons of gas used]]]]\npprop \"feet \"eqns ~\n[[equal [product 1 [feet]] [product 12 [inches]]]\n[equal [product 1 [yards]] [product 3 [feet]]]]\npprop \"feet \"sing \"foot\npprop \"foot \"plural \"feet\npprop \"gallons \"eqns ~\n[[equal [distance] [product [gas consumtion] [number of gallons of gas used]]]]\npprop \"gas \"eqns ~\n[[equal [distance] [product [gas consumtion] [number of gallons of gas used]]]]\npprop \"inch \"plural \"inches\npprop \"inches \"eqns [[equal [product 1 [feet]] [product 12 [inches]]]]\npprop \"people \"sing \"person\npprop \"person \"plural \"people\npprop \"speed \"eqns [[equal [distance] [product [speed] [time]]]]\npprop \"time \"eqns [[equal [distance] [product [speed] [time]]]]\npprop \"yards \"eqns [[equal [product 1 [yards]] [product 3 [feet]]]]\n```\n\nBrian Harvey, `[email protected]`" ]
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https://ncatlab.org/nlab/show/quaternionic+projective+space
[ "Contents\n\n# Contents\n\n## Idea\n\nThe quaternionic projective space $\\mathbb{H}P^n$ is the space of right (or left) quaternion lines through the origin in $\\mathbb{H}^{n+1}$, hence the space of equivalence classes $[q_1, \\cdots, q_{n+1}]$ of (n+1)-tuples of quaternions excluding zero, under the equivalence relation given by right (or left) multiplication with non-zero quaternions\n\n$\\mathbb{H}P^n \\;\\coloneqq\\; \\big\\{ [q_1, \\cdots, q_{n+1}] \\big\\} \\;\\coloneqq\\; \\Big( \\big\\{ (q_1, \\cdots, q_{n+1}) \\big\\} \\setminus \\{(0, \\cdots, 0)\\} \\Big) /_{ (q_1, \\cdots, q_{n+1}) \\sim (q_1 q, \\cdots, q_{n+1} q) \\vert q \\neq 0 }$\n\n## Properties\n\n### As a coset space\n\nAs any Grassmannian, quaternion projective space is canonically a coset space, in this case of the quaternion unitary group $Sp(n+1)$ by the central product group Sp(n).Sp(1):\n\n(1)$\\mathbb{H}P^n \\;\\simeq\\; \\frac{ Sp(n+1) }{ Sp(n)\\cdot Sp(1) }$\n\n### As a quaternion-Kähler symmetric space (Wolf space)\n\nBy the coset space-realization (1), quaternion projective space is naturally a quaternion-Kähler manifold which is also a symmetric space. As such it is an example of a Wolf space.\n\n### General\n\nM-theory on the 8-manifold$\\;$ HP2, hence on a quaternion-Kähler manifold of dimension 8 with holonomy Sp(2).Sp(1), is considered in\n• Michael Atiyah, Edward Witten, p. 75 onwards in $M$-Theory dynamics on a manifold of $G_2$-holonomy, Adv. Theor. Math. Phys. 6 (2001) (arXiv:hep-th/0107177)" ]
[ null ]
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https://greprepclub.com/forum/if-m-and-n-are-the-roots-of-the-equation-10439.html
[ "", null, "It is currently 23 Nov 2020, 08:09", null, "### GMAT Club Daily Prep\n\n#### Thank you for using the timer - this advanced tool can estimate your performance and suggest more practice questions. We have subscribed you to Daily Prep Questions via email.\n\nCustomized\nfor You\n\nwe will pick new questions that match your level based on your Timer History\n\nTrack\n\nevery week, we’ll send you an estimated GMAT score based on your performance\n\nPractice\nPays\n\nwe will pick new questions that match your level based on your Timer History\n\n#### Not interested in getting valuable practice questions and articles delivered to your email? No problem, unsubscribe here.", null, "# If m and n are the roots of the equation", null, "", null, "Question banks Downloads My Bookmarks Reviews Important topics\nAuthor Message\nIntern", null, "Joined: 18 Aug 2018\nPosts: 3\nFollowers: 0\n\nKudos [?]: 2 , given: 0\n\nIf m and n are the roots of the equation [#permalink]\nHI guys!\n\nQuestion:\n\nIf m and n are the roots of the equation $$a^2 - 6a + 8 = 0$$, then find the value of $$(m+n)(m-n)$$\n\nA. 12\n\nB. 8\n\nC. 16\n\nD. 4\n\nE.18\n\nNow, the answer should be 12, because the fractioning of the equation gets me (a-4) (a-2). However, what if I switched places here and put (a-2) (a-4). Then, m = 2 and n=4, thus (2+4) (2-4) = -12. Where am I going wrong? Sorry for this stupid question. And btw, roots of the equation are always positive then, right?\n\nAppreciate any help.\n\nLast edited by Carcass on 18 Aug 2018, 02:03, edited 1 time in total.\nEdited by Carcass\nFounder", null, "", null, "Joined: 18 Apr 2015\nPosts: 13874\nGRE 1: Q160 V160", null, "Followers: 313\n\nKudos [?]: 3671 , given: 12885\n\nRe: If m and n are the roots of the equation [#permalink]\nExpert's post\nHi,\n\nbefore to post a question on the board, please, follow the rule fr posting here https://greprepclub.com/forum/rules-for ... -1083.html and how to format a question here https://greprepclub.com/forum/qq-how-to ... -2357.html\n\nMoreover, post the question under the right section and not in general quant section.\n\nBack to the question.\n\nYou are right m=2 n=4 in which case the answer is -12\n\nBut could be the other way around also: m=4 an n=2 which is 12\n\nNo a good question.\n\nRegards\n_________________", null, "Intern", null, "Joined: 18 Aug 2018\nPosts: 3\nFollowers: 0\n\nKudos [?]: 2 , given: 0\n\nRe: If m and n are the roots of the equation [#permalink]\n1\nKUDOS\nAppreciate the comments, Carcass. Sorry for being careless, and thank you for the clarification on the question.\n\nHowever, I think you made a mistake there. If m=4 and n=2, then (m+n)(m−n) = (4+2) (4-2) = 12. I doesn't make a whole lot of difference though, because I guess we just established that this is not a well-thought-out question.\n\nThanks!", null, "Re: If m and n are the roots of the equation   [#permalink] 18 Aug 2018, 04:46\nDisplay posts from previous: Sort by\n\n# If m and n are the roots of the equation", null, "", null, "Question banks Downloads My Bookmarks Reviews Important topics", null, "", null, "Powered by phpBB © phpBB Group Kindly note that the GRE® test is a registered trademark of the Educational Testing Service®, and this site has neither been reviewed nor endorsed by ETS®." ]
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https://www.hindawi.com/journals/jmath/2021/6668711/
[ "#### Abstract\n\nIn order to simplify the complex calculation and solve the difficult solution problems of neutrosophic number optimization models (NNOMs) in the practical production process, this paper presents two methods to solve NNOMs, where Matlab built-in function “fmincon()” and neutrosophic number operations (NNOs) are used in indeterminate environments. Next, the two methods are applied to linear and nonlinear programming problems with neutrosophic number information to obtain the optimal solution of the maximum/minimum objective function under the constrained conditions of practical productions by neutrosophic number optimization programming (NNOP) examples. Finally, under indeterminate environments, the fit optimal solutions of the examples can also be achieved by using some specified indeterminate scales to fulfill some specified actual requirements. The NNOP methods can obtain the feasible and flexible optimal solutions and indicate the advantage of simple calculations in practical applications.\n\n#### 1. Introduction\n\nTraditional inventory models and production planning models involve deterministic constrained functions and/or objective functions in deterministic environments. Nevertheless, uncertainty is nearly universal in real world. Therefore, many uncertain optimization methods were proposed for optimization problems with uncertain variables, interval numbers, stochastic, and fuzzy logics . In many applied fields, such as management, engineering, and design problems, uncertain programming has been broadly carried out so far. In order to obtain the optimal crisp values of the objective function and the optimal feasible crisp solutions of the decision variables, the constrained functions and/or objective functions are usually changed into some crisp or deterministic programming problems in existing uncertain programming approaches. So, the aforementioned transformed methods are not really meaningful indeterminate approaches because the real indeterminate optimization problems can only indicate indeterminate solutions rather than optimal crisp solutions in indeterminate environments. Nevertheless, indeterminate programming problems imply the corresponding indeterminate optimal values of the objective function and indeterminate optimal solutions for the decision variables under indeterminate environments. So, it is necessary to find some fit optimization approaches for dealing with indeterminate programming problems with indeterminate solutions.\n\nSmarandache is a pioneer of indeterminacy theories which provide the new minds to solve indeterminacy problems. He adopted the imaginary value denoted by I and then introduced a neutrosophic number (NN) z = x + yI for x, y ∈ R (R: the set of all real numbers) composed of the determinate part x and indeterminate part yI. As for describing indeterminate and incomplete information, obviously, NNs in the indeterminacy theories are a useful mathematical tool. With the development of indeterminacy theories, NNs were also applied to fault diagnosis [19, 20] and decision making [21, 22] under indeterminate environments.\n\nFurther, thick function or interval function named neutrosophic function, neutrosophic precalculus, and neutrosophic calculus were provided by Smarandache in 2015, where thick function e: SE(S) (E(S) is the set of all interval functions) as the form of an interval function e(x) = [e1(x), e2(x)]. The indeterminate function was applied in engineering problems successfully. For example, Ye et al. [24, 25] and Chen et al. [26, 27] proposed expressions of neutrosophic function and applied NNs in analyzing the joint roughness coefficient. Later, Ye used neutrosophic linear equations of NNs to solve traffic flow problems.\n\nAt present, neutrosophic linguistic numbers, hesitant neutrosophic linguistic numbers, and their aggregation operators were applied to multiattribute decision making .\n\nBut in real situations, affected by each kind subjective and objective reasons, such as absences of precise information judged by decision makers or experts, loss of data, and measurement errors, there exist some indeterminate problems. As for the concepts of NNs, NN functions containing indeterminacy I can represent the indeterminate problems with partial certainty and partial uncertainty under indeterminate environments. Ye and Jiang and Ye introduced NN nonlinear and linear programming models and their preliminary solution methods. However, existing methods for solving complex NN optimization problems imply some difficulty and calculational complexity in their solution process. Inspired by the previous solution methods, this paper first selects the models of practical applications in production process, such as inventory models and production planning models. Then, NN nonlinear and linear mathematical models and their solution methods (Matlab built-in function “fmincon()” and operations of NNs) are built with indeterminacy I as our preliminary application study. Finally, real examples of NN linear programming (NN-LP) and NN nonlinear programming (NN-NP) problems illustrate the feasibility of the proposed methods. The advantage of the proposed methods is that the optimization calculations are simple and effective in practical applications.\n\nThe remainder of this paper is organized as follows. Section 2 depicts some concepts and their operations of NNs. Section 3 first introduces NN-NP problems with an inventory mathematical model and model formation and then uses two methods (Matlab built-in function “fmincon()” and operations of NNs) to solve the NN-NP problems in indeterminate setting. Section 4 presents NN-LP problems with the production planning mathematical model and model formation and then applies two methods regarding the Matlab built-in function “fmincon()” and operations of NNs to solve the solutions in the NN-NP problems and to show the simplicity and effectiveness of the proposed NN-LP methods. Conclusions and future research are provided in Section 5.\n\n#### 2. Mathematical Preliminaries\n\n##### 2.1. Some Concepts and Their Operations of Neutrosophic Numbers (NNs)\n\nThe concept of NN was first proposed by Smarandache [34, 35], which consists of two parts (a determinate part and an indeterminate part). He defined the mathematical expression form z = x + yI for x, y ∈ R, where R represents all real numbers and I is indeterminacy. So, it is conveniently used in indeterminate environments.\n\nFor example, consider that a NN is z = 13 + 5I. Then, its determinate part value is 13 and its indeterminate part value is 5I. When I ∈ [0, 0.5], it is equivalent to z ∈ [13, 15.5] for sure z ≥ 13.\n\nLet z1 = x1 + y1I and z2 = x2 + y2I be two NNs. Then, Smarandache [34, 35] gave their operations of NNs in the following:(1)z1 + z2 = x1 + x2 + (y1 + y2)I.(2)z1z2 = x1x2 + (y1y2)I.(3)z1 × z2 = x1x2 + (x1y2 + x2y1 + y1y2)I, in particular, when z1 = 0 and z2 = I, we get the equation with 0 × I = 0.(4) = (x1 + y1I)2 =  + (2x1y1 + )I, in particular, when z1 = I, we get the equation with I^2 = I.(5) for x2 ≠ 0 and x2 ≠ –y2.(6).\n\n##### 2.2. Example\n\nThere are two NNs z1 = 5 + 3I and z2 = 2 + 5I. Then, we can obtain the following results according to the above operations:(1)z 1 + z2 = x1 + x2 + (y1 + y2)I = 5 + 2 + (3 + 5)I = 7 + 8I.(2)z 1z2 = x1x2 + (y1y2)I = 5−2 + (3−5)I = 3−2I.(3)z 1 × z2 = x1x2 + (x1y2 + x2y1 + y1y2)I = 5 × 2 + (5 × 5 + 3 × 2 + 3 × 5)I = 10 + 46I.(4) = (x1 + y1I)2 =  + (2x1y1 + )I = 52 + (2 ×  5 × 3 + 32)I = 25 + 39I, = (x2 + y2I)2 =  + (2x2y2 + )I = 22 + (2 × 2 × 5 + 52)I = 4 + 45I.(5).(6).\n\n#### 3. Neutrosophic Number Nonlinear Programming (NN-NP)\n\n##### 3.1. NN-NP Mathematical Model\n\nThe usual mathematical model of NN-NP is represented in the following form [36, 37]:where : ZnZ(Z is the set of all NNs), and I ∈ [IL, IU](the interval range of I).\n\n##### 3.2. Inventory Mathematical Model \n###### 3.2.1. Notations\n\nThe following notations are used in the inventory model.\n\nThree decision variables:(i)D: demand/unit/time(ii)Qp: production quantity/batch(iii)Cs: setup cost/unit/time\n\nExcept the above cost variable CS, three other cost variables are(i)Cta: total average cost/unit/time(ii)Ctp: total production cost/cycle(iii)Ch: time depending on holding cost/unit/item\n\nOther time and space variables:(i)T: every cycle of length(ii)Q(t): inventory level at time t (t ≥ 0)(iii)S: total storage space area(iv)s0: space area/unit/quantity.\n\n###### 3.2.2. Assumptions\n\nThe inventory model is developed by considering the following assumptions:(i)Only one item is involved in the inventory system.(ii)The replenishment occurs with the near instantaneous response.(iii)The startup time can be ignored.(iv)The demand rate at any time is constant.(v)The total production cost Ctp is related to the setup cost CS and production quantity QP.(vi)Holding cost is the time depended function.\n\n##### 3.3. Model Formation\n\nAs shown in Figure 1, in every time period T, the value of the production quantity Q(t) decreases from Qp to zero. The slope of the line is constant negative D and denoted by .\n\nThe total average cost of the cycle T (denoted by Cta) consists of three sections: setup cost (denoted by C1), holding cost (denoted by C2), and production cost (denoted by C3).\n\nBecause we have the equation Q(t) = QpDt, we obtain the cycle T, .\n\nBased on equations (2) and (3), we obtain the following equation:\n\nSo, the inventory model is constructed as follows:\n\n##### 3.4. Solution Corresponding to Matlab Built-In Function “fmincon()”\n\nIn order to conveniently calculate the solutions, we simplify some parameters and set some constants with history records, where e = 18, f = 5, x = 1, y = 3, s0 = 200, and S= 1100. When we assume D = x1, Cs = x2, and Qp = x3, we can obtain the following mathematical model:\n\nAssume  = x1−40.496I,  = x2 + 0.058I, and  = x3−2I; then, equation (6) can be expressed in the following form:\n\nAccording to the de-neutrosophication technique proposed by Ye and considering I = 0 or 0.5 or 1 as the minimum or moderate or maximum indeterminacy, we can obtain three optimal solutions as follows:(1) = 80.615,  = 0.097,  = 7.500, and  = 4.187 for I = 0.(2) = 60.367,  = 0.126,  = 6.5, and  = 4.343 for I = 0.5.(3) = 40.119,  = 0.155,  = 5.5, and  = 4.525 for I = 1.\n\nClearly, using the indeterminacy I ∈ [0, 1], different optimal results are revealed. The optimal solutions of the optimization problem are  = [40.119, 80.615],  = [0.097, 0.155], and  = [5.5, 7.5] for  = [4.187, 4.525], which show the interval optimal ranges.\n\n##### 3.5. Solution Corresponding to Operations of NNs\n\nAccording to the front optimal solutions, we assume  = x1 + y1I = 80.615−40.496I,  = x2 + y2I = 0.097 + 0.058I, and  = x3y3I = 7.500−2I, and then we give the results by equation (9):\n\nBecause  = 80.615−40.496I,  = 0.097 + 0.058 I, and  = 7.500−2I, we can get  = 80.615,  = −40.496,  = 0.097,  = 0.058,  = 7.5, and  = −2. Then, we calculate the three costs, respectively, as follows:\n\nSetup cost:\n\nHolding cost:\n\nProduction cost:\n\nThen, we add the three costs and obtain the total cost Cta with equation (2) as follows:\n\nSo, the calculational results validate that the same solution is obtained by using the two methods of both the Matlab built-in function “fmincon” and the operations of NNs, which are  = [40.119, 80.615],  = [0.097, 0.155], and  = [5.5, 7.5] for  = [4.187, 4.525]. We also obtain every cost C1 = [1.047, 1.134], C2 = [ 2.093, 2.262], and C3 = [1.047, 1.129], which are the interval optimal ranges.\n\n#### 4. Production Planning Mathematical Model\n\n##### 4.1. NN-LP Mathematical Model\n\nThe usual mathematical model of NN-LP is similar to mathematical model (1), so we omit it.\n\n##### 4.2. Production Planning Mathematical Model\n###### 4.2.1. Notations\n\nThe following notations are used in the production planning model.\n\nNine decision variables:(i) to : product quantities of six plans of type I(ii) to : product quantities of two plans of type II(iii): product quantities of two plans of type III\n\nObjective function:(i): maximum profit\n\n###### 4.2.2. Assumptions\n\nThe production planning model is developed by considering the following assumptions:(i)Every product must pass two working procedures: A and B.(ii)The startup time of two working procedures can be ignored.(iii)Product quantities are only affected by validity time of machines.(iv)The demand rate at any time is constant.\n\n##### 4.3. Model Formation\n\nAs shown in Table 1, we consider an application in production planning studied by Hu . A company manufactures three types of products: Types I, II, and III. All types must pass two working procedures: A and B. We consider that procedure A can be operated on machine A1 or A2 and procedure B can be operated on the machines B1, B2, and B3. Type I can be operated on all machines of procedure A and procedure B; Type II can be operated on all machines of procedure A and only machine B1 of procedure B; Type III can be operated on only machine A2 of procedure A and machine B2 of procedure B. Our aim is to schedule the optimal production planning, which can pursue for the maximum profits. All used data are listed in Table 1, including required procedure time of every working procedure, processing fees, material cost, and selling price per unit. So, Type I has six plans to produce products, along with (A1, B1) or (A1, B2) or (A1, B3) or (A2, B1) or (A2, B2) or (A2, B3), respectively. Similarly, we consider the product quantities of the six plans , , , , , and , respectively. Type II has two plans to produce products, along with (A1, B1) or (A2, B1), and Type III has one plan to produce products, along with (A2, B2). We consider the product quantities of the remaining three plans , , and , respectively. So, we can get the following objective function.\n\nSo, we get the followed production planning mathematical model:\n\n##### 4.4. Solution regarding Matlab Built-In Function “fmincon()”\n\nAccording to the de-neutrosophication technique proposed by Ye and considering I = 0 or 0.5 or 1 as the minimum or moderate or maximum indeterminacy, we can obtain three optimal solutions as follows:(1) = 0,  = 778.508,  = 465.936,  = 0,  = 677.953,  = 56.452,  = 0,  = 474.359,  = 0, and  = 1297.389 for I = 0.(2) = 0,  = 0,  = 578.231,  = 0,  = 0,  = 0,  = 167.732,  = 338.221,  = 590.909, and  = 940.871 for I = 0.5.(3) = 0,  = 0,  = 625,  = 0,  = 0,  = 0,  = 146.667,  = 386.667,  = 583.333, and  = 762.717 for I = 1.\n\nClearly, using the indeterminacy I ∈ [0, 1], different optimal results are revealed. The optimal solutions of the optimization problem are  = [0, 0],  = [0, 778.508],  = [465.936, 625],  = [0, 0],  = [0, 677.953],  = [0, 56.452],  = [0, 146.667],  = [386.667, 474.359], and = [0, 583.333] for  = [762.717, 1297.389], which shows the interval optimal ranges.\n\n##### 4.5. Solution regarding Operations of NNs\n\nAccording the front optimal solutions, we next calculate the nine relation formulas of the indeterminacy I and variables , , , , , , , , and . For example, let us calculate  = 465.936 + 159.064I. Firstly, according to three points (0, 465.936), (0.5, 578.231), and (1, 625), we obtain the linear equation ( = 159.06I + 476.86). Next we amend the intercept of trend curve on the vertical coordinate. The other linear equations are obtained in the same way. So,  = x1 + y1I = 0 + 0I = 0,  = x2 + y2I = 778.508−778.508I,  = x3 + y3I = 465.936 + 159.064I,  = x4 + y4I = 0 + 0I = 0,  = x5 + y5I = 677.953−677.953I,  = x6 + y6I = 56.452−56.452I,  = x7y7I = 0 + 146.667I,  = x8 + y8I = 474.359−87.692I, and  = x9 + y9I = 0 + 583.333I; then, we calculate the results of equation (13) as follows:\n\n= [(1.2 + 0.03I) − (0.23 + 0.03I)] × ()  +  [(1.60 + 0.5I)  −  (0.30 + 0.07I)]  ×  ()  + [(2.30 + 0.3I)  −  (0.30 + 0.05I)]  ×   − (0.04 + 0.02I)  ×  [(4.5 + 1.7I) × ()  +  (8 + I) × ]  −  (0.02 + 0.01I) × [(6.7 + 1.8I) × ()  +  (8.6 + 1.4I)  ×      (11  −  I)  ×  ]  −  (0.05 + 0.02I)  ×  [(5.6  –  0.1I) × ( ) + (7.8 + 1.2I) × ()] − (0.10 + 0.02I)  ×  [(3.5 + 2.5I) × ( )  +  (10 + 2I) × ] − (0.04 + 0.02I)  ×  [(6.7 + 1.3I)  ×  ()]  =  0.97 × ( ) + (1.30 + 0.43I)  ×  () + (2.0 + 0.25I) ×  − (0.04 + 0.02I) × [(4.5 + 1.7I) × ( +  + ) + (8 + I) × ] − (0.02 + 0.01I)  ×  [(6.7 + 1.8I)  ×  (    )  +  (8.6  + 1.4I) ×  (11 – I) × ] − (0.05 + 0.02I) × [(5.6  –  0.1I)  ×  ( ) + (7.8 + 1.2I) × ()] − (0.10 + 0.02I)  ×  [(3.5 + 2.5I)× ()(10 + 2I) × ]  –  (0.04  +  0.02I)  ×  [(6.7 + 1.3I)  × ()] = 0.97 × ()  +  (1.30 + 0.43I)  ×  ( ) + (2.0 + 0.25I) ×  − (0.04  +  0.02I) × [(4.5 + 1.7I) × ( + ) + (8 + I) × ] − (0.02 + 0.01I) × [(6.7 + 1.8I) × () + (8.6 + 1.4I) ×  (11 – I) × ]  −  (0.05 + 0.02I) × [(7.8 + 1.2I)× ()]  −  (0.10 + 0.02I) × [(3.5 + 2.5I) × () (10 + 2I) × ] − (0.04 + 0.02I) × [(6.7 + 1.3I)  ×  ()]  =  0.97 × (778.508  −  778.508I  +  465.936  +  159.064I  +  677.953  − 677.953I + 56.452 – 56.452I) + (1.30 + 0.43I) × (0 + 146.667I+ 474.359 − 87.692I) + (2.0 + 0.25I) × (0 + 583.333I) − (0.04+ 0.02I) × [(4.5 + 1.7I) × (778.508 − 778.508I + 465.936 + 159.064I) + (8 + I) × (0 + 146.667I)] − (0.02 + 0.01I) × [(6.7 + 1.8I) × (0 + 677.953 − 677.953I + 56.452 − 56.452I) + (8.6 + 1.4I)  ×  (474.359  −  87.692I)  +  (11  −  I)  ×  (0  +  583.333I)]  − (0.05  +  0.02I)  ×  [(7.8  +  1.2I)  ×  (0  +  146.667I  +  474.359  − 87.692I)] − (0.10 + 0.02I) × [(3.5 + 2.5I)  × (778.508 – 778.508I + 677.953 − 677.953I) + (10 + 2I) × (0 + 583.333I)]−  (0.04  +  0.02I)  ×  [(6.7  +  1.3I)  ×  (465.936  +  159.064I + 56.452 − 56.452I)]  =  0.97  ×  (1978.849  −  1353.849I) + (1.3 + 0.43I)  ×  (474.359  +  58.975I) + (2 + 0.25I) × (0 + 583.333I) − (0.04 + 0.02I) × (5599.998 − 404.995I) − (0.02 + 0.01I) × (9000.001  +  699.9991I)  − (0.05 + 0.02I) × (3700 + 1100.006I)− (0.10 + 0.02I) × (5097.614  +  1902.383I)  −  (0.04  +  0.02I) × (3500 + 1500I) = 1919.484  −  1313.234I + 616.6667 + 306.001I + 1312.499I − 224 − 87.7I  −  180  −  111.000I  −  185 − 509.761 − 330.238I − 140 − 160.000I = 1297.389 − 534.672I.\n\nSo, these calculational results validate that the same solution is obtained by using the two methods of both the Matlab built-in function “fmincon()” and the operations of NNs, which are  = [0, 0],  = [0, 778.508],  = [465.936, 625],  = [0, 0],  = [0, 677.953],  = [0, 56.452],  = [0, 146.667],  = [386.667, 474.359], and = [0, 583.333] for  = [762.717, 1297.389] and show the interval optimal ranges.\n\n#### 5. Conclusion\n\nThis paper first introduced some concepts and their operations of NNs with indeterminacy I. Next, we built a mathematical model with constrained conditions and then constructed the corresponding inventory model and production planning model. Finally, we obtained the optimal solutions by using the two methods of the Matlab built-in function “fmincon()” and the operations of NNs to solve the NN-NP and NN-LP problems with constrained conditions as preliminary application study in indeterminate setting. The final results show that the two methods obtained the same effective solutions, but the former needs the Matlab built-in function along with the simple calculational process, while the latter needs a lot of operations of NNs along with the complex calculational process. Some contributions in this study are that (1) different methods can obtain the same optimal results, (2) the NN-NP and NN-LP methods provided the new application ways for engineering management, (3) the NN-NP and NN-LP methods are more suitable than other ones under uncertain environments as the generalization of traditional programming methods, and (4) the two approaches can obtain the interval solutions for avoiding determinate solutions of traditional programming methods.\n\nObviously, the proposed NN-LP and NN-NP methods can handle indeterminate and/or determinate mathematical programming problems, which are the generalization of existing uncertain or certain linear and nonlinear programming methods. As the preliminary application study in this paper, however, there exist a lot of mathematical solution methods and proof problems along with some complexity/difficulty in the nonlinear programming problems which need to be studied further. Hence, as our future works, one is to further analyze the two presented methods of this paper from the mathematical problems, such as the convexity problem in the nonlinear programming, the stability and solution range problems regarding the changeability of NNs, and the sensitivities of NNs on the solution results, and then NN-LP and NN-NP approaches will be extended to other fields, such as engineering design and management science.\n\n#### Data Availability\n\nThe data used to support the findings of this study are included within the article.\n\n#### Conflicts of Interest\n\nThe authors declare that they have no conflicts of interest." ]
[ null ]
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https://bookdown.org/danbarch/psy_207_advanced_stats_I/categorizing-and-summarizing-information.html
[ "# Chapter 2 Categorizing and Summarizing Information\n\n## 2.1 How to Tell a Story", null, "Figure 2.1: A Heartwarming Tale of Extreme Weather Events and Traumatic Brain Injury\n\nWe make choices about what to include in our stories – sometimes without even thinking about it (and sometimes we don’t remember or don’t know all of the details). When we summarize data, we’re telling stories about that data and we make choices in doing so.\n\nThis page is all about data: how we categorize it and how we summarize it. We are going to cover some of the different types of data, how we summarize data, and how what we leave in and what we leave out affect the story we tell about the data. And, of course, I have made some choices on what to include and what not to include on the page. There’s only so much we can cover.\n\n## 2.2 Types of Data\n\n### 2.2.1 Statistics and Parameters\n\nIn conversational English, pretty much any number that describes a fact can be called a “statistic.” In the field of statistics, however, the term has a specific connotation: a statistic1 is a number that describes a sample or samples2. Something like the proportion of 100 people polled at random who answered “yes” to survey question is a statistic. The average reaction time of 30 participants in a psychology study is a statistic. Something like the number of people who live in Canada? That’s not technically a statistic. Because the people who live in Canada is an entire population.3, the number of them is an example of a parameter4 Thus, statistics describe samples, and parameters describe populations.\n\nWhy is knowing that distinction important? It is not – I repeat, not – so that you can correct people who use the term statistic in casual conversation when you know that technically they should say parameter: that’s not a good way to make friends. It’s important for a couple of reasons:\n\n1. It is specifically important to know whether a number refers to a sample or to a population for use in some statistical procedures.5\n\n2. It is generally important to know that we use statistics to make inferences about parameters.\n\nOn that second point: scientists are rarely interested only in the subjects used in their research. There are exceptions – like case studies or some clinical trials – but usually scientists want to generalize the findings from a sample to the population. A cognitive researcher isn’t interested in the memory performance of a few participants in an experiment so much as what their performance means for all humans; a social psychologist studying the behavioral effects of prejudice does not mean to describe the effects of prejudice for just those who participate in the study but for all of society. It is unrealistic in the vast majority of scientific inquiries to measure that which they are interested in about the entire population – even researchers who do work with population-level data are working with things like census data and are thus somewhat limited in the types of questions they can investigate (that is, they can only work with answers to questions asked in the census they are working with).\n\nHypothetically, if you could invite the entire population to participate in a psychology experiment – if you could bring the nearly 8 billion people on earth to a lab – then most of the statisical tests to be discussed in this course would be irrelevant. If, say, the whole population had an average score of $$x$$ in condition A and an average score of $$x+1$$ in condition B, then the results conclusively would show that scores are higher in condition B than in condition A: no need in that case for fancy stats.\n\nStatistical tests, therefore, are designed for analyzing small samples*6 and for making inferences from those data about larger populations. In part because statistical tests are designed for samples that are much, much smaller in number than populations is that in those cases that researchers do have large amounts of data, the tests we run will almost always end up being statistically significant. Results of statistical tests should always be subject to careful scientific interpretation: perhaps more so when statistical significance is more a product of huge sample sizes than it is a meaningful finding in small ones.\n\nThere is also a notational difference between statistics and parameters. Symbols for statistics use Latin letters, such as $$\\bar{x}$$ and $$s^2$$; symbols for parameters use Greek letters, such as $$\\mu$$ and $$\\sigma^2$$. So, when you see a number associated with a Latin-letter symbol, that is a measurement of a sample, and when you see a number associated with a Greek-letter symbol, that is a measurement of a population.\n\n### 2.2.2 Scales of Measurement\n\nData are bits of information7, and information can take on many forms. The ways we analyze data depend on the types of data that we have. Here’s a relatively basic example: suppose I asked a class of students their ages, and I wanted to summarize those data. A reasonable way to do so would be to take the average of the students’ ages. Now suppose I asked each student what their favorite movie was. In that case, it wouldn’t make any sense to report the average favorite movie – it would make more sense to report the most popular movie, or the most popular category of movie.\n\nThus, knowing something about the type of data we have helps us choose the proper tools for working with our data. Here, we will talk about an extensive – but not exhaustive – set of data types that are encountered in scientific investigations.\n\n#### 2.2.2.1 S.S. Stevens’s Taxonomy of Data\n\nThe psychophysicist S.S. “Smitty” Stevens proposed a taxonomy of measurement scales in his 1946 paper *On the Theory of Scales of Measurement that was so influential that is often described without citation, as if the system of organization Stevens devised were as fundamental as a triangle having three sides, or the fact that $$1+1=2$$. To be fair, it’s a pretty good system. And, it is so common that it would be weird not to know the terminology from that 1946 paper. There are some omissions, though, and we will get to those after we discuss Stevens’s data types.\n\n##### 2.2.2.1.1 Discrete Data\n\nDiscrete data8 are data regarding categories or ranks. They are discrete in the sense that there are gaps between possible values: whereas a continuous measurement like length or weight can take on an infinite amount of values between any two given points (e.g., the distances between 1 and 2 meters include 1.5 meters, 1.25 meters, 1.125 meters, 1.0675 meters, etc.), a measurement of category membership can generally only take on as many values as there are categories; and a measurement of ranks can only take on as many values as there are things to be ranked.\n\n###### 2.2.2.1.1.1 Nominal (Categorical) Data\n\nNominal (categorical) data9 are indicators of category membership. Examples include year in school (e.g., freshman, sophomore, junior, senior, 1st year, etc.) and ice cream flavor (e.g., cookie dough, pistachio, rocky road, etc.). Nominal or categorical (the terms are 100% interchangeable) data are typically interpreted in terms of frequency or proportion, for example, how many 1st-year graduate students are in this course?, or, what proportion of residents of Medford, Massachusetts prefer vanilla ice cream?.\n\n###### 2.2.2.1.1.2 Ordinal (Rank) Data\n\nOrdinal (rank) data10 are measurements of the relative rank of observations. Usually these are numeric ranks (as in a top ten list), but they also can take on other descriptive terms (as in gold, silver, and bronze medal winners in athletic competition). Ordinal (or rank – like nominal and categorical, ordinal and rank are 100% interchangeable) data are interpreted in terms of relative qualities. For example, consider the sensation of pain: it’s impossible to objectively measure pain because it’s an inherently subjective experience that changes from person to person. Instead, medical professionals use a pain scale like the one pictured here:", null, "Figure 2.2: Looks like the red face murdered six people in prison, so maybe that’s more of an emotional pain.\n\nPain is therefore measured in terms of what is particularly painful (or not painful) to the medical patient, and their treatment can be determined as a result of whether pain is mild or severe compared to their baseline experience, or whether pain is improving or worsening.\n\n##### 2.2.2.1.2 Continuous (Scale) Data\n\nContinuous (scale) data11 , in contrast to discrete data, can take an infinite number of values within any given range. That is, a continuous measure can take on values anywhere on a number line, including all the tiny inbetween spots. Continuous (or scale data – these are also 100% interchangeable terms) data have values that can be transformed into things like averages (unlike categorical data) and are meaningful relative to each other regardless of how many measurements there are (unlike rank data). There are two main subcategories of continuous data in Stevens’s taxonomy, and the difference between those two categories is in the way you can compare measurements to each other.\n\n###### 2.2.2.1.2.1 Interval Data\n\nInterval data12 are data with meaningful subtractive differences – but not meaningful ratios – between measurements. The classic example here has to do with temperature scales. Imagine a day where the temperature is $$1^{\\circ}$$ Celsius. That’s pretty cold! Now imagine that the temperature the next day is $$2^{\\circ}$$ Celsius. That’s still cold! You likely would not say that the day when it’s $$2^{\\circ}$$ Celsius is twice as warm as the day before when it was $$1^{\\circ}$$ out, because it wouldn’t be! The Celsius scale (like the Fahrenheit scale) is measured in degrees because it is a measure of temperature relative to an arbitrary 0. Yes, $$0^{\\circ}$$ isn’t completely arbitrary because it’s the freezing point of water, but it’s also not like $$0^{\\circ}$$ C is the bottom point of possible temperatures (0 Kelvin is, but we’ll get to that in a bit). In that sense, the intervals between Celsius measurements are consistently meaningful: $$2^{\\circ}$$ C is 1 degree warmer than $$1^{\\circ}$$ C, which is the same difference between $$10^{\\circ}$$ C and $$11^{\\circ}$$ C, which is the same difference between $$36^{\\circ}$$ C and $$37^{\\circ}$$ C. But ratios between Celsius measurements are not meaningful – $$2^{\\circ}$$ is not twice as warm as $$1^{circ}$$, $$15^{\\circ}$$ is not a third as warm as $$45{\\circ}$$ C, and $$-25{\\circ}$$ C is certainly not negative 3 times as warm as $$75^{\\circ}$$ C.\n\n###### 2.2.2.1.2.2 Ratio Data\n\nRatio data13, as the name implies, do have meaningful ratios between values. If we were to use the Kelvin scale instead of the Celsius scale, then we could say that 2 K (notice there is no degree symbol there because Kelvin is not relative to any arbitrary value) represents twice as much heat as 1 K, and that 435 K represents 435 times as much heat as 1 K because there is a meaningful 0 value to that scale – it’s absolute zero (0 K). Any scale that stops at 0 will produce ratio data. A person who weighs 200 pounds weighs twice as much as a person who weighs 100 pounds because the weight scale starts at 0 pounds; a person who is 2 meters tall is 6/5ths as tall as somebody who is 1.67 meters tall (note that it doesn’t matter that you will never observe a person who weighs 0 pounds or stands 0 meters tall – it doesn’t matter what the smallest observation is, just where the bottom part of the scale is). Interval differences are also meaningful for ratio data, so all ratio data are also interval data, but not all interval data are ratio data (it’s a squares-and-rectangles situation).\n\nHere is an important note about the difference between interval and ratio data:", null, "just replace “a kid” with “in stats class” and “quicksand” with “the difference between interval and ratio data.” The important thing is to know that both are continuous data and that continuous data are very different from discrete data.\n\n##### 2.2.2.1.3 Categories that Stevens Left Out\n\nSo, our man Smitty has taken some heat for leaving out some categories, and subsequently people have proposed alternate taxonomies. I’m not going to pile on poor Smitty – leaving things out is a major theme of this page! – but keeping in mind what we said at the beginning of this section about the type of data informing the type of analysis, there are a couple of additional categories that I would add. Data of these types all have a place in Stevens’s taxonomy, but have special features that allow and/or require special types of analyses.\n\n###### 2.2.2.1.3.1 Cardinal (Count) Data\n\nCardinal (count)14 data are, by definition, ratio data: counts start at zero, and a count of zero is a meaningful zero. But, counts also have features of ordinal (rank) data: counts are discrete (like most of the dialogue in the show, Two and a Half Men is an unfunny joke15, based on the absurdity of continuous count data) and their values imply relativity between each other. As counts become larger and more varied, the more appropriate it is to treat them like other ratio data, but data with small counts (the actually most famous example of this is the number of 19th century Prussian Soldiers who died by being kicked by horses or mules – as you may imagine, the counts were pretty small) are distributed in specific ways and are ideally analyzed using different tools like Poisson and negative binomial modeling.\n\n###### 2.2.2.1.3.2 Proportions\n\nProportions16, like counts, can rightly be categorized as ratio data but have special features of their own. For example, the variance and standard deviation of a proportion can be calculated in both the traditional manner (follow the hyperlinks or scoll down to find the traditional equations), but also in its own way.17 Because proportions by definition are limited to the range between zero and one, they tend to arrange themselves differently than data that are unbounded (that is, data look different when they are squished).\n\nProportional data are also similar to count data in that they A. are often treated like ratio data (which is not incorrect) and B. are often analyzed using special tools. In general, the shape of distributions of proportions are beta distributions – we will talk about those later.\n\n###### 2.2.2.1.3.3 Binary Data\n\nBinary (dichotomous) data18 are, as the name implies, data that can take one of two different values. Binary data can be categorical – as in yes or no or pass or fail – or numeric – as in having 0 children or more than 0 children – but regardless can be given the values $$0$$ or $$1$$. Binary data have a limited set of possible distributions – all $$0$$, all $$1$$, and some $$0$$/some $$1$$. We will discuss several treatments of binary data, including uses of binomial probability and logistic regression.\n\n### 2.2.3 Dependent and Independent Variables, Predictor Variables and Predicted Variables\n\nAnother important way to categorize variables is in terms of input and output. Take for example a super-simple physics experiment: rolling a ball down a ramp. In that case, the input is whether we push the ball or not (that’s a binary variable); and the output is whether it rolls or not (also binary). Most of the time, we are going to use the term independent variable19 to describe the input and dependent variable20 to describe the output, and our statistical analyses will focus on the extent to which the dependent variable changes as a function of changes to the independent variable.\n\nThe other terminology we will use to describe inputs and outputs is in terms of predictor variable21 and predicted (outcome) variable. Those terms are used in the context of correlation and regression (although the terms independent and dependent are used there as well). The predictor/predicted terms are similar to the independent/dependent terms in that the latter is considered to change as some kind of function of changes in the former. They are also similar in that the former are usually assigned to be the $$x$$ variable and the latter are usually assigned to be the $$y$$ variable.", null, "They are different – and this is super-important – in that changes in an independent variable are hypothesized to cause changes in the dependent variable, while the changes in a predictor variable are hypothesized to be associated with changes in the predicted variable, because correlation does not imply causation.\n\n## 2.3 Summary Statistics\n\n### 2.3.1 A Brief Divergence Regarding Histograms\n\nThe histogram22 is both one of the simplest and one of the most effective forms of visualizing sets of data. They will be covered at length on the page on data visualization, but a brief introduction here will be helpful tools for describing the different ways that we summarize data.\n\nA histogram is a univariate23 visualization. Possible values of the variable being visualized are represented on the $$x$$-axis and the frequency of observations of each of those values are represented on the $$y$$-axis (this frequency can be an absolute frequency – the count of observations – or a relative frequency – the number of observations as a proportion or percentage of the total number of observations). The possible values represented on the $$x$$-axis can be divided into either each possible value of the variable or into bins of adjacent possible values: for example, a histogram of people’s chronological ages might put values like $$1, 2, 3, ..., 119$$ on the $$x$$-axis, or it might use bins like $$0 - 9, 10 - 19, ..., 110-119$$. There is no real rule for how to arrange the values on the $$x$$-axis, despite the fact that default values for binwidth and/or number of bins are built in to statistical software packages that produce histograms: it is up to the person doing the visualizing to choose the width of bins that best represents the distribution of values in a data set.\n\nHere’s an example of a histogram:", null, "Figure 2.3: Histogram of Points Scored by Players in the 2019-2020 NBA Season\n\nThis histogram represents the number of points scored by each player in the 2019-2020 NBA season (data from Basketball Reference). Each bar represents the number of players who scored the number of points represented on the $$x$$-axis. The number of points are sorted into bins of 50, so the first bar represents the number of players who scored 0 – 50 points, the second bar represents the number of players who scored 51 – 100 points, etc. All of the bars in a histogram like this one are adjacent to each other, which is a standard feature of histograms that shows that each bin is numerically adjacent to the next. That layout implies that difference between one bar and the next is a difference in the grouping of the one variable – gaps between all of the bars (as in bar charts) imply a categorical difference between observations, which is not the case with histograms. Apparent gaps in histograms – as we see in Figure 2.3 between 1900 and 1950 and again between 2000 and 2300, are really bars with no height. In the case of our NBA players, nobody scored between 1900 and 1950 points, and nobody scored between 2000 and 2300 points.24\n\nAgain: histograms will be covered in more detail in the page on data visualization. For now, it suffices to say that histograms are a good way to see an entire dataset and to pick up on patterns. Thus, we will use a few of them to help demonstrate what we leave in and what we leave out when we summarize data.\n\n### 2.3.2 Central Tendency\n\nCentral tendency25 is, broadly speaking, where a distribution of data is positioned. The central tendency of a dataset is similar to a dot on a geographic map that indicates a city’s position: while the dot indicates a central point in the city, it doesn’t tell you how far out the city is spread in each direction from that point, nor does it tell you things like where most of the people in that city live. In that same sense, the central tendency of a distribution of data gives an idea of the midpoint of the distribution, but doesn’t tell you anything about the spread of a distribution, or the shape of a distribution, or how concentrated the distribution is in different places.\n\nSo, the central tendency of a distribution is basically the middle of a distribution – but there are several ways to define the middle: each measure is a different way to tell the story of the center aspect of a distribution.\n\n#### 2.3.2.1 Mean\n\nWhen we talk about the mean26 in the context of statistics, we are usually referring to the arithmetic mean of a distribution: the sum of all of the numbers in a distribution divided by the number of numbers in a distribution. If $$x$$ is a variable, $$x_i$$ represents the $$i^{th}$$ observation of the variable $$x$$, and there are $$n$$ observations, then the arithmetic mean symbolized by $$\\bar{x}$$ is given by:\n\n$\\bar{x}=\\frac{\\sum_{i=1}^n{x_i}}{n}.$ That equation might be a little more daunting than it needs to be.27\n\nFor example, if we have $$x=\\{1, 2, 3\\}$$, then:\n\n$\\bar{x}=\\frac{1+2+3}{3}=2.$ The calculation for a population mean is the same as for a sample mean. In the equation, we simply exchange $$\\bar{x}$$ for $$\\mu$$ (the Greek letter most similar to the Latin m) and the lower-case $$n$$ for a capital $$N$$ to indicate that we’re talking about all possible observations (that distinction is less important and less-frequently observed than the distinction between Latin letters for statistics and Greek letters for parameters, but I find it useful):\n\n$\\mu=\\frac{\\sum_{i=1}^Nx_i}{N}.$\n\n##### 2.3.2.1.1 What the Mean Tells Us\n1. The mean gives us the expected value28 of a distribution of data. In probability theory, the expected value is the average event that could result from a gamble (or anything similar involving probability): for example, for every 10 flips of a fair coin, you could expect to get $$5~heads$$ and $$5~tails$$. The expected value is not necessarily the most likely value – in one flip of a fair coin, the expected value would be $$1/2~heads~and~1/2~tails$$, which is absurd (a coin can’t land half-heads and half-tails) – but it is the value you could expect, on average, in repeated runs of gambles.\n\nIn the context of a variable $$x$$, the expected value of $$x$$ – symbolized $$E(x)$$ – is the value you would expect, on average, from repeatedly choosing a single value of $$x$$ at random. Let’s revisit the histogram of point totals for NBA players in the 2019-2020 season, now adding a line to indicate where the mean of the distribution lies:", null, "Figure 2.4: Histogram of Points Scored by Players in the 2019-2020 NBA Season; Dashed Line Indicates Mean Points Scored\n\nOn average, NBA players scored 447.61 points in the 2019-2020 season. Of course, nobody scored exactly 447.61 points – that’s not how basketball works. But, the expected value of an NBA player’s scoring in that season was 447.61 points: if you selected a player at random and looked up the number of points, occasionally you would draw somebody who scored more than 1500 points, and occasionally you would draw somebody who scored fewer than 50 points, but the average of your draws would be the average of the distribution.\n\n1. For any given set of data $$x$$, we can take a number $$y$$ and find the errors29 between $$x_i$$ and $$y$$: $$x_i-y$$. The mean of $$x$$ is the number that minimizes the squared errors $$\\left( x_i-y \\right)^2$$. For example, imagine you were asked to guess a number from a set of six numbers. If those numbers were $$x=\\{1, 1, 1, 2, 3, 47\\}$$, if you guessed “2,” then you would be off by a little bit if one of the first five numbers were drawn, but you would be off by a lot –45 – if the sixth number were drawn, and that error would look even worse if you were judged by _the amount you were off were squared – $$45^2=2,025$$. Now, you may ask, in what world would such a scenario even happen? Well, as it turns out, it happens all the time in statistics: when we describe data, we often have to balance our errors to make consistent predictions over time, and when our errors can be positive or negative and exist in a 2-dimensional $$x, y$$ plane, minimizing the square of our errors becomes super-important (for more, see the page on correlation and regression).\n\n2. Related to points (1) and (2), the mean can be considered the balance point of a dataset: for every number or number less than the mean, there is a number or are numbers greater than the mean to balance out the distance. Mathematically, we can say that:\n\n$\\sum_{i=1}^n \\left( x_i-\\bar{x} \\right)=0$ For those reasons, the mean is the best measure of central tendency for taking all values of $$x$$ into account in summarizing a set of data. While that is often a positive thing, there are drawbacks to that quality as well, as we are about to discuss.\n\n#### 2.3.2.2 What the Mean Leaves Out\n\n1. The mean is the most susceptible of the measures of central tendency to outliers.30 In Figure 2.5, the gross revenue of major movie releases for the year 1980 are shown in a histogram. In that year, the vast majority of films earned betwee $0 and$103 million, with one exception…", null, "Figure 2.5: Luke, I am your outlier!\n\nThe exception was Star Wars Episode V: The Empire Strikes Back, which made $203,359,628 in 1980 (that doesn’t count all the money it made in re-releases), nearly twice as much as the second-highest grossing film (9 to 5, which is a really good movie but is not part of a larger cinematic universe). The mean gross of 1980 movies was$24,370,093, but take out The Empire Strikes Back and the mean was $21,698,607, a difference of about$2.7 million (which is more than 13% of 1980-released movies made on their own). The other measures of central tendency don’t move nearly as much: the median changes by $63,098 depending on whether you include Empire or not, and the mode doesn’t change at all. We’re left with a bit of a paradox: the mean is useful because it can balance all values in a dataset but can be misleading because the effect of outliers on it can be outsized relative to other measures of central tendency. So is the mean’s relationship with extreme values a good thing or a bad thing? The (probably unsatisfying) answer is: it depends. More precisely, it depends on the story we want to tell about the data. To illustrate, please review a pair of histograms. Figure 2.6 is a histogram depicting the daily income in one month for an imaginary person who works at an imaginary job where they get paid imaginary money once a month.", null, "Figure 2.6: Daily Expenditures for a Real Month for an Imaginary Person We can see that for 29 of the 30 days in September, this imaginary person has negative net expenditures – they spend more money than they earn – and for one day they have positive net expeditures (the day that they both get paid and have to pay the rent) – they earn much more than they spend. That day with positive net expeditures is the day of the month when they get paid. Payday is a clear outlier – it sits way out from the rest of the distribution of daily expenditures. But, if we exclude that outlier, the average daily expenditure for our imaginary person is$-35.19 and if we include the outlier, the average daily expenditure is \\$5.99 – the difference between our imaginary person losing money every month and earning money every month. Thus, in this case, using the mean with all values of $$x$$ is a better representation of the financial experience of our imaginary hero.\n\nNow, let’s look at another histogram, this one with a dataset of 2 people. Figure 2.7 is a histogram of the distribution of years spent as President of the United States of America in the dataset $$x=\\{me, Franklin~Delano~Roosevelt\\}$$.", null, "Figure 2.7: Terms Spent as US President: Me and Franklin Delano Roosevelt\n\nHere is a case where using the mean is obviously misleading. Yes, it is true that the average number of years spent as President of the United States between me and Franklin Delano Roosevelt is six years. I didn’t contribute anything to that number: I’ve never been president and I don’t really care to ever be president. So, to say that I am part of a group of people that averages six years in office is true, but truly useless. Thus, some judgment is required when choosing to use the mean to summarize data.\n\n1. This is also going to be true of the median, and to a lesser extent the mode, but using the mean to summarize data leaves out information about the shape of the distribution beyond the impact of outliers. In Figure 2.8, we see three distributions of data with the same mean but very different shapes.", null, "Figure 2.8: Histogram of Three Distributions with the Same Mean\n\nAs shown in Figure 2.8, Distribution A has a single peak, Distribution B has two peaks, and Distribution C has three peaks (the potential meanings of multiple peaks in distributions is discussed below in the section on the mode). But, you wouldn’t know that if you were just given the means of the three distributions. We lose that information when we go from a depiction of the entire distributions (as the histograms do visually) to a depiction of one aspect of the distributions – in this case, the means of the distributions. Information loss is a natural consequence of summarization:31 it happens every time we summarize data. It is up to the responsible scientist to understand which information is being lost in any kind of summarization (incidentally, histograms and other forms of data visualization are great ways to reveal details about distributions of data) and to choose summary statistics accordingly.\n\n#### 2.3.2.3 Median\n\nThe median32 is the value that splits a distribution evenly in two parts. If there are $$n$$ numbers in a dataset, and $$n$$ is odd, then the median is the $$\\left( \\frac{n}{2}+\\frac{1}{2} \\right)^{th}$$ largest value in the set; if $$n$$ is even, then the median is the average of the $$\\left( \\frac{n}{2}\\right)^{th}$$ and the $$\\left( \\frac{n}{2}+1 \\right)^{th}$$ largest values. That makes it sound a lot more complicated than it is – here are two examples to make it easier:\n\n$if~x=\\{1, 2, 3, 4, 5\\},$ $then~median(x)=3$ $if~x =\\{1, 2, 3, 4\\},$ $then~median(x)=\\frac{2+3}{2}=2.5$\n\n##### 2.3.2.3.1 What the Median Tells us\n1. The median tells us more about the typical values of datapoints in a distribution than does the mean or the mode. For that reason, the median is famously used in economics to describe the central tendency of income – income can’t be negative (net worth can) so it is bounded by 0, and has no upper bound and thus is skewed very, very positively.33\n\nThe median is used for a lot of skewed distributions in lieu of the mean not only because it is more resistant to outliers than is the mean, but also because it minimizes the absolute errors made by predictions. By absolute errors we mean the absolute value of the errors $$|x_i-y|$$, where $$y$$ is the prediction and $$x_i$$ is one of the predicted scores. Thus, when we use the median in the case of income, we are saying that representation is closer (positively or negatively) to more of the observed values than any other number.\n\n1. The median is the basis of comparison used in two important nonparametric tests: The Mann-Whitney $$U$$ test and the Wilcoxon Signed-ranks test. It is used in those tests due to its applicability to both continuous data and ordinal data.\n\nThe median is also the basis of a set of analytic tools known as robust statistics, a field established to try to limit the influence of outliers and non-normal distributions. Robust statistics as a field is beyond the scope of this course, but I encourage you to read more if you are interested.\n\n##### 2.3.2.3.2 What the Median Leaves Out\n1. Like the mean, the median does not tell us much about the shape of a distribution.\n\n2. Outside of the field of Robust Statistics and certain nonparametric tests, the median, unlike the mean, is not a measure of central tendency used in classical statistical tests.\n\n#### 2.3.2.4 Mode\n\nThe mode34 The mode is the most likely value or values of a distribution to be observed. A distribution is unimodal if it has one clear peak, as in part a of Figure 2.9. A distribution is bimodal if it has two clear peaks, as in part b. Distributions with more than one peak are collectively known as multimodal distributions.", null, "Figure 2.9: A Unimodal and a Bimodal Distribution\n\nMultimodality itself is of great scientific interest. As we will cover at length when we discuss frequency distributions, unimodality is a common assumption regarding patterns of data found in nature. When multiple modes are encountered, it may be a sign that there are multiple processes going on – for example, the distribution of gas mileage statistics for a car will have different peaks for driving in a city (with lots of starts and stops that consume more gas) and for driving on the highway (which is generally more fuel-efficient). Multimodality can also suggest that there is actually a mixture of distributions in a dataset – for example, a dataset of the physical heights of people might show two peaks that reflect a mixture of people assigned male at birth and people assigned female at birth, two groups that tend to grow to different adult heights.\n\nOne note on multimodality: multiple peaks don’t have to be exactly as high as each other. Multimodality is more about a peaks-and-valleys pattern than a competition between peaks.\n\n##### 2.3.2.4.1 What the Mode Tells us\n1. In a unimodal frequency distribution, the mode is the maximum likelihood estimate35 of a distribution. In terms of sampling, it’s the most likely value to draw from a distribution (because there are the most observations of it). In a multimodal distributions, the modes are related to local maxima of the likelihood functions. Don’t worry too much about that for now.\n\n2. The mode minimizes the total number of errors made by a prediction. A nice example that I am stealing from my statistics professor is that of a proprietor of a shoe store. If you want to succeed in shoe-selling, you don’t want to stock up on the mean shoe size – that could be a weird number like 8.632 – nor on the median shoe size – being off by a little bit doesn’t help you a lot here – you want to stock up the most on the modal shoe size to fit the most customers.\n\n3. Uniquely among the mean, median, and mode, the mode can be used with all kinds of continuous data and all kinds of discrete data. There is no way to take the mean or median of categorical data. You can but probably shouldn’t use the mean of rank data36 (the median is fine to use with rank data). Because the mode is the most frequent value, it can be the most frequent continuous value (or range of continuous values, depending on the precision of the measurement), the most frequent response on an ordinal scale, or the most frequent observed category.\n\n4. Unlike the mean and the median, the mode can tell us if a distribution has multiple peaks.\n\n##### 2.3.2.4.2 What the Mode Leaves Out\n1. Like the other measures of central tendency, the mode doesn’t tell us anything about the spread, the shape, or the height on each side of the peak of a distribution. There are some sources out there – and I know this because I have never said it in class nor written it down in a text but have frequently encountered it as an answer to the question what is a drawback of using the mode? – that say that the mode is for some reason less useful because “it only takes one value of a distribution into account.” That’s wrong for one reason – there can be more than one mode, so it doesn’t necessarily take only one value into account – and misleading for another: the peak of a distribution depends, in part, on all the other values being less high than the peak. To me, saying that the peak of a distribution only considers one value is like saying that identifying the winner of a footrace only takes one runner into account. I think the germ of a good idea in that statement is that we don’t know how high the peak of a distribution is, or what the distribution around it looks like, but that’s a problem with central tendency in general.\n\n2. Although, related to that last part: the mode doesn’t really account for extreme values, but neither does the median.\n\n### 2.3.3 Quantiles\n\nQuantiles37 are values that divide distributions into sections of equal size. We have already discussed one quantile: the median, which divides a distribution into two sections of equal size. Other commonly-used quantiles are:\n\nQuantile Name Divides The Distribution Into\nQuintiles Fifths\nQuartiles Fourths\nDeciles Tenths\nPercentiles Hundreths\n\nAt points where quantiles coincide, their names are often interchanged. For example, the median is also known as the 50th percentile and vice versa, the first quartile is often known as the 25th percentile and vice versa, etc.\n\n#### 2.3.3.1 Finding quantiles\n\nDefining the quantile cutpoints of a distribution of data is easy if the number of values in the distribution are easily divided. For example, if $$x=\\{0, 1, 2, 3, ..., 100\\}$$, the median is $$50$$, the deciles are $$\\{10, 20, 30, 40, 50, 60, 70, 80, 90\\}$$, the 77th percentile is $$77$$, etc.. When $$n$$ is not a number that is easily divisible by a lot of other numbers, it gets a bit more complicated because there are all kinds of tiebreakers and different algorithms and stuff. The things that are important to know about finding quantiles are:\n\n1. We can use software to find them (for example, the R code is below),\n2. Occasionally, different software will disagree with each other and/or what you would get by counting out equal proportions of a distribution by hand, and\n3. Any disagreement between methods will be pretty small, probably inconsequential, and explainable by checking on the algorithm each method uses.\n\n#### 2.3.4.1 Range\n\nThe Range38 is expressed either as the minimum value of a variable and the maximum value of a variable (e.g._$$x$$ is between $$a$$ and $$b$$), or as the difference between the highest value in a distribution and the lowest value in a distribution (e.g., the range of $$x$$ is $$b-a$$). For example:\n\n$x=\\{0, 1, 1, 2, 3, 5, 8, 13, 21, 34, 55\\}$ $Range(x) = 55 – 0 = 55$\n\nThe range is highly susceptible to outliers: just one weird min or max value can risk gross misrepresentation of the dataset. For that reason, researchers tend to favor our next measure of spread…\n\n#### 2.3.4.2 Interquartile Range\n\nThe Interquartile range39 is the width of the middle 50% of the data in a set. To find the interquartile range, we simply subtract the 25th percentile of a dataset from the 75th percentile of the data.\n\n$IQR=75th~percentile-25th~percentile$\n\n#### 2.3.4.3 Variance\n\nVariance40 is both a general descriptor of the way things are distributed (we could, for example, talk about variance in opinion without collecting any tangible data) and a specific summary statistic that can be used to evaluate data. The variance is, along with the mean, one of the two key statistics in making inferences.\n\nThere are two equations for variance: one is for a population variance parameter, and the other is for a sample variance statistic. Both equations represent the average squared error of a distribution. However, to apply the population formula to a sample would consistently underestimate the variance of a sample41 and thus an adjustment is made in the denominator.\n\n##### 2.3.4.3.1 Population Variance\n\n$\\sigma^2=\\frac{\\sum{\\left(x-\\mu \\right)^2}}{N}$\n\n##### 2.3.4.3.2 Sample Variance\n\n$s^2=\\frac{\\sum{\\left(x-\\bar{x} \\right)^2}}{n-1}$\n\nAside from the differences in symbols between the population and sample equations – Greek letters for population parameters are replaced by their Latin equivalents for the sample statistics – the main difference is in the denominator. The key reason for the difference is related to the nature of $$\\mu$$ and $$\\bar{x}$$. For any given population, there is only one population mean – that’s $$\\mu$$ – but there can be infinite values of $$\\bar{x}$$ (it just depends on which values you sample). In turn, that means that the error term $$x-\\bar{x}$$ depends on the mean of the sample (which, again, itself can vary). That mean is going to vary a lot more if $$n$$ is small – it’s a lot easier to sample three values with a mean wildly different from the population mean than it is to sample a million values with a mean wildly different from the population mean – so the bias that comes from using the population mean equation to calculate sample variance is bigger for small $$n$$ and smaller for big $$n$$.\n\nTo correct for that bias, the sample variance equation divides the squared errors not by the number of observations but by the number of observations that are free to vary given the sample mean. That sounds like a very weird concept, but hopefully this example will help:\n\nIf the mean of a set of five numbers is $$3$$ and the first four numbers are $$\\{1, 2, 4, 5\\}$$, what is the fifth number?\n\n$3=\\frac{1+2+4+5+x}{5}$\n\n$15=12+x$ $x=3$\n\nThis means that if we know the mean and all of the $$n$$ values in a dataset but one, then we can always find out what that one is. In turn, that means that if you know the mean, then $$n-1$$ of the values of a dataset are free to vary except one: that last one has to be whatever value makes the sum of all the values equal $$\\bar{x}/n$$.In general, the term that describes the number of things that are free to vary is degrees of freedom42, and for calculating a sample mean, the degrees of freedom – abbreviated df – is equal to $$n-1$$, so that is the denominator we use for the sample variance.\n\nOn a technical note, the default calculation in statistical softwares is, unless otherwise specified, the sample standard variance. If you happen to have population-level data and want to find the population variance parameter, just multiply the result you get from the software by $$(n-1)/n$$ to change the denominator.\n\n#### 2.3.4.4 Standard Deviation\n\nThe standard deviation43 is the square root of the variance. It is a measure of the typical deviation (reminder: deviation = error = residual) from the mean (we can’t really say “average deviation from the mean,” because technically the average deviation from any mean is zero). The standard deviation has a special mathematical relationship with the normal distribution, which we will cover in the unit on frequency distributions when that kind of thing will make more sense.\n\nAs the standard deviation is the square root of the variance, there is both a population parameter for standard deviation – which is the square root of the population parameter for variance – and a sample statistic for standard deviation – which is the square root of the sample statistic for variance.\n\n##### 2.3.4.4.1 Population Standard Deviation\n\n$\\sigma=\\sqrt{\\sigma^2}=\\sqrt{\\frac{\\sum{\\left(x-\\mu \\right)^2}}{N}}$\n\n##### 2.3.4.4.2 Sample Standard Deviation\n\n$s=\\sqrt{s^2}=\\sqrt{\\frac{\\sum{\\left(x-\\bar{x} \\right)^2}}{n-1}}$ As with the variance, the default for statistical software is to give the sample version of the standard deviation, so multiply the result by $$\\sqrt{n-1}/\\sqrt{n}$$ to get the population parameter.\n\n### 2.3.5 Skew\n\nLike the variance, the skew44 or skewness is both a descriptor of the shape of a distribution and a summary statistic that can be used to evaluate the way a variable is distributed. Unlike the variance, the skewness statistic isn’t used in many statistical tests, so here we will focus more on skewness as a shape and less on skewness as a quantity.\n\nThe skew of a distribution be described in one of three ways. A positively skewed distribution has relatively many small values and relatively few large values, creating a distribution that appears to point in the positive direction on the $$x$$ axis. Positive skew is often a sign that a variable has a relatively strong lower bound and a relatively weak upper bound – for example, we can again think of income, which has an absolute lower bound at 0 and no real upper bound (at least in a capitalistic system). A negatively skewed distribution has relatively few small values and relatively many large values, creating a distribution that appears to point in the negative direction on the $$x$$ axis. Negative skew is a sign that a variable has a relatively strong upper bound and relatively weak lower bound – for example, the grades on a particularly easy test. Finally, a balanced distribution is considered symmetrical. Symmetry indicates a lack of bounds on the data or, at least, that the bounds are far enough away from most of the observations to not make much of a difference – for example, the speeds of cars on highways tend to be symmetrically distributed: even though there is an obvious lower bound (0 mph) and an upper bound on how fast commercially-produced cars can go (based on a combination of physics, cost, and regard for the safety of self and others), neither have much influence on the vast majority of observations.\n\nFigure 2.10 shows examples of a positively skewed distribution, a symmetric distribution, and a negatively skewed distribution.", null, "Figure 2.10: Distributions with Different Skews\n\nWhen we talked about the mode, we talked about the peak (or peaks) of distributions. Here we will introduce another physical feature of distributions: tails45. A tail of a distribution is the longish, flattish part of a distribution furthest away from the peak. For a positively skewed distribution, there is a long tail on the positive side of the peak and a short tail or no tail on the negative side of the peak. For a negatively skewed distribution, there is a long tail on the negative side of the peak and a short tail or no tail on the postive side of the peak. A symmetric distribution has symmetric tails. We’ll talk lots more about tails in the section on kurtosis.\n\nThe term skewness is really most meaningful when talking about unimodal distributions – as you can imagine, having multiple peaks would make it difficult to evaluate the relative size of tails. If, for example, you have one relatively large peak and one relatively small peak, is the small peak part of the tail of the large peak? It’s best not to get into those kinds of philsophical arguments when describing distributions: in a multimodal distribution, the multimodality is likely a more important feature than the skewness.\n\n#### 2.3.5.1 Skewness statistics\n\nAs noted above, skewness can be quantified. The skewness statistic is rarely used, and if it is used, it is to note that negative values indicate negative skew and positive values indicate positive skew. So, let’s dive briefly into the skewness statistic (and the statistic parameter), and if you should ever need to make a statement about its value, you will know how it is calculated.\n\nAs with the variance and the standard deviation, there is an equation describing (mostly theoretical) population-level skewness and another equation describing sample skewness that includes an adjustment for bias in sub-population-level samples.\n\n##### 2.3.5.1.1 Population Skewness\n\nThe skewness of population-level data is given by\n\n$\\widetilde{\\mu}_3=E\\left[ \\left( \\frac{x-\\mu}{\\sigma} \\right)^3 \\right]=\\frac{\\frac{1}{n}\\sum(x-\\mu)^3}{\\sigma^3}$ with $$\\widetilde{\\mu}_3$$ indicating that it is the standardized third moment of the distribution (for more on what that barely-in-English phrase means, please see the bonus content below) and $$\\sigma$$ is the standard deviation.\n\n##### 2.3.5.1.2 Sample Skewness\n\nThe sample skewness formula used by statistical software packages (all of them, as far as I can tell from my research) is:\n\n$sample~skewness=\\frac{n}{(n-1)(n-2)}\\frac{\\sum(x-\\bar{x})^3}{s^3}$ where $$s$$ is the sample standard deviation\n\n### 2.3.6 Kurtosis\n\nKurtosis46 is a measure of the lightness or heaviness of the tails of a distribution. The heavier the tails, the more extreme values (relative to the peak) will be observed. A light-tailed or platykurtic distribution will have very few extreme values. A medium-tailed or mesokurtic distribution will produce extreme values at the same rate as the normal distribution (which is the standard for comparison), and a heavy-tailed or leptokurtic will produce more extreme values than the normal distribution. An example of a platykurtic distribution, an example of a mesokurtic distribution, and an example of a leptokurtic distribution are shown in Figure 2.11.", null, "Figure 2.11: Distributions with Different Kurtosis\n\n#### 2.3.6.1 Kurtosis statistics\n\nThe kurtosis statistic is used even less frequently than the skewness statistic (this section is strictly for the curious reader). For a perfectly mesokurtic (read: a normal distribution), the kurtosis is 347.\n\n##### 2.3.6.1.1 Population Kurtosis\n\nThe kurtosis of population-level data is given by^[The excess kurtosis parameter is given by simply subtracting 3: $\\frac{\\sum_{i=1}^N \\left( x-\\mu\\right)^4 }{\\left(\\sum_{i=1}^N(x-\\mu)^2 \\right)^2 }-3$\n\n$Kurtosis(x)=E\\left[ \\left( \\frac{x-\\mu}{\\sigma}\\right )^4\\right]=\\frac{\\sum_{i=1}^N \\left( x-\\mu\\right)^4 }{\\left(\\sum_{i=1}^N(x-\\mu)^2 \\right)^2 }$\n\n##### 2.3.6.1.2 Sample Kurtosis\n\nThe kurtosis of sample data is given by^[The sample excess kurtosis is given by $\\frac{n(n+1)(n-1)}{(n-2)(n-3)}\\frac{\\sum_{i=1}^n\\left(x_i-\\bar{x} \\right)^4}{s^4}-\\frac{3(n-1)^2}{(n-2)(n-3)}$\n\n$sample~kurtosis=\\frac{n(n+1)(n-1)}{(n-2)(n-3)}\\frac{\\sum_{i=1}^n\\left(x_i-\\bar{x} \\right)^4}{s^4}$ and that’s all we’ll say about that.\n\n## 2.4 R Commands\n\n### 2.4.1 mean\n\nmean()48\n\nexample:\n\nx<-c(1, 2, 2, 3, 3, 3, 4, 4, 4, 4, 5, 5, 5, 6, 6, 7)\nmean(x)\n## 4\n\n### 2.4.2 median\n\nmedian(x)\n## 4\n\n### 2.4.3 mode\n\nThere is no built-in R function to get the mode (there is a mode() function, but it means something different). But, we can install the package DescTools to get the mode we’re looking for.\n\ninstall.packages(DescTools)49\n\nlibrary(DescTools) Mode()\n\nMode(x) #Be sure to capitalize \"Mode\" so you get the correct Mode function\n## 4\n## attr(,\"freq\")\n## 4\n\n### 2.4.4 quantiles\n\nquantile(array, quantile)\n\nExample 1: 80th percentile of $$x$$\n\nquantile(x, 0.8)\n## 80%\n## 5\n\nExample 2: quartiles of $$x$$\n\nquantile(x, c(0.25, 0.5, 0.75))\n## 25% 50% 75%\n## 3 4 5\n\n### 2.4.5 range\n\nThe range() command returns the endpoints of the range.\n\nexample:\n\nrange(x)\n## 1 7\n\nto get the size of the range, you can use either range(x)-range(x) or max(x)-min(x)\n\nrange(x)-range(x)\n## 6\nmax(x)-min(x)\n## 6\n\n### 2.4.6 variance\n\nvar()\n\nexample:\n\nvar(x)\n## 2.666667\n\n### 2.4.7 standard deviation\n\nsd()\n\nexample:\n\nsd(x)\n## 1.632993\n\n### 2.4.8 Skewness and kurtosis\n\nSkewness and kurtosis are not part of the base R functions, so we will just need to install a package to calculate those (there are a couple packages that can do that, I just picked e1071).\n\ninstall.packages(e1071)50\n\nlibrary(e1071)\n\nskewness(x)\n\nskewness(x)\n## 0\nkurtosis(x)\n## -0.9609375\n\n## 2.5 Bonus Content\n\n1. Statistic: a number that summarizes information about a sample.↩︎\n\n2. Sample: a subset of a population↩︎\n\n3. Population: the entirety of things (including people, animals, etc.) of interest in a scientific investigation↩︎\n\n4. Parameter: a number that summarizes information about a population↩︎\n\n5. Most importantly, whether we use fixed effects or random effects models – this is covered in the page on ANOVA and and will be discussed at length in PSY 208.↩︎\n\n6. *there are probably exceptions, but I can’t really think of any right now↩︎\n\n7. The word data is the plural of the word datum and should take plural verb forms but often doesn’t. It’s a good habit to say things like “the data are” and “the data show” rather than things like “the data is” and “the data shows” in scientific communication. It’s a bad habit to correct people when they use data as a singular noun: try to let that stuff slide because we live in a society.↩︎\n\n8. Discrete: data with a limited set of values in a limited range.↩︎\n\n9. Nominal or categorical Data: Data that refer to category membership or to names.↩︎\n\n10. Data with relative values.↩︎\n\n11. Data that can take on infinite values in a limited range (i.e. data with values that are infinitely divisible).↩︎\n\n12. Interval data: Continuous data with meaningful mathematical differences between values.↩︎\n\n13. Ratio data: Continuous data with meaningful differences between values and meaningful relative magnitudes among values.↩︎\n\n14. _Cardinal (count) data:_Integers describing the number of occurrences of events↩︎\n\n15. *trenchant TV criticism↩︎\n\n16. _Proportion:_Part of a whole, expressed as a fraction or decimal↩︎\n\n17. For a proportion $$p$$ with $$n$$ observations, the variance is equal to $$\\frac{p(1-p)}{n}$$ and the standard deviation is equal to $$\\sqrt{\\frac{p(1-p)}{n}}.$$↩︎\n\n18. Binary (dichotomous) data: data that can take one of two values; those values are often assigned the values of either 0 or 1.↩︎\n\n19. Independent variable: A variable in an experimental or quasiexperimental design that is manipulated.↩︎\n\n20. Dependent variable: a variable in an experimental or quasiexperimental design that is measured↩︎\n\n21. Predictor variable: A variable associated with changes in an outcome. Predicted (outcome) variable: A variable associated with changes in a predicted variable↩︎\n\n22. Histogram: A chart of data indicating the frequency of observations of a variable↩︎\n\n23. Univariate: having to do with one variable.↩︎\n\n24. In case you’re interested: the two little bars at 1950 – 2000 points and at 2300 – 2350 points each represent single players: Damian Lillard (who scored 1,978 points) and James Harden (who scored 2,335 points). Congratulations, Dame and James!↩︎\n\n25. Central tendency: a summarization of the overall position of a distribution of data.↩︎\n\n26. Mean: generally understood in statistics to be the arithmetic mean of a distribution; the ratio of the sum of the values in a distribution to the number of values in that distribution.↩︎\n\n27. There are other means than the arithmetic mean, most famously the geometric mean $\\left( \\prod_{i=1}^nx_1 \\right)^{\\frac{1}{n}}$ and the harmonic mean $\\frac{n}{\\sum_{i=1}^n\\frac{1}{x_i}}.$ Both of those have important applications, but we won’t get to those in this course.↩︎\n\n28. Expected value: the average outcome of a probabilistic sample space↩︎\n\n29. Error: the difference between a prediction and an observed value, also known as residual and deviation↩︎\n\n30. Outlier: a datum that is substantially different from the data to which it belongs.↩︎\n\n31. Information loss is also a major theme of this page – it’s what the introduction was all about!↩︎\n\n32. Median: The value for which an equal number of data in a set are less than the value and greater than the value, also known as the 50th percentile.↩︎\n\n33. Let’s put income skew this way: if you put Jeff Bezos in a room with any 30 people, on average, everybody in that room would be making billions of dollars a year.↩︎\n\n34. Mode: The most frequently-occurring value or values in a distribution of data.↩︎\n\n35. Maximum Likelihood Estimate: the most probable value of observed data given a statistical model↩︎\n\n36. The use of means and similar mathematical transformations including the variance and standard deviation with interval data is a matter of some debate. To illustrate, let’s imagine that you are asked to evaluate the quality of your classes on a 1 – 5 integer scale (you won’t have to imagine for long – it happens at the end of every semester at this university). The argument in favor of using the mean is that if one class has an average rating of 4.2 and another class has an average rating of 3.4, then of course the first class is generally preferred to the second and the use of means is perfectly legitimate. The argument against using the mean is that there is no way of knowing if, say, a rating of 2 indicates precisely twice as much quality as a rating of 1 or if the difference between a 3 and a 4 is the same as the difference between a 4 and a 5, and that the use of means implies continuity that isn’t there. For the record: I’m in the latter camp, and I would say just use the median or the mode.↩︎\n\n37. Quantiles: values that divide the distributions into equal parts↩︎\n\n38. Range: The difference between the largest and smallest values in a distribution of data.↩︎\n\n39. Interquartile Range: The difference between the 75th percentile value and the 25th percentile value of a distribution of data; the range of the central 50% of values in a dataset.↩︎\n\n40. Variance: A measure of the spread of a dataset equal to the average of the squared deviations from the mean of the dataset.↩︎\n\n41. A statistic that is consistently wrong in the same direction is known as a biased estimator. The population variance equation is a biased estimator of sample variance.↩︎\n\n42. Degrees of freedom (df): the number of items in a set that are free to vary.↩︎\n\n43. Standard deviation: The typical deviation from the mean of the data set, equal to the square root of the variance.↩︎\n\n44. Skew (or skewness): The balance of a distribution about its center↩︎\n\n45. Tail(s): the area or areas of a distribution furthest from the peak.↩︎\n\n46. Kurtosis: The relative sizes of the tails of a symmetric distribution.↩︎\n\n47. Some prefer a kurtosis statistic that is equal to zero for a mesokurtic distribution and so sometimes you will see an excess kurtosis statistic that is recentered at 0↩︎\n\n48. 1. c() is the combine command, which tells R to combine everything inside the parentheses into one object (in this case, an array called $$x$$). 2. The is just an indicator that this is the first (and in this case, only) line of the results↩︎\n\n49. You only need to install a package once to your computer. After that, every time you start a new R session, you just have to call library(insert package name) to turn it on. The best analogy I have encountered to describe the process is from Nathaniel D. Phillips’s book YaRrr! The Pirate’s Guide to R: a package is like a lightbulb – install.packages() puts the lightbulb in the socket and then library() turns it on.↩︎\n\n50. You only need to install a package once to your computer. After that, every time you start a new R session, you just have to call library(insert package name) to turn it on. The best analogy I have encountered to describe the process is from Nathaniel D. Phillips’s book YaRrr! The Pirate’s Guide to R: a package is like a lightbulb – install.packages() puts the lightbulb in the socket and then library()` turns it on.↩︎" ]
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https://brilliant.org/discussions/thread/an-accidental-hint-at-eulers-equation/
[ "# An Accidental Hint at Euler's Equation\n\nI had this thought at lunch today. It's not a sophisticated treatment of the subject, but I found it amusing.\n\nWe know that when you differentiate a sinusoid twice, you get back a scaled and negated version of the original. Here the scaling factor is unity.\n\n$y = sin(t) \\\\ \\ddot{y} = -sin(t) = -y$\n\nWe also know that double-differentiating an exponential gets us back a scaled (but not negated) version of the original. Here again, the scaling factor is unity.\n\n$y = e^t \\\\ \\ddot{y} = e^t = y$\n\nThese two behaviors are tantalizingly similar. So how might we get the exponential to behave like the sinusoid with respect to double-differentiation? Maybe we could throw in the square root of negative one.\n\n$y = e^{j t} \\\\ \\ddot{y} = j^2 e^{j t} = -e^{j t} = -y$\n\nMaking the exponent complex makes the exponential behave like a sinusoid with respect to double-differentiation. Hence, we've stumbled onto something like Euler's equation (shown below for reference).\n\n$e^{j t } = cos \\, t + j \\, sin \\, t$", null, "Note by Steven Chase\n3 years, 1 month ago\n\nThis discussion board is a place to discuss our Daily Challenges and the math and science related to those challenges. Explanations are more than just a solution — they should explain the steps and thinking strategies that you used to obtain the solution. Comments should further the discussion of math and science.\n\nWhen posting on Brilliant:\n\n• Use the emojis to react to an explanation, whether you're congratulating a job well done , or just really confused .\n• Ask specific questions about the challenge or the steps in somebody's explanation. Well-posed questions can add a lot to the discussion, but posting \"I don't understand!\" doesn't help anyone.\n• Try to contribute something new to the discussion, whether it is an extension, generalization or other idea related to the challenge.\n\nMarkdownAppears as\n*italics* or _italics_ italics\n**bold** or __bold__ bold\n- bulleted- list\n• bulleted\n• list\n1. numbered2. list\n1. numbered\n2. list\nNote: you must add a full line of space before and after lists for them to show up correctly\nparagraph 1paragraph 2\n\nparagraph 1\n\nparagraph 2\n\n[example link](https://brilliant.org)example link\n> This is a quote\nThis is a quote\n # I indented these lines\n# 4 spaces, and now they show\n# up as a code block.\n\nprint \"hello world\"\n# I indented these lines\n# 4 spaces, and now they show\n# up as a code block.\n\nprint \"hello world\"\nMathAppears as\nRemember to wrap math in $$ ... $$ or $ ... $ to ensure proper formatting.\n2 \\times 3 $2 \\times 3$\n2^{34} $2^{34}$\na_{i-1} $a_{i-1}$\n\\frac{2}{3} $\\frac{2}{3}$\n\\sqrt{2} $\\sqrt{2}$\n\\sum_{i=1}^3 $\\sum_{i=1}^3$\n\\sin \\theta $\\sin \\theta$\n\\boxed{123} $\\boxed{123}$\n\nSort by:\n\nGood Lord. Thanks sir for posting these.\n\n- 3 years, 1 month ago\n\n- 3 years, 1 month ago\n\nVery interesting. Great work.\n\n- 2 years, 9 months ago\n\nThanks\n\n- 2 years, 9 months ago" ]
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https://fr.mathworks.com/matlabcentral/cody/problems/660-find-a-subset-that-divides-the-vector-into-equal-halves/solutions/1615561
[ "Cody\n\nProblem 660. Find a subset that divides the vector into equal halves\n\nSolution 1615561\n\nSubmitted on 24 Aug 2018 by jj L\nThis solution is locked. To view this solution, you need to provide a solution of the same size or smaller.\n\nTest Suite\n\nTest Status Code Input and Output\n1   Pass\nx = [1 2 3 4 5 6 7]; xi = split_it(x); assert(isequal(sum(x(xi)),sum(x)/2));\n\n2   Pass\nx = [2 2 2 2 2 2]; xi = split_it(x); assert(isequal(sum(x(xi)),sum(x)/2));\n\n3   Pass\nx = [2 5 4 5 4]; xi = split_it(x); assert(isequal(sum(x(xi)),sum(x)/2));\n\n4   Pass\nx = [1 3 1 1 9 7]; xi = split_it(x); assert(isequal(sum(x(xi)),sum(x)/2));\n\n5   Pass\nx = primes(100); xi = split_it(x); assert(isequal(sum(x(xi)),sum(x)/2));" ]
[ null ]
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https://www.gurufocus.com/term/turnover/NAS:ITCI/Asset-Turnover/Intra-Cellular%20Therapies
[ "Switch to:\n\n# Intra-Cellular Therapies Asset Turnover\n\n: 0.00 (As of Jun. 2020)\nView and export this data going back to 2013. Start your Free Trial\n\nAsset Turnover measures how quickly a company turns over its asset through sales. It is calculated as Revenue divided by Total Assets. Intra-Cellular Therapies's Revenue for the three months ended in Jun. 2020 was \\$1.91 Mil. Intra-Cellular Therapies's Total Assets for the quarter that ended in Jun. 2020 was \\$461.09 Mil. Therefore, Intra-Cellular Therapies's Asset Turnover for the quarter that ended in Jun. 2020 was 0.00.\n\nAsset Turnover is linked to ROE % through Du Pont Formula. Intra-Cellular Therapies's annualized ROE % for the quarter that ended in Jun. 2020 was -62.93%. It is also linked to ROA % through Du Pont Formula. Intra-Cellular Therapies's annualized ROA % for the quarter that ended in Jun. 2020 was -55.27%.\n\n## Intra-Cellular Therapies Asset Turnover Historical Data\n\n* All numbers are in millions except for per share data and ratio. All numbers are in their local exchange's currency.\n\n Intra-Cellular Therapies Annual Data Dec12 Mar13 Dec14 Dec15 Dec16 Dec17 Dec18 Dec19 Asset Turnover", null, "", null, "", null, "0.00 0.00 0.00 0.00 0.00\n\n## Intra-Cellular Therapies Asset Turnover Calculation\n\nAsset Turnover measures how quickly a company turns over its asset through sales.\n\nIntra-Cellular Therapies's Asset Turnover for the fiscal year that ended in Dec. 2019 is calculated as\n\n Asset Turnover = Revenue / Average Total Assets = Revenue (A: Dec. 2019 ) / ( (Total Assets (A: Dec. 2018 ) + Total Assets (A: Dec. 2019 )) / count ) = 0.061 / ( (357.206 + 251.186) / 2 ) = 0.061 / 304.196 = 0.00\n\nIntra-Cellular Therapies's Asset Turnover for the quarter that ended in Jun. 2020 is calculated as\n\n Asset Turnover = Revenue / Average Total Assets = Revenue (Q: Jun. 2020 ) / ( (Total Assets (Q: Mar. 2020 ) + Total Assets (Q: Jun. 2020 )) / count ) = 1.907 / ( (481.243 + 440.931) / 2 ) = 1.907 / 461.087 = 0.00\n\n* All numbers are in millions except for per share data and ratio. All numbers are in their local exchange's currency.\n\nCompanies with low profit margins tend to have high Asset Turnover, while those with high profit margins have low Asset Turnover. Companies in the retail industry tend to have a very high turnover ratio.\n\nIntra-Cellular Therapies  (NAS:ITCI) Asset Turnover Explanation\n\nAsset Turnover is linked to ROE % through Du Pont Formula.\n\nIntra-Cellular Therapies's annulized ROE % for the quarter that ended in Jun. 2020 is\n\n ROE %** (Q: Jun. 2020 ) = Net Income / Total Stockholders Equity = -254.848 / 404.989 = (Net Income / Revenue) * (Revenue / Total Assets) * (Total Assets / Total Stockholders Equity) = (-254.848 / 7.628) * (7.628 / 461.087) * (461.087/ 404.989) = Net Margin % * Asset Turnover * Equity Multiplier = -3340.95 % * 0.0165 * 1.1385 = ROA % * Equity Multiplier = -55.27 % * 1.1385 = -62.93 %\n\nNote: The Net Income data used here is four times the quarterly (Jun. 2020) net income data. The Revenue data used here is four times the quarterly (Jun. 2020) revenue data.\n\n* All numbers are in millions except for per share data and ratio. All numbers are in their local exchange's currency.\n\n** The ROE % used above is for Du Pont Analysis only. It is different from the defined ROE % page on our website, as here it uses Net Income instead of Net Income attributable to Common Stockholders in the calculation.\n\nIt is also linked to ROA % through Du Pont Formula:\n\nIntra-Cellular Therapies's annulized ROA % for the quarter that ended in Jun. 2020 is\n\n ROA % (Q: Jun. 2020 ) = Net Income / Total Assets = -254.848 / 461.087 = (Net Income / Revenue) * (Revenue / Total Assets) = (-254.848 / 7.628) * (7.628 / 461.087) = Net Margin % * Asset Turnover = -3340.95 % * 0.0165 = -55.27 %\n\nNote: The Net Income data used here is four times the quarterly (Jun. 2020) net income data. The Revenue data used here is four times the quarterly (Jun. 2020) revenue data.\n\n* All numbers are in millions except for per share data and ratio. All numbers are in their local exchange's currency.\n\nBe Aware\n\nIn the article Joining The Dark Side: Pirates, Spies and Short Sellers, James Montier reported that In their US sample covering the period 1968-2003, Cooper et al find that firms with low asset growth outperformed firms with high asset growth by an astounding 20% p.a. equally weighted. Even when controlling for market, size and style, low asset growth firms outperformed high asset growth firms by 13% p.a. Therefore a company with fast asset growth may underperform.\n\nTherefore, it is a good sign if a company's Asset Turnover is consistent or even increases. If a company's asset grows faster than sales, its Asset Turnover will decline, which can be a warning sign." ]
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https://www.got-it.ai/solutions/excel-chat/excel-help/how-to/crossed/crossed-out-letters
[ "", null, "# Get instant live expert help on How do I crossed out letters", null, "“My Excelchat expert helped me in less than 20 minutes, saving me what would have been 5 hours of work!”\n\n## Post your problem and you’ll get expert help in seconds.\n\nOur professional experts are available now. Your privacy is guaranteed.\n\n## Here are some problems that our users have asked and received explanations on\n\nCan't figure out if I need to be using Countifs formula and counta formula or one or the other to count cells with numbers and letters\nSolved by F. E. in 29 mins\nI have a row of letters and numbers i need to remove the letters and add them to another column. Example BSN17525\nSolved by V. Q. in 28 mins\nHello, I need check the format of a cell I need it to return the following logic: IF the first two letters in column E = GB AND has 9 numbers are the two letters then that should return correct. OR IF the first two letters in column E = FR AND has 11 numbers are the two letters then that should return correct. OR IF the first two letters in column E = DE AND has 9 numbers are the two letters then that should return correct. SO the the logic is IF left and len is number.\nSolved by T. J. in 30 mins\nHi there, i would like to create a column with initial letters in capital letters and seperated by . (Dot)\nSolved by Z. F. in 24 mins\ni want to get rid of letters from a combination of numbers and letters and but values with a specific letter i want to be negative and the rest positive\nSolved by B. J. in 22 mins" ]
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https://www.cpalms.org/PreviewCourse/Preview/1763
[ "# Access Informal Geometry   (#7912060)", null, "Export Print", null, "Create CMAP\n\n## General Course Information and Notes\n\n### General Notes\n\nAccess Courses: Access courses are intended only for students with a significant cognitive disability. Access courses are designed to provide students with access to the general curriculum. Access points reflect increasing levels of complexity and depth of knowledge aligned with grade-level expectations. The access points included in access courses are intentionally designed to foster high expectations for students with significant cognitive disabilities.\n\nAccess points in the subject areas of science, social studies, art, dance, physical education, theatre, and health provide tiered access to the general curriculum through three levels of access points (Participatory, Supported, and Independent). Access points in English language arts and mathematics do not contain these tiers, but contain Essential Understandings (or EUs). EUs consist of skills at varying levels of complexity and are a resource when planning for instruction.\n\n### General Information\n\nCourse Number: 7912060\nCourse Path:\nAbbreviated Title: ACCESS INF GEOMETRY\nNumber of Credits: Course may be taken for up to two credits\nCourse Length: Year (Y)\nCourse Attributes:\n• Class Size Core Required\nCourse Status: Terminated\n\n## Educator Certifications\n\nOne of these educator certification options is required to teach this course.\n\n## Student Resources\n\nVetted resources students can use to learn the concepts and skills in this course.\n\n## Original Student Tutorials\n\nHighs and Lows Part 2: Completing the Square:\n\nLearn the process of completing the square of a quadratic function to find the maximum or minimum to discover how high a dolphin jumped in this interactive tutorial.\n\nThis is part 2 of a 2 part series. Click HERE to open part 1.\n\nType: Original Student Tutorial\n\nHighs and Lows Part 1: Completing the Square:\n\nLearn the process of completing the square of a quadratic function to find the maximum or minimum to discover how high a dolphin jumped in this interactive tutorial.\n\nThis is part 1 of a 2 part series. Click HERE to open Part 2.\n\nType: Original Student Tutorial\n\nMovies Part 2: What’s the Spread?:\n\nFollow Jake along as he relates box plots with other plots and identifies possible outliers in real-world data from surveys of moviegoers' ages in part 2 in this interactive tutorial.\n\nThis is part 2 of 2-part series, click HERE to view part 1.\n\nType: Original Student Tutorial\n\nMovies Part 1: What's the Spread?:\n\nFollow Jake as he displays real-world data by creating box plots showing the 5 number summary and compares the spread of the data from surveys of the ages of moviegoers in part 1 of this interactive tutorial.\n\nThis is part 1 of 2-part series, click HERE to view part 2.\n\nType: Original Student Tutorial\n\nExponential Functions Part 2: Growth:\n\nLearn about exponential growth in the context of interest earned as money is put in a savings account by examining equations, graphs, and tables in this interactive tutorial.\n\nType: Original Student Tutorial\n\nSolving Rational Equations: Cross Multiplying:\n\nLearn how to solve rational linear and quadratic equations using cross multiplication in this interactive tutorial.\n\nType: Original Student Tutorial\n\nSolving Inequalities and Graphing Solutions Part 2:\n\nLearn how to solve and graph compound inequalities and determine if solutions are viable in part 2 of this interactive tutorial series.\n\nType: Original Student Tutorial\n\nSolving Inequalities and Graphing Solutions: Part 1:\n\nLearn how to solve and graph one variable inequalities, including compound inequalities, in part 1 of this interactive tutorial series.\n\nType: Original Student Tutorial\n\nThe Year-Round School Debate: Identifying Faulty Reasoning – Part Two:\n\nThis is Part Two of a two-part series. Learn to identify faulty reasoning in this interactive tutorial series. You'll learn what some experts say about year-round schools, what research has been conducted about their effectiveness, and how arguments can be made for and against year-round education. Then, you'll read a speech in favor of year-round schools and identify faulty reasoning within the argument, specifically the use of hasty generalizations.\n\nMake sure to complete Part One before Part Two! Click HERE to launch Part One.\n\nType: Original Student Tutorial\n\nThe Year-Round School Debate: Identifying Faulty Reasoning – Part One:\n\nLearn to identify faulty reasoning in this two-part interactive English Language Arts tutorial. You'll learn what some experts say about year-round schools, what research has been conducted about their effectiveness, and how arguments can be made for and against year-round education. Then, you'll read a speech in favor of year-round schools and identify faulty reasoning within the argument, specifically the use of hasty generalizations.\n\nMake sure to complete both parts of this series! Click HERE to open Part Two.\n\nType: Original Student Tutorial\n\nEvaluating an Argument – Part Four: JFK’s Inaugural Address:\n\nExamine President John F. Kennedy's inaugural address in this interactive tutorial. You will examine Kennedy's argument, main claim, smaller claims, reasons, and evidence.\n\nIn Part Four, you'll use what you've learned throughout this series to evaluate Kennedy's overall argument.\n\nMake sure to complete the previous parts of this series before beginning Part 4.\n\n• Click HERE to launch Part Two.\n• Click HERE to launch Part Three.\n\nType: Original Student Tutorial\n\nEvaluating an Argument – Part Three: JFK’s Inaugural Address:\n\nExamine President John F. Kennedy's inaugural address in this interactive tutorial. You will examine Kennedy's argument, main claim, smaller claims, reasons, and evidence. By the end of this four-part series, you should be able to evaluate his overall argument.\n\nIn Part Three, you will read more of Kennedy's speech and identify a smaller claim in this section of his speech. You will also evaluate this smaller claim's relevancy to the main claim and evaluate Kennedy's reasons and evidence.\n\nMake sure to complete all four parts of this series!\n\n• Click HERE to launch Part Two.\n\nType: Original Student Tutorial\n\nHigh Tech Seesaw:\n\nLearn how to find the point on a directed line segment that partitions it into a given ratio in this interactive tutorial.\n\nType: Original Student Tutorial\n\nFinding the Zeros of Quadratic Functions:\n\nLearn to find the zeros of a quadratic function and interpret their meaning in real-world contexts with this interactive tutorial.\n\nType: Original Student Tutorial\n\nReady for Takeoff! -- Part Two:\n\nThis is Part Two of a two-part tutorial series. In this interactive tutorial, you'll practice identifying a speaker's purpose using a speech by aviation pioneer Amelia Earhart. You will examine her use of rhetorical appeals, including ethos, logos, pathos, and kairos. Finally, you'll evaluate the effectiveness of Earhart's use of rhetorical appeals.\n\nBe sure to complete Part One first. Click here to launch PART ONE.\n\nType: Original Student Tutorial\n\nReady for Takeoff! -- Part One:\n\nThis is Part One of a two-part tutorial series. In this interactive tutorial, you'll practice identifying a speaker's purpose using a speech by aviation pioneer Amelia Earhart. You will examine her use of rhetorical appeals, including ethos, logos, pathos, and kairos. Finally, you'll evaluate the effectiveness of Earhart's use of rhetorical appeals.\n\nType: Original Student Tutorial\n\nExpository Writing: Eyes in the Sky (Part 4 of 4):\n\nPractice writing different aspects of an expository essay about scientists using drones to research glaciers in Peru. This interactive tutorial is part four of a four-part series. In this final tutorial, you will learn about the elements of a body paragraph. You will also create a body paragraph with supporting evidence. Finally, you will learn about the elements of a conclusion and practice creating a “gift.”\n\nThis tutorial is part four of a four-part series. Click below to open the other tutorials in this series.\n\nType: Original Student Tutorial\n\nExpository Writing: Eyes in the Sky (Part 3 of 4):\n\nLearn how to write an introduction for an expository essay in this interactive tutorial. This tutorial is the third part of a four-part series. In previous tutorials in this series, students analyzed an informational text and video about scientists using drones to explore glaciers in Peru. Students also determined the central idea and important details of the text and wrote an effective summary. In part three, you'll learn how to write an introduction for an expository essay about the scientists' research.\n\nThis tutorial is part three of a four-part series. Click below to open the other tutorials in this series.\n\nType: Original Student Tutorial\n\nFinding the Maximum or Minimum of a Quadratic Function:\n\nLearn to complete the square of a quadratic expression and identify the maximum or minimum value of the quadratic function it defines. In this interactive tutorial, you'll also interpret the meaning of the maximum and minimum of a quadratic function in a real world context.\n\nType: Original Student Tutorial\n\nLearn to rewrite products involving radicals and rational exponents using properties of exponents in this interactive tutorial.\n\nType: Original Student Tutorial\n\nNinja Nancy Slices:\n\nLearn how to determine the shape of a cross-section created by the intersection of a slicing plane with a pyramid or prism in this ninja-themed, interactive tutorial.\n\nType: Original Student Tutorial\n\nI Scream! You Scream! We All Scream for... Volume!:\n\nLearn to calculate the volume of a cone as you solve real-world problems in this ice cream-themed, interactive tutorial.\n\nType: Original Student Tutorial\n\nCancer: Mutated Cells Gone Wild!:\n\nExplore the relationship between mutations, the cell cycle, and uncontrolled cell growth which may result in cancer with this interactive tutorial.\n\nType: Original Student Tutorial\n\nWriting Inequalities with Money, Money, Money:\n\nWrite linear inequalities for different money situations in this interactive tutorial.\n\nType: Original Student Tutorial\n\n## Educational Software / Tool\n\nTransformations Using Technology:\n\nThis virtual manipulative can be used to demonstrate and explore the effect of translation, rotation, and/or reflection on a variety of plane figures. A series of transformations can be explored to result in a specified final image.\n\nType: Educational Software / Tool\n\n## Perspectives Video: Experts\n\nMathematically Exploring the Wakulla Caves:\n\nThe tide is high!  How can we statistically prove there is a relationship between the tides on the Gulf Coast and in a fresh water spring 20 miles from each other?\n\nType: Perspectives Video: Expert\n\nMicroGravity Sensors & Statistics:\n\nStatistical analysis played an essential role in using microgravity sensors to determine location of caves in Wakulla County.\n\nType: Perspectives Video: Expert\n\n## Perspectives Video: Professional/Enthusiasts\n\nUnit Conversions:\n\nType: Perspectives Video: Professional/Enthusiast\n\nMaking Candy: Uniform Scaling:\n\nDon't be a shrinking violet. Learn how uniform scaling is important for candy production.\n\nType: Perspectives Video: Professional/Enthusiast\n\nUsing Geometry and Computers to make Art with CNC Machining:\n\nSee and see far into the future of arts and manufacturing as a technician explains computer numerically controlled (CNC) machining bit by bit.\n\nType: Perspectives Video: Professional/Enthusiast\n\nEstimating Oil Seep Production by Bubble Volume:\n\nYou'll need to bring your computer skills and math knowledge to estimate oil volume and rate as it seeps from the ocean floor. Dive in!\n\nType: Perspectives Video: Professional/Enthusiast\n\nSpeed Trap:\n\nThe purpose of this task is to allow students to demonstrate an ability to construct boxplots and to use boxplots as the basis for comparing distributions.\n\nSAT Scores:\n\nThis problem solving task challenges students to answer probability questions about SAT scores, using distribution and mean to solve the problem.\n\nHaircut Costs:\n\nThis problem could be used as an introductory lesson to introduce group comparisons and to engage students in a question they may find amusing and interesting.\n\nShould We Send Out a Certificate?:\n\nThe purpose of this task is to have students complete normal distribution calculations and to use properties of normal distributions to draw conclusions.\n\nDo You Fit in This Car?:\n\nThis task requires students to use the normal distribution as a model for a data distribution. Students must use given means and standard deviations to approximate population percentages.\n\nRandom Walk III:\n\nThe task provides a context to calculate discrete probabilities and represent them on a bar graph.\n\nBank Shot:\n\nThis task asks students to use similarity to solve a problem in a context that will be familiar to many, though most students are accustomed to using intuition rather than geometric reasoning to set up the shot.\n\nAre They Similar?:\n\nIn this problem, students are given a picture of two triangles that appear to be similar, but whose similarity cannot be proven without further information. Asking students to provide a sequence of similarity transformations that maps one triangle to the other, using the definition of similarity in terms of similarity transformations.\n\nExstensions, Bisections and Dissections in a Rectangle:\n\nThis task involves a reasonably direct application of similar triangles, coupled with a moderately challenging procedure of constructing a diagram from a verbal description.\n\nToilet Roll:\n\nThe purpose of this task is to engage students in geometric modeling, and in particular to deduce algebraic relationships between variables stemming from geometric constraints.\n\nAlgae Blooms:\n\nIn this example, students are asked to write a function describing the population growth of algae. It is implied that this is exponential growth.\n\nCoins in a circular pattern:\n\nUsing a chart of diameters of different denominations of coins, students are asked to figure out how many coins fit around a central coin.\n\nThe Lighthouse Problem:\n\nThis problem asks students to model phenomena on the surface of the earth by examining the visibility of the lamp in a lighthouse from a boat.\n\nSolar Eclipse:\n\nThis problem solving task encourages students to explore why solar eclipses are rare by examining the radius of the sun and the furthest distance between the moon and the earth.\n\nA Midpoint Miracle:\n\nThis problem solving task gives students the opportunity to prove a fact about quadrilaterals: that if we join the midpoints of an arbitrary quadrilateral to form a new quadrilateral, then the new quadrilateral is a parallelogram, even if the original quadrilateral was not.\n\nSeven Circles III:\n\nThis provides an opportunity to model a concrete situation with mathematics. Once a representative picture of the situation described in the problem is drawn (the teacher may provide guidance here as necessary), the solution of the task requires an understanding of the definition of the sine function.\n\nDilating a Line:\n\nThis task asks students to make deductions about a line after it has been dilated by a factor of 2.\n\nRunning around a track II:\n\nThe goal of this task is to model a familiar object, an Olympic track, using geometric shapes. Calculations of perimeters of these shapes explain the staggered start of runners in a 400 meter race.\n\nRunning around a track I:\n\nIn this problem, geometry is applied to a 400 meter track to find the perimeter of the track.\n\nPaper Clip:\n\nIn this task, a typographic grid system serves as the background for a standard paper clip. A metric measurement scale is drawn across the bottom of the grid and the paper clip extends in both directions slightly beyond the grid. Students are given the approximate length of the paper clip and determine the number of like paper clips made from a given length of wire.\n\nIce Cream Cone:\n\nIn this task, students will provide a sketch of a paper ice cream cone wrapper, use the sketch to develop a formula for the surface area of the wrapper, and estimate the maximum number of wrappers that could be cut from a rectangular piece of paper.\n\nHow thick is a soda can? (Variation II):\n\nThis problem solving task asks students to explain which measurements are needed to estimate the thickness of a soda can.\n\nHow thick is a soda can? (Variation I):\n\nThis problem solving task challenges students to find the surface area of a soda can, calculate how many cubic centimeters of aluminum it contains, and estimate how thick it is.\n\nHow many leaves on a tree? (Version 2):\n\nThis is a mathematical modeling task aimed at making a reasonable estimate for something which is too large to count accurately, the number of leaves on a tree.\n\nHow many leaves on a tree?:\n\nThis is a mathematical modeling task aimed at making a reasonable estimate for something which is too large to count accurately, the number of leaves on a tree.\n\nHow many cells are in the human body?:\n\nThis problem solving task challenges students to apply the concepts of mass, volume, and density in the real-world context to find how many cells are in the human body.\n\nHexagonal pattern of beehives:\n\nThe goal of this task is to use geometry to study the structure of beehives.\n\nGlobal Positioning System II:\n\nReflective of the modernness of the technology involved, this is a challenging geometric modeling task in which students discover from scratch the geometric principles underlying the software used by GPS systems.\n\nEratosthenes and the circumference of the earth:\n\nThis problem solving task gives an interesting context for implementing ideas from geometry and trigonometry.\n\nArchimedes and the King's Crown:\n\nThis problem solving task uses the tale of Archimedes and the King of Syracuse's crown to determine the volume and mass of gold and silver.\n\nUnit Squares and Triangles:\n\nThis problem solving task asks students to find the area of a triangle by using unit squares and line segments.\n\nDoctor's Appointment:\n\nThe purpose of the task is to analyze a plausible real-life scenario using a geometric model. The task requires knowledge of volume formulas for cylinders and cones, some geometric reasoning involving similar triangles, and pays attention to reasonable approximations and maintaining reasonable levels of accuracy throughout.\n\nWhy Does ASA Work?:\n\nThis problem solving task ask students to show the reflection of one triangle maps to another triangle.\n\nWhen Does SSA Work to Determine Triangle Congruence?:\n\nIn this problem, we considered SSA. The triangle congruence criteria, SSS, SAS, ASA, all require three pieces of information. It is interesting, however, that not all three pieces of information about sides and angles are sufficient to determine a triangle up to congruence.\n\nSeven Circles II:\n\nThis task provides a concrete geometric setting in which to study rigid transformations of the plane.\n\nWhy Does SAS Work?:\n\nThis problem solving task challenges students to explain the reason why the given triangles are congruent, and to construct reflections of the points.\n\nReflections and Isosceles Triangles:\n\nThis activity uses rigid transformations of the plane to explore symmetries of classes of triangles.\n\nReflections and Equilateral Triangles II:\n\nThis task gives students a chance to see the impact of reflections on an explicit object and to see that the reflections do not always commute.\n\nReflections and Equilateral Triangles:\n\nThis activity is one in a series of tasks using rigid transformations of the plane to explore symmetries of classes of triangles, with this task in particular focusing on the class of equilaterial triangles\n\nCenterpiece:\n\nThe purpose of this task is to use geometric and algebraic reasoning to model a real-life scenario. In particular, students are in several places (implicitly or explicitly) to reason as to when making approximations is reasonable and when to round, when to use equalities vs. inequalities, and the choice of units to work with (e.g., mm vs. cm).\n\nUse Cavalieri’s Principle to Compare Aquarium Volumes:\n\nThis task presents a context that leads students toward discovery of the formula for calculating the volume of a sphere.\n\nTennis Balls in a Can:\n\nThis task is inspired by the derivation of the volume formula for the sphere. If a sphere of radius 1 is enclosed in a cylinder of radius 1 and height 2, then the volume not occupied by the sphere is equal to the volume of a \"double-naped cone\" with vertex at the center of the sphere and bases equal to the bases of the cylinder\n\nTwo Wheels and a Belt:\n\nThis task combines two skills: making use of the relationship between a tangent segment to a circle and the radius touching that tangent segment, and computing lengths of circular arcs given the radii and central angles.\n\nRight triangles inscribed in circles II:\n\nRight triangles inscribed in circles I:\n\nThis task provides a good opportunity to use isosceles triangles and their properties to show an interesting and important result about triangles inscribed in a circle: the fact that these triangles are always right triangles is often referred to as Thales' theorem.\n\nWhy does SSS work?:\n\nThis particular problem solving task exhibits congruency between two triangles, demonstrating translation, reflection and rotation.\n\nBuilding a tile pattern by reflecting octagons:\n\nThis task applies reflections to a regular octagon to construct a pattern of four octagons enclosing a quadrilateral: the focus of the task is on using the properties of reflections to deduce that the quadrilateral is actually a square.\n\nBuilding a tile pattern by reflecting hexagons:\n\nThis task applies reflections to a regular hexagon to construct a pattern of six hexagons enclosing a seventh: the focus of the task is on using the properties of reflections to deduce this seven hexagon pattern.\n\nAre the Triangles Congruent?:\n\nThe purpose of this task is primarily assessment-oriented, asking students to demonstrate knowledge of how to determine the congruency of triangles.\n\nTangent Lines and the Radius of a Circle:\n\nThis problem solving task challenges students to find the perpendicular meeting point of a segment from the center of a circle and a tangent.\n\nNeglecting the Curvature of the Earth:\n\nThis task applies geometric concepts, namely properties of tangents to circles and of right triangles, in a modeling situation. The key geometric point in this task is to recognize that the line of sight from the mountain top towards the horizon is tangent to the earth. We can then use a right triangle where one leg is tangent to a circle and the other leg is the radius of the circle to investigate this situation.\n\nWhat functions do two graph points determine?:\n\nThis problem solving task challenges students to find the linear, exponential and quadratic functions based on two points.\n\nUS Population 1982-1988:\n\nThis problem solving task asks students to predict and model US population based on a chart of US population data from 1982 to 1988.\n\nUS Population 1790-1860:\n\nThis problem solving task asks students to solve five exponential and linear function problems based on a US population chart for the years 1790-1860.\n\nRising Gas Prices - Compounding and Inflation:\n\nThe purpose of this task is to give students an opportunity to explore various aspects of exponential models (e.g., distinguishing between constant absolute growth and constant relative growth, solving equations using logarithms, applying compound interest formulas) in the context of a real world problem with ties to developing financial literacy skills. In particular, students are introduced to the idea of inflation of prices of a single commodity, and are given a very brief introduction to the notion of the Consumer Price Index for measuring inflation of a body of goods.\n\nLinear or exponential?:\n\nThis task gives a variation of real-life contexts which could be modeled by a linear or exponential function. The key distinguishing feature between the two is whether the change by equal factors over equal intervals (exponential functions), or by a constant increase per unit interval (linear functions). The task could either be used as an assessment problem on this distinction, or used as an introduction to the differences between these very important classes of functions.\n\nLinear Functions:\n\nThis task requires students to use the fact that on the graph of the linear function h(x) = ax + b, the y-coordinate increases by a when x increases by one. Specific values for a and b were left out intentionally to encourage students to use the above fact as opposed to computing the point of intersection, (p,q), and then computing respective function values to answer the question.\n\nComparing Exponentials:\n\nThis task gives students an opportunity to work with exponential functions in a real world context involving continuously compounded interest. They will study how the base of the exponential function impacts its growth rate and use logarithms to solve exponential equations.\n\nCarbon 14 Dating, Variation 2:\n\nThis exploratory task requires the student to use properties of exponential functions in order to estimate how much Carbon 14 remains in a preserved plant after different amounts of time.\n\nThis task involves a fairly straightforward decaying exponential. Filling out the table and developing the general formula is complicated only by the need to work with a fraction that requires decisions about rounding and precision.\n\nCash Box:\n\nThe given solutions for this task involve the creation and solving of a system of two equations and two unknowns, with the caveat that the context of the problem implies that we are interested only in non-negative integer solutions. Indeed, in the first solution, we must also restrict our attention to the case that one of the variables is further even. This aspect of the task is illustrative of mathematical practice standard MP4 (Model with mathematics), and crucial as the system has an integer solution for both situations, that is, whether or not we include the dollar on the floor in the cash box or not.\n\nExponential Functions:\n\nThis task requires students to use the fact that the value of an exponential function f(x) = a · b^x increases by a multiplicative factor of b when x increases by one. It intentionally omits specific values for c and d in order to encourage students to use this fact instead of computing the point of intersection, (p,q), and then computing function values to answer the question.\n\nEqual Factors over Equal Intervals:\n\nThis problem assumes that students are familiar with the notation x0 and ?x. However, the language \"successive quotient\" may be new.\n\nEqual Differences over Equal Intervals 2:\n\nThis task assumes that students are familiar with the ?x and ?y notations. Students most likely developed this familiarity in their work with slope.\n\nEqual Differences over Equal Intervals 1:\n\nAn important property of linear functions is that they grow by equal differences over equal intervals. In F.LE Equal Differences over Equal Intervals 1, students prove this for equal intervals of length one unit, and note that in this case the equal differences have the same value as the slope.\n\nIn the Billions and Linear Modeling:\n\nThis problem-solving task asks students to examine if linear modeling would be appropriate to describe and predict population growth from select years.\n\nIn the Billions and Exponential Modeling:\n\nThis problem-solving task provides students an opportunity to experiment with modeling real data by using population growth rates from the past two centuries.\n\nInteresting Interest Rates:\n\nThis problem-solving task challenges students to write expressions and create a table to calculate how much money can be gained after investing at different banks with different interest rates.\n\nIllegal Fish:\n\nThis problem-solving task asks students to describe exponential growth through a real-world problem involving the illegal introduction of fish into a lake.\n\nIdentifying Functions:\n\nThis problem-solving emphasizes the expectation that students know linear functions grow by constant differences over equal intervals and exponential functions grow by constant factors over equal intervals.\n\nWeed Killer:\n\nThe principal purpose of the task is to explore a real-world application problem with algebra, working with units and maintaining reasonable levels of accuracy throughout. Students are asked to determine which product will be the most economical to meet the requirements given in the problem.\n\nRegular Tessellations of the Plane:\n\nThis task examines the ways in which the plane can be covered by regular polygons in a very strict arrangement called a regular tessellation. These tessellations are studied here using algebra, which enters the picture via the formula for the measure of the interior angles of a regular polygon (which should therefore be introduced or reviewed before beginning the task). The goal of the task is to use algebra in order to understand which tessellations of the plane with regular polygons are possible.\n\nChecking a Calculation of a Decimal Exponent:\n\nIn this example, students use properties of rational exponents and other algebraic concepts to compare and verify the relative size of two real numbers that involve decimal exponents.\n\nFuel Efficiency:\n\nThe problem requires students to not only convert miles to kilometers and gallons to liters but they also have to deal with the added complication of finding the reciprocal at some point.\n\nHow Much Is a Penny Worth?:\n\nThis task asks students to calculate the cost of materials to make a penny, utilizing rates of grams of copper.\n\nForms of Exponential Expressions:\n\nThere are many different ways to write exponential expressions that describe the same quantity, in this task the amount of a radioactive substance after t years. Depending on what aspect of the context we need to investigate, one expression of the quantity may be more useful than another. This task contrasts the usefulness of four equivalent expressions. Students first have to confirm that the given expressions for the radioactive substance are equivalent. Then they have to explain the significance of each expression in the context of the situation.\n\nRunner's World:\n\nStudents are asked to use units to determine if the given statement is valid.\n\nHarvesting the Fields:\n\nThis is a challenging task, suitable for extended work, and reaching into a deep understanding of units. Students are given a scenario and asked to determine the number of people required to complete the amount of work in the time described. The task requires students to exhibit , Make sense of problems and persevere in solving them. An algebraic solution is possible but complicated; a numerical solution is both simpler and more sophisticated, requiring skilled use of units and quantitative reasoning. Thus the task aligns with either MAFS.912.A-CED.1.1 or MAFS.912.N-Q.1.1, depending on the approach.\n\nThrowing a Ball:\n\nStudents manipulate a given equation to find specified information.\n\nPaying the Rent:\n\nStudents solve problems tracking the balance of a checking account used only to pay rent. This simple conceptual task focuses on what it means for a number to be a solution to an equation, rather than on the process of solving equations.\n\nStudents extrapolate the list price of a car given a total amount paid in states with different tax rates. The emphasis in this task is not on complex solution procedures. Rather, the progression of equations, from two that involve different values of the sales tax, to one that involves the sales tax as a parameter, is designed to foster the habit of looking for regularity in solution procedures, so that students don't approach every equation as a new problem but learn to notice familiar types.\n\nPlanes and Wheat:\n\nIn this resource, students refer to given information which defines 5 variables in the context of real world government expenses. They are then asked to write equations based upon specific known values for some of the variables. The emphasis is on setting up, rather than solving, the equations.\n\nIn this resource, a method of deriving the quadratic formula from a theoretical standpoint is demonstrated. This task is for instructional purposes only and builds on \"Building an explicit quadratic function.\"\n\nProfit of a Company:\n\nThis task compares the usefulness of different forms of a quadratic expression. Students have to choose which form most easily provides information about the maximum value, the zeros and the vertical intercept of a quadratic expression in the context of a real world situation. Rather than just manipulating one form into the other, students can make sense out of the structure of the expressions.\n\n(From Algebra: Form and Function, McCallum et al., Wiley 2010)\n\nIncreasing or Decreasing? Variation 2:\n\nThe purpose of this task is to help students see manipulation of expressions as an activity undertaken for a purpose.\n\nVariation 1 of this task presents a related more complex expression already in the correct form to answer the question.\n\nThe expression arises in physics as the reciprocal of the combined resistance of two resistors in parallel. However, the context is not explicitly considered here.\n\nIce Cream:\n\nThis task illustrates the process of rearranging the terms of an expression to reveal different aspects about the quantity it represents, precisely the language being used in standard MAFS.912.A-SSE.2.3. Students are provided with an expression giving the temperature of a container at a time t, and have to use simple inequalities (e.g., that 2t>0 for all t) to reduce the complexity of an expression to a form where bounds on the temperature of a container of ice cream are made apparent.\n\nStudents compare graphs of different quadratic functions, then produce equations of their own to satisfy given conditions.\n\nThis exploration can be done in class near the beginning of a unit on graphing parabolas. Students need to be familiar with intercepts, and need to know what the vertex is. It is effective after students have graphed parabolas in vertex form (y=a(x–h)2+k), but have not yet explored graphing other forms.\n\nTraffic Jam:\n\nThis resource poses the question, \"how many vehicles might be involved in a traffic jam 12 miles long?\"\n\nThis task, while involving relatively simple arithmetic, promps students to practice modeling (MP4), work with units and conversion (N-Q.1), and develop a new unit (N-Q.2). Students will also consider the appropriate level of accuracy to use in their conclusions (N-Q.3).\n\nSeeing Dots:\n\nThe purpose of this task is to identify the structure in the two algebraic expressions by interpreting them in terms of a geometric context. Students will have likely seen this type of process before, so the principal source of challenge in this task is to encourage a multitude and variety of approaches, both in terms of the geometric argument and in terms of the algebraic manipulation.\n\nSelling Fuel Oil at a Loss:\n\nThe task is a modeling problem which ties in to financial decisions faced routinely by businesses, namely the balance between maintaining inventory and raising short-term capital for investment or re-investment in developing the business.\n\nFelicia's Drive:\n\nThis task provides students the opportunity to make use of units to find the gas needed (). It also requires them to make some sensible approximations (e.g., 2.92 gallons is not a good answer to part (a)) and to recognize that Felicia's situation requires her to round up. Various answers to (a) are possible, depending on how much students think is a safe amount for Felicia to have left in the tank when she arrives at the gas station. The key point is for them to explain their choices. This task provides an opportunity for students to practice MAFS.K12.MP.2.1: Reason abstractly and quantitatively, and MAFS.K12.MP.3.1: Construct viable arguments and critique the reasoning of others.\n\n## Tutorials\n\nFinding congruent triangles:\n\nIn this tutorial, students will use the SSS, ASA, SAS, and AAS postulates to find congruent triangles\n\nType: Tutorial\n\nDilation and scale factor:\n\nIn this tutorial, students will use a scale factor to dilate one line onto another.\n\nType: Tutorial\n\nUsing SSS in a proof:\n\nThis tutorial discusses the difference between a theorem and axiom. It also shows how to use SSS in a proof.\n\nType: Tutorial\n\nTriangle congruence postulates:\n\nThis tutorial discusses SSS, SAS, ASA and AAS postulates for congruent triangles. It also shows AAA is only good for similarity and SSA is good for neither.\n\nType: Tutorial\n\nCongruent Triangles and SSS:\n\nIn this video, students will learn about congruent triangles and the \"Side-Side-Side\" postulate.\n\nType: Tutorial\n\nRotating polygons 180 degrees about their center:\n\nStudents will investigate symmetry by rotating polygons 180 degrees about their center.\n\nType: Tutorial\n\nLine of reflection:\n\nStudents are shown, with an interactive tool, how to reflect a line segment. Students should have an understanding of slope and midpoint before viewing this video.\n\nType: Tutorial\n\nLine of reflection:\n\nThis tutorial uses the midpoint of two lines to find the line of reflection.\n\nType: Tutorial\n\nPoints after rotation:\n\nStudents will see what happens when a figure is rotated about the origin -270 degrees. Having a foundation about right triangles is recommended before viewing this video.\n\nType: Tutorial\n\nSpecifying planes in three dimensions:\n\nIn this tutorial, students are introduced to the concept that three non-collinear points are necessary to define a unique plane.\n\nType: Tutorial\n\nThe language of geometry:\n\nBefore learning any new concept it's important students learn and use common language and label concepts consistently. This tutorial introduces students to th point, line and plane.\n\nType: Tutorial\n\nIdentifying parallel and perpendicular lines:\n\nThis tutorial is great practice for help in identifying parallel and perpendicular lines.\n\nType: Tutorial\n\nBasic Geometry Language and Labels:\n\nIn this tutorial we will learn the basics of geometry, such as identifying a line, ray, point, and segment.\n\nType: Tutorial\n\nHow to evaluate an expression with variables:\n\nLearn how to evaluate an expression with variables using a technique called substitution (or \"plugging in\").\n\nType: Tutorial\n\nWhat is a variable?:\n\nOur focus here is understanding that a variable is just a letter or symbol (usually a lower case letter) that can represent different values in an expression. We got this. Just watch.\n\nType: Tutorial\n\nPower of a Power Property:\n\nThis tutorial demonstrates how to use the power of a power property with both numerals and variables.\n\nType: Tutorial\n\nCalculating Mixtures of Solutions:\n\nThis lecture shows how algebra is used to solve problems involving mixtures of solutions of different concentrations.\n\nType: Tutorial\n\n## Video/Audio/Animations\n\nRational Exponents:\n\nExponents are not only integers and unit fractions. An exponent can be any rational number expressed as the quotient of two integers.\n\nType: Video/Audio/Animation\n\nRadical expressions can often be simplified by moving factors which are perfect roots out from under the radical sign.\n\nType: Video/Audio/Animation\n\nSolving Mixture Problems with Linear Equations:\n\nMixture problems can involve mixtures of things other than liquids. This video shows how Algebra can be used to solve problems involving mixtures of different types of items.\n\nType: Video/Audio/Animation\n\nUsing Systems of Equations Versus One Equation:\n\nWhen should a system of equations with multiple variables be used to solve an Algebra problem, instead of using a single equation with a single variable?\n\nType: Video/Audio/Animation\n\nParallel Lines:\n\nThis video illustrates how to determine if the graphs of a given set of equations are parallel.\n\nType: Video/Audio/Animation\n\nAverages:\n\nThis Khan Academy video tutorial introduces averages and algebra problems involving averages.\n\nType: Video/Audio/Animation\n\n## Virtual Manipulatives\n\n3-D Conic Section Explorer:\n\nUsing this resource, students can manipulate the measurements of a 3-D hourglass figure (double-napped cone) and its intersecting plane to see how the graph of a conic section changes.  Students will see the impact of changing the height and slant of the cone and the m and b values of the plane on the shape of the graph. Students can also rotate and re-size the cone and graph to view from different angles.\n\nType: Virtual Manipulative\n\nCombining Transformations:\n\nIn this manipulative activity, you can first get an idea of what each of the rigid transformations look like, and then get to experiment with combinations of transformations in order to map a pre-image to its image.\n\nType: Virtual Manipulative\n\nCross Section Flyer - Shodor:\n\nWith this online Java applet, students use slider bars to move a cross section of a cone, cylinder, prism, or pyramid. This activity allows students to explore conic sections and the 3-dimensional shapes from which they are derived. This activity includes supplemental materials, including background information about the topics covered, a description of how to use the application, and exploration questions for use with the java applet.\n\nType: Virtual Manipulative\n\nBox Plot:\n\nIn this activity, students use preset data or enter in their own data to be represented in a box plot. This activity allows students to explore single as well as side-by-side box plots of different data. This activity includes supplemental materials, including background information about the topics covered, a description of how to use the application, and exploration questions for use with the Java applet.\n\nType: Virtual Manipulative\n\nData Flyer:\n\nUsing this virtual manipulative, students are able to graph a function and a set of ordered pairs on the same coordinate plane. The constants, coefficients, and exponents can be adjusted using slider bars, so the student can explore the affect on the graph as the function parameters are changed. Students can also examine the deviation of the data from the function. This activity includes supplemental materials, including background information about the topics covered, a description of how to use the application, and exploration questions for use with the java applet.\n\nType: Virtual Manipulative\n\nNormal Distribution Interactive Activity:\n\nWith this online tool, students adjust the standard deviation and sample size of a normal distribution to see how it will affect a histogram of that distribution. This activity allows students to explore the effect of changing the sample size in an experiment and the effect of changing the standard deviation of a normal distribution. Tabs at the top of the page provide access to supplemental materials, including background information about the topics covered, a description of how to use the application, and exploration questions for use with the java applet.\n\nType: Virtual Manipulative\n\nFunction Flyer:\n\nIn this online tool, students input a function to create a graph where the constants, coefficients, and exponents can be adjusted by slider bars. This tool allows students to explore graphs of functions and how adjusting the numbers in the function affect the graph. Using tabs at the top of the page you can also access supplemental materials, including background information about the topics covered, a description of how to use the application, and exploration questions for use with the java applet.\n\nType: Virtual Manipulative\n\nThis is an online graphing utility that can be used to create box plots, bubble graphs, scatterplots, histograms, and stem-and-leaf plots.\n\nType: Virtual Manipulative\n\nA Plethora of Polyhedra:\n\nThis program allows users to explore spatial geometry in a dynamic and interactive way. The tool allows users to rotate, zoom out, zoom in, and translate a plethora of polyhedra. The program is able to compute topological and geometrical duals of each polyhedron. Geometrical operations include unfolding, plane sections, truncation, and stellation.\n\nType: Virtual Manipulative\n\nHistogram Tool:\n\nThis virtual manipulative histogram tool can aid in analyzing the distribution of a dataset. It has 6 preset datasets and a function to add your own data for analysis.\n\nType: Virtual Manipulative\n\nHistogram:\n\nIn this activity, students can create and view a histogram using existing data sets or original data entered. Students can adjust the interval size using a slider bar, and they can also adjust the other scales on the graph. This activity allows students to explore histograms as a way to represent data as well as the concepts of mean, standard deviation, and scale. This activity includes supplemental materials, including background information about the topics covered, a description of how to use the application, and exploration questions for use with the java applet.\n\nType: Virtual Manipulative\n\n## Parent Resources\n\nVetted resources caregivers can use to help students learn the concepts and skills in this course." ]
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https://www.howmany.wiki/u/How-many--kilogram--in--32--pound
[ "## HowMany.wiki\n\nPlease get in touch with us if you:\n\n1. Have any suggestions\n2. Have any questions\n3. Have found an error/bug\n4. Anything else ...\n\n# How many kilograms in 32 pounds?\n\n32 pounds equals 14.515 kilograms because 32 times 0.453592 (the conversion factor) = 14.515\n\n## How to convert 32 pounds to kilograms\n\nTo calculate a value in pounds to the corresponding value in kilograms, just multiply the quantity in pounds by 0.45359237 (the conversion factor).\n\nHere is the formula:\n\nValue in kilograms = value in pounds × 0.45359237\n\nSupose you want to convert 32 pounds into kilograms. In this case you will have:\n\nValue in kilograms = 32 × 0.45359237 = 14.51495584\n\nBy using this converter you can get answers to questions like:\n\n• How many kilograms are there in 32 pounds?\n• 32 pounds are equal to how many kilograms?\n• How much are 32 pound in kilograms?\n• How to convert pounds to kilograms?\n• How to transform pounds in kilograms?\n• What is the formula to convert from pounds to kilograms? among others.\n\n## Pounds to Kilograms Conversion Chart Near 26 pounds\n\nPounds to Kilograms\n26 pounds = 11.79 kilograms\n27 pounds = 12.25 kilograms\n28 pounds = 12.7 kilograms\n29 pounds = 13.15 kilograms\n30 pounds = 13.61 kilograms\n31 pounds = 14.06 kilograms\n32 pounds = 14.51 kilograms\n33 pounds = 14.97 kilograms\n34 pounds = 15.42 kilograms\n35 pounds = 15.88 kilograms\n36 pounds = 16.33 kilograms\n37 pounds = 16.78 kilograms\n38 pounds = 17.24 kilograms\n\nNote: Values are rounded to 4 significant figures. Fractions are rounded to the nearest 8th fraction.\n\n### Disclaimer\n\nWhile every effort is made to ensure the accuracy of the information provided on this website, neither this website nor its authors are responsible for any errors or omissions. Therefore, the contents of this site are not suitable for any use involving risk to health, finances, or property." ]
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https://www.cagednomoremovie.com/how-do-you-do-a-left-arrow-in-latex/
[ "# How do you do a left arrow in LaTeX?\n\n## How do you do a left arrow in LaTeX?\n\nAlternate commands for simple arrows. Long LaTeX arrows….Arrow LaTeX Symbols.\n\nDescription LaTeX command Output\nLeft Arrow, Right arrow \\leftarrow, \\rightarrow ←, →\nDouble Left Arrow, Double right arrow \\Leftarrow, \\Rightarrow ⇐, ⇒\nLong double Left Arrow \\Longleftarrow\nLong Left Arrow \\longleftarrow\n\n### How do you insert an arrow in LaTeX?\n\nLatex provides a huge number of different arrow symbols. Arrows would be used within math enviroment. If you want to use them in text just put the arrow command between two $like this example:$parrow\\$ now you got an up arrow in text.\n\n#### How do you write an if and only arrow in LaTeX?\n\n\\iff (= \\Leftrightarrow ) or.\n\nWhat is a right arrow in math?\n\nThe → symbol (right arrow) is used in math to describe a variable approaching another value in the limit operator. The right arrow symbol is typically used in an expression like this. x→nlimf(x) In plain language, this means take the limit of the expression f(x) as the variable x approaches the value n.\n\nHow do I type an implies symbol in LaTeX?\n\n1. \\Rightarrow.\n2. \\to or \\rightarrow.\n3. \\supset.\n4. \\implies.\n\n## How do you make a symbol in LaTeX?\n\nYou may be wondering how to insert symbols in LaTeX. It is possible to add certain symbols in-text while others require LaTeX’s math mode to be activated. ”, you can use the command \\star in your code.\n\n### How do you write partial derivatives in LaTeX?\n\nThe code for such an example is given below:\n\n1. \\documentclass[12pt]{article}\n2. sepackage{mathtools}\n3. sepackage{xfrac}\n4. \\begin{document}\n5. $6. \\frac{\\partial u}{\\partial t} = \\frac{\\partial^2 u}{\\partial x^2} + \\frac{\\partial^2 u}{\\partial y^2} 7.$\n8. \\end{document}\n\n#### How do I write an if statement in LaTeX?\n\nlatex Counters, if statements and loops with latex If statements\n\n1. Comparing two integers: \\ifnum\\value{num}>n {A} \\else {B}\\fi. This code executes A if num>n else B.\n2. If a number is odd: \\ifodd\\value{num} {A}\\else {B}\\fi. If num is odd then it executes A else B.\n3. If with condition: \\ifthenelse{condition}{A}{B}\n\nHow do you write belongs in LaTeX?\n\nHow to write Latex symbol belongs to : \\in means “is an element of”, “a member of” or “belongs to”.\n\nWhat does left right arrow mean in math?\n\n:\\Leftrightarrow. definition. is defined as. everywhere. x ≔ y or x ≡ y means x is defined to be another name for y (but note that ≡ can also mean other things, such as congruence).\n\n## What does left arrow mean in math?\n\nIt means “set”, or assignment. So in most syntax, those lines are i = 0 and i = i + 1 . This was probably avoided because in math, = means == , and assignment isn’t a useful concept.\n\n### What does arrow mean in logic?\n\nIn mathematical logic the implication arrows \\Rightarrow and \\Leftrightarrow are used to connect expressions as follows: p\\Rightarrow q means ‘IF p is true THEN q is true. p\\Leftrightarrow q means both p\\Rightarrow q AND q \\Rightarrow p simultaneously.\n\n#### How to use arrow symbols in latex?\n\nArrows can be used in equations, text, pictures, and so on. Here is a list of arrow LaTeX commands that can be used without loading any package: The following multitude of arrow symbols require an additional package called amssymb: We can use the LaTeX arrow symbol both in mathematical formulas and text mode, even in pictures and margin indicators.\n\nWhat are the different types of latex arrows?\n\nLatex Up and down arrows, Latex Left and right arrows, Latex Direction and Maps to arrow and Latex Harpoon and hook arrows are shown in this article.\n\nWhat are the special mathematical symbols in latex?\n\nLaTeX has dozens of special mathematical symbols. A few of them, such as +,-, <, and >, are produced by typing the corresponding keyboard characters. Others are obtained with LaTeX commands as the case with arrow symbols which is the purpose of this post!" ]
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https://www.zora.uzh.ch/id/eprint/21572/
[ "", null, "# Chen-Ruan cohomology of ADE singularities\n\nPerroni, F (2007). Chen-Ruan cohomology of ADE singularities. International Journal of Mathematics, 18(9):1009-1059.\n\n## Abstract\n\nWe study Ruan's cohomological crepant resolution conjecture for orbifolds with transversal ADE singularities. In the An-case, we compute both the Chen–Ruan cohomology ring and the quantum corrected cohomology ring H*(Z)(q1,…,qn). The former is achieved in general, the later up to some additional, technical assumptions. We construct an explicit isomorphism between and H*(Z)(-1) in the A1-case, verifying Ruan's conjecture. In the An-case, the family H*(Z)(q1,…,qn) is not defined for q1 = ⋯ = qn = -1. This implies that the conjecture should be slightly modified. We propose a new conjecture in the An-case (Conjecture 1.9). Finally, we prove Conjecture 1.9 in the A2-case by constructing an explicit isomorphism.\n\n## Abstract\n\nWe study Ruan's cohomological crepant resolution conjecture for orbifolds with transversal ADE singularities. In the An-case, we compute both the Chen–Ruan cohomology ring and the quantum corrected cohomology ring H*(Z)(q1,…,qn). The former is achieved in general, the later up to some additional, technical assumptions. We construct an explicit isomorphism between and H*(Z)(-1) in the A1-case, verifying Ruan's conjecture. In the An-case, the family H*(Z)(q1,…,qn) is not defined for q1 = ⋯ = qn = -1. This implies that the conjecture should be slightly modified. We propose a new conjecture in the An-case (Conjecture 1.9). Finally, we prove Conjecture 1.9 in the A2-case by constructing an explicit isomorphism.\n\n## Statistics\n\n### Citations\n\nDimensions.ai Metrics\n12 citations in Web of Science®\n11 citations in Scopus®\n\n### Altmetrics\n\nDetailed statistics\n\nItem Type: Journal Article, refereed, original work 07 Faculty of Science > Institute of Mathematics 510 Mathematics Physical Sciences > General Mathematics Chen–Ruan cohomology, Ruan's conjecture, McKay correspondence English 2007 02 Nov 2009 12:37 25 Feb 2020 12:42 World Scientific Publishing 0129-167X Green https://doi.org/10.1142/S0129167X07004436 http://arxiv.org/abs/math.AG/0605207\n\n##", null, "", null, "", null, "Preview\nContent: Accepted Version\nFiletype: PDF (Accepted manuscript, Version 2)\nSize: 502kB\nView at publisher", null, "", null, "Preview\nContent: Accepted Version\nFiletype: PDF (Accepted manuscript, Version 1)\nSize: 498kB" ]
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http://athensmutualaid.net/eureka-math-grade-7-module-1-lesson-2-answer-key/
[ "Eureka Math Grade 7 Module 1 Lesson 2 Answer Key. Eureka math grade 7 module 2 lesson 1 exit ticket answer key question 1. The fish is 8 feet below the water’s surface.\n\nEureka math grade 7 module 2 lesson 16 exercise answer key exercise 1. Find three different pairs that would complete your hand and result. Eureka math grade 7 module 2 lesson 1 exit ticket answer key question 1.\n\n### Eureka Math Grade 7 Module 2 Lesson 7 Problem Set Answer Key Represent Each Of The Following Problems Using.\n\nEureka math grade 7 module 2 lesson 1 exit ticket answer key question 1. Find three different pairs that would complete your hand and result. Find an efficient strategy to evaluate the expression and complete the necessary work.\n\n### Eureka Math Grade 7 Module.\n\nYour hand starts with the 7 card. Eureka math grade 7 module 2 lesson 16 exercise answer key exercise 1. Eureka math grade 7 module 2 rational numbers.", null, "" ]
[ null, "http://athensmutualaid.net/wp-content/themes/rectusminimum/images/pagetop.png", null ]
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https://hsm.stackexchange.com/questions/3486/did-wave-optics-anticipate-quantum-mechanics
[ "# Did wave optics anticipate quantum mechanics?\n\nI heard in wave optics and electromagnetism that Hamilton could have discovered the Schrödinger equation, or that he was the first man who used the expression\n\n$$\\Psi(x)= \\exp(i S(x)/\\hbar)\\,.$$\n\nI also heard that Hamilton got the idea from the eikonal equation\n\n$$(\\nabla S)^{2}=n(x)\\,,$$\n\nbut that he couldn't complete it.\n\nHe was trying to show that light particles could also be described as a wave, but had no way to prove it. Is this what happened?\n\n• Hamilton did not discover quantum mechanics. But he discovered some mathematics which was later used in quantum mechanics. Mar 4 '16 at 21:05\n\nIt is more accurate to say that Hamilton anticipated some of the ideas of mathematics and heuristics of quantum mechanics, that would later inspire Schrödinger to produce his formulation of wave mechanics. The reason he was able to anticipate those ideas is that the quantum wave-particle duality had a classical predecessor, the optico-mechanical analogy. Indeed, it was optics, not mechanics, that originally inspired the Hamiltonian formalism. But no, Hamilton was not about to discover the Schrödinger equation. There is a qualitative difference between the first order Hamilton-Jacobi equation, and the second order Schrödinger equation, the connection is only recovered in the quasi-classical limit. And it is only for the latter that the stationary phase approximation for integrals of $$\\exp(i S(x)/\\hbar)$$ is used. The approximation itself was only introduced by Kelvin in 1887, Hamilton's approach was more geometric.\n\nIn a simple form the analogy was discovered by Huygens around 1670 (published in Traitė de la Lumiere, 1678), who noticed that propagation of waves could be dually described in terms of wavefronts and rays (\"characteristics\") perpendicular to them. The latter can be considered as trajectories of particles, and massive amounts of particles spreading along characteristics can create the appearence of a continuous wave. But it also works vise versa, and Huygens suggested that light may well be a wave, with geometric optics of rays being only the first approximation. In particular, Huygens showed how Fermat's least time principle follows from the analogy, Johann Bernoulli used it to solve the famous brachistochrone problem in 1696, and in 1818 Fresnel showed how not only geometric optics but also diffraction and interference can be explained by wave optics, which led to its wide acceptance in the 19th century.\n\nBut it was Hamilton who explored the analogy in its full generality. As Guillemin writes in Geometric Asymptotics:\n\n\"In 1828 Hamilton published his fundamental paper on geometrical optics, introducing his \"characteristics\", as a key tool in the study of optical instruments. It wasn't until substantially later that Hamilton realized that his method applied equally well to the study of mechanics. Hamilton's method was developed by Jacobi and has been a cornerstone of theoretical mechanics ever since... It is interesting to note that although Hamilton was aware of the work of Fresnel, he chose to ignore it completely in his fundamental papers on geometrical optics.\"\n\nThe eikonal equation is only the simplest case of the Hamilton-Jacobi equation, when the Hamiltonian of the mechanical system only has the standard kinetic energy term. In general, the familiar equations of Hamilton dynamics are solved by the characteristics of the corresponding Hamilton-Jacobi equation. Although the method of stationary phase is often used to derive geometric asymptotics today, it was not available to Hamilton.\n\nWhen the conflict between the wave optics and the newly introduced light quanta Schrödinger, a big fan of Hamiltonian dynamics, was reminded of the optico-mechanical analogy, and started thinking about classical mechanics being the limit of a new mechanics along the lines of geometric optics being a limit of wave optics. This led him to his celebrated equation. In the quasi-classical limit the surfaces of equal phase are the \"wave fronts\", and the trajectories of the particles are the characteristics. A systematic development of this approach is known as the WKB (Wentzel–Kramers–Brillouin) method.\n\nWhat Hamilton discovered is a mathematical \"Hamiltonian formalism\". It was applied to those parts of physics which were known at the time of Hamilton: classical mechanics and optics. There was no slightest reasons at the time of Hamilton to suspect that matter on small scale does not obey the laws of classical mechanics.\n\nThat this is so, is a late 19s century discovery. However it turned out that Hamiltonian formalism is so general that it applies to quantum mechanics as well. Thus many equations written by Hamilton (and not only by Hamilton, but by other late 18s and early 19s century researchers in mechanics, like Lagrange) actually apply, if they are correctly interpreted.\n\nSimilarly, Calculus, a mathematical tool invented in 17s century serves not only mechanics, but all physics discovered later. But nobody claims on this ground that Newton and Leibniz discovered all physics which was discovered later.\n\nEDIT. Of course this is a miracle that the same mathematical tool applies to a very wide class of phenomena in the universe, including those which were not known when the tool was invented/discovered, but this is the way our world is created." ]
[ null ]
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https://dev.opencascade.org/doc/refman/html/class_geom2d_gcc___function_tan_obl.html
[ "Geom2dGcc_FunctionTanObl Class Reference\n\nThis class describe a function of a single variable. More...\n\n`#include <Geom2dGcc_FunctionTanObl.hxx>`\n\nInheritance diagram for Geom2dGcc_FunctionTanObl:", null, "[legend]\n\n## Public Member Functions\n\nGeom2dGcc_FunctionTanObl (const Geom2dAdaptor_Curve &Curve, const gp_Dir2d &Dir)\n\nStandard_Boolean Value (const Standard_Real X, Standard_Real &F)\nComputes the value of the function F for the variable X. It returns True if the computation is successfully done, False otherwise. More...\n\nStandard_Boolean Derivative (const Standard_Real X, Standard_Real &Deriv)\nComputes the derivative of the function F for the variable X. It returns True if the computation is successfully done, False otherwise. More...\n\nStandard_Boolean Values (const Standard_Real X, Standard_Real &F, Standard_Real &Deriv)\nComputes the value and the derivative of the function F for the variable X. It returns True if the computation is successfully done, False otherwise. More...", null, "Public Member Functions inherited from math_FunctionWithDerivative\nvirtual ~math_FunctionWithDerivative ()", null, "Public Member Functions inherited from math_Function\nvirtual ~math_Function ()\nVirtual destructor, for safe inheritance. More...\n\nvirtual Standard_Integer GetStateNumber ()\nreturns the state of the function corresponding to the latest call of any methods associated with the function. This function is called by each of the algorithms described later which defined the function Integer Algorithm::StateNumber(). The algorithm has the responsibility to call this function when it has found a solution (i.e. a root or a minimum) and has to maintain the association between the solution found and this StateNumber. Byu default, this method returns 0 (which means for the algorithm: no state has been saved). It is the responsibility of the programmer to decide if he needs to save the current state of the function and to return an Integer that allows retrieval of the state. More...\n\n## Detailed Description\n\nThis class describe a function of a single variable.\n\n## ◆ Geom2dGcc_FunctionTanObl()\n\n Geom2dGcc_FunctionTanObl::Geom2dGcc_FunctionTanObl ( const Geom2dAdaptor_Curve & Curve, const gp_Dir2d & Dir )\n\n## ◆ Derivative()\n\n Standard_Boolean Geom2dGcc_FunctionTanObl::Derivative ( const Standard_Real X, Standard_Real & Deriv )\nvirtual\n\nComputes the derivative of the function F for the variable X. It returns True if the computation is successfully done, False otherwise.\n\nImplements math_FunctionWithDerivative.\n\n## ◆ Value()\n\n Standard_Boolean Geom2dGcc_FunctionTanObl::Value ( const Standard_Real X, Standard_Real & F )\nvirtual\n\nComputes the value of the function F for the variable X. It returns True if the computation is successfully done, False otherwise.\n\nImplements math_FunctionWithDerivative.\n\n## ◆ Values()\n\n Standard_Boolean Geom2dGcc_FunctionTanObl::Values ( const Standard_Real X, Standard_Real & F, Standard_Real & Deriv )\nvirtual\n\nComputes the value and the derivative of the function F for the variable X. It returns True if the computation is successfully done, False otherwise.\n\nImplements math_FunctionWithDerivative.\n\nThe documentation for this class was generated from the following file:" ]
[ null, "https://dev.opencascade.org/doc/refman/html/class_geom2d_gcc___function_tan_obl__inherit__graph.png", null, "https://dev.opencascade.org/doc/refman/html/closed.png", null, "https://dev.opencascade.org/doc/refman/html/closed.png", null ]
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https://www.geeksforgeeks.org/class-12-rd-sharma-solutions-chapter-17-increasing-and-decreasing-functions-exercise-17-1/?ref=rp
[ "# Class 12 RD Sharma Solutions – Chapter 17 Increasing and Decreasing Functions – Exercise 17.1\n\n### Question 1: Prove that the function f(x) = loge x is increasing on (0,∞).\n\nSolution:\n\nLet x1, x2 ∈ (0, ∞)\n\nWe have, x1<x2\n\n⇒ loge x1 < loge x\n\n⇒ f(x1) < f(x2)\n\nTherefore, f(x) is increasing in (0, ∞).\n\n### Question 2: Prove that the function f(x) = loga (x) is increasing on (0,∞) if a>1 and decreasing on (0,∞) if 0<a<1.\n\nSolution:\n\nCase 1:\n\nWhen a>1\n\nLet x1, x2 ∈ (0, ∞)\n\nWe have, x1<x2\n\n⇒ loge x1 < loge x2\n\n⇒ f(x1) < f(x2)\n\nTherefore, f(x) is increasing in (0, ∞).\n\nCase 2:\n\nWhen 0<a<1\n\nf(x) = loga x = logx/loga\n\nWhen a<1 ⇒ log a< 0\n\nlet x1<x2\n\n⇒ log x1<log x2\n\n⇒ ( log x1/log a) > (log x2/log a)                                [log a<0]\n\n⇒   f(x1) > f(x2)\n\nTherefore, f(x) is decreasing in (0, ∞).\n\n### Question 3: Prove that f(x) = ax + b,  where a, b are constants and a>0 is an increasing function on R.\n\nSolution:\n\nWe have,\n\nf(x) = ax + b, a > 0\n\nLet x1, x2 ∈ R and x1 >x2\n\n⇒ ax1 > ax2 for some a>0\n\n⇒ ax1 + b > ax2 + b for some b\n\n⇒ f(x1) > f(x2)\n\nHence, x1 > x2  ⇒   f(x1) > f(x2)\n\nTherefore, f(x) is increasing function of  R.\n\n### Question 4: Prove that f(x) = ax + b, where a, b are constants and a<0 is a decreasing function on R.\n\nSolution:\n\nWe have,\n\nf(x) = ax + b, a < 0\n\nLet x1, x2 ∈ R and x1 >x2\n\n⇒ ax1 < ax2 for some a>0\n\n⇒ ax1 + b <ax2 + b for some b\n\n⇒ f(x1) <f(x2)\n\nHence, x1 > x2  ⇒   f(x1) <f(x2)\n\nTherefore, f(x) is decreasing function of  R.\n\n### Question 5: Show that f(x) = 1/x is a decreasing function on (0,∞).\n\nWe have,\n\nf(x) = 1/x\n\nLet x1, x2 ∈  (0,∞) and x1 > x2\n\n⇒  1/x1 < 1/x2\n\n⇒ f(x1) < f(x2)\n\nThus, x1 > x2 ⇒ f(x1) < f(x2)\n\nTherefore, f(x) is decreasing function.\n\n### Question 6: Show that f(x) = 1/(1+x2) decreases in the interval [0, ∞] and increases in the interval [-∞,0].\n\nSolution:\n\nWe have,\n\nf(x) = 1/1+ x\n\nCase 1:\n\nwhen x ∈ [0, ∞]\n\nLet x1, x2 ∈  [0,∞] and x1 > x2\n\n⇒  x12 > x22\n\n⇒  1+x12 < 1+x22\n\n⇒ 1/(1+ x12 )> 1/(1+ x2 )\n\n⇒ f(x1) < f(x2)\n\nTherefore, f(x) is decreasing in [0, ∞].\n\nCase 2:\n\nwhen x ∈ [-∞, 0]\n\nLet x1 > x2\n\n⇒  x12 < x2                           [-2>-3 ⇒   4<9]\n\n⇒  1+x12 < 1+x22\n\n⇒ 1/(1+ x12)> 1/(1+ x22  )\n\n⇒ f(x1) > f(x2)\n\nTherefore, f(x) is increasing in [-∞,0].\n\n### Question 7: Show that f(x) = 1/(1+x2) is neither increasing nor decreasing on R.\n\nSolution:\n\nWe have,\n\n(x) = 1/1+ x2\n\nR can be divided into two intervals [0, ∞] and [-∞,0]\n\nCase 1:\n\nwhen x ∈ [0, ∞]\n\nLet x1 > x2\n\n⇒  x12 > x22\n\n⇒  1+x12 < 1+x22\n\n⇒ 1/(1+ x12 )> 1/(1+ x22  )\n\n⇒ f(x1) < f(x2)\n\nTherefore, f(x) is decreasing in [0, ∞].\n\nCase 2:\n\nwhen x ∈ [-∞, 0]\n\nLet x1 > x2\n\n⇒  x12 < x22                            [-2>-3 ⇒   4<9]\n\n⇒  1+x12 < 1+x22\n\n⇒ 1/(1+ x12)> 1/(1+ x22 )\n\n⇒ f(x1) > f(x2)\n\nTherefore, f(x) is increasing in [-∞,0].\n\nHere, f(x) is decreasing in [0, ∞] and f(x) is increasing in [-∞,0].\n\nThus, f(x) neither increases nor decreases on R.\n\n### (i) strictly increasing in (0,∞)                      (ii) strictly decreasing in (-∞,0)\n\nSolution:\n\n(i). Let x1, x2 ∈  [0,∞] and x1 > x2\n\n⇒  f(x1) > f(x2)\n\nThus, f(x) is strictly increasing in [0,∞].\n\n(ii). Let x1, x2 ∈  [-∞, 0] and x1 > x2\n\n⇒  -x1<-x2\n\n⇒  f(x1) < f(x2)\n\nThus, f(x) is strictly decreasing in [-∞,0].\n\n### Question 9: Without using the derivative show that the function f(x) = 7x – 3 is strictly increasing function on R.\n\nSolution:\n\nf(x) = 7x-3\n\nLet x1, x2 ∈ R and x1 >x2\n\n⇒  7x1 > 7x2\n\n⇒  7x1 – 3 > 7x2 – 3\n\n⇒  f(x1) > f(x2)\n\nThus, f(x) is strictly increasing on R\n\nWhether you're preparing for your first job interview or aiming to upskill in this ever-evolving tech landscape, GeeksforGeeks Courses are your key to success. We provide top-quality content at affordable prices, all geared towards accelerating your growth in a time-bound manner. Join the millions we've already empowered, and we're here to do the same for you. Don't miss out - check it out now!\n\nPrevious\nNext" ]
[ null ]
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https://www.effortlessmath.com/math-topics/how-to-solve-piecewise-functions/
[ "# How to Solve Piecewise Functions?\n\nA piecewise function is a function that has several curves in its graph. In this post blog, you learn more about the piecewise function.", null, "The Piecewise function has different definitions depending on the amount of input, i.e., a piecewise function behaves differently for different inputs.\n\n## A step-by-step guide to piecewise functions\n\npiecewise function is a function $$f(x)$$ which has different definitions in different intervals of $$x$$. The graph of a piecewise function has different parts that correspond to each of its definitions. The absolute value function is a very good example of a piecewise function.  Let us see why is it called so. We know that an absolute value function $$f(x)=| x |$$ and is defined as follows: $$\\begin{cases}x, \\ if\\ x≥0\\ \\\\ -x, \\ if\\ x<0\\end{cases}$$, We need to read this piecewise function as:\n\n• $$f(x)$$ is equal to $$x$$ when $$x$$ is greater than or equal to $$0$$ and\n• $$f(x)$$ is equal to $$-x$$ when $$x$$ is lesser than $$0$$\n\nThen the diagram $$f(x)$$ has two pieces, one corresponding to $$x$$ (when $$x$$ is in the interval $$[0, ∞)$$) and the other corresponding to $$-x$$ (when $$x$$ is in the interval $$(-∞, 0)$$).\n\n### Piecewise function graph\n\nThe diagram of a piecewise function has several pieces, where each piece corresponds to its definition in an interval. Here are the steps to graph a piecewise function.\n\n• Step 1: First, understand what each definition of a function represents. For example, $$f(x)= ax + b$$ represents a linear function (which gives a line), $$f(x)= ax^2+ bx+c$$ represents a quadratic function (which gives a parabola), and so on. So that we will have an idea of what shape the piece of the function would result in.\n• Step 2: Write the intervals shown in the function definition along with their definitions.\n• Step 3: Create a two-column table labeled $$x$$ and $$y$$ corresponding to each interval. Insert the endpoints of the interval without fail. If the endpoint is removed from the interval, note that we get an open dot corresponding to that point in the graph.\n• Step 4: In each table, get more numbers (random numbers) in the $$x$$ column that lies in the corresponding interval to get the perfect shape of the graph. If the piece is a straight line, $$2$$ values are enough for $$x$$. If the piece is not a straight line, take $$3$$ or more for $$x$$.\n• Step 5: Substitute each $$x$$ value from each table into the function definition to obtain the corresponding $$y$$ values.\n• Step 6: Now, just draw all the points from the table (taking care of the open dots) in a graph sheet and connect them by curves.\n\n### Domain and range of piecewise function\n\nTo find the domain of a piecewise function, we can only look at the definition of the given function. Take the union of all intervals with $$x$$ and that will give us the domain.\n\nTo find the range of a piecewise function, the easiest way is to plot it and look at the $$y$$-axis. See what $$y$$-values are covered by the graph.\n\n### Evaluating piecewise function\n\nTo evaluate a piecewise function at any given input,\n\n• First, see which of the given intervals (or inequalities) the given input belongs.\n• Then just replace the given input in the function definition corresponding to that particular interval.\n\n### Piecewise continuous function\n\nA piecewise continuous function, as its name implies, is a continuous function, which means, its graph has different pieces in it but still we will be able to draw the graph without lifting the pencil.\n\n## Exercises for Piecewise Functions\n\n### Graph the piecewise function.\n\n• $$\\color{blue}{\\begin{cases}-2^x, x<−2 \\\\ −|x|, −2≤x≤0\\\\2-x^2, x>0\\end{cases}}$$\n• $$\\color{blue}{\\begin{cases}x+1, x<0 \\\\ −x+1, 0≤x≤2\\\\x-1, x>2\\end{cases}}$$\n• $$\\color{blue}{\\begin{cases}-2^x, x<−2 \\\\ −|x|, −2≤x≤0\\\\ 2-x^2, x>0\\end{cases}}$$\n• $$\\color{blue}{\\begin{cases}x+1, x<0 \\\\ −x+1, 0≤x≤2\\\\x-1, x>2\\end{cases}}$$\n\n### What people say about \"How to Solve Piecewise Functions? - Effortless Math: We Help Students Learn to LOVE Mathematics\"?\n\nNo one replied yet.\n\nX\n30% OFF\n\nLimited time only!\n\nSave Over 30%\n\nSAVE $5 It was$16.99 now it is \\$11.99" ]
[ null, "https://www.effortlessmath.com/wp-content/uploads/2022/04/Blog-How-to-Solve-Piecewise-Functions-512x240.jpg", null ]
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https://forum.qt.io/topic/54601/implementing-a-time-left-function
[ "# Implementing a \"Time Left\" Function\n\n• Hello everyone.\n\nSo, I was able to get a system process delay function working, which gets passed an integer and delays system processes for that many milliseconds that the integer asked for.\nI'm trying to work this code into being able to display the time left, in seconds, into a label. So far, nothing has been working.\n\nAny help would be necessary.\nCODE\n\n``````void MainGame2::gameDelay(int msecs)\n{\n///variables\nint timeLeft = msecs; //used in tandem with progress bar\n\nwhile( QTime::currentTime() < endTime )\n{\n///QCoreApplication handles event loops without UIs\nQCoreApplication::processEvents(QEventLoop::AllEvents, 100);\n}\n}//end function delay\n``````\n\n• @Thugzook\nIt is not completely clear what problem are you see. However, I think you should have a look at the msecsTo funtionality. This is also available for QDateTime and may be easier for bridging days. Also currentDateTime may be of use for you.\n\n• I'm not quite sure how to convert to seconds, it what I'm saying.\nI'm trying to use a while loop to continue to processEvents until the variable endTime.\n\nNot quite sure how to work this out nor how to effectively work an integer countDown within that loop.\n\n• I would suggest taking a look at QElapsedTimer. This class allows you to start a \"count up\" timer.\n\nOne of the methods of the class is elapsed() which returns the number of milliseconds since the timer was started.\n\nBy knowing how long you want to allow (total time perhaps) and using an elapsed timer with elapsed() the difference between the two will be the remaining time, in milliseconds.\n\nTo convert it to a nice human readable form there are lots of ways but you could simply code up (not the prettiest code, downloaded from a stack overflow post):\n\n``````QString ConvertMStoHumanTime( qint64 ms, bool showDays, bool showMS )\n{\nQString Result;\ndouble interval;\nqint64 intval;\n\n// Days\ninterval = 24.0 * 60.0 * 60.0 * 1000.0;\nintval = (qint64)trunc((double)ms / interval);\nif( intval<0 )\nintval = 0;\nms -= (qint64)trunc(intval * interval);\nqint32 days = intval;\n\n// Hours\ninterval = 60.0 * 60.0 * 1000.0;\nintval = (qint64)trunc((double)ms / interval);\nif( intval<0 )\nintval = 0;\nms -= (qint64)trunc(intval * interval);\nqint32 hours = intval;\n\n// Minutes\ninterval = 60.0 * 1000.0;\nintval = (qint64)trunc((double)ms / interval);\nif( intval<0 )\nintval = 0;\nms -= (qint64)trunc(intval * interval);\nqint32 minutes = intval;\n\n// Seconds\ninterval = 1000.0;\nintval = (qint64)trunc((double)ms / interval);\nif( intval<0 )\nintval = 0;\nms -= (qint64)trunc(intval * interval);\nqint32 seconds = intval;\n\n// Whatever is left over is milliseconds\n\nchar buffer;\nmemset( buffer, 0, 25 );\n\nif( showDays )\n{\nif( days<10 )\nsprintf_s( buffer, \"%d\", days );\nResult.append( QString(\"%1d \").arg(buffer) );\n}\n\nif( hours<10 )\nsprintf_s( buffer, \"0%d\", hours );\nelse\nsprintf_s( buffer, \"%d\", hours );\nResult.append( QString(\"%1:\").arg(buffer) );\n\nif( minutes<10 )\nsprintf_s( buffer, \"0%d\", minutes );\nelse\nsprintf_s( buffer, \"%d\", minutes );\nResult.append( QString(\"%1:\").arg(buffer) );\n\nif( seconds<10 )\nsprintf_s( buffer, \"0%d\", seconds );\nelse\nsprintf_s( buffer, \"%d\", seconds );\nResult.append( QString(\"%1\").arg(buffer) );\n\nif( showMS )\n{\nif( ms<10 )\nsprintf_s( buffer, \"00%d\", ms );\nelse if( ms<100 )\nsprintf_s( buffer, \"0%d\", ms );\nelse\nsprintf_s( buffer, \"%d\", ms );\nResult.append( QString(\".%1\").arg(buffer) );\n}\n\nreturn Result;\n}``````" ]
[ null ]
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https://answers.everydaycalculation.com/multiply-fractions/56-24-times-3-63
[ "Solutions by everydaycalculation.com\n\n## Multiply 56/24 with 3/63\n\n1st number: 2 8/24, 2nd number: 3/63\n\nThis multiplication involving fractions can also be rephrased as \"What is 56/24 of 3/63?\"\n\n56/24 × 3/63 is 1/9.\n\n#### Steps for multiplying fractions\n\n1. Simply multiply the numerators and denominators separately:\n2. 56/24 × 3/63 = 56 × 3/24 × 63 = 168/1512\n3. After reducing the fraction, the answer is 1/9\n\nMathStep (Works offline)", null, "Download our mobile app and learn to work with fractions in your own time:" ]
[ null, "https://answers.everydaycalculation.com/mathstep-app-icon.png", null ]
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https://www.probabilitycourse.com/chapter7/7_2_5_convergence_in_probability.php
[ "## 7.2.5 Convergence in Probability\n\nConvergence in probability is stronger than convergence in distribution. In particular, for a sequence $X_1$, $X_2$, $X_3$, $\\cdots$ to converge to a random variable $X$, we must have that $P(|X_n-X| \\geq \\epsilon)$ goes to $0$ as $n\\rightarrow \\infty$, for any $\\epsilon > 0$. To say that $X_n$ converges in probability to $X$, we write\n\n\\begin{align}%\\label{eq:union-bound} X_n \\ \\xrightarrow{p}\\ X . \\end{align} Here is the formal definition of convergence in probability:\n\nConvergence in Probability\n\nA sequence of random variables $X_1$, $X_2$, $X_3$, $\\cdots$ converges in probability to a random variable $X$, shown by $X_n \\ \\xrightarrow{p}\\ X$, if \\begin{align}%\\label{eq:union-bound} \\lim_{n \\rightarrow \\infty} P\\big(|X_n-X| \\geq \\epsilon \\big)=0, \\qquad \\textrm{ for all }\\epsilon>0. \\end{align}\n\nExample\n\nLet $X_n \\sim Exponential(n)$, show that $X_n \\ \\xrightarrow{p}\\ 0$. That is, the sequence $X_1$, $X_2$, $X_3$, $\\cdots$ converges in probability to the zero random variable $X$.\n\n• Solution\n• We have \\begin{align}%\\label{eq:union-bound} \\lim_{n \\rightarrow \\infty} P\\big(|X_n-0| \\geq \\epsilon \\big) &=\\lim_{n \\rightarrow \\infty} P\\big(X_n \\geq \\epsilon \\big) & (\\textrm{ since $X_n\\geq 0$ })\\\\ &=\\lim_{n \\rightarrow \\infty} e^{-n\\epsilon} & (\\textrm{ since $X_n \\sim Exponential(n)$ })\\\\ &=0 , \\qquad \\textrm{ for all }\\epsilon>0. \\end{align}\n\nExample\n\nLet $X$ be a random variable, and $X_n=X+Y_n$, where \\begin{align}%\\label{} EY_n=\\frac{1}{n}, \\qquad \\mathrm{Var}(Y_n)=\\frac{\\sigma^2}{n}, \\end{align} where $\\sigma>0$ is a constant. Show that $X_n \\ \\xrightarrow{p}\\ X$.\n\n• Solution\n• First note that by the triangle inequality, for all $a,b \\in \\mathbb{R}$, we have $|a+b| \\leq |a|+|b|$. Choosing $a=Y_n-EY_n$ and $b=EY_n$, we obtain \\begin{align}%\\label{eq:union-bound} |Y_n| \\leq \\left|Y_n-EY_n\\right|+\\frac{1}{n}. \\end{align} Now, for any $\\epsilon>0$, we have \\begin{align}%\\label{eq:union-bound} P\\big(|X_n-X| \\geq \\epsilon \\big)&=P\\big(|Y_n| \\geq \\epsilon \\big)\\\\ & \\leq P\\left(\\left|Y_n-EY_n\\right|+\\frac{1}{n} \\geq \\epsilon \\right)\\\\ & = P\\left(\\left|Y_n-EY_n\\right|\\geq \\epsilon-\\frac{1}{n} \\right)\\\\ & \\leq \\frac{\\mathrm{Var}(Y_n)}{\\left(\\epsilon-\\frac{1}{n} \\right)^2} &\\textrm{(by Chebyshev's inequality)}\\\\ &= \\frac{\\sigma^2}{n \\left(\\epsilon-\\frac{1}{n} \\right)^2}\\rightarrow 0 \\qquad \\textrm{ as } n\\rightarrow \\infty. \\end{align} Therefore, we conclude $X_n \\ \\xrightarrow{p}\\ X$.\n\nAs we mentioned previously, convergence in probability is stronger than convergence in distribution. That is, if $X_n \\ \\xrightarrow{p}\\ X$, then $X_n \\ \\xrightarrow{d}\\ X$. The converse is not necessarily true. For example, let $X_1$, $X_2$, $X_3$, $\\cdots$ be a sequence of i.i.d. $Bernoulli\\left(\\frac{1}{2}\\right)$ random variables. Let also $X \\sim Bernoulli\\left(\\frac{1}{2}\\right)$ be independent from the $X_i$'s. Then, $X_n \\ \\xrightarrow{d}\\ X$. However, $X_n$ does not converge in probability to $X$, since $|X_n-X|$ is in fact also a $Bernoulli\\left(\\frac{1}{2}\\right)$ random variable and\n\n\\begin{align}%\\label{eq:union-bound} P\\big(|X_n-X| \\geq \\epsilon \\big)&=\\frac{1}{2}, \\qquad \\textrm{ for } 0<\\epsilon<1. \\end{align}\n\nA special case in which the converse is true is when $X_n \\ \\xrightarrow{d}\\ c$, where $c$ is a constant. In this case, convergence in distribution implies convergence in probability. We can state the following theorem:\n\nTheorem If $X_n \\ \\xrightarrow{d}\\ c$, where $c$ is a constant, then $X_n \\ \\xrightarrow{p}\\ c$.\n• Proof\n• Since $X_n \\ \\xrightarrow{d}\\ c$, we conclude that for any $\\epsilon>0$, we have \\begin{align}%\\label{eq:union-bound} \\lim_{n \\rightarrow \\infty} F_{X_n}(c-\\epsilon)=0,\\\\ \\lim_{n \\rightarrow \\infty} F_{X_n}(c+\\frac{\\epsilon}{2})=1. \\end{align} We can write for any $\\epsilon>0$, \\begin{align}%\\label{eq:union-bound} \\lim_{n \\rightarrow \\infty} P\\big(|X_n-c| \\geq \\epsilon \\big) &= \\lim_{n \\rightarrow \\infty} \\bigg[P\\big(X_n \\leq c-\\epsilon \\big) + P\\big(X_n \\geq c+\\epsilon \\big)\\bigg]\\\\ &=\\lim_{n \\rightarrow \\infty} P\\big(X_n \\leq c-\\epsilon \\big) + \\lim_{n \\rightarrow \\infty} P\\big(X_n \\geq c+\\epsilon \\big)\\\\ &=\\lim_{n \\rightarrow \\infty} F_{X_n}(c-\\epsilon) + \\lim_{n \\rightarrow \\infty} P\\big(X_n \\geq c+\\epsilon \\big)\\\\ &= 0 + \\lim_{n \\rightarrow \\infty} P\\big(X_n \\geq c+\\epsilon \\big) \\hspace{50pt} (\\textrm{since } \\lim_{n \\rightarrow \\infty} F_{X_n}(c-\\epsilon)=0)\\\\ &\\leq \\lim_{n \\rightarrow \\infty} P\\big(X_n > c+\\frac{\\epsilon}{2} \\big)\\\\ &= 1-\\lim_{n \\rightarrow \\infty} F_{X_n}(c+\\frac{\\epsilon}{2})\\\\ &=0 \\hspace{140pt} (\\textrm{since } \\lim_{n \\rightarrow \\infty} F_{X_n}(c+\\frac{\\epsilon}{2})=1). \\end{align} Since $\\lim \\limits_{n \\rightarrow \\infty} P\\big(|X_n-c| \\geq \\epsilon \\big) \\geq 0$, we conclude that \\begin{align}%\\label{eq:union-bound} \\lim_{n \\rightarrow \\infty} P\\big(|X_n-c| \\geq \\epsilon \\big)&= 0, \\qquad \\textrm{ for all }\\epsilon>0, \\end{align} which means $X_n \\ \\xrightarrow{p}\\ c$.\n\nThe most famous example of convergence in probability is the weak law of large numbers (WLLN). We proved WLLN in Section 7.1.1. The WLLN states that if $X_1$, $X_2$, $X_3$, $\\cdots$ are i.i.d. random variables with mean $EX_i=\\mu<\\infty$, then the average sequence defined by\n\n\\begin{align}%\\label{} \\overline{X}_n=\\frac{X_1+X_2+...+X_n}{n} \\end{align}\n\nconverges in probability to $\\mu$. It is called the \"weak\" law because it refers to convergence in probability. There is another version of the law of large numbers that is called the strong law of large numbers (SLLN). We will discuss SLLN in Section 7.2.7.\n\nThe print version of the book is available through Amazon here.", null, "" ]
[ null, "https://www.probabilitycourse.com/images/home/book_cover.jpg", null ]
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http://oeis.org/A010490
[ "This site is supported by donations to The OEIS Foundation.", null, "Hints (Greetings from The On-Line Encyclopedia of Integer Sequences!)\n A010490 Decimal expansion of square root of 35. 18\n 5, 9, 1, 6, 0, 7, 9, 7, 8, 3, 0, 9, 9, 6, 1, 6, 0, 4, 2, 5, 6, 7, 3, 2, 8, 2, 9, 1, 5, 6, 1, 6, 1, 7, 0, 4, 8, 4, 1, 5, 5, 0, 1, 2, 3, 0, 7, 9, 4, 3, 4, 0, 3, 2, 2, 8, 7, 9, 7, 1, 9, 6, 6, 9, 1, 4, 2, 8, 2, 2, 4, 5, 9, 1, 0, 5, 6, 5, 3, 0, 3, 6, 7, 6, 5, 7, 5, 2, 5, 2, 7, 1, 8, 3, 1, 0, 9, 1, 7 (list; constant; graph; refs; listen; history; text; internal format)\n OFFSET 1,1 COMMENTS Continued fraction expansion is 5 followed by {1, 10} repeated. - Harry J. Smith, Jun 04 2009 A010490^2 = 35 is the only integer > 0 of form n(n+2), one less than a square, that is also of form n(n+1)(n+2)/6, a tetrahedral number (true for n = 5). Consequence of this, sqrt (35) is the only n in R > 0 such that the following equivalency holds (for n = 5): Where Spin(n/2) = h/(4*Pi)sqrt(n(n+2)) and h = Planck's Constant (A003676), then I. 4*Pi/h*Spin(n/2) = II. The square root of the sum of the relative intensities of the transition states of a Spin(n/2) particle (relative to spin 1/2). Regarding II., for clarification see comments dated May 26 2012 by Stanislav Sykora in A003991. - Raphie Frank, Dec 19 2012 This sequence is associated with Sophie Germain triangular numbers of the first and second kinds, as defined in A217278, by the formula sqrt 35 = sqrt ((A217278(n) - A217278(n-12))/(A217278(n-4) - A217278(n-8))). - Raphie Frank, Dec 22 2012 LINKS Harry J. Smith, Table of n, a(n) for n = 1..20000 Wikipedia, Spin (Physics) EXAMPLE 5.916079783099616042567328291561617048415501230794340322879719669142822... MATHEMATICA RealDigits[N[Sqrt, 105]][] (* Vladimir Joseph Stephan Orlovsky, Feb 20 2011 *) PROG (PARI) { default(realprecision, 20080); x=sqrt(35); for (n=1, 20000, d=floor(x); x=(x-d)*10; write(\"b010490.txt\", n, \" \", d)); } \\\\ Harry J. Smith, Jun 04 2009 CROSSREFS Cf. A040029 (continued fraction). Sequence in context: A186192 A231532 A086201 * A021173 A266553 A306980 Adjacent sequences:  A010487 A010488 A010489 * A010491 A010492 A010493 KEYWORD nonn,cons AUTHOR STATUS approved\n\nLookup | Welcome | Wiki | Register | Music | Plot 2 | Demos | Index | Browse | More | WebCam\nContribute new seq. or comment | Format | Style Sheet | Transforms | Superseeker | Recent\nThe OEIS Community | Maintained by The OEIS Foundation Inc.\n\nLast modified October 14 14:45 EDT 2019. Contains 328019 sequences. (Running on oeis4.)" ]
[ null, "http://oeis.org/banner2021.jpg", null ]
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https://calculatorsonline.org/scientific-notation-to-decimal/20e-5
[ "# Convert 20e-5 to decimal number\n\nHere you will see step by step solution to convert 20e-5 scientific number to decimal. 20e-5 conversion to decimal is 0.0002, please check the explanation that how to convert 20e-5 to as a decimal.\n\n## Answer: 20e-5 as a decimal is\n\n= 0.0002\n\n### How to convert 20e-5 to number?\n\nTo convert the scientific notation 20e-5 number simply multiply the coefficient part with by 10 to the power of exponent[-5]. Scientific notation 20e-5 is same as 2 × 10-4.\n\n#### Solution for 20e-5 to number\n\nFollow these easy steps to convert 20e-5 to number-\n\nGiven scientific notation is => 20e-5\n\ne = 10\n\n20 = Coefficient\n\n-5 = Exponent\n\n=> 20e-5 = 2 × 10-4\n= 0.0002\n\nHence, the 20e-5 is in decimal number form is 0.0002." ]
[ null ]
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https://oeis.org/A070319
[ "This site is supported by donations to The OEIS Foundation.", null, "Hints (Greetings from The On-Line Encyclopedia of Integer Sequences!)\n A070319 Max( tau(k) : k=1,2,3,...,n ) where tau(n)=A000005(n) is the number of divisors of x. 8\n 1, 2, 2, 3, 3, 4, 4, 4, 4, 4, 4, 6, 6, 6, 6, 6, 6, 6, 6, 6, 6, 6, 6, 8, 8, 8, 8, 8, 8, 8, 8, 8, 8, 8, 8, 9, 9, 9, 9, 9, 9, 9, 9, 9, 9, 9, 9, 10, 10, 10, 10, 10, 10, 10, 10, 10, 10, 10, 10, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12, 12 (list; graph; refs; listen; history; text; internal format)\n OFFSET 1,2 COMMENTS Is this the same as A068509? - David Scambler, Sep 10 2012 They are different even asymptotically: A068509(n)=O(sqrt(n)), while a(n) does not have polynomial growth. One example where the sequences differ: a(625) = 24 < A068509(625). (The inequality is implied by the set {1,2,..,25} where each pair of the elements has lcm <= 625.) - Max Alekseyev, Sep 11 2012 The two sequences first differ when n = 336, due to the set of 21 elements {1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 12, 14, 15, 16, 18, 21, 24, 30, 36, 42, 48} where each pair of elements has lcm <= 336, while no positive integer <= 336 has more than 20 divisors. Therefore A068509(336) = 21 and A070319(336) = 20. - William Rex Marshall, Sep 11 2012 REFERENCES Sándor, J., Crstici, B., Mitrinović, Dragoslav S. Handbook of Number Theory I. Dordrecht: Kluwer Academic, 2006, p. 44. S. Wigert. Sur l’ordre de grandeur du nombre des diviseurs d’un entier. Arkiv. for Math. 3 (1907), 1-9. LINKS Charles R Greathouse IV, Table of n, a(n) for n = 1..10000 S. Ramanujan, Highly composite numbers, Proceedings of the London Mathematical Society, 2, XIV, 1915, 347 - 409. FORMULA a(n) = exp(log(2) log(n) / log(log(n)) + O(log(n) log(log(log(n))) / (log(log(n)))^2)). (See Sándor reference for more formulas.) - Eric M. Schmidt, Jun 30 2013 a(n) = A002183(A261100(n)). - Antti Karttunen, Jun 06 2017 MATHEMATICA a = {0}; Do[AppendTo[a, Max[DivisorSigma[0, n], a[[n]]]], {n, 120}]; Rest@ a (* Michael De Vlieger, Sep 29 2015 *) PROG (PARI) a(n)=vecmax(vector(n, k, numdiv(k))) (PARI) v=vector(100); v=1; for(n=2, #v, v[n]=max(v[n-1], numdiv(n))); v \\\\ Charles R Greathouse IV, Sep 12 2012 (Haskell) a070319 n = a070319_list !! (n-1) a070319_list = scanl1 max \\$ map a000005 [1..] -- Reinhard Zumkeller, Apr 01 2011 (PARI) A070319(n, m=1, s=2)={for(k=s, n, m\n\nLookup | Welcome | Wiki | Register | Music | Plot 2 | Demos | Index | Browse | More | WebCam\nContribute new seq. or comment | Format | Style Sheet | Transforms | Superseeker | Recent\nThe OEIS Community | Maintained by The OEIS Foundation Inc.\n\nLast modified July 22 07:23 EDT 2019. Contains 325216 sequences. (Running on oeis4.)" ]
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https://cloud.r-project.org/web/packages/stacks/vignettes/basics.html
[ "# Getting Started With stacks\n\nIn this article, we’ll be working through an example of the workflow of model stacking with the stacks package. At a high level, the workflow looks something like this:\n\n1. Define candidate ensemble members using functionality from rsample, parsnip, workflows, recipes, and tune\n2. Initialize a `data_stack` object with `stacks()`\n3. Iteratively add candidate ensemble members to the `data_stack` with `add_candidates()`\n4. Evaluate how to combine their predictions with `blend_predictions()`\n5. Fit candidate ensemble members with non-zero stacking coefficients with `fit_members()`\n6. Predict on new data with `predict()`!\n\nThe package is closely integrated with the rest of the functionality in tidymodels—we’ll load those packages as well, in addition to some tidyverse packages to evaluate our results later on.\n\n``````library(tidymodels)\nlibrary(stacks)``````\n\nIn this example, we’ll make use of the `tree_frogs` data exported with `stacks`, giving experimental results on hatching behavior of red-eyed tree frog embryos!\n\nRed-eyed tree frog (RETF) embryos can hatch earlier than their normal 7ish days if they detect potential predator threat. Researchers wanted to determine how, and when, these tree frog embryos were able to detect stimulus from their environment. To do so, they subjected the embryos at varying developmental stages to “predator stimulus” by jiggling the embryos with a blunt probe. Beforehand, though some of the embryos were treated with gentamicin, a compound that knocks out their lateral line (a sensory organ.) Researcher Julie Jung and her crew found that these factors inform whether an embryo hatches prematurely or not!\n\nWe’ll start out with predicting `latency` (i.e. time to hatch) based on other attributes. We’ll need to filter out NAs (i.e. cases where the embryo did not hatch) first.\n\n``````data(\"tree_frogs\")\n\n# subset the data\ntree_frogs <- tree_frogs %>%\nfilter(!is.na(latency)) %>%\nselect(-c(clutch, hatched))``````\n\nTaking a quick look at the data, it seems like the hatch time is pretty closely related to some of our predictors!\n\n``````theme_set(theme_bw())\n\nggplot(tree_frogs) +\naes(x = age, y = latency, color = treatment) +\ngeom_point() +\nlabs(x = \"Embryo Age (s)\", y = \"Time to Hatch (s)\", col = \"Treatment\")``````", null, "Let’s give this a go!\n\n# Define candidate ensemble members\n\nAt the highest level, ensembles are formed from model definitions. In this package, model definitions are an instance of a minimal `workflow`, containing a model specification (as defined in the `parsnip` package) and, optionally, a preprocessor (as defined in the `recipes` package). Model definitions specify the form of candidate ensemble members.", null, "Defining the constituent model definitions is undoubtedly the longest part of building an ensemble with `stacks`. If you’re familiar with tidymodels “proper,” you’re probably fine to skip this section, keeping a few things in mind:\n\n• You’ll need to save the assessment set predictions and workflow utilized in your `tune_grid()`, `tune_bayes()`, or `fit_resamples()` objects by setting the `control` arguments `save_pred = TRUE` and `save_workflow = TRUE`. Note the use of the `control_stack_*()` convenience functions below!\n• Each model definition must share the same rsample `rset` object.\n\nWe’ll first start out with splitting up the training data, generating resamples, and setting some options that will be used by each model definition.\n\n``````# some setup: resampling and a basic recipe\nset.seed(1)\ntree_frogs_split <- initial_split(tree_frogs)\ntree_frogs_train <- training(tree_frogs_split)\ntree_frogs_test <- testing(tree_frogs_split)\n\nset.seed(1)\nfolds <- rsample::vfold_cv(tree_frogs_train, v = 5)\n\ntree_frogs_rec <-\nrecipe(latency ~ ., data = tree_frogs_train)\n\nmetric <- metric_set(rmse)``````\n\nTuning and fitting results for use in ensembles need to be fitted with the control arguments `save_pred = TRUE` and `save_workflow = TRUE`—these settings ensure that the assessment set predictions, as well as the workflow used to fit the resamples, are stored in the resulting object. For convenience, stacks supplies some `control_stack_*()` functions to generate the appropriate objects for you.\n\nIn this example, we’ll be working with `tune_grid()` and `fit_resamples()` from the tune package, so we will use the following control settings:\n\n``````ctrl_grid <- control_stack_grid()\nctrl_res <- control_stack_resamples()``````\n\nWe’ll define three different model definitions to try to predict time to hatch—a K-nearest neighbors model (with hyperparameters to tune), a linear model, and a support vector machine model (again, with hyperparameters to tune).\n\nStarting out with K-nearest neighbors, we begin by creating a `parsnip` model specification:\n\n``````# create a model definition\nknn_spec <-\nnearest_neighbor(\nmode = \"regression\",\nneighbors = tune(\"k\")\n) %>%\nset_engine(\"kknn\")\n\nknn_spec\n#> K-Nearest Neighbor Model Specification (regression)\n#>\n#> Main Arguments:\n#> neighbors = tune(\"k\")\n#>\n#> Computational engine: kknn``````\n\nNote that, since we are tuning over several possible numbers of neighbors, this model specification defines multiple model configurations. The specific form of those configurations will be determined when specifying the grid search in `tune_grid()`.\n\nFrom here, we extend the basic recipe defined earlier to fully specify the form of the design matrix for use in a K-nearest neighbors model:\n\n``````# extend the recipe\nknn_rec <-\ntree_frogs_rec %>%\nstep_dummy(all_nominal_predictors()) %>%\nstep_zv(all_predictors()) %>%\nstep_impute_mean(all_numeric_predictors()) %>%\nstep_normalize(all_numeric_predictors())\n\nknn_rec\n#> Recipe\n#>\n#> Inputs:\n#>\n#> role #variables\n#> outcome 1\n#> predictor 4\n#>\n#> Operations:\n#>\n#> Dummy variables from all_nominal_predictors()\n#> Zero variance filter on all_predictors()\n#> Mean imputation for all_numeric_predictors()\n#> Centering and scaling for all_numeric_predictors()``````\n\nStarting with the basic recipe, we convert categorical variables to dummy variables, remove column with only one observation, impute missing values in numeric variables using the mean, and normalize numeric predictors. Pre-processing instructions for the remaining models are defined similarly.\n\nNow, we combine the model specification and pre-processing instructions defined above to form a `workflow` object:\n\n``````# add both to a workflow\nknn_wflow <-\nworkflow() %>%\n\nknn_wflow\n#> ══ Workflow ════════════════════════════════════════════════════════════════════\n#> Preprocessor: Recipe\n#> Model: nearest_neighbor()\n#>\n#> ── Preprocessor ────────────────────────────────────────────────────────────────\n#> 4 Recipe Steps\n#>\n#> • step_dummy()\n#> • step_zv()\n#> • step_impute_mean()\n#> • step_normalize()\n#>\n#> ── Model ───────────────────────────────────────────────────────────────────────\n#> K-Nearest Neighbor Model Specification (regression)\n#>\n#> Main Arguments:\n#> neighbors = tune(\"k\")\n#>\n#> Computational engine: kknn``````\n\nFinally, we can make use of the workflow, training set resamples, metric set, and control object to tune our hyperparameters. Using the `grid` argument, we specify that we would like to optimize over four possible values of `k` using a grid search.\n\n``````# tune k and fit to the 5-fold cv\nset.seed(2020)\nknn_res <-\ntune_grid(\nknn_wflow,\nresamples = folds,\nmetrics = metric,\ngrid = 4,\ncontrol = ctrl_grid\n)\n\nknn_res\n#> # Tuning results\n#> # 5-fold cross-validation\n#> # A tibble: 5 × 5\n#> splits id .metrics .notes .predictions\n#> <list> <chr> <list> <list> <list>\n#> 1 <split [343/86]> Fold1 <tibble [4 × 5]> <tibble [0 × 3]> <tibble [344 × 5]>\n#> 2 <split [343/86]> Fold2 <tibble [4 × 5]> <tibble [0 × 3]> <tibble [344 × 5]>\n#> 3 <split [343/86]> Fold3 <tibble [4 × 5]> <tibble [0 × 3]> <tibble [344 × 5]>\n#> 4 <split [343/86]> Fold4 <tibble [4 × 5]> <tibble [0 × 3]> <tibble [344 × 5]>\n#> 5 <split [344/85]> Fold5 <tibble [4 × 5]> <tibble [0 × 3]> <tibble [340 × 5]>``````\n\nThis `knn_res` object fully specifies the candidate members, and is ready to be included in a `stacks` workflow.\n\nNow, specifying the linear model, note that we are not optimizing over any hyperparameters. Thus, we use the `fit_resamples()` function rather than `tune_grid()` or `tune_bayes()` when fitting to our resamples.\n\n``````# create a model definition\nlin_reg_spec <-\nlinear_reg() %>%\nset_engine(\"lm\")\n\n# extend the recipe\nlin_reg_rec <-\ntree_frogs_rec %>%\nstep_dummy(all_nominal_predictors()) %>%\nstep_zv(all_predictors())\n\n# add both to a workflow\nlin_reg_wflow <-\nworkflow() %>%\n\n# fit to the 5-fold cv\nset.seed(2020)\nlin_reg_res <-\nfit_resamples(\nlin_reg_wflow,\nresamples = folds,\nmetrics = metric,\ncontrol = ctrl_res\n)\n\nlin_reg_res\n#> # Resampling results\n#> # 5-fold cross-validation\n#> # A tibble: 5 × 5\n#> splits id .metrics .notes .predictions\n#> <list> <chr> <list> <list> <list>\n#> 1 <split [343/86]> Fold1 <tibble [1 × 4]> <tibble [0 × 3]> <tibble [86 × 4]>\n#> 2 <split [343/86]> Fold2 <tibble [1 × 4]> <tibble [0 × 3]> <tibble [86 × 4]>\n#> 3 <split [343/86]> Fold3 <tibble [1 × 4]> <tibble [0 × 3]> <tibble [86 × 4]>\n#> 4 <split [343/86]> Fold4 <tibble [1 × 4]> <tibble [0 × 3]> <tibble [86 × 4]>\n#> 5 <split [344/85]> Fold5 <tibble [1 × 4]> <tibble [0 × 3]> <tibble [85 × 4]>``````\n\nFinally, putting together the model definition for the support vector machine:\n\n``````# create a model definition\nsvm_spec <-\nsvm_rbf(\ncost = tune(\"cost\"),\nrbf_sigma = tune(\"sigma\")\n) %>%\nset_engine(\"kernlab\") %>%\nset_mode(\"regression\")\n\n# extend the recipe\nsvm_rec <-\ntree_frogs_rec %>%\nstep_dummy(all_nominal_predictors()) %>%\nstep_zv(all_predictors()) %>%\nstep_impute_mean(all_numeric_predictors()) %>%\nstep_corr(all_predictors()) %>%\nstep_normalize(all_numeric_predictors())\n\n# add both to a workflow\nsvm_wflow <-\nworkflow() %>%\n\n# tune cost and sigma and fit to the 5-fold cv\nset.seed(2020)\nsvm_res <-\ntune_grid(\nsvm_wflow,\nresamples = folds,\ngrid = 6,\nmetrics = metric,\ncontrol = ctrl_grid\n)\n\nsvm_res\n#> # Tuning results\n#> # 5-fold cross-validation\n#> # A tibble: 5 × 5\n#> splits id .metrics .notes .predictions\n#> <list> <chr> <list> <list> <list>\n#> 1 <split [343/86]> Fold1 <tibble [6 × 6]> <tibble [0 × 3]> <tibble [516 × 6]>\n#> 2 <split [343/86]> Fold2 <tibble [6 × 6]> <tibble [0 × 3]> <tibble [516 × 6]>\n#> 3 <split [343/86]> Fold3 <tibble [6 × 6]> <tibble [0 × 3]> <tibble [516 × 6]>\n#> 4 <split [343/86]> Fold4 <tibble [6 × 6]> <tibble [0 × 3]> <tibble [516 × 6]>\n#> 5 <split [344/85]> Fold5 <tibble [6 × 6]> <tibble [0 × 3]> <tibble [510 × 6]>``````\n\nAltogether, we’ve created three model definitions, where the K-nearest neighbors model definition specifies 4 model configurations, the linear regression specifies 1, and the support vector machine specifies 6.", null, "With these three model definitions fully specified, we are ready to begin stacking these model configurations. (Note that, in most applied settings, one would likely specify many more than 11 candidate members.)\n\n# Putting together a stack\n\nThe first step to building an ensemble with stacks is to create a `data_stack` object—in this package, data stacks are tibbles (with some extra attributes) that contain the assessment set predictions for each candidate ensemble member.", null, "We can initialize a data stack using the `stacks()` function.\n\n``````stacks()\n#> # A data stack with 0 model definitions and 0 candidate members.``````\n\nThe `stacks()` function works sort of like the `ggplot()` constructor from ggplot2—the function creates a basic structure that the object will be built on top of—except you’ll pipe the outputs rather than adding them with `+`.\n\nThe `add_candidates()` function adds ensemble members to the stack.\n\n``````tree_frogs_data_st <-\nstacks() %>%\n\ntree_frogs_data_st\n#> # A data stack with 3 model definitions and 11 candidate members:\n#> # knn_res: 4 model configurations\n#> # lin_reg_res: 1 model configuration\n#> # svm_res: 6 model configurations\n#> # Outcome: latency (numeric)``````\n\nAs mentioned before, under the hood, a `data_stack` object is really just a tibble with some extra attributes. Checking out the actual data:\n\n``````as_tibble(tree_frogs_data_st)\n#> # A tibble: 429 × 12\n#> latency knn_res_1_1 knn_res…¹ knn_r…² knn_r…³ lin_r…⁴ svm_r…⁵ svm_r…⁶ svm_r…⁷\n#> <dbl> <dbl> <dbl> <dbl> <dbl> <dbl> <dbl> <dbl> <dbl>\n#> 1 142 76.5 67.8 83.2 83.0 114. 71.0 71.0 84.6\n#> 2 79 74.3 71.0 64.2 63.9 78.6 72.5 72.5 71.4\n#> 3 50 75.0 71.4 64.9 64.3 81.5 71.0 71.0 70.6\n#> 4 68 47.9 49.7 54.0 54.0 78.6 71.1 71.1 70.4\n#> 5 64 60.9 53.1 48.4 48.3 36.5 71.0 71.0 51.5\n#> 6 52 207. 168. 129. 124. 124. 71.1 71.1 92.1\n#> 7 39 30.8 29.1 32.7 33.0 35.2 72.5 72.5 50.6\n#> 8 46 32.3 31.1 35.0 34.6 37.1 72.5 72.5 51.2\n#> 9 137 75.9 78.8 90.4 90.6 78.8 71.1 71.1 70.6\n#> 10 73 67.7 73.6 67.9 67.4 38.8 72.5 72.5 51.7\n#> # … with 419 more rows, 3 more variables: svm_res_1_5 <dbl>, svm_res_1_2 <dbl>,\n#> # svm_res_1_6 <dbl>, and abbreviated variable names ¹​knn_res_1_2,\n#> # ²​knn_res_1_3, ³​knn_res_1_4, ⁴​lin_reg_res_1_1, ⁵​svm_res_1_1, ⁶​svm_res_1_4,\n#> # ⁷​svm_res_1_3``````\n\nThe first column gives the first response value, and the remaining columns give the assessment set predictions for each ensemble member. Since we’re in the regression case, there’s only one column per ensemble member. In classification settings, there are as many columns as there are levels of the outcome variable per candidate ensemble member.\n\nThat’s it! We’re now ready to evaluate how it is that we need to combine predictions from each candidate ensemble member.\n\n# Fit the stack\n\nThe outputs from each of these candidate ensemble members are highly correlated, so the `blend_predictions()` function performs regularization to figure out how we can combine the outputs from the stack members to come up with a final prediction.\n\n``````tree_frogs_model_st <-\ntree_frogs_data_st %>%\nblend_predictions()``````\n\nThe `blend_predictions` function determines how member model output will ultimately be combined in the final prediction by fitting a LASSO model on the data stack, predicting the true assessment set outcome using the predictions from each of the candidate members. Candidates with nonzero stacking coefficients become members.", null, "To make sure that we have the right trade-off between minimizing the number of members and optimizing performance, we can use the `autoplot()` method:\n\n``autoplot(tree_frogs_model_st)``", null, "To show the relationship more directly:\n\n``autoplot(tree_frogs_model_st, type = \"members\")``", null, "If these results were not good enough, `blend_predictions()` could be called again with different values of `penalty`. As it is, `blend_predictions()` picks the penalty parameter with the numerically optimal results. To see the top results:\n\n``autoplot(tree_frogs_model_st, type = \"weights\")``", null, "Now that we know how to combine our model output, we can fit the candidates with non-zero stacking coefficients on the full training set.\n\n``````tree_frogs_model_st <-\ntree_frogs_model_st %>%\nfit_members()``````", null, "Model stacks can be thought of as a group of fitted member models and a set of instructions on how to combine their predictions." ]
[ null, 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", null, 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", null, 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", null, 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", null, 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null, 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", null, 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", null, 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", null, 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W5zaG90PC9leGlmOlVzZXJDb21tZW50PgogICAgICAgICA8ZXhpZjpQaXhlbFlEaW1lbnNpb24+NDA0PC9leGlmOlBpeGVsWURpbWVuc2lvbj4KICAgICAgPC9yZGY6RGVzY3JpcHRpb24+CiAgIDwvcmRmOlJERj4KPC94OnhtcG1ldGE+Chfs0skAAAAcaURPVAAAAAIAAAAAAAAAygAAACgAAADKAAAAygAAdUatUNbqAABAAElEQVR4AezdB5xk2VkY+q+rc5gcOkyOu9ogpH1EAY9sG2QwMtgiWEIPCWQRBAL8DCIYJEw0fsZgeNiAMZLhkYxtwIDBRAshwq6kHa12cu440xM7h3rn1mhmZ3Z6ZjpUdd+q+p/fb7a7q+4995z/uXeru+5X39dQTC00AgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECCwxgINAtrWeAUcngABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgRKAgLanAgECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgkAsBAW25WAaDIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAEBbc4BAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIEMiFgIC2XCyDQRAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQICAgDbnAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAjkQkBAWy6WwSAIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAQECbc4AAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIEciEgoC0Xy2AQBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQICCgzTlAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABArkQENCWi2UwCAIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAQ0OYcIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAIFcCAhoy8UyGAQBAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQICGhzDhAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIBALgQEtOViGQyCAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAS0OQcIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAIBcCAtpysQwGQYAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIC2pwDBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIJALAQFtuVgGgyBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAW3OAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBDIhYCAtlwsg0EQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAgIA25wABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQI5EJAQFsulsEgCBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQEBAm3OAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBHIhIKAtF8tgEAQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECAgoM05QIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQK5EBDQlotlMAgCBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQENDmHCBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgACBXAgIaMvFMhgEAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECAhocw4QIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAQC4EBLTlYhkMggABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQEtDkHCBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQCAXAgLacrEMBkGAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECAtqcAwQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECCQCwEBbblYBoMgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQFtzgECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQyIWAgLZcLINBECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgICANucAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECORCQEBbLpbBIAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIEBAQJtzgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgRyISCgLRfLYBAECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgIKDNOUCAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECuRAQ0JaLZTAIAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIEBDQ5hwgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAgVwICGjLxTIYBAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgIaHMOECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgEAuBAS05WIZDIIAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIEBLQ5BwgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIEAgFwIC2nKxDAZBgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgLanAMECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgkAsBAW25WAaDIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAEBbc4BAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIEMiFgIC2XCyDQRAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQICAgDbnAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAjkQkBAWy6WwSAIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAQECbc4AAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIEciEgoC0Xy2AQBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQICCgzTlAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABArkQENCWi2UwCAIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAQ0OYcIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAIFcCAhoy8UyGAQBAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQICGhzDhAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIBALgQEtOViGQyCAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAS0OQcIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAIBcCAtpysQwGQYAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIC2pwDBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIJALAQFtuVgGgyBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAW3OAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBDIhYCAtlwsg0EQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAgIA25wABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQI5EJAQFsulsEgCBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQEBAm3OAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBHIhIKAtF8tgEAQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECAgoM05QIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQK5EBDQlotlMAgCBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQENDmHCBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgACBXAgIaMvFMhgEAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECAhocw4QIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAQC4EBLTlYhkMggABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQEtDkHCBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQCAXAgLacrEMBkGAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECAtqcAwQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECCQCwEBbblYBoMgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQFtzgECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQyIWAgLZcLINBECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgICANucAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECORCQEBbLpbBIAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIEBAQJtzgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgRyISCgLRfLYBAECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgIKDNOUCAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECuRAQ0JaLZTAIAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIEBDQ5hwgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAgVwICGjLxTIYBAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgIaHMOECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgEAuBAS05WIZDIIAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIEBLQ5BwgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIEAgFwIC2nKxDAZBgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgLanAMECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgkAsBAW25WAaDIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAEBbc4BAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIEMiFgIC2XCyDQRAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQICAgDbnAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAjkQkBAWy6WwSAIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAQECbc4AAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIEciEgoC0Xy2AQBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQICCgzTlAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABArkQENCWi2UwCAIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAQ0OYcIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAIFcCAhoy8UyGAQBAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQIECBAgAABAgQICGhzDhAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIBALgQEtOViGQyCAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBObm52NmdjbaWlpgECBQQwLZtT02NRHr2ztraFamQoBApQQEtFVKVr8ECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgsGiBKzdvxLH+c6WAtn3dfbFjy7ZF72tDAgTyK3D72p6ano7ezVtjf09fNBYa8ztgIyNAYM0FBLSt+RIYAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBOpXYHZuLk4NXoyBK5fvQVjf3hGHd+yOzrb2ex73AwEC1SHwoGu7tbk5DvXtii3rNlTHRIySAIFVFxDQturkDkiAAAECBAgQIECAAAECBAgQIECAAAECBAgQIFBOgWKxGA0NDeXsUl8ECKySwKXrV+N4//mYTmVGF2qFdG3v3tYTu7Z1R/a9RoBAdQg86trOZrF946Y42LMzmpuaqmNSRkmAwKoJCGhbNWoHIkCAAAECBAgQIECAAAECBAgQIECAAAECBAgQKKfAfHE+zg0PRf/oSOxN5Qn7UhkzjQCB6hCYmpkpBbJdvnFtUQPuaG2Lx1K2tvUdnYva3kYECKyNwPTsrWv70vXFXdvNjU1xsHdnKbhtbUbsqAQI5FFAQFseV8WYCBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIEHipwbexmHOs/F+NTU3e2ywJdsoCXLPBFI0AgvwJZadFTAxdjdn5uSYPM8rPt2LItBbD2RmOhcUn72pgAgcoLDKZr+2QqH5yVGl1q29y1Pg7t2BVtzS1L3dX2BAjUoICAthpcVFMiQIAAAQIECBAgQIAAAQIECBAgQIAAgVsC41OTAlucDARqTGAuBcCcGuyPgdFLUVxgbllJwj3bU3nCrd3KkC7g4yECaykwkQJQs0DUqykgdSWtNQW8HO7bFZvXrV9JN/YlQKBMAhPT6dq+uPJru7FQiP09O2RcLdO66IZANQsIaKvm1TN2AgQIECBAgAABAgQIECBAgAABAgQIEFhQIAtkO9Z/Pq6nG+a9qQThvlSKsKlRJpcFsTxIoIoEstKEx9O1nZUqfFTrTFnaDitP+CgmzxNYFYFisRgXLo/EmaH+mE/fl6t1b9wcB3p3RFayUCNAYPUFsmv7Yir7fXpoIObn58s2gA0p42r2Gi7jatlIdUSg6gQEtFXdkhkwAQIECBAgQIAAAQIECBAgQIBAZQSKMT8xGjE7FYXO7REFN8Uq46xXApUVyG6qnb80HGeH0021u26YtzY3x6GUyWXLug2VHYDeCRCoiMD07GycGDgfI9euLqn/UnnCrdtj7/asPGFhSfvamACB8gjcmBgvZW66OTlRng5f1ktzU1Mc7N0Z2zdsetkzfiRAoJICY+maPpqysmXXeCXarYyrvSnj6nYZVysBrE8CORcQ0JbzBTI8AgQIECBAgAABAgQIECBAgACBygsUZydj/uZAKZitdLSGxih0pTJlrUoYVV7fEQiUT2AxN8y3bdhYuund0tRcvgPriQCBigoMXR2NkwMXYmZubtnHaUvlCQ/tSOUJu7y2LxvRjgSWKJBlazo7MlgKNM8CzivdsvKjWRnSrBypRoBA5QSyD42cy67tkaF7PkBSqSN2trXHYylb27r2jkodQr8ECORQQEBbDhfFkAgQIECAAAECBAgQIEAgvwLFmelo8OZ4fhfIyAgsVSC9ET8/cSmK4ykzW9x/k62hpTMFtvWkbG0CX5ZKa3sCqymQ3TA/MzyYSpkNx2JumDen0qMHUiaXrEyZRoBAfgUmp6dKpYOv3LxRtkH2pOt+v/KEZfPUEYEHCVwdu5Gysp2PiXQdr2bLMjHu79kRfancuEaAQPkFro+PlbKyjU9Nlr/zh/TY0NAQO7dkGVd7oiDj6kOkPEWgdgQEtNXOWpoJAQIECBAgQIAAAQIECFRSIAW9TJ05ERMnPhrN23qi44mPi4aW1koeUd8ECFRYoDgznrKyDUbMTT/8SA2FUgnShraND9/OswQIrInArRvm59IN80dcywuMblPXulImlzav6QvoeIjA2glkgakXR0fizNBAzKWA1XK3llJ5wl2RZWzUCBAor8BsyqR4eqg/+kcvlbfjJfa2vqOzlNGpo7VtiXvanACBhQSy1+Mz6dq+eHlkgY+CLbRHZR5rT7+3H04ZVzd2rqvMAfRKgEBuBAS05WYpDIQAAQIECBAgQIAAAQIE8iowd+N6jB95NuauXbkzxCxLW/srXhktqZyJRoBAlQkU52N+PL0JP/HSNb2oGTS3p2xtvdHQqITRorxsRKDCAtkN81ODF2PgyuUVHSnL5LK3uzd2bN4WWeYHjQCBtRUYm5woZX7JSghXum1J5QkPKU9YaWb915HA5RvX4njKyjY1O5OLWRfS6/qelM1p19Zur/G5WBGDqFaB0ZvXS9f2ZKpakJfWm7Iw7u/ui6aUeVkjQKA2BQS01ea6mhUBAgQIECBAgAABAgQIlEMgffp08tTRmDx5LFUiXDgzRFOWre3JV0Whrb0cR9QHAQIVFihOj93Kyja/zJts6aZYoSMFvbRvSiMV+FLh5dI9gQcKXLp+NY73X4jpMt4wX9feUcrk0uk1/YHuniBQSYH5lJXt3Mhg+je0qNLB5RqL8oTlktRPPQtkr8cn0uvySHp9zmPrbGtLGZ12x/r2zjwOz5gI5FZgZm42Tg1cjMGro7kcY2tTcxxK2dq2rNuQy/EZFAECKxMQ0LYyP3sTIECAAAECBAgQIECAQI0KZNnYxp5/NgW+XH/kDBtSyaK2x56K1l37HrmtDQgQWCOB4lzMjw1HcfJaeQbQ1JaytfVEQ/qqESCwegLZDfMskC0LaKtEyzK57NrWHbtTwHr2vUaAwOoIXBu7Gcf6z8X41NTqHHCBo2xI5QmzgBflCRfA8RCBhwgMXhmNk4MXIsucmueWvarv3Lo9ZWzrjSyQVSNA4OECI9euxomB8+kDJLMP3zAHz2YlxA/27oqspLhGgEDtCAhoq521NBMCBAgQIECAAAECBAgQKINAMb0JP3niozF15kTKylZcUo9NqdxBx1PPpOxNPvW9JDgbE6iwQHH6RgpOHYqYL/cb8Q3R0LElCu1bUrI2gS8VXkbdE4jBVFr0ZCoxuho3zDtaW0uBLRs6usgTIFBBgbn5uTg92B/9o5diab95V2ZQyhNWxlWvtSkwMT1VKkF4ZexGVU2wraUlDvftjk1d66pq3AZLYLUEpmayD5Ccj6yEcDW15lR69EDvzujeuLmahm2sBAg8REBA20NwPEWAAAECBAgQIECAAAEC9SUwm26kjR9JWdnGx5Y/8fQGWvuhJ6J1zwEBLstXtCeB8gikALYskC0LaKtoa2xJ2dp6o6FZ6eGKOuu8bgWyG+bHLp6LqymD02q2LEy1b8u22NedZXJpXM1DOxaBuhDIbpRnN8yzG+d5a8oT5m1FjCdPAsX0wa+LoyNxemgg5ufn8zS0JY2lZ9OWONCzI5rS3/AaAQK3BAbSB0iyEqOzKeC8WlsWrJoFrWbBqxoBAtUtIKCtutfP6AkQIECAAAECBAgQIECgDALFVD5h4uiRmD5/ugy93eqiccOm6Hj6mWjsWl+2PnVEgMDiBYpT11Iw23DKtLh6b8Q3tG9OGRq3pmBWJYwWv1K2JPBggdIN88vphvnw2t4wb21ujkN9u2LLug0PHqxnCBBYtEBWuuzkwIUYvnZl0fusxYZZUOuOVJ5wr/KEa8HvmDkVuDk5UQoyvzExntMRLm1YWXnCg+k1ftv6jUvb0dYEakxgrT5AUinGrKzwvu6+2JE+nKIRIFC9AgLaqnftjJwAAQIECBAgQIAAAQIEyiAwMzIYEx/5YMynN+bL3tIbaG37H4u2A4cFuJQdV4cEHiAwN5MC2QajOLOCTIsP6HpRDxeao7CuJ2VrU3p4UV42IvAAgTzeMN++cVMc7NkZzenmt0aAwPIEhq6OloLZZuZWL+B8eSN9aS/lCV+y8F39CswX5+Pc8FCcu5SyH6cMbbXWsqD1LHg9C2LXCNSTQHY9X0gfIDkz1B/zNXhtr+/ojMM7dkdna1s9Lau5EqgZAQFtNbOUJkKAAAECBAgQIECAAAECSxEozkzHxEc/HNOpzFGlW+O69dHxVMrWlrK2aQQIVE6gOHkl5sdGUla2tS991NC2MQqd6dPgDUoYVW7F9VyLAtkN87PDg3H+0nAub5g3N6ZMLr07Iwtu0wgQWLzA5PR0HOs/F1duVrgM+OKHtOQtezZtjv2pPGH2/wGNQD0JXEslv7Prd3xqqqan3ZTKi+/v3RG9qRSpRqAeBPL4AZJKuBcaGmL3tp70rzsa0vcaAQLVIyCgrXrWykgJECBAgAABAgQIECBAoEwCM4MXY/yFD0VxehXfkE9vmrXuPRhtB1+R4lsEuJRpKXVDoCRQnJtOWdkGImYqkGlxJcaFpih0pWxtLV0r6cW+BOpGoJpumG9OJcUP7dgVbc0tdbM+JkpgOQJZ5pf+0UtxOmV+mZtf+4Dz5czh7n1K5Ql7U3nCDcoT3u3i+9oUmJufi9OD/aVruPZysj14zTZ2dsXhvt3R3tr64I08Q6CKBWo94+KDlibL0nZ45+5Y3y6b+oOMPE4gbwIC2vK2IsZDgAABAgQIECBAgAABAhUTmJ+aLJUXnRlOgS9r1AodXSlb26ujafPWNRqBwxKoJYFizE+MRnHsUppUfm+zNbSuS9nauiNSgJtGgMD9AtkN81PphvlACnrJ75V8/7gbU2nxfd19sWNLysaoESBwn8DY5EQcvXgubkyM3/dctT+gPGG1r6DxP0rg8o1rcTxlM5+amXnUpjX5fJbRaW93b+zcsl1Gp5pc4fqdVDV9gKQSq5TlZ9uxdXvs3d4b2e/yGgEC+RYQ0Jbv9TE6AgQIECBAgAABAgQIECiTwPSFszFx9Pko5uQN+Zbd+6L98FPR0CTApUxLrJs6EyjOTt7Kyja7ipkWV2KcSo8WulKJk9b1K+nFvgRqTqAWbpiv7+iMwzt2R5b1QSNAIGI+ZWU7N5JKB48Mlb6vVZPsRnhWgrTPB1VqdYnrcl4zs7NxYvBCDF+9Upfzf/mku9raS6/x69o7Xv6UnwlUlUC9Zlx80CK1tbSUMjFu6lr3oE08ToBADgQEtOVgEQyBAAECBAgQIECAAAECBConMJ8yQowfeS5mLw9X7iDL7LmQ3hxvf/LV0bwtZW7SCBBYnEC6ST4/kbI4jY+m7aspl9Ot6TW0dJbKkEaheXHztRWBGhWYTjfMTw6kG+bXauOGeZbJZfe2nvQvBa6m7zUC9SpwbfxmHEtZ2canqiTgvAwLteFjQa0dglrLoKmLtRQYujpaem2emZtby2Hk7tjZ6/qulNFpT3qdL8jolLv1MaBHC4zeuB7H+s/VbcbFhwn1bNoSB1JwelNj48M28xwBAmskIKBtjeAdlgABAgQIECBAgAABAgQqLJCCXqbOnYqJYy9EzM1W+GAr676lb3e0v+LpaGhuWVlH9iZQ4wLFmYlbWdnmpqt7pg2FVII0lS9q21jd8zB6AssUqOUb5lmWtixbW5a1TSNQTwKlzC9DA9F/eaQKw81XvlJZUOueVL4sC3oR1LpyTz2srsDk9HQqL3ouRm/eWN0DV9nR2lta02v8rtjYKaNTlS1d3Q53Jr0Xln2AZEjGxYeeAy2pcsKhvl2xdb2/zx8K5UkCayAgoG0N0B2SAAECBAgQIECAAAECBCorMDd2I8affzbm0ifMq6U1pDfHO574uGhOnwzVCBB4mUBxPubH0g3yydrI5HRnds3tKVtbbzQ0Cma9Y+KbmhbIbphn2SGu1PgN8yw/244t22Nvd29kJQk1ArUuUAulg8u1Rp0pA/NjKahVecJyieqn0gIXUxDq6aH+mJufr/Shaqb/3lRmeH93n4xONbOitTmRLAvyiRTMlpUR1hYnkAW0HerbGS1NsqkvTsxWBCovIKCt8saOQIAAAQIECBAgQIAAAQKrJZCysk2ePh6TJz4aUaVvyDenN8bbU2BbQcmi1TprHCfnAsXpsZSVbTBd0zM5H+kyh5cyuhQ6tkVD+6bUgTKFy1S0WxUI1OMN87aUeTXL5LKpa30VrJAhEli6QHaTPLtZXiulg5cusPAe2av5zqw8YcrYJqh1YSOPrr3A2ORkKcj8+vjY2g+mCkfQmgJesoxOW9ZvqMLRG3ItC0zNZBkXz8flVGZUW7pAVno0K0GalSLVCBBYewEBbWu/BkZAgAABAgQIECBAgAABAmUQmLt+NcaPPBfZ12pvWenR9sefjpaU3UEjULcCxbmUlW04ZWW7Vh8ETW0pW1tPNKSvGoFaEhibnIhjF8/F9YnxWprWkubSs3Fz7O/dEc2NTUvaz8YE8ixQy6WDy+Xe1pKCWvt2p6BW5QnLZaqflQsU04fAzo0MpX+DMZ++11YmsC1ldDooo9PKEO1dNoH+0UtxavCijItlEN2USgtnH0xpS9UUNAIE1k5AQNva2TsyAQIECBAgQIAAAQIECJRDIGVimzzxYsrMdiyixt6Qb0qZHTqefHUU2jvKIaUPAlUjUJy+kbKyDaWsbPVWHqUhGjq2pGs+fRo8ZW7TCFSzQHaTPLtZfj7dNHfDPFLpoqY42Lsztm3IsjFqBKpXICsdfDyVDh6t8dLB5VyhLMtLlu0ly/qiEVhLgSwbWxZkPjY1uZbDqLljy+hUc0tadRMaT9f0sYvn49r4zaobe54HnGVZ3dvdGzs2p4zq/j7P81IZWw0LCGir4cU1NQIECBAgQIAAAQIECNS6wOzV0Rh//tmUxelG7U41ZXNpP/xktO7ZX7tzNDMCtwVSAFsWyJYFtNV1a2xJ2dp6o6G5va4ZTL56BbIb5kfTDfPs5pp2r8CWdRtKJcpam5vvfcJPBKpAoB5LB5drWW4Fte5KQa0by9WlfggsWmAufQjszFB/ZNewnGyLZlvyhllGp0Mpo1O7jE5LtrPD8gSyjIvnLw3H2eEBHyBZHuGi9lqXPmT6WKqg0Nnm7/NFgdmIQBkFBLSVEVNXBAgQIECAAAECBAgQILA6AsW5uZg89pGYOneq5rKyPUiwKWV26HjqmSh0dj1oE48TqGqB4tS1FMw2nK7puaqeRzkH39C+OQodW1O2tkI5u9UXgYoJzM3Pxemhgeh3w/yhxlm2h/0pW1Pf5nR9awSqQEDp4PItkqDW8lnqaXECozevx/GUuWlyZnpxO9hqRQKF9Bq/b3vK6LRFRqcVQdr5kQI3JsZLGRdvTk48clsbrFygkDK07drWHbu39UT2vUaAwOoICGhbHWdHIUCAAAECBAgQIECAAIEyCcxeHo7xI8/FfHrzru5aoTHaDj4ebfsOKUdYd4tfwxOem0mBbINRnBmr4UmuYGqF5iis60nZ2jpX0IldCVReYPTG9TjWfz6m3DBfNPaGjq44nDK5dLS2LXofGxJYTQGlgyuj3ZR+p9/f0xe9glorA6zXksDM3GycHLgYQymrubb6AllGp8Mpo1OXjE6rj1/jR5xPGRfPjgyWMrNlGdq01RXIfm/PsrWt7/D3+erKO1q9Cghoq9eVN28CBAgQIECAAAECBAhUmUBxZiYmjj4f0xfOVtnIyz/cxvUbo+PpZ6IxlS3TCFSzQHHiSsyPj6SsbPPVPI1VGXtD28aUoXFbCmZtXJXjOQiBxQq4Yb5YqYW3yzI87EmZXHZt3R4Nsj0sjOTRNRFQOrjy7IJaK29cr0cYuXYlTgxciOnZ2XolyMW8s9f13VtTRqft3Smjk4zLuViUKh/E1bGbpaxsE9NTVT6T6h5+lp+tL2Vh3NfdF1nmZY0AgcoJCGirnK2eCRAgQIAAAQIECBAgQKBMAjPDAzH+kQ9GcWqyTD3WQDfpzfG2/Yej7cDjEd5Aq4EFra8pFOemU1a2gYgZ5VGWtPKFpih0pWxtLUoPL8nNxhUTGL6abpgPXogZN8xXbJxlcMkyuWQZXTQCaymgdPDq6gtqXV3vWj9aliX1eMqWejllTdXyI9DR2hqH+3bHhk6/w+dnVaprJLNzc3F6qD8GRi+FnGz5Wbu25pY4lLItb+5an59BGQmBGhMQ0FZjC2o6BAgQIECAAAECBAgQqCWBYvrU6fhHPxwz6dPl2sICha510fHUM9G0cfPCG3iUQK4Eiikj22gUxy+lUXkrfrlL09C6LmVr607BrE3L7cJ+BFYkkN0wz8qLZmVGtfIJZJlcdqZsD3tTxraCYPXywepp0QJKBy+aquwbCmotO2ndddifAl1ODV6MuVSOUMufQJbRKSsznJUbbkxlhzUCixW4fONaKVB1KlUt0PIp0JPej9vfuyOaG/19ns8VMqpqFhDQVs2rZ+wECBAgQIAAAQIECBCoYYHpdKN8IgWzFdNNc+0RAukGeOueA9F26IlUjdCb44/Q8vQaCRRnJ1NWtsGI9FUrg0AqPVro6o6GVp8GL4OmLpYg0D86km6Y97thvgSzpW7a3tJSyuSyMQWtawRWQyDLsphlW8yyLmprJyCode3sq/nI4ymL+bGL5+La+Fg1T6Nuxt7a3ByH+nbFlnUb6mbOJro8gdJrc/pw53AqIazlX6ClqSkO9u6KbRs25n+wRkigigQEtFXRYhkqAQIECBAgQIAAAQIE6kFgfnKiVF50diQFvmhLEii0d6Zsba+OppTdRSOQG4Fiyso2kUqjpMxssrKVf1UaWjpLZUij0Fz+zvVI4C4BN8zvwlilb3s3bUmZXHZEk2D1VRKvz8MMXR2NkwMXY2Zutj4Bcjjrto8FtW4S1JrD1cnPkIrpd+zzl4bj7PBAzKfvteoS2L5hUwp+2RnNKQhGI/BygVuvzRfSa/Pcy5/yc84FsmDVLGg1C17VCBBYuYCAtpUb6oEAAQIECBAgQIAAAQIEyiQwdf50TB49EsWUJUJbvkDLzr3R/vhT0dDkDbTlK9qzHALFmYmUlW0gYk6mxXJ4PrCPhkIqQbo9Gtp8GvyBRp5YtsCtG+ZD6Yb5oBvmy1Zc/o4t6bX8UN/O2Lre9b18RXsuJDA5PV0qYTZ6U+nghXzy8FhPCmo9IKg1D0uRuzHcmBiPoykr21j6MJhWvQLNKWD9QApq607lCjUCmcBkqlBw/OL58Npc3edDUyornJUgzT6cohEgsDIBAW0r87M3AQIECBAgQIAAAQIECJRBYD6VRxk/8mzMjl4qQ2+6yAQaWtui48lXRfP2XiAEVl+gOB/zYyNRnFQeZVXxm9ujsStd840tq3pYB6tdgesTY6UyZmOTSgWv9SpvXX8r20MW4KYRWKnAxcsjcXpI6eCVOq7G/qUSZinTyzZBravBnftjzM/Px5mUke1CuoazgHOtNgQ2p2yMh/p2R5adUatfAa/Ntbf2Gzu74vCO3dHe0lp7kzMjAqskIKBtlaAdhgABAgQIECBAgAABAgQWEEhvwk+dPRkTx19IGZyUUlhAaMUPNadPfHe84pXR4A20FVvqYHECxemxlJUtlQyen1ncDrYqr0BDQzR0bItC+6bUb0N5+9Zb3QjMfeyG+cVUyszt8vwse1Z6NCtBKttDftak2kaSBace6z8X19OHSbTqElDCrLrWqxKjvXLzRun6zbIrarUn0FgoxL7uvtixZVvtTc6MHiowPjVZyrjotfmhTFX7ZCFd23vTB013pmu7If2trhEgsDQBAW1L87I1AQIECBAgQIAAAQIECJRJYC6VNxp//tmYuyaDU5lIH9hNQ/qkd/srPi5aUnCbRqBiAsW5lJUtBb9MXqvYIXS8BIGmtih09aTSw21L2MmmBCLcMM//WSDbQ/7XKG8jzDI5nRsZTP+GlA7O2+IsYTylEmY9fdG7eesS9rJptQvMpg9+nRy8GINXLlf7VIx/EQLrOzrjcMrW1tnmd/hFcFX1Jtlr8/lLQ3F2eNBrc1Wv5OIGv669o5StrautfXE72IoAgZKAgDYnAgECBAgQIECAAAECBAisrkAqRTh58lhMnjqaMjjNr+6x6/xozdt7ov2JV0XBG2h1fiaUf/rF6RspK9tQuqZny9+5HlcgkGVr25yytaUb3z4NvgLH+tj11g3zC+mG+Wh9TLjKZynbQ5Uv4CoOP8v4cvTiucgywGi1IbAhlTB7LAW8tLcqYVYbK/rgWVy6fjWO95+P6Vm/Yz9YqfaeKaTf23dv60n/umV0qr3lLc3oxsR46bV5bHKiRmdoWgsJZBnadm/tjt3pvbnsOtcIEHi0gIC2RxvZggABAgQIECBAgAABAgTKJJBlYxs/krKy3bheph51s1SBhqbmaH/sqWjZtXepu9qewP0CKYAtC2TLAtq0HAs0tqRsbb3R0OzT4DlepTUd2si1q3FiwA3zNV2EZR5ctodlwtXBbnPzc3F6aCD6L48oHVyD653dCN+TSpjt2rpdwEsNru/07EwpkO3SdZmPa3B5Fz2lzta2UkanLGubVhsC8+lDnWeGB+JC9tqcMrRp9SnQkQLSD+/YHRs6uuoTwKwJLEFAQNsSsGxKgAABAgQIECBAgAABAssTKKYyKZMnPhpTZ05EetdueZ3Yq6wCTVu2RceTr46CN8fL6lpPnRWnrqVgtuF0Tc/V07Sreq4N7ZvSNb8tZWsrVPU8DL58AlMzt26YX77hhnn5VFe/pyzbQxbUsqeU7cH1vforkL8jjqYPjxxLWZ2mZqbzNzgjKqtAVrosuymeBbdqtSEwkEqLnkolRrPMqRqBLIdTX/rbfV93XzQWvMZX8xlxdexGHEsZUyemvTZX8zqWa+ylazuVEN+XSok3FhrL1a1+CNScgIC2mltSEyJAgAABAgQIECBAgEC+BGavXIrx55+L+fGb+RqY0UQ0Nkb7oSeidc8B5QidD4sXmJtJgWyDUZwZW/w+tsyPQKE5Cut6UrY2mR7ysyhrM5KB0Uvphnl/zKYsTlptCLS3tMZjWbaHVI5Qq0+BmVSW8OTghRi6eqU+Aep01llQ684U8LI3ZWzLyhFr1SkwMT1VCna5Oubv5upcwcqOuq25JQ7t2BWbu9ZX9kB6L7tAFpyaBalmwaoagZcLtKZr+3BfurbXubZfbuNnApmAgDbnAQECBAgQIECAAAECBAhURKCYbqhNHDsS0+dOV6R/nZZPoHHj5uh46plo7FpXvk71VJMCxYkrKTh1JGVlm6/J+dXTpBraNkShc3t6d9Cnwetp3bO5TkylG+b958IN89pc+SzbQ2+W7SFlcmlKgeta/QgMpyC2EwMXYmZutn4mbab3CLS3ZDfFd8dGv9Pf45L3H7KygxcuD8eZVCJ4XjbzvC/Xmo+vO/3tfqB3RzQ3Nq35WAzg0QKXrl+NE/0XYiqVEdYIPEyge+OmdG3vdG0/DMlzdSkgoK0ul92kCRAgQIAAAQIECBAgUFmBmZGhmPhIyso2OVHZA+m9fAIpm0Pbgcejbf8h5QjLp1ozPRXnplNWtoGIGdd0zSxqNpFCUxS6uqOhRTBrTa3rAyaT3TA/f2k4zg67Yf4Aopp6uLW5OQ717oot6zfU1LxM5n6ByVRW9PjF8zF68/r9T3qkLgV6Nm2JAz07BLVWwerfTH8vH714Nm5O+B27CpYrN0NsaWoqBb5s37ApN2MykHsFplMAWxZkPnLt6r1P+InAQwSa07V9MAW1ubYfguSpuhMQ0FZ3S27CBAgQIECAAAECBAgQqJxAMd1Qm3jx+Zi+eK5yB9FzRQUa122IjqdTtrb1Gyt6HJ1Xi0AxZWQbjeL4pTTgYrUM2jiXKNDQui5la+suBbgtcVebV4nAjYnxUhmz7Ma5Vl8C2Q2xLNtDdvNbqz2Bi5dH4vRQf8zNy5xae6u7shll1/yhVMJsq9/pVwZZob3nU7bjs8ODpUDzLOBcI7AcgS2pRGF2nWclC7X8CAxeGU0lRrOMqXP5GZSRVJWAa7uqlstgKywgoK3CwLonQIAAAQIECBAgQIBAvQjMDF6M8Y9+KIqplJlW5QINDdG671C0HXw8GgrKlVX5ai57+MXZyZSVbTAifdXqQCCVHi10bY+GVtmcamm151OQy5l0wzwrZeaGeS2t7NLm0pxKj+7v2Rk9mzYvbUdb51ZgbGqyFKR6fXwst2M0sHwIbE1ZGrOAl5am5nwMyChKJb+PpQ+ATUz7u9npsHKBxpRpfX/KyNiXyo1rayswOT0dx/rPxZWbN9Z2II5eEwKu7ZpYRpMog4CAtjIg6oIAAQIECBAgQIAAAQL1LDCfbqhNvPChmEnZIbTaEih0dkXHU89EUypbpNWRQMoSMZ8yshUnRtOkZYyoo5UvTbWhpTMFtvWkbG1ufFf72l8du5ECXs67YV7tC1nG8W/qWheH+3ZHW4tMLmVkXdWussDUcyND6d9gzMvqtKr21XywplJQ647o9Tv9mi7jbMrWdCr9zTw4mn7PXtOROHgtCmzo6IzDO3ZHR2tbLU4v93PKPjxyZmhAxtTcr1T1DXBDel/ucApMd21X39oZcXkEBLSVx1EvBAgQIECAAAECBAgQqEuBrLRoVmI0KzWq1a5A6+790fbYk9HQqFxZ7a7yrZkVZyZSVraBiDnXdK2v9UPn11BIJUi3RUPbpodu5sl8CpRumKesqQNXLudzgEa1pgJZtoe93b2xY3O6xlNGVq16BLJsbFlWpyw7m0ZgOQIbSzfFd0d7a+tydrfPCgQuXb8WJwbOx9TMzAp6sSuBhwsU0uv6nu09sWtrt9f4h1OV7dmxyZQxNWVlkzG1bKQ6WkDg1rXdm67tlFHd7+8LCHmolgUEtNXy6pobAQIECBAgQIAAAQIEKiQwPzEe4x95LmYvDVfoCLrNm0ChvSM6nnxVNKU3x7UaFCjOx/zYSBQnr9Tg5Exp2QLN7dHY1RvRKJvTsg1XecdL16/Gif4LMTXrhvkq01fd4dal1/XHUiaXzrb2qht7vQ14LpUOPp2yOvVfTq/T9TZ58y27gJviZSd9aIfTs7OlQLaRa1cfup0nCZRTIHttz17js9d6rTICMqZWxlWvDxfo+ti13eXafjiUZ2tKQEBbTS2nyRAgQIAAAQIECBAgQKDyAlPnTsXE0Y+kDE6zlT+YI+ROoCW9Md7++CujoVk5wtwtzjIHVJweS1nZBiPmBcAsk7C2d0ufAG/o2BaF9ixbm2xOeV3s6RTAlgWyjaSANo3AYgWywJZd27pj97aeyL7X8icweuN6HO8/H5OyIedvcap8RNlN8aw8oYCXyi3k4JXRODV4IWZSqVGNwGoLZFmcdm7ZFnu390YhZWfVyicgY2r5LPW0dIHs2s4ytWXZGAsps7pGoNYFBLTV+gqbHwECBAgQIECAAAECBMokMD92M8aPPBuzSpiVSbR6u2lobYuOJz4umrv7qncSRh5RnEuBbMNRnLpGg8CjBZraotDVEw3pq5YvgcH0unwylRjNSo1qBJYj0JFe17NMLus7Opezu30qIDCTPjhycuBiDF0drUDvuiRwS0DAS2XOhMnpqVSC8HxcuXmjMgfQK4ElCLS1tMThvt2xqWvdEvay6UICWcbUM0MDcfFy+ht6oQ08RmAVBdpbWku/v29I5cQ1ArUsIKCtllfX3AgQIECAAAECBAgQIFAOgWIxJk8fj8kTL6YMTm6Wl4O0Vvpo7tlRCmxrSG+kadUlUJy6kUqMDqVrWqbF6lq5tR5tlq1tc8rWtjUla5PNaa1XYyLdMD9+Md0wH3PDfK3XohaOn13RfZu3xr6evmgsNNbClKp2DsNXr8SJLKtTKlWoEVgNgeym+OEdu2Jjp4CXlXhnJQgvptLAZ4YHIgt80QjkSaBn05Y4kP5+b2r0Gr+cdckCVI/1n4vJ6enl7G4fAhURyH5/702/v+/3+3tFfHWaDwEBbflYB6MgQIAAAQIECBAgQIBALgXmblyL8eefjTklzHK5PnkYVENzSypB+nRkpUi1KhBIAWzzN4eiOC0ApgpWK79DbGxJ2dp6U+nh9vyOsYZHdvuG+el0w3zeDfMaXum1mVprel0/3LcrNq9bvzYDqOOjTqWyollWp6zMqEZgLQR6U8DLfgEvy6Ifm5yIoxfPxY2J8WXtbycCqyHQ0tQUB9Nr/Lb1G1fjcDVxjCwD8skUZJ6VENYI5FWgtbk5DqVre8u6DXkdonERWLaAgLZl09mRAAECBAgQIECAAAECNSyQbpBPnnwxJk8dT2UJfbq8hle6bFNr2todHU+9KgptHWXrU0flFShOXktZ2YZLpUbL27Pe6lWgoX1TFDq2pWxthXolWPV530w3zI+5Yb7q7vV4wO0bN8XBnp3RnG5+a5UXyLI6nR7ql9Wp8tSO8AiBlqbspvjO2Crg5RFSt56eT1nZzg0PxvlLQ5F9rxGoBoGt6zeUgl+y6117sMBI+mDniRRoPi1j6oORPJMrge0b0u/vvX5/z9WiGMyKBQS0rZhQBwQIECBAgAABAgQIEKgtgdmrozF+5NmUxUkGp9pa2VWYTbrp3X74yWjdvX8VDuYQixaYm0nX82AUZ8YWvYsNCSxaoNAchXU9KVtb56J3seHSBeZTcPnZ0g3z4cgytGkEVkOguTFlckk3xbLgNq0yAuNTk6WsTtfHvUZXRlivyxUQ8PJouWvjN1OQ+fnIrmONQLUJZKVHs4yMWWZG7V6B6dmZOJ4C2S5dv3bvE34iUAUC2e/vB3p3RPfGzVUwWkMk8GgBAW2PNrIFAQIECBAgQIAAAQIE6kKgmEopTB5/IabOnkwZnNwsr4tFr9AkmzZvTdnaXp0yN3VV6Ai6XaxAceJKzI+PyLS4WDDbLVug2df/vAAANQZJREFUoW1DFDq3p2xtjcvuw44LC1wbSzfM+8+lG+ZTC2/gUQIVFtjctT4O79gVWTlSrTwCWWDquZGh9G9QVqfykOqlAgICXhZGnZufi9OD/dE/ein81bywkUerR2BjZ1d6jd8d7S2t1TPoCo508MrlVGL0YmSlRjUC1Szg9/dqXj1jv1tAQNvdGr4nQIAAAQIECBAgQIBAnQrMpjJH4x95LgW+yA5Rp6dA+addaIz2Q6+I1r0HU4BLQ/n71+NDBYpz0ykr20DEzMRDt/MkgbIKFJqi0NUdDS3rytptvXaW3TA/lW6YD7hhXq+nQK7m3VgoxL7uvtixJZUZ1lYkkGVjy0oHj8nqtCJHO6+egICXl6xHb1xPQebnY2pm+qUHfUegygUK6e/1vd29sXPL9vSne33+7T4xPRXHU8bFK2MqFVT56Wz4dwn4/f0uDN9WrYCAtqpdOgMnQIAAAQIECBAgQIDAygWKqZTCxNEjMX3+zMo70wOBBQQaN2xK2dqeicZ16xd41kPlFyimwNTRKI5fSl3LGVF+Xz0uRqChdV3K1tYdkQLctOUJXL5xrVTqaGpmZnkd2ItAhQTWd3TGYymTS0drW4WOULvdzs3Px5mh/riYPkjiFbp217lWZ1bvAS8zs7NxYuBCDF+7UqtLbF4Eoqu9Pb3G74mutva60cgypmavy6eHB2I+vU5rBGpRYEP6/T3LxOj391pc3dqfk4C22l9jMyRAgAABAgQIECBAgMCCAjPDgzH+wgejOCmD04JAHiyfQEMh2g4cjrb9j6UAl0L5+tXTPQLF2cmUlW0wIn3VCKy5QCo9WuhKWR5aN6z5UKppAG6YV9Nq1e9Ys8CW3dt60r+UkbFOM7ksdfVHb14vZX6ZlNVpqXS2z5lAKeClb3cKfOnI2cgqN5yhq6NxcuBizMzNVu4geiaQE4HsdX3X1u2xJ73OF2r8b/ex9F7Y0ZQx9cbEeE70DYNA5QSy39/3bO9J17ff3yunrOdKCAhoq4SqPgkQIECAAAECBAgQIJBjgeL0dIx/9EMxkz5hrhFYTYFC1/pStramjZtW87C1f6z0qfL5lJGtODGa5irnS+0veHXNsKGlMwW29aRg1ubqGvgajPbWDfML6Yb53Boc3SEJLF2gM2VpO7xzd6xv71z6znWyRxYAkwXCZNe3RqBWBLKAl6w04d50Y7yWA16yANSsBGEWkKoRqDeB9pbWUkanrORwrbX59PfzufQBz/OXhiL7XiNQTwJZBsYsW9u6OgpMr6f1rcW5CmirxVU1JwIECBAgQIAAAQIECDxAYDoFsU2kYLYsqE0jsCYC6QZY654D0XboiWhobFyTIdTSQYszEykr20DEnGu6lta15uaSsjQWOrdFQ5tg1oXWdjK9Jh/vP5dumN9Y6GmPEci1QEMa3Y4ssKW7NxprPJPLUhciK014Mv3uPZ1KFWoEalHgVsDLrtjYua7mplcqQZhKBGelgjUC9SqQvcb3bNoS+3t2RFON/O1+fXyslJVtfEpW83o9r807ShmWd27ZlgLTe2s6MN1a14aAgLbaWEezIECAAAECBAgQIECAwEMF5lMphYlUXjQrM6oRyINAoaPzVra2zVvzMJzqG0NxPubHRlLJ4CvVN3Yjrl+B5vZo7OqNaGypX4OXzfzC5eE4MzTghvnLXPxYfQJtLS1xOJUh3NRVe4EtS12NqSyrU//5uHxDVqel2tm+OgV6ayjgJQtyyUoQZkEvGgECtwRam5vjYO+u2Lp+Q9WSZMGpp1OQav/l9Dd01c7CwAmUV6CWA9PLK6W3tRQQ0LaW+o5NgAABAgQIECBAgACBVRCYvnAmJl48EsXZmVU4mkMQWJpAy6690f7Y09HQ1LS0Het46+L0WMrKloJT513TdXwaVO/UU5bGho6tUWjfnOaQ5X2ozzY2ORnHUlY2N8zrc/1redbdGzfHgd4d0dxYn6/r/aMjcWpQVqdaPsfNbWGB1qYU8NK3MwW8bFx4g5w/WsxKEI4MpX+DShDmfK0Mb+0Etm3YmALbdkZLut6rqWVlg7PywVkZYY0AgfsFaikw/f7ZeaTaBQS0VfsKGj8BAgQIECBAgAABAgQeIDCfPlU+/pHnYjZ9AlUjkGeBQlt7tD/5qmje1pPnYa792IpzKZBtOIpT19Z+LEZAYKUCTW1RSNnaGppaV9pTVe2f3TA/m26Wn083zefT9xqBWhRoSUHq2Q3vbRvqp8xwltXpWMrqdE1Wp1o8pc1pCQLbUkBbFthWTQEvWXB5dv2OKUG4hJVe/U2Ld5d/zT4gkf6tVbtnLLcHscZjuj2MSn9tTqVHsxKkWSnSvLeZudlU+vtiDF0dzftQ63p891xPa3wd3TOW26uyxmO6PYxKf70VmF7dmRgrbaT/tREQ0LY27o5KgAABAgQIECBAgACBygmkG+RTZ0/GxPEXIubmKnccPRMos0BL365of8Uro6FZOcKX0xanbqQSo0MpK9vsy5/yM4EqFsiytW1O2dpS6eE1vCm5WoDZDfOsjFkW+KIRqAeBLes2xKH02p6VKqvVJqtTra6sea1EoOljAS9Zxpc8t6wE4ZlUgvCiEoR5Xqb46PNH4ru/+dvi0vDwnXE2pdeVd/7Ld8Vnf/7fvfPYanzz4pGPxHd907feM5bbx20oFOINX/Pm+OpveNvth2r6a1Zi/HB6jW9ryeeHU0auXYkTAxdietbfz3k9EV3b+VyZW5kYd6XA9PrMtpzPVanvUQloq+/1N3sCBAgQIECAAAECBGpMYO7mjRg/8mzM+QRqja1s/UynIb0hngW1taTMLloSSAFs8zeHojh9AweB2hVobLmVra25vSbnmN0wP51umPe7YV6T62tSDxdoKjTGvp6+6NucAldrrF2f+FhWp1RCWCNA4H6BjZ1dcXjH7mjPacBLlrXpxQtn7x+4R3Il8Dv/5b/Gj/6Ld903pjd/w9fFG976lvser+QDv/Mbvxk/+r3vfuAhPu2zPyu+/8d/7IHP19oTPanM+GM79+RuWlmw+fuPHokZwWy5W5u7B+TavlsjX99nmZZ3bNmWr0EZTd0KCGir26U3cQIECBAgQIAAAQIEakqgOB+Tp47H5MkXUwDMfE1NzWTqU6B5e2+pDGmhta0+AdKsi5PXUla2lIkglRrVCNSDQEP7pih0pDfOGwo1M93RG9fjeP/5mJyZrpk5mQiB5QhsyAJbUiaXjhp4XZfVaTlnwOrvc0/ZsDUuF3bPWG5TrPGYbg+j0l8LKWvV3u09sXPL9jUtEbnQPOfm5+L9Lx6J7JrW8iswPTUdv/9bvx2XR0ZSZrSR+O1f/y+lwa5FQNvU1FT8wW/9Tly+dClmpmfuoP3Sz/3H9DbMfNRbQNsr9x6MLFNbHtvJlJ3tQvowiZZfAdd2PtcmK+f8yY89WVWlw/MpaVTlEhDQVi5J/RAgQIAAAQIECBAgQGCNBOauX43x51NWthvX1mgEDkugMgINqZRM+2NPR0sOP/VdmRl/rNe5mZSVbTCKM2MVPYzOCeRSoNAchXU9qfRwZy6Ht9hBzczNRnYjbejqlcXuYjsCNS9QSDfI9qSA9V1b8xfYslj8Kzevx7EsSHVakOpizVZ7OyXMVlt8ccfram+Px3bsia62fGVjzTK0ZZnatOoQOHPiZLzpdf+oNNg3f+PXxxu+9s25GPjn/R+fnALcpuPTP+ez4t3/pj4ytLU2NccnpaCXLPglj+3mxHj87cmjeRyaMS0g4NpeAGWNHtqybn08tefAGh3dYQncLyCg7X4TjxAgQIAAAQIECBAgQKAqBIrpE+WTJ16MqdPHUwanYlWM2SAJLEegKWV06Hjq1VFo71jO7lW1T3HiSsyPp0+Sp6yLGoF6Fmho2xCFzu0pW1tj1TEMpyC2E4MXlDmqupUz4NUSyAJasjKE66rsdf36+Fg8d+rYajE5zjIFlDBbJtwq7JbHrC9Xbt6ID585sQqzd4hyCAh6KYdiefrYva079nX3laezCvXy18dfiPGUVU/Lv4BrOz9r9MSufbFtw8b8DMhI6l5AQFvdnwIACBAgQIAAAQIECBCoRoHZK5dj/MizqRzhzWocvjETWLpAY1O0H34iWnfvTwEu+fwU+NIn9dIexbnplJVtIGJm4qUHfUeg3gUKTVHo6o6GlnyWMnr58kylsqJZedHLqcyoll+Be0r/pdeTtcwscs9YbpOt8ZhuD6PSXzP3nVu2pVKEvZGVJKyGVkwfIHn/i8/HzJxS4HleLyXM8rs661MQ66sPPJarAWbX9QeOfiSmZl8qH5mrARrMPQKCXu7hWNMfPv7g49GZs4yLLwc5f2koTg32v/xhP+dQwLWdj0VpTL+Tv+bxp6vmd/N8qBlFpQUEtFVaWP8ECBAgQIAAAQIECBAoo0AxlTCbzN5wP3eqjL3qikD1CDRu3BwdTz8TjZ3VEeDyaNliysg2GsXxS2lTmRYf7WWLehRoaF2XsrV1R6QAt7y2/tGR0g2zuXnZFfO6RsoQ5nNl2ltaU7a2XbGxSl7XT6RSwhcvp0yqWlUIuEGer2U61Lcr+jZvzdeg0mhOD/XHuZGh3I1rKQPKyl0ef/FozMzcCszr6e2N7r7e+MiHPhwf+PP3xcDFi/HEK5+O13zmZ0R3b0+p6+z6+Jv3fyCOfuSF2NbTHa/+hI+PT/jUT1nUYedSYO+Fs+fi7KnTcfbkqbg0MhJ9u3bG3gP7Y8/+fekYvcsOGJ9Pv0udO30mptOc9h08EM3NzXfGtNxr+vY4z5w6FedPn42u9V1pnPtL4338qSejLZXEXUmrt5KjWYbVZ3IWnLrQ+mUfNskCVqv5r2zX9kIr+9Jjru2XLMrxXe+mLaUsyuXoSx8EyiUgoK1ckvohQIAAAQIECBAgQIBAhQVmLw3H+Eeei/mJ8QofSfcEci6QPjXalj4R3rbvcFVnayvOTqasbIMR6auWX4HsptrtlmUUWstsTnePJS9juj2Oin9NpUcLXdujoXVDxQ+11AMcOXtSVraloq3B9soQrgH6Eg55oGdH7NyaygznvN1Iv4c/e/JozkdpeLcFlhv8cnv/Sn2tt+CXzLGQfof65MefiuaUdTlvbWxyIv7mxIt5G9aSxvPGL/qHpSCw2zt1dHbEF3/Z6+OXf/4XIstCd7tt3b49fv43fiX+9i8/EN//7d8ZWWDa3e31X/WGeNu3vePuh+77/n1//Cfxb3/oR2OoP2WXfkDLgufe8V3fEYde8fgDtrj34Sxj6a+995fiD3/nd+PMyZORZVrMWlMKZtufgto+/XM+O77ya746zqUAuje97h+VnnvzN359vOFr31z6/kH/OX/2bPw/7/7BePYDf/WgTSIz+cZv/7b4jM/73Adu86gn6u2aPti7M3akLKvV0LKSwllp4Wptru2FV861vbDLSh991b5DsaGza6Xd2J9AWQUEtJWVU2cECBAgQIAAAQIECBAov0Axfcp6IpU3mr54tvyd65FAFQs0rt8QHU+lbG3rN1bXLNJNpfmUka04MZrG/dINpuqaRO2P9q+f/XB86ZveHhcHXsrY0dLSHP/xJ38oXv+6L1hVgL957vn4kq/6xnvGcnsAWam+d77jrfG93/722w/V9NeGls4U2JYyixReytax1hPOyoz2j2ZZFrU8CyhDmOfViXhi177YtqE6Xs//+vgLMT41lW9QoysJCGjLz4mwNf2+/uTuffkZ0MtGkgWqZgGr1dq+9vVfGcde+Oiihr//0ME4nbKqLVj2OvXw73/1l+LwAoFol4ZH4sfe9f3x/j/983uO07VuXWzr7o7+8+dj6q7/N2a/o37xl/3j+Kff8s3R0tpyzz53/3Dx3Pn4we/6F3HkuQ/e/fB9378qZZB741vfEt/yln9aeu5RAW2/8NM/E+/9Dz8fsx/LWpd9KGXLtm2xI2WSu3H9epxPGeay7Fe32yd+2mvie//VD0dHZ+fthxb9tZ4C2jLHT37sqWhpyl9w6kILNnR1NF68UL3vpbm2719V1/b9JuV4pK25JT7psSfL0ZU+CJRVQEBbWTl1RoAAAQIECBAgQIAAgfIKzKTyJ+MvfCiKUzI4lVe2fL3N3/WJ94bU7Zpmb7prLLdnuNZjuj2Oin1Nb6i3pk+Rth98RQpwKVTsMOXseH5s+GPBbOXsVV/lFvj5//wb8bXf/F33dft93/H2+M5vedt9j1fygZ9776/HW9/x3Q88xD/4gs+N3/hPP/HA52vuicaWaNy0PzfTuj4+Fs+dOpab8RjIowUEuTzaaDW3aGpsjE9JmZsKDdXxOn7+0lCpxPBqGpX7WEqYPVxUCbOH+yzn2Sd374+t6cMoeW1ZKeGspHC1tiyL78Vz5+L//bEfj/f9yZ+WppGV0cyypGWBWu/7oz+Jn/vJn44rly/fmWIW2Pbt//JdKcBrV/zaL743siCRrH3RP/7S+Jbvfued7bJvsv7f/qa33Ak6a0rBTF/5lq+O137J62J7KleatSxALgsSe8/P/Gz8we/8j9Jj2X/+4Vd8Wbz9O/7vOz/f/U3/+Qvx5i/9spgYvxVM2NraGp/2OZ8VBw4fis1bt5RKmj7/3IfuHLe1rS2mJm+9N/KwgLbf/vX/Ev/q+76/dKjG9Brz+a/7BykY7mvujDV7YnZ2Nv7rL/9qad43b9zK4PV5r/2C+M4furXf3eN81Pf1FNC2Zd2GeGpPfn4Pf9TazM3PxV+8eKR0Dj9q2zw+79q+d1Vc2/d6lPOnPdt7Yu/23nJ2qS8CZREQ0FYWRp0QIECAAAECBAgQIECgvALF6alSINvM4MXydqy3sgn87dHj8YZ3/3AMXM6ybN1q2aeUf+rb3h5f8hmfdvuhVfn67LET8U/e9UP3jOX2gbPyPt/65V8a73zDl99+qCa/FjrXRcfTz0TTxs25n19xZjzmr53L/TjrfYCTKcPEe37lv8XA0Ej0pyxtP/ueXyuRrEVA20S6cfeff+23SmO5XYIpG8yP/MTPlkpF1VtAW0P75ih0bs/VKfpXx16IifTarVWHgIC2fK1T76YtcXjH7nwN6iGjmZqZjg8c/UhV51hVwmzhBVbCbGGXlT7aXApafXpNP/jzqDlMp+Cmvzx65J7ynI/aJ4/P/+t3/0D891/99dLQvu9f/8g9ZTR/9t/+u5Sx7OdKz2VBXr/0u78V3b0p621qWenRL/zUz4jxsfF4+plXxU/8p58vPX77P+/59z8XP/cT/67046YtW+Jf/cy/iwOPHb799H1fs7Kk3/OOf1bqN/vA1w//1E+UAuvu3jArhfrNX/218aG/+dvSw1mZ0u/4gXfFrj177t6s9P3//K3fiX/7gz8StwPPsgff/A1fF29461vu27b/wsV485e8vhQklx07C1D73C/4/Pu2u/3AiRePxtf/kzfdyS73z9/9vfH5X/xFt59e1Nd6Cmirpoyqtxcvy9CWZWqr5ubajnBtV/YM/oRDr4iO1rbKHkTvBJYhIKBtGWh2IUCAAAECBAgQIECAQCUFZkaGYvzDfxPFdLNMy6/Ae37/D+Pt/+an7hvgd77xy+Pbvvwf3fd4JR/4xd/7w/imH79/LLeP+dpP+aR47/f889s/1u7XdMOidW/K1lYFZRLmRk+kVAeztbsWNTazF148Ea/89C8szepd7/ymVOLzVqmjtZ5m546Pi6lUKumLX/u58eu/UD8Z2gob90VDU+ta899z/LPDg3FmeOCex/yQXwEBbflam1ftPxQbOrryNahHjObDZ07ElZu3Mvo8YtNcPq2E2f3LooTZ/SblemTHlm1xsHdnubqrWD9Hzp6KyzeuVaz/1ej47qCX3/ur90WWpe12+/Czz8Xbv+rNpR+zrG0/8tM/efup0tev+8qvihc+/Hzs3LM73vvb//XOc1kWtTd84etKwWnZg+/+Nz8Wn/45n3Xn+Qd9kwXAZYFwWcuyrf36//r9lFD7pUycWeBdNt6sbd2+PX7xv//GQ8t9vu+P/zS+8+3vKG2f/edBAW3f/nVvj7/88/9d2u4r3vx/pYzL33hnnwd985u//Cvx4z/ww6Wne3fsiF/+vd960KYLPl4vAW1NhZRR9RXVk1H19mJlr9fZ63Y1N9d2hGu7cmfw+o7OePX+BwcpV+7IeibwaAEBbY82sgUBAgQIECBAgAABAgRWVSDLyjb2wb9a1WM62NIFpqZn4pf/1x/H0OiVGLg0Gv/p9/6g1MlaBLRNpoCWX/mjPy2NZWpm5s5kfvxXfzPmUumXugloSzNv6dsVHa/8+DsGef1mfmwklR19qeRPXsdpXLcEBLTl6ExobE3lRvflaEC3hpL9f/ivjlV3xqZsJsoQPvzUUobw4T7LebatpSU+6fCTy9l1TffJMr1kGV+qtSlhdu/KKWF2r0e5f3rmwGOxrr2j3N2Wvb+R61fjhXOny97vanb4sKCXLDDtK77gVuax13356+Ob3nnvB57+2Vu/Pv76L94fXevWxW//xa2ypdnYs+xoP/DO7y5N4xNe8ynxoyk722LaTPq79Mv/3hfGpeHh0ua/8Ju/FnsPHriz6ze88avvlBL93h/74fjMv/N5d5570Dff845viz/7wz8qPb1QQFuW9e3vv+b/jLGbY5FlofuV//k/UrDctgd1d+fxa1euxhd/5ueWyqZmD/63P/uj2LBp453nH/VNvQS09W7eGofT39vV1rLz4i9TZtXp2ZfeK6m2Obi2XduVPGcPpeu6L13fGoE8Cghoy+OqGBMBAgQIECBAgAABAnUtUJyfi+t/9LtRrOI32+ptAV88ez4+5Z9+U2na3/VVXxHf+mVfmguCni96fWQBbn//NZ8U7/nue29Y5GKAFRhE58e/Jpq3dleg5/J2WZydivmr1X3DrLwi+e5NQFt+1icrNZqVHM1j+9Dp43F17GYeh7boMSlDuDCVMoQLu5Tj0b3be2LP9t5ydLWqfWQfGHj/i8+XPjiwqgcu88HuvkGuPOF4qSSm8oTlPck6WlvjEw49Ud5OK9TbfDG7ro/EbCq/Wa3t7mv65Rna7g5oe9Pb3hpv+rq33jPN7/qmb43//Ud/HO0dHfG7H7iV4Szb4Kd+9F/Hr/7ie0vbfvU3vC3e+NavuWe/h/1wu89sm+za+rzXfsGdzV/7KZ9eCjzLyoL+bpZNru3Rpe7+x2/+t/iR7/m+Uh8LBbQNXLxYCqLLNsgC8z7p0z/1zvEe9c1f/MmflcqUZttl2euyLHaLbfUS0JZlcMoyOVVjO5U+OHr+0q3gymocv2vbtV2p87aQ/h/8yY8/Fc2NTZU6hH4JrEhAQNuK+OxMgAABAgQIECBAgACBygiMH3kupi+cqUznei27gIC2spMuq8OGdMNsw2d+fqS7kcvaf7V3mrt6JmJ2crUPW9bjZeUuP/jhj8b0xzID7t7ZF3t29cVf/vUH4/f+15/F6XMX4xOfeWV84d/77Ni981bAQhYc9gd/+hfxtx88Ert29MRnfOonxt/5rE9b1LhmZ+fi+Kkz8eKxU/HCsRMxMDgS+/fuiiceOxCPHz4Qe9Lxs5tiy2lz6eblsRNnYnJqKp58/FC0tDTf6Wa5AW0fPXYysn8vHD2Z+j4dGzesi1ccPlga78e/+uno7HipDNSdgy3hm3osOdq4+WBEIZ9vtg9euRxHL55bwgrmb1NlCO9fE2UI7zcp5yOfePiJaG/JVwnhxc7vaMrQNpgytVVze9gNcuUJH7yyyhM+2Oblz+zr7ovd2/L/YZPb4z7efz76Ry/d/rHqvj7smr4noC0Fs2VBbXe328FnLw9o+5a3vDWe/cBflzb9/h//sfi0z/6su3d76Pc//5M/Hb/4M/+htM3r3/TGeNu3fnPp+8H+/viyv/v3S9/39PXF//f7v/3Qfm4/+dHnj8TbvuKNpR8XCmh73x//SSpL+i23N1/21598z3+Mp171cYvevx4C2qo1o+rtRbw5ORF/e+LF2z9W3VfXtmu7Uift1vUb48nd+yrVvX4JrFhAQNuKCXVAgAABAgQIECBAgACB8gvMpjfRb/7Vn5e/Yz1WREBAW0VYl9xp696D0f7400veb612KE6MxvxY9X5KPHN78jWvjaPHT90hXNfVGV/35q+IH/n/2bsOsCiuLnrsgCgqKr1ZsMbYgt3fGnsXI9bYYsGu2GPB3jV2I/YYjS12E2NvKIo9NgQEFHsBK7b/3beZcVe2oazssO9+nzuv3FfmzLyVnTnv3F+WgEK7SObi5IDQA39i76HjaNc9AERMU7f+PTpgyphB6kWJ0lt37UW/4RNwM/p2ojqpoEzpbzFvyigU/6aQVKT3SCHXZi9aid83bgeR1ojMRkZkNiK1Na5XA0P6/MTOMQLFKjXgdYHD+mBYv248revj2o1I9Bw0BvsOBetyAWEyY/xQNGtQS6ePoQpLI7SlyWCDtHbuhmBJsXpSdCHFpvdq936KTeYzBxZhCDWBE2EINfFI7pwdU3kpztRelGpPnsfjXESYUqfP523sC3IRnlDzMovwhJp46MrRFoMyBYogU4aMulzMrjzuxXOcCb9mdvMydkLGrmlSZzOW0DbEvw+CD6meTfw8eQKq161t7HSwYPosrFu+kvuTshspvJGFXbmKzr5+PO3m6YFV2zbztKGPi2fOgkKVkmkjtJHCHBHzyHLmzo1ipUrwtDEftCnGytoaLu5u8GPkuzRp0xrTjPtYAqHNk6mpejBVVSUbEdqI2KZEE2tbrG1T3bdF3PMgZ1Y7U3Uv+hUIfDECgtD2xRCKDgQCAgGBgEBAICAQEAgIBAQCAgGBgGkQiDvwF96/emGazr9SrxTu8sKNCKbe9JaP6OaQC265cyHk8lXsORWKm3fuoXSB/KhT1geuuXNyHyKH7T9zDmeY+pJLrpyoWKwoqpcqbtSMiUwQfjsWV6Ni2L9oxD58DC8nRxT0cIW3mysf+7PVmxjxJSzmFl4lvEEhT3dkTP9RIehzCW3XomNAbWm+11nfdowMVJA9QC/g7oqSTMXJxoiwK/qAsbSQo1nKV0U6trtUMfb+Ld49UvaLcJ8azRF67pJRkBct5M2UysJAhBltFrJ3I0oUSxyS6jb7nug+YBR2/H1Ao1k2u6xwcXZAeEQ0Xr76qHSXLl06dO/gh0mjB8KKqfbpsrCIKPZSbSiOnQzV5cLLSUFueP/u+L5ZB543RGgLnDoPk2YtQgL7riCj7xxnx9xcSe7xkzhcZ2Q3UraTrFa1SlgbNBNEBkyqWRqhLa2tE9JYmffD9svRkbj39HFSL6XZ+au/NBNhCEUYQlPdoN7ObnDKofr7z1RjmLrf4KsXeXh3U49jqv7V17oITyjCEyb3fZbdNguKsQ0nSrMT1y6x33wf/1ZT0vyNXtNJILQFzZmHVYuDOAytO3dElz49jYYkoJs/Qo4e5/6BM6ehco1qPJ3wOgG1fMrjA/tdkJYRx3afPIaMmQwTH7eu34gZgeN5H9oIbeoqdEkhyhl9QjocLYHQpmRFVemyxTy8hxuxt6Ssoo5ibcegVd2G/JqJtZ18t24G9uykLNsUSmFHhQkEzBUBQWgz1ysj5iUQEAgIBAQCAgGBgEBAICAQEAhYPAIv2YP01wreHU4X0OenXrge/fGBoS3b8dy5QR3MXr9ZQ73JyT4HjsyfiQNnz6PrlFkgYpq69WzWCGM7t1cvSpTeefwkhiwMQvS9+4nqpILvCnpjWs+uKJbXODl9UtlZsHkbNhw4jMs3oxgJRUVQITIbkdrqly+Dfj804+dYrlsfPsyI9q0woGVzaUitx7BbtzFw7mIcZOerywiTid06oVHFcrpcDJZbEqEtbeYsyFqphkFMzM3hfVw0PiQ8N7dpGT0fCtNJxLAhY6Zh2+59vB2F0ZzLVNJqVa+Irbv2YdTE2bh7/6HcJxHbls2diLxe7pi1YDmIAEbW9ceWmDd1lOxHCeq/asN2MuksQ4b0XDGtYxtfHq6UfIggR4poE2YsxJoN26iIW8/ObTBr4nApq3G8ERmFUlWa4NlzFWnYmpFHG9Wtjm8KF4CjQ04e0vToiVB5XBtrK7x4qSLN6SO0LVm1Ht36j+RjpU+fDj/6NcXwAT3kuVLFG0bwnb90Dcay837yNI77tmreACsXTOHppHxYFKGNPWRPlyM/Ywgar5aRFCyTy/dRfBwu3LyRXN2lWD/6XpqJMIS6L4sIQ6gbm09r6MVZOfYCLT17kaZki7h7G1H37yr2FPStdXViSFLUnER4QsO3gyWQXwiFgq4ecMiWwzAgZuZx894dRN6LNbNZGTcdU6zpg3v+waj+KiVl70IFsWjtaqPUy0jJsHW9RngWH88nv2bXNji7usgn0rZ+E0TfvMnz43+ZgQpVq8h1uhIDunTH6eATvFoboY0IcrXLVMRrttmFNpVsObwPWe1Mvxkita9pOxtbpqjK/g5XuCW8fYPgq5c0nkUp5ZTE2hZr2xT3qjPbWJKfbTARJhAwZwQEoc2cr46Ym0BAICAQEAgIBAQCAgGBgEBAIGDRCLx7Fo/4I/8oGoOqvQNw9rpxL/YLs1AjVxhpTFeotgNzpuHbfHkS4XHn4SP0nbMQf504pVFHamfOOe0RcfuOxg77dGwHeKf6tRHYqT0ysbCCuoyU3npMn4MT/17R5cLLSUFuoF9zNB46mucNEdom/7YOM9ZuRMJblWodPWh3zJGdK8k9efYcNxjZjZTtJKteugSWDxsIIgMm1SyJ0GblXQRWCgxb9uF1HN7H6w6hmdRrnlL+/gFjsGj5Wj78uqWzNMJo/jx+FiYyxTIyInldC9kDd1cnnqfQo7nyl0E8u/crlCmFg9tX83LpY8LMhRg5YTbPOuSyx671S1CsSEGpOtGRwpK26NiHhzSltbV97SKQApq6USjU6o3b49CxEF5MYUqXzZ0E77ye6m48vfqPreg7bLxMPKPCMUN7c8W2T53Dmdpiyf815iQ5GpsIan7N6n/qJufPXbyCinX8ZHW5Jb+M5wQ42cGIhCUR2tJkyoq0WZyNQCVlXej+IsUm6Ts+ZWfz+aMb+9JMhCHUxFiEIdTEQ18ut112FHLz1OeiiLoXr18h5PplRcxV2ySNXetJIbSJ8ITakNYsS+3kFzpb+s1VrmBRdlQeafVlwmucvPav5kVTSM4Ua/rxo0do16Ap4uNUGzG6D+yHH9q3NYhIYMAQ7Nv9N/fLkz8fgjau4yQzqeH0MeOwbcMmnqXwoCu2bEBmW1upOtHx7207MGHYz3K5NkIbVQ7u3gsnjhzlfg19m6H/SO0bXOSO1BKPHjxkm2Xe8XClasUGk6l9TXu7uMMpu71BHJTgQBtPaAOK0kysbbG2TXHPlsjrjazWSVeKN8VcRJ8CAV0ICEKbLmREuUBAICAQEAgIBAQCAgGBgEBAICAQMAME4o/tx7u4J2Ywk8+bwju2Q5qIYaOCVmJXsIo8YmOVCdOZSlr1UiWwM/gkJqz8HffY7m3JiNg2f0Av5HF2xLxN20AEMLIO9WphBmunbtR/vYARMuksAyPL9GvRDO1q1+DhSsmXCHI3Ym5j6u/rsX7/Ibn5Tw3rYnL3znJePREReweV/Pvj+X+KTFYZM6IeU2Mr6uWB3Nmz4RpTnQu+dFke15qFNXz5+jXvQh+hbcXuPeg7ewH3I0WS1jWrIaCVrzxXqnjDCD5Ltu/i5/2UkXzIfKtWxuJBfXk6KR+WRGjL+r9aSGttkxR4zMP3w3tV2FF2VLKpE9qe3gwFqbRJdiT4NKo0aMOzRC7bsW6xVMWPFeq0xIlT55A/jwcun9gt15GKWpFydTk5jQo3LJ+DxvUMq/ARAY6IcGSOLJTxzfMHQGFIJSPiHc2XzMXJAReP7dAb7pOU55q09Zea6yS0NfDril3/qL5jBvfpgvEj+sttdCXmLfkNfYaO49VeLNTw9dN7dLlqLbckQlvarK5Ik1H3S06tAKVQYfidW4h+cC+FRk+eYY1+ada9K4joom4j+gzAkX37YW1jg10njshV86fOwB8rV/N8x57d0a5rF7nOUELqk/yGTxqHmvXqyk3qlauE5+z/SyKS7jp5FFZGhOveuXkLpoxUfQ9oeyEee+sW/Go34GPYZhFhCGWwkzHxjUde5MiSNRl7TLmuzty4iriXKsXPlJvF541s9FoX4Qk/D2AdrVI7+YVOm5TZSKFNqXY2/DqevnimuOmbYk0TCPsZMW0MI6iRUWjQfiOGoU5jVfg/Xqj28YaFa102fxHWBC3jpRnYb2lSdSNSm7o9efwY7Ro2RdyTp7yY1N8GjxuDvN6aSmC0WWDj6t/x6+w5eP3fb25qoO3/byq/HXMLHZu2wKuXLymLPsOGoHFLXw0yHa/474PUnoMPHQGprJ46Hsz9Vm7dBFcPd3U3venUvKZTi6KqdAHvPX2My9GRUlYxR7G2xdpO7pvVOmMmUChhYQIBc0dAENrM/QqJ+QkEBAICAYGAQEAgIBAQCAgEBAIWjcDryDC8vHJB8Rj0n7sIy3b8xc9j+fAAjTCaY1f8xhXLqJJIXmeWLoArI6GQUehRL992eMYeRpctUgi7po3n5dLH9LUbMG7FGp4lotnGcSNRNI+nVJ3oSGFJ24+fyvulF99/BI5ADaaApm70wLzB4JE4euESL6YwpfMH9kY+l8TKQOv2HsTghUsgEc+owfB2fkyxzVe9S56OvHMXFXv04yQ5GntxQF80r6qpHKXe6EJ4BL7vN1RWl5vbrydaf19N3cVg2lIIbelZmARbH91YGgQqhR1IoY2U2pRs+ghtREwr8F0tfnr+nVpj9qQRGqdax7cz9hw4imx2WfEgTBVCiBxIHe1H/8Hct2aVClydTaOhjkwCCw2cv3RN3Iq9yz3OH96GwgU/vkCrXK+1HEp0bdBMNG9YW0dPH4t9O/TG5u0qspk2hTb63rDP64O4+GdchS78zD44O+b+2IGO1INHj+FcqCIPm0oud64eQ06m2GisWQyhjam7pMtB1zCNsdCkqN+zVy9xOky/umeKTtCIwU3x0kyEITQMfGp+Ia5+9hS6vWyBojrJBeq+SkjffnQf12/HKGGqieZoirUuwhMmgjlRgSWs9W898yGbbZZE566UgtjHD3HtVpRSpouoiEhcOHMW25ni2eULF/m8O/h3g2fePChbuRIysQ1Y6mGES5bxQZ0mDVG2UkVkyaoiF0vk8fQZMrDNH/1R5Nti8C5cSMaA1NFIJU2y0uXKclKbFyOq5XLIjRimth5+7Tonr99kv2Ul8x80AL5tW0tZjePuLdswacQouSw9+/+hTMUKyOOdDzly5kTkjXBcCD2D8Oth3IfCh8Y9VRHgSpUtg0rVq8KnQnk4u7nKfVDiz7V/YNb4SXIZkeWatvaDu5cnHJ2dudpcbEwMTh49zsl6pEInGRHw1u7eDvtcqmcSUjkdjx88zOZyPVHIyqVzF/C/5wnvGvXqqDfhaTqXarW/h9VnqK4n6uwrF6QWRVUJNiIwHmPP2GhzpBJMrG2xtk11n3o5OME9l6Opuhf9CgSSDQFBaEs2KEVHAgHLRYB2xWzZskUGwN3dHWXLlpXzIiEQEAgIBAQCAgGBgEBAIPD5CLxnYYziDuwGe2L6+Z2YQUt1QtutzWtgo6aecvziv6jLVNbIKLzmhrEfw4hQ2ff9hiDkyjXkdXHCqSXzqIgbqaj5dOnFyWlUsOrnwajPVNQMGRHgiAhH5sBIcJdWL+EhcaR2SxnxbgAj4JE52efAyV/n6A33ScpzrcZMlJrrJLS1GDkOe0JCuV/fFk0xqkMbuY2uxK9bd2LQgiW82sPRAWeXqdTddPl/Wm4phDaboiWQ0dXz09NXTP7Dm+d4/zRaMfPVNlFjCW0jA/wxclBPjS6ate+FLTv/gW1mGzyJPC3XBYycjJkLlvP86CG9MWJAd7nOUELqk/wo9Ger5iqlJcrnyPMdJ54RsZTU5GysrahYry1bsxFd+qi+p7QR2iKiYpC/VE3eBxHzalc3nmC5/a/9PEwpNSb1uk9DpOqbmKUQ2tJYZ0fazA76oDC7OiK0EbFNqWYKkosIQ2j4brAEkguh4GqfG3mdXAwDohCPN+/eIvjKRa4KrJApy9M0xVoX4QlleHUmUvtaz8QIUURaVbLRxqrjjPRCat9KsPaNmkGdRKY+5yFM9ax2owa4f/cufGtokq2I9Na+20/cfeqoQOzY9KfclIhuWw/vQxoWPpYs4XUCfluyFGuWLgepsBkyO/Zb+6e+vVG3SSO9BOYNq9dg8axfeP+6+qS/2/06/ggXRlybOnqshluhYkWx4LeVGmW02WTTmrUImjMPL54bp6BJYxQrVRK9hw5KpBJHnV+/fAVdWrTSGCcpmUGBozgWSWljDr5FPfLAPoudOUwl2eZwlZFV7zDSqhJMrG2xtk11n5Zh6mxWTKVNmEDA3BEQhDZzv0JifgIBBSAQEhICHx8feaYBAQGYMmWKnBcJgYBAQCAgEBAICAQEAgKBL0Pg2aljePvg7pd1ksKt9RHaiJhWsmMPPsMuDepiSo/OGrNtNjwQ+0LPws42MyLXr5LrSB2t27TZPF+tZHFsHD9SrtOXSHj7FsV/7IbYh6pd2McXzkZBDze5Se0Bw+RQosuGDUTjSuXlOl2JduOmYNvRYF6tTaGNHqh7NG+L+BcvuArdhRWL4MjIcobsYVwcvFt2kF+khK1bDvv/dtAbakv1FkFoYy9Y7KrWRRr24kzJ9u5RGIuP+1axp2A0oY2R2YjUpm4S+exTQlvNph2w/7BqXW1cMReN6lZXb6Y3PXrSLxg3XUUAHeDfEZNHB3D/SBYuOF/JGjzt6eaCsNB/9PYjVYaEnke5Wj/wrDZC29Zde9G0nSZRT2qblOPhnWtQ7rsSRjexFEJb2myeSJPeMPHQaOC+gmMMCzl6g4UeVaqZguRCL5VXLQ7ikLTu3JGRRI1fMwHd/BHCVFTIAmdOQ+Ua1XiaXq7X8imPD0xlIy37/2D3yWM8FBqv1POxdf1GzAhUqb5qC1mmrmLjxkKhr9q2WU9vyVeV2kkuElKl8hWErZW1lE0Vx0tREXgQ90Rx52KKtU4giPCE+m+F1L7W3XM5wMshsbq1flTMr5bCElJ4QiXYzHETsWPjZrxlv3XVLWfu3Oz/zakoXOwbriDWr1NXnD8dyhXGKKT2sAljUb5KZd6Ewm2SCtujBw85Aa1itSoYO2u6enc8fSsqGnOnTENo8EmNEKCSY2ZbW65G1qVvL5CimjEWERaGKYxQd4WppNNvZ8no/3ZSgOvIiHcVqlbB6eATCOjqL6sbp2MK7y07tNf5N8WDe/cxf+p0HN1/UOtcaRw3Dw/UZM8hatavCycX3WTr58+eoXf7TrjBVOiSaurXIaltU9I/A1PMK5eKFFUlLJ88f4ZzEUm/jlL7r3kUa1v77wWxtr/sLsyW2RbfeuX/sk5Ea4HAV0JAENq+EtBiGIFAakYgKCgInTt/fOm4atUqtGnTJjWfsjg3gYBAQCAgEBAICAQEAl8VgYTb0Xhx/tRXHTO5BzOW0Da49Q8Y0kZFGpHm0CZwMnYcP4HMTEUpZpMqvCjVjfh1OeZt2srdhrX1Q0CrxGE+pT4+PUp9UvniQX3hW1X1EJ/y7s3acOIZ7dAmNTlrFp7FkK3+ey96zVSpx2kjtN1k4UaLd1CpSxExr0bpkoa6lOt3nwjhYUqpYD1Tr/s0RKrsqCVhCYS2DI4uyFz84wYbLTAoouj983v48PJjqBtFTFptkqYgtDVs1Q079xzko6xeNA0tm9ZTG1F/cvDoqZg+byl3ImU3UngjO3fxCkpVbcLTBfJ54dLxnTxt6OPYyVBQqFIybYS2LTv3oll71cN2FycHVCxbylCXcj1912S2sUZeLw8M7NmRk3LkSgMJiyC0pcuIdNnzGEDC/KoT3r5B8FXNl7LmN0vdMzIFyUWEIdSNt1ST2kkudJ6ZM1mhdP5C0imnmuODuKe4FBWumPMRIcxcNa6VCE+oAccXZ2iN01pXuj2Kj8OFmzeUfhommz+RyWNvxyIqPBxELnF2c4NHHi+toTqNncRLtgEsjKmzR0VGwt3TE/kLF4SVmrq7sf186kdzvRMby1Xs7rHf5vYsBKijsxMcXZxBBDxh2hFwtc/FFFU1vy+1eyqvlP5Of/3GsNKg8s7sy2cs1vaXY2juPRRwcYdjdntzn6aYn0CAI/B/AAAA///9WQbQAABAAElEQVTsXQVcFVkfPYKANLaCLYLdgd3d3V1rra69dn3m2t3dtWvrutba3aKoIBYoIiClCH73P29neO/xEkF58+7/+307d27fc9/gezNnzkn1jQV4cAQSicDvv/8Of3//BK379euHSpUqJchP6ozAwEAMHTpUY7dLly6Fi4uLxjKembQIDBkyBAsXLpQ6vXPnDooWLSqd8wRHgCPAEeAIcAQ4AhwBjsD3IfAtNhahp44AsV+/r6Of2HrokpVYf/i4MIPX+7fBLk0aaTa+bwNQskd/4Xx0p7YY1bGtVEaJTlNm4fClK7C3TYNX+7ZJZU1HT8S5O/eE8y0TRqFh+XJSmb7E9M3bMWfbbqHaoJZNMaVXVyHtH/gOxbr9IqRzZM6EOxtW6OtKKL/x2Ae1howS0mO7tMfw9q1V2h25dBUdp8xUyUvMyfG501G2YH6Dm2Zp0hafY2LQqEI5bB6vmJ/BjU2kon1JL1hlymois9U+zW9foxEX4qe9QgovGTBiMlZu2CHMMvTFTdjb2UozfubnD88ydYXzCSMHYsKIAVIZJVp2HYS/jpyEg70dQvxuSGUTpi/E9PmKa3D0kD6YNvY3qUxfokGb3jhx+rxQbff6RWjeqLaQjv78GU45SiIuLg6WlpYIfXEDaWxs9HWHVRt3ov/wSUK9yb//irFD+6m0UV6jp3tuPLjE/mb/gLB3K4bPX76gWcNa2LNh8Q8Y8ccPkcouIyzs0v/4gZNgxHsvniH4U1gS9PTju5g3dToO7NojDHzs6gWksY2/pt+8fIUODZoIZd3690W3fn1VJjhu8DCcP3UatnZ2OHpFcR1ShY/BwejSuAU+hSkw6Tf8N7Tt2lmlraaTKSNG49SxE0JRnnzuWLt3J1KlSiVVnTt5Gg7u2SecZ8iUCRv/2gN7BwepXD1x4uBhTB8zXsruObA/OvftJZ2LiVH9BuHK+QvCaZPWLTF0wlixSO8xOOgD+zsTC5qPMVG7lBdi2DVduWZ1TF0w15imJlM3TxY3ZM9gHC6msDh6zHLJ+x5i2Pd2U4iuTVvixXNfjVMdPW0y6jVtjPfs3nvrWvVV6nQf8Au6/tJHyJszcQoO7/tTKnd0csKBf08hlYWFkPfl8xdsXbMO29ZtED7XUkUtCee0Lugz5Fc0aN5U5RpXr75nyzasWrAI1L+2oL8R7Xt0g1v2bJgzaapKtQJFC2P51k0qebR/+7btwNrFSxEZEalSpu2ExihaqiR+/X0k8nrkS1DN55E3erfpkCDf0IyRUyYKWBhaP6XUc7S1Q8m8nillOt81D/pcXH58H1++mu7v8O8CgDc2ewRKsWvZgV3Tcgy/wLd48T5Ajkvja+II6ETAgn1/KZ+/CFKz+yE8OAKmgEAq9oWME9pMYadS4Bzpo+Po6IiIiIgEsyOS2dy5yX/TpUePHli/fn2C8R3YTaswdnNM+eZWgko8I8kQqFmzJk6dOiX0Z2VlhfDwcFhbWydZ/7wjjgBHgCPAEeAIcAQ4AhwBIPLuDXx5k/BlElPBJjkIbW0n/g8nrirIL2tG/YaW1SobDMeENRuxeO9fQv0RHVpjTOf2Qvrec19UGTBMSOfL5oarqw0jiFx56I16w8YI7TQR2oiQR8Q8iqzp06FC4YJC2qD/sJtN9mlskNs1K35t1Qx088nQkDuhLZWVNZyrswet/z04NRSXlFov9uNzRlzV/nA2pc6b5pUchLa9B4+jbY8hwrJLFC2IK3/vZluteEiuC4ug4I/IX7YeQkIVpJkn108gT87sUpOCXvXx5JmfcL5v0xI0qV9TKtOWqNuqB/45e0ko1kRoI4KcS65SiIyKFu5FBD6+hHRpnbV1l2T55kBos0ybF7C0SjLMfmRH70I/4tFLvx85ZJKNlRyENprcaUZMm8wIahTWNtb4bdwY1G+mIMcJmUr/IWLX+mUrsW2t4t6fFbvXtHLHFhCpTTlCPn5ElyYtEBYSKmR7FMiPUYyQo04woXuZe7dsx+qFi/GZkVvF0EZoe/PqNXq0aIPoqCih6uAxo9GsXWut9xvp78Dlc+exf/tOXL90Wai36cA+ZMuZQxxK71HuhDb6BlPOszBs2P1DOcbTt6/w+sN7k1ja/GkzcHjvfnxVI+oQCXPK/DkoWLSIQP7+rWdf3L1xE3T9OLBnAWOmT0WFalWENdLnnMihROCk+/CValTTSMR87f8SS2b/gZuXr6pceyJQRECtUa8Oeg8ZBCdnw/7t9H36FLMZoc773gNhbmJf9D0hN/sb0YMR7ypWr4Ybl69gRN8BwlqoDpHZ23Xvit6DB4pNVI5B795j2Zy5uHD6rMa5UuXsOXOiduMGqN2oAbK6uam0Vz6JYPfIf+3aE8+e+ChnG5RW3geDGqSgSu5Zs8EtfcYUNKPvm8qzt6/x6sO77+uEt+YImCACdjZpUCZfAROcuWFTjvwcjWs+jwyrzGtxBGSEQCbntCiQPZeMVsSXIncEOKFN7jucjOt79uwZ3N1VbyCJw5UrVw6XL18WT5PlePXqVXh5ean8YBUHovxLlxQ3msU8fkw+BDJmzIigoCBhgMKFC+PevXvJNxjvmSPAEeAIcAQ4AhwBjoCZIvA16B3CrytUQkwRguQgtE3buA1zdyjUY35r2xITunU0GJpW46bgnxu3hfqbxo1E44peQvrzlxi4NmuHOPbQzpI9EHu9fztsrPU/dF1/5ASGLlYoSWkitCmr0BlDlDN4QVoqyp3QZp0jN+wKFteyetPLjov6gG8RpvEgXB3d5CC0vWMPyAuVb4CPIQpi2uzJIzG0f3f1oROcd+g9FLv+PCrkFy7ggVtn/1QhoPQbNhGrN+0Syt2yZsbd8wfh7OSYoB8xY8uuA+g2YJR4Ck2ENips1K4vjv1zTqjXp2tbLPtjkpA25D8B74IQy1R9aD7GhNwJbams7GDhbDgZyBjsfkRdIjhd8r6Pr0ypy1TC39cP927dxiGmePbo3n1h2qTIlCtvHnhVqQwbpmiorNBWslxZ1G/eBF6VK4HUmShEhbbUjLQ0YMRQFCpWFB4F4x+IEgGGVNLEKF3eSyC1EQklI1NHffXCH88ZAWTXpi0qClIDRg5D686a/60/9tdBzBw3UewSqVOnRrlKFZHHwx3pMmSA37PnuHfzFp77PBXqEGkmLFRBgCvlVU5QRCtbsQJcmZqTcvy5YxcW/G+mlEVkuRYd2yNH7lzI4uoqqM29ffUKVy9cEsh6pEInBhHwdhw7hPQZM4hZ0vHS2X/ZXHwS3Ndct2S5QLwhvGs1ZIRttaC1EPFHWTFPrUqKPk3n4IgiuTTfT07REzdwcp+iInHz2WMDa5tftW/sb+LbN2/h//w5iDjmmj07cubJrfEaMRSdqMhIPPV+An8/P+TIlQv5mJJxmjRpDG2utR7NNeAtU+9hL7u8CwhEenbtZWEvl2Rxc9WpAKm1QzMpoBdvvBhp1Yr9DZZLhEdH4cZTb7ksh6+DI2AwAnmyuDJFVeN+mxjceQqpeIv9mx3G/u3mwREwJwSK5MyLdI6K323mtG6+VtNFgBPaTHfvfvrM9+/fjxYtWmicB6lzhbKbQknx41HTAPRGWPny5XHlyhVNxejduzdWrVqlsYxnJi0CAQEByJo13t6nQ4cO2Lp1a9IOwnvjCHAEOAIcAY4AR4AjwBEAe+KJ0DPH8I29RWqKkRyEtr/OX0K3/80R4CjmngenFs0xSL3sA1NzLtVzAELDFWrTt9YvR64s8Tdqy/QaiKev3wj9bp0wGg3Kl9ULefMxk3Dm1l2hniZCGxHksjXvgCimCEMKFs92bkRaR+12aHoHNLCC3AltDl5VkdolnYFomEC1uBjEBj8zgYkmnGJyENpoFCKmEUGNgqxBl8yZgG7tNd+LIOvNKbOXYNbC1UJ9G3Zv4srJ3SBSm3K8/xCMwhUa4kNwiJBN6m/rFk9HkYKq9lh072HRqs0YN20+oqLj//ZqI7Q9f/ESJao0RURklNDvopnj0a9HexUynfI8iMB29OQ5LF2zFSfPXhTU5+5fPIx8eXIqV9OZljuhzcIhC1KlcdGJQUovfPLaH28/fkjp05Tmx20IuQ2h9GFIhkSBbLmQySVtMvSccrq85vMQkUoKgClnZnwmHIHkRyCDkzMK5ciT/AP94BGuMxWnCBP9Hf6DoeLDyQQBuSuqitv0Jvg9fN68Ek/5kSMgewSsGeGciOfc4U72Wy2rBXJCm6y288cuZsqUKZg4Mf7NR/XRz507h8qVK6tnJ8n5xo0b0a1bN619LVq0CIMGDdJazguSDoETJ06gbt26UoczZszA6NGjpXOe4AhwBDgCHAGOAEeAI8ARSDoEorzv4bOfQlkk6Xr9MT0lB6HtPbMWK9t7EEKYnQ/F1F7dMLClZtsy5VX2nDEX+84p1O4K5sqJ88vmqdzM+W3RCmw4ekJoQvagl1cugpO9nXIXKumd/5zFL38slPI0EdqosPX4aTh5/aZQr3uDOpg36Bepjb7Eu48hiGVKETQfY0LOhDYLO3s4ValjDBwmUTcu1B/fYkznLXFvn+e4ePWWoHh27eZdAeOJowahoGdeNKhdFbZMJeWZnz88yyh+N9ao4iUQ0urXqoq0Loq3glt2HYS/jpyENVNDnDN5FMqXKY6SxQpJ+0XqaKSSJkatahWEPgoXyMcUzbLg6XM/3H34BPOXb4D3k3hC4B9TR2PIL13FZirHTTv+RI9Bv0t5VlapUa9mFRRh5LfMmTLgEevn/OUbuP/oiVCH7EODPyrUnGpWLY9mDWqjTo2KyJtLVT1s+brtGDRqitQvkeUG9e4MT/fcyJnDjanNhcL3xSucOHVeIOuRCp0YRMB7evMksmZOaNN1+MQZ3GNr/Mb+pxyTZi4WlN0KMLw7tGqsXCSks7C1tGnWAPZ2tgnKUn5GKlimZ0pOqSxT/lR1zDA0Ihy3fY23m9PRZbIWcRtCbkOYXB8wUr6tkL+IQdbRyTWHH9Gv//tA+AYqXoz4EePxMTgCKQmBQkw9OYOTaRPRNeH5kqmlPw94ramI53EEZIlAWqaoWlTGiqripsUw2+1Lj+8nUMwVy/mRIyA3BLKlz4S8Wd3ktiy+HpkjwAltMt/g5Fxe69atsWePwt6HxnFwcED4fw+S6HzmzJkYNWoUJZM0wpiagqenJ0gZTAx7e3tERCjUFSjv9OnTqFatmljMj8mIwNy5czF8+HBphMOHD6NBgwbSOU9wBDgCHAGOAEeAI8AR4AgkHQKxYaH4dPFU0nX4A3tKDkIbTZ+IaURQoyBr0LkD+qJjnRrCufp/PsfEYOaWnViwa59QZMOs0E4tmg0itSlHUGgYyvUZhOCwT0I2qb8tHToIhXKr1iP1phV/HcaU9VsQzZShxNBGaPNjdkUV+w1BZPRnoeqc/r3Rs1E9FTKd2AcdicD297UbWH3gKE7fuiOoz11ZtRh53eIVkpXra0rLmdCWxp1ZSrnHW9hpWr8p5n2LDkVc+FuTmXrhio1USGTKE1+3eAa6tGuGV28CkKtYdeUiEOlt/PD+Ql6fIeOwbuteqZyIboGPL0mkh2imdDNrwSrMXrQGpMKmLzKkS4vpE4ahe4cWWq8v6mPRqk0YM2UeqH9tQW8uj/y1F/Iw4lrf38arVCtbqiguHtupkkd/F5as2YIJ0xfi038qkCoVNJzQGJXLl8bCGWMTqMRR9dv3HqF0jRYaWhqWtXrhNIZFS8Mqp6BaqWwcYeEoj5vtV548UPl3IgXBnCKmwm0IU8Q2JPsksqRNB0831e9SyT7oTxjgc8wXXHn8QI1+/BMmwofkCPxgBKwsLeFFpFX2vUZuQb8jrxDpRW4L4+vhCGhBIH+2nMgsJyV0Leuk7Af+zAab3WvjwREwBwRK5fWEg632F3bNAQO+RtNDgBPaTG/PUsyM8+fPj8ePH0vzGTJkCBYsWCCdN27cGAcOxL9BLRV8Z2LEiBH4448/pF7atGmDs2fPIjAwUMoLCgpC+vTppXOeSD4ESCmPFPPEePnyJbJlyyae8iNHgCPAEeAIcAQ4AhwBjkASIxB2/iQjuyiIVkncdbJ05/PyNS4/fISNR//GjccKhZrfO7eDZ47sqFu2FNIwRSLftwEo2UNBbKlavKhASKtdpiRc2EszFJ2mzMLhS1dA0vjTendDmQKeKJ4vrzRfUkcjlTQxqpcsho61a6AAI6C4ZkiPZ6/f4oHvCyzddwBPXsbbSfyvT3f0b55Q0Yj62X7yNPrPXSx2CavUlqhVuqRAfsuc1gXe/q9w+cEjPPR7IdQh+9CPnxRKcdVKFEWjCl6oUao4cjP1KOVYe+gYhi9dJWURWa5v04bIl80NOTJnEtTm/N4G4p8bt7CfkfVIhU4MIuDd2bACmRlZRz2OX7kuzIVxaVRi+ubtAjGO8G5TvYpKGZ1kSueCFlUqwo6paJlaOFWpDQs7xWfE1Oauc77f4pjtKLtW1DdTZ6OfVzhw5BSs3bIbMTFfVSbhljUzdq1biHKliwkKYrVbdMe/l64Lb7+7ODthw9KZaFS3utDm5JmLIBW2gHdBAgGtaYOa2LMh/voTO37q649h42bg1LnLKhagYrmzkyNTI6uP/40bClJUMyQePPJB79/G4drNeypv5luyh7KF8ufDpFED0aR+Tfxz9hIatO0trIX6Tc3+Jgwf2BPTxv6mcZg3Ae8wfPxMHDx2WuNcqZFH3lzo0LoJOrZujNw5tP+ODmXk2mqNOzOFtvh7MBoH1ZCpvA8ailN0loWTG1JZO6boORo6Ob93b/HiXfyLmYa24/U4AnJCoFhud7jYy+Oa1rcvd5mi8kcT+r6ubz28nCNgCAJu6TLA3TW7IVVNss49dl0H8+vaJPeOT9o4BEhRtTwjp9LRHCIoLISR2nzNYal8jWaOgJ1NGpTJJ7+XQs18W81i+ZzQZhbbnPSLjIqKgqOjo3Qj183NDVu3blVRRcuQIQPev3+fpIMTga5IkSLsRnmM0C8ps5G1aalSpaRxXF1d8fo1l3+WAEnmRMmSJXHr1i1hlLRp0yI4ODiZR+TdcwQ4AhwBjgBHgCPAETBvBKKfP0E0U3oxlSjX51cVEpnyvJcNG4T2tarjDbPcK9S5t3IRiPQ2skMbIe/XBcuw+fhJqZyIbs92bZTe/v/8JQbzdu7Fwt37QW/P64v0Tk6Y2KMTOtWpqVO9acWfhzBp/WamCKW9T1JWGty6uUBcG7xwmcrQpT098PeCmSp5pN606sARTNu4DeHsd5UhQWNUKFwQs/r1SqASR+3vPvNF1YHDDOlKY53Fvw0QsNBYmEIzLV3SwtGrWgqd3fdPK+7TG3z7HPb9Hcm0hzimXujHyLLeT56DiGN5c2VHfo+8Gq06DYUgPCISd+4/wuOnfsweNBdKFC0EO9vvJ3rSXF+8eiPM9SUj15KdaM7sruz/biACHg8tCDCbUcFuFKm0VDCt7Kgvn3H1yUPTmjSfLUcgCRGwsbKGl2e8lXQSdp0iuwoMCYb3K8VLDylygnxSHIFkQKAkU31xlLHqC7+uk+FDw7tMkQhkYcpsnkyhzVwijt2jueR9D19jY81lyXydZopAniyuyJ4hs5muni/blBHghDZT3r2fOPebN2+qkMjq1auHffv2wcXFBV+U7D+8vb0Fe9CkmipZWR49elTqbsaMGShbtixq1qwp5dWtWxfHjh2Tznki+RCIZV/wyGo2OjpaGKRKlSqCWl7yjch75ghwBDgCHAGOAEeAI8ARiIuORNiZ4yYDxLAlqxgZ7W/EfFW9OZg1fTpsGjcSpfN7CApiTUdPxMX7DwWFJGcHe6wY/ivqlSsjrPP0zTvox1TYAj+GCAS0huXLYvP4UQkweP7mLcasWo+zt+5qtHZzsrdjamSVMKF7J5CimiHxyM8fRKi78cRHVb2Jva1MCnC/d2qHBmw+Z9iYrcZNEdZC/aZm6k6DWjXDhG4dNQ4T8CEYY9lcj1y+pnGu1MjdzRVtalRl/6+CnFm033QKY0ScBiPGCip0GgfTkam8Dzqqpbgi24LFYJMjT4qbV1JN6NuXcMSFxasJJlW/vB+OgKkgkCqNCywcVBUuTWXu2uZ5ixHSwyIjtBXzfI6ArBHIkTEzcmd2lfUalRdHtvH0cJyOPDgC5oCArbUNynoUlPVS+XUt6+3li1NCwJwUVcVl+7x5iTfBQeIpP3IEZIcAvSZWjr1cQi+Z8OAImBoCnNBmajuWQua7YcMGdO/eXZoN2YDOnj0blSpVwoULF6T8devWqdSTChKROHToEMjGVAwPDw/cu3cPy5cvB9mdijF8+HDMmTNHPOXHZESACIsFCsTLkw4cOBCLFye0hUnGKfCuOQIcAY4AR4AjwBHgCJglAuFX/8VXfrNN697TG7b+ge/whNmCvmUKwmT76Zk9m0arTq2dqBVEREXj3nNf+Lx6LdiDklWorY2NWi3jT2muL2muzAr11fsPyMLsRLNnyijYjxIBj4cGBJhinXP1+syK8Pvx19B7Csn6htgPT5ntqCoRNIVMjk+DI5DsCFg450QqK9tkH+dHDkAPyehhGQ+OgDkiQPZGZHNkTkEKbaToxIMjYA4IEGGViKtyj8fsug7g17Xct9ms12djZcUUVQubHQb00gm9fMKDIyBXBNI6OKJoLne5Lo+vS+YIcEKbzDc4uZY3bNgwzJs3T+p+06ZN6Ny5M8aMGQNSTROjZ8+eWLNmjXia6OPnz59RuHBhPH3Kbuj/F6TURspwvXr1wtq1a8VsbNy4EV26dJHOeSL5ENi1axfatm0rDbBq1Sr07q1qFSUV8gRHgCPAEeAIcAQ4AhwBjkCSIfCF3UiPvH8zyfrjHXEETAkBq0xZYF+yvClNOVFzjQsPxLfoj4lqyxtxBEwaAUsrWKbNa9JL0DR5sjEixSYiMvPgCJgTAk529iiRx8OcliysNST8E+74xd/LNjsA+ILNBgFSfSnLVF/SmIHqS0gEu659+XVtNh9uM1youSmqKm/x1ScPEKXkQKZcxtMcAVNHID+zEc7M7IR5cARMEQFOaDPFXUsBc65Tpw7+/vtvaSa3b99GsWLFBKvP+vXrS/mk3vXw4UPpPLGJmTNn4vfff5eaN2vWDPv37xfOy5Urh6tXr0plt27dQvHixaVznkg+BMaPH49p06ZJA1y6dAleXl7SOU9wBDgCHAGOAEeAI8AR4AgkDwLfvsYg9NRRII6rNyUPwrzXlIyAffGysMrilpKnmCRz+/Y1GnEhfknSF++EI2BKCKSyywAL9n85xsOXvngfGiLHpfE1cQS0IpDPNTtc08nzmta66P8KLj++j88xMfqq8XKOgEkjkNaeqb7kNh/VF35dm/THlU9eDwLmqKgqQvLiXQD83r0VT/mRIyAbBCwtLFA+fxHQkQdHwBQR4IQ2U9y1FDDnrFmzIiAgQJhJ6tSpER4eDhtmtxMWFoZ06dIhlr11SpGKWcEEBQUJeUJGIv7z5s0beHp6CmNQc1tbW4EklytXLsTFxcHR0RGRkZFCz5aWloiIiBDmkoiheBMjEWjatCkOHDggtKK9pv13cHAwshdenSPAEeAIcAQ4AhwBjgBHIDEIRNy+ipiA14lpyttwBEwWgVTs96dT9QZIxX77mUPEfnwOxH4xh6XyNXIEJAQs0+YBLK2lczklPnwKxf0X7LrmwREwEwQs2P1Cr/yFYWWZ2kxWrLpM38A38H8fqJrJzzgCMkPA3FRf+HUtsw8wX46EgKOtHUrm9ZTOzS0R9eUzrj75foEWc8ONrzflI0DKbPRvNQ+OgKkiwAltprpzP3He79+/R6ZMmaQZFCxYEA8ePJDOS5cujRs3bkjnhw4dQsOGDaVzYxNkZbplyxap2aRJkzBx4kThnCxI8+XLJ5UlhSLc/fv3sXfvXjx58gSvX78WiHuZM2eGh4eHQKyjI63R1dVVGtfYxKdPn+Dt7S01c3d3R9q0aaVzSpw9e1aYh6+vL/z8/GDBmNM0JinS9ejRAzly5FCpr37y4cMHwX71zp07QvvAwEBky5ZNwIvGq1atGkqVKqXezKjzPHnygOZHkTdvXhVLWMojcuHu3btx7do1oR6tgwiQGTJkEOZfo0YN1KpV67uwpHG0xTdm43HhwgWBdEdj034SLoSduJ9ElixbtixcXFy0daM3n8idL1++lOqRWqG1dfzNd8KBrHBJSfDZs2d4+/Yt7Ozs0KhRI0yfPl1qpylx/vx5/PPPP8Ie0hqI4EmfFTc3N2EvW7ZsiTJlymhqyvM4AhwBjgBHgCPAEZA5AjHs7dGIm5dkvkq+PI6AKgLW7CacXeGSqpkyPouLDMI39n8eHAGzQSC1LSxd5Huzne5TXGKKTTFfv5rNlvKFmjcCGZxcUChHbrMFIeJzNK77PDLb9fOFyx8BhepLYab6Yh4vm9CORrLr+hq/ruX/4TbDFbpnzQa39BnNcOXxS7793AehkeHxGTzFEZABAkVzMQ6Cg6MMVsKXYK4IcEKbue78d6z71KlTqFmzptRD27ZtsWPHDul86NChmD9/vnROVqH6SDtSZbUEkZEqVaok5ebOnVtQZ0uTJo2QR7ajLVq0kMrbtGmDnTt3SueGJkhRbsWKFVi+fLkKOU9bexp/7NixGDlypApxSVt99XwiedFcxTh9+rRAMKNzUjwbN24c7t27JxYnOBK5rX///li4cKFAdFOuQITDUaNGYfv27YiOjlYuUkmTolqHDh1Adq5EdDM2iJTn7OwMuhlLoWwDS8SxKVOmCHOgerrCysoKw4YNw4QJEwT1PV11DS2jMWfPno0NGzbg1atXepsRwW7u3Lno0qWL3rqaKtBnnHAUIzQ0FE5OTohhlgJkybp48WJ8/PhRLJaOQ4YMUblWxALat23btmHJkiUgC119QQRFusZat26tryov5whwBDgCHAGOAEdATgh8ixNsR7/FcPUmOW0rX4tuBBzKVkLqdGZ0kz02BrEfn+kGhZdyBGSEgIVDZqRKo/rCn4yWJyzl6dtXeP3hvdyWxdfDEdCIQKEceZDByVljmblk3nz2GJ+iFO4i5rJmvk7zQcBcVV/4dW0+n3FzWSk9LyzvyRRVmSCFOcfb4CA8eRMvXmHOWPC1ywMBm9RWKOdZSHDUk8eK+CrMEQFOaDPHXf/ONROJiog4YhBhh8hdYvz5559o3ry5eIqqVavizJkz0rmhCbITJeWpmzdvSk3++usvNGnSRDon0pSo1kaZU6dOFchgUgUDEqSENmjQIJ0EMm3dkCLcypUrUblyZW1VNOb/8ccfGDFihFRGql2kGjZ69GiBWCUV6Em0a9cOmzdvFlTPqOrt27cFYtmLFy/0tIwvJgtXwrV27drxmQakLl26hAoVKkg1iZA2efJkgcQ2YMAAjQQuqbKGBJEVly1bhnr16mkoNTxr69atArakgmZskGIcERuVVf8M6YOIgUQgpCCSX0hICN69e4dWrVrh33//1doFXStk26ocZN9bv359kDKbsUGEtvXr18Pe3t7Yprw+R4AjwBHgCHAEOAImikDUwzv47M+ty0x0+/i0jUTAIo0tnKrWBbsTZ2RL064eG8p+38VEmfYi+Ow5AgYhkAqW6dwBmau8ELGFHoTz4AjIHQErZg9ePn8Rs3+ARgRWIrLy4AjIEQFzVX3h17UcP83mvab0js4onDOPeYPAVv+ViZ9c8r6HuP+EPMweEA6AySOQPUNm5MmSeMc5kweAL0AWCHBCmyy28ccuolevXli7dq00qDrJLCgoSLAkFZW7yFqRCD6kxGVMrF69Gn369JGaEMnnyJEj0jkliMCzZ88eKU8TQUgq1JAgVa0xY8ZIKmNUhSwxyUaVbCPp/2RJSeSox48fg+xIT5w4kaD+9evXhboahtCYRQQ6Ut+iIFyIxNS+fXvs27dPyqtYsSLKly8vkPrIspLsVQ8fPgwaSznIjrVjx46CrSfZiEZGKt74S5cundBniRIlkDVrVpBym4+PD4iIRip7ykHlpAiXPn165Wyd6VWrVqFv375SHdoHsjclUqEYtLY6deqgSpUqgkUm2XoSjnfv3hXqUn3xcyK2UbaUFfMMOZIaGn02N23apFKdPn9FihQR9qdo0aLImTOnYH9K8yAsr1y5olKf7HQfPXoEws/QoL26ePGiUL1kyZLCZ4TImKIdKxWQBSl9rsialRTcyNKWCIjKVrO0zw0aNMC5c+ekoUmNj/aVPv+kpEeEObIdpf0i8h5db8pBJEeRXKecz9McAY4AR4AjwBHgCMgTga8hwQi/fFaei+Or4gioIWCTxwO2HoXUcuV/+i06BHHhAfJfKF+h2SOQytoBFk7GK8ibInBkVUaWZTw4AnJGwC1dBri7ZpfzEg1aG1kMX2ZWw/zhuEFw8UomhIANu/fvxRSdzDHouiYLcfVnG+aIBV+zPBAge3CyCecBPHzpi/ehIRwKjoAsECjtnh/27OVQHhwBU0aAE9pMefd+0tzLlSuHq1evSqM/f/4cpK6lHIUKFRKsQcU8qk8EH0ODCHAeHh4CCYvaEBmIyGTqyln58+cXCFJiv5rmIpYpH0n9jUhlpAimHHXr1sXSpUsF0pFyvnKalLOIaEekJzFobUQUs2RvHhoSRPL6+++/haq0BlK0mzFjhnBO2JHqGhHR1IPmPWfOHEHJTSwjS1Yi+lF9UnqjIBvYDcxuU7RmFeuKRyJCkWVpWFiYmCWoiZEVqqGhTMqjNkQMFK1lSZ54+PDhICtOZcKWet///PMPunXrpmILShgSOaxs2bLq1bWek8UoWc+ePHlSqkNzIIIbkRZ1kdOI/EWKg6SoJkaPHj1USJtivrYjWZZ++PBBKCYrWUrT2ijos0GqhqVKldJrT0tkNGXLXLrW6JxIeJri8+fPGDhwINasWSMVk9XptWvXhOtHyuQJjgBHgCPAEeAIcARkjUDYub8RFxku6zXyxXEECAHHSjVh6eBkfmB8i0Xsh6ds3d/Mb+18xWaFgIWjG1LZOJrFml8GBeJ5wBuzWCtfpPkiUDKvJxxt7cwXAKWVP2CKykFhoUo5PMkRMH0EcmTMjNyZzVf1hV/Xpv8Z5itQIJCaPZMjRVULM1NC17b/Hz6F4v4L7oSgDR+ebzoIODCHtlJ585vOhPlMOQJaEOCENi3A8GzNCBChiggzpCRF4ejoKKhNEXlIOfr16ydYN4p58+fPV7EpFfO1HQcPHoxFixZJxUSMEslSYmZUVJQwfiyTgKVwcHAQCFrqcxHrKx+JfCUSyCg/S5YsAumIyEiGxJcvXwSbUWVinzFrJEW0gADFG/aEIRGyKH799VfMmjVLKxFNnFv16tVVbFzJ1pWsUymGDh0KsjTVh4O6dSwRyWgeZEFqSNCYykpiNB69kUQqbxs3bkTDhg0N6UZQ7yNSGyn9iUFWrmQ1q42QJ9ajI43ZqFEjFfW+woULC1awypaoym3U00RmIxU3ZVIbqdgRzvqC1PtcXeN/uIv7aWNjI1iwErHPEKIjqbm5u7uDrjEKLy8vQUlP337Q+om4t27dOkHRj8iK6gRTfWvg5RwBjgBHgCPAEeAImDYC0U+9Ef00/mUL014Nnz1HQDMClk7OcKxQQ3OhGeTGhb3Gty+K341msFy+RHNEIJUFsxvNZzaWwp+ZyvwVUnYxx73mazYLBOzYfbEy+QqaxVoNWWRQWAge+PsaUpXX4QiYDAKl8xWAvU0ak5lvUk+UX9dJjSjv72ch4MoUVfNxRVUJfnrmRgqMpMTIgyNgygjkzeqGbOkzmfIS+Nw5AgICnNDGPwhGIUC2l8oqaWSJKVotKndEqlcdOnSQssgadNeuXdK5rsSDBw9QvHhxfP3vy0L27NkFNTR7e3uVZkR4ItUrMYgARCpp+uLgwYNo2rSpJAdNBL3Lly+DSFTGBNlm0vjiPMkK8uPHj3qJZKTeRYpe6mEMRnv37hUU1dT7IEIcEdUMCVL3ypUrl0Ssozak7FW6dGlDmguqZ7Re5SAC2Y4dO0B7ZkyQUhxZu4okP2o7cuRIgdynr59p06Zh/PjxUjVS9iMbUbI3NSa2bdsmWLeKbcgmVSQJinmajqS0R4p76kEKeV27dlXP1npO9bt37y6Vr1ixQsXSVSrQkCASHCm5ESHTEPKchi54FkeAI8AR4AhwBDgCJoxAXGQEws6dMOEV8KlzBPQjYMveGLfJ5a6/okxrEJmNSG08OAJyRSBVGhdYOGSR6/I0ruuu31N8DOdEVY3g8EyTR4BUm0i9iYcCAbIbvex9DzH/vZjNceEImDoCpL5IKozmHHRdX2LX9Vd+XZvzx0AWay+RxwNOdqrPX2WxsO9YxNO3r/D6w/vv6IE35Qj8XARIhMbLsxCsU1v93Inw0TkCSYAAJ7QlAYjm1MX+/fsFa0dxzWS9uXLlSvFUOr569UqF1OTm5qZiKylV1JCoVauWZNdIxUSEI7KXeqgTgHr37o1Vq1apV1M5Dw4OFlSwRCKWhYUFiODWoEEDlXqGnhABieYhBqlsEUlMV5w5cyaB8le2bNlABDld9pzKfVLdYsWKKWcJynk0vi57TZUG7KRx48Y4dOiQlL127VqQ3aa+UN9fqp83b14QGZGUyRITZLPapUsXqSkRBIOCgpA6dWopTz1x/fp1kC2nqGpGbYjMRuS4xATZtt6+fVtoSoQ48XOiq6958+Zh2LBhKlXIQnbfvn0qefpOpk6digkTJkjVyGKX7Gd5cAQ4AhwBjgBHgCPAETAEgU+XzyI2JNiQqrwOR8D0EGA34pyq1YOFGStAsDeyEBvMbEeZ/SgPjoAcEbBwzoFUVuZlTRjI/t32fvVCjtvJ12TmCKRi6y/HHqDZWFmbORKqy/d58xJvgoNUM/kZR8BEEXDPmg1u6TOa6OyTbtr8uk46LJOrp3DmShT4lrklsd9TuiKza1Y4MDclcwtbaxuU9eCKqur7/ikqEjefPVbP5ucmgIDf02e4eO5fvHn5CsHsGXPMlxg4uTijdeeOyF/YfJ65pnd0QuGceU1gx/gUOQL6EeCENv0Y8RpKCEyZMgUTJ06UchYvXoyBAwdK58oJIjg9fx7vM+7n54ecOXMqV0mQJhJQy5YtpfyaNWvi5MmT0rlygkhERCYSgyxKBw0aJJ5qPJJ16cyZM6UysjGlvMTG0qVLVdZP5DB9VpuEGSmpiUGkun/++QfVqlUTs/QeAwMDBZtU5YqTJk1S2RvlMm1pmgfNRwyyYR09erR4qvV49OjRBCTAI0eOoH79+lrbGFJARLQnT55IVYn8R9am2oLGO3bsmFR8+PDhBPOSCg1IEClyzZo1Uk0i7hEZU1eokxozZ84MIqNpUuHT1Q9Zhvbs2VOqQuTRZs2aSec8wRHgCHAEOAIcAY4AR0AXAp+ZhVHUQwUxX1c9XsYRMEUEUjOLBIcyFU1x6kk657jwAHyLDknSPnlnHIEUgYBFamY3an4KjLFMbZ2UXejIgyMgJwRc7B1QLHc+OS0pSdbCH44nCYy8kxSAAKm+lPcsDCsdL6KngGn+kCmEMbX0W8/jn2f8kEFT0CBkzfg+8B1evXjB/u8PK2trZHVzRf4ihZEmTRqEhYbC1+cp8np6/BSy2LmTpzBx6AjJrUkXdPScbsTkCajfrImuarIry5UpK3JmMi+VZEM38ZrPQ0QypytzjJR+bWvak+uXLmPp7HnwZU5zmqJWg/oYN+t/mopkmVcgey5kck4ry7XxRZkfApzQZn57/l0rJqW0PXv2SH3oIhypE322bt2qYkMqdfJfIjo6WrD9JOIbhZWVlaCWVbCg5rcDyOaR7B7F0DUXqvP+/Xvkzp0bERERQhNS4Hrz5g1sbW3FLow+0pjVq1eX2s2aNUuwypQyNCRI1W716tVSSe3atXHihHEWUffu3UPRokWlPmgNZNdJ9qnGBFl1kmWnGKS2R/PTF7Nnz8aoUaOkakS8IgLW90bbtm1VrGnnz5+PIUOGaOyWrG4rVox/qEVKbWQd+z2xYMEC/Pbbb1IXx48f12gnKlVgCbJovXHjhpSVWJIkkeCKFCki9UPEyL/++otbiEqI8ARHgCPAEeAIcAQ4AroQ+BbzBaGnjrK3jvlDcV048TLTRMCuaClYu+Ywzckn4ay/xUQhLpSrOSUhpLyrFIJAKtv0sLA3T5UXUmgjpTYeHAE5IeDplhNZ0qaT05KSbC3m/HA8yUDkHf10BDI4OaNQjjw/fR4pZQJXnzxE1BfzI71cPHMOK+cvxIvnvgm2woaR2byqVMKHd+9x//YdVKpRHdMWzlWpN2fSVNy9cZPdw1DJho1tGhQpURyDx8Q/f6Iafs+eY8W8hUx16SW77aHayDK1JRq0aIY2XTqpdLZ+6QpsXKHb1Um5QbvuXfHL0MHKWbJPl2PqbGmYShuPhAj4vw+Eb+CbhAUyzzGFa1t5C2KZ7fOciVNx7K8Dytlwz++JzFmzwiVdWuRmAjxV69RERiZIYg5hyQi6FfIXARF1eXAE5IAAJ7TJYRd/4Bry58+Px4/jZVY/fPig1eJy/fr1KvaVAwYMwJIlS7TOVl39jRTY/vjjD631s7J/iIjEJYauuVAddWtIUnMjVbfvCcKCMBGjX79+WLZsmXiq8Vi+fHkV4tXy5cvxyy+/aKyrLZMIcHXr1pWKyaZVmdwnFehJ9OrVC2QzKoYhBC6q26lTJxBBkcLOzg4PHz7Uq74nVNbzn8mTJ4OU5sQgtThSjdMUZE9KNqViGGqXKtbXdNy5cyfatWsnFekj+JHVqYODA6KioqQ2ibUKpb6yZ88ukCzFzlq1aoW5c+ciRw7+8E7EhB85AhwBjgBHgCPAEdCOQMTNy4h591Z7BV7CETBFBCwt4VyjAVJZpjbF2Sf5nGODnwFxMUneL++QI/AzEbBIm5td4+b5IC0k/BPu+GlWEfiZe8LH5ggkFgF6gFY+f2FYWlgmtgtZtzPXh+Ny2NQ7jHizf9tOZMuZAwWLFkGFalXksKxEraFQjtzI4OSSqLZybPTiXQD8zOh3+JfPXzBm0BCQGpJyWNtYg8o0RYZMmbDnn3inHbIBbVyxmlblNFIBPHD+NByVBBx2bdqCZXPmaepeyMvO3KE2H1IVXVAmtDVv3xaprbT/pnRjz2ZqNqinMqbWwWRSwBVVdW/kZ/bi6JXHD9Q5l7obmXCpKV3bIswxMTGYNGwULpw+I2TZ2NigeYd2gtJizjy5xWpmd8yaNj083PhzZbPbeBkvmBPaZLy5Sb00Iu0QeYeINxSurq54/fq11mGeMlnPfPni5eWLFy+OW7duaazv7+8vqLNFRkYK5URWI7KYoxbPelJby8S+BIuhby5Ur0aNGjh9+rTYBHfv3lVRxJIKjEhcv34dZcqUkVroI+GRTKuzszM+sS/sFPTFnFTismQxTtJ3w4YNIAU8MRKrCtagQQOQfagYtA9EqtIXxYoVE/CjemTTuWqV4W+56Op7+/btKip+2giC9Bkka88g5n9OQcp0hKO9vb2u7vWWkd0orUcMIswReU9bkD0q2aSKkSdPHjx7xh4wJTIuXLggKP7RlzAx6AsY2fC2aNFCsHQlAiEPjgBHgCPAEeAIcAQ4ApoQiAl4jYjbVzUV8TyOgMkiYO2aHXZFS5vs/JN64nGR7/Et8kNSd8v74wj8PARSp4GlS66fN34KGPny4/v4rHQfIAVMiU+BI5BoBDK7pEX+bLkS3V7uDaPZw/GrZvRwXH0/TdHCjNbwmVnOdW3SEgHs/jMF3dM/euU80nyH84vQkQn+x4q9bOJFqi8MAx4KBKK/sOv6ifmQXv43ehz+PnxEWHyuvHnQtV9fFC9dEmnTp0fIx4/weeSNg7v3guw+xSDFtuPXLoqnwvHArj04c+Ikbl5R3MPIkCkj8hcuDGtrK5QsVxaNWrVQqf8xOBg7N2zGa/YMiz1mg/f9Bwh6906oU6dxQ9SoXxdelSuptFEmtB1j45MNKo94BDwZ4SULI77w0I7AXd+n+BiheJ6rvZY8Skzp2hYR37lhE5bPXSCcOjA+wcylC1GYKTyaexTPnQ/O9g7mDgNfv4wQ4IQ2GW1mci+FbBXJXlEMUgg7diz+rQoxX/no5uYmKU5Zsh87ISEhAilOuQ6l1a0m9RGJiJhGBDUx9M0lNDQUGTJkwNevX4Um9KOTSHPfG/RjlpThxNBHLPP19QWRnsSoUKECiMRkbJByGdmbikFWm2S5aWyQxSUpilGkTZsWwexHgb4gshURG7+wH2oU+/btQ/PmzfU1M6hcnag3btw4TJ06NUFbdbtRa2trYX8TVDQyIzw8HGFhYVKrI0eOCCQyKUMtsXfvXpCKmhhkj0o2qd8TGzduRP/+/SGSO5X7ItxpvG7duqFKlSrCzRPlcp7mCHAEOAIcAY4AR8C8EfgWF4swZjv67Ws8Od68EeGrlwMC9qUrwCqDedhCGLJf32K/IO7jc0Oq8jocAZNAwMI+E1LZpjOJuSbXJMnKiFSbeHAE5IBA0VzuSOvgKIelJNsazOnhuDKIpmZhpjz3DctXYsOylcpZOPDvaTi5OKvkmcOJa7oMyMdeOOGhisAdXx+ERISrZsrwjIhsRHqhIKXChetXw4o9m9EU6tfN3zevwMrKSqVqdHQ0WlavjYjwCIEQt/vkUaROrV1FTWxMggdtajcQCG1FShbH4o3rxCKVIye0qcChckKk1PKMnJqaPbfloR2BgI/BePz6hfYKMikxtWubYP/EnuV2qN9EOBLBfNnWjciTz10mO5L4ZaSxskY5z0KJ74C35AikQAQ4oS0FbkpKnZI62Wj48OGYM2eOzumSfSPZOIpBtphkj6kcZ86cEVSpxLzKlSvj3Llz4qnGI1mFDh48WCrTN5d///1XIABJDZIpsWfPHkFNS1v3Bw8eRJMmTaTimTNnYtSoUdK5oQllZTUic0VERBj0RV+5f3VimiG4U3siwBERTgwiKZLqXFIEWcyOGDFC6mrx4sUYOHCgdC4mKP/XX38VT5PtSCqDeZm3urZQt0jV9PnW1lZXvp+fn/D5PnDggNZqNC8izzVu3FhrHV7AEeAIcAQ4AhwBjoD5IRB5/xa+vPIzv4XzFcsSgVRMrdi5Wn2SwZDl+hK7qNgQP+BrdGKb83YcgRSEQCpYpmO/uS30P7hMQZNO8qlEfo7GNZ9HSd4v7zB5EAh88xaPHzyEj7c3nvs8g0u6tMLDs+JlSiOvR77kGdREerVhRAUvz8ImMtufN83AkGB4v5L/w3ERYVO0MBPnTke65rs0aYEv7CXvMhW8cPW8QmWK7BCdkuieuPJ4KT1dIq8HnGy/zyUlpa8xMfML+PiBkV78E9PUpNrMGDsBxw8cEua8ds8O5PX00Dn/bs1bw++pwtHmz3P/wIWJKqjHvCn/wwGm6EYxdcFcVK5ZXb1KgnO6Dkf2Uzw3GjllIho0b5qgDmVwQptGWITMTM5pUSB7Lu0VeImAQCx7cfSi933JuUyusJjatU37sPyP+di5cbOwJV1/6YPuA36R6/YYta6cGbMgV+bvF/QxalBemSOQzAhwQlsyAyyn7slOc968eI/6TZs2oXPnzjqXuGzZMgwYMECqQwSgCRMmSOexsbEoWbKkZF9JKm6kBEeWlrqCbCHJHlIMfXPZvXs32rRpI1YXLCqTw7qRlOPy588vjaOeIAW3sWPHStmJJUBly5ZNsnslrG7fvi31aWhCnZhG+7RkyRK9zZVtQckSVlnRTG9jPRWIvLZ06VKpFimgkdWmehCGhKUY6dKlY1LU1uJpkhypv+fPn4M+k9qC1NJojmKQWh/NJamC7EvXr18PUm179eqVxm7JjnTlypVIzyS9eXAEOAIcAY4AR4AjwBH4GhyE8Kv/ciA4ArJAwIapvNiyt8Z5qCLwLeoj4iK4mpMqKvzMFBFIZW0PCyeu8kJ7d/PZY3yKijTFbUySOZuCDSGpQKyavwiH9u5nVmfM60wtUllYoGWHduj16wCztCEkOLIzRdU8WVzVkOGn6gjQw/FL7OF4LFMYMocwRQsz5X2Z8NtwwTqxXtMmSJ8xA7auUShBmSOhzdbaBmU9CirDw9P/IfCVPee65H0PcRr+fZATSJ0aNcOrF/6wYS8eHbt6AfRvn664fukyRg8YjOw5c2Ldvp0aHWeIJN63XSehG7IMnblska4uhbLJw0fj9PETsLWzw77TiqOmRpzQpgkVRV6RnHmRztFJewVeIiHg/coPgSEfpXM5Jkzt2iayeafGzRHDnMSIKLvt6AHY2XOyNX02y+QrADsbbq8sx+vUnNfECW3mvPtGrr1OnTogApYYt27dQvHiur2o1UlT1Mfx48fFLgTykrICF6VJfUtfkL3m1atXpWr65qKu6KWPACd1nMSJ9u3bY8eOHVKvAQEByJzZOPscIk2RfaoYnTp1Alm0GhvKxDRqu2LFCvTt21dvN7///jtIWY7C3d0dPj4+etsYWkHZApVsYd++fasRn549e2LdungZ6bt376qoxhk63vfW8/T0xJMnT4RuXF1dJZLh9/ar3p4ktE+ePCmQ24icSURQ5aDriux/CTMeHAGOAEeAI8AR4AhwBMLOHEdctPk+FOefAPkg4FihOiydXOSzoKRaCXsQHhv8lPWWkFCRVEPwfpIegYjIKJy7eA2n/72MIgU90bmtZiWJpB855fZo4eiKVDb8QRrt0OsP7/H0reYX2VLuDibNzEzBhvDyuX8xa/xkfAwOlhZt7+AAd6ZME/T+Pd68fCWR3EitZsW2TVot2KQOZJgo7V4A9mn4AzRDtpYU2kipTe5hihZmynty4/IVDOvdDzbsc7318F/Yv32nWRPacjPFlxxM+YWHZgQevfTDu1B5k166N28DX+ZqQ88hiNTp6KT/e1z4p0+wZ0QTXeS3nq3a4dnjJ7BgBLmdJw4jo45nZmGhoWhZo65AZKnfrAlGTZ2keUNYrjqhLeDVa9y7fQfvAwKR2io1+3fcE/kKeOocT2vnJlxgzWxdSVGVP08ybBM/hofhrp9CadCwFqZXy9Su7S2r12LNIoU4Soce3dDnt19ND/RkmLGTnT1K5NGtnJkMw/IuOQLJjgAntCU7xPIZIGvWrCACFgX52IeHhwtvYuhaIb2xSOSr4P9u+JA1JaXpiykRszw8PKSyjBkzCuQgFxfdDyyI3OPEviiTzaahc5k7dy7IllSM1atXo1evXuLpDzsWLlwYDx48EMaj9b57987osc+cUbVonTVrFkaOHGl0P2PGjMGMGTOkdhcvXkT58uWlc22JRo0a4fDhw0Kxm5ubVuUwbe215RN5jfoT33ItXbo0rl27prE6KQNu2bJFKqN6VP9HRlRUFBzYzUv6PFLUrVtXIJUl9xweP34MIhXu379fZSiy/1X+jKsU8hOOAEeAI8AR4AhwBMwKgagnD/D5uYJ0b1YL54uVFQIW9o5wqlxLVmtKysXEhTHyxJfwpOyS95UMCFy/dQ8nzlzAyTMXcenaLcTEfBVG8XTPjQeXjiTDiCbUZSoLZjfqziyFdSt7mNCKvmuqMbFfcZnsjGSu7KIMkinZEDYsXwUR7D4oRVZ272rM9KkoXKKY9CD4wZ27mDpyDALevBHqtO3aGf2G/yakzeU/jrZ2KJnX01yW+93r/Bj+iT0cJ3K6vMMULczEHaEXinu0aIMXz33RrV9fdOvfF6sXLjFbQhu9Rl3WoxDSWCetS4qItxyOwZ/CcO+FvEkvyoqLZPM5YtJ4nUQ1Q/eVyKILp88SqvcY2A9d+vbW2lS57uKN61CkpHbRDWVCG5Hk3gdqVrlu2KIZBo4aLii+aR1YRgXZMmRC3ixuMlpR8i6FnllefvwAX77GJO9AP7F3U7u2Z46bhGN/HRAQm7l0ITwKFsTBPXtx5/oNPHvigxy5c8GzUCE0ad1SSP9EaH/o0Plcs8E1XcYfOiYfjCPwIxDghLYfgbIMxnjP3jbMlCmTtJICBQrg4cOH0rmu9X1R4wAAQABJREFURLNmzfDXX39JVe7cuYOiRYuif//+WL58uZRPFqKkvKUvyIaRlMHEMGQupGDWpUsXsYkwtrK1pVSQjIkvTPqU3kT5+lVxA7t69eo4deqU0SMuWrQIgwcPltodOXIE9evXl84NTSgT0+hNjFD2ZgtZiOqLnEwe2t/fX6pGBMW0TNL1e4PU4VatWiV1M3HiREyaNEk6V06o299SO7Kh/ZFB1rjKJDqa0x9//PHDpqBuz0pkyXv37v2w8flAHAGOAEeAI8AR4AikXARi2QOyT+dPptwJ8pl9FwIv2Nvkp2/dwd1nvhjcqhlyZjFO8fm7Bv+BjdMwO6M0efiDcW2Qf/schrhPCuKEtjpyyJ8+fwV27DuMr/8RwbStiX7TVqtUDkvnTNRWRcp//yEYnfoOx8tXb4U8C0tLFC3ogcWzJiB9Ou0v2N194I1x/1uAZ77+8S9ilSiCTctnS30rJzr0Hopdfx5VzpLSObO74tnNf6Rzc0yksnGGhWNWc1y61jU/8H+OoLBQreVyK1B+cJYrbx50ZYSR4qVLIm369Aj5+BE+j7xxcPdewepPXDupJB2/dlE8FY4Hdu3BmRMncfOKwskhQ6aMyM/ukVhbW6FkubJo1KqFSn1SWdu5YTNes3tbxB/0vv8AQf+9cFqncUPUqF8XZHkmBr3IWKd0efZ3KIY9LCuAeWtWwEHD/TPqp1/HrvjG6tPfpN0njyKD0r1UsT+5Ht2zZoNbev4AzZj9vfz4Pj6zz5Wcw9QszJT3YtemLVg2Z57CZpSps6WxtTVrQpuLvQOK5c6nDBFPqyGgIL3cZ6QXxfMftWJZnNK/taRaKIoS5GbP6Zq0aYnCxYuB/i23SiThkWy9W9aoAyK7Z2FOONuPHZRI4+rA9WnTAU/Yd4RsOXNgy6E/1YtVzjcsX4kNy1aq5NGJk4szwkJUv3O5ZnNjdqeLzYL8Uso9PxzS2CbAhWdoR+B5wGu8DDJeoER7jymrxNSu7YFdeuD+rdvC34nFG9di6uixIBtS9aDfDoPHjAIRcOUeFuz3h1f+wrCyTC33pfL1mSECnNBmhpuemCUT8apmzZpS0zZt2mDnzp3Sua7EvHnzQGQfMYjE5uXlJZCBROtEshC9dOmS1i+pYls6/vnnn2jevLmUZchcyK6xdu3aUhtSIiNFsh8ZZItZrFgxachff/0VCxculM4NTZCy3Nq1a6XqL1++RLZs2aRzQxPKxLTcuXPj+fPnepsS6U1dQe/cuXOoXLmy3ra6KhA2JUqUkNTObNkNAiIukiqgpiDi2IgRI6Sifv36YdmyZdL5j0hs2LAB3bt3l4ai865du0rnyZ2gH420h7T/FKSaSKqF1on80Zjc8+X9cwQ4AhwBjgBHgCPwYxH4dPE0YsNCfuygfLRkQSAiKhqnbt4WSGxnbt6B71uFajYNNrVXNwxs2SRZxv3ZnTpVrQsLpvbCQwsC7PdAbLAPcx1VKEZrqWXy2dkLV8HbwPcGrYOU4N/7XIazk+4Xtc6cv4Jazbsl6LNHx5ZYtWBagnwxo0TVZrj38LF4KhwtGRnu3ZNLGsf0qtMGpNDmYG+HcqWLoXL5MliwfANCQsPACW2AhXN2pLKyV8HT3E+C2L/bD/x9zQIGU7MhHDd4GJ56P8a8tStBD7y1xdBefRmxTuE28L9F81CxejVtVWWVTwS+8sy6zIrdm+JhOAK+gW/g/16zWpDhvaTsmqZmYSai+ZE5yxAZLyI8AiOnTJQehJuzQpunW05kSZtOhIgftSDwjJFeXsmY9ELLVlY9U4aB/i1InzEDsjAl04JFCqN4mdIoVroU7B0M+76nTHSfu3o5SnmVU+5eSJPyUs+WbYV078ED0bFXjwR1lDNIwYmUnGxsbATCeqny5Rh5vjQjnGdE6McQXDx7DktnzwXZolIUKFoYyzZvSBLVOeV5pKQ0WYOTRTgP4xAIj47CjafexjUysdqmdG03r1Yb9G81EdasrKyEa5j+1hRkYjp27Oh97z4Cle6dEamteXvF3w4T2xaDp5vByRmFcuQxuD6vyBEwJQQ4oc2UdusnzpWIV0OGDJFmMHXqVIwbN04615UgO8iyZctKVTp16iQofBERioJuOl+5ckVF7UqqrCFBY0+YMEEqMWQun9gXUrI+JZU0Cjs7O8Eq83uUxYiMRzevDY2tW7eC1i5GYm1PCUvRipPmL9q5iv0acgwJCVFRVWvSpImKip62Ps6fP5+AvDZ58mSV/dDWVld+jRo1cPr0aakKfdbmz58vnasnrl69CiJBilGISccSKY4+S4kNY/dTXSWOFNtKliyZ2OET1a59+/bYsWOH1JbsbAsyaV0eHAGOAEeAI8AR4AhwBD4zC6Mob9NTbz1+5Tqmb96OyOjPCTbRmt2kKpo3Nxb/NgCp2ffwv6/dYHV3IDwySqUufSdsV7MqfmvbUsg/zUhgqw4cgV9AAGJjFeSfbJkyYP6gXzSqm/WaNR8PfP2YsnJsgn6bV6mI0Z0UN8GmbNiKi/ceIJj91vgW9w02TAmmBrM7mdIr4UsOt32eYeTyNQj5FC69zS52ntbRAf/r0x1lCiRUI3vO3jCtO/R3BDECjKYY37UjhrZTrFNTuanmpU6XAQ5lv++lGVNduzHzjgt/i2/RqsoCxrQ3hbqkcHbw2ClERUcLSkqXmW1n4PsPwtQb1K4q3LymkzQ21vAqUxyDenfWuyz67bd972HsOXAMh47H/w51ZDe+3zw6D1t2U1w97tz3Rqnq8S/WUfkv3dujUd1qqFezinp14ZzsRZ/6vkC+PLnYC0iKewciQc/sCW0WqRV2oxqRM99Mshu9zP7tjmGfUbmHKdsQ6tqbRTNmY982xX0afZZpuvoxtbL0js4onJM/QDN23yI+R+O6zyNjm5lUfWWCiinYE4rgilZmeT09sGbXNoncYq6ENvp9VYGpvlhaGP4sRMTS3I7mQHqhPSXy9oq58wWlNF17TIqmfYcORqOWzfWKWdy+dh1DevQRuqtRrw4mzJmZoOsljHy2Z/NW4TnQrr9JCVW3Mmg0+w1x/tRpgRyXNp1mQuY7poBOqm+kDksxaPQItOzYPsHYcskgq1GyHOVhPAJEaKNrXM5hCtd2JBP2aOCler+oRNky7G/GDIjXOSkmr1u2AptXrhG2y469ZLbpwD5ZqycXypEbGZy0K87L+XPL1yZ/BDihTf57nCQrVFcFI5W0pk0Nk+gki00iXoWHhwtzIbZ0jJKcOllFKltN6pswKbLt3r1bqkZ2pkTI0hd169bFiRMnpGpEBtq2bZt0bkyC5k8qcUQuUybX6epj9OjRmDVrllTl8uXLKqQsqUBHgmwOHBwcEBWl+NJUpUoVnD17VkcLzUXqxLSxY8di2jTtb6KLvZC6HlnFKgeRA+/fvw9SeUtMkNJfu3btpKakAPfo0SNkyZJFylNPkDqZK5OeDmAPJcUgbEeOHCmeGnX8wJj8tWrVEkiaLVsa9kCwTp06+Pvvv4VxiNhIn+80Gh58GDIRUick1UBjg+a6b98+qdnr168FXKQMnuAIcAQ4AhwBjgBHwGwRiGMPyMLOHGPqTd9MCoM+sxdg92nFiy/aJn5tzRK4u7nit0UrsOFo/Pd75fpu7M3w+5sUdvadpszC4UtXlIuFdIl87ji5cBZIll+Md+wt7fwdeyYgnYnlGZyd4LNjA3TVmzuwL3o0rCs2EY5ztu0WiHoqmUonw9q1wriuHZRyFEkiwtUcPBJEcsiRORPKFy6ANFbW2HhM8T1UroQ2u8IlYJ0tVwI8eIYqAt9iIhEX6q+aKfOzxu374uhJxd+I9z5XkNbFKdErXrlhBwaMmCw8XHNixNLQsE/YsXY+WjWpl6DPsdPmYdbC1XBhfwNIYY3i0vGdKFOyaIK6ujI4oU2BTirbdLCw5w/SNH1WfN68xJvgIE1FssozZRtCXRsxZeTvOHX0uFBl6ISxaNLasHtMuvo0hbKC2XMjozN/gJaYvbr57DE+RUUmpqlJtDE1CzMC9eHdexjQqZvwe0BdJcpcCW2ZXdIiP/9ubvA1d/3pI0QwIpU5xIvnvrh38xbu374DH6Zk+ublK0RFJvyb1qRNKwwdP0YnJPTMh74fvPZ/KViX7v3nuGANKjai54xkS0rKamQNPnPZIrHou48njxzFtFFjhX7ysPsE6/bt+u4+U2IHdOeDLAmtU1ulxOml+DmR+iKpMJpDpORr29/XD12atJC2wYXxD7Ye+YupQTpIeWJi8vDROH1ccd+wYYtmGDE5XixHrCOHoxV7Ru2Vv4jK/U05rIuvgSMgIsAJbSIS/KgTAVLDIlUsMcgOMk8ew9+8UyeTif2kY29FPH78WFBPE/P0HQsUKABvb2+pGlllGkKmIuIXKYERKUwMIsa1atVKPDXoSG91dOnSRSLVkfXl7Nmz9bZt1KgRDh8+LNQj+eWwsDCBnKa3oVKFJ0+ewNMzXrlhwIABWLJkiVINw5Jkz0ltxSBSGREF9QVZe65YsSJBNSJ3HT+uuGGXoFBLBv1AIRIaKf2J1rOECxEUGzdurKVVfPbixYtBtq1ikGw0qaSRWpsx8e7dOzRo0EBoS8S0devWCfurrw8i1L19+1ao5uHhIXyO9bVRLycC2i+//IJDhw5h48aNBo0r9kGYpU+fHmQDS+HI3naiNGHIgyPAEeAIcAQ4AhwBjgAhEH79Ir4GmZaN0S1G4Fpz8CjC2BuXj17449lrxfetSsz6I3O6tCjunley2PR5+RqrWd2jV67i1TvFw//MaV1Qr1wZNKxQFrXLlBI+CI/8/LH60FEEMxLKiWs3EfX5s/QBWTC4H7rWqy2dU2LLiX9w7vY9QSXuOfu+R+0p2tSoiobly6JJJcWLCJuOncQFptDmH/gOlx/Eq2ukY3aH19csBSmviUEEuBV/HcbTV6/Z75FvzD70ttA/Ee+aVa6A3o3ra1SLo/bUNpb9hsmaXvFGOanYtZs0XehaloQ2pgDhXL0BsyLkN9nFz4+uY2zwUyDuq64qsipLSkLbwpWbMGzcDFgzdcUOLRtjw/Z9aNawFvZsWJwAM/eSteDH/ub06doWqzbuFMpPH9jMbERLJ6irK4MT2hToWLjkQqrUaXRBZbZlYZERuPX8iezXb6o2hLo2Jpq9fNq2bkPhQTvVW7t3J/J65NPVRBZlpJpbnj0ct0hlIYv1/OhFvP7wHk/fvvrRw/7Q8UzJwowUXX7p0AWPHzzUSJgxV0Jb0VzuSOug29L9h36oUvhg5kR60bQVQex5y/EDh/Dnjt14Hxh/P0KdIKqp7ba167FqgeK7+MCRw9Gqc/xLX//+cxrjhwwTmk2ZNwdVatfU1EWi8ujar1euEj6zZ3+pmX32sWsXhWOiOkvBjdI5OKFIrrwpeIYpe2pfvsbg8uMHWl+ATNmz//7ZpZRrmyyCG1WoKi2o+4Bf0PUXhbqjlPlfwvfpU9DvDorc7u5Yv1+eZFVX5nKQzzX7f6vmB46A/BDghDb57WmSr4gIYESWifzvzYrEEGf+97//abQoJWIVkaQMDSKTkUKZSIAydi6k4DVnzhxpOCcnJ8ydOxc9e/Y0iAhESmSk7EZHMSpVqiQov9na2opZGo85c+YUrFapkAh4RMQzNoiAp0w8I3JZ3759je1GwFyZmPbw4UMQUVBf0FovXLggVCMCGRESRVJXx44dsWjRIiFPXz9kk0qkQJHgJ9YnFbsZM2aIpzqPRIirV6+eiupejhw5QFauRLAzJIiE17VrVwQq/bDq0aMH1q5dq7M5KbqRha0YpJS2Z88e8dSgI43dtm1biZBmbW0t2KyqK+Bp6ozWPmjQICxdulQqpuuIriceHAGOAEeAI8AR4AhwBEQEvjCVl8i718VTkztOXrcZC3bvF+Z9atEclMiX8MbrwQuX0XPmXMQwe9DszG7kr5mTkTtrFq1rLdG9H7Mejb+pntHFWSCfOTH7AU2xeO9fmLBmo1D05s/tsGXfgdXj7O27aPb7JJXs3o0bYHb/Xip5yielew0QyHqtq1fBqpFDlIv0puVOaLNiFij2xcvqxYFXUCAQF/Ee36IUFpzmgElSEtpIcY2U1+ztbLFv01LUbdWDWQdbC7ajzoyYKsbVG3dRoV5buOfOgbHD+qP7wNFC0bHda1GrWgWxmkFHTmhjMFnawDJtboPwMtdKV588RNSXePK1HHEwVRtCXXuxcv5CbF+n+M5QpmJ5zFkRf89GVztTL8vKHqB58Adoid7GGKY4dOnxfdk/HDcFCzPaxMN792POpKmCnSEpNOXKq/pCvzkS2mzYSyblPAoZ9Owk0ReCzBqaO+lF3E56hjdr/CScOKgQeajXtAlGT5skFms8fngfhDa16wvP/9TJJ2MGDcHFM+fgzF5i28PU28gJKimjb7tOApmV+tywfzdysZfp5BYFmNJiJqa4yCPxCNzze4bgcIVid+J7Me2WKeHabli+CiL+c4WbumAuKtesrhFUIqvWLl0eX5nrmpzJqiXyeMDJzl4jBjyTIyAHBDihTQ67mMxreMoYzPnyxb9R6OXlBbJINCb+/fdfkD2mcpQoUQLXr18XfiAq5+tK37x5E6VKKZQWqJ6xc/ny5QvKlCmDu3fvqgxTvXp1kOKXNnWva9euCWSh7du347OSogO1O3jwIOztdf9DQcpZZKUpBlmkkhKZsTF+/HgVa1Ail1WoYNwNdBqzYsWKuHjxojA82WSSXSapk+kLZ2dnQVmO6tH+kcIaqe8RwYqCbEJJMY4U1oigpR4hISEgu9qJEydK5D6xDpENZ86cadSP4zdv3qBIkSIggpxyEEmNSJRubm7K2UKaCJpEJiPyFxHqxLlTIZEDyVZVn8rZmTNnQHsvxqRJk4Q1ieeGHD9+/CjsA9mrKgdhR6p/lStXVs6W0leuXBFw379f8XCXCrJmzSpck0Sa5MER4AhwBDgCHAGOAEdAROAbu4EceuoIEGua6k36CG37zl1AX2ZR+pWtk0hsB2ZOQbZM8S8diDgoH0VCWzH3PLj3zFew8hzQogmm9e6mXE1KG0toIxvTWz5PQWol/y6dh/w5s0t9KSc4oU0ZDdW0fUkvWGXKqprJz7Qi8O3rZ8SF+Gotl1tBUhLapsxegilzmJoisy0N8L6IHEWqIvD9B6xZ9D90ax9vYUIqbqTmNnZoPxTM746OfRTKEH9uWYZGdeN/FxqCNSe0AansM8LCNr0hcJltHf/3AfANfCvr9ZuiDaGuDXl09z4Gde0BskNLxZRGV27fDI+C+l8c1dWnqZTxB2jfv1P3XzzHh08KB4bv7y1l9/Diecq1J6QH4x0bNEUIu2erzR7RHAlt2TNkRp4srin7g5UCZydH0gvZ/JFCWhbmXPO/xfMNUjALfBuAtnUaCDvkWaggVu7Yone3xv46FBdOnxHqLd+6CQWYWntw0Ae0rlVPILq16tQBA0cN19uPsRV6tmqHZ4+fCM12njiCzDpelDO275RQ35J9P6lAloTsyCPxCLwL+YhHr/wS30EKbGmK17by9frHqmUoXd5LK7KtatYDqctR/HnuH5BFqZzC1toGZT0KymlJfC0cgQQIcEJbAkh4hjoCRJxp0SL+Zm7v3r2xatUq9Wo6z4kERmQokQxGhKHz588bTcYiW8Zu3bpJYyVmLqSuVqtWLRVVLrFDmmOxYsUEkhTN1d+f2Rwxe1X6v3qQutb69euhT5mN2hHxjNTNxBg7dqwKMU3M13ds2rQpDhw4IFQjDIkgRipzxoY6MY2IgvrixYsXyJUrl1SNFNZoP9RV76gCMd3JGpXIZmTNGRAQgJcvX4LIWEQqVA6qS8puxij1KbcnYiCp5kUxawf1yJw5M4oXLy6ozxGBjNZAFreiqpxYn8h8pA43depUvWQ2aqNud7p3716Va0TsV9+R5kOERCLmqQeRSAsWLAhSnaM3HqjOgwcP4OPjo1KVlOLITpfq8uAIcAQ4AhwBjgBHgCOgjkDk3Rv48kZhmaleltLPdRHadp06i/5zFwtWnPmyu+HAjMnI8p8lp651iYS2znVrse99ANmGWqW2xIXlC5AvW8KXIYwltO2aMhZ9Zi9ECHsgVq1EUeyfPknjdDihTSMszGbUmtmN1ge7y665As/ViEAsEdoYsc0cIikJbWOmzsXsRWuQKUN6QZXttzHTsXj1ZtSsWh7H96wT4KQXonIVq443Ae9w99+DePLMD626DRLKdqydj1ZN6hkFOye0MYG2dEztwiJpFTWM2gQTqBzN7ptcfcLsjExgrt8zRVOyIdS1TrJTI1UXethO0a1/X3Tr11dXE9mU8QdoSbOVQWEheOBvPuR0ddRSioXZgd17MW/K/2BtY41lWzbChTmTqMfWNeuwf/tOIZsUnB7cvYcvn7+geXuFnZl6fTmcl3YvAHv2QjwP4xB4F8pILy/9jGuUwmvv3rwVS2fPFWY5YtJ4NGzZXO+M6blGrZLlQCpJ7vk9sWb3dr1tLp39F78PHCzUozForB3rN2HFvAVCXnJYehMhvV7ZioKKkyN73nbwwhm98zS1ClnSpoenWw5Tm3aKmy/9PrzofU+4F5XiJpfICZnitT15+GicPn5CWPFv435H07atNa4+himz1WUKbYITnUyv7VzshdCcmbQ7VWgEhmdyBEwMAU5oM7EN+xnTnTJlior6FJGPyO7Q2KhatSrOnTsnNBPJUMb2MXz4cMEiVGxHxKKBAweKpwYfSTFtElPVIjUx+rJqTOTNm1doR3aXhgbZeyoTtkjprV27doY2l+qRVamfn59wTuQyX1/jb3aoE9NIzWzDhg3SGNoShw4dEpTXxPI//vgDw4Yp3kxfs2YNBg8eLNnSinX0HUndbf78+QbZnerqi4iHQ4cOBRHLjI3y5csLqmxEZDQ0+vTpI1ibivWJJOfh4SGeGnUkdTki0xGGympxhnRChL2jR48KanmG1Od1OAIcAY4AR4AjwBEwPwS+Br1D+PULJrlwbYS2LSf+weAFywR1tYK5cuLPGZNA1qGGhDKhbXy3jijVcwA+RUaidpmS2DVlXIIujCW0nVwwCzce+2DU8jVCX1smjELD8uUS9MsJbQkgETKsc+SGXcHimgt5rlYEvkUFIy5C8cax1koyKUhKQtvQsTOwaNUmuGXNjBd3z+DK9TuoWL+doF5O51mY4uO5i9dQo2kXFCqQD3fOHcCRv8+iSYdfBDQ3LJ2FTm2aGIWsuRPaUlnZwcKZP0gz5ENzx9cHIRHhhlQ16TqmYkOoDeSI8AgM6dEbPo+8hSpkNTp72WJBpU1bGznl8wdoSbObccz54jJ7OB7DiB/mHD/bwmzKyN9x6uhxo7eAbEk3/LnH6Ham0MDR1g4l83qawlRT3BzlSHrZuXEzlv8xX8Ca1NaWb9ukV+3rycNH6NO2o9BGJKfp2yzCjmxHg969h62dHfadPoFf2ncGKTyS+umqnVv1dWF0+Z4t27Bk1h9Cu+JlSmPBOuMEPYwe8Cc0KJY7H1zsHX7CyPIb8vHrFwj4qOoaZcqrNMVr+86NmxjcrZcAe7lKFTFr+WKNW0C/NYb2UrxoUrh4MSzZvF5jPVPOLMfU2dIwlTYeHAE5I8AJbXLe3SRaW+vWrbFnT/yPstOnT6NatWpG9y7aZZKi2JMnT0BkHGODCFAnTihY19SWrB+JKJfYIMWrIUOGgNZEP5q1BSl40ZpJla1z584gm05jYsCAAYLFpdiGVOK02ZuKddSPYWFhgsqdmE/WlKJam5hnyJEsUsnyVAxlYpqYp+k4ffp0kLKcGGTbWadOHfFU2NM5c+Zg165dki2pVKiUcHBwQMOGDdG9e3fBrlSp6LuTJ0+eBJEe79y5o7MvUtVr0KABOnTogObNmxukyqbcIZHgLl++LGRRX2TZ+r1SzVevXsXSpUsFG9QPHxRv9SqPqZwuXLiw8Lnt2LGj0Z9F5X54miPAEeAIcAQ4AhwBM0CAPSALPXMM3z5Hm9xiNRHa1h85gWFLVgovAhTPlxd7p01AOidHg9emTGhbNKQ/lu47gHGrNwjtSV2tdplSKn0lhtBGdqaVBwyF94uXghXqpZULYWOlqkbECW0qMEsnDl5VkdoloRqGVIEnNCMQ9xWxwU81l8ksNykJbf2HT8KqjTuRO0c2+Nz4W0AqX6na8PV/hfnTx2BQ784YMGIyVm7YgSljBmPMb7/g5JmLqNe6p1B3xbwp6NVZ85vg2mA3d0Lb/9u7DzC5rvJgwN/uSruSVlr1bvVqWe62LNvEuMS0ACEhJCSEJBgTik0voYc4EIwpoUPA4ackECAkgSTYBmNqXGTZcpFl9d67VlpJq23/vSNWVteudnb2zsx7nsfemTv3nvOd99yx5J1vzlfZf3RU9OlYAvKpDMvl+OZdO2LJhrXlMt3ch9RPProgFj72eCxbvCQ2rlsfB5KE8+PbqcoAHn1e+mXBP3/hS2LD2nXRu7o6fvCze6LuqMT39IutL73+ObFn1+6Y+zvPitu/+NmjL+/w4/0NDfHO194STz3+RO6aSVOnxme+/tWoS6o/lEvzAVr+VnrZxnWxcef2/HWYgZ6KrYTZ7e//27j7h//dabnn/f6L490f/lCnryuGC6aOPifGDh1eDKFmMsb0z/H0z/NSaf/z7/8Rn/i7Dx+ZznXPfU68/2MfyX0Z5MjBox40JTvOvuOv3xBp4kna/ubvPxTPf8kzn0sddeoJD//5c1+Ib33ln3PHX/hHfxjp2Gl7y/veHS95ecd2REx3Zlq44LFIk+/61dbmrj/Zv9I/x9/26tceqS718S9/IdIE9VJqNclO6HNnnFdKU+rRuexu2BuPryqd//8utvd2++KnCW3t/325/QufibnX/E77S7mf6d/5b33lq2Lxwqdyz1/71jfHn970l8ecU+xPBiZJqhclyaoagVIXkNBW6itsfh0SSMuLprtspQluixYtyu2ClpZyHDt2bIwbNy6uu+66GDFiRIf6KveT0tKfd999d640ZrobXJqIN3r06Fzp0anJL/duuOGGDpVp7YpjmmCWrmP7em5Jyj+MGjUqt57pLnfXX399pIl1WWxpYmVajvfJJ5/MlUZNy7WmLd2RL/0nLeU6Z86cLIYuJgIECBAgQCCjAgeSHR8aVxffL9uOT2h7+OklR3Y+u3zm9Pj3JJmtrrZfp9SPT2hram6Jq1//lli2fkOu5GhaejQtQdreziah7dIZ0+IXC56IP3jvh3Ld/O2r/jze8sd/2N5l7qeEtmM4ck8q+9VG3TXPfGHmxDMcOZ1A65510dbUcLpTSuK1fCa0verWd8e3vvvDmD5lYix68K6czwc+8un46Kf/Ka647ML45X//a6QJaNt27IwlD98TUyaOP7JjW3rypz/6vrj15j/vlGtZJ7RVVCTlRpNftldUdsqsXE9uaW1JyhktzJXHKVeDrJQhPJl/msz2rtfdmkvAS18fl+wY+9mv3xmDhw492ekleWxgv+QDtMk+QMvX4tbvb4gFK5fmq7tM9FNsJcxWL18RP/7PH572S+9p0u2SpxblfF+UJNn0T75Y86I/emmMGXdOJszzGURF8uf2lTNmJ/9v1Cuf3ZZVX+lOq+mOq6XSfn73T+Lv3vnuY6Zz1bXXJCV3/yRmzj4v0lKd7W3+Aw/G1z7/pViUlOVN2yVXXB6f+MqXOrwpwMbk/89f8YIXH1PRJi0H/IP7fnLMOO3jneznxz/09/G/P/jPXBnhy6+6Ks678PyYNnNmTJs1MxfHmhWr4r6774n/+u73cyVR0z7SsoVp+cJSaxOGj4qJI0eX2rR6dD4PLnkqGpsO9WgM+Rq82N7b7fN+9KF5ye5rh3dP75X8WfWat7wxrn3OjTFk2NBYnnxBJi2RnP65nbb07+pf+4/vRe/jvmza3lex/pyelBEenZQT1giUuoCEtlJfYfMjQIAAAQIECBAgQKCsBVrqd8fe+39edAZHJ7S97Lpr4vs//9WROfzV858Tb3v5S2PciM7tGHB8Qlva4U8ffiT++IMfyfX94df8Vdzyh898a/xsE9rSzv78to/F/z7wUNT27ROP3PmFGDlkcG6M9F8S2o5QHHnQZ+rM6DP13CPPPeicQFvjnmjdu6lzFxXh2WeT0LZ9564YOnjQCTtz/+nNb4vv//CumDVzajzx68M7sjz19LK48JrD/w34/B0fjFvfdVtcdvH58eBPvpfTai9Lmj65/W/fEe+49fBubR2lLOeEtoqauqgcMKajVM5LBJ5etzq27tlV9hY9XYbw+AVoSL5EmSazte/MNjr5Muxnv3FnDD+LShTH911Mz32Alv/Vmrd0URw41Jj/jnuox2IsYXYmqq9+5vPxr3d+LXfaj37z85LekXHogIExe8LkM5F4/QwCDyVJLwdLJOll3m/uj3e9/taTzjhNgBw7flz0SpJFNiXJaI0Hn9khfsw5Y5PypN+KgcnfxzvT3vvGt8T9v3jmdwDPffEL4z0fua3DXXz369+ML33y0x0+P03O++AdH40+SUWeUmuXTzs3+tV0rupUqRnkez6rtmyMtdu25LvbHumv2N7bRyP97Md3x+0f+FCkO0K2t4rKyiNJqumx2mRzk9u/8Nk4/5KL2k8piZ+VaeL5zPOjV1JhTiNQ6gIS2kp9hc2PAAECBAgQIECAAIGyF6j/zb3Rum9vUTkcndB2ssD7J79o/pcP/k08+6ILTvbySY+dLKEtPfGPP/jhJLHt0dyOb/OT5LPhvy1N1pWEttWbt8Tcv35T8q3dpnj5DdfGl97xpiMxSWg7QnHkQd01N0ZlstuLdpYCba2Hy44mP0u5dTah7V++96O46Y3viRuvvTr+97tfOYbmD155S/z33ffFReefG/Pv+48jr110ze/HwqeXRm2/vtGw/0B8/La/ibe+/q9yry94YlFcfsNLc48/9O43xfvf/voj13XkQTkntFXWnRMV1d7jHblP2s/Zta8+nli9ov1pyfwstjKER8OnZUrf+do3xNKnF+cOj5swIT5555djxKiRR59W8o99gNY9S7x22+ZYtaV0ktOLtYTZ6Va3nBLazhs/KYbVdS4B6XR25fra6uQ9vSZ5b5dC2751W/zRDc/NTSXdca3/gAHxwK9+c0wiydHzTMt9v+LVr4qXJDu41dTUHP1Shx6vX7M2bnnlX+VKhKfXf/X734nxkyZ26Nr2k+798V3xjS99JdatXtN+6ISfQ4cPize9513x7Bt/94TXSuFAXbIT+sWTp5fCVDI1h/2NB+PhZU9nKqazDaYY39tHzzXdhe1Db39XpPM4vs2++KJ4/+0fjlFjSu+LVSMGDo5zx008fsqeEyhJAQltJbmsJkWAAAECBAgQIECAAIFnBA4mJYwOLn3qmQNF8Oj4hLbfuXB2vOEPXhTfuudn8eMH5uVmUJ2UFfjRx26LK5KyIR1pp0poW75hY1z1ujdHWoL0L573u/GZN78h111XEtrSDm77+r/GP373B7mdoX76j7dHWo40bRLacgxH/lU1aHAMmHvtkecenJ1A696N0dZYf3YXF8lVnU1oe+cHPxb/+KWvx4D+tbFr1fxjZvn8l90cP/3F/8Xll1wQD9zz3SOvfeafvhlvf/9Hc8/79umTKzc6ZtSI3POjd3B771tfF7e9981HruvIg7JNaKusSsqNTk2IKjrC5JzfCrS1tUVazuhQc1NJmRRbGcJ2/F07d8bbXv26WLX8cBn3SVOnxqfu/FJZlRltt/ABWrtEfn8eTHYXmZf8fb0tv932WG/FWsLseLA0CfeBX/06l7Tz8P0PxuPzH8md8hevfU1Mnj41Lrtybi6x5/jrivl5uttLuutLmryqdU2glJJeUonvfO0bsXDBY/HqN90Sk6dNjXTX0keSXck3bdgQWzZtjr79+uVK8Ka7ss04b1b0q63tEuChxkOxctmyXJ91AweedV9bNm6KJx5dEDu3b489u/fkSo5OnDo5Jk2ZkkuS611dfdZ9Z/3CaWPGxZghw7IeZlHG9+iKJbH3wP6ijP34oIv1vd0+j/T/m9avWZPsoPxkpH9uj580Iaade25Mnjol0h3bSrGlu6imu6lqBMpBQEJbOayyORIgQIAAAQIECBAgUNYCrQf3R/0v7ikqg6MT2p4z59L45vveFTXVvXNz+PJ//U+8558Ol/sZm3yj+oEvfzoGJL88P1M7VUJbet0H7vxGfP4HP8x9cHPfZz8eFya/4O5qQlvDgYNx6c23xJak5OHlM6fHPZ/6aC65TULbsSvVd9aFUTNeSaNjVTr/rO1QQ7TWr+v8hUV0RWcT2t707r+PL/7zt6N/bb/YvfrwB9Dt073uxa+MXz8wP66ac0n86n//tf1wNDU1x1ve+5FYumJ13PSKl8afvvSFR15Lj82a+/zc87e94VVxx9+968hrHXlQrgltFX0GR2X/8trBqiP3Q0fOWbl5Q6zbvrUjpxbNOcVYhjBNZnvLq14Ta1auyjlPn3VufOKfvhjp7jPHt+bm5li2aHHMnD2rZD9AO3/ClBgyoO74qXueB4HHVy2L3Q378tBTz3dRzCXMjta79S9uyiXwHH3s6MevuPmmeM2bbz36UNE/TpNf0iQYLT8CC5Ivl9Xvb8hPZ3oh0AmBNCl17szZ0buqVyeucmpHBTbs2BbLN63v6OnOI5A3gfTLvXNnzM79fjFvneqIQIYFJLRleHGERoAAAQIECBAgQIAAgXwJ7Jv362jeuT1f3XV7P0cntKUJZhdPm3LMmO//6tfjC//xo9yxm37vefHJW//6mNdP9uR0CW179++PS199S2xLvrF9ZfIh9I8//uEuJ7SlMXz3Z7+M133iM7lwvvyON8ef3PBsO7QdvTjJL9kHXvf8pBRh58vQHN2Nx4cFWnYmOwe1NpcsRz4T2q587p/Ew48+Edc+64q49z+/3iGzNes2xpRLbsid+4ZX/1l89vYPdOi69pPKNaGtctDEqOjVp53Bz04INBw8EPOXHy5v2YnLMn1qsZUhbGxsjDf/1c2xeOHhnW5nX3RhfOxLn4va/v1P6nz7+/827v7hf8erbnld/OXrzvx3k5N2kuGDPkDr3sXZvGtnLNlw6tJ43Tt6fnsv9hJm7Rpf+cfPxg++/W/RePBg+6EjPwcNHhzv/LsPxNXXXXvkWCk8SMsTpmUKtfwIbEz+H3zZxtL+0kl+pPSSb4FhdQPjPF8cyzfrkf6aki8xPLBkYaS7g2kECikwdujwmDr6nEIOaSwCPSogoa1H+Q1OgAABAgQIECBAgACBwggcWr8m9i98tDCD5WGUMyW0NTY1xdWvf0us2LApt6vazz5zR1x0XNLb8WGcLqEtPfdb99wbb/r0F3OX3fnut8XG7Tvig8nObWnb+F/fib41JyZd/fKxJ+Il7/lQ7px7P/2xI2VFcweSf6W/3HzOW98T85csjVFDh8T8r34+nv3Gt+fiftl118RX3vWW9lM79POeh+bHyz/0D7lzP/CXr4i3vfylHbouqyf1Hj4qai+9MqvhFV1crQ1bo+3AzqKLu6MB5zOh7eJnvySeXLQkbrz26rjr+3d2KIRNW7ZFmpSWtnT3tq98+sMduq79pLJMaKuqjqrBdmBsvwfO5ucjSULbviSxrVRasZUh/MLHPxnf/+YzuzhOmT4tapJyxKdqy5csibRE2vXPf2588I7D5YtPdW4xHj9n2IiYMmpsMYZeFDG3tLbE/YsXRmtra1HEe6Ygi72E2ZnmV4qv902+ZDJn+qxSnFqPzamppTkeTN/Xkl56bA3KdeDzxk+KYXWDynX6BZn3wjUrY8fePQUZyyAE2gUumTIjBvQ9c5WK9vP9JFDsAhLain0FxU+AAAECBAgQIECAAIEOCLQ1N8We++5Kdm9q6cDZPX/KmRLa0gh/9shj8Ufvvy0X7JxZM+OeTx5O9DpV9GdKaEs/ZLjhze+Kx5atiLSU6V8873fjo9/6t1x3Z5vQll78yJJlceNb351Lbnvrn7w0fvSb+yW0/XaRai+aE719MP5bja7/aGs+GK27V3e9o4z2kM+EtrR0aFpC9AU3Pjt+9O0vd2jGO3bujpEzDidg/tkfvSi++aU7OnRd+0nlmNBW0W9YVCb/aGcvsH7H1lixacPZd5CxK4utDOGfveDFsXFd58tJ/clfvjJe/463Zky/6+FcOnVm9O/Tt+sd6eGUAovXr44tu3ed8nUvEOhOgUkjR8f45AsnWn4Fnlq7KrbX785vp3ojcBqB3lVVceXM85UkPI1RPl7alryvFyXvb41AoQT61fSJy6edW6jhjEMgEwIS2jKxDIIgQIAAAQIECBAgQIBA9ws0PDYvmjYXx4fiHUloS8XS3dHSXdLS9rX3vD3+4Jqrc49P9q8zJbSl1zy0aHE87+3vzV0+cvCg2LLr8AcPXUloSzt7wyc/F9+59+dR07t39Kmpjj37GqLcd2ir6NUr6q57QVQkv2zX8ifQsmtlRMuh/HXYgz3NX/Bk/OahR+PAb8t8fevf/iuXhJaG9L63vT769D1x18Sjw/2fe34eD81/PPrX9ovdqx/JvfTrB+bHgicXxW13fCF276mPmdOnxCte9qKYOG5s3Hjd1TFsyOCju8g9XrJ8Vfzk57+JnUlC299/4vAujuedOy3ecNOfxdVXXBKzz51+wjU//cX/xVOLlx+JPT3hjs98NfYm7/1BA+vi7bfelLumIiqib98+ccUlF8Tcyy86oZ9iP1A1eEpEVe9in0aPxn8oKWf0YAmVMyq2MoT/+Z3vxb/e+bXYvnVrh++Dfsl/cz72xc/H+ZeU1nu6NtmZ7rKpPkDr8I1wlifu2rc3nlidlBDXCBRYoCIZb87086JPdXWBRy794bbX74mn1iZ/R9cIFEhgzJBhMW3MuAKNVr7DpF+KfGDxk9HcUhxfHC3flSqdmU8aOSZJPB9ZOhMyEwIdEJDQ1gEkpxAgQIAAAQIECBAgQKAUBJq2bo6GRx8oiql0NKEt3U3t+mRXtbS056TRo+Khr3wuevc6eYJURxLaUpzX3PGP8e8///UxTl1NaNuyc1dcdvOtse/AM2Xjyj2hrfqcCdFv9iXHOHvSdYHW/Tuibf+2rneUgR4mX3x9rF2/qcuRpAlk25c/FNuT9+HYWb8TLaf4wOHmV74svvypw7s+Hj3oFTe+LB55bOHRh448ThPhlj9675Hn6YONm7fGxAuv61TJuLoB/WPz4vujurqEkr96942qgROOsfHk7AQWrlmRlDOqP7uLM3iVMoQZXJQOhJSWGk1LjmrdK5D+nfahpU9FY1NT9w6kdwLHCQyq7R8XTpp23FFP8yGQvq/TpJemU/wdNB9j6IPA0QIXT5kedX1rjz7kcTcJLN24Ljbt3N5NveuWwDMCaeL5FTPOS74oK/H8GRWPykFAQls5rLI5EiBAgAABAgQIECBAIBVoa82VHW1ryubuTZt37Iy7Hpofu+r3JuVEF8T9Cxfl1u2m33teTBk7Oi6aOiWuOn/WCWt58+2fih/88je543/6u9fFDZddHDdedknUJTukpO3p1Wvj/558Kv7hW9+JXXv3xUXTpsSLrpqblN+ImDRmdDzn8kuiX7LrSHvbuH1HLvnsQGNj+6E4PqEt/SbuXQ/Oi3sfXhBfv+snufNe9XvPTT7oHZbbgW3OuTPispnH7tr06e//Z6SJeu3tTAlt9Q3744dJedKdiUdLS2vusqXr18d3f/bL3OPrLrkwnnX+7NzjyqrKGJwkxPzelVfEsCR5pxha/znPil5DhhdDqMUVY2tTtOxcUVwxnyLam9/0vvjmd/+rU4lhx3fVK0lwfeNrXhkfv+1vorm5Ja5+/stPmpw2dvTIuO29b46/fPkfHN9FvPfvPxlf/eb3YtfuYxOKKisrc+d/9TMfPuaapqbmuO73X5nbHS79APNMrSrZpfBFz7su/v3rnzvTqUX1emX/UVHRZ1BRxZzVYLft2RWL1q3OanjiKgOBiuQvTXOTD9Cqe5VQ0m2G123l5o2xbvuWDEcotFIUmDF2fIwaPLQUp5aJOS1Pkl42SHrJxFqUehD9amqSkoQn/t6k1OfdU/Or398QC1Yu7anhjVtGAoP7D4gLJk4toxmbKoHDAhLa3AkECBAgQIAAAQIECBAoI4EDix6PxoyWO7nlU5+Pb//0vlOuRvph6qNf+2JMHHXs9vqrN2+JK17zxkjLsrW3v73plfGWlx1OTJmTvLZs/Yb2l074+Q+vvSle/5IXHnP8E9/5fnzkm985cuz4hLYHkmS7F7zz/UdeP/5BdVJOc+m//b8YWPvMt6LT+Ob+9Zti1abNudPPlNB2x7e/Fx/91r8d3/Vpn7/2938vbn/dq097ThZerOzTN+qe/dzIZRVmIaASi6F1z9poa9pfYrMyneISqIiqockv2ytOvmNmcc2l56NtTRLSH1i8UDmjnl+Kso1gSP+6OH/ilLKdf6En3pCU2p6//OlCD2u8MhZIk/Svmjk7qir9ud1dt8HeA/vj0RVLuqt7/RI4IjBp5OikJOGoI8896H6BecnOqgcOZfOLo90/eyMUSmBmUuVg5KAhhRrOOAQyIyChLTNLIRACBAgQIECAAAECBAh0v0Dz7p2x78HDO3x1/2idG+Ebd/803vPlr8XRO6O195AmiF0wZXL89x23RZ/qE7fX/9wPfpgkoH07Gg815XYqu/Pdb4vrL7kod/k7vvCV+MZdPz0hESBNkBtaNyC+8b53nbDzW9rPtW96Ryxesy76Jt9wXvuDf4leyS5K7S3dTS5NaGtPTms/nv5MY71o+tS4+xMfSfK10qIAz7RfLHgi/vB9f5crkXrzi54fH3/Da5558bhH985fELd86nOxddfu4145+dMhyVw+fstfxx9ec/XJT8jQ0ZrJ06Pv9PMyFFFphdJ2cHe07jucOFlaMzObYhGoqB4QlXVjiyXcoohz6Ya1sWnXjqKIVZClJ3DuORNjxKDBpTexDM8oTXxJE2A0AoUQSN/f6ftc616Bh5ctiv1H7QLevaPpvRwF0t8+zEl2VO2jJGFBl3/N1k2xeqv//y4oepkNVpUknl8p8bzMVt102wUktLVL+EmAAAECBAgQIECAAIEyEaj/1U+jdf++Mpnt2U9z+576JKFtbYwfOSL3z9n3dOyVi1avibSc6OzJE6N/377HvlgmzwY864aoSnZ70bpJINnNqWXHsqTzM5e77KYIdFvmAmkyW5rUpuVPYE/DvnhsVfq+1ggUViD9AO2qmedHuoOTVjiBDTu2xfJN6ws3oJHKWuCCZAfGwf5u3u33wNptW2LVlo3dPo4ByldgUG3/uHDStPIF6KGZHzjUGPOWLuqh0Q1bDgIjk8TzmRLPy2GpzfEkAhLaToLiEAECBAgQIECAAAECBEpZ4ODyxXFQGaNSXuJMz62qbmAMuOr6TMdYCsG17t0QbY17S2Eq5lBsAkmZ0aohabnRY3eoLLZpZDHeh5JyRgeVM8ri0pR0TKMGD40ZY8eX9ByzOLmmpFT9A0sW5nb1zWJ8YiodgZpeveOKZEen43eWLp0ZZmcmB5sOxbwlT/nKSXaWpOQiSf+8Tv/c1gov8NjKpbFnf0PhBzZiWQhcMHFqknjuC2NlsdgmeYKAhLYTSBwgQIAAAQIECBAgQIBAaQu0Jr9kq//VT0p7kmaXWYG+yS4vNckv47TuFWg7tC9a6+3s0r3Kej+ZQEWfQVHZf9TJXnKsiwKrk3JGa5Qz6qKiyzsrkO70ku74ohVeYOGalbFj757CD2zEshIYN2xETB6lTHihFv3xZLfV3cmuqxqBfAukO6lepSRhvlk73N+mndtj6cZ1HT7fiQQ6KiDxvKNSzitVAQltpbqy5kWAAAECBAgQIECAAIHTCOx98JfRsnvnac7wEoFuEEh2bKq79nlRWdOnGzrX5bECbUnZ0eVJ1dGWYw97RqCbBSoHToiK3uVZTrmbaUM5o+4W1v/xAn16V+d2bjr+uOeFEdhWvzsWrV1VmMGMUrYCl02dGbV9/LldqBtg864dsWTD2kINZ5wyEhiRlCQ8V0nCHlvx5paWeGDxk9Ha1tZjMRi4NAUknpfmuppVxwUktHXcypkECBAgQIAAAQIECBAoGYHGtSvjwKLHS2Y+JlIcAr2Gjoj+l19dHMGWQJSt+7ZE28FdJTATUygagcreSbnRKUUTbjEGqpxRMa5a8cY8YfiomDhydPFOoMgjTz8UTz8cTz8k1wh0h0D/vn3j0ikzu6NrfZ5CoKW1Je5fvDBaW1tPcYbDBM5O4IKJU5KShHVnd7Gr8iKQJqGnyegagXwKSDzPp6a+ilFAQlsxrpqYCRAgQIAAAQIECBAg0EWBtqZDsee+u5Ldm/wivYuULu+EQL8LLo3qMeM7cYVTuyLQ1nwgWnev6UoXriXQKYGKfsOiMvlH6z4B5Yy6z1bPJwrMmTYr+tbUnPiCIwUTWJaUL9uYlDHTCHSHwNTR58TYocO7o2t9nkbg6fWrY+tuXzo5DZGXOilQ3at3zJ1xXlQkO6JrPSeQlglPy4VrBPIl0D/ZQfXSZCdVjUA5C0hoK+fVN3cCBAgQIECAAAECBMpaoOHRB6Np66ayNjD5AgpUVcXA618QFVW9CjiooVp2Jb9QbzkEgkBBBCoHT07e49UFGatcB1HOqFxXvvDzrutXGxdPnl74gY14jED9/oZYsHLpMcc8IZAPgTTx5coZs6N3L383z4dnZ/rYta8+nli9ojOXOJfAaQWUJDwtT8FebMvtrLowmlqaCzamgUpbYMqosXHOsBGlPUmzI3AGAQltZwDyMgECBAgQIECAAAECBEpVoGnzhmh4bF6pTs+8MiZQPWZc9LvgsoxFVfrhtO7fHm3JPxqBbhfo1SeqBk3s9mEMELFoXVLOaI9yRu6F7hWYlvy5PWaIHRe7V7ljvc9buigOHGrs2MnOItBBgaEDBsbsCZM7eLbT8imQJr08tOSpaGxuyme3+ipjASUJs7P4yzetjw07tmUnIJEUrUCaeJ7uvJjuwKgRKGcBCW3lvPrmToAAAQIECBAgQIBAWQu0tbZEfVJ2tM0v0sv6PijU5Gsvuyp6DxtZqOGM0y7Q0hQtu+wA0c7hZ/cJVNaOjIq+g7tvAD0fEVDO6AiFB90kUJnu3DTz/OiV7K6q9bzA2m2bY9UWuyr3/EqUVgSzxk2K4QMHldakimg2K5Mvl63bvrWIIhZqVgWUJMzWyuw9sD8eXbEkW0GJpigFhvSvi/MnTinK2AVNIJ8CEtryqakvAgQIECBAgAABAgQIFJnA/oUL4tD61UUWtXCLTaCipiYGXvv8iOQDcq3wAi2710Q0Hyj8wEYsI4GKqBoyNaJS8kshFj3d2eXBJQvjULNyRoXwLscxhtcNilnjJ5Xj1DM554OHDsW8pU9FWyajE1QxCqTJqmnSapq8qvWMQMPBAzF/+eKeGdyoJSWgJGH2lvPhZYtif6OdVbO3MsUV0bnjJsaIgb4wVlyrJtruEJDQ1h2q+iRAgAABAgQIECBAgECRCDTv3B775v26SKIVZrEK1EycGn2TD820nhFoO7g7Wvdt7pnBjVoWAhXV/aOy7pyymGtWJrkiKWe0XjmjrCxHycUxe/zkGFo3sOTmVcwTenzVstjdsK+YpyD2DAmk5YTTssJazwo8kiS07UsS2zQCZyugJOHZynXvdWu3bUl2Vt3YvYPovaQFqior46o08Tz5qREodwEJbeV+B5g/AQIECBAgQIAAAQJlL1D/i3ui9eD+sncA0H0CA666LqqS3V60HhJoa4mWHcuTwe3t0kMrUPLDVg4YExU1dSU/zyxNcF9SzugR5YyytCQlE0vvql7Jzk2zk01V7dyUpUXdvGtHLNmwNkshiaWIBS6ePD3q+tUW8QxKI/T1O7bGik0bSmMyZtEjAkMGJCUJJyhJ2CP4pxn0YFOys+oSO6uehshLZxAYNdtJhS0AACcJSURBVHhozBg7/gxneZlAeQhIaCuPdTZLAgQIECBAgAABAgQInFLgQFLCqHHl0lO+7gUCXRGo7D8g6p71u13pwrV5EGitXx9th+zskgdKXRwvUFGZlBudpqTw8S4FeD5/2dPR0HiwACMZopwExg4dHlNH23Exa2ve0toS9y9eGK2trVkLTTxFJtC3uibmTJ9VZFGXZriHmpuSEuJJ0ktSSlwjcDYCShKejVphrrGzamGcS3WUCydNi0G1/Ut1euZFoFMCEto6xeVkAgQIECBAgAABAgQIlJ5Ay769sfc395bexMwoEwJ9kg/M+kyekYlYyjmItsa90brXDhDlfA9019wr+gyMyv6ju6t7/Z5GYN32LbFys3JGpyHy0lkIXDJlRgzo2+8srnRJdws8vX51bN29q7uH0X+JC0wcMTomjBhV4rMsnuktXLMiduytL56ARZoZgV6VVbkdVZUkzMySHBOInVWP4fCkEwJ9elfHFTPO68QVTiVQ2gIS2kp7fc2OAAECBAgQIECAAAECHRLYe//Po6V+d4fOdRKBzgjUPfu5UemD8c6Qdc+5yc4PLTuTsqNJ+VGNQD4FKgeOj4rekl/yadrRvhqbmuKhJQsVE+4omPPOKNCvpk9cPu3cM57nhJ4R2LWvPp5YvaJnBjdqSQikhYTnTD8v+lRXl8R8SmES2/bsikXrVpfCVMyhwAKjk5KE05UkLLB6x4ezs2rHrZx5rMD44SNj0sgxxx70jEAZC0hoK+PFN3UCBAgQIECAAAECBAi0CzSuXh4HFj/Z/tRPAnkR6DVkWPSf8zt56UsnXRdo3bc52g5KXO26pB6OCFT2SsqNTj3y1IPCCzyR/Pm9K9lpVSOQD4H0w7P0QzQtmwJpWcKHkvKEjUmZQo3A2Qik5cvSMmZadgTSMsIPJOWEm5OywhqBzghclLyXBypJ2Bmygp/7dJKsujVJWtUIdEYg/XJJ+iUTjQCBwwIS2twJBAgQIECAAAECBAgQIBCtjQej/hd3J7s3tdEgkDeBfuddHNXjJuatPx11TaCtaX+07lnbtU5cTeAogYq+Q6OydvhRRzwstMCW3Ttj8fo1hR7WeCUokO7clJY3qknKHGnZFVi5eUOs2741uwGKLNMCM5LdnEYluzpp2RJYumFtbNq1I1tBiSbTAukui1ckuy1q2RbYmeys+qSdVbO9SBmLbkBS3eCSKTMyFpVwCPSsgIS2nvU3OgECBAgQIECAAAECBDIjsG/+/dG8fUtm4hFIkQtUVsbA616QlCLsXeQTKa3wW3Ympcpa7exSWqvac7OpHDwpKqpqei4AI0dLbmeXJ3M/cRDoisDg2gFxwSQ7LnbFsBDXNhw8EPOXLy7EUMYoMYHK5O/mV82cHVWVVSU2s+Kfzp6GffHYqmXFPxEzKJjAhBGjYuKI0QUbz0BnJ5DurPpgsrPqITurnh1gGV41dfQ5MXaoL4yV4dKb8mkEJLSdBsdLBAgQIECAAAECBAgQKCeBQxvXxf4n5pfTlM21GwV6jxoTtRdd0Y0j6PpsBFr3b4u2/XaAOBs71xwn0KtPVA2aeNxBT3tCYEmyQ9vmZKc2jUBXBGaeMyFGDhrSlS5cWyCBR1Ysjn0HDhRoNMOUisCIgYPjXDsnZ3Y5H1r6VBw8dCiz8QksWwJzps+KvtW+VJKtVTl5NCuSnVXX21n15DiOHiNQWVERc5PE895VvY457gmBcheQ0Fbud4D5EyBAgAABAgQIECBA4LcCbS0tsee+H0e0NDMh0GWB2kvmRm/fGu+yY747aGs5FK27Vua7W/2VoUBl7Yio6Cv5JQtLv7thbzy+ankWQhFDkQpUJTs3XTnz/GTnpsoinUF5hb1+x9ZYsWlDeU3abLsscP7EKTGkf12X+9FB9wis3rop1mzd3D2d67WkBOr61cbFk6eX1JxKeTL7kp1VH7Gzaikvcd7mNnTAwJg9YXLe+tMRgVIRkNBWKitpHgQIECBAgAABAgQIEMiDQLpDW7pTm0agKwIVvauTcqPPj/DBeFcYu+3alt2rI5oPdlv/Oi4PgaohSWnCSt8ez8pqp+WMGpvs7JKV9Si2ONKd2dId2rTiEGhqbo4HliyMtJSZRqAjAtW9esfcGedFRbL7i5ZNgQOHGmPe0kXZDE5UmRKYNmZcjBkyLFMxCeb0Ammp8LRkuEbgdALnjZ8Uw+oGne4UrxEoSwEJbWW57CZNgAABAgQIECBAgACBkws0J6UQ9s3/v5O/6CiBDgpUJ7+I6zfrog6e7bRCC7Qd2BWtDVsKPazxSkigondtVA4cV0IzKv6prNqyMdZu874u/pXsmRlcMHFqDO4/oGcGN+pZCSxcszJ27N1zVte6qPwExg0bEZNHjS2/iRfZjBesXBr1+xuKLGrhFlIgLUmY7qjaq6qqkMMaq4sCacnRtPSoRuBUAr2T9/Tc5L2dvsc1AgSOFZDQdqyHZwQIECBAgAABAgQIEChvgWSnhz2/uDvaGu3eVN43Qtdm33/us6NXstuLllGB1uZo2bkiCc7OLhldocyHVTlgdFTUDMx8nOUU4P7kz+2Hlz1dTlM21zwJ1PROd26anafedFMogW17dseidasKNZxxilzgsqkzo7ZP3yKfRemHv3Hn9lhmt/TSX+guzHB4snvTrOTLY1pxCRxqbooHFyc7qxZX2KItoEC662K6+6JGgMCJAhLaTjRxhAABAgQIECBAgAABAmUtcGDxk9G4enlZG5j82QtU9quNumuec/YduLIgAq3166LtkB0gCoJdaoNUVEau3GjyU8uWwIIVS6L+wP5sBSWazAuMHz4yJo0ck/k4BXisQGvyJZQHkr+zN7e0HPuCZwSOE+ifJLJdmiS0adkXSN/P6fs6fX9rBE4mMHvC5Bg6wJdKTmaT9WNPJr9j27lvb9bDFF8PCVw8eXrUJb9L0wgQOFFAQtuJJo4QIECAAAECBAgQIECgrAVa6nfH3vt/XtYGJn/2An2SD8z6TD337DtwZUEE2hrro3XvxoKMZZDSEqioqYvKAZJfsriqG3duS3Z2WZ/F0MSUYYHLp50b/Wr6ZDhCoZ1KIN3JKd3RSSNwOoEpo8fGOUNHnO4Ur2VIYNHaVbEt+f9xjcDxAr179Yorkx1VK5QkPJ6mKJ5v3b0rnl6/uihiFWRhBfpW18Sc6bMKO6jRCBSRgIS2IlosoRIgQIAAAQIECBAgQKBQAvW/uTdafXu0UNwlNU7dNTdGZb/+JTWnkpxMW2tSdjTZiTH5qRHojEBl3bioqPbt8c6YFercppbmXDkjO7sUSrz4xxnQt19cMmVG8U+kTGdQv78hFqxcWqazN+2OCKSJL2lJ4eokEUYrDoEde/fEwjUriyNYURZUYOzQ4TF19DkFHdNg+RNobW2N+5MdGFuSnxqBowUmjhgdE0aMOvqQxwQIHCUgoe0oDA8JECBAgAABAgQIECBA4LDAweTDsYNLn8JBoFMCVYMGx4C513bqGif3nEDr3k3R1rin5wIwcvEJVPY6XG60+CIvm4ifWrsyttd7X5fNgndxoukH4+kH5FrxCsxbuigOHGos3gmIvFsFhg6oi9kTpnTrGDrPr0BbWk54ycJoam7Ob8d6K3qBNAE9TUTXildgyfo1sXn3zuKdgMi7ReCKZHe2PskubRoBAicXkNB2chdHCRAgQIAAAQIECBAgUNYCrQf3R/0v7ilrA5PvvEDfcy+MmgmTO3+hK3pEoK2pIVr3rOuRsQ1anAIVfYdEZa2yZVleve1JmbKnknJlGoEzCaQ7N6Wly9ISZlrxCqzZujlWb91UvBMQebcKzBo3KYYPHNStY+g8/wLLN62PDTu25b9jPRatQFoaPC0RrhW3wO6GvfH4qmSXdI3AbwUG9quNiyZP50GAwGkEJLSdBsdLBAgQIECAAAECBAgQKGeBffN+Hc07t5czgbl3RiD5YHzgdS9IShFWd+Yq5/awQK7saKsdIHp4GYpm+MpBE6OiV5+iibccA83t7JKUM2pqaSnH6ZtzJwSGDhiY7NwkCb0TZJk89eChQzEv2VW5LZPRCaonBXpVVcWVM2dHZUVlT4Zh7LMQ2Htgfzy6YslZXOmSUhWYNHJMjB8+slSnV1bzejDZgbGxqams5myypxaYPmZcjB4y7NQneIUAgZDQ5iYgQIAAAQIECBAgQIAAgZMKHErKIexf+OhJX3OQwPECvYePitpLrzz+sOcZF2ht2BptB5Q9yfgyZSO8qpqoGjwpG7GI4rQCyzaui40S0k9r5MWIWeOTnZvq7NxUCvfC46uWxe6GfaUwFXPIo0D6AXn6QblWnAIPL3s69jceLM7gRZ1XgYqktytmnBc1vX1xLK+wPdTZqi0bY+22LT00umGzJFCZ7pY88/xIE9A1AgROLSCh7dQ2XiFAgAABAgQIECBAgEBZC7Q1N8We++6KaLXLS1nfCB2cfO1Fc6L3qLEdPNtpWRFoa26M1t3KE2ZlPbIcR0Xt8KjsOzTLIYrttwL1BxpiwYqlPAicUqB38sHZ3OQDtPSDNK34BTbv2hFLNqwt/omYQV4FLk5KmNUlpcy04hRIE17SxBeNwODaAXHBpKkgSkQgTVRNE1Y1AmlJ8LQ0uEaAwOkFJLSd3serBAgQIECAAAECBAgQKGuBhsfmRdPmDWVtYPJnFqjo1Svq0nKjvll6ZqwMntGSJrQliW0agdMJVA2ZElHZ+3SneC1DAg8vW5Ts7OJ9naElyVQoY5Kdm6bZuSlTa9KVYFqSL5/cv3hhtLa2dqUb15aQQN/qmpgzfVYJzaj8ptLYdCgeWqKccPmt/IkznnnOhBg5aMiJLzhStAJpSeG0tLBW3gKzJ0yOoQMGljeC2RPogICEtg4gOYUAAQIECBAgQIAAAQLlKtC0dXM0PPpAuU7fvDsoUD12QvQ7/5IOnu20rAmkJUfT0qMagVMJVPTuF5UDx5/qZcczKLB22+ZkZ5dNGYxMSFkQsHNTFlYhvzE8vW51bN2zK7+d6q1oBSaOGB0TRowq2vgFfljgidXLY9e+vTjKWKCqsjJXkjD9qZWOwIYd22L5pvWlMyEz6bRAdfKl0LkzZkeF3ZI7beeC8hOQ0FZ+a27GBAgQIECAAAECBAgQ6LhAW2uu7Ghb8g1xjcCpBPrPeVb0GjL8VC87nnWB1uZo2bk861GKrwcFKvuPioo+g3owAkN3VsDOLp0VK5/z7dxUmmu9c199PLl6RWlOzqw6JZAWEk53Z+uT7NKmESBAgAABAgQIEChmAQltxbx6YidAgAABAgQIECBAgEABBPYvejwOrV1ZgJEMUYwClX36Rt2znxvJV0uLMXwx/1agdc/aaGtS9sQNcRKB5L1dNWRa8h63M8RJdDJ96PFVy2J3w75Mxyi4wgvYuanw5oUYsa2tLVeesLG5qRDDGSPDAgNr+8dFk5I/tzUCBAgQIECAAAECRS4goa3IF1D4BAgQIECAAAECBAgQ6G6B5t07Y9+Dv+zuYfRfpAI1k6dH3+nnFWn0wm4XaGvcE617lSds9/DzGYGKmgFROWDsMwc8KhqBzbt2xJINa4smXoF2v8DhnZvOS3Zuqu7+wYxQcIGVmzfEuu1KiBccPmMDTh87PkYPHpqxqIRDgAABAgQIECBAoPMCEto6b+YKAgQIECBAgAABAgQIlJ1A/a9+Gq377fJSdgvfgQkPeNYNUdW/rgNnOiXTAkl54VzZ0eSnRuBogcq6c6Kiuv/RhzwuEoGW1pZ4YPHCaGn1vi6SJev2MAclOzddaOembnc2AAECBAgQIECAAAECBAh0XUBCW9cN9UCAAAECBAgQIECAAIGSFzi4fHEcXP50yc/TBDsnUFU3MAZcdX3nLnJ2ZgVa926Mtsb6zMYnsB4QqKxKyo1OTQZWUrgH9PMy5OL1q2PL7l156UsnxS8wI9m5aZSdm4p/Ic2AAAECBAgQIECAAAECZSAgoa0MFtkUCRAgQIAAAQIECBAg0FWB1v0NUf+rn3S1G9eXmEDfmedHzcQ02UUrBYG2Qw3RWr+uFKZiDnkSqOgzOCr7j8xTb7rpCYFd+/bGE6uX98TQxsyYQGVlZVw1c3ZUJYmqGgECBAgQIECAAAECBAgQyLqAhLasr5D4CBAgQIAAAQIECBAgkBGBvQ/+Mlp278xINMLocYGKiqi79nlRWdOnx0MRQL4E2pKyoysiWpvz1aF+ilygctCEqOjVt8hnUd7ht7W1xUNLn4rGpqbyhjD7GDFwcJw7biIJAgQIECBAgAABAgQIECBQFAIS2opimQRJgAABAgQIECBAgACBnhdoXLsyDix6vOcDEUEmBHoNHRH9L786E7EIIn8CrQ1bou2A8oT5Ey3inqqqo2rw5CKegNAJECBAgAABAgQIECBAgAABAgSKVUBCW7GunLgJECBAgAABAgQIECBQYIG2pkOx5767ItpaCzyy4bIo0O/8S6N67PgshiamLgi0NR+M1t2ru9CDS0tFoKLfsKhM/tEIECBAgAABAgQIECBAgAABAgQIFFpAQluhxY1HgAABAgQIECBAgACBIhZoePTBaNq6qYhnIPS8CFRVxcDrXxAVVb3y0p1OsiXQsmtlRMuhbAUlmoILVA2eElHVu+DjGpAAAQIECBAgQIAAAQIECBAgQICAhDb3AAECBAgQIECAAAECBAh0WKBp84ZoeGxeh893YmkK9B49LmovvKw0J2dWBAgQIECAAAECBAgQIECAAAECBAgQINCjAhLaepTf4AQIECBAgAABAgQIECgugbbWlqhPyo62NTcVV+CizatA7WVXRe9hI/Pap84IECBAgAABAgQIECBAgAABAgQIECBAgEAqIKHNfUCAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECmRCQ0JaJZRAEAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECEhocw8QIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAQCYEJLRlYhkEQYAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIS2twDBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIJAJAQltmVgGQRAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQICAhDb3AAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAhkQkBCWyaWQRAECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgIKHNPUCAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECmRCQ0JaJZRAEAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECEhocw8QIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAQCYEJLRlYhkEQYAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIS2twDBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIJAJAQltmVgGQRAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQICAhDb3AAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAhkQkBCWyaWQRAECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgIKHNPUCAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECmRCQ0JaJZRAEAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECEhocw8QIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAQCYEJLRlYhkEQYAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIS2twDBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIJAJAQltmVgGQRAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQICAhDb3AAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAhkQkBCWyaWQRAECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgIKHNPUCAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECmRCQ0JaJZRAEAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECEhocw8QIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAQCYEJLRlYhkEQYAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIS2twDBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIJAJAQltmVgGQRAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQICAhDb3AAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAhkQkBCWyaWQRAECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgIKHNPUCAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECmRCQ0JaJZRAEAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECEhocw8QIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAQCYEJLRlYhkEQYAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIS2twDBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIJAJAQltmVgGQRAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQICAhDb3AAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAhkQkBCWyaWQRAECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgIKHNPUCAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECmRCQ0JaJZRAEAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECEhocw8QIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAQCYEJLRlYhkEQYAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIS2twDBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIJAJAQltmVgGQRAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQICAhDb3AAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAhkQkBCWyaWQRAECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgIKHNPUCAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECmRCQ0JaJZRAEAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECEhocw8QIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAQCYEJLRlYhkEQYAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIS2twDBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIJAJAQltmVgGQRAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQICAhDb3AAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAhkQkBCWyaWQRAECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgIKHNPUCAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECmRCQ0JaJZRAEAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECEhocw8QIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAQCYEJLRlYhkEQYAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIS2twDBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIJAJAQltmVgGQRAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQICAhDb3AAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAhkQkBCWyaWQRAECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgIKHNPUCAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECmRCQ0JaJZRAEAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAAQIECEhocw8QIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAAAECBAgQIECAQCYEJLRlYhkEQYAAAQIECBAgQIAAAQIECBAgQIAAAQIECBAgQIAAA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null ]
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https://encyclopediaofmath.org/wiki/Homogeneous_space
[ "# Homogeneous space\n\nh0476901.png 132 0 132 A set together with a given transitive group action. More precisely, $M$ is a homogeneous space with group $G$ if a mapping$$( g ,\\ x ) \\rightarrow g x$$ of the set $G \\times M$ into $M$ is given, such that\n\n1) $( g h ) x = g ( h x )$ ;\n\n2) $e x = x$ ;\n\n3) for any $x ,\\ y \\in M$ there exists a $g \\in G$ such that $g x = y$ .\n\nThe elements of the set $M$ are called the points of the homogeneous space, and the group $G$ is called the group of motions, or the basic (fundamental) group of the homogeneous space.\n\nAny point $x$ in $M$ determines a subgroup$$G _{x} = \\{ {g \\in G} : {g x = x} \\}$$ of $G$ . It is called the isotropy group, or stationary subgroup, or stabilizer of the point $x$ . The stabilizers of different points are conjugate in $G$ by inner automorphisms.\n\nWith an arbitrary subgroup of $G$ is associated a certain homogeneous space for $G$ , namely, the set $M = G / H$ of left cosets of $H$ in $G$ , on which $G$ acts by the formula$$g ( a H ) = ( g a ) H , g ,\\ a \\in G .$$ This homogeneous space is called the quotient space of $G$ by $H$ , and the subgroup $H$ turns out to be the stabilizer of the point $e H = H$ of this space ($e$ is the identity of $G$ ). Any homogeneous space $M$ with group $G$ can be identified with the quotient space of $G$ by the subgroup $H = G _{x}$ , the stabilizer of a fixed point $x \\in M$ , by means of the bijection$$M \\ni y \\iff g H \\in G / H ,$$ where $g$ is any element of $G$ such that $g x = y$ .\n\nIf $G$ is a topological group and $H$ is a subgroup of it (respectively, $G$ is a Lie group and $H$ is a closed subgroup of $G$ ), then $M = G / H$ is endowed with the structure of a topological space (respectively, of a differentiable manifold) in a canonical way, relative to which the action of $G$ on $M$ is continuous (respectively, differentiable). If a Lie group $G$ acts transitively and differentiably on a differentiable manifold $M$ , then, for any point $x _{0} \\in M$ , the subgroup $H = G _ {x _{0}}$ is closed and the bijection $g H \\rightarrow g x _{0}$ above is differentiable; if the number of connected components of $G$ is at most countable, then this bijection is a diffeomorphism.\n\nOther cases which have been studied are when $G$ is an algebraic group and $M$ an algebraic variety (see Homogeneous space of an algebraic group), and when $M$ is a complex manifold and $G$ is a real (or complex) Lie group (see Homogeneous complex manifold).\n\nIn what follows $M$ is always a differentiable manifold and $G$ is a Lie group.\n\n## Geometry of homogeneous spaces.\n\nAccording to F. Klein's Erlangen program, the subject of the geometry of a homogeneous space is the study of invariants of the group of motions of a homogeneous space. The classical area of research here is the classification of the various subsets of a homogeneous space, in particular submanifolds and their unions, families of submanifolds, etc., up to motions of the group $G$ . Such a classification can be obtained by constructing a complete system of invariants of subsets of given type (examples of such systems of invariants are the length of the sides of a triangle, or the curvature and torsion of a smooth curve in the three-dimensional Euclidean space). A general method for constructing a complete system of local invariants (the moving-frame method) for a smooth submanifold in an arbitrary homogeneous space of a Lie group was developed by E. Cartan (see , ).\n\nAnother direction of research is the discovery and study of invariant geometric objects on a homogeneous space (see Invariant object on a homogeneous space). The action of the basic Lie group $G$ on a homogeneous space $M$ induces an action of $G$ on the space of various geometric objects on $M$ ( functions, vector and tensor fields, connections, differential operators, etc.). Geometric objects that are fixed under this action are called invariant objects. Examples of such objects are the Euclidean metric on a Euclidean space regarded as a homogeneous space of the group of Euclidean motions, and the conformal metric giving the angle between curves in a conformal space. Closely related to this area is the problem of describing and studying homogeneous spaces having a particular invariant. For example, one can consider Riemannian and pseudo-Riemannian spaces, spaces with an affine connection, symplectic homogeneous spaces, homogeneous complex manifolds, that is, homogeneous spaces having an invariant metric (Riemannian or pseudo-Riemannian), an affine connection, a symplectic structure, or a complex structure, respectively. See also Riemannian space, homogeneous; Symplectic homogeneous space; Homogeneous complex manifold.\n\nAn important class of homogeneous spaces is the class of reductive homogeneous spaces, that is, homogeneous spaces $G / H$ such that the Lie algebra $\\mathfrak g$ of the Lie group $G$ has the decomposition$$\\tag{*} \\mathfrak g = \\mathfrak f + \\mathfrak m , \\mathfrak f \\cap \\mathfrak m = \\{ 0 \\} ,$$ where $\\mathfrak f$ is the Lie algebra of $H$ and $\\mathfrak m$ is a subspace invariant under the adjoint representation of $H$ in $\\mathfrak g$ ( cf. Adjoint representation of a Lie group). Such a decomposition defines a geodesically-complete linear connection on $G / H$ with parallel curvature and torsion tensors. Conversely, a simply-connected manifold with a complete linear connection having parallel curvature and torsion tensors is a reductive homogeneous space with respect to the automorphism group of this connection (see ). A special case of a reductive homogeneous space is a symmetric space, for which the decomposition (*) satisfies the additional condition $[ \\mathfrak m ,\\ \\mathfrak m ] \\subseteq \\mathfrak f$ . Geometrically this condition means that the corresponding connection has zero torsion. Examples of symmetric spaces are the globally symmetric Riemannian spaces (cf. Globally symmetric Riemannian space), as well as the space of an arbitrary Lie group, on which the group of motions is generated by left or right translations.\n\n## Homogeneous bundles and representation theory.\n\nThe action of $G$ can be extended not only to bundles of geometric objects, but also to the larger class of so-called homogeneous bundles. A homogeneous bundle $\\pi$ over the homogeneous space $G / H$ is given by the left action of the subgroup $H$ on an arbitrary manifold $F$ ( a typical fibre) and is defined as the natural projection$$\\pi : G \\times _{H} F \\rightarrow G / H ,$$ where $G \\times _{H} F$ is the fibre product as the quotient of the direct product $G \\times F$ by the equivalence relation$$( g ,\\ f \\ ) \\sim ( g h ^{-1} ,\\ h f \\ ) , g \\in G , k \\in H , f \\in F .$$ If $P$ is a vector space on which $H$ acts linearly, then the corresponding homogeneous bundle $\\pi$ is a vector bundle, and in the space of its sections $\\Gamma ( \\pi )$ there is a linear representation of $G$ , induced by the representation of the subgroup $H$ in $F$ . The study of induced representations (cf. Induced representation) (the properties of which turn out to be closely related to the geometry of the corresponding homogeneous space) and their generalizations plays an important role in the representation theory of Lie groups (see ).\n\n## Analysis on homogeneous spaces.\n\nAmong the most developed areas are: 1) the study of various function spaces on a homogeneous space (spaces of functions, spaces of sections of homogeneous vector bundles, cohomology spaces with values in appropriate sheaves); 2) the study of invariant differential operators acting on these spaces; and 3) the study of various dynamical systems related to homogeneous spaces.\n\nThe first area includes the theory of spherical functions (and, more generally, spherical sections), which studies finite-dimensional spaces of functions on a homogeneous space which are invariant with respect to the basic group (see Representation function), many special functions of mathematical physics can be interpreted as spherical functions on some homogeneous space, and the study of representations of the basic group in such function spaces enables one to obtain in a unified way the basic results of the theory of special functions (integral representations, recurrence formulas, addition theorems, etc., see ). A natural generalization of the theory of Fourier series and integrals is abstract harmonic analysis (cf. Harmonic analysis, abstract) on homogeneous spaces, one of the basic problems in which consists of the description of the decomposition of the space of square-integrable functions on a homogeneous space as the sum of subspaces irreducible under the action of the basic group. The majority of results obtained here are connected with the case when the homogeneous space is the space of a semi-simple Lie group (see ).\n\nThe theory of automorphic functions leads to the more general problem of the decomposition into irreducible components of the space of square-integrable sections of a homogeneous vector bundle over a homogeneous space $G / H$ which are invariant relative to a discrete subgroup $\\Gamma \\subset G$ .\n\nAs well as function spaces, various measure spaces on homogeneous spaces are also studied, for example in connection with applications to probability theory (see , ).\n\nThe second area includes problems of the description of invariant differential operators (cf. Invariant differential operator) on homogeneous spaces, the study of their properties, finding their spectrum and fundamental solution, and the investigation of the solutions of the corresponding partial differential equations (see , ).\n\nThe third area includes the study of various dynamical systems (cf. Dynamical system) related to the homogeneous space, for example, the flow generated by a one-parameter subgroup of the basic group, the flow generated by the canonical connection of a Lie group, the geodesic flow of a homogeneous Riemannian space, etc. Conditions for the ergodicity of flows have been investigated, and a description of their first integrals have been given (see ).\n\nIntegral geometry is also related to analysis on homogeneous spaces, being connected with the theory of invariant measures on homogeneous spaces and on manifolds related to these, with as points submanifolds of one sort or another.\n\n## The topology of homogeneous spaces.\n\nThe methods of algebraic topology in many cases allow one to reduce the problem of computing basic topological invariants of a homogeneous space (the cohomology ring, characteristic classes, $K$ - functor, homotopy groups, etc.) to certain algebraic problems concerning the algebraic structure of the basic group and the isotropy group of the homogeneous space. Explicit results of this kind have been obtained for several classes of homogeneous spaces. For example, a theorem of H. Cartan gives an algorithm for computing the real cohomology algebra $H ^{*} ( G / H ; \\ \\mathbf R )$ , where $G$ and $H$ are connected compact Lie groups, in terms of invariants of the Weyl groups (cf. Weyl group) of $G$ and $H$ ( see ). In particular, if $G / H$ has non-zero Euler characteristic (this is equivalent to $G$ and $H$ having the same rank), then the Poincaré polynomial (cf. Künneth formula) of the manifold $G / H$ has the form$$P ( G / H ,\\ t ) = \\prod _{i=1} ^ r \\frac{1 - t ^ {2k _{i}}}{1 - t ^ {2l _{i}}} ,$$ where $k _{1} \\dots k _{r}$ and $l _{1} \\dots l _{r}$ are the degrees of the basis invariant polynomials of the Weyl groups for $G$ and $H$ , respectively (Hirsch's formula).\n\nA very detailed study has been made of the topological structure of homogeneous spaces of compact Lie groups, symmetric spaces and solv manifolds (homogeneous spaces of solvable Lie group, cf. Solv manifold). The Mostow–Karpelevich theorem, which states that any homogeneous space of a Lie group having a finite basic group is diffeomorphic to a vector bundle over the homogeneous space of a compact Lie group, reduces the study of the topology of homogeneous spaces to a considerable extent to the case when the basic group is compact.\n\n## The classification of homogeneous spaces.\n\nThe basic problems in this area consist in the determination of those manifolds which are homogeneous spaces of connected Lie groups and in the enumeration of all transitive actions of connected Lie groups on these manifolds. For example, the only homogeneous spaces of dimension 2 are the plane, the cylinder, the sphere, the torus, the Möbius strip, the projective plane, and the Klein bottle. At present (1982), the classification of three-dimensional homogeneous spaces has also been carried out, as well as the classification (up to finite-sheeted coverings) of all compact homogeneous spaces of dimensions $\\leq 6$ ( see ).\n\nFor a number of important classes of homogeneous spaces $M$ of high dimension, a classification of all transitive actions of Lie groups on $M$ is known (see ). For example, the classification of all transitive actions of compact Lie groups on spheres has the following form. Any continuous, transitive and effective action of a connected compact Lie group on $S ^{n}$ can be transformed by a homeomorphism of the sphere $S ^{n}$ to the standard linear action of the group $\\mathop{\\rm SO}\\nolimits ( n + 1 )$ or one of the following subgroups of it:\n\n$G = \\mathop{\\rm SU}\\nolimits (k)$ or $U (k)$ if $n = 2 k - 1$ ;\n\n$G = \\mathop{\\rm Sp}\\nolimits (k)$ , $\\mathop{\\rm Sp}\\nolimits (k) \\times U (1)$ or $\\mathop{\\rm Sp}\\nolimits (k) \\times \\mathop{\\rm Sp}\\nolimits (1)$ if $n = 4 k - 1$ ;\n\n$G = \\mathop{\\rm Spin}\\nolimits (7)$ or $\\mathop{\\rm Spin}\\nolimits (9)$ if $n = 7 ,\\ 15$ ;\n\n$G = G _{2}$ if $n = 6$ ( the Montgomery–Samelson–Borel theorem, see ). As for transitive actions of non-compact Lie groups on the sphere $S ^{n}$ , for even $n$ the only such actions are essentially the projective action of $\\mathop{\\rm SL}\\nolimits ( n + 1 )$ and the conformal action of $\\mathop{\\rm SO}\\nolimits ( 1 ,\\ n + 1 )$ . For odd $n$ , the result is more complicated: Transitive and effective actions can exist of a Lie group with a radical of arbitrarily large dimension.\n\nHow to Cite This Entry:\nHomogeneous space. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Homogeneous_space&oldid=44251\nThis article was adapted from an original article by D.V. Alekseevskii (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article" ]
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https://docs.simpeg.xyz/content/api/generated/SimPEG.utils.face_info.html
[ "# SimPEG.utils.face_info#\n\nSimPEG.utils.face_info(xyz, A, B, C, D, average=True, normalize_normals=True, **kwargs)[source]#\n\nReturns normal surface vector and area for a given set of faces.\n\nLet xyz be an (n, 3) array denoting a set of vertex locations. Now let vertex locations a, b, c and d define a quadrilateral (regular or irregular) in 2D or 3D space. For this quadrilateral, we organize the vertices as follows:\n\nCELL VERTICES:\n\n a -------Vab------- b\n/ /\n/ /\nVda (X) Vbc\n/ /\n/ /\nd -------Vcd------- c\n\n\nwhere the normal vector (X) is pointing into the page. For a set of quadrilaterals whose vertices are indexed in arrays A, B, C and D , this function returns the normal surface vector(s) and the area for each quadrilateral.\n\nAt each vertex, there are 4 cross-products that can be used to compute the vector normal the surface defined by the quadrilateral. In 3D space however, the vertices indexed may not define a quadrilateral exactly and thus the normal vectors computed at each vertex might not be identical. In this case, you may choose output the normal vector at a, b, c and d or compute the average normal surface vector as follows:\n\n$\\bf{n} = \\frac{1}{4} \\big ( \\bf{v_{ab} \\times v_{da}} + \\bf{v_{bc} \\times v_{ab}} + \\bf{v_{cd} \\times v_{bc}} + \\bf{v_{da} \\times v_{cd}} \\big )$\n\nFor computing the surface area, we assume the vertices define a quadrilateral.\n\nParameters\nxyz(n, 3) numpy.ndarray\n\nThe x,y, and z locations for all verticies\n\nA(n_face) numpy.ndarray\n\nVector containing the indicies for the a vertex locations\n\nB(n_face) numpy.ndarray\n\nVector containing the indicies for the b vertex locations\n\nC(n_face) numpy.ndarray\n\nVector containing the indicies for the c vertex locations\n\nD(n_face) numpy.ndarray\n\nVector containing the indicies for the d vertex locations\n\naveragebool, optional\n\nIf True, the function returns the average surface normal vector for each surface. If False , the function will return the normal vectors computed at the A, B, C and D vertices in a cell array {nA,nB,nC,nD}.\n\nnormalize_normalbool, optional\n\nIf True, the function will normalize the surface normal vectors. This is applied regardless of whether the average parameter is set to True or False. If False, the vectors are not normalized.\n\nReturns\nN(n_face) numpy.ndarray or (4) list of (n_face) numpy.ndarray\n\nNormal vector(s) for each surface. If average = True, the function returns an ndarray with the average surface normal vectos. If average = False , the function returns a cell array {nA,nB,nC,nD} containing the normal vectors computed using each vertex of the surface.\n\narea(n_face) numpy.ndarray\n\nThe surface areas.\n\nExamples" ]
[ null ]
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https://scioly.org/wiki/index.php?title=Wind_Power&diff=prev&oldid=52825
[ "# Difference between revisions of \"Wind Power\"\n\nWind Power\nThis event is an event held in the current season.\n\nType Physics\nCategory Lab\n\nWind Power, previously known as Physical Science Lab and Physics Lab, is an event for the 2017 season which involves the construction of a device that can turn wind into energy and the answering of questions relating to alternative energy.\n\n## The Basics of the Event\n\nHalf of the scoring for Wind Power comes from the building portion. Competitors must build a wind turbine mounted to an unmodified 12cm diameter CD. During competition, the judges will attach the device to a DC motor. They will then place a fan in front of the device and turn it on. The blades will spin, thereby creating voltage.\n\nThe other portion of the event is a written test on wind power, power generation, and alternative energy. One 3-ring binder full of notes from any source is allowed for each team, as long as the material in the binder is attached securely. Teams may bring multiple calculators of any type.\n\nCategory B safety spectacles are required for the blade testing portion of this event.\n\n## The Building Section\n\nWhen you plan to build your device, there are many factors to consider. Some of them include:\n\n1. Wind Turbine Diameter\n2. Weight\n\nThis event has changed since 2016. Instead of trying to get the blades to spin as fast as possible with no resistance, you have 5 to 25 ohms of resistance the blades have to 'push' against, which will be wired into the setup. You can buy resistors of varying size or wire 2 in parallel. For example, two 14 ohm resistors in parallel = 7 ohms of resistance.\n\nWeight\n\nLighter blades will spin faster, but since in 2017 you must produce power (due to the resistors), a slightly heavier blade will have a higher momentum. There will be 2.5 minutes of preparation in order to get the blades up to highest attainable speed, so they can be somewhat heavy.\n\nVarious items can be used to construct the blades, but any type of metal is not allowed. Balsa wood or paper are often used for they are lighter materials. Everyday items can often be constructed into blades. For example, a plastic cup can be cut into fourths. Keep experimenting with different materials.\n\nDiameter\n\nAccording to the New York Coaches Conference, doubling the diameter of the circle made by the blades produces a 4-fold increase in power. However, keep in mind that the radius of the circle created by the blades can be no more than 20cm (Div B) and 14cm (Div C).\n\nMany teams have found that since real life wind turbines can create more power (watts, not voltage) by increasing the diameter of the blades, it is to your advantage to do so.\n\nIt is advised that the blade contains some curve, although it is not necessary in order to generate spin. A V-shape might also work. Materials may be morphed into the desired shape whether it be by cutting or molding. With some materials, such as wood, a certain shape can be achieved by soaking and bending the material in water. Not much curve is necessary. It is recommended that the blades have a curve to simulate an airfoil, while still keeping the blades aerodynamic. Keep in mind that more force is generated when the wind from the fan is blowing on the outside of the blade curve, but this is not what most people do. Most people curve it so that the wind hits the inside of the curve, as this provides quick acceleration (which isn't totally necessary, as long as it accelerates to top speed within 2.5 minutes), but also resulting in a top speed that is lower than if the wind was on the outside of the blade.\n\nBlade pitch refers to the angle of the blades relative to the CD. Generally, a lower pitch results in a higher speed and thus a higher power (it will have a much slower acceleration but a higher top speed). One may want a higher pitch the closer the blade gets to the center of the turbine (eg. 20 degrees towards the center and make the front edge gradually get lower until around 5-10 degrees or so at the outside). Make sure your blade pitch is not 0 degrees, as the blades will not generate lift.\n\nThe number of blades is another adjustable variable. 2-3 blades is the most popular amount. Remember that more weight will gain more momentum, but at a point, too much weight will lower the high speed of the turbine. 4 or more blades can often be too heavy if the material is not light enough. However, if the blades are light enough, 4 may work better than 2 or 3.\n\nBalance\n\nBalance is also an important factor. If a turbine is terribly off balance, it may wobble on the mount, and possibly even break. As such, a well-balanced turbine will be able to spin faster since there will be less friction against the mount and less energy will be lost to vibration. It is best if a turbine's center of gravity is at or near the center. This can be accomplished by taking some mass off of the turbine on the heavy side, or by adding mass on the lighter side. A way to help make sure that you build your blade as balanced as possible is to make a device with a thin 1ft by 1ft thin piece of plywood with a metal/wood rod sticking straight out, and lines can be drawn on the sheet of ply going away from the rod at equal increments for which you can line up your blades as you glue them to the CD.\n\nAlthough it may otherwise be a good idea, the rules say that \"modification of the CD is not allowed (except to affix the blades via tape, glue, etc.)\".\n\nMake sure that your turbine is clearly within specs and labeled with your team's name and number.\n\n## The Written Section\n\nThe other half of the score is the written portion. The rules recommend that teams look at Alliant Energy and American Wind Energy Association.\n\n### Alternative Energy\n\nAlternative energy is generally defined as energy that does not harm the environment directly. They usually do not produce carbon emissions and many times they are also renewable. There are several types of renewable energy, each with its own advantages and disadvantages.\n\n• Solar power converts sunlight into energy via photovoltaic panels or concentration. In the long-term it is relatively constant; however, days are longer in the summer and shorter in the winter, resulting in less solar energy generated in the winter. Also, solar power is only available during the day and is less powerful when there are many clouds.\n• Wind power converts the kinetic energy of the wind into other forms of energy, usually into electrical energy with turbines. Wind is plentiful and the method has no emissions, but turbines can be unwelcome both visually and environmentally. Also, periods of wind are more unpredictable than some other methods.\n• Hydroelectric power converts the movement of water into energy, generally with turbines as well. The flow of water is abundant, constant, and hydroelectric plants can store energy for times when it is more necessary, but there are concerns in respect to the reservoirs created by dams.\n• Tidal power is a major subset of hydroelectric power. It uses the movement of water created by tides to get energy. Tides are regular and predictable, but less power can be generated this way than some other ways.\n• Ocean Thermal Energy Conversion (OTEC) utilizes the difference in temperature from shallow water to deeper water. When heat goes from the warmer water to cooler water, an engine converts the flow to energy. This is constant, but not very cost-effective and finding locations where this technology can be used is difficult.\n• Geothermal power converts underground heat into energy. This method is reliable, cost-effective, and environmentally friendly, but is mostly limited to areas with a high tectonic activity.\n\nTo conserve energy, the adage \"reduce, reuse, recycle\" can be followed. These three concepts can be applied to many techniques used to conserve energy.\n\n#### Energy\n\nEnergy is the capacity to perform work. Work, in turn, is when a force is exerted on an object and the object moves parallel to the direction of the force. Work, in joules (J), can be calculated by multiplying the force applied in Newtons (N) to the distance traveled in meters (m). Power is the rate at which this work is performed, and is found by dividing the work by the time. It is measured in watts.\n\nThere are two major types of energy:\n\n• Kinetic energy is the energy contained by an object in motion\n• Potential energy is how much work an outside force like gravity can do on an object depending on its position.\n\nThe Conservation of Energy principle states that energy cannot be created nor destroyed, and that it can only be transformed from one form to another.\n\n#### Heat\n\nHeat is the transfer of energy from a high-temperature object to a low-temperature object.\n\nTemperature\n\nTemperature is the average energy contained in the particles of an object. It is produced by the thermal energy in free particles. Many scales can measure temperature.\n\nHeat Transfer\n\nThere are three main vehicles for transferring heat:\n\n• Conduction is the transfer of heat by direct contact. The heat transfer for convection can be calculated by the following formula:\n$Q=\\frac {kA\\left (T_{hot}-T_{cold}\\right )}{d}$\nWhere\nQ is the heat transferred in $Watts$\nk is the barrier's thermal conductivity in $k=\\frac {Watts}{m K}$\nA is the cross-sectional area in $m^2$\nT is the temperature in °C ($T_{hot}$ represents the warmer temperature and $T_{cold}$ represents the cooler temperature)\nd is the barrier's length in $m$\n• Convection is the transfer of heat from a solid or liquid to another fluid. Forced convection is a fluid flowing over a surface. Natural convection is when a fluid is heated and rises due to buoyancy such as when hot air rises and cooler air sinks, creating circular currents. The heat transfer for convection can be calculated by the following formula:\n$Q=hA(T_{hot}-T_{cold})$\nWhere\nQ is the heat transferred in $Watts$\nh is the film coefficient in $h=\\frac{watts}{m^2 K}$\nA is the surface area in contact with the fluid in $m^2$\nT is the temperature in °C ($T_{hot}$ represents the warmer temperature and $T_{cold}$ represents the cooler temperature)\n• Radiation is where the heat is carried by electromagnetic waves. The Stefan-Boltzmann Law can help calculate this transfer:\n$P=e\\sigma A \\left (T^4-{T_C}^4\\right )$\nWhere\nP is the radiated power in $Watts$\ne is the object's emissivity\nσ is Stefan's constant (equal to $5.6703 \\cdot10^{-8} \\frac {W}{m^2K^4}$)\nA is the radiating area in $m^2$\nT is the temperature of the radiating source in K and $T_C$ is the surrounding temperature.\n\nSpecific Heat\n\nThis is the amount of heat per unit mass needed to raise a substance's temperature by 1 °C. It is represented by the following formula:\n\n$Q=mC\\Delta T$\n\nWhere Q is the heat needed, C is the specific heat, m is the mass, and ΔT is the change in temperature. Every substance has its own specific heat. For example, water's specific heat is 4.184 J/g*K\n\n### Laws\n\nBetz’ law/limit\n\nOnly a certain amount of energy can be harnessed from the wind; 59.3%; the theoretical maximum coefficient of power for any wind turbine.\n\nJoule's Law\n\nEnergy losses are directly proportional to the square of the current. Thus, reducing the current by a factor of two will lower the energy lost to conductor resistance by a factor of four for any given size of conductor.\n\nKelvin's Law\n\nThe optimum size of a conductor for a given voltage and current can be estimated by Kelvin's law for conductor size. Kevin's Law states that the size is at its optimum when the annual cost of energy wasted in the resistance is equal to the annual capital charges of providing the conductor. At times of lower interest rates, Kelvin's law indicates that thicker wires are optimal; while, when metals are expensive, thinner conductors are indicated: however, power lines are designed for long-term use, so Kelvin's law has to be used in conjunction with long-term estimates of the price of copper and aluminum as well as interest rates for capital.\n\nLaws of Thermodynamics\n\nZeroth Law of Thermodynamics: If two systems are each in thermal equilibrium with a third, they are also in thermal equilibrium with each other.\nFirst Law of Thermodynamics (also known as Law of Conservation of Energy): Energy cannot be created or destroyed in an isolated system.\nSecond Law of Thermodynamics: The entropy of any isolated system always increases.\nThird Law of Thermodynamics: The entropy of a system approaches a constant value as the temperature approaches absolute zero.\n\n### History\n\n• 1881: The transmission of electric power with alternating current (AC) became possible after Lucien Gaulard and John Dixon Gibbs built what they called the secondary generator, an early transformer provided with 1:1 turn ratio and open magnetic circuit.\n• 1887: The first electricity-generating wind turbine was a battery charging machine installed by Scottish academic James Blyth to light his holiday home in Marykirk, Scotland.\n• 1888: American inventor Charles F. Brush built the first automatically operated wind turbine.\n• 1891: Danish scientist Poul la Cour constructed a wind turbine to generate electricity, which was used to produce hydrogen by electrolysis. With his Askov mill, he made windmills more efficient.\n• 1919: German physicist Albert Betz discovered the theory of wind energy.\n\n## The Competition\n\nFor the building set-up, there will be 2 stations: high speed and low speed. These may be at the same fan, but if they are at different fans, all teams will test at high speed at one and at low speed at the other. The event supervisors will provide the testing mount for your blades (don't bring your stand, ONLY the cd with blades attached). They will also provide the fan, motor/generator, load resistor, and device to measure voltage. There is a 3-minute time limit for each station. You will get a warning at 2 minutes. In the first 2.5 minutes, you may adjust, modify, and start and stop your blades. Within 2.5 minutes of the start of the testing period, you must tell the ES to begin measuring your voltage for 30 seconds. The ES must record the peak voltage that is measured during that period.\n\nThe written test will take place after impound. If a lengthier test is used for the event, teams will be called up separately to stations and resume the written portion after testing their build.\n\n### Scoring\n\nAs of 2017, the scoring for the building section is calculated as follows:\n\n$25*\\frac{ \\text{Low speed voltage} }{ \\text{Highest low speed voltage out of all teams} } + 25*\\frac{ \\text{High speed voltage} }{ \\text{Highest high speed voltage out of all teams} }$\n\nThe maximum possible score on the building section is 50.\n\nAs of 2017, the scoring for the test section is calculated as follows:\n\n$50*\\frac{ \\text{Test score} }{ \\text{Highest test score out of all teams} }$\n\nThe maximum possible score on the test section is 50.\n\nThe test score and the building score are added together to determine a team's score, with the highest score winning." ]
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https://cheatsheeting.com/show.html?sheet=sq-m-to-ac-conversions
[ "", null, "[PDF Book]\nHome > Conversions (Area) > Conversion tables from/to square meter > sq m to ac Conversion Cheat Sheet (Interactive)\n From: Step: Decimals: 0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 You could also enter the values to convert and print directly on the table\n [Formula: ac = sq m x 0.000247105]   [Printer friendly]  [Acres to Square meters]", null, "sq m   ac\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\nsq m   ac\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\nsq m   ac\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\nsq m   ac\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n=  ##\n\n# Square meters to Acres Conversion Table\n\n sq m  =  0.000247105 ac\n\n# How to convert from Square meters to Acres\n\nSince 1 square meter is equal to 0.000247105 acres, we could say that n square meters are equal to 0.000247105 times n acres. In other words, we could use the following formula:\n\nacres = square meters x 0.000247105\n\nFor example, let's say that we want to convert 2 square meters to acres. Then, we just replace square meters in the abovementioned formula with 2:\n\nacres = 2 x 0.000247105\n\nThat is, 2 square meters are equal to 0.00049421 acres." ]
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https://www.colorhexa.com/ebeefe
[ "# #ebeefe Color Information\n\nIn a RGB color space, hex #ebeefe is composed of 92.2% red, 93.3% green and 99.6% blue. Whereas in a CMYK color space, it is composed of 7.5% cyan, 6.3% magenta, 0% yellow and 0.4% black. It has a hue angle of 230.5 degrees, a saturation of 90.5% and a lightness of 95.9%. #ebeefe color hex could be obtained by blending #ffffff with #d7ddfd. Closest websafe color is: #ffffff.\n\n• R 92\n• G 93\n• B 100\nRGB color chart\n• C 7\n• M 6\n• Y 0\n• K 0\nCMYK color chart\n\n#ebeefe color description : Light grayish blue.\n\n# #ebeefe Color Conversion\n\nThe hexadecimal color #ebeefe has RGB values of R:235, G:238, B:254 and CMYK values of C:0.07, M:0.06, Y:0, K:0. Its decimal value is 15462142.\n\nHex triplet RGB Decimal ebeefe `#ebeefe` 235, 238, 254 `rgb(235,238,254)` 92.2, 93.3, 99.6 `rgb(92.2%,93.3%,99.6%)` 7, 6, 0, 0 230.5°, 90.5, 95.9 `hsl(230.5,90.5%,95.9%)` 230.5°, 7.5, 99.6 ffffff `#ffffff`\nCIE-LAB 94.298, 1.956, -8.047 82.722, 85.967, 105.996 0.301, 0.313, 85.967 94.298, 8.282, 283.664 94.298, -2.542, -12.972 92.718, -3.002, -2.878 11101011, 11101110, 11111110\n\n# Color Schemes with #ebeefe\n\n• #ebeefe\n``#ebeefe` `rgb(235,238,254)``\n• #fefbeb\n``#fefbeb` `rgb(254,251,235)``\nComplementary Color\n• #ebf8fe\n``#ebf8fe` `rgb(235,248,254)``\n• #ebeefe\n``#ebeefe` `rgb(235,238,254)``\n• #f2ebfe\n``#f2ebfe` `rgb(242,235,254)``\nAnalogous Color\n• #f8feeb\n``#f8feeb` `rgb(248,254,235)``\n• #ebeefe\n``#ebeefe` `rgb(235,238,254)``\n• #fef2eb\n``#fef2eb` `rgb(254,242,235)``\nSplit Complementary Color\n• #eefeeb\n``#eefeeb` `rgb(238,254,235)``\n• #ebeefe\n``#ebeefe` `rgb(235,238,254)``\n• #feebee\n``#feebee` `rgb(254,235,238)``\n• #ebfefb\n``#ebfefb` `rgb(235,254,251)``\n• #ebeefe\n``#ebeefe` `rgb(235,238,254)``\n• #feebee\n``#feebee` `rgb(254,235,238)``\n• #fefbeb\n``#fefbeb` `rgb(254,251,235)``\n• #a2b0fa\n``#a2b0fa` `rgb(162,176,250)``\n• #bac5fc\n``#bac5fc` `rgb(186,197,252)``\n• #d3d9fd\n``#d3d9fd` `rgb(211,217,253)``\n• #ebeefe\n``#ebeefe` `rgb(235,238,254)``\n• #ffffff\n``#ffffff` `rgb(255,255,255)``\n• #ffffff\n``#ffffff` `rgb(255,255,255)``\n• #ffffff\n``#ffffff` `rgb(255,255,255)``\nMonochromatic Color\n\n# Alternatives to #ebeefe\n\nBelow, you can see some colors close to #ebeefe. Having a set of related colors can be useful if you need an inspirational alternative to your original color choice.\n\n• #ebf3fe\n``#ebf3fe` `rgb(235,243,254)``\n• #ebf1fe\n``#ebf1fe` `rgb(235,241,254)``\n• #ebf0fe\n``#ebf0fe` `rgb(235,240,254)``\n• #ebeefe\n``#ebeefe` `rgb(235,238,254)``\n• #ebecfe\n``#ebecfe` `rgb(235,236,254)``\n• #ebebfe\n``#ebebfe` `rgb(235,235,254)``\n• #edebfe\n``#edebfe` `rgb(237,235,254)``\nSimilar Colors\n\n# #ebeefe Preview\n\nThis text has a font color of #ebeefe.\n\n``<span style=\"color:#ebeefe;\">Text here</span>``\n#ebeefe background color\n\nThis paragraph has a background color of #ebeefe.\n\n``<p style=\"background-color:#ebeefe;\">Content here</p>``\n#ebeefe border color\n\nThis element has a border color of #ebeefe.\n\n``<div style=\"border:1px solid #ebeefe;\">Content here</div>``\nCSS codes\n``.text {color:#ebeefe;}``\n``.background {background-color:#ebeefe;}``\n``.border {border:1px solid #ebeefe;}``\n\n# Shades and Tints of #ebeefe\n\nA shade is achieved by adding black to any pure hue, while a tint is created by mixing white to any pure color. In this example, #010311 is the darkest color, while #fefeff is the lightest one.\n\n• #010311\n``#010311` `rgb(1,3,17)``\n• #020724\n``#020724` `rgb(2,7,36)``\n• #030b37\n``#030b37` `rgb(3,11,55)``\n• #040f49\n``#040f49` `rgb(4,15,73)``\n• #05125c\n``#05125c` `rgb(5,18,92)``\n• #06166f\n``#06166f` `rgb(6,22,111)``\n• #061a81\n``#061a81` `rgb(6,26,129)``\n• #071e94\n``#071e94` `rgb(7,30,148)``\n• #0821a7\n``#0821a7` `rgb(8,33,167)``\n• #0925b9\n``#0925b9` `rgb(9,37,185)``\n• #0a29cc\n``#0a29cc` `rgb(10,41,204)``\n• #0b2ddf\n``#0b2ddf` `rgb(11,45,223)``\n• #0c30f2\n``#0c30f2` `rgb(12,48,242)``\n• #1e3ff4\n``#1e3ff4` `rgb(30,63,244)``\n• #304ff5\n``#304ff5` `rgb(48,79,245)``\n• #435ff6\n``#435ff6` `rgb(67,95,246)``\n• #566ff7\n``#566ff7` `rgb(86,111,247)``\n• #687ff7\n``#687ff7` `rgb(104,127,247)``\n• #7b8ff8\n``#7b8ff8` `rgb(123,143,248)``\n• #8e9ff9\n``#8e9ff9` `rgb(142,159,249)``\n• #a0aefa\n``#a0aefa` `rgb(160,174,250)``\n• #b3befb\n``#b3befb` `rgb(179,190,251)``\n• #c6cefc\n``#c6cefc` `rgb(198,206,252)``\n• #d8defd\n``#d8defd` `rgb(216,222,253)``\n• #ebeefe\n``#ebeefe` `rgb(235,238,254)``\n• #fefeff\n``#fefeff` `rgb(254,254,255)``\nTint Color Variation\n\n# Tones of #ebeefe\n\nA tone is produced by adding gray to any pure hue. In this case, #f4f4f5 is the less saturated color, while #eaedff is the most saturated one.\n\n• #f4f4f5\n``#f4f4f5` `rgb(244,244,245)``\n• #f3f4f6\n``#f3f4f6` `rgb(243,244,246)``\n• #f2f3f7\n``#f2f3f7` `rgb(242,243,247)``\n• #f1f2f8\n``#f1f2f8` `rgb(241,242,248)``\n• #f1f2f8\n``#f1f2f8` `rgb(241,242,248)``\n• #f0f1f9\n``#f0f1f9` `rgb(240,241,249)``\n• #eff1fa\n``#eff1fa` `rgb(239,241,250)``\n• #eef0fb\n``#eef0fb` `rgb(238,240,251)``\n• #edf0fc\n``#edf0fc` `rgb(237,240,252)``\n• #edeffc\n``#edeffc` `rgb(237,239,252)``\n• #eceffd\n``#eceffd` `rgb(236,239,253)``\n• #ebeefe\n``#ebeefe` `rgb(235,238,254)``\n• #eaedff\n``#eaedff` `rgb(234,237,255)``\nTone Color Variation\n\n# Color Blindness Simulator\n\nBelow, you can see how #ebeefe is perceived by people affected by a color vision deficiency. This can be useful if you need to ensure your color combinations are accessible to color-blind users.\n\nMonochromacy\n• Achromatopsia 0.005% of the population\n• Atypical Achromatopsia 0.001% of the population\nDichromacy\n• Protanopia 1% of men\n• Deuteranopia 1% of men\n• Tritanopia 0.001% of the population\nTrichromacy\n• Protanomaly 1% of men, 0.01% of women\n• Deuteranomaly 6% of men, 0.4% of women\n• Tritanomaly 0.01% of the population" ]
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http://www.softmath.com/math-com-calculator/inverse-matrices/simplify-cube-root-equation.html
[ "English | Español\n\n# Try our Free Online Math Solver!", null, "Online Math Solver\n\n Depdendent Variable\n\n Number of equations to solve: 23456789\n Equ. #1:\n Equ. #2:\n\n Equ. #3:\n\n Equ. #4:\n\n Equ. #5:\n\n Equ. #6:\n\n Equ. #7:\n\n Equ. #8:\n\n Equ. #9:\n\n Solve for:\n\n Dependent Variable\n\n Number of inequalities to solve: 23456789\n Ineq. #1:\n Ineq. #2:\n\n Ineq. #3:\n\n Ineq. #4:\n\n Ineq. #5:\n\n Ineq. #6:\n\n Ineq. #7:\n\n Ineq. #8:\n\n Ineq. #9:\n\n Solve for:\n\n Please use this form if you would like to have this math solver on your website, free of charge. 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https://ai.stackexchange.com/questions/20176/what-is-the-intuition-behind-the-dot-product-attention
[ "# What is the intuition behind the dot product attention?\n\nI am watching the video Attention Is All You Need by Yannic Kilcher.\n\nMy question is: what is the intuition behind the dot product attention?\n\n$$A(q,K, V) = \\sum_i\\frac{e^{q.k_i}}{\\sum_j e^{q.k_j}} v_i$$\n\nbecomes:\n\n$$A(Q,K, V) = \\text{softmax}(QK^T)V$$\n\nLet's start with a bit of notation and a couple of important clarifications.\n\n$$\\mathbf{Q}$$ refers to the query vectors matrix, $$q_i$$ being a single query vector associated with a single input word.\n\n$$\\mathbf{V}$$ refers to the values vectors matrix, $$v_i$$ being a single value vector associated with a single input word.\n\n$$\\mathbf{K}$$ refers to the keys vectors matrix, $$k_i$$ being a single key vector associated with a single input word.\n\nWhere do these matrices come from? Something that is not stressed out enough in a lot of tutorials is that these matrices are the result of a matrix product between the input embeddings and 3 matrices of trained weights: $$\\mathbf{W_q}$$, $$\\mathbf{W_v}$$, $$\\mathbf{W_k}$$.\n\nThe fact that these three matrices are learned during training explains why the query, value and key vectors end up being different despite the identical input sequence of embeddings. It also explains why it makes sense to talk about multi-head attention. Performing multiple attention steps on the same sentence produces different results, because, for each attention 'head', new $$\\mathbf{W_q}$$, $$\\mathbf{W_v}$$, $$\\mathbf{W_k}$$ are randomly initialised.\n\nAnother important aspect not stressed out enough is that for the encoder and decoder first attention layers, all the three matrices comes from the previous layer (either the input or the previous attention layer) but for the encoder/decoder attention layer, the $$\\mathbf{Q}$$ matrix comes from the previous decoder layer, whereas the $$\\mathbf{V}$$ and $$\\mathbf{K}$$ matrices come from the encoder. And this is a crucial step to explain how the representation of two languages in an encoder is mixed together.\n\nOnce computed the three matrices, the transformer moves on to the calculation of the dot product between query and key vectors. The dot product is used to compute a sort of similarity score between the query and key vectors. Indeed, the authors used the names query, key and value to indicate that what they propose is similar to what is done in information retrieval. For example, in question answering, usually, given a query, you want to retrieve the closest sentence in meaning among all possible answers, and this is done by computing the similarity between sentences (question vs possible answers).\n\nOf course, here, the situation is not exactly the same, but the guy who did the video you linked did a great job in explaining what happened during the attention computation (the two equations you wrote are exactly the same in vector and matrix notation and represent these passages):\n\n• closer query and key vectors will have higher dot products.\n• applying the softmax will normalise the dot product scores between 0 and 1.\n• multiplying the softmax results to the value vectors will push down close to zero all value vectors for words that had a low dot product score between query and key vector.\n\nIn the paper, the authors explain the attention mechanisms saying that the purpose is to determine which words of a sentence the transformer should focus on. I personally prefer to think of attention as a sort of coreference resolution step. The reason why I think so is the following image (taken from this presentation by the original authors).", null, "This image shows basically the result of the attention computation (at a specific layer that they don't mention). Bigger lines connecting words mean bigger values in the dot product between the words query and key vectors, which means basically that only those words value vectors will pass for further processing to the next attention layer. But, please, note that some words are actually related even if not similar at all, for example, 'Law' and 'The' are not similar, they are simply related to each other in these specific sentences (that's why I like to think of attention as a coreference resolution). Computing similarities between embeddings would never provide information about this relationship in a sentence, the only reason why transformer learn these relationships is the presences of the trained matrices $$\\mathbf{W_q}$$, $$\\mathbf{W_v}$$, $$\\mathbf{W_k}$$ (plus the presence of positional embeddings).\n\n• Ive been searching for how the attention is calculated, for the past 3 days. Your answer provided the closest explanation. Thank you. If you have more clarity on it, please write a blog post or create a Youtube video. It'd be a great help for everyone.\n– Nav\nJul 29, 2020 at 16:16\n• @Nav Hi, sorry but I saw your comment only now. I'm not really planning to write a blog post on this topic, mainly because I think that there are already good tutorials and video around that describe transformers in detail. Also, I saw that new posts are share every month, this one for example is really well made, hope you'll find it useful: peterbloem.nl/blog/transformers Aug 31, 2020 at 14:34\n• @Avatrin The weight matrices Eduardo is talking about here are not the raw dot product softmax wij that Bloem is writing about at the beginning of the article. The weight matrices here are an arbitrary choice of a linear operation that you make BEFORE applying the raw dot product self attention mechanism. These can technically come from anywhere, sure, but if you look at ANY implementation of the transformer architecture you will find that these are indeed learned parameters. Bloem covers this in entirety actually, so I don't quite understand your implication that Eduardo needs to reread it Mar 13, 2022 at 9:57\n• @TimSeguine Those linear layers are before the \"scaled dot-product attention\" as defined in Vaswani (seen in both equation 1 and figure 2 on page 4). They are however in the \"multi-head attention\". OPs question explicitly asks about equation 1. There are no weights in it. Mar 13, 2022 at 11:47\n• @Avatrin Yes that's true, the attention function itself is matrix valued and parameter free(And I never disputed that fact), but your original comment is still false: \"the three matrices W_q, W_k and W_v are not trained\". Neither how they are defined here nor in the referenced blog post is that true. Mar 13, 2022 at 14:46" ]
[ null, "https://i.stack.imgur.com/Nnm8a.jpg", null ]
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https://openaccess.biruni.edu.tr/xmlui/browse?value=%C4%B0n%C3%A7,%20Mustafa&type=author
[ "Now showing items 1-20 of 209\n\n• #### Abundant explicit solutions to fractional order nonlinear evolution equations \n\nWe utilize the modified Riemann-Liouville derivative sense to develop careful arrangements of time-fractional simplified modified Camassa-Holm (MCH) equations and generalized (3 + 1)-dimensional time-fractional ...\n• #### Abundant optical solitons to the sasa satsuma higher order nonlinear schrödinger equation \n\nThis paper investigates a diverse collection of exact solutions to a high-order nonlinear Schrödinger equation, called the Sasa-Satsuma equation. These results are obtained for this nonlinear equation using the generalized ...\n• #### Adequate soliton solutions to the space–time fractional telegraph equation and modified third-order KdV equation through a reliable technique \n\nThe space–time fractional Telegraph equation and the space–time fractional modifed thirdorder Kdv equations are signifcant molding equations in theoretic physics, mathematical physics, plasma physics also other felds of ...\n• #### Analysis and simulation of fractional order smoking epidemic model \n\nIn recent years, there are many new definitions that were proposed related to fractional derivatives, and with the help of these definitions, mathematical models were established to overcome the various real-life problems. ...\n• #### Analysis of dengue transmission using fractional order scheme \n\nIn this paper, we will check the existence and stability of the dengue internal transmission model with fraction order derivative as well as analyze it qualitatively. The solution has been determined using Atangana-Baleanu ...\n• #### Analysis of fractional COVID-19 epidemic model under Caputo operator \n\nThe article deals with the analysis of the fractional COVID-19 epidemic model (FCEM) with a convex incidence rate. Keeping in view the fading memory and crossover behavior found in many biological phenomena, we study the ...\n• #### Analysis of fractional MHD convective flow with CTNs’ nanoparticles and radiative heat flux in human blood \n\nAbstract The aim of the article is two-fold. We first analyze and investigate free convective, unsteady, MHD blood flow with single- and multiwalled carbon nanotubes (S&MWCNTs) as nanoparticles. The blood flow has been ...\n• #### Analysis of fractional order diarrhea model using fractal fractional operator \n\nIn this paper, we construct a scheme of fractional-order mathematical model for the population infected by diarrhea disease by using the four compartments S, I, T and R. The fractal-fractional derivative operator (FFO) ...\n• #### Analysis of fractional-order nonlinear dynamic systems under Caputo differential operator \n\nThe current study presents a detailed analysis of two crucial real-world problems under the Caputo fractional derivative in order to deliver some desired results for the ecosystem. In view of the fact that memory effect ...\n• #### Analysis of novel fractional COVID-19 model with real-life data application \n\nThe current work is of interest to introduce a detailed analysis of the novel fractional COVID-19 model. Non-local fractional operators are one of the most efficient tools in order to understand the dynamics of the disease ...\n• #### An analytical approach to the solution of fractional-coupled modified equal width and fractional - coupled Burgers equations \n\nWe opted to construct a traveling wave solution to the nonlinear space-time fractional coupled modified equal width (CMEW) equation and the space-time fractional-coupled Burgers equation, which are often used as an ...\n• #### Analytical novel solutions to the fractional optical dynamics in a medium with polynomial law nonlinearity and higher order dispersion with a new local fractional derivative \n\nNovel solutions for the nonlinear dynamics of Schrödinger equation for polynomial law medium with third-order dispersion (TOD), fourth-order dispersion (FOD), and self-steepening are investigated based in a novel local ...\n• #### Analytical solutions of the fifth-order time fractional nonlinear evolution equations by the unified method \n\n(World Scientific Publishing, 20.01.2022)\nThis key purpose of this study is to investigate soliton solution of the fifth-order Sawada-Kotera and Caudrey-Dodd-Gibbon equations in the sense of time fractional local M-derivatives. This important goal is achieved by ...\n• #### Analytical solutions to the fractional lakshmanan-porsezian-daniel model \n\nA new local fractional-order derivative operator is introduced and the Lakshmanan–Porsezian–Daniel (LPD) model is interpreted via this operator. New analytical solutions to the LPD equation is presented by Jacobi elliptic ...\n• #### Analytical study of nonlinear water wave equations for their fractional solution structures \n\nThis paper examines the three-dimensional nonlinear time-fractional water wave equations for their analytical wave solutions. These are the equations of the names (3 + 1)-Zakharov-Kuznetsov-Burgers equation and (3 + ...\n• #### Attitude of the modulation instability gain in oppositely directed coupler with the effects of the intrapulse raman scattering and saturable function \n\nTo establish the effects of the Higher-Order Dispersion (HOD) and Raman Scattering (RS) on ModulationInstability (MI) in the presence of the Saturable Function (SF), it is used the Coupled Nonlinear SchrödingerEquation ...\n• #### Bifurcation of new optical solitary wave solutions for the nonlinear long-short wave interaction system via two improved models of (G′G) expansion method \n\nThis study performs two recent methods on the nonlinear long-short wave interaction system (NLSWIS) to obtain novel formulas of solitary solutions representing an optical feld that does not alter by multiplication a sensitive ...\n• #### Boundary value problem for nonlinear fractional differential equations of variable order via kuratowski MNC technique \n\nIn the present research study, for a given multiterm boundary value problem (BVP) involving the Riemann-Liouville fractional differential equation of variable order, the existence properties are analyzed. To achieve this ...\n• #### Boundary value problem of Riemann-Liouville fractional differential equations in the variable exponent Lebesgue spaces Lp(.) \n\nThis manuscript deals with the existence, uniqueness and stability of solutions to the boundary value problem (BVP) of Riemann-Liouville (RL) fractional differential equations (FDEs) in the variable exponent Lebesgue spaces ...\n• #### Breather wave, lump - periodic solutions and some other interaction phenomena to the Caudrey – Dodd – Gibbon equation \n\n(Springer Nature Switzerland, 12.07.2020)\nHirota’s bilinear method is used in this paper to obtain some breather wave and lumps solutions to the Caudrey–Dodd–Gibbon equation through the symbolic Mathematica 12 package. This equation is converted into its potential ..." ]
[ null ]
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https://www.intlpress.com/site/pub/pages/journals/items/mrl/content/vols/0013/0006/a003/index.php
[ "# Mathematical Research Letters\n\n## Volume 13 (2006)\n\n### Lipschitz harmonic capacity and Bilipschitz images of cantor sets\n\nPages: 865 – 884\n\nDOI: https://dx.doi.org/10.4310/MRL.2006.v13.n6.a3\n\n#### Authors\n\nJohn Garnett (University of California at Los Angeles)\n\nLaura Prat (Universitat de Barcelona)\n\nXavier Tolsa (Universitat Autonoma de Barcelona)\n\n#### Abstract\n\nFor bilipschitz images of Cantor sets in $\\Rd$ we estimate the Lipschitz harmonic capacity and prove that this capacity is invariant under bilipschitz homeomorphisms. A crucial step of the proof is an estimate of the $L^2$ norms of the Riesz tranforms on $L^2(G,p)$ where $p$ is the natural probability measure on the Cantor set $E$ and $G \\subset E$ has $p(G) > 0.$\n\nPublished 1 January 2006" ]
[ null ]
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https://scholar.archive.org/work/watihvs5nvewxovyqj5e5rwncm
[ "### Improved AMP (IAMP) for non-ideal measurement matrices\n\nYang Lu, Wei Dai\n2015 2015 23rd European Signal Processing Conference (EUSIPCO)\nThis paper studies the sparse recovery problem. Of particular interest is the well known approximate message passing (AMP) algorithm. AMP enjoys low computational complexity and good performance guarantees. However, the algorithm and performance analysis heavily rely on the assumption that the measurement matrix is a standard Gaussian random matrix. The main contribution of this paper is an improved AMP (IAMP) algorithm that works better for non-ideal measurement matrices. The algorithm is\nmore » ... e algorithm is equivalent to AMP for standard Gaussian random matrices but provides better recovery when the correlations between columns of the measurement matrix deviate from those of the standard Gaussian random matrices. The derivation is based on a modification of the message passing mechanism that removes the conditional independence assumption. Examples are provided to demonstrate the performance improvement of IAMP where both a particularly designed matrix and a matrix from real applications are used. Index Terms-AMP, compressed sensing, message passing, sparse signal processing, standard Gaussian random matrix." ]
[ null ]
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https://byjus.com/question-answer/arrhenius-studied-the-effect-of-temperature-on-the-rate-of-a-reaction-and-postulated-that-1/
[ "", null, "", null, "Question\n\n# Arrhenius studied the effect of temperature on the rate of a reaction and postulated that rate constant varies with temperature exponentially as k=Ae−EaRT This method is generally used for finding the activation energy of a reaction. Keeping temperature constant, the effect of catalyst on the activation energy has also been studied. If x is the fraction of molecules having energy greater than Ea it will be given by:x=EaRTx=eEa×RTAny of theseln x=−EaRT\n\nSolution\n\n## The correct option is D ln x=−EaRTIn the Arrhenius equation the factor e−EaRT corresponds to the fraction of molecules that have kinetic energy greater than Ea.  x=e−EaRT Taking natural logarithm of both sides of the equation ln x=−EaRT", null, "", null, "Suggest corrections", null, "", null, "", null, "" ]
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http://research.omicsgroup.org/index.php/Natural_units
[ "Natural units\n\nIn physics, natural units are physical units of measurement based only on universal physical constants. For example, the elementary charge e is a natural unit of electric charge, and the speed of light c is a natural unit of speed. A purely natural system of units has all of its units defined in this way, and usually such that the numerical values of the selected physical constants in terms of these units are exactly 1. These constants are then typically omitted from mathematical expressions of physical laws, and while this has the apparent advantage of simplicity, it may entail a loss of clarity due to the loss of information for dimensional analysis.\n\nIntroduction\n\nNatural units are intended to elegantly simplify particular algebraic expressions appearing in the laws of physics or to normalize some chosen physical quantities that are properties of universal elementary particles and are reasonably believed to be constant. However there is a choice of the set of natural units chosen, and quantities which are set to unity in one system may take a different value or even be assumed to vary in another natural unit system.\n\nNatural units are \"natural\" because the origin of their definition comes only from properties of nature and not from any human construct. Planck units are often, without qualification, called \"natural units\", although they constitute only one of several systems of natural units, albeit the best known such system. Planck units (up to a simple multiplier for each unit) might be considered one of the most \"natural\" systems in that the set of units is not based on properties of any prototype, object, or particle but are solely derived from the properties of free space.\n\nAs with other systems of units, the base units of a set of natural units will include definitions and values for length, mass, time, temperature, and electric charge (in lieu of electric current). Some physicists do not recognize temperature as a fundamental physical quantity,[citation needed] since it expresses the energy per degree of freedom of a particle, which can be expressed in terms of energy (or mass, length, and time). Virtually every system of natural units normalizes Boltzmann's constant kB to 1, which can be thought of as simply a way of defining the unit temperature.\n\nIn the SI unit system, electric charge is a separate fundamental dimension of physical quantity, but in natural unit systems charge is expressed in terms of the mechanical units of mass, length, and time, similarly to cgs. There are two common ways to relate charge to mass, length, and time: In Lorentz–Heaviside units (also called \"rationalized\"), Coulomb's law is F = q1q2/(4πr2), and in Gaussian units (also called \"non-rationalized\"), Coulomb's law is F = q1q2/r2. Both possibilities are incorporated into different natural unit systems.\n\nNotation and use\n\nNatural units are most commonly used by setting the units to one. For example, many natural unit systems include the equation c = 1 in the unit-system definition, where c is the speed of light. If a velocity v is half the speed of light, then as v = 1/2c and c = 1, hence v = 1/2. The equation v = 1/2 means \"the velocity v has the value one-half when measured in Planck units\", or \"the velocity v is one-half the Planck unit of velocity\".\n\nThe equation c = 1 can be plugged in anywhere else. For example, Einstein's equation E = mc2 can be rewritten in Planck units as E = m. This equation means \"The energy of a particle, measured in Planck units of energy, equals the mass of the particle, measured in Planck units of mass.\"\n\nCompared to SI or other unit systems, natural units have both advantages and disadvantages:\n\n• Simplified equations: By setting constants to 1, equations containing those constants appear more compact and in some cases may be simpler to understand. For example, the special relativity equation E2 = p2c2 + m2c4 appears somewhat complicated, but the natural units version, E2 = p2 + m2, appears simpler.\n• Physical interpretation: Natural unit systems automatically subsume dimensional analysis. For example, in Planck units, the units are defined by properties of quantum mechanics and gravity. Not coincidentally, the Planck unit of length is approximately the distance at which quantum gravity effects become important. Likewise, atomic units are based on the mass and charge of an electron, and not coincidentally the atomic unit of length is the Bohr radius describing the orbit of the electron in a hydrogen atom.\n• No prototypes: A prototype is a physical object that defines a unit, such as the International Prototype Kilogram, a physical cylinder of metal whose mass is by definition exactly one kilogram. A prototype definition always has imperfect reproducibility between different places and between different times, and it is an advantage of natural unit systems that they use no prototypes. (They share this advantage with other non-natural unit systems, such as conventional electrical units.)\n• Less precise measurements: SI units are designed to be used in precision measurements. For example, the second is defined by an atomic transition frequency in cesium atoms, because this transition frequency can be precisely reproduced with atomic clock technology. Natural unit systems are generally not based on quantities that can be precisely reproduced in a lab. Therefore, in order to retain the same degree of precision, the fundamental constants used still have to be measured in a laboratory in terms of physical objects that can be directly observed. If this is not possible, then a quantity expressed in natural units can be less precise than the same quantity expressed in SI units. For example, Planck units use the gravitational constant G, which is measurable in a laboratory only to four significant digits.\n\nChoosing constants to normalize\n\nOut of the many physical constants, the designer of a system of natural unit systems must choose a few of these constants to normalize (set equal to 1). It is not possible to normalize just any set of constants. For example, the mass of a proton and the mass of an electron cannot both be normalized: if the mass of an electron is defined to be 1, then the mass of a proton has to be approximately 1836. In a less trivial example, the fine-structure constant, α ≈ 1/137, cannot be set to 1, because it is a dimensionless number. The fine-structure constant is related to other fundamental constants\n\n$\\alpha = \\frac{k_\\text{e} e^2}{\\hbar c},$\n\nwhere ke is the Coulomb constant, e is the elementary charge, ℏ is the reduced Planck constant, and c is the speed of light. Therefore it is not possible to simultaneously normalize all four of the constants c, ℏ, e, and ke.\n\nElectromagnetism units\n\nIn SI units, electric charge is expressed in coulombs, a separate unit which is additional to the \"mechanical\" units (mass, length, time), even though the traditional definition of the ampere refers to some of these other units. In natural unit systems, however, electric charge has units of [mass]1/2 [length]3/2 [time]−1.\n\nThere are two main natural unit systems for electromagnetism:\n\nOf these, Lorentz–Heaviside is somewhat more common, mainly because Maxwell's equations are simpler in Lorentz-Heaviside units than they are in Gaussian units.\n\nIn the two unit systems, the elementary charge e satisfies:\n\n• $e = \\sqrt{4 \\pi \\alpha \\hbar c}$ (Lorentz–Heaviside),\n• $e = \\sqrt{\\alpha \\hbar c}$ (Gaussian)\n\nwhere ℏ is the reduced Planck constant, c is the speed of light, and α ≈ 1/137 is the fine-structure constant.\n\nIn a natural unit system where c = 1, Lorentz–Heaviside units can be derived from SI units by setting ε0 = μ0 = 1. Gaussian units can be derived from SI units by a more complicated set of transformations, such as multiplying all electric fields by (4πε0)−1/2, multiplying all magnetic susceptibilities by 4π, and so on.\n\nSystems of natural units\n\nPlanck units\n\nMain article: Planck units\nQuantity Expression Metric value Name\nLength (L) $l_\\text{P} = \\sqrt{\\hbar G \\over c^3}$ 1.616×1035Lua error: Unmatched close-bracket at pattern character 67. Planck length\nMass (M) $m_\\text{P} = \\sqrt{\\hbar c \\over G}$ 2.176×108Lua error: Unmatched close-bracket at pattern character 67. Planck mass\nTime (T) $t_\\text{P} = \\sqrt{\\hbar G \\over c^5}$ 5.3912×1044Lua error: Unmatched close-bracket at pattern character 67. Planck time\nTemperature (Θ) $T_\\text{P} = \\sqrt{\\frac{\\hbar c^5}{G {k_\\text{B}}^2}}$ 1.417×1032Lua error: Unmatched close-bracket at pattern character 67. Planck temperature\nElectric charge (Q) $q_\\text{P} = \\sqrt{\\hbar c \\over k_\\text{e}}$ 1.876×1018Lua error: Unmatched close-bracket at pattern character 67. Planck charge\n\nPlanck units are defined by\n\n$c = \\hbar = G = k_\\text{e} = k_\\text{B} = 1 ,$\n\nwhere c is the speed of light, ℏ is the reduced Planck constant, G is the gravitational constant, ke is the Coulomb constant, and kB is the Boltzmann constant.\n\nPlanck units are a system of natural units that is not defined in terms of properties of any prototype, physical object, or even elementary particle. They only refer to the basic structure of the laws of physics: c and G are part of the structure of spacetime in general relativity, and ℏ captures the relationship between energy and frequency which is at the foundation of quantum mechanics. This makes Planck units particularly useful and common in theories of quantum gravity, including string theory.\n\nPlanck units may be considered \"more natural\" even than other natural unit systems discussed below, as Planck units are not based on any arbitrarily chosen prototype object or particle. For example, some other systems use the mass of an electron as a parameter to be normalized. But the electron is just one of 16 known massive elementary particles, all with different masses, and there is no compelling reason, within fundamental physics, to emphasize the electron mass over some other elementary particle's mass.\n\nStoney units\n\nMain article: Stoney units\nQuantity Expression Metric value\nLength (L) $l_\\text{S} = \\sqrt{\\frac{G k_\\text{e} e^2}{c^4}}$ 1.381×1036Lua error: Unmatched close-bracket at pattern character 67.\nMass (M) $m_\\text{S} = \\sqrt{\\frac{k_\\text{e} e^2}{G}}$ 1.859×109Lua error: Unmatched close-bracket at pattern character 67.\nTime (T) $t_\\text{S} = \\sqrt{\\frac{G k_\\text{e} e^2}{c^6}}$ 4.605×1045Lua error: Unmatched close-bracket at pattern character 67.\nTemperature (Θ) $T_\\text{S} = \\sqrt{\\frac{c^4 k_\\text{e} e^2}{G {k_\\text{B}}^2}}$ 1.210×1031Lua error: Unmatched close-bracket at pattern character 67.\nElectric charge (Q) $q_\\text{S} = e \\$ 1.602×1019Lua error: Unmatched close-bracket at pattern character 67.\n\nStoney units are defined by:\n\n$c = G = k_\\text{e} = e = k_\\text{B} = 1 ,$\n\nwhere c is the speed of light, G is the gravitational constant, ke is the Coulomb constant, e is the elementary charge, and kB is the Boltzmann constant.\n\nGeorge Johnstone Stoney was the first physicist to introduce the concept of natural units. He presented the idea in a lecture entitled \"On the Physical Units of Nature\" delivered to the British Association in 1874. Stoney units differ from Planck units by fixing the elementary charge at 1, instead of Planck's constant (only discovered after Stoney's proposal).\n\nStoney units are rarely used in modern physics for calculations, but they are of historical interest.\n\nAtomic units\n\nMain article: Atomic units\nQuantity Expression\n(Hartree atomic units)\nMetric value\n(Hartree atomic units)\nLength (L) $l_\\text{A} = \\frac{\\hbar^2 (4 \\pi \\epsilon_0)}{m_\\text{e} e^2}$ 5.292×1011Lua error: Unmatched close-bracket at pattern character 67.\nMass (M) $m_\\text{A} = m_\\text{e} \\$ 9.109×1031Lua error: Unmatched close-bracket at pattern character 67.\nTime (T) $t_\\text{A} = \\frac{\\hbar^3 (4 \\pi \\epsilon_0)^2}{m_\\text{e} e^4}$ 2.419×1017Lua error: Unmatched close-bracket at pattern character 67.\nElectric charge (Q) $q_\\text{A} = e \\$ 1.602×1019Lua error: Unmatched close-bracket at pattern character 67.\nTemperature (Θ) $T_\\text{A} = \\frac{m_\\text{e} e^4}{\\hbar^2 (4 \\pi \\epsilon_0)^2 k_\\text{B}}$ 3.158×105Lua error: Unmatched close-bracket at pattern character 67.\n\nThere are two types of atomic units, closely related.\n\nHartree atomic units:\n\n$e = m_\\text{e} = \\hbar = k_\\text{e} = k_\\text{B} = 1 \\$\n$c = \\frac{1}{\\alpha} \\$\n\nRydberg atomic units:\n\n$\\frac{e}{\\sqrt{2}} = 2m_\\text{e} = \\hbar = k_\\text{e} = k_\\text{B} = 1 \\$\n$c = \\frac{2}{\\alpha} \\$\n\nCoulomb's constant ($k_\\text{e}$) is generally expressed as $\\frac{1}{4\\pi\\varepsilon_0}$\n\nThese units are designed to simplify atomic and molecular physics and chemistry, especially the hydrogen atom, and are widely used in these fields. The Hartree units were first proposed by Douglas Hartree, and are more common than the Rydberg units.\n\nThe units are designed especially to characterize the behavior of an electron in the ground state of a hydrogen atom. For example, using the Hartree convention, in the Bohr model of the hydrogen atom, an electron in the ground state has orbital velocity = 1, orbital radius = 1, angular momentum = 1, ionization energy = 1/2, etc.\n\nThe unit of energy is called the Hartree energy in the Hartree system and the Rydberg energy in the Rydberg system. They differ by a factor of 2. The speed of light is relatively large in atomic units (137 in Hartree or 274 in Rydberg), which comes from the fact that an electron in hydrogen tends to move much slower than the speed of light. The gravitational constant is extremely small in atomic units (around 10−45), which comes from the fact that the gravitational force between two electrons is far weaker than the Coulomb force. The unit length, lA, is the Bohr radius, a0.\n\nThe values of c and e shown above imply that e = (αℏc)1/2, as in Gaussian units, not Lorentz–Heaviside units. However, hybrids of the Gaussian and Lorentz–Heaviside units are sometimes used, leading to inconsistent conventions for magnetism-related units.\n\nQuantum chromodynamics (QCD) units\n\nQuantity Expression Metric value\nLength (L) $l_{\\mathrm{QCD}} = \\frac{\\hbar}{m_\\text{p} c}$ 2.103×1016Lua error: Unmatched close-bracket at pattern character 67.\nMass (M) $m_{\\mathrm{QCD}} = m_\\text{p} \\$ 1.673×1027Lua error: Unmatched close-bracket at pattern character 67.\nTime (T) $t_{\\mathrm{QCD}} = \\frac{\\hbar}{m_\\text{p} c^2}$ 7.015×1025Lua error: Unmatched close-bracket at pattern character 67.\nTemperature (Θ) $T_{\\mathrm{QCD}} = \\frac{m_\\text{p} c^2}{k_\\text{B}}$ 1.089×1013Lua error: Unmatched close-bracket at pattern character 67.\nElectric charge (Q) $q_\\mathrm{QCD} = e/\\sqrt{4\\pi\\alpha}$ (L–H) 5.291×1019Lua error: Unmatched close-bracket at pattern character 67.\n$q_\\mathrm{QCD} = e/\\sqrt{\\alpha}$ (G) 1.876×1018Lua error: Unmatched close-bracket at pattern character 67.\n$c = m_\\text{p} = \\hbar = k_\\text{B} = 1 \\$\n\nThe electron mass is replaced with that of the proton. Strong units are \"convenient for work in QCD and nuclear physics, where quantum mechanics and relativity are omnipresent and the proton is an object of central interest\".\n\n\"Natural units\" (particle physics and cosmology)\n\nUnit Metric value Derivation\n1 eV−1 of length 1.97×107Lua error: Unmatched close-bracket at pattern character 67. $=(1\\,\\text{eV}^{-1})\\hbar c$\n1 eV of mass 1.78×1036Lua error: Unmatched close-bracket at pattern character 67. $= (1\\,\\text{eV})/c^2$\n1 eV−1 of time 6.58×1016Lua error: Unmatched close-bracket at pattern character 67. $=(1\\,\\text{eV}^{-1})\\hbar$\n1 eV of temperature 1.16×104Lua error: Unmatched close-bracket at pattern character 67. $= 1\\,\\text{eV}/k_\\text{B}$\n1 unit of electric charge\n(L–H)\n5.29×1019Lua error: Unmatched close-bracket at pattern character 67. $=e/\\sqrt{4\\pi\\alpha}$\n1 unit of electric charge\n(G)\n1.88×1018Lua error: Unmatched close-bracket at pattern character 67. $=e/\\sqrt{\\alpha}$\n\nIn particle physics and cosmology, the phrase \"natural units\" generally means:\n\n$\\hbar = c = k_\\text{B} = 1.$\n\nwhere $\\hbar$ is the reduced Planck constant, c is the speed of light, and kB is the Boltzmann constant.\n\nBoth Planck units and QCD units are this type of Natural units. Like the other systems, the electromagnetism units can be based on either Lorentz–Heaviside units or Gaussian units. The unit of charge is different in each.\n\nFinally, one more unit is needed to construct a usable system of units that includes energy and mass. Most commonly, electron-volt (eV) is used, despite the fact that this is not a \"natural\" unit in the sense discussed above – it is defined by a natural property, the elementary charge, and the anthropogenic unit of electric potential, the volt. (The SI prefixed multiples of eV are used as well: keV, MeV, GeV, etc.)\n\nWith the addition of eV (or any other auxiliary unit with the proper dimension), any quantity can be expressed. For example, a distance of 1.0 cm can be expressed in terms of eV, in natural units, as:\n\n$1.0\\, \\text{cm} = \\frac{1.0\\, \\text{cm}}{\\hbar c} \\approx 51000\\, \\text{eV}^{-1}$\n\nGeometrized units\n\n$c = G = 1 \\$\n\nThe geometrized unit system, used in general relativity, is not a completely defined system. In this system, the base physical units are chosen so that the speed of light and the gravitational constant are set equal to unity. Other units may be treated however desired. Planck units and Stoney units are examples of geometrized unit systems.\n\nSummary table\n\nQuantity / Symbol Planck\n(with Gauss)\nStoney Hartree Rydberg \"Natural\"\n(with L-H)\n\"Natural\"\n(with Gauss)\nSpeed of light in vacuum\n$c \\,$\n$1 \\,$ $1 \\,$ $\\frac{1}{\\alpha} \\$ $\\frac{2}{\\alpha} \\$ $1 \\,$ $1 \\,$\nPlanck's constant (reduced)\n$\\hbar=\\frac{h}{2 \\pi}$\n$1 \\,$ $\\frac{1}{\\alpha} \\$ $1 \\,$ $1 \\,$ $1 \\,$ $1 \\,$\nElementary charge\n$e \\,$\n$\\sqrt{\\alpha} \\,$ $1 \\,$ $1 \\,$ $\\sqrt{2} \\,$ $\\sqrt{4\\pi\\alpha}$ $\\sqrt{\\alpha}$\nJosephson constant\n$K_\\text{J} =\\frac{e}{\\pi \\hbar} \\,$\n$\\frac{\\sqrt{\\alpha}}{\\pi} \\,$ $\\frac{\\alpha}{\\pi} \\,$ $\\frac{1}{\\pi} \\,$ $\\frac{\\sqrt{2}}{\\pi} \\,$ $\\sqrt{\\frac{4\\alpha}{\\pi}} \\,$ $\\frac{\\sqrt{\\alpha}}{\\pi} \\,$\nvon Klitzing constant\n$R_\\text{K} =\\frac{2 \\pi \\hbar}{e^2} \\,$\n$\\frac{2\\pi}{\\alpha} \\,$ $\\frac{2\\pi}{\\alpha} \\,$ $2\\pi \\,$ $\\pi \\,$ $\\frac{1}{2\\alpha}$ $\\frac{2 \\pi}{\\alpha}$\nGravitational constant\n$G \\,$\n$1 \\,$ $1 \\,$ $\\frac{\\alpha_\\text{G}}{\\alpha} \\,$ $\\frac{8 \\alpha_\\text{G}}{\\alpha} \\,$ $\\frac{\\alpha_\\text{G}}{{m_\\text{e}}^2} \\,$ $\\frac{\\alpha_\\text{G}}{{m_\\text{e}}^2} \\,$\nBoltzmann constant\n$k_\\text{B} \\,$\n$1 \\,$ $1 \\,$ $1 \\,$ $1 \\,$ $1 \\,$ $1 \\,$\nElectron mass\n$m_\\text{e} \\,$\n$\\sqrt{\\alpha_\\text{G}} \\,$ $\\sqrt{\\frac{\\alpha_\\text{G}}{\\alpha}} \\,$ $1 \\,$ $\\frac{1}{2} \\,$ $511 \\text{ keV}$ $511 \\text{ keV}$\n\nwhere:" ]
[ null ]
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https://planetmath.org/TensorProductBasis
[ "# tensor product basis\n\nThe following theorem", null, "", null, "describes a basis of the tensor product (http://planetmath.org/TensorProduct) of two vector spaces", null, "", null, ", in terms of given bases of the spaces. In passing, it also gives a construction of this tensor product. The exact same method can be used also for free modules over a commutative ring with unit.\n\ntensor product\n\n• Theorem.  Let $U$ and $V$ be vector spaces over a field $\\mathcal{K}$ with bases\n\n $\\{\\mathbf{e}_{i}\\}_{i\\in I}\\quad\\text{and}\\quad\\{\\mathbf{f}_{j}\\}_{j\\in J}$\n\nrespectively. Then\n\n $\\{\\mathbf{e}_{i}\\otimes\\mathbf{f}_{j}\\}_{(i,j)\\in I\\times J}$ (1)\n\nis a basis for the tensor product space $U\\otimes V$.\n\n###### Proof.\n\nLet\n\n $W=\\left\\{\\,\\psi\\colon I\\times J\\longrightarrow\\mathcal{K}\\,\\,\\vrule width 1px% \\big{.}\\,\\,f^{-1}\\bigl{(}\\mathcal{K}\\setminus\\{0\\}\\bigr{)}\\text{ is finite}\\,% \\right\\}\\text{;}$\n\nthis set is obviously a $\\mathcal{K}$-vector-space under pointwise addition and multiplication", null, "", null, "by scalar (see also this (http://planetmath.org/FreeVectorSpaceOverASet) article). Let $p\\colon U\\times V\\longrightarrow W$ be the bilinear map which satisfies\n\n $p(\\mathbf{e}_{i},\\mathbf{f}_{j})(k,l)=\\begin{cases}1&\\text{if $$i=k$$ and $$j=% l$$,}\\\\ 0&\\text{otherwise}\\end{cases}$ (2)\n\nfor all $i,k\\in I$ and $j,l\\in J$, i.e., $p(\\mathbf{e}_{i},\\mathbf{f}_{j})\\in W$ is the characteristic function", null, "", null, "", null, "", null, "of $\\bigl{\\{}(i,j)\\bigr{\\}}$. The reasons (2) uniquely defines $p$ on the whole of $U\\times V$ are that $\\{\\mathbf{e}_{i}\\}_{i\\in I}$ is a basis of $U$, $\\{\\mathbf{f}_{i}\\}_{j\\in J}$ is a basis of $V$, and $p$ is bilinear.\n\nObserve that\n\n $\\bigl{\\{}p(\\mathbf{e}_{i},\\mathbf{f}_{j})\\bigr{\\}}_{(i,j)\\in I\\times J}$\n\nis a basis of $W$. Since one may always define a linear map by giving its values on the basis elements, this implies that there for every $\\mathcal{K}$-vector-space $X$ and every map $\\gamma\\colon U\\times V\\longrightarrow X$ exists a unique linear map $\\widehat{\\gamma}\\colon W\\longrightarrow X$ such that\n\n $\\widehat{\\gamma}\\bigl{(}p(\\mathbf{e}_{i},\\mathbf{f}_{j})\\bigr{)}=\\gamma(% \\mathbf{e}_{i},\\mathbf{f}_{j})\\quad\\text{for all $$i\\in I$$ and $$j\\in J$$.}$\n\nFor $\\gamma$ that are bilinear it holds for arbitrary $\\mathbf{u}=\\sum_{i\\in I^{\\prime}}u_{i}\\mathbf{e}_{i}\\in U$ and $\\mathbf{v}=\\sum_{j\\in J^{\\prime}}v_{j}\\mathbf{f}_{j}\\in V$ that $\\gamma(\\mathbf{u},\\mathbf{v})=(\\widehat{\\gamma}\\circ\\nobreak p)(\\mathbf{u},% \\mathbf{v})$, since\n\n $\\displaystyle\\gamma(\\mathbf{u},\\mathbf{v})=\\gamma\\biggl{(}\\sum_{i\\in I^{\\prime% }}u_{i}\\mathbf{e}_{i},\\sum_{j\\in J^{\\prime}}v_{j}\\mathbf{f}_{j}\\biggr{)}=\\sum_% {i\\in I^{\\prime}}\\sum_{j\\in J^{\\prime}}u_{i}v_{j}\\gamma(\\mathbf{e}_{i},\\mathbf% {f}_{j})=\\\\ \\displaystyle=\\sum_{i\\in I^{\\prime}}\\sum_{j\\in J^{\\prime}}u_{i}v_{j}\\widehat{% \\gamma}\\bigl{(}p(\\mathbf{e}_{i},\\mathbf{f}_{j})\\bigr{)}=\\widehat{\\gamma}\\biggl% {(}\\sum_{i\\in I^{\\prime}}\\sum_{j\\in J^{\\prime}}u_{i}v_{j}p(\\mathbf{e}_{i},% \\mathbf{f}_{j})\\biggr{)}=\\\\ \\displaystyle=\\widehat{\\gamma}\\Biggl{(}p\\biggl{(}\\sum_{i\\in I^{\\prime}}u_{i}% \\mathbf{e}_{i},\\sum_{j\\in J^{\\prime}}v_{j}\\mathbf{f}_{j}\\biggr{)}\\Biggr{)}=% \\widehat{\\gamma}\\bigl{(}p(\\mathbf{u},\\mathbf{v})\\bigr{)}\\text{.}$\n\nAs this is the defining property of the tensor product $U\\otimes V$ however, it follows that $W$ is (an incarnation of) this tensor product, with $\\mathbf{u}\\otimes\\mathbf{v}:=p(\\mathbf{u},\\mathbf{v})$. Hence the claim in the theorem is equivalent", null, "", null, "", null, "", null, "", null, "to the observation about the basis of $W$. ∎\n\nTitle tensor product basis TensorProductBasis 2013-03-22 15:24:48 2013-03-22 15:24:48 lars_h (9802) lars_h (9802) 11 lars_h (9802) Theorem msc 15A69 basis construction of tensor product TensorProduct FreeVectorSpaceOverASet" ]
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https://testbook.com/question-answer/the-life-of-a-ball-bearing-at-a-load-of-10-kn-is-8--58492cd1995a2d564c716dbc
[ "# The life of a ball bearing at a load of 10 kN is 8000 hours. If the load is increased to 20 kN, keeping all other conditions the same, then its life in hours is\n\nThis question was previously asked in\nISRO Scientist ME 2015 Paper\nView all ISRO Scientist ME Papers >\n1. 4000\n2. 2000\n3. 1000\n4. 500\n\nOption 3 : 1000\nFree\nST 1: Logical reasoning\n5333\n20 Questions 20 Marks 20 Mins\n\n## Detailed Solution\n\nConcept:\n\nThe approximate rating of the service life of a ball or roller bearing is based on the given fundamental equation.\n\n$${\\rm{L}} = {\\left( {\\frac{{\\rm{C}}}{{\\rm{P}}}} \\right)^{\\rm{k}}} \\times {10^6}{\\rm{revolution}}$$\n\nwhere L is rating lifeC is a basic dynamic load, P is an equivalent dynamic load\n\nk = 3 for ball bearing\n\nk = 10/3 for roller bearing\n\nCalculation:\n\nGiven:\n\nL1 = 8000 hr, P1 = 10 kN, P2 = 20 kN\n\n$$L = {\\left( {\\frac{C}{P}} \\right)^3}\\Rightarrow L\\ \\ \\ \\alpha \\ \\ { {\\frac{1}{P^3}} }\\\\ \\Rightarrow \\frac{{{L_1}}}{{{L_2}}} ={\\left( {\\frac{P_2}{P_1}} \\right)^3}= {2^3}\\\\ \\Rightarrow {L_2} = \\frac{{{L_1}}}{{8}}=\\frac{{{8000}}}{{8}}=1000\\ hours$$" ]
[ null ]
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https://www.jiskha.com/questions/1214461/find-the-probability-for-the-experiment-of-tossing-a-six-sided-die-twice-put-the-answer
[ "# Math\n\nFind the probability for the experiment of tossing a six-sided die twice. Put the answer in a/b form.\n\nP(the sum is odd or prime)\n\n1. 👍\n2. 👎\n3. 👁\n1. I suggest you make a table of sums for 6 rows and 6 columns from the numbers from 1 to 6\nFill in the sums, e.g. the first row and last row would be\n2 3 4 5 6 7\n....\n7 8 9 10 11 12\n\ncount up all the odd ones, obviously 18 of them\nRemember 2 is a prime number so it must be included as well\nAll other primes would be odd, and are already counted.\nso prob(of your event) = 19/36\n\n1. 👍\n2. 👎\n\n## Similar Questions\n\n1. ### Statistics\n\nFind the probability of getting a prime number thrice by tossing a die 10 times.\n\n2. ### math\n\nA six-sided, fair number cube is rolled 100 times as part of an experiment. The frequency of the roll of the number 3 is 20. Which statement about rolling a 3 is correct? The theoretical probability is 1/6. The experimental\n\n3. ### math\n\nA pair of dice is rolled, and a number that appears uppermost on each die is observed, Refer to this experiment and find the probability of the given event. (Enter your answer as a fraction)The sume of the numbers ia an add\n\n4. ### math\n\ntwo 6 sided dice are rolled . what is the probability the sum of the two numbers on the die will be 6\n\n1. ### statistics\n\nyour teacher has invented a fair dice game to play. your teacher will roll one fair eight sided die and you will roll a fair six sided die. each player rolls once and the winner is the person with the higher number. in case of a\n\n2. ### MATH\n\n6. Compute the probability of tossing a six-sided die and getting a 7\n\n3. ### math\n\nA six-sided die (with numbers 1 through 6) and an eight-sided die (with numbers 1 through 8) are rolled. What is the probability that there is exactly one 6 showing? Express your answer as a common fraction.\n\n4. ### Math 221 Week3\n\nA probability experiment consists of rolling a 6 sided die. Find the probability of the event below: rolling a number less than 3? The probability is\n\n1. ### math\n\nA fair, six-sided die is rolled eight times, to form an eight-digit number. What is the probability that the resulting number is a multiple of 8? Express your answer as a common fraction.\n\n2. ### MATH\n\nConsider the experiment of rolling a single die. Find the probability of the event described.What is P(number showing is not odd)?\n\n3. ### Math\n\nTwo 4-sided dice are rolled and the sum is recorded. Determine the theoretical probability of rolling a sum of 6. Hint: You may want to create a dice chart for the sum of two 4-sided die. a. 3/16 b. 6/16 c. 2/16 d. 4/16\n\n4. ### probability\n\nConsider n independent rolls of a k-sided fair die with k≥2: the sides of the die are labelled 1,2,…,k and each side has probability 1/k of facing up after a roll. Let the random variable Xi denote the number of rolls that" ]
[ null ]
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https://mathoverflow.net/questions/89963/exponent-of-metacyclic-groups
[ "# Exponent of metacyclic groups\n\nI am interested in the following related questions in metacyclic groups of the form $\\mathbb{Z}_n \\ltimes_r \\mathbb{Z}_m$, where $r^n \\equiv 1 \\pmod{m}$:\n\n1. The order of an arbitrary element $g = (\\alpha, 0)*(0, \\beta)$ - or some upper bound on the order - where * is the group operation.\n\n2. The exponent of the group\n\nI know that the first question reduces to finding the smallest integer $k$ such that:\n\n$k \\alpha \\equiv 0\\pmod{n}$, and\n\n$\\beta \\frac{r^{k \\alpha} - 1}{r^\\alpha - 1} \\equiv 0 \\pmod{m}$,\n\n• It seems like a homework. Voted to close. – Mark Sapir Mar 1 '12 at 15:41\n• It is not homework. If it looks so easy to you, could you please give me some hint? – Hebert Mar 1 '12 at 16:30\n• This question was posted two days ago at MathStackExchange, and it hasn't got any answer so far. That's why I have posted it here. It is a legitimate research question. – Hebert Mar 1 '12 at 16:57\n• See the paper C. E. Hempel, Metacyclic groups, Comm. Algebra 28 (2000), no. 8, 3865--3897. In particular, Lemma 2.1 gives the answer to your question. – Primoz Mar 1 '12 at 19:34\n• I still haven't got access to the paper, but thank you very much anyway. I'm looking forward to see it. – Hebert Mar 1 '12 at 21:23\n\nHere is an answer which is probably far from optimal (I am no expert). Let $$t:=\\mathrm{ord}_m r, \\qquad k:=\\mathrm{lcm}\\left(\\frac{n}{\\gcd(n,\\alpha)},\\frac{mt}{\\gcd(t,\\alpha)}\\right),$$ then clearly $k\\alpha\\equiv 0\\pmod{n}$, and I claim that $\\frac{r^{k\\alpha}-1}{r^\\alpha-1}\\equiv 0\\pmod{m}$. For the latter observe that $$\\alpha\\ \\Big|\\frac{t\\alpha}{\\gcd(t,\\alpha)}\\quad\\text{and}\\quad \\frac{mt\\alpha}{\\gcd(t,\\alpha)}\\ \\Big|\\ k\\alpha,$$ so that $$\\frac{r^\\frac{mt\\alpha}{\\gcd(t,\\alpha)}-1}{r^\\frac{t\\alpha}{\\gcd(t,\\alpha)}-1}\\ \\Big|\\ \\frac{r^{k\\alpha}-1}{r^\\alpha-1}.$$\nSo it suffices to show that the left hand side is divisible by $m$. The fraction equals $$\\sum_{j=0}^{m-1} r^\\frac{jt\\alpha}{\\gcd(t,\\alpha)}.$$ Here each exponent is divisible by $t$, hence each term in the sum is $\\equiv 1\\pmod{m}$. There are $m$ terms, hence the sum is divisible by $m$ as claimed.\nIt also follows that the exponent of the group divides $\\mathrm{lcm}(n,mt)$. Note that the last quantity is in between $\\mathrm{lcm}(n,m)$ and $nm$.\n• Actually in the definition of $k$ one can lower $m$ to $m/\\gcd(m,\\beta)$. – GH from MO Mar 1 '12 at 21:05\n• Well, it turns out that the exponent of the group is exactly $\\mbox{lcm}(n,m)$. – Hebert Mar 2 '12 at 21:56\n• @Hebert: Thank you. Can you provide an explanation, e.g. as a response to your own question? From Hempel's Lemma 2.1 the answer is not obvious to me, e.g. I don't know the values $k,l,m,n$ in your situation. An elementary number theoretic argument would be even better. – GH from MO Mar 3 '12 at 10:08\n• @GH: In our case, $k=n$, $m=m$, $l=m$, and $n=r$ (the left-hand sides are Hempel's variables, and the right-hand sides are mine). So, the value of $\\lcm(n,m)$ follows from Lemma 2.1 of Hempel's paper. I would still like to obtain that same value by lowering $k$ in your argument. – Hebert Mar 4 '12 at 14:52" ]
[ null ]
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https://www.colorhexa.com/60c6a4
[ "# #60c6a4 Color Information\n\nIn a RGB color space, hex #60c6a4 is composed of 37.6% red, 77.6% green and 64.3% blue. Whereas in a CMYK color space, it is composed of 51.5% cyan, 0% magenta, 17.2% yellow and 22.4% black. It has a hue angle of 160 degrees, a saturation of 47.2% and a lightness of 57.6%. #60c6a4 color hex could be obtained by blending #c0ffff with #008d49. Closest websafe color is: #66cc99.\n\n• R 38\n• G 78\n• B 64\nRGB color chart\n• C 52\n• M 0\n• Y 17\n• K 22\nCMYK color chart\n\n#60c6a4 color description : Moderate cyan - lime green.\n\n# #60c6a4 Color Conversion\n\nThe hexadecimal color #60c6a4 has RGB values of R:96, G:198, B:164 and CMYK values of C:0.52, M:0, Y:0.17, K:0.22. Its decimal value is 6342308.\n\nHex triplet RGB Decimal 60c6a4 `#60c6a4` 96, 198, 164 `rgb(96,198,164)` 37.6, 77.6, 64.3 `rgb(37.6%,77.6%,64.3%)` 52, 0, 17, 22 160°, 47.2, 57.6 `hsl(160,47.2%,57.6%)` 160°, 51.5, 77.6 66cc99 `#66cc99`\nCIE-LAB 73.255, -37.913, 8.021 31.717, 45.553, 42.241 0.265, 0.381, 45.553 73.255, 38.752, 168.055 73.255, -44.873, 17.833 67.493, -34.231, 10.138 01100000, 11000110, 10100100\n\n# Color Schemes with #60c6a4\n\n• #60c6a4\n``#60c6a4` `rgb(96,198,164)``\n• #c66082\n``#c66082` `rgb(198,96,130)``\nComplementary Color\n• #60c671\n``#60c671` `rgb(96,198,113)``\n• #60c6a4\n``#60c6a4` `rgb(96,198,164)``\n• #60b5c6\n``#60b5c6` `rgb(96,181,198)``\nAnalogous Color\n• #c67160\n``#c67160` `rgb(198,113,96)``\n• #60c6a4\n``#60c6a4` `rgb(96,198,164)``\n• #c660b5\n``#c660b5` `rgb(198,96,181)``\nSplit Complementary Color\n• #c6a460\n``#c6a460` `rgb(198,164,96)``\n• #60c6a4\n``#60c6a4` `rgb(96,198,164)``\n• #a460c6\n``#a460c6` `rgb(164,96,198)``\n• #82c660\n``#82c660` `rgb(130,198,96)``\n• #60c6a4\n``#60c6a4` `rgb(96,198,164)``\n• #a460c6\n``#a460c6` `rgb(164,96,198)``\n• #c66082\n``#c66082` `rgb(198,96,130)``\n• #39a07e\n``#39a07e` `rgb(57,160,126)``\n• #40b38d\n``#40b38d` `rgb(64,179,141)``\n• #4dbf99\n``#4dbf99` `rgb(77,191,153)``\n• #60c6a4\n``#60c6a4` `rgb(96,198,164)``\n• #73cdaf\n``#73cdaf` `rgb(115,205,175)``\n• #86d3b9\n``#86d3b9` `rgb(134,211,185)``\n• #98dac4\n``#98dac4` `rgb(152,218,196)``\nMonochromatic Color\n\n# Alternatives to #60c6a4\n\nBelow, you can see some colors close to #60c6a4. Having a set of related colors can be useful if you need an inspirational alternative to your original color choice.\n\n• #60c68b\n``#60c68b` `rgb(96,198,139)``\n• #60c693\n``#60c693` `rgb(96,198,147)``\n• #60c69c\n``#60c69c` `rgb(96,198,156)``\n• #60c6a4\n``#60c6a4` `rgb(96,198,164)``\n``#60c6ad` `rgb(96,198,173)``\n• #60c6b5\n``#60c6b5` `rgb(96,198,181)``\n• #60c6be\n``#60c6be` `rgb(96,198,190)``\nSimilar Colors\n\n# #60c6a4 Preview\n\nThis text has a font color of #60c6a4.\n\n``<span style=\"color:#60c6a4;\">Text here</span>``\n#60c6a4 background color\n\nThis paragraph has a background color of #60c6a4.\n\n``<p style=\"background-color:#60c6a4;\">Content here</p>``\n#60c6a4 border color\n\nThis element has a border color of #60c6a4.\n\n``<div style=\"border:1px solid #60c6a4;\">Content here</div>``\nCSS codes\n``.text {color:#60c6a4;}``\n``.background {background-color:#60c6a4;}``\n``.border {border:1px solid #60c6a4;}``\n\n# Shades and Tints of #60c6a4\n\nA shade is achieved by adding black to any pure hue, while a tint is created by mixing white to any pure color. In this example, #050e0b is the darkest color, while #ffffff is the lightest one.\n\n• #050e0b\n``#050e0b` `rgb(5,14,11)``\n• #0a1d17\n``#0a1d17` `rgb(10,29,23)``\n• #0f2b22\n``#0f2b22` `rgb(15,43,34)``\n• #153a2d\n``#153a2d` `rgb(21,58,45)``\n• #1a4839\n``#1a4839` `rgb(26,72,57)``\n• #1f5644\n``#1f5644` `rgb(31,86,68)``\n• #24654f\n``#24654f` `rgb(36,101,79)``\n• #29735b\n``#29735b` `rgb(41,115,91)``\n• #2f8266\n``#2f8266` `rgb(47,130,102)``\n• #349071\n``#349071` `rgb(52,144,113)``\n• #399f7d\n``#399f7d` `rgb(57,159,125)``\n``#3ead88` `rgb(62,173,136)``\n• #43bc93\n``#43bc93` `rgb(67,188,147)``\n• #52c19c\n``#52c19c` `rgb(82,193,156)``\n• #60c6a4\n``#60c6a4` `rgb(96,198,164)``\n• #6ecbac\n``#6ecbac` `rgb(110,203,172)``\n• #7dd0b5\n``#7dd0b5` `rgb(125,208,181)``\n• #8bd6bd\n``#8bd6bd` `rgb(139,214,189)``\n``#9adbc5` `rgb(154,219,197)``\n• #a8e0cd\n``#a8e0cd` `rgb(168,224,205)``\n• #b7e5d6\n``#b7e5d6` `rgb(183,229,214)``\n``#c5eade` `rgb(197,234,222)``\n• #d4efe6\n``#d4efe6` `rgb(212,239,230)``\n• #e2f5ee\n``#e2f5ee` `rgb(226,245,238)``\n• #f0faf7\n``#f0faf7` `rgb(240,250,247)``\n• #ffffff\n``#ffffff` `rgb(255,255,255)``\nTint Color Variation\n\n# Tones of #60c6a4\n\nA tone is produced by adding gray to any pure hue. In this case, #929493 is the less saturated color, while #2ef8b5 is the most saturated one.\n\n• #929493\n``#929493` `rgb(146,148,147)``\n• #8a9c96\n``#8a9c96` `rgb(138,156,150)``\n• #81a599\n``#81a599` `rgb(129,165,153)``\n``#79ad9c` `rgb(121,173,156)``\n• #71b59e\n``#71b59e` `rgb(113,181,158)``\n• #68bea1\n``#68bea1` `rgb(104,190,161)``\n• #60c6a4\n``#60c6a4` `rgb(96,198,164)``\n• #58cea7\n``#58cea7` `rgb(88,206,167)``\n• #4fd7aa\n``#4fd7aa` `rgb(79,215,170)``\n• #47dfac\n``#47dfac` `rgb(71,223,172)``\n• #3fe7af\n``#3fe7af` `rgb(63,231,175)``\n• #36f0b2\n``#36f0b2` `rgb(54,240,178)``\n• #2ef8b5\n``#2ef8b5` `rgb(46,248,181)``\nTone Color Variation\n\n# Color Blindness Simulator\n\nBelow, you can see how #60c6a4 is perceived by people affected by a color vision deficiency. This can be useful if you need to ensure your color combinations are accessible to color-blind users.\n\nMonochromacy\n• Achromatopsia 0.005% of the population\n• Atypical Achromatopsia 0.001% of the population\nDichromacy\n• Protanopia 1% of men\n• Deuteranopia 1% of men\n• Tritanopia 0.001% of the population\nTrichromacy\n• Protanomaly 1% of men, 0.01% of women\n• Deuteranomaly 6% of men, 0.4% of women\n• Tritanomaly 0.01% of the population" ]
[ null ]
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https://tools.carboncollective.co/compound-interest/42695-at-14-percent-in-22-years/
[ "# What is the compound interest on $42695 at 14% over 22 years? If you want to invest$42,695 over 22 years, and you expect it will earn 14.00% in annual interest, your investment will have grown to become $762,577.08. If you're on this page, you probably already know what compound interest is and how a sum of money can grow at a faster rate each year, as the interest is added to the original principal amount and recalculated for each period. The actual rate that$42,695 compounds at is dependent on the frequency of the compounding periods. In this article, to keep things simple, we are using an annual compounding period of 22 years, but it could be monthly, weekly, daily, or even continuously compounding.\n\nThe formula for calculating compound interest is:\n\n$$A = P(1 + \\dfrac{r}{n})^{nt}$$\n\n• A is the amount of money after the compounding periods\n• P is the principal amount\n• r is the annual interest rate\n• n is the number of compounding periods per year\n• t is the number of years\n\nWe can now input the variables for the formula to confirm that it does work as expected and calculates the correct amount of compound interest.\n\nFor this formula, we need to convert the rate, 14.00% into a decimal, which would be 0.14.\n\n$$A = 42695(1 + \\dfrac{ 0.14 }{1})^{ 22}$$\n\nAs you can see, we are ignoring the n when calculating this to the power of 22 because our example is for annual compounding, or one period per year, so 22 × 1 = 22.\n\n## How the compound interest on $42,695 grows over time The interest from previous periods is added to the principal amount, and this grows the sum a rate that always accelerating. The table below shows how the amount increases over the 22 years it is compounding: Start Balance Interest End Balance 1$42,695.00 $5,977.30$48,672.30\n2 $48,672.30$6,814.12 $55,486.42 3$55,486.42 $7,768.10$63,254.52\n4 $63,254.52$8,855.63 $72,110.15 5$72,110.15 $10,095.42$82,205.58\n6 $82,205.58$11,508.78 $93,714.36 7$93,714.36 $13,120.01$106,834.37\n8 $106,834.37$14,956.81 $121,791.18 9$121,791.18 $17,050.76$138,841.94\n10 $138,841.94$19,437.87 $158,279.81 11$158,279.81 $22,159.17$180,438.99\n12 $180,438.99$25,261.46 $205,700.45 13$205,700.45 $28,798.06$234,498.51\n14 $234,498.51$32,829.79 $267,328.30 15$267,328.30 $37,425.96$304,754.26\n16 $304,754.26$42,665.60 $347,419.86 17$347,419.86 $48,638.78$396,058.64\n18 $396,058.64$55,448.21 $451,506.85 19$451,506.85 $63,210.96$514,717.81\n20 $514,717.81$72,060.49 $586,778.30 21$586,778.30 $82,148.96$668,927.26\n22 $668,927.26$93,649.82 $762,577.08 We can also display this data on a chart to show you how the compounding increases with each compounding period. As you can see if you view the compounding chart for$42,695 at 14.00% over a long enough period of time, the rate at which it grows increases over time as the interest is added to the balance and new interest calculated from that figure.\n\n## How long would it take to double $42,695 at 14% interest? Another commonly asked question about compounding interest would be to calculate how long it would take to double your investment of$42,695 assuming an interest rate of 14.00%.\n\nWe can calculate this very approximately using the Rule of 72.\n\nThe formula for this is very simple:\n\n$$Years = \\dfrac{72}{Interest\\: Rate}$$\n\nBy dividing 72 by the interest rate given, we can calculate the rough number of years it would take to double the money. Let's add our rate to the formula and calculate this:\n\n$$Years = \\dfrac{72}{ 14 } = 5.14$$\n\nUsing this, we know that any amount we invest at 14.00% would double itself in approximately 5.14 years. So $42,695 would be worth$85,390 in ~5.14 years.\n\nWe can also calculate the exact length of time it will take to double an amount at 14.00% using a slightly more complex formula:\n\n$$Years = \\dfrac{log(2)}{log(1 + 0.14)} = 5.29\\; years$$\n\nHere, we use the decimal format of the interest rate, and use the logarithm math function to calculate the exact value.\n\nAs you can see, the exact calculation is very close to the Rule of 72 calculation, which is much easier to remember.\n\nHopefully, this article has helped you to understand the compound interest you might achieve from investing \\$42,695 at 14.00% over a 22 year investment period." ]
[ null ]
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http://1z0-061.korobko.pro/?p=571
[ "INSERT a NUMBER(p,s) value that does not fit precision or scale\n\nIt is an interesting example that deserves to be considered since it is a guaranteed case on your exam.\n\nLet’s consider a typical INSERT statement where everything is right and the value being inserted fits column precision and scale\n\nSo, Precision is the total number of digits and Scale is the number of digits after the decimal point.\n\nPrecision 4, scale 2: 99.99\n\nPrecision 10, scale 0: 9999999999\n\nPrecision 8, scale 3: 99999.999\n\nPrecision 5, scale -3: 99999000\n\nPer Oracle, Precision is the number of significant digits. Oracle guarantees the portability of numbers with precision ranging from 1 to 38.\n\nWhile Scale is the number of digits to the right (positive) or left (negative) of the decimal point. The scale can range from -84 to 127.\n\nLet’s create a table with NUMBER column where precision equals 8 and scale equal 2. And then insert a value that can be described with specified precision and scale.", null, "Let see what do we have in table t1 so far", null, "Now, let’s continue this sequence and try to insert a value with precision 9 and scale 3, but don’t change the maximum allowed number of whole digits which is 6. The maximum allowed number of whole digits is calculated = Precision – Scale. In our case Precision is 8 while Scale is 2, means we get 6 as maximum allowed number of whole digits (digits before the dot)\n\nPay attention, the value that has been entered was 123456.125. As we can see it was successfully inserted despite that wrong precision was used. Let’s verify what we have inside the table now.", null, "It may look a little unexpected because precision 9 does not correspond specified column precision which is 8, and scale 3 does not correspond specified column scale which is 2. So, why was it inserted? it happened because Oracle has inserted the value with precision 2 and not 3. So, Oracle has adjusted the value in INSERT statement with p,s=9,3 to column specified p,s=8,2. But this is not all. The value entered was rounded using standard arithmetic rules. Since initially, we were trying to insert 123456.125, we get 123456.13 inserted. So, Oracle did not reject this INSERT statement. Instead, the value was adjusted to the specified column precision and scale (8 and 2 respectively). See below", null, "You can try to insert basically any scale, it will be adjusted anyway to 2. Let’s have an example with scale equals 5. The value to be inserted is 123456.12111", null, "As you can see this value was also inserted and was rounded as well, This time it was rounded to 123456.12 because the original value was 123456.12111(see below )", null, "So, the intermediate rule we have discovered up to this moment is – You can specify in INSERT statement any scale, not necessarily the scale that your column has. If not matched, Oracle will adjust it using standard math rules for rounding.\n\nNow let’s see if we can insert any number of whole digits (before the dot) not necessarily 6. For instance, let’s try to insert a value 12345.11", null, "yes, it was inserted. See below", null, "Let’s try to insert now 1234567.11 as a value through INSERT statement", null, "It won’t allow because the maximum allowed number of whole digits is 6 and we have tried to enter 7 of those.\n\nSo, the second intermediate rule is – the maximum allowed number of whole digits (digits before the dot) is equal Precision – Scale. In our case 8-2=6." ]
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https://math.stackexchange.com/questions/1224900/a-g-%CE%B4-subset-of-2%CF%89-that-is-homeomorphic-to-%CF%89%CF%89
[ "# A $G_δ$ subset of $2^ω$ that is homeomorphic to $ω^ω$\n\nHow do I show that there is a $G_δ$ subset of the Cantor space $2^ω$ that is homeomorphic to the Baire space $ω^ω$?\n\nI've been given the hint to consider $G = \\{x ∈ 2^ω : x\\text{ is not eventually constant}\\}$, but I'm not entirely sure what to do with it. Any help is appreciated.\n\n• While not exactly a duplicate, Brian M. Scott's answer to a different question provides one method to demonstrate this. – user642796 Apr 8 '15 at 3:31\n• @ArthurFischer Thanks for the link. I've looked at the answer but I'm not familiar with all of the terms. How does showing that X (or in this case G) is separable and metrizable and not locally compact anywhere equate to a homeomorphism? – user2034 Apr 8 '15 at 3:43\n• Arthur Fischer's answer to a different question actually answers your question since the set of infinite words on $\\{0,1\\}$ with an infinite number of $1$ is the intersection of the (open) sets of all infinite words having at least $n$ occurrences of $1$. – J.-E. Pin Apr 8 '15 at 6:33\n\nAs noted in a comment to the question, a previous answer by Brian M. Scott provides one method to demonstrate that the particular subset $G$ is homeomorphic to the Baire space. In particular, he uses the following characterisation of the Baire space:\n\nThe [Baire space $\\omega^\\omega$] is (up to homeomorphism) the unique zero-dimensional, separable, Čech-complete metrizable space that is nowhere locally compact.\n\nHe then shows that $G$ has all of these properties to conclude that it is homeomorphic to the Baire space without explicitly constructing a homeomorphism.\n\nIf you don't have this \"pile-driver\" handy, you'll probably have to construct the homeomorphism by hand.\n\nFirst, to show that $G$ is Gδ, note that $G = \\bigcap_n U_n$ where $$U_n := \\{ \\mathbf{x} \\in 2^\\omega : \\mathbf{x}\\text{ switches between }0\\text{ and }1\\text{ at least }n\\text{ times}\\}.$$ (So $\\mathbf{x} \\in U_n$ iff $\\mathbf{x}$ has an initial segment of the form $0^{k_0} 1^{k_1} \\cdots b^{k_n}$ or $1^{k_0} 0^{k_1} \\cdots b^{k_n}$ where each $k_i > 0$, and $b$ is the appropriate bit.)\n\nTo construct the homeomorphism, note that given any $\\mathbf{x} \\in G$, we may write it as an infinite concatenation as $$\\mathbf{x} = 0^{k_0} 1^{k_1} 0^{k_2} 1^{k_3} \\cdots$$ where $k_0 \\geq 0$, and $k_i > 0$ for all $i > 0$. Using this we define a function $\\varphi : G \\to \\omega^\\omega$ as follows: $$\\varphi ( \\mathbf{x} ) = ( k_0 , k_1 - 1 , k_2 - 1 , k_3 - 1 , \\ldots ).$$ It is not too difficult to show that this function is a homeomorphism from $G$ onto the Baire space.\n\nAs a final note, it is somewhat superfluous to show that $G$ is Gδ since it is a theorem that any completely metrizable subspace of a completely metrizable space must be a Gδ subset of that space. That is, the existence of the homeomorphism between $G$ and the Baire space shows that $G$ is a Gδ subset of the Cantor space. (Also any subspace of the Cantor space which is homeomorphic to the Baire space is a Gδ subset of the Cantor space; e.g, the subspace provided in Arthur Fischer's answer to the same question.)\n\n• Thanks, that was excellent. It cleared up my confusion with Brian's answer as well as answering the question. – user2034 Apr 8 '15 at 12:24\n\nThe required claim easily follows from general facts about metrizable spaces. The Baire space $$\\omega^\\omega$$ is zero-dimensional second countable completely metrizable. Since $$\\omega^\\omega$$ is zero-dimensional second countable, it can be embedded into Cantor Cube $$\\{0,1\\}^\\omega$$ (see, for instance, [Eng, 6.2.16]). Since $$\\omega^\\omega$$ is completely metrizable, it is a $$G_\\delta$$ sibset of $$\\omega$$ for any its embedding (see, for instanse, [Eng, 4.3.24]).\n\nReferences\n\n[Eng] Ryszard Engelking, General Topology, 2nd ed., Heldermann, Berlin, 1989.", null, "", null, "", null, "" ]
[ null, "https://i.stack.imgur.com/5xlud.png", null, "https://i.stack.imgur.com/mXRQa.png", null, "https://i.stack.imgur.com/uOLIm.png", null ]
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http://docs.php.net/manual/ja/fann.constants.php
[ "# 定義済み定数\n\nTraining algorithms\n`FANN_TRAIN_INCREMENTAL` (int)\nStandard backpropagation algorithm, where the weights are updated after each training pattern. This means that the weights are updated many times during a single epoch. For this reason some problems, will train very fast with this algorithm, while other more advanced problems will not train very well.\n`FANN_TRAIN_BATCH` (int)\nStandard backpropagation algorithm, where the weights are updated after calculating the mean square error for the whole training set. This means that the weights are only updated once during a epoch. For this reason some problems, will train slower with this algorithm. But since the mean square error is calculated more correctly than in incremental training, some problems will reach a better solutions with this algorithm.\n`FANN_TRAIN_RPROP` (int)\nA more advanced batch training algorithm which achieves good results for many problems. The RPROP training algorithm is adaptive, and does therefore not use the learning_rate. Some other parameters can however be set to change the way the RPROP algorithm works, but it is only recommended for users with insight in how the RPROP training algorithm works. The RPROP training algorithm is described by [Riedmiller and Braun, 1993], but the actual learning algorithm used here is the iRPROP- training algorithm which is described by [Igel and Husken, 2000] which is an variety of the standard RPROP training algorithm.\n`FANN_TRAIN_QUICKPROP` (int)\nA more advanced batch training algorithm which achieves good results for many problems. The quickprop training algorithm uses the learning_rate parameter along with other more advanced parameters, but it is only recommended to change these advanced parameters, for users with insight in how the quickprop training algorithm works. The quickprop training algorithm is described by [Fahlman, 1988].\n`FANN_TRAIN_SARPROP` (int)\nEven more advance training algorithm. Only for version 2.2\nActivation functions\n`FANN_LINEAR` (int)\nLinear activation function.\n`FANN_THRESHOLD` (int)\nThreshold activation function.\n`FANN_THRESHOLD_SYMMETRIC` (int)\nThreshold activation function.\n`FANN_SIGMOID` (int)\nSigmoid activation function.\n`FANN_SIGMOID_STEPWISE` (int)\nStepwise linear approximation to sigmoid.\n`FANN_SIGMOID_SYMMETRIC` (int)\nSymmetric sigmoid activation function, aka. tanh.\n`FANN_SIGMOID_SYMMETRIC_STEPWISE` (int)\nStepwise linear approximation to symmetric sigmoid\n`FANN_GAUSSIAN` (int)\nGaussian activation function.\n`FANN_GAUSSIAN_SYMMETRIC` (int)\nSymmetric gaussian activation function.\n`FANN_GAUSSIAN_STEPWISE` (int)\nStepwise gaussian activation function.\n`FANN_ELLIOT` (int)\nFast (sigmoid like) activation function defined by David Elliott.\n`FANN_ELLIOT_SYMMETRIC` (int)\nFast (symmetric sigmoid like) activation function defined by David Elliott.\n`FANN_LINEAR_PIECE` (int)\nBounded linear activation function.\n`FANN_LINEAR_PIECE_SYMMETRIC` (int)\nBounded linear activation function.\n`FANN_SIN_SYMMETRIC` (int)\nPeriodical sinus activation function.\n`FANN_COS_SYMMETRIC` (int)\nPeriodical cosinus activation function.\n`FANN_SIN` (int)\nPeriodical sinus activation function.\n`FANN_COS` (int)\nPeriodical cosinus activation function.\nError function used during training\n`FANN_ERRORFUNC_LINEAR` (int)\nStandard linear error function.\n`FANN_ERRORFUNC_TANH` (int)\nTanh error function; usually better but may require a lower learning rate. This error function aggressively targets outputs that differ much from the desired, while not targeting outputs that only differ slightly. Not recommended for cascade or incremental training.\nStop criteria used during training\n`FANN_STOPFUNC_MSE` (int)\nStop criteria is Mean Square Error (MSE) value.\n`FANN_STOPFUNC_BIT` (int)\nStop criteria is number of bits that fail. The number of bits means the number of output neurons which differs more than the bit fail limit (see fann_get_bit_fail_limit, fann_set_bit_fail_limit). The bits are counted in all of the training data, so this number can be higher than the number of training data.\nDefinition of network types used by fann_get_network_type()\n`FANN_NETTYPE_LAYER` (int)\nEach layer only has connections to the next layer.\n`FANN_NETTYPE_SHORTCUT` (int)\nEach layer has connections to all following layers\nErrors\n`FANN_E_NO_ERROR` (int)\nNo error.\n`FANN_E_CANT_OPEN_CONFIG_R` (int)\nUnable to open configuration file for reading.\n`FANN_E_CANT_OPEN_CONFIG_W` (int)\nUnable to open configuration file for writing.\n`FANN_E_WRONG_CONFIG_VERSION` (int)\nWrong version of configuration file.\n`FANN_E_CANT_READ_CONFIG` (int)\nError reading info from configuration file.\n`FANN_E_CANT_READ_NEURON` (int)\nError reading neuron info from configuration file.\n`FANN_E_CANT_READ_CONNECTIONS` (int)\nError reading connections from configuration file.\n`FANN_E_WRONG_NUM_CONNECTIONS` (int)\nNumber of connections not equal to the number expected.\n`FANN_E_CANT_OPEN_TD_W` (int)\nUnable to open train data file for writing.\n`FANN_E_CANT_OPEN_TD_R` (int)\nUnable to open train data file for reading.\n`FANN_E_CANT_READ_TD` (int)\nError reading training data from file.\n`FANN_E_CANT_ALLOCATE_MEM` (int)\nUnable to allocate memory.\n`FANN_E_CANT_TRAIN_ACTIVATION` (int)\nUnable to train with the selected activation function.\n`FANN_E_CANT_USE_ACTIVATION` (int)\nUnable to use the selected activation function.\n`FANN_E_TRAIN_DATA_MISMATCH` (int)\nIrreconcilable differences between two struct fann_train_data structures.\n`FANN_E_CANT_USE_TRAIN_ALG` (int)\nUnable to use the selected training algorithm.\n`FANN_E_TRAIN_DATA_SUBSET` (int)\nTrying to take subset which is not within the training set.\n`FANN_E_INDEX_OUT_OF_BOUND` (int)\nIndex is out of bound.\n`FANN_E_SCALE_NOT_PRESENT` (int)\nScaling parameters not present.\n`FANN_E_INPUT_NO_MATCH` (int)\nThe number of input neurons in the ann and data do not match\n`FANN_E_OUTPUT_NO_MATCH` (int)\nThe number of output neurons in the ann and data do not match.", null, "" ]
[ null, "http://docs.php.net/images/[email protected]", null ]
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https://ask.sagemath.org/question/40976/matrix-group-over-symbolic-ring/?sort=latest
[ "Ask Your Question\n\n# Matrix Group over Symbolic Ring\n\nI have problem on generate matrix group over symbolic ring.\n\nFirst, I define\n\neta=I;\neta2=(1+I)*sqrt(2)/2;\n\n\nThen, define a generator matrix\n\nT=matrix(SR,4,[eta**(i*j)*eta2/2 for i in range(4) for j in range(4)]);\n\n\nI try to make a matrix group by\n\nG=MatrixGroup(T);\n\n\nWhat I get is only very long computation that does not give any result. Can somebody help me? Thank you very much.\n\nI have checked the order of T, I got 8 since T**8=I where I is identity matrix.\n\nedit retag close merge delete\n\n## Comments\n\nI've tried instead:\n\nsage: K.<a> = QuadraticField( -1 )\nsage: R.<X> = K[]\nsage: L.<b> =K.extension( X^2 - 2 )\nsage: eta = a\nsage: eta2 = (1+a)*b/2\nsage: T = matrix(L, 4, [eta**(k*kk)*eta2/2 for k in range(4) for kk in range(4)])\nsage: T^8\n[1 0 0 0]\n[0 1 0 0]\n[0 0 1 0]\n[0 0 0 1]\nsage: G = MatrixGroup(T)\n\n\nrunning into NotImplementedError: Currently, only simple algebraic extensions are implemented in gap. Well... Perhaps gap cannot digest the input in both cases.\n\nWhich is the \"real need\"? Depending on it, the \"other way to get the result\" may be simpler or more complicated. In the above case one can use block matrices representing $\\sqrt{-1}$ and $\\sqrt 2$ as commuting $2\\times 2$ matrices. If such cases are enough, i will write the code.\n\nDo you mean \"real need\" is what I need on that code? Sorry if I am wrong understanding your comment.\n\n## 2 Answers\n\nSort by » oldest newest most voted\n\nCase closed, I finally use CyclotomicField(8) and it works.\n\nmore\n\n## Comments\n\n2\n\n@dimahphone -- You can accept your answer by clicking on the accept (tick mark) button, so that this will appear as the accepted answer, and the question will appear as solved in the list of questions.\n\nWhenever possible, avoid working with Sage's symbolic ring.\n\nHere, you can use the symbolic ring as an intermediate step but move to QQbar.\n\nThis will make your code work. So you could start as you did:\n\nsage: eta = I\nsage: eta2 = (1+I)*sqrt(2)/2\n\n\nthen instead of defining\n\nsage: T = matrix(SR, 4, [eta**(i*j)*eta2/2 for i in range(4) for j in range(4)])\n\n\nyou could define\n\nsage: T = matrix(QQbar, 4, [eta**(i*j)*eta2/2 for i in range(4) for j in range(4)])\n\n\nAnd then things work.\n\nsage: G = MatrixGroup(T)\nsage: G\nMatrix group over Algebraic Field with 1 generators (\n[ 0.3535533905932738? + 0.3535533905932738?*I 0.3535533905932738? + 0.3535533905932738?*I 0.3535533905932738? + 0.3535533905932738?*I 0.3535533905932738? + 0.3535533905932738?*I]\n[ 0.3535533905932738? + 0.3535533905932738?*I -0.3535533905932738? + 0.3535533905932738?*I -0.3535533905932738? - 0.3535533905932738?*I 0.3535533905932738? - 0.3535533905932738?*I]\n[ 0.3535533905932738? + 0.3535533905932738?*I -0.3535533905932738? - 0.3535533905932738?*I 0.3535533905932738? + 0.3535533905932738?*I -0.3535533905932738? - 0.3535533905932738?*I]\n[ 0.3535533905932738? + 0.3535533905932738?*I 0.3535533905932738? - 0.3535533905932738?*I -0.3535533905932738? - 0.3535533905932738?*I -0.3535533905932738? + 0.3535533905932738?*I]\n)\n\n\nCalculations in QQbar are exact and efficient.\n\nIf you need to see the radical expression of an element in QQbar (if it has one), use .radical_expression().\n\nFor example:\n\nsage: T[0,0].radical_expression()\n1/2*(-1)^(1/4)\n\nmore\n\n## Comments\n\nThank you for the suggestion. It works. But, I still have problem when I use QQbar. I can not do anything for groups I get. For example, I can not know the element order of the group. By hand, I get that the order is 8. Do you have any suggestion? Thank you very much. Sorry if it disturbs your time.\n\n## Your Answer\n\nPlease start posting anonymously - your entry will be published after you log in or create a new account.\n\nAdd Answer\n\n## Stats\n\nAsked: 2018-02-05 05:31:14 +0200\n\nSeen: 274 times\n\nLast updated: May 30 '18" ]
[ null ]
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https://stats.stackexchange.com/questions/59085/how-to-test-for-simultaneous-equality-of-choosen-coefficients-in-logit-or-probit/59093
[ "# How to test for simultaneous equality of choosen coefficients in logit or probit model?\n\nHow to test for simultaneous equality of choosen coefficients in logit or probit model ? What is the standard approach and what is the state of art approach ?\n\n## Wald test\n\nOne standard approach is the Wald test. This is what the Stata command test does after a logit or probit regression. Let's see how this works in R by looking at an example:\n\nmydata <- read.csv(\"http://www.ats.ucla.edu/stat/data/binary.csv\") # Load dataset from the web\nmydata$rank <- factor(mydata$rank)\nmylogit <- glm(admit ~ gre + gpa + rank, data = mydata, family = \"binomial\") # calculate the logistic regression\n\nsummary(mylogit)\n\nCoefficients:\nEstimate Std. Error z value Pr(>|z|)\n(Intercept) -3.989979 1.139951 -3.500 0.000465 ***\ngre 0.002264 0.001094 2.070 0.038465 *\ngpa 0.804038 0.331819 2.423 0.015388 *\nrank2 -0.675443 0.316490 -2.134 0.032829 *\nrank3 -1.340204 0.345306 -3.881 0.000104 ***\nrank4 -1.551464 0.417832 -3.713 0.000205 ***\n---\nSignif. codes: 0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1\n\n\nSay, you want to test the hypothesis $\\beta_{gre}=\\beta_{gpa}$ vs. $\\beta_{gre}\\neq \\beta_{gpa}$. This is equivalent of testing $\\beta_{gre} - \\beta_{gpa} = 0$. The Wald test statistic is:\n\n$$W=\\frac{(\\hat{\\beta}-\\beta_{0})}{\\widehat{\\operatorname{se}}(\\hat{\\beta})}\\sim \\mathcal{N}(0,1)$$\n\nor\n\n$$W^2 = \\frac{(\\hat{\\theta}-\\theta_{0})^2}{\\operatorname{Var}(\\hat{\\theta})}\\sim \\chi_{1}^2$$\n\nOur $\\widehat{\\theta}$ here is $\\beta_{gre} - \\beta_{gpa}$ and $\\theta_{0}=0$. So all we need is the standard error of $\\beta_{gre} - \\beta_{gpa}$. We can calculate the standard error with the Delta method:\n\n$$\\hat{se}(\\beta_{gre} - \\beta_{gpa})\\approx \\sqrt{\\operatorname{Var}(\\beta_{gre}) + \\operatorname{Var}(\\beta_{gpa}) - 2\\cdot \\operatorname{Cov}(\\beta_{gre},\\beta_{gpa})}$$\n\nSo we also need the covariance of $\\beta_{gre}$ and $\\beta_{gpa}$. The variance-covariance matrix can be extracted with the vcov command after running the logistic regression:\n\nvar.mat <- vcov(mylogit)[c(\"gre\", \"gpa\"),c(\"gre\", \"gpa\")]\n\ncolnames(var.mat) <- rownames(var.mat) <- c(\"gre\", \"gpa\")\n\ngre gpa\ngre 1.196831e-06 -0.0001241775\ngpa -1.241775e-04 0.1101040465\n\n\nFinally, we can calculate the standard error:\n\nse <- sqrt(1.196831e-06 + 0.1101040465 -2*-0.0001241775)\nse\n 0.3321951\n\n\nSo your Wald $z$-value is\n\nwald.z <- (gre-gpa)/se\nwald.z\n -2.413564\n\n\nTo get a $p$-value, just use the standard normal distribution:\n\n2*pnorm(-2.413564)\n 0.01579735\n\n\nIn this case we have evidence that the coefficients are different from each other. This approach can be extended to more than two coefficients.\n\nUsing multcomp\n\nThis rather tedious calculations can be conveniently done in R using the multcomp package. Here is the same example as above but done with multcomp:\n\nlibrary(multcomp)\n\nglht.mod <- glht(mylogit, linfct = c(\"gre - gpa = 0\"))\n\nsummary(glht.mod)\n\nLinear Hypotheses:\nEstimate Std. Error z value Pr(>|z|)\ngre - gpa == 0 -0.8018 0.3322 -2.414 0.0158 *\n\nconfint(glht.mod)\n\n\nA confidence interval for the difference of the coefficients can also be calculated:\n\nQuantile = 1.96\n95% family-wise confidence level\n\nLinear Hypotheses:\nEstimate lwr upr\ngre - gpa == 0 -0.8018 -1.4529 -0.1507\n\n\nFor additional examples of multcomp, see here or here.\n\n## Likelihood ratio test (LRT)\n\nThe coefficients of a logistic regression are found by maximum likelihood. But because the likelihood function involves a lot of products, the log-likelihood is maximized which turns the products into sums. The model that fits better has a higher log-likelihood. The model involving more variables has at least the same likelihood as the null model. Denote the log-likelihood of the alternative model (model containing more variables) with $LL_{a}$ and the log-likelihood of the null model with $LL_{0}$, the likelihood ratio test statistic is:\n\n$$D=2\\cdot (LL_{a} - LL_{0})\\sim \\chi_{df1-df2}^{2}$$\n\nThe likelihood ratio test statistic follows a $\\chi^{2}$-distribution with the degrees of freedom being the difference in number of variables. In our case, this is 2.\n\nTo perform the likelihood ratio test, we also need to fit the model with the constraint $\\beta_{gre}=\\beta_{gpa}$ to be able to compare the two likelihoods. The full model has the form $$\\log\\left(\\frac{p_{i}}{1-p_{i}}\\right)=\\beta_{0}+\\beta_{1}\\cdot \\mathrm{gre} + \\beta_{2}\\cdot \\mathrm{gpa}+\\beta_{3}\\cdot \\mathrm{rank_{2}} + \\beta_{4}\\cdot \\mathrm{rank_{3}}+\\beta_{5}\\cdot \\mathrm{rank_{4}}$$. Our constraint model has the form: $$\\log\\left(\\frac{p_{i}}{1-p_{i}}\\right)=\\beta_{0}+\\beta_{1}\\cdot (\\mathrm{gre} + \\mathrm{gpa})+\\beta_{2}\\cdot \\mathrm{rank_{2}} + \\beta_{3}\\cdot \\mathrm{rank_{3}}+\\beta_{4}\\cdot \\mathrm{rank_{4}}$$.\n\nmylogit2 <- glm(admit ~ I(gre + gpa) + rank, data = mydata, family = \"binomial\")\n\n\nIn our case, we can use logLik to extract the log-likelihood of the two models after a logistic regression:\n\nL1 <- logLik(mylogit)\nL1\n'log Lik.' -229.2587 (df=6)\n\nL2 <- logLik(mylogit2)\nL2\n'log Lik.' -232.2416 (df=5)\n\n\nThe model containing the constraint on gre and gpa has a slightly higher log-likelihood (-232.24) compared to the full model (-229.26). Our likelihood ratio test statistic is:\n\nD <- 2*(L1 - L2)\nD\n 16.44923\n\n\nWe can now use the CDF of the $\\chi^{2}_{2}$ to calculate the $p$-value:\n\n1-pchisq(D, df=1)\n 0.01458625\n\n\nThe $p$-value is very small indicating that the coefficients are different.\n\nR has the likelihood ratio test built in; we can use the anova function to calculate the likelhood ratio test:\n\nanova(mylogit2, mylogit, test=\"LRT\")\n\nAnalysis of Deviance Table\n\nModel 1: admit ~ I(gre + gpa) + rank\nModel 2: admit ~ gre + gpa + rank\nResid. Df Resid. Dev Df Deviance Pr(>Chi)\n1 395 464.48\n2 394 458.52 1 5.9658 0.01459 *\n---\nSignif. codes: 0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1\n\n\nAgain, we have strong evidence that the coefficients of gre and gpa are significantly different from each other.\n\n## Score test (aka Rao's Score test aka Lagrange multiplier test)\n\nThe Score function $U(\\theta)$ is the derivative of the log-likelihood function ($\\text{log} L(\\theta|x)$) where $\\theta$ are the parameters and $x$ the data (the univariate case is shown here for illustration purposes):\n\n$$U(\\theta) = \\frac{\\partial \\text{log} L(\\theta|x)}{\\partial \\theta}$$\n\nThis is basically the slope of the log-likelihood function. Further, let $I(\\theta)$ be the Fisher information matrix which is the negative expectation of the second derivative of the log-likelihood function with respect to $\\theta$. The score test statistics is:\n\n$$S(\\theta_{0})=\\frac{U(\\theta_{0}^{2})}{I(\\theta_{0})}\\sim\\chi^{2}_{1}$$\n\nThe score test can also be calculated using anova (the score test statistics is called \"Rao\"):\n\nanova(mylogit2, mylogit, test=\"Rao\")\n\nAnalysis of Deviance Table\n\nModel 1: admit ~ I(gre + gpa) + rank\nModel 2: admit ~ gre + gpa + rank\nResid. Df Resid. Dev Df Deviance Rao Pr(>Chi)\n1 395 464.48\n2 394 458.52 1 5.9658 5.9144 0.01502 *\n---\nSignif. codes: 0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1\n\n\nThe conclusion is the same as before.\n\nNote\n\nAn interesting relationship between the different test statistics when the model is linear is (Johnston and DiNardo (1997): Econometric Methods): Wald $\\geq$ LR $\\geq$ Score.\n\n• I wonder why the reduced model simply excludes gre and gpa? Isn't that testing $\\beta_1=\\beta_2=0$, not $\\beta_1=\\beta_2$? To me, to correctly test $\\beta_1=\\beta_2$, we need to keep gre and gpa and meanwhile impose $\\beta_{\\text{gre}}=\\beta_{\\text{gpa}}$. May 11 '15 at 9:07\n• @SibbsGambling Good catch! I updated my answer accordingly. May 11 '15 at 16:06\n• Is this limited to continuous predictors only, or could I - for instance - also see whether two levels of a categorical variable are significantly different? Let's say, is the difference between rank3 and rank4 significant? Jun 4 '15 at 17:16\n• @Daniel Yes, this approach can also be used for levels of a categorical variable. The multcomp packages makes it particularly easy. For example, try this: glht.mod <- glht(mylogit, linfct = c(\"rank3 - rank4= 0\")). But a much easier way would be to make rank3 the reference level (using mydata$rank <- relevel(mydata$rank, ref=\"3\")) and then just use the normal regression output. Each level of the factor is compared to the reference level. The p-value for rank4 would be the desired comparison. Jun 4 '15 at 20:31\n• @Daniel The p-values from the model output (changed reference level) and glht are the same for me (about $0.591$). Regarding your second question: linfct = c(\"rank3 - rank4= 0\") tests only one linear hypothesis whereas mcp(rank=\"Tukey\") tests all 6 pairwise comparisons of rank. So the p-values have to be adjusted for multiple comparisons. This means that the p-values using Tukey's test are generally higher than the single comparison. Jun 5 '15 at 6:31\n\nYou did not specify your variables, if they are binary or something else. I think you talk about binary variables. There also exist multinomial versions of the probit and logit model.\n\nIn general, you can use the complete trinity of test approaches, i.e.\n\nLikelihood-Ratio-test\n\nLM-Test\n\nWald-Test\n\nEach test uses different test-statistics. The standard approach would be to take one of the three tests. All three can be used to do joint tests.\n\nThe LR test uses the differnce of the log-likelihood of a restricted and the unrestricted model. So the restricted model is the model, in which the specified coefficients are set to zero. The unrestricted is the \"normal\" model. The Wald test has the advantage, that only the unrestriced model is estimated. It basically asks, if the restriction is nearly satisfied if it is evaluated at the unrestriced MLE. In case of the Lagrange-Multiplier test only the restricted model has to be estimated. The restricted ML estimator is used to calculate the score of the unrestricted model. This score will be usually not zero, so this discrepancy is the basis of the LR test. The LM-Test can in your context also be used to test for heteroscedasticity.\n\nThe standard approaches are the Wald test, the likelihood ratio test and the score test. Asymptotically they should be the same. In my experience the likelihood ratio tests tends to perform slightly better in simulations on finite samples, but the cases where this matters would be in very extreme (small sample) scenarios where I would take all of these tests as a rough approximation only. However, depending on your model (number of covariates, presence of interaction effects) and your data (multicolinearity, the marginal distribution of your dependent variable), the \"wonderful kingdom of Asymptotia\" can be well approximated by a surprisingly small number of observations.\n\nBelow is an example of such a simulation in Stata using the Wald, likelihood ratio and score test in a sample of only 150 observations. Even in such a small sample the three test produce fairly similar p-values and the sampling distribution of the p-values when the null hypothesis is true does seem to follow a uniform distribution as it should (or at least the deviations from the uniform distribution are no larger than one would expect due to the randomness inherrit in a Monte Carlo experiment).\n\nclear all\nset more off\n\n// data preparation\nsysuse nlsw88, clear\n\ngen byte edcat = cond(grade < 12, 1, ///\ncond(grade == 12, 2, 3)) ///\nlabel define edcat 1 \"less than high school\" ///\n2 \"high school\" ///\n3 \"more than high school\"\nlabel value edcat edcat\nlabel variable edcat \"education in categories\"\n\n// edcat2 compares high school with less than high school\n// edcat3 compares more than high school with high school\ngen byte edcat2 = (edcat >= 2) if edcat < .\ngen byte edcat3 = (edcat >= 3) if edcat < .\n\nkeep union edcat2 edcat3 race south\nbsample 150 if !missing(union, edcat2, edcat3, race, south)\n\n// constraining edcat2 = edcat3 is equivalent to adding\n// a linear effect (in the log odds) of edcat\nconstraint define 1 edcat2 = edcat3\n\n// estimate the constrained model\nlogit union edcat2 edcat3 i.race i.south, constraint(1)\n\n// predict the probabilities\npredict pr\ngen byte ysim = .\ngen w = .\n\nprogram define sim, rclass\n// create a dependent variable such that the null hypothesis is true\nreplace ysim = runiform() < pr\n\n// estimate the constrained model\nlogit ysim edcat2 edcat3 i.race i.south, constraint(1)\nest store constr\n\n// score test\ntempname b0\nmatrix b0' = e(b)\nlogit ysim edcat2 edcat3 i.race i.south, from(b0') iter(0)\nreturn scalar p_score = chi2tail(1,chi[1,1])\n\n// estimate unconstrained model\nlogit ysim edcat2 edcat3 i.race i.south\nest store full\n\n// Wald test\ntest edcat2 = edcat3\nreturn scalar p_Wald = r(p)\n\n// likelihood ratio test\nlrtest full constr\nreturn scalar p_lr = r(p)\nend\n\nsimulate p_score=r(p_score) p_Wald=r(p_Wald) p_lr=r(p_lr), reps(2000) : sim\nsimpplot p*, overall reps(20000) scheme(s2color) ylab(,angle(horizontal))", null, "• score test is a different name for what @jen-bohold called a Lagrange multiplier (LM) test. May 15 '13 at 9:44\n• Nice answer (+1). I especially like the effort of the simulation. I didn't know how to calculate the score test in Stata. Thanks. May 20 '13 at 14:55" ]
[ null, "https://i.stack.imgur.com/8DMVC.png", null ]
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https://www.geogebra.org/m/bbn3auhw
[ "# Experimentation - bisoptic of parabolas\n\n## Multi-experimentation\n\nYou can change: 1. The parameter p of the parabola 2. The parameter a = tan (theta), where theta is the isoptic angle (i.e. the angle under which the parabola is viewed, i.e. the angle between the tangents to the parabola through the given point). The isoptics of a parabola are branches of a hyperbola." ]
[ null ]
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http://vipgames.online/engineering-mechanics-statics-12th-edition-hibbeler-solutions-63/
[ "### ENGINEERING MECHANICS STATICS 12TH EDITION HIBBELER SOLUTIONS PDF\n\nBaixe grátis o arquivo Solution Manual – Engineering Mechanics Statics 12th Edition By enviado por Thaís no curso de Engenharia de. Engineering Mechanics Statics 12e by RC Hibbeler with Solution Manual. Chapter 4 engineering mechanics statics r c hibbeler 12th edition solution pdf file.", null, "Author: Doujinn JoJobar Country: Spain Language: English (Spanish) Genre: Politics Published (Last): 28 May 2012 Pages: 255 PDF File Size: 20.8 Mb ePub File Size: 9.81 Mb ISBN: 568-6-57123-242-1 Downloads: 57969 Price: Free* [*Free Regsitration Required] Uploader: Dojin", null, "Impulse applied to an object produces an equivalent vector change in its linear momentumalso in the same direction.\n\n## Impulse (physics)\n\nIf and ,determine the magnitude 12t the resultant force acting on the eyebolt and its direction measured clockwise from the positive xaxis. The application of Newton’s second law for variable mass allows impulse and momentum to be used as analysis tools for jet – or rocket -propelled vehicles. This is often called the impulse-momentum theorem. Views Read Edit View history. Determine the design angle for strut ABso that the lb horizontal force has a component of lb directed from Atowards C.\n\nSecond law of motion. The impulse may be expressed in a simpler form when the mass is constant:.\n\n### Impulse (physics) – Wikipedia\n\nEngineering Mechanics 12th ed. Impulse J produced from time t 1 to t 2 is defined to be . From Newton’s second lawforce is related to momentum p by. Determine the design angle between struts ABand ACso that the lb horizontal force has a component of lb which acts up to the left,in the same direction as from Btowards A. Ifand the resultant force acts along the positive uaxis,determine the magnitude of the resultant force and the angle.\n\nELSY MICRODRIVE 8-16 PDF\n\nClassical mechanics SI units. Newton’s laws of motion. In the case of rockets, the impulse imparted can be normalized by unit of propellant expended, to create a performance parameter, specific impulse. Formulations Newton’s laws of motion Analytical mechanics Lagrangian mechanics Hamiltonian mechanics Routhian mechanics Hamilton—Jacobi equation Appell’s equation of motion Udwadia—Kalaba equation Koopman—von Neumann mechanics. Vector Mechanics for Engineers; Statics and Dynamics.\n\nAlso,what is the magnitude of the resultant force? This page was last edited on 31 Decemberat If the tension in the cable is N,determine the magnitude and direction of the resultant force acting on.", null, "Retrieved from ” https: The plate is subjected to the two forces at Aand B as shown. Langular impulse: Determine the angle of for connecting member A to the plate so that the resultant force of FAand FBis directed horizontally to editoon right.\n\nBy using this site, you agree to the Terms of Use and Privacy Policy. This sort of change is a step changeand is not physically possible. What is the component of force acting along member AB? A resultant force deition acceleration and a change in the velocity of the body for as long as it acts.\n\nIf ,determine the magnitude of the resultant of these two forces and its direction engineerong clockwise from the horizontal.\n\nThe term “impulse” is also used to refer to a fast-acting force or impact.\n\n## CHEAT SHEET\n\nThis type of impulse is often idealized so that the change in momentum produced by the force happens staticw no change in time. No portion of this material may be reproduced,in any form or by any means,without permission in writing from the publisher.", null, "" ]
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http://alexfrolov.narod.ru/s-wire.htm
[ " single wire power transmission Published in New Energy News, December 1994, p.13-15\n\nThe Single-Wire Electric Power Transmission\nBy Alexander V. Frolov\n\nAny motion of charges is electric current by definition. The electric potential field can also move the electric charges and this work of the potential field is not connected with loss of power. So, it is enough to use the electrical field (scalar potential source) to create the power and work in an electric load circuit.\n\nThe classic conception does not explain this paradox but states: 'The total work of the potential field along a closed trajectory is equal to zero.\" That is correct, sure. But there are simple descriptions of\nexperiments for application of potential field energy to create power in a load . The present paper\ndevelops this concept from another view.\n\nSo, the motion of charged particles is the current. But there are both the wattful current and wattless\ncurrent. To create the free energy system it is necessary to transform the wattless current to wattful\ncurrent.\n\nWhat is the difference in those two versions of current? When the charged particles are moving along wire thanks to electromotive force of potential difference, it is not the reason for loss of power in the source because the electric field of the primary source provides the work to move charged particles without any power loss. A closed electrical circuit is the reason to consume the potential difference of the source. It is possible to separate the load current from source circuit. Dr. T.E. Bearden made detailed description of a concept for this technology by means of note for \"the\nmassless current\" . Massless current is the wattless current, from my point of view.\n\nIt is possible to consider such current as oscillations of a field of free electrical charges (3]. In this case the wattless current is described as displacement current or as longitudinal wave of the electrical field.\n\nLet's consider a simple experiment to prove the possibility of power transmission by means of\ndisplacement current. The equipment that I used:\n1) Generator, output voltage is 30 Volts, frequency is 10 KHz or more.\n2) Electromagnetic transformer to increase the output voltage from 30 Volts to several kiloVolts (2-5 kV in my scheme).\n3) Diodes are connected as shown on Figure 1. This diodes connection is so-called \"Avramenko's plug\" .", null, "Fig. 1\nThere is a high voltage version of this experiment and a high frequency version. For the first version, the load on \"Avramenko's plug\" is an electrical condenser of 10 nanoFarad capacity for maximum voltage 3 kV, for example. The frequency is from 5 to 10 KHz. Both  legs of condenser are bent to make a spark discharger.\n\nI used a spark distance from 0.5 to 1 mm. The frequency of spark discharges in my experiment varied from 1 Hz to 10 Hz. It is possible to calculate the work  for one discharge by means of next formula:\n\nA = 0.5 CV2\n\nFor power we can use the formula:\n\nP=A/T=Af\n\nwhere f is frequency of spark discharges.\n\nSo, for this simple \"home laboratory\" experiment when the voltage V = 2 KV, capacity C =10 nanoFarad, and f = 5 Hz, the P is equal to 0.1 watt. The consumed power is equal to 3 watts DC (0.1 A and 30 V). Therefore, power in a closed circuit of load is about 3% of consumed power in this experiment. But this small power is free since it is not connected with conduction current in source circuit. There is only wattless displacement current in single-wire part of the system.\n\nFor high frequency version it s possible to use the voltage near 30 V and the frequency of generator more than 100 KHz. Simple electric lamp can be used as load of the \"Avramenko's plug\" in this version. By Avramenko, the conduction current is load is 60 mA when voltage V =50 Volts and frequency of generator is 100 KHz . So, load power in Avramenko's experiments is equal to 3 Watts.\n\nFrom my experiments, it is possible to make some  conclusions:\n1. When the output signal is a sine wave there is no difference for wires of secondary coil of transformer and any wire can be connected to diodes. In any case, the power in load is the same. But when the output signal is unipolar pulses (from output of transistor scheme, for example) there is important difference for wires of coil. When the diodes are connected to positive pulsed pole of coil the power in load is maximum. The same difference is easy to verify if one is to bring metal material to end of wires of high voltage coil of transformer. The discharge between metal and positive pulsed wire is more  powerful than discharge between metal and other wire of the coil.\n\nThis note can be explained in conception of longitudinal waves as waves of electron gas in matter.\nWhen the positive potential take place on the wire the electrons of metal are attracted to positive potential.  The spark discharge between metal and wire takes place here since electrons of metal can \"jump\" from metal into positive charged end of coil wire. In opposite case, electrons of metal are in repulsion from negative charged end of the coil wire. There is no condition for electrons to \"jump\" in this case. So, positive pulses of potential field can lead to conduction current. In a metal piece, the \"jumped   electrons\" are compensated by electrons from air. In a closed circuit that uses the Avramenko's plug,\" electrons can be moving only in one direction and it is the reason for producing work in the load.\n\n2. To increase the power in the load, it is necessary to develop that part of the scheme that is responsible for the displacement current. The output power of the generator is not important. Small power is enough to create the wattless current. The question of power in load is the question of amplitude. It is possible to create high values of amplitude for a longitudinal wave of displacement current in a resonance mode.\n\n3. The principle, in general: the electric potential field is the cause for free wattless movement of charged particles (electrons or ions). This movement can be used for power generation. Most\ninteresting is the correlation of this experiment with  known electric induction phenomenon. The\ndevelopment of such technologies is most favorable in this direction, I think.\n\nFinally, I must note that N. Tesla demonstrated the transmission of power along a single wire in London in 1892 . Now all we need is the real interest of industry and official science to this well-known technology for clean power generation by means of potential source.\n\nReferences\n\n1. A.V. Frolov, \"The Application of Potential Energy for Creation of Power, New Energy News, vol. 2, no 2. May 1994.\n2. T. E. Bearden, \"Overunity Electrical Power Efficiency Using Energy Shuttling Between Two Circuits,\"  Proceedings of the 2nd international New Energy Symposium, Denver, Co, May 13-15. 1994.\n3. \"New Electric Transmission,\" summarized by Igor Goryachev, New Energy News, vol. 2, no 6, October 1994.\n4. N.E. Zaev, S.V. Avramenko, V.N. Lisin, \"The Measuring of Conduction Current That is Stimulated by Polarization Current,\" Journal of Russian Physical Society, no 2, 1991. Russian Text." ]
[ null, "http://alexfrolov.narod.ru/s-wire.gif", null ]
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http://arxiv-export-lb.library.cornell.edu/abs/2202.01611
[ "cond-mat.str-el\n\n# Title: On the Divergence of the Ferromagnetic Susceptibility in the SU(N) Nagaoka-Thouless Ferromagnet\n\nAbstract: Using finite temperature strong coupling expansions for the SU(N) Hubbard Model, we calculate the thermodynamic properties of the model in the infinite-$U$ limit for arbitrary density $0\\leq \\rho \\leq 1$ and all $N$. We express the ferromagnetic susceptibility of the model as a Curie term plus a $\\Delta \\chi$, an excess susceptibility above the Curie-behavior. We show that, on a bipartite lattice, graph by graph the contributions to $\\Delta \\chi$ are non-negative in the limit that the hole density $\\delta=1-\\rho$ goes to zero. By summing the contributions from all graphs consisting of closed loops we find that the low hole-density ferromagnetic susceptibility diverges exponentially as $\\exp{\\Delta /T}$ as $T \\to 0$ in two and higher dimensions. This demonstrates that Nagaoka-Thouless ferromagnetic state exists as a thermodynamic state of matter at low enough density of holes and sufficiently low temperatures. The constant $\\Delta$ scales with the SU(N) parameter $N$ as $1/N$ implying that ferromagnetism is gradually weakened with increasing $N$ as the characteristic temperature scale for ferromagnetic order goes down.\n Comments: 5 pages, 1 figure Subjects: Strongly Correlated Electrons (cond-mat.str-el); Quantum Gases (cond-mat.quant-gas) Journal reference: Phys. Rev. B 106, 014424 (2022) DOI: 10.1103/PhysRevB.106.014424 Cite as: arXiv:2202.01611 [cond-mat.str-el] (or arXiv:2202.01611v1 [cond-mat.str-el] for this version)\n\n## Submission history\n\nFrom: Rajiv Singh [view email]\n[v1] Thu, 3 Feb 2022 14:36:53 GMT (242kb)\n\nLink back to: arXiv, form interface, contact." ]
[ null ]
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http://resonantfractals.org/Joe_Cell/VE-333.html
[ "# The Vector Equilibrium\n\nfile / VE-333.html\n\n2016 - 11 - 23", null, "S1 = 29.613 cm\nA1 = 379.73 cm sq\nA2 = 876.94 cm sq\n\nVE consists of 2 basic forms, triangle and square, with common side length, assembled to produce a single point center with 12 equidistant connections in 3D space to the outer structure of the form.\n\nBeginning with the basic concepts under scrutiny:\n\n1 - The vector equilibrium is a form, sustained by the background field, and found at the heart of all matter at it's smallest inner point of manifestation\n\n2 - The background field is resonant at 333000 Hz - and this is what powers all matter and energy forms present on earth\n\n3 - The \"A\" field in electronics is an area, as shown in coils. The energy can be tapped at any point inside a coil of wire and is contained inside the loop with equal intensity at every point inside the loop.\n\n4 - The frequency of the \"A\" field is equal to the area inside the circle, triangle, or square. The larger the area the higher the energy inside the form and the higher the frequency of the mass vibration that is coherent.\n\n5 - We can dimension a Quantum Vector Equilibrium such that the area of the triangle times the area of the square will resonate directly with the background field. This form will couple to the inside of all matter and self power.\n\n6 - The metric system is derived from the properties of water, and thus can be used more efficiently for all calculation, accessing the root background field of space / time, and time / space.\n\n7 - If we extract the correct parameters of the Vector Equilibrium, at fractal dimensions where it couples, we can use this for health application, to create an access to all points on the body as one, and balance the inflow / outflow ratio to improve health.\nModification of size can be done using geometric fractal expansion or contraction.\n\nDerive the dimensions at cm levels for a quantum VE structure that will power off the background field at 333000 Hz.", null, "Split the background field into two factors, that will separate inflow and outflow.\n\nDerivation\n\nA1 * A2 = 333000   [inflow outflow separation factors]\nS1 = square root (A2)\nL1 = S1 * sin(60)\nA1 = L1 * S1 / 2\nA1 = S1 * sin(60) * S1 / 2\nA2 = S1 * S1\n333000 = S1 * S1 * S1 * S1 * sin(60) / 2\n333000 = S1^4 * sin(60) / 2\n666000 / sin(60) = S1^4\n\nS1 = Root 4 (666000 / sin(60))\nS1 = 29.613238 cm\nS1 = 296.13238 mm\n\nA1 = 379.72783 cm^2  Hz\nA2 = 876.94387 cm^2  Hz\n\nA2 / A1 = 2.3094 Frequency Ratio\n\n## Geometric Reduction\n\nS1 = 29.613238 cm             A1 = 379.72783                 A2 = 876.94387\n\nS1 / 2 =  14.806619 cm       A1 / 4   =  94.932               A2 / 4   =  219.236\nS1 / 3 =  9.8710793 cm       A1 / 9   =  42.192               A2 / 9   =   97.43820\nS1 / 4 =  7.4033095 cm       A1 / 16 =  23.733               A2 / 16 =   54.80899\n\n## Health Tube - VE / RA - Whole Body Energy Balancer\n\n[Ra Tube is a catch all group of resonant fractals that peak their energy center around 6 inches or 150 mm]\n[VE is the vector equilibrium form at the core of all matter]\n\nMaterial - Any Diamagnetic Metal such as Aluminum or Copper\nLength     148.07 mm\n\n# Quadrature Field From the Quantum VE", null, "S1 = 29.613238 cm\nS2 = 41.879443 cm\nFrequency = 1753.887729 cm sq", null, "Find the diameter of a circle with area 1753.887729 cm sq\nA = Pi  * r * r\nDiameter S3 = 2  * sqrt (Area / Pi)\n\nDiameter S3 =  47.25589 cm\nS3 / 2 = 23.62794 cm sq\nS3 / 4 = 11.81397 cm sq\n\nFind the diameter of a circle with area 876.9438654 cm sq\n\nS3 * sqrt 2 = 33.41496 cm\n\n# Triangle Spin", null, "Find the diameter of a circle with area 379.72783 cm sq\nA = Pi  * r * r\nDiameter S4 = 2  * sqrt (Area / Pi)\n\nDiameter S4 = 21.98828 cm\nS4 / 2 =  10.99414 cm\n\n#", null, "Find the area of the Hex form\nFind the diameter of a circle with Hex form area\n\nArea = 6 * 379.72783  cm sq\nArea = 2278.36698 cm sq\n\nDiameter = 2  * sqrt (Area / Pi)\n\nDiameter 53.860 cm\nDiameter / 2 = 26.930 cm\nDiameter / 4 = 13.4650 cm\n\n# Square Triangle Angle Differentials", null, "S1 = 29.613238 cm\nL1 = S1 * sin(60)\n\nIn = 20.9397214 cm\nOut =  24.179107 cm\n\nL1 = 25.645816 cm\nL2 = 14.806619\nL3 = 8.548605 cm\n\nArc sin (L3/L1) = 19.4712 Deg\nArc sin (L2/L1) = 35.2644 Deg\nArc sin (In/L1) = 54.735612 Deg\nArc sin (Out/L1) = 70.528778 Deg\n\nInner Differential Angle  =  54.735590 Deg\nOuter Differential Angle  = 125.264390 Deg" ]
[ null, "http://resonantfractals.org/Joe_Cell/VE-333/Vector-Equlibrium.jpg", null, "http://resonantfractals.org/Joe_Cell/VE-333/Drawing-1.jpg", null, "http://resonantfractals.org/Joe_Cell/VE-333/Quadrature-Field.jpg", null, "http://resonantfractals.org/Joe_Cell/VE-333/Spin.jpg", null, "http://resonantfractals.org/Joe_Cell/VE-333/Triangle-Spin.jpg", null, "http://resonantfractals.org/Joe_Cell/VE-333/Hex-Spin.jpg", null, "http://resonantfractals.org/Joe_Cell/VE-333/Sq-Tri-Angle.jpg", null ]
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https://www.shaalaa.com/concept-notes/surface-area-cube-cuboid-cylinder-concept-cube_7866
[ "Share\n\n# Surface Area and Volume of Cube, Cuboid and Cylinder - Concept of Cube\n\n#### notes\n\nA cube is a 3d representation of a square and has all equal sides. The length, breadth, and height in a cube are the same and are termed as sides (s). If s is each edge of the cube then,\nthe surface area of a cube=2 [(s × s) + (s × s) + (s × s)] = 2(3 s^2 ) = 6 s^2.", null, "Lateral Surface Area of Cube :\nThe area of 4 constituting squares gives us the lateral surface area of the cube.\nSo the lateral surface area of the cube shall be s^2+s^2+s^2+s^2 = 4 s^2.\nThe lateral surface area of a cube = 4 s^2\n\nS" ]
[ null, "https://www.shaalaa.com/images/_4:67da10b4ed2749ba9aeb3a0fe63c2a77.png", null ]
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https://www.deeplearningwizard.com/deep_learning/boosting_models_pytorch/lr_scheduling/
[ "# Learning Rate Scheduling¶\n\nRun Jupyter Notebook\n\nYou can run the code for this section in this jupyter notebook link.\n\n## Optimization Algorithm: Mini-batch Stochastic Gradient Descent (SGD)¶\n\n• We will be using mini-batch gradient descent in all our examples here when scheduling our learning rate\n• $\\theta = \\theta - \\eta \\cdot \\nabla J(\\theta, x^{i: i+n}, y^{i:i+n})$\n• Characteristics\n• Compute the gradient of the lost function w.r.t. parameters for n sets of training sample (n input and n label), $\\nabla J(\\theta, x^{i: i+n}, y^{i:i+n})$\n• Use this to update our parameters at every iteration\n• Typically in deep learning, some variation of mini-batch gradient is used where the batch size is a hyperparameter to be determined\n\n## Learning Intuition Recap¶\n\n• Learning process\n• Original parameters $\\rightarrow$ given input, get output $\\rightarrow$ compare with labels $\\rightarrow$ get loss with comparison of input/output $\\rightarrow$ get gradients of loss w.r.t parameters $\\rightarrow$ update parameters so model can churn output closer to labels $\\rightarrow$ repeat\n• For a detailed mathematical account of how this works and how to implement from scratch in Python and PyTorch, you can read our forward- and back-propagation and gradient descent post.\n\n## Learning Rate Pointers¶", null, "• Update parameters so model can churn output closer to labels, lower loss\n• $\\theta = \\theta - \\eta \\cdot \\nabla J(\\theta, x^{i: i+n}, y^{i:i+n})$\n• If we set $\\eta$ to be a large value $\\rightarrow$ learn too much (rapid learning)\n• Unable to converge to a good local minima (unable to effectively gradually decrease your loss, overshoot the local lowest value)\n• If we set $\\eta$ to be a small value $\\rightarrow$ learn too little (slow learning)\n• May take too long or unable to convert to a good local minima\n\n## Need for Learning Rate Schedules¶\n\n• Benefits\n• Converge faster\n• Higher accuracy", null, "## Top Basic Learning Rate Schedules¶\n\n1. Step-wise Decay\n2. Reduce on Loss Plateau Decay\n\n### Step-wise Learning Rate Decay¶\n\n#### Step-wise Decay: Every Epoch¶\n\n• At every epoch,\n• $\\eta_t = \\eta_{t-1}\\gamma$\n• $\\gamma = 0.1$\n• Optimization Algorithm 4: SGD Nesterov\n• Modification of SGD Momentum\n• $v_t = \\gamma v_{t-1} + \\eta \\cdot \\nabla J(\\theta - \\gamma v_{t-1}, x^{i: i+n}, y^{i:i+n})$\n• $\\theta = \\theta - v_t$\n• Practical example\n• Given $\\eta_t = 0.1$ and $\\gamma = 0.01$\n• Epoch 0: $\\eta_t = 0.1$\n• Epoch 1: $\\eta_{t+1} = 0.1 (0.1) = 0.01$\n• Epoch 2: $\\eta_{t+2} = 0.1 (0.1)^2 = 0.001$\n• Epoch n: $\\eta_{t+n} = 0.1 (0.1)^n$\n\nCode for step-wise learning rate decay at every epoch\n\nimport torch\nimport torch.nn as nn\nimport torchvision.transforms as transforms\nimport torchvision.datasets as dsets\n\n# Set seed\ntorch.manual_seed(0)\n\n# Where to add a new import\nfrom torch.optim.lr_scheduler import StepLR\n\n'''\n'''\n\ntrain_dataset = dsets.MNIST(root='./data',\ntrain=True,\ntransform=transforms.ToTensor(),\n\ntest_dataset = dsets.MNIST(root='./data',\ntrain=False,\ntransform=transforms.ToTensor())\n\n'''\nSTEP 2: MAKING DATASET ITERABLE\n'''\n\nbatch_size = 100\nn_iters = 3000\nnum_epochs = n_iters / (len(train_dataset) / batch_size)\nnum_epochs = int(num_epochs)\n\nbatch_size=batch_size,\nshuffle=True)\n\nbatch_size=batch_size,\nshuffle=False)\n\n'''\nSTEP 3: CREATE MODEL CLASS\n'''\nclass FeedforwardNeuralNetModel(nn.Module):\ndef __init__(self, input_dim, hidden_dim, output_dim):\nsuper(FeedforwardNeuralNetModel, self).__init__()\n# Linear function\nself.fc1 = nn.Linear(input_dim, hidden_dim)\n# Non-linearity\nself.relu = nn.ReLU()\nself.fc2 = nn.Linear(hidden_dim, output_dim)\n\ndef forward(self, x):\n# Linear function\nout = self.fc1(x)\n# Non-linearity\nout = self.relu(out)\nout = self.fc2(out)\nreturn out\n'''\nSTEP 4: INSTANTIATE MODEL CLASS\n'''\ninput_dim = 28*28\nhidden_dim = 100\noutput_dim = 10\n\nmodel = FeedforwardNeuralNetModel(input_dim, hidden_dim, output_dim)\n\n'''\nSTEP 5: INSTANTIATE LOSS CLASS\n'''\ncriterion = nn.CrossEntropyLoss()\n\n'''\nSTEP 6: INSTANTIATE OPTIMIZER CLASS\n'''\nlearning_rate = 0.1\n\noptimizer = torch.optim.SGD(model.parameters(), lr=learning_rate, momentum=0.9, nesterov=True)\n\n'''\nSTEP 7: INSTANTIATE STEP LEARNING SCHEDULER CLASS\n'''\n# step_size: at how many multiples of epoch you decay\n# step_size = 1, after every 1 epoch, new_lr = lr*gamma\n# step_size = 2, after every 2 epoch, new_lr = lr*gamma\n\n# gamma = decaying factor\nscheduler = StepLR(optimizer, step_size=1, gamma=0.1)\n\n'''\nSTEP 7: TRAIN THE MODEL\n'''\niter = 0\nfor epoch in range(num_epochs):\n# Decay Learning Rate\nscheduler.step()\n# Print Learning Rate\nprint('Epoch:', epoch,'LR:', scheduler.get_lr())\nfor i, (images, labels) in enumerate(train_loader):\n\n# Forward pass to get output/logits\noutputs = model(images)\n\n# Calculate Loss: softmax --> cross entropy loss\nloss = criterion(outputs, labels)\n\nloss.backward()\n\n# Updating parameters\noptimizer.step()\n\niter += 1\n\nif iter % 500 == 0:\n# Calculate Accuracy\ncorrect = 0\ntotal = 0\n# Iterate through test dataset\n# Load images to a Torch Variable\nimages = images.view(-1, 28*28)\n\n# Forward pass only to get logits/output\noutputs = model(images)\n\n# Get predictions from the maximum value\n_, predicted = torch.max(outputs.data, 1)\n\n# Total number of labels\ntotal += labels.size(0)\n\n# Total correct predictions\ncorrect += (predicted == labels).sum()\n\naccuracy = 100 * correct / total\n\n# Print Loss\nprint('Iteration: {}. Loss: {}. Accuracy: {}'.format(iter, loss.item(), accuracy))\n\nEpoch: 0 LR: [0.1]\nIteration: 500. Loss: 0.15292978286743164. Accuracy: 96\nEpoch: 1 LR: [0.010000000000000002]\nIteration: 1000. Loss: 0.1207798570394516. Accuracy: 97\nEpoch: 2 LR: [0.0010000000000000002]\nIteration: 1500. Loss: 0.12287932634353638. Accuracy: 97\nEpoch: 3 LR: [0.00010000000000000003]\nIteration: 2000. Loss: 0.05614742264151573. Accuracy: 97\nEpoch: 4 LR: [1.0000000000000003e-05]\nIteration: 2500. Loss: 0.06775809079408646. Accuracy: 97\nIteration: 3000. Loss: 0.03737065941095352. Accuracy: 97\n\n\n#### Step-wise Decay: Every 2 Epochs¶\n\n• At every 2 epoch,\n• $\\eta_t = \\eta_{t-1}\\gamma$\n• $\\gamma = 0.1$\n• Optimization Algorithm 4: SGD Nesterov\n• Modification of SGD Momentum\n• $v_t = \\gamma v_{t-1} + \\eta \\cdot \\nabla J(\\theta - \\gamma v_{t-1}, x^{i: i+n}, y^{i:i+n})$\n• $\\theta = \\theta - v_t$\n• Practical example\n• Given $\\eta_t = 0.1$ and $\\gamma = 0.01$\n• Epoch 0: $\\eta_t = 0.1$\n• Epoch 1: $\\eta_{t+1} = 0.1$\n• Epoch 2: $\\eta_{t+2} = 0.1 (0.1) = 0.01$\n\nCode for step-wise learning rate decay at every 2 epoch\n\nimport torch\nimport torch.nn as nn\nimport torchvision.transforms as transforms\nimport torchvision.datasets as dsets\n\n# Set seed\ntorch.manual_seed(0)\n\n# Where to add a new import\nfrom torch.optim.lr_scheduler import StepLR\n\n'''\n'''\n\ntrain_dataset = dsets.MNIST(root='./data',\ntrain=True,\ntransform=transforms.ToTensor(),\n\ntest_dataset = dsets.MNIST(root='./data',\ntrain=False,\ntransform=transforms.ToTensor())\n\n'''\nSTEP 2: MAKING DATASET ITERABLE\n'''\n\nbatch_size = 100\nn_iters = 3000\nnum_epochs = n_iters / (len(train_dataset) / batch_size)\nnum_epochs = int(num_epochs)\n\nbatch_size=batch_size,\nshuffle=True)\n\nbatch_size=batch_size,\nshuffle=False)\n\n'''\nSTEP 3: CREATE MODEL CLASS\n'''\nclass FeedforwardNeuralNetModel(nn.Module):\ndef __init__(self, input_dim, hidden_dim, output_dim):\nsuper(FeedforwardNeuralNetModel, self).__init__()\n# Linear function\nself.fc1 = nn.Linear(input_dim, hidden_dim)\n# Non-linearity\nself.relu = nn.ReLU()\nself.fc2 = nn.Linear(hidden_dim, output_dim)\n\ndef forward(self, x):\n# Linear function\nout = self.fc1(x)\n# Non-linearity\nout = self.relu(out)\nout = self.fc2(out)\nreturn out\n'''\nSTEP 4: INSTANTIATE MODEL CLASS\n'''\ninput_dim = 28*28\nhidden_dim = 100\noutput_dim = 10\n\nmodel = FeedforwardNeuralNetModel(input_dim, hidden_dim, output_dim)\n\n'''\nSTEP 5: INSTANTIATE LOSS CLASS\n'''\ncriterion = nn.CrossEntropyLoss()\n\n'''\nSTEP 6: INSTANTIATE OPTIMIZER CLASS\n'''\nlearning_rate = 0.1\n\noptimizer = torch.optim.SGD(model.parameters(), lr=learning_rate, momentum=0.9, nesterov=True)\n\n'''\nSTEP 7: INSTANTIATE STEP LEARNING SCHEDULER CLASS\n'''\n# step_size: at how many multiples of epoch you decay\n# step_size = 1, after every 2 epoch, new_lr = lr*gamma\n# step_size = 2, after every 2 epoch, new_lr = lr*gamma\n\n# gamma = decaying factor\nscheduler = StepLR(optimizer, step_size=2, gamma=0.1)\n\n'''\nSTEP 7: TRAIN THE MODEL\n'''\niter = 0\nfor epoch in range(num_epochs):\n# Decay Learning Rate\nscheduler.step()\n# Print Learning Rate\nprint('Epoch:', epoch,'LR:', scheduler.get_lr())\nfor i, (images, labels) in enumerate(train_loader):\n\n# Forward pass to get output/logits\noutputs = model(images)\n\n# Calculate Loss: softmax --> cross entropy loss\nloss = criterion(outputs, labels)\n\nloss.backward()\n\n# Updating parameters\noptimizer.step()\n\niter += 1\n\nif iter % 500 == 0:\n# Calculate Accuracy\ncorrect = 0\ntotal = 0\n# Iterate through test dataset\n# Load images to a Torch Variable\n\n# Forward pass only to get logits/output\noutputs = model(images)\n\n# Get predictions from the maximum value\n_, predicted = torch.max(outputs.data, 1)\n\n# Total number of labels\ntotal += labels.size(0)\n\n# Total correct predictions\ncorrect += (predicted == labels).sum()\n\naccuracy = 100 * correct / total\n\n# Print Loss\nprint('Iteration: {}. Loss: {}. Accuracy: {}'.format(iter, loss.item(), accuracy))\n\nEpoch: 0 LR: [0.1]\nIteration: 500. Loss: 0.15292978286743164. Accuracy: 96\nEpoch: 1 LR: [0.1]\nIteration: 1000. Loss: 0.11253029108047485. Accuracy: 96\nEpoch: 2 LR: [0.010000000000000002]\nIteration: 1500. Loss: 0.14498558640480042. Accuracy: 97\nEpoch: 3 LR: [0.010000000000000002]\nIteration: 2000. Loss: 0.03691177815198898. Accuracy: 97\nEpoch: 4 LR: [0.0010000000000000002]\nIteration: 2500. Loss: 0.03511016443371773. Accuracy: 97\nIteration: 3000. Loss: 0.029424520209431648. Accuracy: 97\n\n\n#### Step-wise Decay: Every Epoch, Larger Gamma¶\n\n• At every epoch,\n• $\\eta_t = \\eta_{t-1}\\gamma$\n• $\\gamma = 0.96$\n• Optimization Algorithm 4: SGD Nesterov\n• Modification of SGD Momentum\n• $v_t = \\gamma v_{t-1} + \\eta \\cdot \\nabla J(\\theta - \\gamma v_{t-1}, x^{i: i+n}, y^{i:i+n})$\n• $\\theta = \\theta - v_t$\n• Practical example\n• Given $\\eta_t = 0.1$ and $\\gamma = 0.96$\n• Epoch 1: $\\eta_t = 0.1$\n• Epoch 2: $\\eta_{t+1} = 0.1 (0.96) = 0.096$\n• Epoch 3: $\\eta_{t+2} = 0.1 (0.96)^2 = 0.092$\n• Epoch n: $\\eta_{t+n} = 0.1 (0.96)^n$\n\nCode for step-wise learning rate decay at every epoch with larger gamma\n\nimport torch\nimport torch.nn as nn\nimport torchvision.transforms as transforms\nimport torchvision.datasets as dsets\n\n# Set seed\ntorch.manual_seed(0)\n\n# Where to add a new import\nfrom torch.optim.lr_scheduler import StepLR\n\n'''\n'''\n\ntrain_dataset = dsets.MNIST(root='./data',\ntrain=True,\ntransform=transforms.ToTensor(),\n\ntest_dataset = dsets.MNIST(root='./data',\ntrain=False,\ntransform=transforms.ToTensor())\n\n'''\nSTEP 2: MAKING DATASET ITERABLE\n'''\n\nbatch_size = 100\nn_iters = 3000\nnum_epochs = n_iters / (len(train_dataset) / batch_size)\nnum_epochs = int(num_epochs)\n\nbatch_size=batch_size,\nshuffle=True)\n\nbatch_size=batch_size,\nshuffle=False)\n\n'''\nSTEP 3: CREATE MODEL CLASS\n'''\nclass FeedforwardNeuralNetModel(nn.Module):\ndef __init__(self, input_dim, hidden_dim, output_dim):\nsuper(FeedforwardNeuralNetModel, self).__init__()\n# Linear function\nself.fc1 = nn.Linear(input_dim, hidden_dim)\n# Non-linearity\nself.relu = nn.ReLU()\nself.fc2 = nn.Linear(hidden_dim, output_dim)\n\ndef forward(self, x):\n# Linear function\nout = self.fc1(x)\n# Non-linearity\nout = self.relu(out)\nout = self.fc2(out)\nreturn out\n'''\nSTEP 4: INSTANTIATE MODEL CLASS\n'''\ninput_dim = 28*28\nhidden_dim = 100\noutput_dim = 10\n\nmodel = FeedforwardNeuralNetModel(input_dim, hidden_dim, output_dim)\n\n'''\nSTEP 5: INSTANTIATE LOSS CLASS\n'''\ncriterion = nn.CrossEntropyLoss()\n\n'''\nSTEP 6: INSTANTIATE OPTIMIZER CLASS\n'''\nlearning_rate = 0.1\n\noptimizer = torch.optim.SGD(model.parameters(), lr=learning_rate, momentum=0.9, nesterov=True)\n\n'''\nSTEP 7: INSTANTIATE STEP LEARNING SCHEDULER CLASS\n'''\n# step_size: at how many multiples of epoch you decay\n# step_size = 1, after every 2 epoch, new_lr = lr*gamma\n# step_size = 2, after every 2 epoch, new_lr = lr*gamma\n\n# gamma = decaying factor\nscheduler = StepLR(optimizer, step_size=2, gamma=0.96)\n\n'''\nSTEP 7: TRAIN THE MODEL\n'''\niter = 0\nfor epoch in range(num_epochs):\n# Decay Learning Rate\nscheduler.step()\n# Print Learning Rate\nprint('Epoch:', epoch,'LR:', scheduler.get_lr())\nfor i, (images, labels) in enumerate(train_loader):\n\n# Forward pass to get output/logits\noutputs = model(images)\n\n# Calculate Loss: softmax --> cross entropy loss\nloss = criterion(outputs, labels)\n\nloss.backward()\n\n# Updating parameters\noptimizer.step()\n\niter += 1\n\nif iter % 500 == 0:\n# Calculate Accuracy\ncorrect = 0\ntotal = 0\n# Iterate through test dataset\n# Load images to a Torch Variable\nimages = images.view(-1, 28*28)\n\n# Forward pass only to get logits/output\noutputs = model(images)\n\n# Get predictions from the maximum value\n_, predicted = torch.max(outputs.data, 1)\n\n# Total number of labels\ntotal += labels.size(0)\n\n# Total correct predictions\ncorrect += (predicted == labels).sum()\n\naccuracy = 100 * correct / total\n\n# Print Loss\nprint('Iteration: {}. Loss: {}. Accuracy: {}'.format(iter, loss.item(), accuracy))\n\nEpoch: 0 LR: [0.1]\nIteration: 500. Loss: 0.15292978286743164. Accuracy: 96\nEpoch: 1 LR: [0.1]\nIteration: 1000. Loss: 0.11253029108047485. Accuracy: 96\nEpoch: 2 LR: [0.096]\nIteration: 1500. Loss: 0.11864850670099258. Accuracy: 97\nEpoch: 3 LR: [0.096]\nIteration: 2000. Loss: 0.030942382290959358. Accuracy: 97\nEpoch: 4 LR: [0.09216]\nIteration: 2500. Loss: 0.04521659016609192. Accuracy: 97\nIteration: 3000. Loss: 0.027839098125696182. Accuracy: 97\n\n\n#### Pointers on Step-wise Decay¶\n\n• You would want to decay your LR gradually when you're training more epochs\n• Converge too fast, to a crappy loss/accuracy, if you decay rapidly\n• To decay slower\n• Larger $\\gamma$\n• Larger interval of decay\n\n### Reduce on Loss Plateau Decay¶\n\n#### Reduce on Loss Plateau Decay, Patience=0, Factor=0.1¶\n\n• Reduce learning rate whenever loss plateaus\n• Patience: number of epochs with no improvement after which learning rate will be reduced\n• Patience = 0\n• Factor: multiplier to decrease learning rate, $lr = lr*factor = \\gamma$\n• Factor = 0.1\n• Optimization Algorithm: SGD Nesterov\n• Modification of SGD Momentum\n• $v_t = \\gamma v_{t-1} + \\eta \\cdot \\nabla J(\\theta - \\gamma v_{t-1}, x^{i: i+n}, y^{i:i+n})$\n• $\\theta = \\theta - v_t$\n\nCode for reduce on loss plateau learning rate decay of factor 0.1 and 0 patience\n\nimport torch\nimport torch.nn as nn\nimport torchvision.transforms as transforms\nimport torchvision.datasets as dsets\n\n# Set seed\ntorch.manual_seed(0)\n\n# Where to add a new import\nfrom torch.optim.lr_scheduler import ReduceLROnPlateau\n\n'''\n'''\n\ntrain_dataset = dsets.MNIST(root='./data',\ntrain=True,\ntransform=transforms.ToTensor(),\n\ntest_dataset = dsets.MNIST(root='./data',\ntrain=False,\ntransform=transforms.ToTensor())\n\n'''\nSTEP 2: MAKING DATASET ITERABLE\n'''\n\nbatch_size = 100\nn_iters = 6000\nnum_epochs = n_iters / (len(train_dataset) / batch_size)\nnum_epochs = int(num_epochs)\n\nbatch_size=batch_size,\nshuffle=True)\n\nbatch_size=batch_size,\nshuffle=False)\n\n'''\nSTEP 3: CREATE MODEL CLASS\n'''\nclass FeedforwardNeuralNetModel(nn.Module):\ndef __init__(self, input_dim, hidden_dim, output_dim):\nsuper(FeedforwardNeuralNetModel, self).__init__()\n# Linear function\nself.fc1 = nn.Linear(input_dim, hidden_dim)\n# Non-linearity\nself.relu = nn.ReLU()\nself.fc2 = nn.Linear(hidden_dim, output_dim)\n\ndef forward(self, x):\n# Linear function\nout = self.fc1(x)\n# Non-linearity\nout = self.relu(out)\nout = self.fc2(out)\nreturn out\n'''\nSTEP 4: INSTANTIATE MODEL CLASS\n'''\ninput_dim = 28*28\nhidden_dim = 100\noutput_dim = 10\n\nmodel = FeedforwardNeuralNetModel(input_dim, hidden_dim, output_dim)\n\n'''\nSTEP 5: INSTANTIATE LOSS CLASS\n'''\ncriterion = nn.CrossEntropyLoss()\n\n'''\nSTEP 6: INSTANTIATE OPTIMIZER CLASS\n'''\nlearning_rate = 0.1\n\noptimizer = torch.optim.SGD(model.parameters(), lr=learning_rate, momentum=0.9, nesterov=True)\n\n'''\nSTEP 7: INSTANTIATE STEP LEARNING SCHEDULER CLASS\n'''\n# lr = lr * factor\n# mode='max': look for the maximum validation accuracy to track\n# patience: number of epochs - 1 where loss plateaus before decreasing LR\n# patience = 0, after 1 bad epoch, reduce LR\n# factor = decaying factor\nscheduler = ReduceLROnPlateau(optimizer, mode='max', factor=0.1, patience=0, verbose=True)\n\n'''\nSTEP 7: TRAIN THE MODEL\n'''\niter = 0\nfor epoch in range(num_epochs):\nfor i, (images, labels) in enumerate(train_loader):\n\n# Forward pass to get output/logits\noutputs = model(images)\n\n# Calculate Loss: softmax --> cross entropy loss\nloss = criterion(outputs, labels)\n\nloss.backward()\n\n# Updating parameters\noptimizer.step()\n\niter += 1\n\nif iter % 500 == 0:\n# Calculate Accuracy\ncorrect = 0\ntotal = 0\n# Iterate through test dataset\n# Load images to a Torch Variable\nimages = images.view(-1, 28*28)\n\n# Forward pass only to get logits/output\noutputs = model(images)\n\n# Get predictions from the maximum value\n_, predicted = torch.max(outputs.data, 1)\n\n# Total number of labels\ntotal += labels.size(0)\n\n# Total correct predictions\n# Without .item(), it is a uint8 tensor which will not work when you pass this number to the scheduler\ncorrect += (predicted == labels).sum().item()\n\naccuracy = 100 * correct / total\n\n# Print Loss\n# print('Iteration: {}. Loss: {}. Accuracy: {}'.format(iter, loss.data, accuracy))\n\n# Decay Learning Rate, pass validation accuracy for tracking at every epoch\nprint('Epoch {} completed'.format(epoch))\nprint('Loss: {}. Accuracy: {}'.format(loss.item(), accuracy))\nprint('-'*20)\nscheduler.step(accuracy)\n\nEpoch 0 completed\nLoss: 0.17087846994400024. Accuracy: 96.26\n--------------------\nEpoch 1 completed\nLoss: 0.11688263714313507. Accuracy: 96.96\n--------------------\nEpoch 2 completed\nLoss: 0.035437121987342834. Accuracy: 96.78\n--------------------\nEpoch 2: reducing learning rate of group 0 to 1.0000e-02.\nEpoch 3 completed\nLoss: 0.0324370414018631. Accuracy: 97.7\n--------------------\nEpoch 4 completed\nLoss: 0.022194599732756615. Accuracy: 98.02\n--------------------\nEpoch 5 completed\nLoss: 0.007145566865801811. Accuracy: 98.03\n--------------------\nEpoch 6 completed\nLoss: 0.01673538237810135. Accuracy: 98.05\n--------------------\nEpoch 7 completed\nLoss: 0.025424446910619736. Accuracy: 98.01\n--------------------\nEpoch 7: reducing learning rate of group 0 to 1.0000e-03.\nEpoch 8 completed\nLoss: 0.014696130529046059. Accuracy: 98.05\n--------------------\nEpoch 8: reducing learning rate of group 0 to 1.0000e-04.\nEpoch 9 completed\nLoss: 0.00573748117312789. Accuracy: 98.04\n--------------------\nEpoch 9: reducing learning rate of group 0 to 1.0000e-05.\n\n\n#### Reduce on Loss Plateau Decay, Patience=0, Factor=0.5¶\n\n• Reduce learning rate whenever loss plateaus\n• Patience: number of epochs with no improvement after which learning rate will be reduced\n• Patience = 0\n• Factor: multiplier to decrease learning rate, $lr = lr*factor = \\gamma$\n• Factor = 0.5\n• Optimization Algorithm 4: SGD Nesterov\n• Modification of SGD Momentum\n• $v_t = \\gamma v_{t-1} + \\eta \\cdot \\nabla J(\\theta - \\gamma v_{t-1}, x^{i: i+n}, y^{i:i+n})$\n• $\\theta = \\theta - v_t$\n\nCode for reduce on loss plateau learning rate decay with factor 0.5 and 0 patience\n\nimport torch\nimport torch.nn as nn\nimport torchvision.transforms as transforms\nimport torchvision.datasets as dsets\n\n# Set seed\ntorch.manual_seed(0)\n\n# Where to add a new import\nfrom torch.optim.lr_scheduler import ReduceLROnPlateau\n\n'''\n'''\n\ntrain_dataset = dsets.MNIST(root='./data',\ntrain=True,\ntransform=transforms.ToTensor(),\n\ntest_dataset = dsets.MNIST(root='./data',\ntrain=False,\ntransform=transforms.ToTensor())\n\n'''\nSTEP 2: MAKING DATASET ITERABLE\n'''\n\nbatch_size = 100\nn_iters = 6000\nnum_epochs = n_iters / (len(train_dataset) / batch_size)\nnum_epochs = int(num_epochs)\n\nbatch_size=batch_size,\nshuffle=True)\n\nbatch_size=batch_size,\nshuffle=False)\n\n'''\nSTEP 3: CREATE MODEL CLASS\n'''\nclass FeedforwardNeuralNetModel(nn.Module):\ndef __init__(self, input_dim, hidden_dim, output_dim):\nsuper(FeedforwardNeuralNetModel, self).__init__()\n# Linear function\nself.fc1 = nn.Linear(input_dim, hidden_dim)\n# Non-linearity\nself.relu = nn.ReLU()\nself.fc2 = nn.Linear(hidden_dim, output_dim)\n\ndef forward(self, x):\n# Linear function\nout = self.fc1(x)\n# Non-linearity\nout = self.relu(out)\nout = self.fc2(out)\nreturn out\n'''\nSTEP 4: INSTANTIATE MODEL CLASS\n'''\ninput_dim = 28*28\nhidden_dim = 100\noutput_dim = 10\n\nmodel = FeedforwardNeuralNetModel(input_dim, hidden_dim, output_dim)\n\n'''\nSTEP 5: INSTANTIATE LOSS CLASS\n'''\ncriterion = nn.CrossEntropyLoss()\n\n'''\nSTEP 6: INSTANTIATE OPTIMIZER CLASS\n'''\nlearning_rate = 0.1\n\noptimizer = torch.optim.SGD(model.parameters(), lr=learning_rate, momentum=0.9, nesterov=True)\n\n'''\nSTEP 7: INSTANTIATE STEP LEARNING SCHEDULER CLASS\n'''\n# lr = lr * factor\n# mode='max': look for the maximum validation accuracy to track\n# patience: number of epochs - 1 where loss plateaus before decreasing LR\n# patience = 0, after 1 bad epoch, reduce LR\n# factor = decaying factor\nscheduler = ReduceLROnPlateau(optimizer, mode='max', factor=0.5, patience=0, verbose=True)\n\n'''\nSTEP 7: TRAIN THE MODEL\n'''\niter = 0\nfor epoch in range(num_epochs):\nfor i, (images, labels) in enumerate(train_loader):\n\n# Forward pass to get output/logits\noutputs = model(images)\n\n# Calculate Loss: softmax --> cross entropy loss\nloss = criterion(outputs, labels)\n\nloss.backward()\n\n# Updating parameters\noptimizer.step()\n\niter += 1\n\nif iter % 500 == 0:\n# Calculate Accuracy\ncorrect = 0\ntotal = 0\n# Iterate through test dataset\n# Load images to a Torch Variable\nimages = images.view(-1, 28*28)\n\n# Forward pass only to get logits/output\noutputs = model(images)\n\n# Get predictions from the maximum value\n_, predicted = torch.max(outputs.data, 1)\n\n# Total number of labels\ntotal += labels.size(0)\n\n# Total correct predictions\n# Without .item(), it is a uint8 tensor which will not work when you pass this number to the scheduler\ncorrect += (predicted == labels).sum().item()\n\naccuracy = 100 * correct / total\n\n# Print Loss\n# print('Iteration: {}. Loss: {}. Accuracy: {}'.format(iter, loss.data, accuracy))\n\n# Decay Learning Rate, pass validation accuracy for tracking at every epoch\nprint('Epoch {} completed'.format(epoch))\nprint('Loss: {}. Accuracy: {}'.format(loss.item(), accuracy))\nprint('-'*20)\nscheduler.step(accuracy)\n\nEpoch 0 completed\nLoss: 0.17087846994400024. Accuracy: 96.26\n--------------------\nEpoch 1 completed\nLoss: 0.11688263714313507. Accuracy: 96.96\n--------------------\nEpoch 2 completed\nLoss: 0.035437121987342834. Accuracy: 96.78\n--------------------\nEpoch 2: reducing learning rate of group 0 to 5.0000e-02.\nEpoch 3 completed\nLoss: 0.04893001914024353. Accuracy: 97.62\n--------------------\nEpoch 4 completed\nLoss: 0.020584167912602425. Accuracy: 97.86\n--------------------\nEpoch 5 completed\nLoss: 0.006022400688380003. Accuracy: 97.95\n--------------------\nEpoch 6 completed\nLoss: 0.028374142944812775. Accuracy: 97.87\n--------------------\nEpoch 6: reducing learning rate of group 0 to 2.5000e-02.\nEpoch 7 completed\nLoss: 0.013204765506088734. Accuracy: 98.0\n--------------------\nEpoch 8 completed\nLoss: 0.010137186385691166. Accuracy: 97.95\n--------------------\nEpoch 8: reducing learning rate of group 0 to 1.2500e-02.\nEpoch 9 completed\nLoss: 0.0035198689438402653. Accuracy: 98.01\n--------------------\n\n\n## Pointers on Reduce on Loss Pleateau Decay¶\n\n• In these examples, we used patience=1 because we are running few epochs\n• You should look at a larger patience such as 5 if for example you ran 500 epochs.\n• You should experiment with 2 properties\n• Patience\n• Decay factor\n\n## Summary¶\n\nWe've learnt...\n\nSuccess\n\n• Learning Rate Intuition\n• Update parameters so model can churn output closer to labels\n• Learning Rate Pointers\n• If we set $\\eta$ to be a large value $\\rightarrow$ learn too much (rapid learning)\n• If we set $\\eta$ to be a small value $\\rightarrow$ learn too little (slow learning)\n• Learning Rate Schedules\n• Step-wise Decay\n• Reduce on Loss Plateau Decay\n• Step-wise Decay\n• Every 1 epoch\n• Every 2 epoch\n• Every 1 epoch, larger gamma\n• Step-wise Decay Pointers\n• Larger $\\gamma$\n• Larger interval of decay (increase epoch)\n• Reduce on Loss Plateau Decay\n• Patience=0, Factor=1\n• Patience=0, Factor=0.5\n• Pointers on Reduce on Loss Plateau Decay\n• Larger patience with more epochs\n• 2 hyperparameters to experiment\n• Patience\n• Decay factor\n\n## Citation¶\n\nIf you have found these useful in your research, presentations, school work, projects or workshops, feel free to cite using this DOI." ]
[ null, "https://www.deeplearningwizard.com/deep_learning/boosting_models_pytorch/images/lr1.png", null, "https://www.deeplearningwizard.com/deep_learning/boosting_models_pytorch/images/lr2.png", null ]
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https://apps.dtic.mil/sti/citations/AD0705206
[ "# Abstract:\n\nIn order to obtain approximate solution for the flow in vicinity of the throat of a Laval nozzle assumptions of some kind must be made, but it is desirable to keep the arbitrariness introduced to a minimum. The flows considered in the report have swirl, besides the approximation should be applicable for nozzles which have rather large curvature. The report begins with some general observations regarding the choices that can be made. For the actual computations the flow equations are represented in natural coordinates i.e., they are expressed in terms of derivatives in the direction of the streamlines and in the direction normal to it. It is then assumed that within a narrow strip extending across the nozzle the flow angle and the enthalpy can be represented along each streamline by a polynomial of the second degree. The derivatives in the streamwise direction are replaced by finite differences while the derivatives normal to the streamline direction are retained in their original form. The flow equations then reduce to a system of ordinary differential equations. At the nozzle axis one has obvious symmetry conditions, at the nozzle wall the streamline curvature and its derivative in the streamwise direction can be prescribed. This two point boundary value problem is solved numerically. In the computation the strip has the sonic line as its upstream boundary, the other boundary is chosen and a nearly constant distance downstream. The report contains a number of tables and graphs for swirl flows computed by this method. Author\n\n# Subject Categories:\n\n• Aerodynamics\n• Fluid Mechanics" ]
[ null ]
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https://www.jmag-international.com/conference_doc/uc2002_07/
[ "## Numerical Calculation of AC Loss of Superconductor\n\nThe PDF file is not available.\n\n### Abstract\n\nNumerical calculation of AC transport current loss of cylindrical superconductor was performed by JMAG. The result of calculation agreed well with theoretical analysis. In addition, AC transport loss in which magnetic field dependence of critical current density and geometrical effect of superconductor were taken into account was calculated by JMAG. The calculation result agreeed well with experimental result for QMG oxide superconducting limiting device. The reason for good agreement by prediction of simple Norris formula in which the both effect were neglected was the both effect were complemented each other. The prediction by Norris formula is considered to be accidentally coincided with the experimental result.\nKeywords:finite element method, AC transport loss, Norris formula, Bean model, Kim model, Irie-Yamafuji model" ]
[ null ]
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http://arca.di.uminho.pt/quantum-computation-2021/
[ " Quantum Computation 2020/21\n\nLearning Outcomes\n\nOn successful completion of the course students should be able\n\n• To understand basic concepts of computability, computational complexity, and underlying mathematical structures.\n• To master the quantum computational model.\n• To design and analyse quantum algorithms.\n• To implement and run quantum algorithms in the Qiskit open-source software development kit for IBM Q quantum processors.\n\nSyllabus\n\n• Computability and complexity\n• Mathematical backgound: sets, orders, groups, automata.\n• Turing machines and computability.\n• Computational complexity. Agorithms and complexity classes.\n• Quantum computation and algorithms:\n• The quantum computational model (circuits, gates, measurements).\n• Introduction to quantum algorithms.\n• Algorithms based on phase amplification.\n• Algorithms based on the quantum Fourier transform.\n• Case studies in quantum algorithmics.\n• Quantum complexity.\n• Quantum programming\n• Quantum programming in a functional setting.\n• Quantum programming in Qiskit\n\nSummaries (2020-21)\n\nT Lectures\nNew Virtual classroom: Join here every week\n\n• Feb 19: Introduction to Quantum Computation and the course dynamics (slides).\n\nLink for the first lecture (only): Join here\n\n• Feb 23:\n\nBackground: Discrete mathematical structures -- sets and cardinality (lecture notes).\n\n• Mar 2:\n\nBackground: Discrete mathematical structures -- groups (lecture notes).\n\n• Mar 16:\n\nIntroduction to computability. Turing machines and universal Turing machines. Recursive functions (lecture notes).\n\n• Mar 23:\n\nIntroduction to computational complexity. Basic notions and tools. Complexity classes (lecture notes).\n\n• Abr 9: Introduction to quantum algorithms. Phase kick-back. The Deutsch-Joza algorithm. (slides).\n\nLink for this lecture (only): Join here\n\n• Abr 13:\n\nAmplitude amplification as an algorithimic technique. Search problems and Grover's algorithm. (slides).\n\n• Abr 23:\n\nFurther quantum algorithms: Bernstein-Vazirani and Simon. Variants. (slides).\n\n• May 7:\n\nCase study: Quantum Bayesian decision making (slides) (paper). The quantum phase estimation problem (slides).\n\n• May 7 (14.30):\n\nQuantum Fourier transform. The eigenvalue estimation problem (slides; first section)\n\nLink for this lecture (only): Join here\n\n• May 14:\n\nCase study: Quantum reinforcement learning (slides). Resolution of the QFT exercise (note).\n\n• May 21:\n\nThe algorithm of Shor. Reduction to order-finding. (slides)\n\nThe hidden subgroup problem and its instances: finding the period of a periodic function; the discrete logarithm problem. (slides)\n\nCase study: Quantum walks. (notebook)\n\nBibliography\n\nComputability and Computational Complexity\n• H. R. Lewis and C. H. Papadimitriou. Elements of the Theory of Computation. Prentice Hall (2nd Ed), 1997.\n• S. Arora and B. Barak. Computational Complexity: A Modern Approach. Cambridge University Press, 2009.\nQuantum Computation and Algorithms\n• M. A. Nielsen and I. L. Chuang. Quantum Computation and Quantum Information (10th Anniversary Edition). Cambridge University Press, 2010\n• E. Rieffel and W. Polak. Quantum Computing: A Gentle Introduction. MIT Press, 2011.\n• F. Kaye, R. Laflamme and M. Mosca. An Introduction to Quantum Computing. Oxford University Press, 2007.\n• N. S. Yanofsky and M. A. Mannucci. Quantum Computing for Computer Scientists. Cambridge University Press, 2008.\n• W. Scherer. Mathematics of Quantum Computing. Springer, 2019.\nSome extra references on quantum algorithms NEW\n• N. S. Yanofsky. The Outer Limits of Reason. MIT Press, 2013.\n• S. Aaronson. Quantum Computing since Democritus. Cambridge University Press, 2013.\n\nPragmatics\n\nAssessment\n• FINAL MARKS available here\n• Training assignment (60%): to be discussed on 25 May (with intermediate ckeckpoints)\n• Individual assynchronous test (40%): 2 exercises proposed along the T lectures\n• Problem 1 (16-30 March) (pdf)\n• Problem 2 (6-27 May) (pdf)\n• Problem Extra (pdf)\nContact\n• Appointments - Luis: Wed, 18:00-20:00 and Fri, 18:00-20:00 (please send an email the day before)\n• Appointments - Ana: Wed, 17:00-19:00 (please send an email the day before)\n• Email: lsb at di dot uminho dot pt (Luis) and aicneri at gmail dot com (Ana)\n• Last update: 2021.06.29" ]
[ null ]
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http://www.brightfutura.com/guide-math-section-gre/
[ "", null, "# Guide To Math Section Of The GRE\n\nApplying for the GRE is simple. Studying for the GRE should be as well.\n\nIf you have not signed up for the GRE yet please check out our article on HOW TO APPLY AND REGISTER TO THE GRE\n\nNow that you are scheduled to take the exam lets focus on  the GRE three sections.\n\n• Verbal Reasoning\n• Quantitative Reasoning\n• Analytical Writing\n\nThe Quantitative Reasoning measure of the GRE® revised General Test assesses your:\n\n• basic mathematical skills\n• understanding of elementary mathematical concepts\n• ability to reason quantitatively and to model and solve problems with quantitative methods\n\nPlease note: That Some of the questions in the measure are posed in real-life settings, while others are posed in purely mathematical settings. The skills, concepts and abilities are tested in the four content areas below:\n\n## ARITHMETIC\n\nArithmetic topics include properties and types of integers, such as divisibility, factorization, prime numbers, remainders and odd and even integers; arithmetic operations, exponents and roots; and concepts such as estimation, percent, ratio, rate, absolute value, the number line, decimal representation and sequences of numbers. I have broken these down into the following sections.\n\n1.1 Integers\n1.2 Fractions\n1.3 Exponents and Roots\n1.4 Decimals\n1.5 Real Numbers\n1.6 Ratio\n1.7 Percent\n\n## ALGEBRA\n\nAlgebra topics include operations with exponents; factoring and simplifying algebraic expressions; relations, functions, equations and inequalities; solving linear and quadratic equations and inequalities; solving simultaneous equations and inequalities; setting up equations to solve word problems; and coordinate geometry, including graphs of functions, equations and inequalities, intercepts and slopes of lines.  I have broken these down into the following sections.\n\n2.1 Operations with Algebraic Expressions\n2.2 Rules of Exponents\n2.3 Solving Linear Equations\n2.5 Solving Linear Inequalities\n2.6 Functions\n2.7 Applications\n2.8 Coordinate Geometry\n2.9 Graphs of Functions\n\n## GEOMETRY\n\nGeometry topics include parallel and perpendicular lines, circles, triangles — including isosceles, equilateral and 30°-60°-90° triangles — quadrilaterals, other polygons, congruent and similar figures, three-dimensional figures, area, perimeter, volume, the Pythagorean theorem and angle measurement in degrees. The ability to construct proofs is not tested.  I have broken these down into the following sections.\n\n3.1 Lines and Angles\n3.2 Polygons\n3.3 Triangles\n3.5 Circles\n3.6 Three-Dimensional Figures\n\n## DATA ANALYSIS\n\nData analysis topics include basic descriptive statistics, such as mean, median, mode, range, standard deviation, interquartile range, quartiles and percentiles; interpretation of data in tables and graphs, such as line graphs, bar graphs, circle graphs, boxplots, scatterplots and frequency distributions; elementary probability, such as probabilities of compound events and independent events; random variables and probability distributions, including normal distributions; and counting methods, such as combinations, permutations and Venn diagrams. These topics are typically taught in high school algebra courses or introductory statistics courses. Inferential statistics is not tested.\n\n4.1 Graphical Methods for Describing Data\n4.2 Numerical Methods for Describing Data\n4.3 Counting Methods\n4.4 Probability\n4.5 Distributions of Data, Random Variables, and Probability Distributions\n4.6 Data Interpretation Examples\n\n## Quantitative Reasoning Question Types\n\nThe Quantitative Reasoning measure has four types of questions. Click on the links below to get a closer look at each, including sample questions with rationales.\n\nEach question appears either independently as a discrete question or as part of a set of questions called a Data Interpretation set. All of the questions in a Data Interpretation set are based on the same data presented in tables, graphs or other displays of data.\n\nYou are allowed to use a basic calculator on the Quantitative Reasoning measure. For the computer-based test, the calculator is provided on-screen. For the paper-based test, a handheld calculator is provided at the test center. Read more about using the calculator.\n\n1.", null, "plumbers" ]
[ null, "http://www.brightfutura.com/wp-content/uploads/2014/03/shutterstock_85369759.jpg", null, "http://0.gravatar.com/avatar/415d34e085e404c1e74313f9a290bae5", null ]
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https://stats.stackexchange.com/questions/185491/diagnostics-for-generalized-linear-mixed-models-specifically-residuals
[ "# Diagnostics for generalized linear (mixed) models (specifically residuals)\n\nI am currently struggling with finding the right model for difficult count data (dependent variable). I have tried various different models (mixed effects models are necessary for my kind of data) such as lmer and lme4 (with a log transform) as well as generalized linear mixed effects models with various families such as Gaussian or negative binomial.\n\nHowever, I am quite unsure on how to correctly diagnose the resulting fits. I found a lot of different opinions on that topic on the Web. I think diagnostics on linear (mixed) regression are quite straight-forward. You can go ahead and analyse the residuals (normality) as well as study heteroscedasticity by plotting fitted values compared to residuals.\n\nHowever, how do you properly do that for the generalized version? Let us focus on a negative binomial (mixed) regression for now. I have seen quite opposing statements regarding the residuals here:\n\n1. In Checking residuals for normality in generalised linear models it is pointed out in the first answer that the plain residuals are not normally distributed for a GLM; I think this is clear. However, then it is pointed out that Pearson and deviance residuals are also not supposed to be normal. Yet, the second answer states that deviance residuals should be normally distributed (combined with a reference).\n\n2. That deviance residuals should be normally distributed is hinted at in the documentation for ?glm.diag.plots (from R's boot package), though.\n\n3. In this blog post, the author first studied normality of what I assume are Pearson residuals for a NB mixed-effects regression model. As expected (in my honest opinion) the residuals did not show to be normal and the author assumed this model to be a bad fit. However, as stated in the comments, the residuals should be distributed according to a negative binomial distribution. In my opinion, this comes closest to the truth as GLM residuals can have other distributions than the normal one. Is this correct? How to check for things like heteroscedasticity here?\n\n4. The last point (plotting residuals against quantiles of the estimated distribution) is emphasized in Ben & Yohai (2004). Currently, this seems the way to go for me.\n\nIn a nutshell: How do you properly study the model fits of generalized linear (mixed) regression models specifically with a focus on residuals?\n\n• Residuals for GLMs aren't in general normal (cf here), but note that there are lots of kinds of residuals for GLMs. Eg, glm.diag.plots says it's for jackknifed deviance residual (I suspect that distinction is important). Also, I gather you have count data; you might want to focus on that fact. Eg, counts are supposed (in some sense) to be heteroscedastic. Diagnostic plots for count regression should be helpful for you (although it doesn't address the mixed effects aspect). – gung Dec 9 '15 at 17:18\n• I am familiar with the post you mentioned. However, there is also a statement that suggests that (deviance) residuals should be normal \"we see very large residuals and a substantial deviance of the deviance residuals from the normal (all speaking against the Poisson)\". – fsociety Dec 9 '15 at 18:06\n\n## 2 Answers\n\nThis answer is not based on my knowledge but rather quotes what Bolker et al. (2009) wrote in an influential paper in the journal Trends in Ecology and Evolution. Since the article is not open access (although searching for it on Google scholar may prove successful, I thought I cite important passages that may be helpful to address parts of the questions. So again, it's not what I came up with myself but I think it represents the best condensed information on GLMMs (inlcuding diagnostics) out there in a very straight forward and easy to understand style of writing. If by any means this answer is not suitable for whatever reason, I will simply delete it. Things that I find useful with respect to questions regarding diagnostics are highlighted in bold.\n\nPage 127:\n\nResearchers faced with nonnormal data often try shortcuts such as transforming data to achieve normality and homogeneity of variance, using nonparametric tests or relying on the robustness of classical ANOVA to nonnormality for balanced designs . They might ignore random effects altogether (thus committing pseudoreplication) or treat them as fixed factors . However, such shortcuts can fail (e.g. count data with many zero values cannot be made normal by transformation). Even when they succeed, they might violate statistical assumptions (even nonparametric tests make assumptions, e.g. of homogeneity of variance across groups) or limit the scope of inference (one cannot extrapolate estimates of fixed effects to new groups). Instead of shoehorning their data into classical statistical frameworks, researchers should use statistical approaches that match their data. Generalized linear mixed models (GLMMs) combine the properties of two statistical frameworks that are widely used in ecology and evolution, linear mixed models (which incorporate random effects) and generalized linear models (which handle nonnormal data by using link functions and exponential family [e.g. normal, Poisson or binomial] distributions). GLMMs are the best tool for analyzing nonnormal data that involve random effects: all one has to do, in principle, is specify a distribution, link function and structure of the random effects.\n\nPage 129, Box 1:\n\nThe residuals indicated overdispersion, so we refitted the data with a quasi-Poisson model. Despite the large estimated scale parameter (10.8), exploratory graphs found no evidence of outliers at the level of individuals, genotypes or populations. We used quasi-AIC (QAIC), using one degree of freedom for random effects , for randomeffect and then for fixed-effect model selection.\n\nPage 133, Box 4:\n\nHere we outline a general framework for constructing a full (most complex) model, the first step in GLMM analysis. Following this process, one can then evaluate parameters and compare submodels as described in the main text and in Figure 1.\n\n1. Specify fixed (treatments or covariates) and random effects (experimental, spatial or temporal blocks, individuals, etc.). Include only important interactions. Restrict the model a priori to a feasible level of complexity, based on rules of thumb (>5–6 random-effect levels per random effect and >10–20 samples per treatment level or experimental unit) and knowledge of adequate sample sizes gained from previous studies [64,65].\n\n2. Choose an error distribution and link function (e.g. Poisson distribution and log link for count data, binomial distribution and logit link for proportion data).\n\n3. Graphical checking: are variances of data (transformed by the link function) homogeneous across categories? Are responses of transformed data linear with respect to continuous predictors? Are there outlier individuals or groups? Do distributions within groups match the assumed distribution?\n\n4. Fit fixed-effect GLMs both to the full (pooled) data set and within each level of the random factors [28,50]. Estimated parameters should be approximately normally distributed across groups (group-level parameters can have large uncertainties, especially for groups with small sample sizes). Adjust model as necessary (e.g. change link function or add covariates).\n\n5. Fit the full GLMM. Insufficient computer memory o r too slow: reduce model complexity. If estimation succeeds on a subset of the data, try a more efficient estimation algorithm (e.g. PQL if appropriate). Failure to converge (warnings or errors): reduce model complexity or change optimization settings (make sure the resulting answers make sense). Try other estimation algorithms. Zero variance components or singularity (warnings or errors): check that the model is properly defined and identifiable (i.e. all components can theoretically be estimated). Reduce model complexity. Adding information to the model (additional covariates, or new groupings for random effects) can alleviate problems, as will centering continuous covariates by subtracting their mean . If necessary, eliminate random effects from the full model, dropping (i) terms of less intrinsic biological interest, (ii) terms with very small estimated variances and/or large uncertainty, or (iii) interaction terms. (Convergence errors or zero variances could indicate insufficient data.)\n\n6. Recheck assumptions for the final model (as in step 3) and check that parameter estimates and confidence intervals are reasonable (gigantic confidence intervals could indicate fitting problems). The magnitude of the standardized residuals should be independent of the fitted values. Assess overdispersion (the sum of the squared Pearson residuals should be $\\chi^2$ distributed [66,67]). If necessary, change distributions or estimate a scale parameter. Check that a full model that includes dropped random effects with small standard deviations gives similar results to the final model. If different models lead to substantially different parameter estimates, consider model averaging.\n\nResiduals plots should be used to assess overdispersion and transformed variances should be homogeneous across categories. Nowhere in the article was mentioned that residuals are supposed to be normally distributed.\n\nI think the reason why there are contrasting statements reflects that GLMMs (page 127-128)...\n\n...are surprisingly challenging to use even for statisticians. Although several software packages can handle GLMMs (Table 1), few ecologists and evolutionary biologists are aware of the range of options or of the possible pitfalls. In reviewing papers in ecology and evolution since 2005 found by Google Scholar, 311 out of 537 GLMM analyses (58%) used these tools inappropriately in some way (see online supplementary material).\n\nAnd here are a few full worked examples using GLMMs including diagnostics.\n\nI realize that this answer is more like a comment and should be treated as such. But the comment section doesn't allow me to add such a long comment. Also since I believe this paper is of value for this discussion (but unfortunately behind a pay-wall), I thought it would be useful to quote important passages here.\n\nCited papers:\n\n - G.P. Quinn, M.J. Keough (2002): Experimental Design and Data Analysis for Biologists, Cambridge University Press.\n\n - M.J. Crawley (2002): Statistical Computing: An Introduction to Data Analysis Using S-PLUS, John Wiley & Sons.\n\n - J.C. Pinheiro, D.M. Bates (2000): Mixed-Effects Models in S and S-PLUS, Springer.\n\n - F. Vaida, S. Blanchard (2005): Conditional Akaike information for mixed-effects models. Biometrika, 92, pp. 351–370.\n\n - A. Gelman, J. Hill (2006): Data Analysis Using Regression and Multilevel/Hierarchical Models, Cambridge University Press.\n\n - N.J. Gotelli, A.M. Ellison (2004): A Primer of Ecological Statistics, Sinauer Associates.\n\n - F.J. Harrell (2001): Regression Modeling Strategies, Springer.\n\n - J.K. Lindsey (1997): Applying Generalized Linear Models, Springer.\n\n - W. Venables, B.D. Ripley (2002): Modern Applied Statistics with S, Springer.\n\n• Thanks, that is indeed helpful, I knew about the coding examples of Bolker, but not the actual paper somehow. What I still wonder though is how graphical checking applies to very large-scale data with thousands of groups. The few papers (such as that one) that try give some guidelines on how to properly check your models all only apply to very small-scale data. Then, it is much easier to pick e.g., the groups and visualize something. I really think that a good scientific contribution can be made if someone goes through a more complex example in future. – fsociety Dec 16 '15 at 19:42\n• I'm glad this was useful! I think the presented examples are already quite complex (at least to me). I guess the bigger problem is that larger datasets and more complex models may become computationally infeasible as is mentioned in the text: \"[...] to find ML estimates, one must integrate likelihoods over all possible values of the random effects. For GLMMs this calculation is at best slow, and at worst (e.g. for large numbers of random effects) computationally infeasible.\" What I find amazing though, and what should be kept in mind, is that we are using tools that are under active research! – Stefan Dec 16 '15 at 20:02\n\nThis is an old question, but I thought it would be useful to add that option 4 suggested by the OP is now available in the DHARMa R package (available from CRAN, see here).\n\nThe package makes the visual residual checks suggested by the accepted answer a lot more reliable / easy.\n\nFrom the package description:\n\nThe DHARMa package uses a simulation-based approach to create readily interpretable scaled residuals from fitted generalized linear mixed models. Currently supported are all 'merMod' classes from 'lme4' ('lmerMod', 'glmerMod'), 'glm' (including 'negbin' from 'MASS', but excluding quasi-distributions) and 'lm' model classes. Alternatively, externally created simulations, e.g. posterior predictive simulations from Bayesian software such as 'JAGS', 'STAN', or 'BUGS' can be processed as well. The resulting residuals are standardized to values between 0 and 1 and can be interpreted as intuitively as residuals from a linear regression. The package also provides a number of plot and test functions for typical model mispecification problem, such as over/underdispersion, zero-inflation, and spatial / temporal autocorrelation.\n\n• Very good addition to this thread! – Stefan Feb 15 '17 at 21:05" ]
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http://www.numbersaplenty.com/21180
[ "Search a number\nBaseRepresentation\nbin101001010111100\n31002001110\n411022330\n51134210\n6242020\n7115515\noct51274\n932043\n1021180\n1114a05\n1210310\n139843\n147a0c\n156420\nhex52bc\n\n21180 has 24 divisors (see below), whose sum is σ = 59472. Its totient is φ = 5632.\n\nThe previous prime is 21179. The next prime is 21187. The reversal of 21180 is 8112.\n\nAdding to 21180 its reverse (8112), we get a palindrome (29292).\n\nIt is a happy number.\n\n21180 is digitally balanced in base 4, because in such base it contains all the possibile digits an equal number of times.\n\nIt is a Harshad number since it is a multiple of its sum of digits (12).\n\nIt is a nialpdrome in base 13 and base 15.\n\nIt is a congruent number.\n\nIt is not an unprimeable number, because it can be changed into a prime (21187) by changing a digit.\n\nIt is a polite number, since it can be written in 7 ways as a sum of consecutive naturals, for example, 117 + ... + 236.\n\nIt is an arithmetic number, because the mean of its divisors is an integer number (2478).\n\n221180 is an apocalyptic number.\n\n21180 is a gapful number since it is divisible by the number (20) formed by its first and last digit.\n\nIt is an amenable number.\n\n21180 is an abundant number, since it is smaller than the sum of its proper divisors (38292).\n\nIt is a pseudoperfect number, because it is the sum of a subset of its proper divisors.\n\nIt is a Zumkeller number, because its divisors can be partitioned in two sets with the same sum (29736).\n\n21180 is a wasteful number, since it uses less digits than its factorization.\n\n21180 is an evil number, because the sum of its binary digits is even.\n\nThe sum of its prime factors is 365 (or 363 counting only the distinct ones).\n\nThe product of its (nonzero) digits is 16, while the sum is 12.\n\nThe square root of 21180 is about 145.5335012978. The cubic root of 21180 is about 27.6678440169.\n\nThe spelling of 21180 in words is \"twenty-one thousand, one hundred eighty\"." ]
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https://www.downloadtyphoon.com/downloads/mathematical-equation
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DesktopCalc uses Advanced DAL (Dynamic Algebraic Logic) ... features include the following: * Possibility to enter mathematical formulas as with a keyboard as with built-in ... - minimal positive number: 2.225E-308 * All functions, mathematical and physical constants can also be used in .... Free download of Desktop Calculator - DesktopCalc 2.1.22\n\n## mathematical equation web results\n\n``` SERVER:array(44) {\n[\"REDIRECT_UNIQUE_ID\"]=>\nstring(27) \"Xv-ZY3AM5Vk9PHBgckQpoAAAAAA\"\n[\"REDIRECT_SCRIPT_URL\"]=>\n[\"REDIRECT_SCRIPT_URI\"]=>\n[\"REDIRECT_PERL5LIB\"]=>\nstring(49) \"/usr/share/awstats/lib:/usr/share/awstats/plugins\"\n[\"REDIRECT_HTTPS\"]=>\nstring(2) \"on\"\n[\"REDIRECT_SSL_TLS_SNI\"]=>\n[\"REDIRECT_STATUS\"]=>\nstring(3) \"200\"\n[\"UNIQUE_ID\"]=>\nstring(27) \"Xv-ZY3AM5Vk9PHBgckQpoAAAAAA\"\n[\"SCRIPT_URL\"]=>\n[\"SCRIPT_URI\"]=>\n[\"PERL5LIB\"]=>\nstring(49) \"/usr/share/awstats/lib:/usr/share/awstats/plugins\"\n[\"HTTPS\"]=>\nstring(2) \"on\"\n[\"SSL_TLS_SNI\"]=>\n[\"HTTP_USER_AGENT\"]=>\nstring(40) \"CCBot/2.0 (https://commoncrawl.org/faq/)\"\n[\"HTTP_ACCEPT\"]=>\nstring(63) \"text/html,application/xhtml+xml,application/xml;q=0.9,*/*;q=0.8\"\n[\"HTTP_ACCEPT_LANGUAGE\"]=>\nstring(14) \"en-US,en;q=0.5\"\n[\"HTTP_ACCEPT_ENCODING\"]=>\nstring(7) \"br,gzip\"\n[\"HTTP_HOST\"]=>\n[\"HTTP_CONNECTION\"]=>\nstring(10) \"Keep-Alive\"\n[\"PATH\"]=>\nstring(49) \"/usr/local/sbin:/usr/local/bin:/usr/sbin:/usr/bin\"\n[\"SERVER_SIGNATURE\"]=>\nstring(0) \"\"\n[\"SERVER_SOFTWARE\"]=>\nstring(52) \"Apache/2.4.6 (CentOS) OpenSSL/1.0.2k-fips PHP/5.4.16\"\n[\"SERVER_NAME\"]=>\nstring(11) \"45.55.49.28\"\n[\"SERVER_PORT\"]=>\nstring(3) \"443\"\nstring(13) \"34.231.21.160\"\n[\"DOCUMENT_ROOT\"]=>\n[\"REQUEST_SCHEME\"]=>\nstring(5) \"https\"\n[\"CONTEXT_PREFIX\"]=>\nstring(0) \"\"\n[\"CONTEXT_DOCUMENT_ROOT\"]=>\n[\"SCRIPT_FILENAME\"]=>\n[\"REMOTE_PORT\"]=>\nstring(5) \"50004\"\n[\"REDIRECT_QUERY_STRING\"]=>\nstring(38) \"keywords_encoded=mathematical-equation\"\n[\"REDIRECT_URL\"]=>\n[\"GATEWAY_INTERFACE\"]=>\nstring(7) \"CGI/1.1\"\n[\"SERVER_PROTOCOL\"]=>\nstring(8) \"HTTP/1.1\"\n[\"REQUEST_METHOD\"]=>\nstring(3) \"GET\"\n[\"QUERY_STRING\"]=>\nstring(38) \"keywords_encoded=mathematical-equation\"\n[\"REQUEST_URI\"]=>\n[\"SCRIPT_NAME\"]=>\nstring(21) \"/software-search.html\"\n[\"PHP_SELF\"]=>\nstring(21) \"/software-search.html\"\n[\"REQUEST_TIME_FLOAT\"]=>\nfloat(1593825635.268)\n[\"REQUEST_TIME\"]=>\nint(1593825635)\n}\n```\n\n``` SERVER:array(44) {\n[\"REDIRECT_UNIQUE_ID\"]=>\nstring(27) \"Xv-ZY3AM5Vk9PHBgckQpoAAAAAA\"\n[\"REDIRECT_SCRIPT_URL\"]=>\n[\"REDIRECT_SCRIPT_URI\"]=>\n[\"REDIRECT_PERL5LIB\"]=>\nstring(49) \"/usr/share/awstats/lib:/usr/share/awstats/plugins\"\n[\"REDIRECT_HTTPS\"]=>\nstring(2) \"on\"\n[\"REDIRECT_SSL_TLS_SNI\"]=>\n[\"REDIRECT_STATUS\"]=>\nstring(3) \"200\"\n[\"UNIQUE_ID\"]=>\nstring(27) \"Xv-ZY3AM5Vk9PHBgckQpoAAAAAA\"\n[\"SCRIPT_URL\"]=>\n[\"SCRIPT_URI\"]=>\n[\"PERL5LIB\"]=>\nstring(49) \"/usr/share/awstats/lib:/usr/share/awstats/plugins\"\n[\"HTTPS\"]=>\nstring(2) \"on\"\n[\"SSL_TLS_SNI\"]=>\n[\"HTTP_USER_AGENT\"]=>\nstring(40) \"CCBot/2.0 (https://commoncrawl.org/faq/)\"\n[\"HTTP_ACCEPT\"]=>\nstring(63) \"text/html,application/xhtml+xml,application/xml;q=0.9,*/*;q=0.8\"\n[\"HTTP_ACCEPT_LANGUAGE\"]=>\nstring(14) \"en-US,en;q=0.5\"\n[\"HTTP_ACCEPT_ENCODING\"]=>\nstring(7) \"br,gzip\"\n[\"HTTP_HOST\"]=>\n[\"HTTP_CONNECTION\"]=>\nstring(10) \"Keep-Alive\"\n[\"PATH\"]=>\nstring(49) \"/usr/local/sbin:/usr/local/bin:/usr/sbin:/usr/bin\"\n[\"SERVER_SIGNATURE\"]=>\nstring(0) \"\"\n[\"SERVER_SOFTWARE\"]=>\nstring(52) \"Apache/2.4.6 (CentOS) OpenSSL/1.0.2k-fips PHP/5.4.16\"\n[\"SERVER_NAME\"]=>\nstring(11) \"45.55.49.28\"\n[\"SERVER_PORT\"]=>\nstring(3) \"443\"\nstring(13) \"34.231.21.160\"\n[\"DOCUMENT_ROOT\"]=>\n[\"REQUEST_SCHEME\"]=>\nstring(5) \"https\"\n[\"CONTEXT_PREFIX\"]=>\nstring(0) \"\"\n[\"CONTEXT_DOCUMENT_ROOT\"]=>\n[\"SCRIPT_FILENAME\"]=>\n[\"REMOTE_PORT\"]=>\nstring(5) \"50004\"\n[\"REDIRECT_QUERY_STRING\"]=>\nstring(38) \"keywords_encoded=mathematical-equation\"\n[\"REDIRECT_URL\"]=>\n[\"GATEWAY_INTERFACE\"]=>\nstring(7) \"CGI/1.1\"\n[\"SERVER_PROTOCOL\"]=>\nstring(8) \"HTTP/1.1\"\n[\"REQUEST_METHOD\"]=>\nstring(3) \"GET\"\n[\"QUERY_STRING\"]=>\nstring(38) \"keywords_encoded=mathematical-equation\"\n[\"REQUEST_URI\"]=>\n[\"SCRIPT_NAME\"]=>\nstring(21) \"/software-search.html\"\n[\"PHP_SELF\"]=>\nstring(21) \"/software-search.html\"\n[\"REQUEST_TIME_FLOAT\"]=>\nfloat(1593825635.268)\n[\"REQUEST_TIME\"]=>\nint(1593825635)\n}\n```\n``` SERVER:array(44) {\n[\"REDIRECT_UNIQUE_ID\"]=>\nstring(27) \"Xv-ZY3AM5Vk9PHBgckQpoAAAAAA\"\n[\"REDIRECT_SCRIPT_URL\"]=>\n[\"REDIRECT_SCRIPT_URI\"]=>\n[\"REDIRECT_PERL5LIB\"]=>\nstring(49) \"/usr/share/awstats/lib:/usr/share/awstats/plugins\"\n[\"REDIRECT_HTTPS\"]=>\nstring(2) \"on\"\n[\"REDIRECT_SSL_TLS_SNI\"]=>\n[\"REDIRECT_STATUS\"]=>\nstring(3) \"200\"\n[\"UNIQUE_ID\"]=>\nstring(27) \"Xv-ZY3AM5Vk9PHBgckQpoAAAAAA\"\n[\"SCRIPT_URL\"]=>\n[\"SCRIPT_URI\"]=>\n[\"PERL5LIB\"]=>\nstring(49) \"/usr/share/awstats/lib:/usr/share/awstats/plugins\"\n[\"HTTPS\"]=>\nstring(2) \"on\"\n[\"SSL_TLS_SNI\"]=>\n[\"HTTP_USER_AGENT\"]=>\nstring(40) \"CCBot/2.0 (https://commoncrawl.org/faq/)\"\n[\"HTTP_ACCEPT\"]=>\nstring(63) \"text/html,application/xhtml+xml,application/xml;q=0.9,*/*;q=0.8\"\n[\"HTTP_ACCEPT_LANGUAGE\"]=>\nstring(14) \"en-US,en;q=0.5\"\n[\"HTTP_ACCEPT_ENCODING\"]=>\nstring(7) \"br,gzip\"\n[\"HTTP_HOST\"]=>\n[\"HTTP_CONNECTION\"]=>\nstring(10) \"Keep-Alive\"\n[\"PATH\"]=>\nstring(49) \"/usr/local/sbin:/usr/local/bin:/usr/sbin:/usr/bin\"\n[\"SERVER_SIGNATURE\"]=>\nstring(0) \"\"\n[\"SERVER_SOFTWARE\"]=>\nstring(52) \"Apache/2.4.6 (CentOS) OpenSSL/1.0.2k-fips PHP/5.4.16\"\n[\"SERVER_NAME\"]=>\nstring(11) \"45.55.49.28\"\n[\"SERVER_PORT\"]=>\nstring(3) \"443\"\nstring(13) \"34.231.21.160\"\n[\"DOCUMENT_ROOT\"]=>\n[\"REQUEST_SCHEME\"]=>\nstring(5) \"https\"\n[\"CONTEXT_PREFIX\"]=>\nstring(0) \"\"\n[\"CONTEXT_DOCUMENT_ROOT\"]=>\n[\"SCRIPT_FILENAME\"]=>\n[\"REMOTE_PORT\"]=>\nstring(5) \"50004\"\n[\"REDIRECT_QUERY_STRING\"]=>\nstring(38) \"keywords_encoded=mathematical-equation\"\n[\"REDIRECT_URL\"]=>\n[\"GATEWAY_INTERFACE\"]=>\nstring(7) \"CGI/1.1\"\n[\"SERVER_PROTOCOL\"]=>\nstring(8) \"HTTP/1.1\"\n[\"REQUEST_METHOD\"]=>\nstring(3) \"GET\"\n[\"QUERY_STRING\"]=>\nstring(38) \"keywords_encoded=mathematical-equation\"\n[\"REQUEST_URI\"]=>\n[\"SCRIPT_NAME\"]=>\nstring(21) \"/software-search.html\"\n[\"PHP_SELF\"]=>\nstring(21) \"/software-search.html\"\n[\"REQUEST_TIME_FLOAT\"]=>\nfloat(1593825635.268)\n[\"REQUEST_TIME\"]=>\nint(1593825635)\n}\n```\n``` SERVER:array(44) {\n[\"REDIRECT_UNIQUE_ID\"]=>\nstring(27) \"Xv-ZY3AM5Vk9PHBgckQpoAAAAAA\"\n[\"REDIRECT_SCRIPT_URL\"]=>\n[\"REDIRECT_SCRIPT_URI\"]=>\n[\"REDIRECT_PERL5LIB\"]=>\nstring(49) \"/usr/share/awstats/lib:/usr/share/awstats/plugins\"\n[\"REDIRECT_HTTPS\"]=>\nstring(2) \"on\"\n[\"REDIRECT_SSL_TLS_SNI\"]=>\n[\"REDIRECT_STATUS\"]=>\nstring(3) \"200\"\n[\"UNIQUE_ID\"]=>\nstring(27) \"Xv-ZY3AM5Vk9PHBgckQpoAAAAAA\"\n[\"SCRIPT_URL\"]=>\n[\"SCRIPT_URI\"]=>\n[\"PERL5LIB\"]=>\nstring(49) \"/usr/share/awstats/lib:/usr/share/awstats/plugins\"\n[\"HTTPS\"]=>\nstring(2) \"on\"\n[\"SSL_TLS_SNI\"]=>\n[\"HTTP_USER_AGENT\"]=>\nstring(40) \"CCBot/2.0 (https://commoncrawl.org/faq/)\"\n[\"HTTP_ACCEPT\"]=>\nstring(63) \"text/html,application/xhtml+xml,application/xml;q=0.9,*/*;q=0.8\"\n[\"HTTP_ACCEPT_LANGUAGE\"]=>\nstring(14) \"en-US,en;q=0.5\"\n[\"HTTP_ACCEPT_ENCODING\"]=>\nstring(7) \"br,gzip\"\n[\"HTTP_HOST\"]=>\n[\"HTTP_CONNECTION\"]=>\nstring(10) \"Keep-Alive\"\n[\"PATH\"]=>\nstring(49) \"/usr/local/sbin:/usr/local/bin:/usr/sbin:/usr/bin\"\n[\"SERVER_SIGNATURE\"]=>\nstring(0) \"\"\n[\"SERVER_SOFTWARE\"]=>\nstring(52) \"Apache/2.4.6 (CentOS) OpenSSL/1.0.2k-fips PHP/5.4.16\"\n[\"SERVER_NAME\"]=>\nstring(11) \"45.55.49.28\"\n[\"SERVER_PORT\"]=>\nstring(3) \"443\"\nstring(13) \"34.231.21.160\"\n[\"DOCUMENT_ROOT\"]=>\n[\"REQUEST_SCHEME\"]=>\nstring(5) \"https\"\n[\"CONTEXT_PREFIX\"]=>\nstring(0) \"\"\n[\"CONTEXT_DOCUMENT_ROOT\"]=>\n[\"SCRIPT_FILENAME\"]=>\n[\"REMOTE_PORT\"]=>\nstring(5) \"50004\"\n[\"REDIRECT_QUERY_STRING\"]=>\nstring(38) \"keywords_encoded=mathematical-equation\"\n[\"REDIRECT_URL\"]=>\n[\"GATEWAY_INTERFACE\"]=>\nstring(7) \"CGI/1.1\"\n[\"SERVER_PROTOCOL\"]=>\nstring(8) \"HTTP/1.1\"\n[\"REQUEST_METHOD\"]=>\nstring(3) \"GET\"\n[\"QUERY_STRING\"]=>\nstring(38) \"keywords_encoded=mathematical-equation\"\n[\"REQUEST_URI\"]=>\n[\"SCRIPT_NAME\"]=>\nstring(21) \"/software-search.html\"\n[\"PHP_SELF\"]=>\nstring(21) \"/software-search.html\"\n[\"REQUEST_TIME_FLOAT\"]=>\nfloat(1593825635.268)\n[\"REQUEST_TIME\"]=>\nint(1593825635)\n}\n```\n``` SERVER:array(44) {\n[\"REDIRECT_UNIQUE_ID\"]=>\nstring(27) \"Xv-ZY3AM5Vk9PHBgckQpoAAAAAA\"\n[\"REDIRECT_SCRIPT_URL\"]=>\n[\"REDIRECT_SCRIPT_URI\"]=>\n[\"REDIRECT_PERL5LIB\"]=>\nstring(49) \"/usr/share/awstats/lib:/usr/share/awstats/plugins\"\n[\"REDIRECT_HTTPS\"]=>\nstring(2) \"on\"\n[\"REDIRECT_SSL_TLS_SNI\"]=>\n[\"REDIRECT_STATUS\"]=>\nstring(3) \"200\"\n[\"UNIQUE_ID\"]=>\nstring(27) \"Xv-ZY3AM5Vk9PHBgckQpoAAAAAA\"\n[\"SCRIPT_URL\"]=>\n[\"SCRIPT_URI\"]=>\n[\"PERL5LIB\"]=>\nstring(49) \"/usr/share/awstats/lib:/usr/share/awstats/plugins\"\n[\"HTTPS\"]=>\nstring(2) \"on\"\n[\"SSL_TLS_SNI\"]=>\n[\"HTTP_USER_AGENT\"]=>\nstring(40) \"CCBot/2.0 (https://commoncrawl.org/faq/)\"\n[\"HTTP_ACCEPT\"]=>\nstring(63) \"text/html,application/xhtml+xml,application/xml;q=0.9,*/*;q=0.8\"\n[\"HTTP_ACCEPT_LANGUAGE\"]=>\nstring(14) \"en-US,en;q=0.5\"\n[\"HTTP_ACCEPT_ENCODING\"]=>\nstring(7) \"br,gzip\"\n[\"HTTP_HOST\"]=>\n[\"HTTP_CONNECTION\"]=>\nstring(10) \"Keep-Alive\"\n[\"PATH\"]=>\nstring(49) \"/usr/local/sbin:/usr/local/bin:/usr/sbin:/usr/bin\"\n[\"SERVER_SIGNATURE\"]=>\nstring(0) \"\"\n[\"SERVER_SOFTWARE\"]=>\nstring(52) \"Apache/2.4.6 (CentOS) OpenSSL/1.0.2k-fips PHP/5.4.16\"\n[\"SERVER_NAME\"]=>\nstring(11) \"45.55.49.28\"\n[\"SERVER_PORT\"]=>\nstring(3) \"443\"\nstring(13) \"34.231.21.160\"\n[\"DOCUMENT_ROOT\"]=>\n[\"REQUEST_SCHEME\"]=>\nstring(5) \"https\"\n[\"CONTEXT_PREFIX\"]=>\nstring(0) \"\"\n[\"CONTEXT_DOCUMENT_ROOT\"]=>\n[\"SCRIPT_FILENAME\"]=>\n[\"REMOTE_PORT\"]=>\nstring(5) \"50004\"\n[\"REDIRECT_QUERY_STRING\"]=>\nstring(38) \"keywords_encoded=mathematical-equation\"\n[\"REDIRECT_URL\"]=>\n[\"GATEWAY_INTERFACE\"]=>\nstring(7) \"CGI/1.1\"\n[\"SERVER_PROTOCOL\"]=>\nstring(8) \"HTTP/1.1\"\n[\"REQUEST_METHOD\"]=>\nstring(3) \"GET\"\n[\"QUERY_STRING\"]=>\nstring(38) \"keywords_encoded=mathematical-equation\"\n[\"REQUEST_URI\"]=>" ]
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https://origin.geeksforgeeks.org/athenahealth-interview-experience-on-campus/
[ "", null, "GFG App\nOpen App", null, "Browser\nContinue\n\n# AthenaHealth Interview Experience (On – Campus)\n\nRound 1: Hakerrank – 12 Questions – 90 mins\n\n10 MCQ: Based on core subjects like OS, CN, and OOPS concepts. Also, Code related questions to predict the output of the given code.\n\n2 Coding Questions:\n\n1. Profit Target: Given an array of n elements where each element gives the yearly profit of a corresponding stock, find the max number of distinct pairs (pairs differing in at least one element) from the array that adds up to the given profit target.\n\nSample Input 1:\n\n```[1,3,46,1,3,9] , sum = 47\npossible pairs are: (1,46), (46,1), (46,1), (1,46)\nindexes: \n- four times due to repetition of '1'\n- return only once - (46,1)\nHence, output = 1```\n\nSample Input 2:\n\n```[5,7,9,13,11,6,6,3,3] sum = 12\npossible pairs are: (5,7), (7,5), (9,3),\n(9,3), (3,9), (9,3),\n(6,6), (6,6)\nindexes: \n \nreturn only distinct - (5,7), (9,3), (6,6)\nHence, output = 3```\n2. Simple Max Difference: Given an array of size n where elements are closing prices of a particular stock on n days in order, find the maximum profit spread of the stock. Profit spread it the difference between the closing price of a day and the closing price on any of the previous days in history. If the prices remain flat or are continuously decreasing, return -1.\n\nSample input 1:\n\n```[7,1,2,5]\n1<7 -> continue;\n2>1 -> 2-1 = 1 : diff\n5>2 -> 5-2 = 3\n5-1 = 4 : maximum diff = output```\n\nSample Input 2:\n\n```[7,5,2,1]\n5<7 , 2<5 , 1<2 -> continuously decreasing : return -1;```\n\nRound 2: Technical Interview on Hakerrank CodePair – 60 mins\n\n1. Based on projects – Blockchain\n\n• What is blockchain?\n• How is it useful?\n• How does it ensure data confidentiality and integrity\n• Explain its working.\n2. Based on projects – MEAN Stack\n\n• What did you do?\n• What is mongo?\n• What do you know about nonstructural databases?\n3. Based on programming languages – C, C++, Java\n\n• What is the difference between C, C++, and Java?\n• What are object-oriented and procedural languages?\n•  Is java a true object-oriented language? Is C++? Explain.\n•  If yes, then how does java use primitive data types like int and char?\n•  What is the difference between Integer Class and int data type?\n•  For particular application development, how would you choose between C++ and Java\n• What constraints would you focus on for the selection?\n• What are pointers and how is the memory allocated for them?\n• What is the problem with pointers – why were they removed when java was built?\n• What are the Object-oriented concepts?\n• Explain the difference between Encapsulation and Abstraction\n• What is Inheritance?\n• What are the types of inheritance?\n• Do we need to explicitly call the parent class constructor from the child class constructor?\n• Does C++ support all types of inheritance? Does Java support all?\n• How are multiple inheritances handled in C++?" ]
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https://www.colorhexa.com/86a3a6
[ "# #86a3a6 Color Information\n\nIn a RGB color space, hex #86a3a6 is composed of 52.5% red, 63.9% green and 65.1% blue. Whereas in a CMYK color space, it is composed of 19.3% cyan, 1.8% magenta, 0% yellow and 34.9% black. It has a hue angle of 185.6 degrees, a saturation of 15.2% and a lightness of 58.8%. #86a3a6 color hex could be obtained by blending #ffffff with #0d474d. Closest websafe color is: #999999.\n\n• R 53\n• G 64\n• B 65\nRGB color chart\n• C 19\n• M 2\n• Y 0\n• K 35\nCMYK color chart\n\n#86a3a6 color description : Dark grayish cyan.\n\n# #86a3a6 Color Conversion\n\nThe hexadecimal color #86a3a6 has RGB values of R:134, G:163, B:166 and CMYK values of C:0.19, M:0.02, Y:0, K:0.35. Its decimal value is 8823718.\n\nHex triplet RGB Decimal 86a3a6 `#86a3a6` 134, 163, 166 `rgb(134,163,166)` 52.5, 63.9, 65.1 `rgb(52.5%,63.9%,65.1%)` 19, 2, 0, 35 185.6°, 15.2, 58.8 `hsl(185.6,15.2%,58.8%)` 185.6°, 19.3, 65.1 999999 `#999999`\nCIE-LAB 64.975, -9.316, -4.893 29.81, 34.015, 41.069 0.284, 0.324, 34.015 64.975, 10.523, 207.712 64.975, -15.252, -5.712 58.322, -10.829, -0.925 10000110, 10100011, 10100110\n\n# Color Schemes with #86a3a6\n\n• #86a3a6\n``#86a3a6` `rgb(134,163,166)``\n• #a68986\n``#a68986` `rgb(166,137,134)``\nComplementary Color\n• #86a699\n``#86a699` `rgb(134,166,153)``\n• #86a3a6\n``#86a3a6` `rgb(134,163,166)``\n• #8693a6\n``#8693a6` `rgb(134,147,166)``\nAnalogous Color\n• #a69986\n``#a69986` `rgb(166,153,134)``\n• #86a3a6\n``#86a3a6` `rgb(134,163,166)``\n• #a68693\n``#a68693` `rgb(166,134,147)``\nSplit Complementary Color\n• #a3a686\n``#a3a686` `rgb(163,166,134)``\n• #86a3a6\n``#86a3a6` `rgb(134,163,166)``\n• #a686a3\n``#a686a3` `rgb(166,134,163)``\n• #86a689\n``#86a689` `rgb(134,166,137)``\n• #86a3a6\n``#86a3a6` `rgb(134,163,166)``\n• #a686a3\n``#a686a3` `rgb(166,134,163)``\n• #a68986\n``#a68986` `rgb(166,137,134)``\n• #5f7e81\n``#5f7e81` `rgb(95,126,129)``\n• #6a8c8f\n``#6a8c8f` `rgb(106,140,143)``\n• #77989b\n``#77989b` `rgb(119,152,155)``\n• #86a3a6\n``#86a3a6` `rgb(134,163,166)``\n• #95aeb1\n``#95aeb1` `rgb(149,174,177)``\n• #a3b9bc\n``#a3b9bc` `rgb(163,185,188)``\n• #b2c5c6\n``#b2c5c6` `rgb(178,197,198)``\nMonochromatic Color\n\n# Alternatives to #86a3a6\n\nBelow, you can see some colors close to #86a3a6. Having a set of related colors can be useful if you need an inspirational alternative to your original color choice.\n\n• #86a6a1\n``#86a6a1` `rgb(134,166,161)``\n• #86a6a4\n``#86a6a4` `rgb(134,166,164)``\n• #86a6a6\n``#86a6a6` `rgb(134,166,166)``\n• #86a3a6\n``#86a3a6` `rgb(134,163,166)``\n• #86a0a6\n``#86a0a6` `rgb(134,160,166)``\n• #869ea6\n``#869ea6` `rgb(134,158,166)``\n• #869ba6\n``#869ba6` `rgb(134,155,166)``\nSimilar Colors\n\n# #86a3a6 Preview\n\nThis text has a font color of #86a3a6.\n\n``<span style=\"color:#86a3a6;\">Text here</span>``\n#86a3a6 background color\n\nThis paragraph has a background color of #86a3a6.\n\n``<p style=\"background-color:#86a3a6;\">Content here</p>``\n#86a3a6 border color\n\nThis element has a border color of #86a3a6.\n\n``<div style=\"border:1px solid #86a3a6;\">Content here</div>``\nCSS codes\n``.text {color:#86a3a6;}``\n``.background {background-color:#86a3a6;}``\n``.border {border:1px solid #86a3a6;}``\n\n# Shades and Tints of #86a3a6\n\nA shade is achieved by adding black to any pure hue, while a tint is created by mixing white to any pure color. In this example, #020303 is the darkest color, while #f7f9f9 is the lightest one.\n\n• #020303\n``#020303` `rgb(2,3,3)``\n• #0b0e0f\n``#0b0e0f` `rgb(11,14,15)``\n• #13191a\n``#13191a` `rgb(19,25,26)``\n• #1b2425\n``#1b2425` `rgb(27,36,37)``\n• #242f31\n``#242f31` `rgb(36,47,49)``\n• #2c3a3c\n``#2c3a3c` `rgb(44,58,60)``\n• #344547\n``#344547` `rgb(52,69,71)``\n• #3d5052\n``#3d5052` `rgb(61,80,82)``\n• #455b5e\n``#455b5e` `rgb(69,91,94)``\n• #4d6669\n``#4d6669` `rgb(77,102,105)``\n• #567174\n``#567174` `rgb(86,113,116)``\n• #5e7c80\n``#5e7c80` `rgb(94,124,128)``\n• #66888b\n``#66888b` `rgb(102,136,139)``\n• #6f9295\n``#6f9295` `rgb(111,146,149)``\n• #7b9a9e\n``#7b9a9e` `rgb(123,154,158)``\n• #86a3a6\n``#86a3a6` `rgb(134,163,166)``\n• #91acae\n``#91acae` `rgb(145,172,174)``\n• #9db4b7\n``#9db4b7` `rgb(157,180,183)``\n• #a8bdbf\n``#a8bdbf` `rgb(168,189,191)``\n• #b3c5c7\n``#b3c5c7` `rgb(179,197,199)``\n• #bfced0\n``#bfced0` `rgb(191,206,208)``\n``#cad7d8` `rgb(202,215,216)``\n• #d5dfe0\n``#d5dfe0` `rgb(213,223,224)``\n• #e0e8e9\n``#e0e8e9` `rgb(224,232,233)``\n• #ecf0f1\n``#ecf0f1` `rgb(236,240,241)``\n• #f7f9f9\n``#f7f9f9` `rgb(247,249,249)``\nTint Color Variation\n\n# Tones of #86a3a6\n\nA tone is produced by adding gray to any pure hue. In this case, #8e9c9e is the less saturated color, while #2debff is the most saturated one.\n\n• #8e9c9e\n``#8e9c9e` `rgb(142,156,158)``\n• #86a3a6\n``#86a3a6` `rgb(134,163,166)``\n• #7eaaae\n``#7eaaae` `rgb(126,170,174)``\n• #76b0b6\n``#76b0b6` `rgb(118,176,182)``\n• #6eb7be\n``#6eb7be` `rgb(110,183,190)``\n• #66bdc6\n``#66bdc6` `rgb(102,189,198)``\n• #5ec4ce\n``#5ec4ce` `rgb(94,196,206)``\n``#56cad6` `rgb(86,202,214)``\n• #4dd1df\n``#4dd1df` `rgb(77,209,223)``\n• #45d8e7\n``#45d8e7` `rgb(69,216,231)``\n• #3ddeef\n``#3ddeef` `rgb(61,222,239)``\n• #35e5f7\n``#35e5f7` `rgb(53,229,247)``\n• #2debff\n``#2debff` `rgb(45,235,255)``\nTone Color Variation\n\n# Color Blindness Simulator\n\nBelow, you can see how #86a3a6 is perceived by people affected by a color vision deficiency. This can be useful if you need to ensure your color combinations are accessible to color-blind users.\n\nMonochromacy\n• Achromatopsia 0.005% of the population\n• Atypical Achromatopsia 0.001% of the population\nDichromacy\n• Protanopia 1% of men\n• Deuteranopia 1% of men\n• Tritanopia 0.001% of the population\nTrichromacy\n• Protanomaly 1% of men, 0.01% of women\n• Deuteranomaly 6% of men, 0.4% of women\n• Tritanomaly 0.01% of the population" ]
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