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https://handwiki.org/wiki/Physics:Giant_magnetoresistance | [
"# Physics:Giant magnetoresistance\n\nGiant magnetoresistance (GMR) is a quantum mechanical magnetoresistance effect observed in multilayers composed of alternating ferromagnetic and non-magnetic conductive layers. The 2007 Nobel Prize in Physics was awarded to Albert Fert and Peter Grünberg for the discovery of GMR.\n\nThe effect is observed as a significant change in the electrical resistance depending on whether the magnetization of adjacent ferromagnetic layers are in a parallel or an antiparallel alignment. The overall resistance is relatively low for parallel alignment and relatively high for antiparallel alignment. The magnetization direction can be controlled, for example, by applying an external magnetic field. The effect is based on the dependence of electron scattering on the spin orientation.\n\nThe main application of GMR is magnetic field sensors, which are used to read data in hard disk drives, biosensors, microelectromechanical systems (MEMS) and other devices. GMR multilayer structures are also used in magnetoresistive random-access memory (MRAM) as cells that store one bit of information.\n\nIn literature, the term giant magnetoresistance is sometimes confused with colossal magnetoresistance of ferromagnetic and antiferromagnetic semiconductors, which is not related to the multilayer structure.",
null,
"The founding results of Albert Fert and Peter Grünberg (1988): change in the resistance of Fe/Cr superlattices at 4.2 K in external magnetic field H. The current and magnetic field were parallel to the axis. The arrow to the right shows maximum resistance change. Hs is saturation field.[note 1]\n\n## Formulation\n\nMagnetoresistance is the dependence of the electrical resistance of a sample on the strength of an external magnetic field. Numerically, it is characterized by the value\n\n$\\displaystyle{ \\delta_H = \\frac{R(H)-R(0)}{R(0)} }$\n\nwhere R(H) is the resistance of the sample in a magnetic field H, and R(0) corresponds to H = 0. Alternative forms of this expression may use electrical resistivity instead of resistance, a different sign for δH, and are sometimes normalized by R(H) rather than R(0).\n\nThe term \"giant magnetoresistance\" indicates that the value δH for multilayer structures significantly exceeds the anisotropic magnetoresistance, which has a typical value within a few percent.\n\n## History\n\nGMR was discovered in 1988 independently by the groups of Albert Fert of the University of Paris-Sud, France, and Peter Grünberg of Forschungszentrum Jülich, Germany. The practical significance of this experimental discovery was recognized by the Nobel Prize in Physics awarded to Fert and Grünberg in 2007.\n\n### Early steps\n\nThe first mathematical model describing the effect of magnetization on the mobility of charge carriers in solids, related to the spin of those carriers, was reported in 1936. Experimental evidence of the potential enhancement of δH has been known since the 1960s. By the late 1980s, the anisotropic magnetoresistance had been well explored, but the corresponding value of δH did not exceed a few percent. The enhancement of δH became possible with the advent of sample preparation techniques such as molecular beam epitaxy, which allows manufacturing multilayer thin films with a thickness of several nanometers.\n\n## Experiment and its interpretation\n\nFert and Grünberg studied electrical resistance of structures incorporating ferromagnetic and non-ferromagnetic materials. In particular, Fert worked on multilayer films, and Grünberg in 1986 discovered the antiferromagnetic exchange interaction in Fe/Cr films.\n\nThe GMR discovery work was carried out by the two groups on slightly different samples. The Fert group used (001)Fe/(001) Cr superlattices wherein the Fe and Cr layers were deposited in a high vacuum on a (001) GaAs substrate kept at 20 °C and the magnetoresistance measurements were taken at low temperature (typically 4.2 K). The Grünberg work was performed on multilayers of Fe and Cr on (110) GaAs at room temperature.\n\nIn Fe/Cr multilayers with 3-nm-thick iron layers, increasing the thickness of the non-magnetic Cr layers from 0.9 to 3 nm weakened the antiferromagnetic coupling between the Fe layers and reduced the demagnetization field, which also decreased when the sample was heated from 4.2 K to room temperature. Changing the thickness of the non-magnetic layers led to a significant reduction of the residual magnetization in the hysteresis loop. Electrical resistance changed by up to 50% with the external magnetic field at 4.2 K. Fert named the new effect giant magnetoresistance, to highlight its difference with the anisotropic magnetoresistance. The Grünberg experiment made the same discovery but the effect was less pronounced (3% compared to 50%) due to the samples being at room temperature rather than low temperature.\n\nThe discoverers suggested that the effect is based on spin-dependent scattering of electrons in the superlattice, particularly on the dependence of resistance of the layers on the relative orientations of magnetization and electron spins. The theory of GMR for different directions of the current was developed in the next few years. In 1989, Camley and Barnaś calculated the \"current in plane\" (CIP) geometry, where the current flows along the layers, in the classical approximation, whereas Levy et al. used the quantum formalism. The theory of the GMR for the current perpendicular to the layers (current perpendicular to the plane or CPP geometry), known as the Valet-Fert theory, was reported in 1993. Applications favor the CPP geometry because it provides a greater magnetoresistance ratio (δH), thus resulting in a greater device sensitivity.\n\n## Theory\n\n### Fundamentals\n\n#### Spin-dependent scattering",
null,
"Electronic density of states (DOS) in magnetic and non-magnetic metals. 1: the structure of two ferromagnetic and one non-magnetic layers (arrows indicate the direction of magnetization). 2: splitting of DOS for electrons with different spin directions for each layer (arrows indicate the spin direction). F: Fermi level. The magnetic moment is antiparallel to the direction of total spin at the Fermi level.\n\nIn magnetically ordered materials, the electrical resistance is crucially affected by scattering of electrons on the magnetic sublattice of the crystal, which is formed by crystallographically equivalent atoms with nonzero magnetic moments. Scattering depends on the relative orientations of the electron spins and those magnetic moments: it is weakest when they are parallel and strongest when they are antiparallel; it is relatively strong in the paramagnetic state, in which the magnetic moments of the atoms have random orientations.\n\nFor good conductors such as gold or copper, the Fermi level lies within the sp band, and the d band is completely filled. In ferromagnets, the dependence of electron-atom scattering on the orientation of their magnetic moments is related to the filling of the band responsible for the magnetic properties of the metal, e.g., 3d band for iron, nickel or cobalt. The d band of ferromagnets is split, as it contains a different number of electrons with spins directed up and down. Therefore, the density of electronic states at the Fermi level is also different for spins pointing in opposite directions. The Fermi level for majority-spin electrons is located within the sp band, and their transport is similar in ferromagnets and non-magnetic metals. For minority-spin electrons the sp and d bands are hybridized, and the Fermi level lies within the d band. The hybridized spd band has a high density of states, which results in stronger scattering and thus shorter mean free path λ for minority-spin than majority-spin electrons. In cobalt-doped nickel, the ratio λ can reach 20.\n\nAccording to the Drude theory, the conductivity is proportional to λ, which ranges from several to several tens of nanometers in thin metal films. Electrons \"remember\" the direction of spin within the so-called spin relaxation length (or spin diffusion length), which can significantly exceed the mean free path. Spin-dependent transport refers to the dependence of electrical conductivity on the spin direction of the charge carriers. In ferromagnets, it occurs due to electron transitions between the unsplit 4s and split 3d bands.\n\nIn some materials, the interaction between electrons and atoms is the weakest when their magnetic moments are antiparallel rather than parallel. A combination of both types of materials can result in a so-called inverse GMR effect.\n\n#### CIP and CPP geometries",
null,
"Spin valves in the reading head of a sensor in the CIP (left) and CPP (right) geometries. Red: leads providing current to the sensor, green and yellow: ferromagnetic and non-magnetic layers. V: potential difference.\n\nElectric current can be passed through magnetic superlattices in two ways. In the current in plane (CIP) geometry, the current flows along the layers, and the electrodes are located on one side of the structure. In the current perpendicular to plane (CPP) configuration, the current is passed perpendicular to the layers, and the electrodes are located on different sides of the superlattice. The CPP geometry results in more than twice higher GMR, but is more difficult to realize in practice than the CIP configuration.\n\n#### Carrier transport through a magnetic superlattice",
null,
"Spin valve based on the GMR effect. FM: ferromagnetic layer (arrows indicate the direction of magnetization), NM: non-magnetic layer. Electrons with spins up and down scatter differently in the valve.\n\nMagnetic ordering differs in superlattices with ferromagnetic and antiferromagnetic interaction between the layers. In the former case, the magnetization directions are the same in different ferromagnetic layers in the absence of applied magnetic field, whereas in the latter case, opposite directions alternate in the multilayer. Electrons traveling through the ferromagnetic superlattice interact with it much weaker when their spin directions are opposite to the magnetization of the lattice than when they are parallel to it. Such anisotropy is not observed for the antiferromagnetic superlattice; as a result, it scatters electrons stronger than the ferromagnetic superlattice and exhibits a higher electrical resistance.\n\nApplications of the GMR effect require dynamic switching between the parallel and antiparallel magnetization of the layers in a superlattice. In first approximation, the energy density of the interaction between two ferromagnetic layers separated by a non-magnetic layer is proportional to the scalar product of their magnetizations:\n\n$\\displaystyle{ w = - J (\\mathbf M_1 \\cdot \\mathbf M_2). }$\n\nThe coefficient J is an oscillatory function of the thickness of the non-magnetic layer ds; therefore J can change its magnitude and sign. If the ds value corresponds to the antiparallel state then an external field can switch the superlattice from the antiparallel state (high resistance) to the parallel state (low resistance). The total resistance of the structure can be written as\n\n$\\displaystyle{ R = R_0 + \\Delta R \\sin^2 \\frac{\\theta}{2}, }$\n\nwhere R0 is the resistance of ferromagnetic superlattice, ΔR is the GMR increment and θ is the angle between the magnetizations of adjacent layers.\n\n### Mathematical description\n\nThe GMR phenomenon can be described using two spin-related conductivity channels corresponding to the conduction of electrons, for which the resistance is minimum or maximum. The relation between them is often defined in terms of the coefficient of the spin anisotropy β. This coefficient can be defined using the minimum and maximum of the specific electrical resistivity ρ for the spin-polarized current in the form\n\n$\\displaystyle{ \\rho_{F\\pm}=\\frac{2\\rho_F}{1\\pm\\beta}, }$\n\nwhere ρF is the average resistivity of the ferromagnet.\n\n#### Resistor model for CIP and CPP structures\n\nIf scattering of charge carriers at the interface between the ferromagnetic and non-magnetic metal is small, and the direction of the electron spins persists long enough, it is convenient to consider a model in which the total resistance of the sample is a combination of the resistances of the magnetic and non-magnetic layers.\n\nIn this model, there are two conduction channels for electrons with various spin directions relative to the magnetization of the layers. Therefore, the equivalent circuit of the GMR structure consists of two parallel connections corresponding to each of the channels. In this case, the GMR can be expressed as\n\n$\\displaystyle{ \\delta_H = \\frac{\\Delta R}{R}=\\frac{R_{\\uparrow\\downarrow}-R_{\\uparrow\\uparrow}}{R_{\\uparrow\\uparrow}}=\\frac{(\\rho_{F+}-\\rho_{F-})^2}{(2\\rho_{F+}+\\chi\\rho_N)(2\\rho_{F-}+\\chi\\rho_N)}. }$\n\nHere the subscript of R denote collinear and oppositely oriented magnetization in layers, χ = b/a is the thickness ratio of the magnetic and non-magnetic layers, and ρN is the resistivity of non-magnetic metal. This expression is applicable for both CIP and CPP structures. Under the condition $\\displaystyle{ \\chi\\rho_N \\ll \\rho_{F\\pm} }$ this relationship can be simplified using the coefficient of the spin asymmetry\n\n$\\displaystyle{ \\delta_H = \\frac{\\beta^2}{1-\\beta^2}. }$\n\nSuch a device, with resistance depending on the orientation of electron spin, is called a spin valve. It is \"open\", if the magnetizations of its layers are parallel, and \"closed\" otherwise.\n\n#### Valet-Fert model\n\nIn 1993, Thierry Valet and Albert Fert presented a model for the giant magnetoresistance in the CPP geometry, based on the Boltzmann equations. In this model the chemical potential inside the magnetic layer is split into two functions, corresponding to electrons with spins parallel and antiparallel to the magnetization of the layer. If the non-magnetic layer is sufficiently thin then in the external field E0 the amendments to the electrochemical potential and the field inside the sample will take the form\n\n$\\displaystyle{ \\Delta\\mu = \\frac{\\beta}{1-\\beta^2}eE_0\\ell_se^{z/\\ell_s}, }$\n$\\displaystyle{ \\Delta E = \\frac{\\beta^2}{1-\\beta^2}eE_0\\ell_se^{z/\\ell_s}, }$\n\nwhere s is the average length of spin relaxation, and the z coordinate is measured from the boundary between the magnetic and non-magnetic layers (z < 0 corresponds to the ferromagnetic). Thus electrons with a larger chemical potential will accumulate at the boundary of the ferromagnet. This can be represented by the potential of spin accumulation VAS or by the so-called interface resistance (inherent to the boundary between a ferromagnet and non-magnetic material)\n\n$\\displaystyle{ R_i= \\frac{\\beta(\\mu_{\\uparrow\\downarrow}-\\mu_{\\uparrow\\uparrow})}{2ej} = \\frac{\\beta^2\\ell_{sN}\\rho_N}{1+(1-\\beta^2)\\ell_{sN}\\rho_N/(\\ell_{sF}\\rho_F)}, }$\n\nwhere j is current density in the sample, sN and sF are the length of the spin relaxation in a non-magnetic and magnetic materials, respectively.\n\n## Device preparation\n\n### Materials and experimental data\n\nMany combinations of materials exhibit GMR, and the most common are the following:\n\n• FeCr\n• Co10Cu90: δH = 40% at room temperature\n• Co95Fe5/Cu: δH = 110% at room temperature.\n\nThe magnetoresistance depends on many parameters such as the geometry of the device (CIP or CPP), its temperature, and the thicknesses of ferromagnetic and non-magnetic layers. At a temperature of 4.2 K and a thickness of cobalt layers of 1.5 nm, increasing the thickness of copper layers dCu from 1 to 10 nm decreased δH from 80 to 10% in the CIP geometry. Meanwhile, in the CPP geometry the maximum of δH (125%) was observed for dCu = 2.5 nm, and increasing dCu to 10 nm reduced δH to 60% in an oscillating manner.\n\nWhen a Co(1.2 nm)/Cu(1.1 nm) superlattice was heated from near zero to 300 K, its δH decreased from 40 to 20% in the CIP geometry, and from 100 to 55% in the CPP geometry.\n\nThe non-magnetic layers can be non-metallic. For example, δH up to 40% was demonstrated for organic layers at 11 K. Graphene spin valves of various designs exhibited δH of about 12% at 7 K and 10% at 300 K, far below the theoretical limit of 109%.\n\nThe GMR effect can be enhanced by spin filters that select electrons with a certain spin orientation; they are made of metals such as cobalt. For a filter of thickness t the change in conductivity ΔG can be expressed as\n\n$\\displaystyle{ \\Delta G = \\Delta G_{SV} + \\Delta G_f (1 - e^{\\beta t/\\lambda}), }$\n\nwhere ΔGSV is change in the conductivity of the spin valve without the filter, ΔGf is the maximum increase in conductivity with the filter, and β is a parameter of the filter material.\n\n### Types of GMR\n\nGMR is often classed by the type of devices which exhibit the effect.\n\n#### Films\n\n##### Antiferromagnetic superlattices\n\nGMR in films was first observed by Fert and Grünberg in a study of superlattices composed of ferromagnetic and non-magnetic layers. The thickness of the non-magnetic layers was chosen such that the interaction between the layers was antiferromagnetic and the magnetization in adjacent magnetic layers was antiparallel. Then an external magnetic field could make the magnetization vectors parallel thereby affecting the electrical resistance of the structure.\n\nMagnetic layers in such structures interact through antiferromagnetic coupling, which results in the oscillating dependence of the GMR on the thickness of the non-magnetic layer. In the first magnetic field sensors using antiferromagnetic superlattices, the saturation field was very large, up to tens of thousands of oersteds, due to the strong antiferromagnetic interaction between their layers (made of chromium, iron or cobalt) and the strong anisotropy fields in them. Therefore, the sensitivity of the devices was very low. The use of permalloy for the magnetic and silver for the non-magnetic layers lowered the saturation field to tens of oersteds.\n\n##### Spin valves using exchange bias\n\nIn the most successful spin valves the GMR effect originates from exchange bias. They comprise a sensitive layer, \"fixed\" layer and an antiferromagnetic layer. The last layer freezes the magnetization direction in the \"fixed\" layer. The sensitive and antiferromagnetic layers are made thin to reduce the resistance of the structure. The valve reacts to the external magnetic field by changing the magnetization direction in the sensitive layer relatively to the \"fixed\" layer.\n\nThe main difference of these spin valves from other multilayer GMR devices is the monotonic dependence of the amplitude of the effect on the thickness dN of the non-magnetic layers:\n\n$\\displaystyle{ \\delta_H(d_N) = \\delta_{H0} \\frac{\\exp\\left(-d_N/\\lambda_N\\right)}{1 + d_N/d_0}, }$\n\nwhere δH0 is a normalization constant, λN is the mean free path of electrons in the non-magnetic material, d0 is effective thickness that includes interaction between layers. The dependence on the thickness of the ferromagnetic layer can be given as:\n\n$\\displaystyle{ \\delta_H(d_F) = \\delta_{H1} \\frac{1 - \\exp\\left(-d_F/\\lambda_F\\right)}{1 + d_F/d_0}. }$\n\nThe parameters have the same meaning as in the previous equation, but they now refer to the ferromagnetic layer.\n\n##### Non-interacting multilayers (pseudospin valves)\n\nGMR can also be observed in the absence of antiferromagnetic coupling layers. In this case, the magnetoresistance results from the differences in the coercive forces (for example, it is smaller for permalloy than cobalt). In multilayers such as permalloy/Cu/Co/Cu the external magnetic field switches the direction of saturation magnetization to parallel in strong fields and to antiparallel in weak fields. Such systems exhibit a lower saturation field and a larger δH than superlattices with antiferromagnetic coupling. A similar effect is observed in Co/Cu structures. The existence of these structures means that GMR does not require interlayer coupling, and can originate from a distribution of the magnetic moments that can be controlled by an external field.\n\n##### Inverse GMR effect\n\nIn the inverse GMR, the resistance is minimum for the antiparallel orientation of the magnetization in the layers. Inverse GMR is observed when the magnetic layers are composed of different materials, such as NiCr/Cu/Co/Cu. The resistivity for electrons with opposite spins can be written as $\\displaystyle{ \\rho_{\\uparrow,\\downarrow}=\\frac{2\\rho_F}{1\\pm\\beta} }$; it has different values, i.e. different coefficients β, for spin-up and spin-down electrons. If the NiCr layer is not too thin, its contribution may exceed that of the Co layer, resulting in inverse GMR. Note that the GMR inversion depends on the sign of the product of the coefficients β in adjacent ferromagnetic layers, but not on the signs of individual coefficients.\n\nInverse GMR is also observed if NiCr alloy is replaced by vanadium-doped nickel, but not for doping of nickel with iron, cobalt, manganese, gold or copper.\n\n#### GMR in granular structures\n\nGMR in granular alloys of ferromagnetic and non-magnetic metals was discovered in 1992 and subsequently explained by the spin-dependent scattering of charge carriers at the surface and in the bulk of the grains. The grains form ferromagnetic clusters about 10 nm in diameter embedded in a non-magnetic metal, forming a kind of superlattice. A necessary condition for the GMR effect in such structures is poor mutual solubility in its components (e.g., cobalt and copper). Their properties strongly depend on the measurement and annealing temperature. They can also exhibit inverse GMR.\n\n## Applications\n\n### Spin-valve sensors\n\n#### General principle\n\nOne of the main applications of GMR materials is in magnetic field sensors, e.g., in hard disk drives and biosensors, as well as detectors of oscillations in MEMS. A typical GMR-based sensor consists of seven layers:\n\n1. Silicon substrate,\n2. Binder layer,\n3. Sensing (non-fixed) layer,\n4. Non-magnetic layer,\n5. Fixed layer,\n6. Antiferromagnetic (Pinning) layer,\n7. Protective layer.\n\nThe binder and protective layers are often made of tantalum, and a typical non-magnetic material is copper. In the sensing layer, magnetization can be reoriented by the external magnetic field; it is typically made of NiFe or cobalt alloys. FeMn or NiMn can be used for the antiferromagnetic layer. The fixed layer is made of a magnetic material such as cobalt. Such a sensor has an asymmetric hysteresis loop owing to the presence of the magnetically hard, fixed layer.\n\nSpin valves may exhibit anisotropic magnetoresistance, which leads to an asymmetry in the sensitivity curve.\n\n#### Hard disk drives\n\nIn hard disk drives (HDDs), information is encoded using magnetic domains, and a change in the direction of their magnetization is associated with the logical level 1 while no change represents a logical 0. There are two recording methods: longitudinal and perpendicular.\n\nIn the longitudinal method, the magnetization is normal to the surface. A transition region (domain walls) is formed between domains, in which the magnetic field exits the material. If the domain wall is located at the interface of two north-pole domains then the field is directed outward, and for two south-pole domains it is directed inward. To read the direction of the magnetic field above the domain wall, the magnetization direction is fixed normal to the surface in the antiferromagnetic layer and parallel to the surface in the sensing layer. Changing the direction of the external magnetic field deflects the magnetization in the sensing layer. When the field tends to align the magnetizations in the sensing and fixed layers, the electrical resistance of the sensor decreases, and vice versa.\n\n### Magnetic RAM",
null,
"The use of a spin valve in MRAM. 1: spin valve as a memory cell (arrows indicate the presence of ferromagnetic layers), 2: row line, 3: column line. Ellipses with arrows denote the magnetic field lines around the row and column lines when electric current flows through them.\n\nA cell of magnetoresistive random-access memory (MRAM) has a structure similar to the spin-valve sensor. The value of the stored bits can be encoded via the magnetization direction in the sensor layer; it is read by measuring the resistance of the structure. The advantages of this technology are independence of power supply (the information is preserved when the power is switched off owing to the potential barrier for reorienting the magnetization), low power consumption and high speed.\n\nIn a typical GMR-based storage unit, a CIP structure is located between two wires oriented perpendicular to each other. These conductors are called lines of rows and columns. Pulses of electric current passing through the lines generate a vortex magnetic field, which affects the GMR structure. The field lines have ellipsoid shapes, and the field direction (clockwise or counterclockwise) is determined by the direction of the current in the line. In the GMR structure, the magnetization is oriented along the line.\n\nThe direction of the field produced by the line of the column is almost parallel to the magnetic moments, and it can not reorient them. Line of the row is perpendicular, and regardless of the magnitude of the field can rotate the magnetization by only 90 °. With the simultaneous passage of pulses along the row and column lines, of the total magnetic field at the location of the GMR structure will be directed at an acute angle with respect to one point and an obtuse to others. If the value of the field exceeds some critical value, the latter changes its direction.\n\nThere are several storage and reading methods for the described cell. In one method, the information is stored in the sensing layer; it is read via resistance measurement and is erased upon reading. In another scheme, the information is kept in the fixed layer, which requires higher recording currents compared to reading currents.\n\nTunnel magnetoresistance (TMR) is an extension of spin-valve GMR, in which the electrons travel with their spins oriented perpendicularly to the layers across a thin insulating tunnel barrier (replacing the non-ferromagnetic spacer). This allows to achieve a larger impedance, a larger magnetoresistance value (~10x at room temperature) and a negligible temperature dependence. TMR has now replaced GMR in MRAMs and disk drives, in particular for high area densities and perpendicular recording.\n\n### Other applications\n\nMagnetoresistive insulators for contactless signal transmission between two electrically isolated parts of electrical circuits were first demonstrated in 1997 as an alternative to opto-isolators. A Wheatstone bridge of four identical GMR devices is insensitive to a uniform magnetic field and reacts only when the field directions are antiparallel in the neighboring arms of the bridge. Such devices were reported in 2003 and may be used as rectifiers with a linear frequency response."
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https://contents.driverguide.com/content.php?id=1202325&path=data2.cab%2FApp_MyLogo%2FMyLogo.ini | [
"# MyLogo.ini Driver File Contents (AsusUpdt_V71304.zip)\n\nDriver Package File Name: AsusUpdt_V71304.zip\nFile Size: 8.8 MB\n\n```[SUPPORT MB]\nNUMBER = 22\nMB(1)= CUSL2-CB<R>\nMB(2)= P4B<R>\nMB(3)= P4B-E<R>\nMB(4)= P4B266<R>\nMB(5)= P4B266-E<R>\nMB(6)= P4B266-C<R>\nMB(7)= P4S333<R>\nMB(8)= A7V333<R>\nMB(9)= P4S133<R>\nMB(10)=A7S333<R>\nMB(11)=P4B533<R>\nMB(12)=P4B533-E<R>\nMB(13)=P4B533-V<R>\nMB(14)=P4T533<R>\nMB(15)=P4T533-C<R>\nMB(16)=P4S533<R>\nMB(17)=P4S533-E<R>\nMB(18)=P4SE\nMB(19)=A7V8X<R>\nMB(20)=P4S8X<R>\nMB(21)=P4G8X<R>\nMB(22)=P4PE<R>```"
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https://www.gaageegoo.info/2015/01/behaviour-of-gases10th-science-notes.html | [
"# Behaviour of Gases–10th Science Notes and Question Bank\n\n### Text Book Question and Answers\n\n1. Define Charles law.\n\n“At constant pressure, the volume of a fixed mass of a gas is directly proportional to its absolute temperature”– This is Charles law.\n\n2. Caution “store in cool and dry place” is printed on medicine bottles. Why?\n\nWhen the bottle is exposed, due to heat, it expands as the gas inside the bottle expands as temperature rises. To increase the volume the bottle explodes.\n\n3. Define Boyle’s law.\n\n“At constant temperature, the volume of a given mass of dry gas is inversely proportional to its pressure” – This is Boyles law.\n\n4. What do you mean by Diffusion?\n\nRandom movement of gaseous molecules from the region of higher concentration to the region of lower concentration is called diffusion.\n\n5. Define rate of diffusion?\n\nThe volume of gas diffusing per unit time is called rate of diffusion.\n\n6. What is the relation between diffusion and mass?\n\nThe rate of diffusion is inversely proportional to square root of mass\n\nr = K\n\nWhere m = mass, r = rate of diffusion, v = volume.\n\n7. The volume of the gas found to be at a pressure of 2500 Pa. when the pressure was decreased by 500 Pa the gas occupied a volume of 2400 litres. Calculate the initial volume occupied by gas before the change was done at constant temperature?\n\nData:\n\nP1 = 2500,\n\nP2 = 2500-500 = 2000\n\nV2 = 2400\n\nV1 =?\n\nSolution:\n\nAccording to Boyle’s law\n\nP1 V1 = P2 V2 (at constant temperature)\n\n2500 x V1 = 2000 x 2400\n\nV1 = 1920 litres\n\n8. About 6 litres of oxygen gas is collected at 300K. If for a particular use, the volume has to be reduced to 1/3 of its original volume, find the gas has to be cooled? (pressure is kept constant)\n\nData:\n\nV1 = 6 litre\n\nV2 = 1/3 x 6 = 2 litre\n\nT1 = 300K,\n\nT2 =?\n\nSolution:\n\nAccording to Charles law (at constant pressure)\n\nV1/T1 = V2/T2\n\n6/300 = 2/ T2\n\nT2 = 100K.\n\nThe gas has to be cooled to 100k,\n\nII. For each of the following statements or questions four alternatives are given. Choose the most appropriate alternative:\n\n1. The expression which do not says relation between volume and temperature at constant temperature is -------\n\na. V = KT b. T = KV c. V/T = K d. V = K/T\n\n2. The temperature which is also called Absolute zero is ------\n\na.00C b. 00F c. -273 0C d. -273 0K\n\n3. The expression for relation between volume and pressure at constant temperature is\n\na. P/V = K b. T = PV c. V/ P = K d. PV = K\n\nIII. Fill in the blanks with right answer\n\n1. Under constant pressure , per degree rise in temperature , the volume of gas is increased by ------- of the original volume at 00C. ( 1 / 273)\n\n2. The S.I unit of temperature is --------- (kelvin)\n\n3. The volume of gas diffusing per unit time is --------- ( rate of diffusion )\n\nIV. Match the followings\n\n A B C 1.Charle’s law i)Volume of gas diffused / Time(3) a) TV= PK 2. Boyle’s law ii) constant volume b) V = KT (1) 3. Rate of diffusion iii) constant temperature (2) c) PV = K (2) iv) Constant pressure (1) d) r = k √v / √m (3)\n\n1. List the main features of gases.\n\na) Gases are highly compressible.\n\nb) Gases excerts pressure equally in all directions\n\nc) Gases mix evenly in all proportions without any mechanical aid\n\nd) Gases are least dense than other two states of matter.\n\n2. Give the formula for Charles law.\n\nVolume α temperature\n\nV α T\n\nV = KT here V= volume T= temperature K = proportionality constant\n\n3. List the applications of Charles law.\n\na) Soda bottles should store in cool and dry place.\n\nb) Air balloons pops out during hot summer than in winter.\n\n4. Give the formula for Boyle’s law.\n\nV α 1 / P\n\nV α K / P\n\nPV =K here V= volume , P= Pressure , K = proportionality constant\n\n5. List the applications of Boyle’s law.\n\na)Popping of balloon when squeezed due to increase in the pressure.\n\nb) Deep sea fishes die when suddenly they brought to surface due to low pressure.\n\nc) Scuba driver’s life is under threat when he suddenly comes to surface quickly.\n\n6. State Graham’s law of diffusion.\n\n“The rate of diffusion of gas is inversely proportional to the square root of its density”- This is called Graham’s law of diffusion\n\n7. Give the formula for Graham’s law of diffusion\n\nr α 1 / √d\n\nr = K / √d\n\nK = r x √d\n\nhere r = rate of diffusion, d = density of gas, K = proportionality constant\n\nYou Might Like\n\n1.",
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https://calculus7.com/how-do-you-calculate-the-volume-of-a-tank-in-gallons-and-litres/ | [
"# How do you calculate the volume of a tank in Gallons and Litres\n\n### How Can I Find Out How Much Water My Fish Tank Holds\n\nRectangular Tanks\n\nThe measurements are 20 inches by 12 inches by 12 inches, i.e Length 12 inches, Width 12 inches, height 20 inches\n\nthe volume is 2,880 cubic inches.\n\nFinally, divide the cubic volume in inches by 231, as a gallon is equal to 231 cubic inches.\n\nA 2,880 cubic-inch tank is 12.47 gallons"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.8082949,"math_prob":0.97052383,"size":352,"snap":"2022-27-2022-33","text_gpt3_token_len":96,"char_repetition_ratio":0.20114942,"word_repetition_ratio":0.0,"special_character_ratio":0.30397728,"punctuation_ratio":0.13414635,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.97920924,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2022-06-30T00:39:50Z\",\"WARC-Record-ID\":\"<urn:uuid:8ec0755b-af12-41cc-8267-9dcd5b1402f7>\",\"Content-Length\":\"57708\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:bb43407b-e1e9-4fbb-8bac-ed21924f9ec0>\",\"WARC-Concurrent-To\":\"<urn:uuid:3007160d-3319-4fb8-8661-1db26864c946>\",\"WARC-IP-Address\":\"104.21.11.128\",\"WARC-Target-URI\":\"https://calculus7.com/how-do-you-calculate-the-volume-of-a-tank-in-gallons-and-litres/\",\"WARC-Payload-Digest\":\"sha1:HDB2NVJQJF5JSCIZA5XOKGGZQ5BPEON3\",\"WARC-Block-Digest\":\"sha1:WOFIWX7JRIBI5RVCTFYXEJJONFA44Y6B\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2022/CC-MAIN-2022-27/CC-MAIN-2022-27_segments_1656103646990.40_warc_CC-MAIN-20220630001553-20220630031553-00786.warc.gz\"}"} |
https://mathoverflow.net/questions/342926/coinciding-weak-operator-and-strong-operator-topologies | [
"# Coinciding weak operator and strong operator topologies\n\nLet $$A \\subset \\mathcal{B}(H)$$ a subalgebra, not necessarily a $$*$$-algebra. In Murphy's book 'C*-algebras and Operator Theory', in Remark 4.2.1 you can find a proof of the failure of strong compactness for the ball of $$\\mathcal{B}(H)$$:\n\nIf the ball is strongly compact, then the identity map of the ball with the relative strong topology to the ball with the relative weak operator topology is a continuous bijection from a compact space to a Hausdorff one, and therefore a homeomorphism, so the relative strong operator and the relative weak operator topologies coincide. But the involution operator is weakly continuous but not strongly continuous restricted to the ball, and it shows that the unit ball can't be strongly compact.\n\nIt is clear that this proof relies in the fact that the two topologies can't coincide in the unit ball because the non-strong continuity of the involution operator, and it is clearly an extendable method to the $$*$$-subalgebras setting. But, if we have a subalgebra $$A$$, not necessarily closed by the adjoint map, are there any 'invariants' of the relative topologies that we can analyze to decide if the two topologies cannot coincide in the ball of $$A$$?\n\n## 1 Answer\n\nI'm not sure there is a definitive answer here, as it's asked if there are \"invariants\", not a complete characterisation. Further, it's not clear to me if the question is asking about compactness or just whether the WOT and SOT are different.\n\nIndeed, if all we are interested in is to show that the SOT is not the same as the WOT when restricted to the unit ball of $$B(H)$$, then we don't need to consider compactness at all. As you say, Murphy observes (this is Example 4.1.1 in his book) that the adjoint is WOT continuous but not SOT continuous.\n\nActually, there is another example which doesn't use the adjoint. We can just consider $$S$$ the unilateral shift acting on $$\\ell^2$$, and let $$S_n = S^n$$. Then $$S_n\\rightarrow 0$$ weakly, but of course as each $$S_n$$ is an isometry, not subnet of $$(S_n)$$ can converge to $$0$$ in the SOT.\n\nI don't think it is obvious that the same argument will work for self-adjoint subalgebras $$A\\subseteq B(H)$$. For example, if $$A$$ is commutative, then the adjoint is continuous for the SOT restricted to the unit ball of $$A$$.\n\n1. Let $$A=L^\\infty(\\mathbb T)$$ acting on $$H=L^2(\\mathbb T)$$ by multiplication, and let $$a_n(e^{i\\theta}) = e^{in\\theta}$$. The Riemann-Lebesgue Lemma shows that $$(a_n)$$ is WOT convergent to $$0$$, but clearly $$(a_n)$$ is not SOT convergent to $$0$$.\n\n2. However, let $$A=\\ell^\\infty$$ acting on $$H=\\ell^2$$. Then a bounded sequence $$(x_n)$$ in $$A$$ is WOT convergent to $$0$$ exactly when $$x_n(k)\\rightarrow 0$$ for each $$k$$ (thinking of $$x_n$$ as a bounded function $$\\mathbb N\\rightarrow\\mathbb C$$). This implies that $$x_n\\rightarrow 0$$ in the SOT.\n\nLet $$X\\subseteq B(H)$$ be just a subspace. Identify $$B(H\\oplus H)$$ with $$2\\times 2$$-matrices with entries in $$B(H)$$. Define $$Y(X) = \\left\\{ \\begin{pmatrix} \\lambda & x \\\\ 0 & \\lambda \\end{pmatrix} : x\\in X, \\lambda\\in\\mathbb C \\right\\}.$$ The $$Y(X)$$ is a subalgebra, not self-adjoint, and $$Y(X)$$ is closed in all the various operator topologies if and only if $$X$$ is closed in that topology. While the unit ball of $$Y(X)$$ and $$X$$ do not biject, bounded subsets to correspond to bounded subsets. In this way, we can transport (counter-)examples from subspaces to subalgebras.\n\nLet $$X$$ be a \"row space\" of $$H$$. That is, fixed a unit vector $$\\xi_0\\in H$$ and let $$X$$ be the collection of rank-one operators $$\\{ \\theta_\\xi : \\xi\\in H \\}$$ where $$\\theta_\\xi:H\\rightarrow H; \\eta\\mapsto (\\eta|\\xi)\\xi_0$$. Then $$X$$ is anti-linearly isomorphic to $$H$$. A bounded net $$(\\theta_{\\xi_n})$$ converges to $$x\\in B(H)$$ in the WOT if and only if $$(\\eta|\\xi_n) (\\xi_0|\\eta') \\rightarrow (x(\\eta)|\\eta') \\qquad (\\eta, \\eta'\\in H).$$ This is equivalent to $$(\\xi_n)$$ being weakly-convergent in $$H$$, say to $$\\xi$$, in which case $$\\theta_{\\xi_n}\\rightarrow\\theta_\\xi$$. Similarly, $$(\\theta_{\\xi_n})$$ converges strongly to $$x\\in B(H)$$ when $$\\|(\\eta|\\xi_n) \\xi_0 - x(\\eta)\\|\\rightarrow 0 \\qquad (\\eta\\in H).$$ This gives the same condition on $$(\\xi_n)$$. So, the WOT and SOT agree on the bounded subsets of $$X$$, and hence on the unit ball of $$Y(X)$$."
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.8486312,"math_prob":0.9999478,"size":3012,"snap":"2021-21-2021-25","text_gpt3_token_len":952,"char_repetition_ratio":0.10638298,"word_repetition_ratio":0.008213553,"special_character_ratio":0.31407702,"punctuation_ratio":0.0995106,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":1.0000076,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-06-18T07:01:37Z\",\"WARC-Record-ID\":\"<urn:uuid:24193e05-5f5a-43a6-8618-70eee676e183>\",\"Content-Length\":\"135395\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:4b0f166d-4f06-4692-badc-c3a5ea7d40a0>\",\"WARC-Concurrent-To\":\"<urn:uuid:3f9ac61e-e04a-4179-8ad7-e0d34f015707>\",\"WARC-IP-Address\":\"151.101.129.69\",\"WARC-Target-URI\":\"https://mathoverflow.net/questions/342926/coinciding-weak-operator-and-strong-operator-topologies\",\"WARC-Payload-Digest\":\"sha1:PTXULODI4P4JSFJ37DEVEAZIWSMKUNQU\",\"WARC-Block-Digest\":\"sha1:O7W7XI3YCHKQPMOKHZSPF2QMTKKLO3R7\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-25/CC-MAIN-2021-25_segments_1623487635724.52_warc_CC-MAIN-20210618043356-20210618073356-00263.warc.gz\"}"} |
http://philropost.com/2-x-2-x-2.html | [
"2 X 2 X 2\n\nstep by step math solutions with wolfram alpha pro.\n\nadd or subtract fractions with step by step math problem solver.\n\nx2 t01 02 solving quadratics 2013.\n\ngraph x 2 y 2 4 youtube.\n\nalgebra calculator mathpapa.\n\nx 1 x 5 then find the value of x 2 1 x 2 and x 3 1 x 3 mathematics.\n\nstep by step math solutions with wolfram alpha pro.\n\nsolve inequalities with step by step math problem solver.\n\ninverse of a matrix.\n\nwolfram alpha examples step by step solutions.\n\ninverse of a matrix.\n\nsimplify radical rational expression with step by step math problem.\n\nhow to integrate 1 x 2 youtube.\n\nsolve the 2x2 rubik s cube you can do the rubiks cube.\n\nalgebra calculator mathpapa.\n\nstep by step math solutions with wolfram alpha pro.\n\nsolve quadratic equation with step by step math problem solver.\n\ninverse of a matrix.\n\n12 6 arc length.\n\nother types of graph.\n\nalgebra 2 worksheets systems of equations and inequalities worksheets.\n\nfinding domain and range.\n\nhow to solve a 2x2 rubik s cube ortega method kewbzuk uk speed.\n\nderivative calculator with steps.\n\nintegral of 1 1 x 2 substitution youtube.\n\nsquare algebra wikipedia.\n\nalgebra 2 worksheets matrices worksheets.\n\nfinding the slope of a line.\n\nhow to solve a 2x2 rubik s cube ortega method kewbzuk uk speed.\n\nsolving absolute value equations and inequalities she loves math.\n\nunits algebra ii composition of functions d inverses of functions and.\n\n2 times table with games at timestables com.\n\nsolve the 2x2 rubik s cube you can do the rubiks cube.\n\nlumber composites the home depot canada.\n\nsharetechnote.\n\nhow to solve a 2x2 rubik s cube the pocket cube.\n\nsolve inequalities with step by step math problem solver.\n\nopenepi 2 x 2 table statistics.\n\ncalculus building intuition for the derivative betterexplained.\n\nstep by step math solutions with wolfram alpha pro.\n\ndouble and half angle formulas.\n\nunits algebra ii composition of functions d inverses of functions and.\n\n10 7 the method of partial fractions.\n\nsolving quadratics by factoring and completing the square she.\n\nopenepi 2 x 2 table statistics.\n\nlogarithm rules chilimath.\n\nlong division of polynomials.\n\nmultiplying 2 digit by 1 digit numbers a.\n\nhow to solve a 2x2 rubik s cube the pocket cube.\n\neigenvalues and eigenvectors.\n\ngraphs of functions.\n\nbusiness card size specifications and dimensions.\n\nmultiplication worksheets free commoncoresheets.\n\necuaciones de segundo grado ppt descargar.\n\ndistance formula chilimath.\n\nonline 2x2 rubik s cube solver.\n\nintegration by parts.\n\nlong division of polynomials.\n\n2x2 rubik s cube beginner s solution tutorial with algorithms.\n\nintroduction to calculus with derivatives.\n\nhow to solve a 2x2 rubik s cube kewbzuk uk speed cubes.\n\nbodmas rule.\n\nsolve the 2x2 rubik s cube you can do the rubiks cube.\n\n4 expansion r k bansal solutions for class 9 mathematics icse.\n\nend behavior of a function.\n\nbinary multiplier types binary multiplication calculator.\n\nlet x be the greatest integer less than or equal to xdot then at.\n\nsharetechnote.\n\n1 2 x 2 3 8 uniform nameplate agent gear usa.\n\neigenvalues and eigenvectors.\n\ncover up rule or how to make partial fractions easy.\n\nassignment 1 exploring sine curves.\n\narea under a curve mathematics a level revision.\n\nmathsteps grade 7 linear equations what is it.\n\n2x2 rubik s cube beginner s solution tutorial with algorithms.\n\ngraph inequalities with step by step math problem solver.\n\ndomain and range free math help.\n\nintroduction to calculus with derivatives.\n\n4 expansion r k bansal solutions for class 9 mathematics icse.\n\nassignment 1 exploring sine curves.\n\nlive scan fingerprinting passport visa citizenship id custom size.\n\nunits algebra ii composition of functions d inverses of functions and.\n\nstandard label sizes sheetlabels com.\n\nsolving absolute value equations and inequalities she loves math.\n\nanalytical geometry examples.\n\narea under a curve mathematics a level revision.\n\n2x2 free shipping available.\n\nhow to solve quadratic equation by completing the square method.\n\nchi square test of independence spss tutorials libguides at kent.\n\nact form 74f math answer explanations act helper.\n\nex square a 2x2 matrix youtube.\n\nintegration algebraic fractions integration from a level maths tutor.\n\nceiling tiles the home depot canada.\n\nvariance wikipedia."
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.7054857,"math_prob":0.9937634,"size":3759,"snap":"2019-26-2019-30","text_gpt3_token_len":862,"char_repetition_ratio":0.12037284,"word_repetition_ratio":0.20672269,"special_character_ratio":0.2037776,"punctuation_ratio":0.12554744,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9991636,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-06-19T07:05:09Z\",\"WARC-Record-ID\":\"<urn:uuid:d1dc8dc3-f67d-49f8-83e1-902df0b4ad73>\",\"Content-Length\":\"76647\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:21ed1c24-32b8-402a-8ed9-c13546f0dc73>\",\"WARC-Concurrent-To\":\"<urn:uuid:252e64a4-68f9-429f-adfb-40fa15d3dc15>\",\"WARC-IP-Address\":\"104.31.89.18\",\"WARC-Target-URI\":\"http://philropost.com/2-x-2-x-2.html\",\"WARC-Payload-Digest\":\"sha1:VYUDPXDSV3SWWGO5Q3LD4R6JVZFNBY2T\",\"WARC-Block-Digest\":\"sha1:VKIBTY6EIGLMCTSIOFTV4AVVMORA46M2\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-26/CC-MAIN-2019-26_segments_1560627998923.96_warc_CC-MAIN-20190619063711-20190619085711-00426.warc.gz\"}"} |
https://socratic.org/questions/what-does-the-first-law-of-reflection-state | [
"# What does the first law of reflection state?\n\nJan 1, 2015\n\nThe First Law of reflection States that the angle made by the incident light ray with the normal to the surface at the point of incidence is equal to angle made by the reflected light ray with the normal.\n\nThe following figures are examples of this law under different circumstances:\n1) A flat Mirror",
null,
"2)Curved Mirrors",
null,
"One note of caution though always take the Normal at the point of incidence, telling this is trivial for plane mirrors as normal is always the same but in curved mirrors the normal changes from point to point so always remember to take the normal at the point of incidence.\n\nNice applet on this website: http://www.physicsclassroom.com/mmedia/optics/lr.cfm"
]
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"https://d2jmvrsizmvf4x.cloudfront.net/ixWP16kYQxGbxtK3Jy5b_Screenshot_2015-01-02-01-50-29.png",
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"https://d2jmvrsizmvf4x.cloudfront.net/4aSy8aZeRBuCAdhj9UDz_Screenshot_2015-01-02-01-49-50.png",
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.89606005,"math_prob":0.9187474,"size":837,"snap":"2019-51-2020-05","text_gpt3_token_len":171,"char_repetition_ratio":0.13565426,"word_repetition_ratio":0.0,"special_character_ratio":0.19235365,"punctuation_ratio":0.06369427,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.95686394,"pos_list":[0,1,2,3,4],"im_url_duplicate_count":[null,1,null,2,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-12-16T12:50:42Z\",\"WARC-Record-ID\":\"<urn:uuid:5de0fff6-c799-45e2-8ada-3b93b9a693e4>\",\"Content-Length\":\"35162\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:3f2b53fc-943b-431a-94f3-87ce3f93573e>\",\"WARC-Concurrent-To\":\"<urn:uuid:47eea308-2ca3-4c9d-995a-9edd2ac6a368>\",\"WARC-IP-Address\":\"54.221.217.175\",\"WARC-Target-URI\":\"https://socratic.org/questions/what-does-the-first-law-of-reflection-state\",\"WARC-Payload-Digest\":\"sha1:KVQEFUFZ2KZ6247WDAMUMJZAOTRAWYXC\",\"WARC-Block-Digest\":\"sha1:EREWH33W5V6PBJAIRBY6B6UD3M7HV5PQ\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-51/CC-MAIN-2019-51_segments_1575540565544.86_warc_CC-MAIN-20191216121204-20191216145204-00067.warc.gz\"}"} |
https://smartwritings.org/let-true-population-model-be-y-01xu-0-not-0-consider-following-empirical-models-correctly-sp/ | [
"# let true population model be y 01xu 0 not 0 consider following empirical models correctly sp\n\nLet the true population model be: y = ?0+?1x+u with ?0 not= 0. Consider the following empirical models: ! The correctly specied model: y = ?^0 + ?^1x ! The misspecied model: y = ?^x Answer the following questions. 1. Derive the expression for the OLS estimators ?^ and ?^1. 2. Is the OLS estimator ?^ an unbiased estimator of ?1? If your answer is no, determine the bias. 3. Derive an expression for the variances of ?^ and ?^1. 4. Compare the expressions for the variances of ?^ with the variance of ?^1 from the correctly specified regression. Is Var(?^) > V ar( ?^1)? 5. Comment on the tradeoff between bias and variance when choosing between these estimators."
]
| [
null
]
| {"ft_lang_label":"__label__en","ft_lang_prob":0.65191597,"math_prob":0.99052066,"size":1040,"snap":"2022-40-2023-06","text_gpt3_token_len":304,"char_repetition_ratio":0.11003861,"word_repetition_ratio":0.15584415,"special_character_ratio":0.31346154,"punctuation_ratio":0.20982143,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9987271,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2022-10-03T18:38:32Z\",\"WARC-Record-ID\":\"<urn:uuid:0cca9b2a-87b0-4eb7-af45-cbb8abe2ec03>\",\"Content-Length\":\"40306\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:3c8c2b50-bf5d-457b-aff8-34c1e0c985a4>\",\"WARC-Concurrent-To\":\"<urn:uuid:54493901-c66a-4c54-9be4-ead7ccffcd42>\",\"WARC-IP-Address\":\"162.0.232.59\",\"WARC-Target-URI\":\"https://smartwritings.org/let-true-population-model-be-y-01xu-0-not-0-consider-following-empirical-models-correctly-sp/\",\"WARC-Payload-Digest\":\"sha1:XQHW6FUYOKKSPBHGP2W3VIMG26C27XMR\",\"WARC-Block-Digest\":\"sha1:HFTDK2STZ6OFPHUEMRGHOJSHC5OQYMR2\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2022/CC-MAIN-2022-40/CC-MAIN-2022-40_segments_1664030337428.0_warc_CC-MAIN-20221003164901-20221003194901-00603.warc.gz\"}"} |
https://www.metafunction.co.uk/post/all-about-digital-oscillators-part-1-aliasing-foldover | [
"Search\n\n# All About Digital Oscillators Part 1 – Aliasing & Foldover",
null,
"At the core of any synth is it’s oscillator – the device that produces the raw waveforms that form the building blocks of synthesis. In the analogue world, these are typically voltage controlled and built via electronic components such as op-amps and diodes. In the digital world, such as in a plug-in, there are many ways to build an oscillator and one of the most popular methods is via an algorithmic technique (i.e. a mathematical equation). The most important and deployed approach in digital synthesizer design within the modern landscape is the use of quasi band-limited oscillators to reduce aliasing. Quasi what? To answer that question we first need to consider aliasing in terms of synthesis….\n\n## Folding Over\n\nYou are most likely familiar with aliasing from your experience of the world of digital audio theory. We typically tend to set our DAW to operate with a sampling frequency (i.e. 44.1kHz or 48kHz) that conforms to the Nyquist-Shannon sampling theorem. This theorem states that we need to sample a signal at twice its highest frequency to be able to uniquely reconstruct it. This frequency is called the Nyquist frequency. When recording an acoustic signal into our DAW via an audio interface, the A/D converter in the interface has a brick-wall lowpass filter which is set to our Nyquist frequency. The filters job is to only allow content lower than the Nyquist frequency in, therefore providing us with a signal that has been appropriately band-limited (i.e. at 22,050 Hz or 24,000 Hz). So, in the digital audio world, aliasing happens if you do not properly band-limit the input signal. Alias signals ‘foldover’ at the Nyquist frequency and are reflected back down along the frequency spectrum (see figure 1). They are most noticeable as distortion in our audio signal and not a lot can be done to remove them.",
null,
"Figure 1: Frequency domain representation of aliasing\n\nHere the dotted red line shows foldover, the mirror-like reflection of aliased signal components, at a Nyquist frequency of 24kHz\n\nWithin our digital synthesizer, we simply replace the input signal that exists when we are recording an acoustic signal with the output of our oscillator algorithm. The output of the oscillator algorithm IS our input signal – but it has not been sent through the brick-wall lowpass filter in our A/D converter. So technically, when using algorithmic techniques to create a digital oscillator within a computer, it is possible to create a signal that extends well beyond the Nyquist frequency and contains aliased components. We perceive this aliasing as subtle distortion.\n\n## Time & Frequency\n\nAs we can see in figure 1, aliased components foldover around the Nyquist frequency and are visible in the frequency domain on a spectrogram. It is easy to see and hear this via a simple Max patch as shown in figure 2. On the left hand side is the Max Saw~ object (a band-limited oscillator), whilst on the right hand side we have the Max Phasor~ object which provides an ‘ ideal mathematical ramp without filtering out frequency information above Nyquist’ (i.e. a non band-limited saw oscillator). On the left side we can see a clean signal in the spectrogram, whilst on the right side we can see aliased components folding over around the Nyquist frequency and being reflected back down the frequency spectrum.",
null,
"Figure 2: Using Max to show a frequency domain representation of aliasing\n\nOn the left we can see that the band-limited Saw~ object produces a nice clean signal on the spectrogram whilst on the right we can see that the non band-limited Phasor~ produces alias components that foldover around the Nyquist frequency and are reflected back down the frequency spectrum\n\nThe easiest wave to see aliasing in the frequency domain is via 3D spectrogram plots. These give us a very clear indication of the amount of aliasing and how it is represented as distortion spread across the frequency spectrum, down from the Nyquist frequency. In fact, using these type of plots the amount of foldover and distortion in the signal is really surprising. To show this off, the authour developed a band-limited and non band-limited oscillator algorithm in C++ and generated plots. Figure 3 shows a 3D spectrogram plot of a non band-limited square wave and figure 4 shows a 3D spectrogram plot of a band-limited square wave. As aliasing is often much more noticeable at higher frequencies, these plots are of the oscillator running at C6 (MIDI note number 96), which has a fundamental frequency of approx~ 2093Hz.",
null,
"Figure 3: 3D spectrogram representation of aliased oscillator Non band-limited square wave plot at approx~ 2kHz. Notice the high levels of aliasing appearing as ripples down the frequency spectrum",
null,
"Figure 4: 3D spectrogram representation of non aliased oscillator Band-limited square wave plot at approx~ 2kHz. Notice the reduced levels of aliasing\n\n‘OK, that all makes sense, but what about the time domain?’ I hear you ask. As it happens, in the time domain, aliased components are visualized a bit differently. In the time domain aliased components are seen as discontinuities in the edges of the synthesized waveforms. That is, at the fast changing edges of waveforms. For example, during the cycle of a waveform there are moments when the waveform changes amplitude over time. These moments give the characteristic shape to our waveform (i.e. square). In the digital world, if we were to plot out a series of instantaneous values for frequency and amplitude for many samples over time we would see our waveshape. The higher the frequency or pitch of the oscillator the more rapid the edges of waveforms change, and hence the more discontinuities in the edges of the synthesized waveforms. Figure 5 shows a time domain oscilloscope plot of a non band-limited square wave. Notice the amount of discontinuity at the edges of the waveshape. This is the time domain representation of aliasing – visible at the fast changing edges of waveforms. A non band-limited oscillator is often known as a ‘naive’ oscillator. Figure 6 shows a time domain oscilloscope plot of a band-limited square wave. Notice the reduced amount of discontinuity at the edges of the waveshape.",
null,
"Figure 5: Time domain oscilloscope plot of a naive, non band-limited square wave Notice the amount of discontinuity at the edges of the waveshape",
null,
"Figure 6: Time domain oscilloscope plot of a band-limited square wave Notice the reduced amount of discontinuity at the edges of the waveshape\n\n## Quasi Solution?\n\nThere are a number of ways around this problem. The most obvious may be to use different techniques to generate our oscillator in the first place that bypass the problem. This is a common solution and several options exist. A frequency limited Fourier series representation can be used to generate an aliasing free signal, or additive synthesis techniques could be used. However, these may both be computationally expensive. Another technique is that a wave is precalculated using a mathematical equation, and stored in memory (i.e. a table). We then use a look-up table technique to read the values from the table to generate our oscillator. This is a technique known as a wavetable (or look-up table) oscillator. However, clever tricks are needed here to ensure the wavetable oscillator is band-limited and free from other types of distortion (i.e. quantization & interpolation distortion). So what’s the solution? Well, one of the most popular techniques is really a compromise – we allow a little bit of aliasing as long as the aliased components are far away from the fundamental frequency and low in amplitude. For example, if we trigger our band-limited oscillator with a fundamental frequency of approx~ 2kHz (which is C6 on a MIDI keyboard), we may expect to see aliased components stretching down to somewhere in the region of -60dB at approx~ 10kHz. Remember, the dynamic range of the human ear is considered to be 130dB and arguably aliased components at -60dB would be difficult, if not impossible, to hear. Don’t believe me? Take this test to find out.\n\nAs these modern techniques don’t really remove aliasing, they suppress it enough so we cant hear it, they are known as quasi band-limited techniques. So this links nicely back to our opening paragraph – the most important and deployed approach in digital synthesizer design within the modern landscape is the use of quasi band-limited oscillators to reduce aliasing. ‘Ok – got it, but how does it work?’ I hear you say. In our next blog post, entitled ‘All About Digital Oscillators Part 2 – BLITS & BLEPS’ we will explore how these techniques work. So for now, happy wiggling."
]
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null
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https://projecteuclid.org/proceedings/geometry-integrability-and-quantization/Proceedings-of-the-Seventeenth-International-Conference-on-Geometry-Integrability-and/Chapter/Functionals-on-Toroidal-Surfaces/10.7546/giq-17-2016-270-283 | [
"Translator Disclaimer\nVOL. 17 | 2016 Functionals on Toroidal Surfaces\nMetin Gürses\n\nEditor(s) Ivaïlo M. Mladenov, Guowu Meng, Akira Yoshioka\n\nAbstract\n\nWe show that the torus in ${\\mathbb R}^3$ is a critical point of a sequence of functionals ${\\mathcal F}_{n}$ ($n=1,2,3, \\ldots$) defined over compact surfaces (closed membranes) in ${\\mathbb R}^3$. When the Lagrange function ${\\mathcal E}$ is a polynomial of degree $n$ of the mean curvature $H$ of the torus, the radii ($a,r$) of the torus are constrained to satisfy $\\frac{a^2}{r^2}=\\frac{n^2-n}{n^2-n-1},~~ n \\ge 2$. A simple generalization of torus in ${\\mathbb R}^3$ is a tube of radius $r$ along a curve ${\\bf \\alpha}$ which we call it toroidal surface (TS). We show that toroidal surfaces with non-circular curve ${\\bf \\alpha}$ do not provide minimal energy surfaces of the functionals ${\\mathcal F}_{n}$ ($n=2,3$) on closed surfaces. We discuss possible applications of the functionals discussed in this work on cell membranes.\n\nInformation\n\nPublished: 1 January 2016\nFirst available in Project Euclid: 15 December 2015\n\nzbMATH: 1346.53012\nMathSciNet: MR3445435\n\nDigital Object Identifier: 10.7546/giq-17-2016-270-283",
null,
"",
null,
""
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null,
"https://projecteuclid.org/Content/themes/SPIEImages/Share_black_icon.png",
null,
"https://projecteuclid.org/images/proceedings/cover_pgiq.jpg",
null
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https://www.thelearningpoint.net/computer-science/python-for-data-5-data-analysis-with-pandas-basic | [
"Computer Science > \n\n### Why pandas ?\n\nThere are many data analysis tools available, so why pandas ?\nIf you've spent time in a spreadsheet software like Microsoft Excel, Apple Numbers, or Google Sheets and are eager to take your data analysis skills to the next level, this tutorial is for you! and you are at the right place.\n\nPandas is a powerful tool that allows you to do anything and everything with colossal data sets. These are the major task that we performs, analyzing, organizing, sorting, filtering, pivoting, aggregating, munging, cleaning, calculating, and more! We can say it's \"Excel on steroids\"!\n\nHere one can find data set (also available in the reference) on which we are gonna analyse some important statistics. Here we are gonna use 3 python libraries. pandas for data analysis, numpy for calculation and mathematics and lastly matplotlib for visualization of graphs.\nYou can see that we have 128 rows and 8 columns here. we are going to perform following task with this 'house.csv' data set.\n\n1. Load the data using pandas\n\n2. Summarize each field in the data, i.e. mean, average etc.\n\n3. Group data by the field [nbhd].\n\n(a) Give average sqft, average price and average bedroom of each group.\n\n(b) Plot for each field ([sqft], [bedroom], [price] etc). Use a boxplot that visualizes the statistical information about them.\n\n(c) For each group of [nbhd], draw a prediction line for [price] vs [sqft]\n\nHere we are gonna see the data description i.e. Mean, max, standard deviation etc. of each column. 'Transpose' here is working similar to matrix transpose where it rotate our columns. see below - Now let's summarize our data using pandas 'groupby'Here is the output of this line of our code. we want to plot the dependency of prices on the size of the house and number of bathrooms ans so on. Therefore, we used 'groupby' here. Boxplots of (sqft, bedroom, price) with respect to \"nbhd\" groupby field.Prediction line plot \"price vs sqft\" for \"nbhd\"= nbhd01Here one can see the plot and nice visualization by 'matplotlib' libraryhere you see, how price is increasing with respect to square fit/size of the house for group 01 i.e. [nbhd01]. Now let's see for second group. here is the plot. Similarly for last group [nbhd03Here we are done with basic pandas operations. We have seen how we can visualize data and it's analysis. We saw how price is dependent on size of the house and other factor among 3 groups of house data.\n\n### What's Next\n\nLinear Regression via Normal Equations using same 'house.csv' data.\nwhere we will learn below matrix decomposition methods to perform Linear regression.\n(a) Gaussian elimination\n(b) Cholesky decomposition\n(c) QR decomposition"
]
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null
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https://www.findfilo.com/maths-question-answers/if-lim-xvec0-a-e-x-b-x-2-then-find-the-value-of-aa3m2 | [
"",
null,
"If (\"lim\")_(xvec0)(a e^x-b)/x = 2 , then find the value of aa n d | Filo",
null,
"",
null,
"Class 11\n\nMath\n\nCalculus\n\nLimits And Derivatives",
null,
"563\n\nIf then find the value of",
null,
"563",
null,
"Connecting you to a tutor in 60 seconds."
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.71354574,"math_prob":0.9958686,"size":671,"snap":"2021-31-2021-39","text_gpt3_token_len":241,"char_repetition_ratio":0.11694153,"word_repetition_ratio":0.0,"special_character_ratio":0.29955292,"punctuation_ratio":0.11612903,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.97772956,"pos_list":[0,1,2,3,4,5,6,7,8,9,10,11,12],"im_url_duplicate_count":[null,null,null,null,null,null,null,null,null,null,null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-07-30T17:51:32Z\",\"WARC-Record-ID\":\"<urn:uuid:0c0c1a64-8d40-4eeb-9b69-8f5998d0701f>\",\"Content-Length\":\"71374\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:99aea219-a432-411c-9777-c7bbe8c9254e>\",\"WARC-Concurrent-To\":\"<urn:uuid:500234a2-fdb6-4453-9ad9-ad86d35fda5d>\",\"WARC-IP-Address\":\"34.117.94.82\",\"WARC-Target-URI\":\"https://www.findfilo.com/maths-question-answers/if-lim-xvec0-a-e-x-b-x-2-then-find-the-value-of-aa3m2\",\"WARC-Payload-Digest\":\"sha1:64B252GUV4BOMWCFPI6QQMBGTOV2E5RS\",\"WARC-Block-Digest\":\"sha1:BS7WAXZYYXKUKN2VIFJL3CSISFXCLEQO\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-31/CC-MAIN-2021-31_segments_1627046153971.20_warc_CC-MAIN-20210730154005-20210730184005-00319.warc.gz\"}"} |
http://irerahihu3.megafile.ru.net/fe_sample-stoichiometry-problems-and-answers-gy/qezer.htm | [
"##### Sample stoichiometry problems and answers",
null,
"Stoichiometry sat ii chemistry.",
null,
"Stoichiometry example problem 1 (video) | khan academy.",
null,
"Stoichiometry 7: limiting reagents and percentage yield calculations.",
null,
"## Icechart.",
null,
"Solution stoichiometry practice problems & examples finding.",
null,
"##### Stoichiometry with solutions problems.",
null,
"### Stoichiometry and balancing reactions chemistry libretexts.",
null,
"Ideal stoichiometry (practice) | khan academy.",
null,
"Chapter 13 – stoichiometry.",
null,
"###### Practice problems: stoichiometry (answer key).",
null,
"##### Stoichiometry problem | wyzant ask an expert.",
null,
"How do you solve a stoichiometry problem? + example.",
null,
"#### Worksheet stoichiometry ap level.",
null,
"Sparknotes: stoichiometric calculations: problems.",
null,
"# Solving stoichiometry problems.",
null,
"#### Stoichiometry (solutions, examples, videos).",
null,
"# Gas stoichiometry sample problems, assignment, and answers.",
null,
"Chemistry and more practice problems with answers.",
null,
"",
null,
"Chemteam: stoichiometry: mass-mass examples."
]
| [
null,
"https://i.ytimg.com/vi/TdpOZTPAKbg/maxresdefault.jpg",
null,
"https://i.ytimg.com/vi/Ab3wfKjaWWQ/maxresdefault.jpg",
null,
"http://intro.chem.okstate.edu/1314F97/Chapter4/Molarity7.1.GIF",
null,
"https://images.sampletemplates.com/wp-content/uploads/2016/11/17162322/Mass-to-Mass-Stoichiometry-Worksheet.jpg",
null,
"https://i.ytimg.com/vi/5RRVfI2fItk/maxresdefault.jpg",
null,
"http://www.chem.tamu.edu/class/fyp/stone/tutorialnotefiles/stoich9.gif",
null,
"http://alistairtheoptimist.org/wp-content/uploads/2018/02/ap-chemistry-page-practice-test-ch-14-wanswers-word-acrobat-and-worked-out-answers-.gif",
null,
"https://images.sampletemplates.com/wp-content/uploads/2016/11/17162238/Molarity-Stoichiometry-Worksheet.jpg",
null,
"https://images.sampletemplates.com/wp-content/uploads/2016/11/17162546/Stoichiometry-Practice-Worksheet.jpg",
null,
"http://intro.chem.okstate.edu/1314F97/Chapter4/Molarity8.GIF",
null,
"https://i.ytimg.com/vi/aB_S-C02bgM/maxresdefault.jpg",
null,
"http://colgurchemistry.com/Chem12/SCANNED%20KEYS/Worksheet3-2/Assignment3-2_KEYp3.jpg",
null,
"https://images.sampletemplates.com/wp-content/uploads/2016/11/17162152/Gas-Stoichiometry-Worksheet.jpg",
null,
"https://s3.studylib.net/store/data/008351429_1-690533bd35cd021cad902f8855cbaa92-260x520.png",
null,
"https://s3.studylib.net/store/data/008711874_1-d12f29b6b62688faeae95fc3bd7c9543-260x520.png",
null,
"http://www.colgurchemistry.com/Chem11/SCANNED%20KEYS/Un6ReviewKEY/Un6ReviewKEYp4.jpg",
null,
"https://i.ytimg.com/vi/F_TiekZIFgU/maxresdefault.jpg",
null,
"https://images.sampletemplates.com/wp-content/uploads/2016/11/17162413/Mole-to-Mole-Stoichiometry-Worksheet.jpg",
null,
"https://i.ytimg.com/vi/iTwQ9jX3xwM/hqdefault.jpg",
null,
"https://img.yumpu.com/52027820/1/358x462/stoichiometry-worksheet-answers.jpg",
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]
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https://www.ques10.com/p/16293/programming-in-c-data-structures-question-paper--1/ | [
"0\nProgramming in C & Data Structures : Question Paper Dec 2014 - First Year Engineering (C Cycle) (Semester 2) | Visveswaraya Technological University (VTU)\n\n## Programming in C and Data Structures - Dec 2014\n\n### First Year Engineering (C Cycle) (Semester 2)\n\nTOTAL MARKS: 100\nTOTAL TIME: 3 HOURS\n(1) Question 1 is compulsory.\n(2) Attempt any four from the remaining questions.\n(3) Assume data wherever required.\n(4) Figures to the right indicate full marks.\n1(a) What is pseudo code? How it is used as a prob lem-solving tool. (6 marks) 1(b) What is an operator? Explain the arithmetic, relational, logical, and assignment operators in C language. (10 marks) 1(c) Write a program in C to print the numbers from 4 to 9 and their squares. (4 marks) 10(a) Explain the array of pointers with example. (4 marks) 10(b) Write and explain any two preprocessor directives in C.(4 marks) 10(c) What is a stack? Explain it with its applications. (4 marks) 10(d) Write a C program to read n unsorted numbers to a n array of size n and pass the address of this array to a function to sort the numbers in ascending order using bubble sort technique. (8 marks) 2(a) Write and explain the basic concepts of a C program. (8 marks) 2(b) Write the guidelines to use printf() function in C language. (8 marks) 2(c) Write a program in C to find the area and perimeter of a circle. (4 marks) 3(a) Explain the two way selection (if, if-else, nested if- lse, cascaded if-else) in C language with syntax . (8 marks) 3(b) Explain the switch statement with syntax and example. (8 marks) 3(c) Design and develop a C program to read a year as an input and find whether it is leap year or not. Also consider end of the centuries. (4 marks) 4(a) Explain the different types of loops in C with syntax a nd example. (8 marks) 4(b) Explain the use of break and continue statement in loops with example. (6 marks) 4(c) Design and develop a C program to reverse of an integer number NUM and check whether it is PALINDROME or NOT. (6 marks) 5(a) What is an array? Explain the declaration and initialization of one and two dimensional arrays with example. (6 marks) 5(b) Explain void and parameter less functions in C with examples. (6 marks) 5(c) Write a C program that:\ni. Implements string copy operation STRCOPY (str1,str2) that copies a string str1 to another string str2 without using library function.\nii. Reads a sentence and prints frequency of each of the vowels and total count of consonants.\n(8 marks)\n6(a) Explain any five string manipulation library functions with examples. (10 marks) 6(b) What is function parameter? Explain different types of parameters in C functions. (4 marks) 6(c) Write a C function isprime (num) that accepts an integer argument and returns 1 if the argument is prime, a 0 otherwise. Write a C program that invokes this function to generate prime numbers between the given ranges. (6 marks) 7(a) What is a structure? Explain the syntax of structure declaration with example. (4 marks) 7(b) What is a file? Explain how the file open and file close functions handled in C. (6 marks) 7(c) Write a C program to maintain a record of n\"student details using an array of structures with four fields (Roll number(10 marks) 8(a) Explain array of structures and structure within a structure with examples. (8 marks) 8(b) Explain how the structure variable passed as a param eter to a function with example. (6 marks) 8(c) Write a C program to read and display a text from the file.(6 marks) 9(a) What is a pointer? Explain how the pointer variable de clared and initialized. (4 marks) 9(b) What is dynamic memory allocation? Write and explain the different dynamic memory allocation functions in C. (6 marks) 9(c) What are primitive and non-primitive data types? (4 marks) 9(d) Write a C program to swap two numbers using call by pointers method. (6 marks)\n\n0"
]
| [
null
]
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https://xianblog.wordpress.com/tag/ila/ | [
"## Hyper-g priors\n\nPosted in Books, R, Statistics with tags , , , , , , on August 31, 2010 by xi'an\n\nEarlier this month, Daniel Sabanés Bové and Leo Held posted a paper about g-priors on arXiv. While I glanced at it for a few minutes, I did not have the chance to get a proper look at it till last Sunday. The g-prior was first introduced by the late Arnold Zellner for (standard) linear models, but they can be extended to generalised linear models (formalised by the late John Nelder) at little cost. In Bayesian Core, Jean-Michel Marin and I do centre the prior modelling in both linear and generalised linear models around g-priors, using the naïve extension for generalised linear models,",
null,
"$\\beta \\sim \\mathcal{N}(0,g \\sigma^2 (\\mathbf{X}^\\text{T}\\mathbf{X})^{-1})$\n\nas in the linear case. Indeed, the reasonable alternative would be to include the true information matrix but since it depends on the parameter",
null,
"$\\beta$ outside the normal case this is not truly an alternative. Bové and Held propose a slightly different version",
null,
"$\\beta \\sim \\mathcal{N}(0,g \\sigma^2 c (\\mathbf{X}^\\text{T}\\mathbf{W}\\mathbf{X})^{-1})$\n\nwhere W is a diagonal weight matrix and c is a family dependent scale factor evaluated at the mode 0. As in Liang et al. (2008, JASA) and most of the current literature, they also separate the intercept",
null,
"$\\beta_0$ from the other regression coefficients. They also burn their “improperness joker” by choosing a flat prior on",
null,
"$\\beta_0$, which means they need to use a proper prior on g, again as Liang et al. (2008, JASA), for the corresponding Bayesian model comparison to be valid. In Bayesian Core, we do not separate",
null,
"$\\beta_0$ from the other regression coefficients and hence are left with one degree of freedom that we spend in choosing an improper prior on g instead. (Hence I do not get the remark of Bové and Held that our choice “prohibits Bayes factor comparisons with the null model“. As argued in Bayesian Core, the factor g being an hyperparameter shared by all models, we can use the same improper prior on g in all models and hence use standard Bayes factors.) In order to achieve closed form expressions, the authors use Cui and George ‘s (2008) prior",
null,
"$\\pi(g) \\propto (1+g)^{1+a}\\exp\\{-b/(1+g)\\}$\n\nwhich requires the two hyper-hyper-parameters a and b to be specified.\n\nThe second part of the paper considers computational issues. It compares the ILA solution of Rue, Martino and Chopin (2009, Series B) with an MCMC solution based on an independent proposal on g resulting from linear interpolations (?). The marginal likelihoods are approximated by Chib and Jeliazkov (2001, JASA) for the MCMC part. Unsurprisingly, ILA does much better, even with a 97% acceptance rate in the MCMC algorithm.\n\nThe paper is very well-written and quite informative about the existing literature. It also uses the Pima Indian dataset (The authors even dug out a 1991 paper of mine I had completely forgotten!) I am actually thinking of using the review in our revision of Bayesian Core, even though I think we should stick to our choice of including",
null,
"$\\beta_0$ within the set of parameters…"
]
| [
null,
"https://s0.wp.com/latex.php",
null,
"https://s0.wp.com/latex.php",
null,
"https://s0.wp.com/latex.php",
null,
"https://s0.wp.com/latex.php",
null,
"https://s0.wp.com/latex.php",
null,
"https://s0.wp.com/latex.php",
null,
"https://s0.wp.com/latex.php",
null,
"https://s0.wp.com/latex.php",
null
]
| {"ft_lang_label":"__label__en","ft_lang_prob":0.91915125,"math_prob":0.9290526,"size":2744,"snap":"2021-04-2021-17","text_gpt3_token_len":614,"char_repetition_ratio":0.09854015,"word_repetition_ratio":0.0,"special_character_ratio":0.21027696,"punctuation_ratio":0.08429119,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99097747,"pos_list":[0,1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16],"im_url_duplicate_count":[null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-04-15T05:11:48Z\",\"WARC-Record-ID\":\"<urn:uuid:1fa7eb40-1800-4c6d-b45d-7510228fbccf>\",\"Content-Length\":\"56856\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:971489ef-9c2c-4f00-bec2-3bd46bbdcd83>\",\"WARC-Concurrent-To\":\"<urn:uuid:da44ef2e-2615-4e9e-ab09-4357a0981b92>\",\"WARC-IP-Address\":\"192.0.78.13\",\"WARC-Target-URI\":\"https://xianblog.wordpress.com/tag/ila/\",\"WARC-Payload-Digest\":\"sha1:33XIHRORMNGLJ4VEBCVOX5NMLHLN2A6K\",\"WARC-Block-Digest\":\"sha1:732PPRBR27R4SCYMSJBXYIKEX3RAMGUS\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-17/CC-MAIN-2021-17_segments_1618038083007.51_warc_CC-MAIN-20210415035637-20210415065637-00295.warc.gz\"}"} |
https://mathhelpboards.com/threads/some-very-basic-questions-on-topology.2796/ | [
"# Some very basic questions on topology!\n\n#### Mathelogician\n\n##### Member\nhello everybody!\nMy knowledge in the field is so basic. So please answer as clear and simple as possible:\nThe following 4 questions are the ones i couldn't solve after trying!\n++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++\n\n1-Prove [0,1] is not isometric to [0,2].\n2-For which intervals [a,b] in R is the intersection of [a,b] and Q a clopen (closed and open) subset of the metric space Q?\n3-Find a metric space in which the boundary of Mr(p)={xEM :d(x,p)< r} is not equal to the sphere of radius r at p ,{xEM : d(x,p)=r}.\n4- For a subspace N of a metric space M,prove that if the openness of S c N is equivalent to openness of S in M, then N is open in M.\n============================================================\n\nThe next is about my proof of the following problem:\n\nLet (An) be a nested decreasing sequence of non-empty closed sets in the metric space M.\nIf M is complete(every Cauchy is convergent) and diam(An) -> 0 as n -> infinity, show that S=Intersection of (An) is exactly one point( note that diam X= sup{d(x,y): x,y E X} ).\nMy proof : (I use Euclidean metric on R for simplicity of the proof- it can be done for any other metric on R)\nLets x,y E S. we must show that d(x,y)=0.\nLets d(x,y)= t > 0. By the red part: there exists a N1 such that for all n>N1 , we have diam(An)<t\nLet k > n. So diam(Ak)<t.\nIn other hand, d(x,y) =< diam(Ak)< t. So d(x,y)< t which contradicts the blue.\n\nNow my question is : What was the usage of supposing Ai's as Closed subspaces of M and M's being complete, in this proof?\n\n#### Opalg\n\n##### MHB Oldtimer\nStaff member\nRe: Some very basic quastions on topology!\n\nhello everybody!\nMy knowledge in the field is so basic. So please answer as clear and simple as possible:\nThe following 4 questions are the ones i couldn't solve after trying!\n++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++\n\n1-Prove [0,1] is not isometric to [0,2]. The interval [0,2] contains two points whose distance apart is 2, but the interval [0,1] does not.\n2-For which intervals [a,b] in R is the intersection of [a,b] and Q a clopen (closed and open) subset of the metric space Q? Think about what difference it makes whether a and b are rational or irrational.\n3-Find a metric space in which the boundary of Mr(p)={xEM :d(x,p)< r} is not equal to the sphere of radius r at p ,{xEM : d(x,p)=r}. Think about a space with a discrete metric.\n4- For a subspace N of a metric space M, prove that if the openness of S c N is equivalent to openness of S in M, then N is open in M. What happens if you take S = N?\n============================================================\n(See the hints in red.)\n\nThe next is about my proof of the following problem:\nLet (An) be a nested decreasing sequence of non-empty closed sets in the metric space M.\nIf M is complete(every Cauchy is convergent) and diam(An) -> 0 as n -> infinity, show that S=Intersection of (An) is exactly one point( note that diam X= sup{d(x,y): x,y E X} ).\nMy proof : (I use Euclidean metric on R for simplicity of the proof- it can be done for any other metric on R)\nLets x,y E S. we must show that d(x,y)=0.\nLets d(x,y)= t > 0. By the red part: there exists a N1 such that for all n>N1 , we have diam(An)<t\nLet k > n. So diam(Ak)<t.\nIn other hand, d(x,y) =< diam(Ak)< t. So d(x,y)< t which contradicts the blue.\n\nNow my question is : What was the usage of supposing Ai's as Closed subspaces of M and M's being complete, in this proof?\nYour proof shows that S cannot contain more than one point. But how do you know that it contains any points at all? Answer: You need those extra conditions to ensure that S is not empty."
]
| [
null
]
| {"ft_lang_label":"__label__en","ft_lang_prob":0.9178247,"math_prob":0.99695724,"size":2841,"snap":"2021-31-2021-39","text_gpt3_token_len":789,"char_repetition_ratio":0.17377512,"word_repetition_ratio":0.8023256,"special_character_ratio":0.36149243,"punctuation_ratio":0.13364056,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9979302,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-09-20T23:07:22Z\",\"WARC-Record-ID\":\"<urn:uuid:fe8c3530-1a2e-4edc-9912-e80e2dad2f21>\",\"Content-Length\":\"60301\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:d4e9c8c4-0c35-4afc-8085-c800a7c0066b>\",\"WARC-Concurrent-To\":\"<urn:uuid:574cd4be-034f-462b-874a-67e40e2be1f9>\",\"WARC-IP-Address\":\"50.31.99.218\",\"WARC-Target-URI\":\"https://mathhelpboards.com/threads/some-very-basic-questions-on-topology.2796/\",\"WARC-Payload-Digest\":\"sha1:AQ3WQX6AKUVWPG7IO6KT7NCVD5AGQAKP\",\"WARC-Block-Digest\":\"sha1:GC64WXQYLGXQEA2WWE56I7A6IHFHKYLZ\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-39/CC-MAIN-2021-39_segments_1631780057119.85_warc_CC-MAIN-20210920221430-20210921011430-00099.warc.gz\"}"} |
https://neon-lang.dev/html/files/binary-neon.html | [
"# binary\n\nBitwise binary logical operations on 32-bit words.\n\nSummary\n binary Bitwise binary logical operations on 32-bit words. Functions and32 Bitwise logical “and” of two 32-bit words. and64 Bitwise logical “and” of two 64-bit words. andBytes Bitwise logical “and” of two Bytes buffers. extract32 Extract a range of bits from a 32-bit word. extract64 Extract a range of bits from a 64-bit word. get32 Get a specific bit from a 32-bit word. get64 Get a specific bit from a 64-bit word. not32 Invert all bits in a 32-bit word. not64 Invert all bits in a 64-bit word. notBytes Invert all bits in a Bytes buffer. or32 Bitwise logical “or” of two 32-bit words. or64 Bitwise logical “or” of two 64-bit words. orBytes Bitwise logical “or” of two Bytes buffers. replace32 Replace a range of bits in a 32-bit word. replace64 Replace a range of bits in a 64-bit word. set32 Set a specific bit in a 32-bit word. set64 Set a specific bit in a 64-bit word. shiftLeft32 Shift a 32-bit word left by a given number of bits. shiftLeft64 Shift a 64-bit word left by a given number of bits. shiftRight32 Shift a 32-bit word right by a given number of bits. shiftRight64 Shift a 64-bit word right by a given number of bits. shiftRightSigned32 Shift a 32-bit word right by a given number of bits, preserving the sign bit. shiftRightSigned64 Shift a 64-bit word right by a given number of bits, preserving the sign bit. xor32 Bitwise logical “exclusive-or” of two 32-bit words. xor64 Bitwise logical “exclusive-or” of two 64-bit words. xorBytes Bitwise logical “exclusive-or” of two Bytes buffers.\n\n### and32\n\n DECLARE NATIVE FUNCTION and32( x, y: Number ): Number\n\nBitwise logical “and” of two 32-bit words.\n\nFor each bit in the inputs, the following truth table determines the output bit:\n\n``` | 0 | 1 | <- x\n---+---+---+\n0 | 0 | 0 |\n---+---+---+\n1 | 0 | 1 |\n---+---+---+\n^\ny```\n\n### and64\n\n DECLARE NATIVE FUNCTION and64( x, y: Number ): Number\n\nBitwise logical “and” of two 64-bit words.\n\nFor each bit in the inputs, the following truth table determines the output bit:\n\n``` | 0 | 1 | <- x\n---+---+---+\n0 | 0 | 0 |\n---+---+---+\n1 | 0 | 1 |\n---+---+---+\n^\ny```\n\n### andBytes\n\n DECLARE NATIVE FUNCTION andBytes( x, y: Bytes ): Bytes\n\nBitwise logical “and” of two Bytes buffers. The size of both input parameters must be the same.\n\nFor each bit in the inputs, the following truth table determines the output bit:\n\n``` | 0 | 1 | <- x\n---+---+---+\n0 | 0 | 0 |\n---+---+---+\n1 | 0 | 1 |\n---+---+---+\n^\ny```\n\n### extract32\n\n DECLARE NATIVE FUNCTION extract32( x, n, w: Number ): Number\n\nExtract a range of bits from a 32-bit word.\n\n#### Parameters\n\n x number to extract bits from n bit position of the lowest order bit to extract w width of bit range to extract\n\n#### Description\n\nThis function extracts a given range of bits. The bits in an word are numbered starting at 0 for the least significant bit.\n\nThe function call\n\n`binary.extract(x, 5, 3)`\n\nwill extract the following bits from the word\n\n```31 28 24 20 16 12 8 4 0\n+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+\n| | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | |\n+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+\n| |\n+-----+```\n\n### extract64\n\n DECLARE NATIVE FUNCTION extract64( x, n, w: Number ): Number\n\nExtract a range of bits from a 64-bit word.\n\n#### Parameters\n\n x number to extract bits from n bit position of the lowest order bit to extract w width of bit range to extract\n\n#### Description\n\nThis function extracts a given range of bits. The bits in an word are numbered starting at 0 for the least significant bit.\n\nThe function call\n\n`binary.extract(x, 5, 3)`\n\nwill extract the following bits from the word\n\n```31 28 24 20 16 12 8 4 0\n+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+\n| | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | |\n+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+\n| |\n+-----+```\n\n### get32\n\n DECLARE NATIVE FUNCTION get32( x, n: Number ): Boolean\n\nGet a specific bit from a 32-bit word.\n\n#### Parameters\n\n x number to extract the bit from n bit position of the bit to extract\n\n#### Description\n\nThis function returns a Boolean value indicting whether the indicated bit is set (TRUE) or not (FALSE).\n\n### get64\n\n DECLARE NATIVE FUNCTION get64( x, n: Number ): Boolean\n\nGet a specific bit from a 64-bit word.\n\n#### Parameters\n\n x number to extract the bit from n bit position of the bit to extract\n\n#### Description\n\nThis function returns a Boolean value indicting whether the indicated bit is set (TRUE) or not (FALSE).\n\n### not32\n\n DECLARE NATIVE FUNCTION not32( x: Number ): Number\n\nInvert all bits in a 32-bit word.\n\n### not64\n\n DECLARE NATIVE FUNCTION not64( x: Number ): Number\n\nInvert all bits in a 64-bit word.\n\n### notBytes\n\n DECLARE NATIVE FUNCTION notBytes( x: Bytes ): Bytes\n\nInvert all bits in a Bytes buffer.\n\n### or32\n\n DECLARE NATIVE FUNCTION or32( x, y: Number ): Number\n\nBitwise logical “or” of two 32-bit words.\n\nFor each bit in the inputs, the following truth table determines the output bit:\n\n``` | 0 | 1 | <- x\n---+---+---+\n0 | 0 | 1 |\n---+---+---+\n1 | 1 | 1 |\n---+---+---+\n^\ny```\n\n### or64\n\n DECLARE NATIVE FUNCTION or64( x, y: Number ): Number\n\nBitwise logical “or” of two 64-bit words.\n\nFor each bit in the inputs, the following truth table determines the output bit:\n\n``` | 0 | 1 | <- x\n---+---+---+\n0 | 0 | 1 |\n---+---+---+\n1 | 1 | 1 |\n---+---+---+\n^\ny```\n\n### orBytes\n\n DECLARE NATIVE FUNCTION orBytes( x, y: Bytes ): Bytes\n\nBitwise logical “or” of two Bytes buffers. The size of both input parameters must be the same.\n\nFor each bit in the inputs, the following truth table determines the output bit:\n\n``` | 0 | 1 | <- x\n---+---+---+\n0 | 0 | 1 |\n---+---+---+\n1 | 1 | 1 |\n---+---+---+\n^\ny```\n\n### replace32\n\n DECLARE NATIVE FUNCTION replace32( x, n, w, y: Number ): Number\n\nReplace a range of bits in a 32-bit word.\n\n#### Parameters\n\n x number to replace bits into n bit position of the lowest order bit to replace w width of bit range to replace y new bits to replace\n\n#### Description\n\nThis function replaces a given range of bits with new bits. The bits in an word are numbered starting at 0 for the least significant bit.\n\nThe function call\n\n`binary.replace(x, 5, 3, 7)`\n\nwill replace the following bits in the word\n\n```31 28 24 20 16 12 8 4 0\n+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+\n| | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | |\n+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+\n| |\n+-----+```\n\nEach of the bits numbered 5, 6, and 7 would be set to 1 (from the input value 7).\n\n### replace64\n\n DECLARE NATIVE FUNCTION replace64( x, n, w, y: Number ): Number\n\nReplace a range of bits in a 64-bit word.\n\n#### Parameters\n\n x number to replace bits into n bit position of the lowest order bit to replace w width of bit range to replace y new bits to replace\n\n#### Description\n\nThis function replaces a given range of bits with new bits. The bits in an word are numbered starting at 0 for the least significant bit.\n\nThe function call\n\n`binary.replace(x, 5, 3, 7)`\n\nwill replace the following bits in the word\n\n```31 28 24 20 16 12 8 4 0\n+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+\n| | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | |\n+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+\n| |\n+-----+```\n\nEach of the bits numbered 5, 6, and 7 would be set to 1 (from the input value 7).\n\n### set32\n\n DECLARE NATIVE FUNCTION set32( x, n: Number, v: Boolean ): Number\n\nSet a specific bit in a 32-bit word.\n\n#### Parameters\n\n x number to set the bit n bit position of the bit to set v bit value to set, 0 (FALSE) or 1 (TRUE)\n\n#### Description\n\nThis function returns a new value with the given bit set according to the parameter v.\n\n### set64\n\n DECLARE NATIVE FUNCTION set64( x, n: Number, v: Boolean ): Number\n\nSet a specific bit in a 64-bit word.\n\n#### Parameters\n\n x number to set the bit n bit position of the bit to set v bit value to set, 0 (FALSE) or 1 (TRUE)\n\n#### Description\n\nThis function returns a new value with the given bit set according to the parameter v.\n\n### shiftLeft32\n\n DECLARE NATIVE FUNCTION shiftLeft32( x, n: Number ): Number\n\nShift a 32-bit word left by a given number of bits.\n\n#### Parameters\n\n x word to shift n number of bits to shift left\n\n#### Description\n\nNew bits shifted into the right hand side of the word are 0.\n\n### shiftLeft64\n\n DECLARE NATIVE FUNCTION shiftLeft64( x, n: Number ): Number\n\nShift a 64-bit word left by a given number of bits.\n\n#### Parameters\n\n x word to shift n number of bits to shift left\n\n#### Description\n\nNew bits shifted into the right hand side of the word are 0.\n\n### shiftRight32\n\n DECLARE NATIVE FUNCTION shiftRight32( x, n: Number ): Number\n\nShift a 32-bit word right by a given number of bits.\n\n#### Parameters\n\n x word to shift n number of bits to shift right\n\n#### Description\n\nNew bits shifted into the left hand side of the word are 0.\n\n### shiftRight64\n\n DECLARE NATIVE FUNCTION shiftRight64( x, n: Number ): Number\n\nShift a 64-bit word right by a given number of bits.\n\n#### Parameters\n\n x word to shift n number of bits to shift right\n\n#### Description\n\nNew bits shifted into the left hand side of the word are 0.\n\n### shiftRightSigned32\n\n DECLARE NATIVE FUNCTION shiftRightSigned32( x, n: Number ): Number\n\nShift a 32-bit word right by a given number of bits, preserving the sign bit.\n\n#### Parameters\n\n x word to shift n number of bits to shift right\n\n#### Description\n\nNew bits shifted into the left hand side of the word are the same as the original leftmost bit.\n\n### shiftRightSigned64\n\n DECLARE NATIVE FUNCTION shiftRightSigned64( x, n: Number ): Number\n\nShift a 64-bit word right by a given number of bits, preserving the sign bit.\n\n#### Parameters\n\n x word to shift n number of bits to shift right\n\n#### Description\n\nNew bits shifted into the left hand side of the word are the same as the original leftmost bit.\n\n### xor32\n\n DECLARE NATIVE FUNCTION xor32( x, y: Number ): Number\n\nBitwise logical “exclusive-or” of two 32-bit words.\n\nFor each bit in the inputs, the following truth table determines the output bit:\n\n``` | 0 | 1 | <- x\n---+---+---+\n0 | 0 | 1 |\n---+---+---+\n1 | 1 | 0 |\n---+---+---+\n^\ny```\n\n### xor64\n\n DECLARE NATIVE FUNCTION xor64( x, y: Number ): Number\n\nBitwise logical “exclusive-or” of two 64-bit words.\n\nFor each bit in the inputs, the following truth table determines the output bit:\n\n``` | 0 | 1 | <- x\n---+---+---+\n0 | 0 | 1 |\n---+---+---+\n1 | 1 | 0 |\n---+---+---+\n^\ny```\n\n### xorBytes\n\n DECLARE NATIVE FUNCTION xorBytes( x, y: Bytes ): Bytes\n\nBitwise logical “exclusive-or” of two Bytes buffers. The size of both input parameters must be the same.\n\nFor each bit in the inputs, the following truth table determines the output bit:\n\n``` | 0 | 1 | <- x\n---+---+---+\n0 | 0 | 1 |\n---+---+---+\n1 | 1 | 0 |\n---+---+---+\n^\ny```\n DECLARE NATIVE FUNCTION and32( x, y: Number ): Number\nBitwise logical “and” of two 32-bit words.\n DECLARE NATIVE FUNCTION and64( x, y: Number ): Number\nBitwise logical “and” of two 64-bit words.\n DECLARE NATIVE FUNCTION andBytes( x, y: Bytes ): Bytes\nBitwise logical “and” of two Bytes buffers.\n DECLARE NATIVE FUNCTION extract32( x, n, w: Number ): Number\nExtract a range of bits from a 32-bit word.\n DECLARE NATIVE FUNCTION extract64( x, n, w: Number ): Number\nExtract a range of bits from a 64-bit word.\n DECLARE NATIVE FUNCTION get32( x, n: Number ): Boolean\nGet a specific bit from a 32-bit word.\n DECLARE NATIVE FUNCTION get64( x, n: Number ): Boolean\nGet a specific bit from a 64-bit word.\n DECLARE NATIVE FUNCTION not32( x: Number ): Number\nInvert all bits in a 32-bit word.\n DECLARE NATIVE FUNCTION not64( x: Number ): Number\nInvert all bits in a 64-bit word.\n DECLARE NATIVE FUNCTION notBytes( x: Bytes ): Bytes\nInvert all bits in a Bytes buffer.\n DECLARE NATIVE FUNCTION or32( x, y: Number ): Number\nBitwise logical “or” of two 32-bit words.\n DECLARE NATIVE FUNCTION or64( x, y: Number ): Number\nBitwise logical “or” of two 64-bit words.\n DECLARE NATIVE FUNCTION orBytes( x, y: Bytes ): Bytes\nBitwise logical “or” of two Bytes buffers.\n DECLARE NATIVE FUNCTION replace32( x, n, w, y: Number ): Number\nReplace a range of bits in a 32-bit word.\n DECLARE NATIVE FUNCTION replace64( x, n, w, y: Number ): Number\nReplace a range of bits in a 64-bit word.\n DECLARE NATIVE FUNCTION set32( x, n: Number, v: Boolean ): Number\nSet a specific bit in a 32-bit word.\n DECLARE NATIVE FUNCTION set64( x, n: Number, v: Boolean ): Number\nSet a specific bit in a 64-bit word.\n DECLARE NATIVE FUNCTION shiftLeft32( x, n: Number ): Number\nShift a 32-bit word left by a given number of bits.\n DECLARE NATIVE FUNCTION shiftLeft64( x, n: Number ): Number\nShift a 64-bit word left by a given number of bits.\n DECLARE NATIVE FUNCTION shiftRight32( x, n: Number ): Number\nShift a 32-bit word right by a given number of bits.\n DECLARE NATIVE FUNCTION shiftRight64( x, n: Number ): Number\nShift a 64-bit word right by a given number of bits.\n DECLARE NATIVE FUNCTION shiftRightSigned32( x, n: Number ): Number\nShift a 32-bit word right by a given number of bits, preserving the sign bit.\n DECLARE NATIVE FUNCTION shiftRightSigned64( x, n: Number ): Number\nShift a 64-bit word right by a given number of bits, preserving the sign bit.\n DECLARE NATIVE FUNCTION xor32( x, y: Number ): Number\nBitwise logical “exclusive-or” of two 32-bit words.\n DECLARE NATIVE FUNCTION xor64( x, y: Number ): Number\nBitwise logical “exclusive-or” of two 64-bit words.\n DECLARE NATIVE FUNCTION xorBytes( x, y: Bytes ): Bytes\nBitwise logical “exclusive-or” of two Bytes buffers."
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https://www.economicsdiscussion.net/demand-curve/single-firms-demand-curve-for-capital/20670 | [
"Keynes defined the marginal efficiency of capital (MEC) as the rate of discount, e, that will just equate the present value of the flow of receipts a capital good (such as a machine) generates equal to its purchase price.\n\nIf the future cash flow or monetary return that can be obtained (expected) from a piece of capital is assumed to remain uniform throughout we can calculate the MEC by applying the following simple formula:\n\nC = R/e\n\nwhere C is the purchase price of the piece of capital, R is its constant flow of gross returns and e is the unknown value of MEC.\n\nNow we can easily solve for e by using this formula:\n\ne = R/C\n\nIf we assume that a firm is having a large number of capital equipment and is making a decision, at the margin, to acquire one extra unit of capital, we may call the e associated with this marginal addition to the firm’s stock of capital the MEC.\n\nHere e is the efficiency of any unit of capital, and MEC is the efficiency of the marginal unit. What is true of a firm is equally true of society. So we can refer to MEC for the whole economy.\n\nWe have noted earlier that the value to the firm now of a flow of future cash flows is its present value while the purchase price is the cost to the firm now of the capital that produces that flow of receipts. While the former is the addition to revenue made by an extra cost of acquiring the piece of capital the latter is the extra cost of acquiring the piece of capital.\n\nAccording to the famous marginal productivity theory of income distribution a profit-maximizing firm will go on adding units of capital so long as its marginal revenue product (MRP) exceeds it cost. Thus a firm will go on adding to its existing stock of capital as long as the present value of the flow of receipts from the marginal units exceeds the purchase price.\n\nThe value of e is the rate of discount which makes the two (R) and (C) equal. But we calculate the present value on the basis of the market rate of interest (r). (This is exactly what we have done earlier in this section).\n\nThus, when MEC is exactly equal to r, the present value of future cash flows from the marginal unit of capital equals its current purchase price (or acquisition cost). When this happens the firm’s capital stock is said to be in equilibrium and firm would no longer consider it worthwhile to add another unit of capital.\n\nAn interesting question that arises at this stage is the following: How does the firm take decision regarding whether or not to acquire (buy) one extra unit of capital?\n\nThe usual method used by modern business firms is to use the market rate of interest to arrive at the present value of the gross return. Then, in the next step, it has to be compared with the purchase price of the piece of equipment. A simple example, may make the point clear.\n\nLet us suppose that a firm can buy a machine for Rs. 8,000. It is expected to yield Rs. 1,000 per annum, net of all non-capital costs, for an indefinite period. Also suppose that the market rate of interest at which it can borrow (and lend) money is 10 per cent. Thus, the present value of the future cash flow generated by the machine (i.e., the capitalized value of the machine) is R/r = Rs. 1000/0.10= Rs. 10,000.\n\nOn the other hand the present value of Rs. 8,000 today is (obviously) Rs. 8,000. The firm can make a gain if it purchases the machine for Rs. 8,000 to derive an income of Rs. 10,000. We may alternatively suppose that the firm is left with two options—either to buy the machine or lend the money (Rs. 8,000) at 10 per cent interest.\n\nThe firm would prefer to buy the machine because, by doing do, it can get an income of Rs. 1000. On the other hand if it lends the money at 10 per cent interest, it gets, at the end of a year, a sum of Rs. 800 as interest.\n\nThus, it is quite clear that the first option is better than the second one.\n\nSo as a general rule a profit- maximizing firm will purchase a capital good like a machine if the following condition holds:\n\nR/r > C\n\nwhere R is the infinite stream of future (gross) cash flows. The term R/r is the present value of the stream of gross cash flows generated by the capital good, i.e., the capitalized value of the machine.\n\nIt will, therefore, be worthwhile, on the part of a profit-maximizing firm, to purchase a capital good as and when the present value of its future stream of gross returns exceeds the purchase price of the good.\n\nThe above inequality may also be expressed in the an alternative way:\n\nR/C > r\n\nBut R/C is the MEC. So we obtain the following rule of investment decision at the micro level, i.e., at the level of an individual firm: it is always profitable for a firm to acquire extra units of capital whenever its MEC exceeds the market rate of interest.\n\nLooked at from this angle, MEC measures the return on an extra (marginal unit of capital to the firm, while r is a measure of the opportunity cost of capital (always assuming that the firm can borrow and lend at the existing market rate of interest, which is 10 per cent in our example).\n\nA firm’s MEC curve is shown is Fig. 32.5. It is a schedule that relates the efficiency of each additional rupee’s worth of capital to the size of the capital stock. On the horizontal axis we measure the value of the firm’s capital stock. On the vertical axis we measure the money value of the product of capital, expressed in terms of percentage yields on that capital.\n\nThe MEC curve is downward sloping, as stated earlier, due to the operation of the law of diminishing returns. .Thus, in Fig. 32.5 when the stock of capital is k1 the MEC is r1. When the stock of capital increases to k2 the MEC falls to r2 and so on.\n\nIn fact, the MEC curve is known as the firm’s demand curve for capital. It shows the amount of capital that a firm would choose to employ at different costs of employing it (i.e., at different rates of interest). The MEC curve is indeed the demand curve for capital of a firm because it shows how much capital the firm will demand at different prices, or yields, of capital.\n\nWe may note here that the cost of capital is the market rate of interest, i.e., the interest that the firm has to pay to borrow funds to acquire capital (or, for a firm that has generated funds internally, the cost of capital is the rate of interest that could be earned by lending them elsewhere).\n\nKeynes pointed out that so long as the MEC exceeds the rate of interest, net return from a project will be positive. So the firm will employ more capital. But as MEC gradually falls, it will ultimately be equal to r and the firm’s stock of capital will be optimum. This point may also be illustrated diagrammatically.\n\nSuppose in Fig. 32.5 the rate of interest (the cost of capital to the firm) is r1. Now the firm will certainly employ all capital upto k1 because the MEC is greater than the rate of interest. At the same time, it will not be profitable for the firm to employ, say, units of capital because the MEC of the k2-th unit of capital is less than the rate of interest.\n\nIn a like manner, it will not pay the firm to employ any capital in excess of k1. Hence k1 represents the optimum stock of capital of the firm, when the rate of interest is r1. Thus the equilibrium amount of capital of a profit-making firm is that at which the MEC is exactly equal to the rate of interest.\n\nThere is another way of establishing the fundamental principle stated above. In our previous example, a machine producing children’s toys was supposed to generate a yield of 10 per cent. If the market rate of interest is 10 per cent or less, it will be profitable to buy the machine: If the rate of interest is more than 10 per cent, it will not be profitable to buy or install it."
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https://www.colorhexa.com/59f1dc | [
"# #59f1dc Color Information\n\nIn a RGB color space, hex #59f1dc is composed of 34.9% red, 94.5% green and 86.3% blue. Whereas in a CMYK color space, it is composed of 63.1% cyan, 0% magenta, 8.7% yellow and 5.5% black. It has a hue angle of 171.7 degrees, a saturation of 84.4% and a lightness of 64.7%. #59f1dc color hex could be obtained by blending #b2ffff with #00e3b9. Closest websafe color is: #66ffcc.\n\n• R 35\n• G 95\n• B 86\nRGB color chart\n• C 63\n• M 0\n• Y 9\n• K 5\nCMYK color chart\n\n#59f1dc color description : Soft cyan.\n\n# #59f1dc Color Conversion\n\nThe hexadecimal color #59f1dc has RGB values of R:89, G:241, B:220 and CMYK values of C:0.63, M:0, Y:0.09, K:0.05. Its decimal value is 5894620.\n\nHex triplet RGB Decimal 59f1dc `#59f1dc` 89, 241, 220 `rgb(89,241,220)` 34.9, 94.5, 86.3 `rgb(34.9%,94.5%,86.3%)` 63, 0, 9, 5 171.7°, 84.4, 64.7 `hsl(171.7,84.4%,64.7%)` 171.7°, 63.1, 94.5 66ffcc `#66ffcc`\nCIE-LAB 87.094, -44.849, -1.74 48.489, 70.198, 78.7 0.246, 0.356, 70.198 87.094, 44.883, 182.222 87.094, -59.816, 4.531 83.784, -43.317, 2.956 01011001, 11110001, 11011100\n\n# Color Schemes with #59f1dc\n\n• #59f1dc\n``#59f1dc` `rgb(89,241,220)``\n• #f1596e\n``#f1596e` `rgb(241,89,110)``\nComplementary Color\n• #59f190\n``#59f190` `rgb(89,241,144)``\n• #59f1dc\n``#59f1dc` `rgb(89,241,220)``\n• #59baf1\n``#59baf1` `rgb(89,186,241)``\nAnalogous Color\n• #f19059\n``#f19059` `rgb(241,144,89)``\n• #59f1dc\n``#59f1dc` `rgb(89,241,220)``\n• #f159ba\n``#f159ba` `rgb(241,89,186)``\nSplit Complementary Color\n• #f1dc59\n``#f1dc59` `rgb(241,220,89)``\n• #59f1dc\n``#59f1dc` `rgb(89,241,220)``\n• #dc59f1\n``#dc59f1` `rgb(220,89,241)``\n• #6ef159\n``#6ef159` `rgb(110,241,89)``\n• #59f1dc\n``#59f1dc` `rgb(89,241,220)``\n• #dc59f1\n``#dc59f1` `rgb(220,89,241)``\n• #f1596e\n``#f1596e` `rgb(241,89,110)``\n• #14eacc\n``#14eacc` `rgb(20,234,204)``\n• #2aedd2\n``#2aedd2` `rgb(42,237,210)``\n• #41efd7\n``#41efd7` `rgb(65,239,215)``\n• #59f1dc\n``#59f1dc` `rgb(89,241,220)``\n• #71f3e1\n``#71f3e1` `rgb(113,243,225)``\n• #88f5e6\n``#88f5e6` `rgb(136,245,230)``\n• #a0f7eb\n``#a0f7eb` `rgb(160,247,235)``\nMonochromatic Color\n\n# Alternatives to #59f1dc\n\nBelow, you can see some colors close to #59f1dc. Having a set of related colors can be useful if you need an inspirational alternative to your original color choice.\n\n• #59f1b6\n``#59f1b6` `rgb(89,241,182)``\n• #59f1c3\n``#59f1c3` `rgb(89,241,195)``\n• #59f1cf\n``#59f1cf` `rgb(89,241,207)``\n• #59f1dc\n``#59f1dc` `rgb(89,241,220)``\n• #59f1e9\n``#59f1e9` `rgb(89,241,233)``\n• #59edf1\n``#59edf1` `rgb(89,237,241)``\n• #59e0f1\n``#59e0f1` `rgb(89,224,241)``\nSimilar Colors\n\n# #59f1dc Preview\n\nThis text has a font color of #59f1dc.\n\n``<span style=\"color:#59f1dc;\">Text here</span>``\n#59f1dc background color\n\nThis paragraph has a background color of #59f1dc.\n\n``<p style=\"background-color:#59f1dc;\">Content here</p>``\n#59f1dc border color\n\nThis element has a border color of #59f1dc.\n\n``<div style=\"border:1px solid #59f1dc;\">Content here</div>``\nCSS codes\n``.text {color:#59f1dc;}``\n``.background {background-color:#59f1dc;}``\n``.border {border:1px solid #59f1dc;}``\n\n# Shades and Tints of #59f1dc\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, #010f0d is the darkest color, while #fcfffe is the lightest one.\n\n• #010f0d\n``#010f0d` `rgb(1,15,13)``\n• #03211d\n``#03211d` `rgb(3,33,29)``\n• #04332d\n``#04332d` `rgb(4,51,45)``\n• #06453c\n``#06453c` `rgb(6,69,60)``\n• #07574c\n``#07574c` `rgb(7,87,76)``\n• #09695c\n``#09695c` `rgb(9,105,92)``\n• #0a7b6c\n``#0a7b6c` `rgb(10,123,108)``\n• #0c8e7c\n``#0c8e7c` `rgb(12,142,124)``\n• #0da08b\n``#0da08b` `rgb(13,160,139)``\n• #0fb29b\n``#0fb29b` `rgb(15,178,155)``\n• #11c4ab\n``#11c4ab` `rgb(17,196,171)``\n• #12d6bb\n``#12d6bb` `rgb(18,214,187)``\n• #14e8cb\n``#14e8cb` `rgb(20,232,203)``\n• #23ecd1\n``#23ecd1` `rgb(35,236,209)``\n• #35eed4\n``#35eed4` `rgb(53,238,212)``\n• #47efd8\n``#47efd8` `rgb(71,239,216)``\n• #59f1dc\n``#59f1dc` `rgb(89,241,220)``\n• #6bf3e0\n``#6bf3e0` `rgb(107,243,224)``\n• #7df4e4\n``#7df4e4` `rgb(125,244,228)``\n• #8ff6e7\n``#8ff6e7` `rgb(143,246,231)``\n• #a1f7eb\n``#a1f7eb` `rgb(161,247,235)``\n• #b3f9ef\n``#b3f9ef` `rgb(179,249,239)``\n• #c6faf3\n``#c6faf3` `rgb(198,250,243)``\n• #d8fcf7\n``#d8fcf7` `rgb(216,252,247)``\n• #eafdfb\n``#eafdfb` `rgb(234,253,251)``\n• #fcfffe\n``#fcfffe` `rgb(252,255,254)``\nTint Color Variation\n\n# Tones of #59f1dc\n\nA tone is produced by adding gray to any pure hue. In this case, #9eacaa is the less saturated color, while #4bffe6 is the most saturated one.\n\n• #9eacaa\n``#9eacaa` `rgb(158,172,170)``\n• #97b3af\n``#97b3af` `rgb(151,179,175)``\n• #90bab4\n``#90bab4` `rgb(144,186,180)``\n• #89c1b9\n``#89c1b9` `rgb(137,193,185)``\n• #83c7be\n``#83c7be` `rgb(131,199,190)``\n• #7ccec3\n``#7ccec3` `rgb(124,206,195)``\n• #75d5c8\n``#75d5c8` `rgb(117,213,200)``\n• #6edccd\n``#6edccd` `rgb(110,220,205)``\n• #67e3d2\n``#67e3d2` `rgb(103,227,210)``\n``#60ead7` `rgb(96,234,215)``\n• #59f1dc\n``#59f1dc` `rgb(89,241,220)``\n• #52f8e1\n``#52f8e1` `rgb(82,248,225)``\n• #4bffe6\n``#4bffe6` `rgb(75,255,230)``\nTone Color Variation\n\n# Color Blindness Simulator\n\nBelow, you can see how #59f1dc 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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| {"ft_lang_label":"__label__en","ft_lang_prob":0.5296015,"math_prob":0.6727387,"size":3711,"snap":"2021-43-2021-49","text_gpt3_token_len":1703,"char_repetition_ratio":0.12489884,"word_repetition_ratio":0.011111111,"special_character_ratio":0.53058475,"punctuation_ratio":0.23809524,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9812372,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-12-08T15:03:07Z\",\"WARC-Record-ID\":\"<urn:uuid:a696cd22-76ed-4f8e-897d-6dc0070be04b>\",\"Content-Length\":\"36203\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:5764220f-28bd-4f99-891f-45da2cdb5c09>\",\"WARC-Concurrent-To\":\"<urn:uuid:a662d2c0-2e12-4f2b-b561-07b114b7b0cf>\",\"WARC-IP-Address\":\"178.32.117.56\",\"WARC-Target-URI\":\"https://www.colorhexa.com/59f1dc\",\"WARC-Payload-Digest\":\"sha1:VP6O263H2BG2YIU3XJXCKNXIO7MMRTCW\",\"WARC-Block-Digest\":\"sha1:XM6Y7UWIKSC2FTDOMSAGDRJDO5KD3UBQ\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-49/CC-MAIN-2021-49_segments_1637964363515.28_warc_CC-MAIN-20211208144647-20211208174647-00264.warc.gz\"}"} |
https://www.jiskha.com/questions/1674867/1-how-fast-does-the-radius-of-a-spherical-soap-bubble-change-when-you-blow-air-into-it-at | [
"# 4 Calculus Related-Rates Problems\n\n1. How fast does the radius of a spherical soap bubble change when you blow air into it at the rate of 15 cubic centimeters per second? Our known rate is dV/dt, the change in volume with respect to time, which is 15 cubic centimeters per second. The rate we want to find is dr/dt, the change in the radius with respect to time. Remember that the volume of a sphere is V=4/3 pi r^3.\n\n2. A baseball diamond is a square 90 feet on a side. A player runs from first base to second base at a rate of 15 feet per second. At what rate is the player's distance from third base decreasing when the player is halfway between first and second base? We've already set part of this problem up. If we let x be the distance between the player and second base,and y be the distance between the player and third base, then dx/dt=-15 feet per second, and dy/dt will tell us what we want to know. Use the picture to find a relationship that will help you answer the question.\n\n3. A man 2 meters tall walks at the rate of 2 meters per second toward a streetlight that's 5 meters above the ground. At what rate is the tip of his shadow moving? We've already set this up part of the way. We know that dx/dt=-2 meters per second, and we're looking for dv/dt . Use the picture to help you find the relationship between x and y, and use it to answer the question asked here.\n\n4. Here's one we haven't worked with before: A circular oil slick of uniform thickness is caused by a spill of 1 cubic meter of oil. The thickness of the oil is decreasing at the rate of 0.1 cm/hr as the slick spreads. (Note: 1 cm = 0.01 m.) At what rate is the radius of the slick increasing when the radius is 8 meters? (You can think of this oil slick as a very flat cylinder; its volume is given by V = pi(r^2)h, where r is the radius and h is the height of this cylinder.)\n\n1. 👍\n2. 👎\n3. 👁\n1. These are all just applications of the chain rule. If y is a function of u, and u is a function of t, then\ndy/dt = dy/du * du/dt\n\nSo, now we see what do do:\n#1\nv=4/3 π r^3\ndv/dt = 4πr^2 dr/dt\ndr/dt = 15/(4πr^2)\nAs expected, if the volume changes at a steady rate, the bigger the balloon gets, the slower the radius increases.\n\n#2\nUsing the Pythagorean Theorem, we know that\n\nx^2 + 90^2 = y^2\nx dx/dt = y dy/dt\nSo, find y when x=45, and then just plug in dx/dt = -15\n\n#3\nYou don't say what y is, but suppose y is the distance of the tip of the shadow from the man. In that case, using similar triangles,\n\ny/2 = (x+y)/5\ny = 2/3 x\nSo,\ndy/dt = 2/3 dx/dt\n\n#4\n1st way: use the product rule\nv = πr^2h\ndv/dt = 2πrh dr/dt + πr^2 dh/dt\nYou know that dv/dt=0, since the volumem of oil is constant.\nNow, what is h? πr^2h = 1, so h = 1/(π*.01^2)\nNow you can plug in the numbers.\n\n2nd way: use the fact that v is constant\nπr^2h = 1, so\nπh = 1/r^2\nπ dh/dt = -2/r^3 dr/dt\nnow just plug in your numbers to find dh/dt\n\ndon't forget to watch the units.\n1m^3 = 10^6 cm^3\n\n1. 👍\n2. 👎\n2. Steve is tha goat\n\n1. 👍\n2. 👎\n3. Thanks bestie Steve! Hope ur thriving bc im not! <3\n\n1. 👍\n2. 👎\n\n## Similar Questions\n\n1. ### Calculus\n\na spherical balloon is inflated with gas at the rate of 500 cubic centimeters per minute. how fast is the radius of the balloon increasing at the instant the radius is 30 centimeters?\n\n2. ### Calculus\n\nAir is being pumped into a spherical balloon so that its volume increases at a rate of 30 cubic centimeters per second. How fast is the surface area of the balloon increasing when its radius is 19 cm? V= 4/3*pi*r^3 S= 4 pi r^2\n\n3. ### calculus\n\nA spherical balloon is losing air at the rate of 2 cubic inches per minute. How fast is the radius of the ballon shrinking when the radius is 8 inches.\n\n4. ### math-calculus\n\nA spherical party balloon is being inflated with helium pumped in at a rate of 12 cubic feet per minute. How fast is the radius growing at the instant when the radius has reached 1 ft?\n\n1. ### physics\n\nA 1.6 air bubble is released from the sandy bottom of a warm, shallow sea, where the gauge pressure is 1.6 . The bubble rises slowly enough that the air inside remains at the same constant temperature as the water. What is the\n\n2. ### Calculus: need clarification to where the #'s go\n\nAir is being pumped into a spherical balloon so that its volume increases at a rate of 80 \\mbox{cm}^3\\mbox{/s}. How fast is the surface area of the balloon increasing when its radius is 14 \\mbox{cm}? Recall that a ball of radius r\n\n3. ### Math( Can you help me with starting this problem)\n\nHow fast does the radius of a spherical soap bubble change when you blow air into it at the rate of 15 cubic centimeters per second? Our known rate is dv/dt , the change in volume with respect to time, which is 15 cubic\n\n4. ### calculus\n\nThe radius of a spherical balloon is increasing at a rate of 2 centimeters per minute. How fast is the volume changing when the radius is 8 centimeters? Note: The volume of a sphere is given by 4(pi)r^3\n\n1. ### calc\n\nAir is being pumped into a spherical balloon so that its volume increases at a rate of 100 {cm}^3}. How fast is the surface area of the balloon increasing when its radius is 16{cm}?\n\n2. ### physics\n\nCalculate the gauge pressure inside a soap bubble 0.0002m in radius using the surface tension for soapy water\n\n3. ### algebra\n\nSara goes on a slingshot ride in an amusement park. She is strapped into a spherical ball that has a radius of centimeters. What is the volume of air in the spherical ball?\n\n4. ### science\n\n1) In a syringe, what happens to the air paricles when you push the plunger? 2) In a syring, what happens the the air particles in the bubble from the bubble wrap when you pull up the plunger? 3) Are there more air particles in"
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http://discountgiftcards.club/draw-log-math/ | [
"# Draw Log Math",
null,
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null,
"http://discountgiftcards.club/wp-content/uploads//2019/03/draw-log-math-dot-plot-of-data-of-figure-2-shown-on-a-log-scale-with-base-of-math-games-online.jpg",
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null,
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]
| {"ft_lang_label":"__label__en","ft_lang_prob":0.7662531,"math_prob":0.9146902,"size":1275,"snap":"2019-35-2019-39","text_gpt3_token_len":259,"char_repetition_ratio":0.23524784,"word_repetition_ratio":0.026785715,"special_character_ratio":0.19137254,"punctuation_ratio":0.061728396,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99946064,"pos_list":[0,1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30],"im_url_duplicate_count":[null,1,null,1,null,1,null,1,null,1,null,1,null,1,null,1,null,1,null,1,null,1,null,1,null,1,null,1,null,1,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-08-21T11:41:43Z\",\"WARC-Record-ID\":\"<urn:uuid:55226a5b-1a62-4e77-b797-611fac5969b3>\",\"Content-Length\":\"24368\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:a1effcfe-3f5d-4690-87d0-6ea6e3db465c>\",\"WARC-Concurrent-To\":\"<urn:uuid:925671d6-1d9d-4351-b68e-1f93ce0f0ccb>\",\"WARC-IP-Address\":\"104.27.143.197\",\"WARC-Target-URI\":\"http://discountgiftcards.club/draw-log-math/\",\"WARC-Payload-Digest\":\"sha1:FPSUZ2EQ6RR2P7JI3TKTQBGJWM26YO42\",\"WARC-Block-Digest\":\"sha1:FFVATCTYXIKAG7PU6X3KGSJHDFYI7U4L\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-35/CC-MAIN-2019-35_segments_1566027315936.22_warc_CC-MAIN-20190821110541-20190821132541-00161.warc.gz\"}"} |
https://socratic.org/questions/simplify-this-index-law-question-1#455314 | [
"Simplify this index law question?\n\n${\\left(2 x {y}^{3}\\right)}^{2} / \\left(7 {x}^{3}\\right) \\times \\frac{3 {x}^{5} {y}^{2}}{4 y}$\n\nJul 23, 2017\n\n$= \\frac{3 {x}^{4} {y}^{7}}{7}$\n\nExplanation:\n\n${\\left(2 x {y}^{3}\\right)}^{2} / \\left(7 {x}^{3}\\right) \\cdot \\frac{3 {x}^{5} {y}^{2}}{4 y}$\n\nexpand\n\n$= \\frac{{2}^{2} {x}^{2} {\\left({y}^{3}\\right)}^{2} \\cdot \\left(3 {x}^{5} {y}^{2}\\right)}{7 {x}^{3} \\cdot 4 y}$\n\n$= \\frac{4 \\cdot {x}^{2} \\cdot {y}^{6} \\cdot 3 \\cdot {x}^{5} \\cdot {y}^{2}}{7 \\cdot {x}^{3} \\cdot 4 \\cdot y}$\n\n$= \\frac{12 \\cdot {x}^{2 + 5} \\cdot {y}^{6 + 2}}{28 \\cdot {x}^{3} \\cdot y}$\n\n$= \\frac{12 \\cdot {x}^{7 - 3} \\cdot {y}^{8 - 1}}{28}$\n\n$= \\frac{3 \\cdot {x}^{4} \\cdot {y}^{7}}{7}$\n\n$= \\frac{3 {x}^{4} {y}^{7}}{7}$"
]
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.57259524,"math_prob":1.0000097,"size":242,"snap":"2022-05-2022-21","text_gpt3_token_len":75,"char_repetition_ratio":0.12605043,"word_repetition_ratio":0.0,"special_character_ratio":0.30165288,"punctuation_ratio":0.06666667,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99998665,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2022-01-24T22:22:57Z\",\"WARC-Record-ID\":\"<urn:uuid:f2d91e43-8026-456e-add0-ac2655f2cf73>\",\"Content-Length\":\"31983\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:e9ab2d7d-f3a2-4db1-9e9d-205c91911aa2>\",\"WARC-Concurrent-To\":\"<urn:uuid:6faefcbf-c5eb-416f-a5f1-1a1dc8190e50>\",\"WARC-IP-Address\":\"216.239.38.21\",\"WARC-Target-URI\":\"https://socratic.org/questions/simplify-this-index-law-question-1#455314\",\"WARC-Payload-Digest\":\"sha1:KWXKOOT3YX3R2SAJZR6QWXCFABMWDCTD\",\"WARC-Block-Digest\":\"sha1:IZ2VYRXDZKZ6QAIZIZZZXGB2VHS4QKSP\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2022/CC-MAIN-2022-05/CC-MAIN-2022-05_segments_1642320304686.15_warc_CC-MAIN-20220124220008-20220125010008-00391.warc.gz\"}"} |
http://topcoder.bgcoder.com/print.php?id=183 | [
"### Problem Statement\n\nThis problem involves an elaborate marble maze game. The maze is composed of choosers that look like this:\n``` Right Oriented Left Oriented\n| | | |\n| | | |\n| | | |\n/ \\ \\ / / \\\n/ \\ \\ / / \\\n/ \\ \\ / / \\\n/ O \\ / O \\\n/ / \\ \\ / / \\ \\\n/ / \\ \\ / / \\ \\ ```\nA marble is put in the top of the chooser. The bar in the middle of the chooser determines whether the marble will leave to the left or the right. After a marble passes through the chooser the bar moves. For example, if a marble enters the right oriented chooser pictured above, it would leave toward the right but, the next marble to pass through would leave toward the left. The exact opposite would hold true for the left oriented chooser pictured above. We can make a game by networking a bunch of choosers together using tubes. For example:\n\ngame = {\"L 1 2\",\"R 2 0\",\"L X X\"}\n\nThis means that chooser 0 begins oriented to the left. Its left path leads to chooser 1, and its right path leads to chooser 2. Chooser 1 begins oriented to the right. Its left path leads to chooser 2, and its right path leads to chooser 0. Chooser 2 begins oriented to the left. Its left and right path both leave the game. If I place a marble in chooser 0 it will pass through 4 choosers before leaving the game (namely 0 then 1 then 0 then 2). Given a network of choosers, and a chooser that we drop the marble into, determine how many choosers the marble will pass through before leaving the game. If it will never leave return -1.\n\nCreate a class Choosers that contains the method length, which takes a String[] game, and an int chooser, and returns an int representing how many choosers the marble will pass through before leaving the game. Return -1 if it will never leave.\n\n### Definition\n\n Class: Choosers Method: length Parameters: String[], int Returns: int Method signature: int length(String[] game, int start) (be sure your method is public)\n\n### Constraints\n\n-game will contain between 1 and 15 elements, inclusive.\n-Each element of game will be formatted as \"<dir> <left> <right>\" with no extra, leading or trailing spaces, or extra leading 0's.\n-<dir> is either 'L' or 'R'\n-<left> and <right> are each either the character 'X' or integers between 0 and the length of game - 1, inclusive.\n\n### Examples\n\n0)\n\n `{\"L 1 2\",\"R 2 0\",\"L X X\"}` `0`\n`Returns: 4`\n The marble goes from 0 to 1 to 0 to 2 and then leaves.\n1)\n\n `{\"L 1 2\",\"R 2 0\",\"L X X\"}` `2`\n`Returns: 1`\n The marble leaves immediately.\n2)\n\n `{\"L 0 0\"}` `0`\n`Returns: -1`\n Clearly, the marble never leaves.\n\n#### Problem url:\n\nhttp://www.topcoder.com/stat?c=problem_statement&pm=1125\n\n#### Problem stats url:\n\nhttp://www.topcoder.com/tc?module=ProblemDetail&rd=4375&pm=1125\n\nbrett1479\n\n#### Testers:\n\nalexcchan , lbackstrom\n\nSimulation"
]
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.9176009,"math_prob":0.80833364,"size":2103,"snap":"2019-51-2020-05","text_gpt3_token_len":542,"char_repetition_ratio":0.1676989,"word_repetition_ratio":0.16747573,"special_character_ratio":0.27960056,"punctuation_ratio":0.09701493,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.95061094,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-01-23T02:15:53Z\",\"WARC-Record-ID\":\"<urn:uuid:01ff2fd2-d75c-4894-9c27-7f3e31ce8128>\",\"Content-Length\":\"7631\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:2e1c8199-4198-481a-abcd-2f90aed3d14f>\",\"WARC-Concurrent-To\":\"<urn:uuid:0fdb1001-9713-4bb9-ada9-245efb09c2f9>\",\"WARC-IP-Address\":\"78.128.6.10\",\"WARC-Target-URI\":\"http://topcoder.bgcoder.com/print.php?id=183\",\"WARC-Payload-Digest\":\"sha1:RPDV3RTAUZV6ULEBBXPJKEBYOWUJOC2P\",\"WARC-Block-Digest\":\"sha1:S7L5CSRKXL6WUM6R53CTKXKT3DXBR7XY\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-05/CC-MAIN-2020-05_segments_1579250608062.57_warc_CC-MAIN-20200123011418-20200123040418-00555.warc.gz\"}"} |
https://brainmass.com/math/basic-algebra/multiples-quadratic-equations-167033 | [
"Explore BrainMass\nShare\n\n### Explore BrainMass\n\nThis content was COPIED from BrainMass.com - View the original, and get the already-completed solution here!\n\nTwo quadratic equations that are multiples of each other are actually the same equation, and that they don't count as being \"more than one QE that have the same solution set\". However, if you plot the two equations on a graph, will they be different from each other, but have the same x-axis intercepts, which are the answer set?\nPlease explain, If they are different graphs, does that mean that they are really two different equations?"
]
| [
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.96904886,"math_prob":0.9923105,"size":1164,"snap":"2019-51-2020-05","text_gpt3_token_len":245,"char_repetition_ratio":0.15517241,"word_repetition_ratio":0.5363129,"special_character_ratio":0.20360824,"punctuation_ratio":0.11818182,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99181545,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-01-28T04:43:56Z\",\"WARC-Record-ID\":\"<urn:uuid:c9cecdaa-dfac-45a5-98b9-11d6000623fe>\",\"Content-Length\":\"52126\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:e7adb1cc-440e-4910-9010-34b1ef1284fa>\",\"WARC-Concurrent-To\":\"<urn:uuid:ad311966-e8cf-47f9-a353-39a748f70393>\",\"WARC-IP-Address\":\"65.39.198.123\",\"WARC-Target-URI\":\"https://brainmass.com/math/basic-algebra/multiples-quadratic-equations-167033\",\"WARC-Payload-Digest\":\"sha1:EMRPKM6A44PDGHICKGCUCM2SJPWEKETR\",\"WARC-Block-Digest\":\"sha1:IYRJT36VRFTMXNPN345ZFRR2YZVYIQFU\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-05/CC-MAIN-2020-05_segments_1579251773463.72_warc_CC-MAIN-20200128030221-20200128060221-00366.warc.gz\"}"} |
https://wohin-woher.com/jp/contents/uk/mo1-5/F5_monograph_1-5.htm | [
"< = back | = > volume 2 (overview)\n\nBlue links lead to the fully translated html versions of the page, purple links lead to pages whose start pages (as well as introductions and tables of contents at least) are already set up, green links lead to extern sites, grey means that no file is available yet).\n\n/Notes in this color and between two / are from the operator of the German mirror site and translator/.\n\nChapter F: The Oscillatory Chamber\n\nF5. Mathematical model of the Oscillatory Chamber\n\nOur present knowledge of magnetic and electric phenomena enables us to deduce the equations expressing the values of the resistance, inductance and capacitance of the Oscillatory Chamber. Further combination of these equations will lead to the prediction of the behaviour of this device.\n\nThis subsection is just intended to describe the Oscillatory Chamber in such language of mathematics. Therefore it supplies the vital interpretative foundations for all the researchers experimenting with this device. Unfortunately for the readers less oriented towards mathematics, it may spoil the pleasure of familiarizing themselves with the content of this monograph. For this reason, those readers who experience a revival of sleepiness each time they encounter a mathematical equation are recommended to shift from this point directly into the beginning of subsection F6.\n\nF5.1. Resistance of the Oscillatory Chamber\n\nThe general form of the equation for the resistance of any resistor of cross-section \"A\" and length \"l\" is as follows:\n\nR = Ω*(l/A)\n\nIn this equation the \"Ω\" represents the resistivity of a material from which the resistor is made. In our case it will be the maximal resistivity of the dielectric gas that fills the Oscillatory Chamber, determined for the conditions of the initial moment of electric breakdown. In turn operators \"*\" and \"/\" adopted from computer programming, mean \"multiply\" and \"divide\".\n\nIf in the above general equation, we replace the variables by the specific parameters determined for the Oscillatory Chamber, i.e. l=a and A=a2 (compare with Img.012 (F1b), this gives:\n\nR = Ω/a (F1)\n\nThe equation (F1) received here represents the resistance of the Oscillatory Chamber, which is a function of the chamber's side wall dimension \"a\".\n\nF5.2. Inductance of the Oscillatory Chamber\n\nThe determination of the chamber's inductance is an extremely difficult and complex task. Completing it with total accuracy is beyond the author's knowledge of the subject. Also a number of experts consulted in this matter were unable to help. (Perhaps some of the readers know how to resolve this problem - in such a case the author would warmly welcome a review of their deductions and the final equation they derived.) Being unable to find the exact solution, the author decided to apply temporarily a simplified one. To justify this simplification it should be stated that the deducted equation (F2) for the value of inductance will be used only once in the entire monograph, when the meaning of factor \"s\" (see (F5)) is interpreted. Therefore all the vital equations in this work remain unaffected.\n\nIn the simplified deductions of the chamber's inductance an assumption is made that a unitary inductance of a stream of sparks (i.e. the inductance related to the unit of a spark's length) will be equal to the inductance of the equivalent strand of wires. This assumption allows for the application of a well-known equation for the inductance of a solenoid (see the book [1F5.2] by David Halliday et al, \"Fundamentals of Physics\", John Willey & Sons, 1966):\n\nL = μ*n2*l*A\n\nWhen in this equation we substitute: n=p/a, l=a, and A=a2 (where \"p\" is the number of segments in each of the chamber's plates, whereas \"a\" is the dimension of the chamber's walls), the simplified equation for the inductance of the Oscillatory Chamber is derived:\n\nL = μ*p2*a (F2)\n\nIt can be theoretically asserted that the unitary electrical inertia of a stream of sparks should be greater than such an inertia in the equivalent strand of wires. The justification for this assertion can be obtained from the analysis of the inertia mechanism. The inertia reveals itself only when the motion involves the reversible phenomena or media which absorb energy in the initial stage of the motion's development, and which release this energy when the motion declines. The greater the number of such phenomena and media involved, and the higher their energy absorption, the larger is the resultant inertia. The stream of sparks jumping through gas in every aspect manifests better potentials for causing an inertia higher than the one of a current flowing through wires. The first reason for this lies in the more efficient energy absorption and releasing by sparks, occurring because:\n\na) The speed of electrons in a spark can be higher than in a wire,\n\nb) The contiguous sparks can pass closer to each other because they do not require thick insulation layers in between them (as is the case for wires).\nThe second reason for the higher inertia of sparks in gas results from them involving a variety of reversible phenomena - not appearing at all during flows of currents through wires. These are:\n\nc) The ionization of surrounding gases. This, due to the returning of the absorbed energy, supports the inertia of the process at the moment of the sparks' decline.\n\nd) The motion of heavy ions, whose mass absorbs and then releases the kinetic energy.\n\ne) The initiation of hydrodynamic phenomena (e.g. dynamic pressure, rotation of the gas) which also will be the cause of the charges' dislocation and energy return at the moment of the sparks' decline.\n\nThe above theoretical premises should not be difficult to verify by experiments described in subsection F8.2. (e.g. stage 1c).\n\nF5.3. Capacitance of the Oscillatory Chamber\n\nWhen we use the well-known equation for the capacitance of a parallel-plate capacitor, of the form:\n\nC = ε*A/l\n\n(where \"ε\" is the dielectric constant of this capacitor, \"A\" is the surface area of electrodes, while \"l\" is the distance between these electrodes), and when we apply the substitutions: A=a5, l=a, this yields the final equation for the capacitance \"C\" of a cubical Oscillatory Chamber:\n\nC = ε*a (F3)\n\n(i.e. the capacitance \"C\" of a cubical Oscillatory Chamber is equal to the value of the dielectric constant \"ε\" for the dielectric gas that fills this chamber, multiplied by the side dimension \"a\" of this chamber).\n\nF5.4. The \"sparks' motivity factor\" and its interpretation\n\nEach of the equations (F1), (F2) and (F3) describes only one selected parameter of the Oscillatory Chamber. On the other hand, it would be very useful to obtain a single complex factor which would express simultaneously all electromagnetic and design characteristics of this device. Such a factor is now introduced, and will be called a \"sparks' motivity factor\". Its defining equation is the following:\n\ns = p*(R/2)*√(C/L) (F4)\n\nNotice, that after expressing this in the notation of computer languages, in which the symbol \"*\" means multiplication, the symbol \"/\" means division, the symbol \"+\" means addition, the symbol \"-\" means subtraction, while the symbol \"sqrt()\" means the square roof from the parameter provided in brackets \"()\", the above equation (F4) takes the following form:\n\ns = p*(R/2)*sqrt(C/L).\n\nNotice that, according to the definition, this \"s\" factor is dimensionless.\nIndependently from the above defining equation (F4), the \"s\" factor has also an interpretative description. This is obtained when in (F4) the variables R, L and C are substituted by the values expressed by equations (F1), (F2) and (F3). When this is done, the following interpretative equation for \"s\" is received:\n\ns = (1/(2a))Ω√(ε/μ). (F5)\n\nNotice, that after expressing this in the notation of computer languages, in which the symbol \"*\" means multiplication, the symbol \"/\" means division, the symbol \"+\" means addition, the symbol \"-\" means subtraction, while the symbol \"sqrt()\" means the square roof from the parameter provided in brackets \"()\", the above equation (F5) takes the following form:\n\ns = (1/(2*a))Ω*sqrt(ε/μ).\n\nEquation (F5) reveals that the \"s\" factor perfectly represents the current state of all environmental conditions in which the sparks occur, and which determine their course and effectiveness. It describes the type and consistency of the gas used as a dielectric, and the actual conditions under which this gas is stored. It also describes the size of the chamber. Therefore the \"s\" factor constitutes a perfect parameter which is able to inform exactly about the working situation existing within the chamber at any particular instant in time.\n\nThe value of the \"s\" factor can be controlled at the design stage and at the exploitation stage. At the design stage it is achieved by changing the size \"a\" of a cubical chamber. At the exploitation stage it requires the change of the pressure of a gas within the chamber or altering its composition. In both cases this influences the constants Ω, μ and ε, describing the properties of this gas. (Note that constants \"Ω\", \"μ\", and \"ε\", are: Ω = resistivity of a dielectric gas within the chamber determined at the moment of electric breakdown in [Ohm*meter], μ = magnetic permeability of a dielectric in [Henry/metre], ε = dielectric constant for a gas filling the chamber in [Farad/metre].)\n\nF5.5. Condition for the oscillatory response\n\nFrom the electric point of view the Oscillatory Chamber represents a typical RLC circuit. The research on Electric Networks has determined for such circuits the condition under which, once they are charged, they will maintain the oscillatory response. This condition, presented in the book [1F5.5] by Hugh H. Skilling, \"Electric Network\" (John Willey & Sons, 1974), takes the form:\n\nR2 < 4*L/C\n\nIf the above relation is transformed and then its variables are substituted by the equation (F4), it takes the final form:\n\np > s (F6)\n\nThe above condition describes the design requirement for the number \"p\" of segments separated within the plates of the Oscillatory Chamber, in relation to the environmental conditions \"s\" existing in the area where the sparks appear. If this condition is fulfilled, the sparks produced within the Oscillatory Chamber will acquire an oscillatory character.\n\nTo interpret the condition (F6), a possible range of values taken by the factor \"s\" should be considered (compare with the equation (F5)).\n\nF5.6. The period of pulsation of the chamber's field\n\nFrom the RLC circuits we know that the period of their oscillations is described by the equation:",
null,
"Notice, that after expressing this in the notation of computer languages, in which the symbol \"*\" means multiplication, the symbol \"/\" means division, the symbol \"+\" means addition, the symbol \"-\" means subtraction, the symbol \"x**2\" means \"x\" to the power of \"2\", while the symbol \"sqrt()\" means the square roof from the parameter provided in brackets \"()\", the above equation takes the following form:\n\nT = (2*π)/(sqrt(1/(L*C) - (R/(2***2) = 2*π*sqrt(L*C/(1 - ((R**2)*C)/(4*L))).\n\nIf the defining equation (F4) on the factor \"s\" replaces in the above a combination of R, L, and C parameters, whereas equation (F1) and equation (F3) provide the values for R and C, then this period is described as:",
null,
"(F7)\n\nNotice, that after expressing this in the notation of computer languages, in which the symbol \"*\" means multiplication, the symbol \"/\" means division, the symbol \"+\" means addition, the symbol \"-\" means subtraction, division, while the symbol \"sqrt()\" means the square root from the parameter provided in brackets \"()\", the equation (F7) takes the following form:\n\nT = (π*(p/s)*Ω*ε)/sqrt(1 - (s/p)**2).\n\nThe final equation (F7) not only illustrates which parameters determine the value of the period of pulsations \"T\" in the Oscillatory Chamber, but also shows how the value of \"T\" can practically be controlled. Thus this equation will be highly useful for the understanding of the amplifying control of the period \"T\" of field pulsation described in subsection F6.5.\n\nIf we know the period \"T\" of chamber's field pulsations, then we can easily determine the frequency \"f\" of pulsations of this field. The well known equation linking these two parameters is as follows:\n\nf = 1/T (F8)\n\nOf course, according to the above equation (F8), the control over the frequency \"f\" of the field's pulsations will be achieved via influencing the value of the period \"T\" of this field pulsations.\n\nF6.\n\nVisitors since 15.12.22: (english sites)"
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"https://wohin-woher.com/jp/contents/uk/mo1-5/formelF7a.jpg",
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"https://wohin-woher.com/jp/contents/uk/mo1-5/formelF7b.jpg",
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.9085277,"math_prob":0.97799104,"size":12192,"snap":"2023-40-2023-50","text_gpt3_token_len":2725,"char_repetition_ratio":0.16401379,"word_repetition_ratio":0.10465116,"special_character_ratio":0.2245735,"punctuation_ratio":0.09606792,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99743485,"pos_list":[0,1,2,3,4],"im_url_duplicate_count":[null,1,null,1,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-09-21T13:26:39Z\",\"WARC-Record-ID\":\"<urn:uuid:0727f321-8ec5-43f4-b7fa-cc19b39b8f74>\",\"Content-Length\":\"16309\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:41abc999-1b0d-4fa8-9808-de3189c2ea4e>\",\"WARC-Concurrent-To\":\"<urn:uuid:e39fdecc-f103-4b3a-b560-5bc2f127cd19>\",\"WARC-IP-Address\":\"178.77.80.187\",\"WARC-Target-URI\":\"https://wohin-woher.com/jp/contents/uk/mo1-5/F5_monograph_1-5.htm\",\"WARC-Payload-Digest\":\"sha1:RO2QS6WEIGNIQJTCMU2LS3RQ4GI5JK4Y\",\"WARC-Block-Digest\":\"sha1:FJGGCNZDWR32FPAK633UXQTW5MYB2BOE\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-40/CC-MAIN-2023-40_segments_1695233506027.39_warc_CC-MAIN-20230921105806-20230921135806-00746.warc.gz\"}"} |
https://gradeup.co/undecidability-i-32c748fa-bea5-11e5-8fa3-b0415042f6e8 | [
"# Study Notes on Undecidability\n\nUpdated : Oct 13, 2019, 9:00\nBy : Richa Tiwari\n\n## There are two types of TMs (based on halting):\n\n1. Halting TM : (Accepts Recursive languages) : TMs that always halt, no matter accepting or non no matter accepting or non-accepting (called as decidable problems)\n2. TM : (Accepts Recursively enumerable): TMs that are guaranteed to halt are guaranteed to halt only on acceptance only on acceptance. If non-accepting, it may or may not halt (i.e., could loop forever). (Either decidable or partially decidable)\n\n## Decidable Problem\n\n• If there is a Turing machine that decides the problem, called as Decidable problem.\n• A decision problem that can be solved by an algorithm that halts on all inputs in a finite number of steps.\n• A problem is decidable, if there is an algorithm that can answer either yes or no.\n• A language for which membership can be decided by an algorithm that halts on all inputs in a finite number of steps.\n• Decidable problem is also called as totally decidable problem, algorithmically solvable, recursively solvable.\n\n## Undecidable Problem (Semi-dedidable or Totally not decidable)\n\n• A problem that cannot be solved for all cases by any algorithm whatsoever.\n• Equivalent Language cannot be recognized by a Turing machine that halts for all inputs.\n\nThe following problems are undecidable problems:\n\n• Halting Problem: A halting problem is undecidable problem. There is no general method or algorithm which can solve the halting problem for all possible inputs.\n• Emptyness Problem: Whether a given TM accepts Empty?\n• Finiteness Problem: Whether a given TM accepts Finite?\n• Equivalence Problem: Whether Given two TM’s produce same language?. Is L(TM1) = L(TM2) ?\n• Is L(TM1) ⊆ L(TM2) ? (Subset Problem)\n• Is L(TM1) Ո L(TM2) = CFL?\n• Is L(TM1) = Σ* ? (Totality Problem)\n• Is the complement of L(G1) context-free ?\nUndecidable problems are two types: Partially decidable (Semi-decidable) and Totally not decidable.\n• Semi decidable: A problem is semi-decidable if there is an algorithm that says yes. if the answer is yes, however it may loop infinitely if the answer is no.\n• Totally not decidable (Not partially decidable): A problem is not decidable if we can prove that there is no algorithm that will deliver an answer.\n\n### Decidability table for Formal Languages:\n\n Problems RL DC CFL Rec RE Membership Y Y Y Y N Finiteness Y Y Y N N Emptiness Y Y Y N N Equivalence Y Y N N N Is L1 ⊆ L2 ?(SUBSET) Y N N N N Is L = REGULAR? Y Y N N N Is L Ambiguous? Y N N N N L=∑* ?(UNIVERSAL) Y Y N N N L1 ∩ L2= Ф ?(DISJOINT) Y N N N N Is L= Regular? Y Y N N N L1 ∩ L2= L Y N N Y Y Is L' also same type? Y Y N Y N\n\nNotes : RL= Regular Language , DC = Deterministic context-free languages (DCFL), CFL= Context Free Languages (CFL), Rec = Recursive language, RE= Recusively Enumerable Language.\n\nAll the Best\n\nThanks,\n\nPrep Smart, Score Better. Go Gradeup.\n\nOct 13GATE & PSU CS\n\nPosted by:",
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"Want to create my own success story✌️\nMember since Feb 2019",
null,
"GradeStack Learning Pvt. Ltd.Windsor IT Park, Tower - A, 2nd Floor,Sector 125, Noida,Uttar Pradesh [email protected]"
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null,
"https://gs-post-images.grdp.co/2018/12/screenshot-2018-12-21-at-3-img1545387500435-75.png-rs-high-webp.png",
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"https://gs-post-images.grdp.co/2018/12/screenshot-2018-12-21-at-3-img1545387500435-75.png-rs-high-webp.png",
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.84935325,"math_prob":0.8997585,"size":2753,"snap":"2020-34-2020-40","text_gpt3_token_len":786,"char_repetition_ratio":0.16769734,"word_repetition_ratio":0.102,"special_character_ratio":0.24300763,"punctuation_ratio":0.11721612,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9909439,"pos_list":[0,1,2,3,4],"im_url_duplicate_count":[null,null,null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-10-01T20:19:01Z\",\"WARC-Record-ID\":\"<urn:uuid:4898f01f-593e-4b8c-90a9-a6077a16fea2>\",\"Content-Length\":\"145740\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:0894b8ed-3647-4d10-b59a-ed3e1a77b928>\",\"WARC-Concurrent-To\":\"<urn:uuid:f4fce1f8-5222-455f-b5a8-69a994fb3390>\",\"WARC-IP-Address\":\"104.17.13.38\",\"WARC-Target-URI\":\"https://gradeup.co/undecidability-i-32c748fa-bea5-11e5-8fa3-b0415042f6e8\",\"WARC-Payload-Digest\":\"sha1:VMETIELCSVHHIJSN6O65CLHMLCH22TJA\",\"WARC-Block-Digest\":\"sha1:6O55LY7NOAMAVVVWIQOV2B6TXLBDTKFR\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-40/CC-MAIN-2020-40_segments_1600402131986.91_warc_CC-MAIN-20201001174918-20201001204918-00006.warc.gz\"}"} |
https://cstheory.stackexchange.com/questions/44273/efficient-graph-isomorphism-for-similar-graph-queries | [
"# Efficient graph isomorphism for similar graph queries\n\nGiven the graph G1, G2 and G3, we want to perform isomorphism test F between G1 and G2 as well as G1 and G3. If G2 and G3 are very similar such that G3 is formed by deleting one node and inserting one node from G2, and we have the result of F(G1,G2), can we compute F(G1,G3) without computing it from scratch by extending any existing state-of-the-art methods?\n\nFor example, if G2 is formed by nodes 2,3,4,5 and G3 is formed by nodes 3,4,5,6, can we make use of the result of F(G1,G2) to compute F(G1,G3) more efficiently?\n\nThis is a simple polynomial time reduction to show that the problem is GI complete: even if you know that $$G_1, G_2$$ are isomorphic, checking if $$G_3$$, built from $$G_2$$ deleting and adding a node, is isomorphic to $$G_1$$ is as hard as graph isomorphism itself (in the worst case).\n\nGiven two graphs $$G = (V, E), G'= (V', E')$$ build\n\n$$G_1 = ( V \\cup V' \\cup \\{u\\},\\; E \\cup E' \\cup \\{ (v_i,u) \\mid v_i \\in V \\})$$\n\ni.e. the union of the two graphs plus an extra node $$u$$ connected to all the vertices of $$V$$\n\npick $$G_2 = G_1$$; and clearly they are isomorphic.\n\nNow build $$G_3$$ deleting $$u$$ and adding $$u'$$ connected to all the vertices of $$V'$$:\n\n$$G_3 = ( V \\cup V' \\cup \\{u'\\},\\; E \\cup E' \\cup \\{ (v_i',u') \\mid v_i' \\in V'\\} )$$\n\n$$G_1, G_3$$ are isomorphic iff $$G, G'$$ are isomorphic.\n\n• This is a nice reduction! However, I would add that GI-completeness alone doesn't necessarily mean there is no advantage, only that in the worst case their complexities are polynomially related. As another example, note that vertex-colored GI is also GI-complete, but most algorithms I know of can still take advantage of vertex colors in a useful way. – Joshua Grochow Jul 16 at 17:40\n• @JoshuaGrochow: thanks, I clarified that point. – Marzio De Biasi Jul 16 at 19:02\n• @MarzioDeBiasi: thank you for the explanations. Based on my understanding about your explanations, we can no take any advantage to compute F(G1,G3) knowing F(G1,G2) if the vertices connected to u and u' are different (not necessarily connected to all vertices of V or V') even if we know G and G' are isomorphic. Is that correct? In this case, is this problem as hard as the graph isomorphism itself? – Eric Huang Jul 17 at 3:06\n• @EricHuang: the reduction says that given two isomorphic graphs $G_1, G_2$ and an explicit way to build $G_3$ by deleting/adding one node (and some edges) to $G_2$ the problem of checking whether $G_1, G_3$ are isomorphic is as hard as graph isomorphism. BTW, this result also extends to the associated promise problem in which you're not given the explicit way to build $G_3$, but only the promise that $G_1,G_3$ are isomorphic up to a node delete/add operation. – Marzio De Biasi Jul 17 at 6:48\n• You may try the Weisfeiler-Lehman method or its variations, especially if your original graphs have structures like planar, tree, interval graph or bounded treewidth graph, their Weisfeiler-Lehman dimension is a small constant, in the refinement step, I guess you can take advantage of the relationship between the two graphs. – Rupei Xu Jul 29 at 0:44"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.9646398,"math_prob":0.99462855,"size":521,"snap":"2019-51-2020-05","text_gpt3_token_len":158,"char_repetition_ratio":0.13926499,"word_repetition_ratio":0.0,"special_character_ratio":0.29942417,"punctuation_ratio":0.14179105,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9993518,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-12-08T07:31:58Z\",\"WARC-Record-ID\":\"<urn:uuid:c5bd8e00-ceb5-453b-87c6-8e6718fe72f9>\",\"Content-Length\":\"139032\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:e6f2698f-4c96-472f-89f2-f8de26e3947e>\",\"WARC-Concurrent-To\":\"<urn:uuid:7b8c224b-ef9a-4358-ba66-ce974aa41c04>\",\"WARC-IP-Address\":\"151.101.129.69\",\"WARC-Target-URI\":\"https://cstheory.stackexchange.com/questions/44273/efficient-graph-isomorphism-for-similar-graph-queries\",\"WARC-Payload-Digest\":\"sha1:FEHNZOSKSHHBJ7JUE4FFGEMWRU2CBMJG\",\"WARC-Block-Digest\":\"sha1:REWFCLHS6LD2S7AJ4CBX7BW5XMJ67KO3\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-51/CC-MAIN-2019-51_segments_1575540507109.28_warc_CC-MAIN-20191208072107-20191208100107-00348.warc.gz\"}"} |
https://mran.revolutionanalytics.com/snapshot/2020-12-31/web/packages/RestRserve/vignettes/ContentHandlers.html | [
"# Encoding\n\nLet’s consider an example. We develop an application which calculates factorial of a number:\n\nlibrary(RestRserve)\nbackend = BackendRserve$new() application = Application$new()\napplication$add_get(path = \"/factorial\", function(.req, .res) { x = .req$get_param_query(\"x\")\nx = as.integer(x)\n.res$set_body(factorial(x)) }) Here is how request will be processed: request = Request$new(\npath = \"/factorial\",\nmethod = \"GET\",\nparameters_query = list(x = 10)\n)\nresponse = application$process_request(request) response #> <RestRserve Response> #> status code: 200 OK #> content-type: text/plain #> <Headers> #> Server: RestRserve/0.4.0 Let’s take a closer look to the response object and its body property: str(response$body)\n#> chr \"3628800\"\n\nAs we can see it is a numeric value. HTTP response body however can’t be an arbitrary R object. It should be something that external systems can understand - either character vector or raw vector. Fortunately application helps to avoid writing boilerplate code to encode the body. Based on the content_type property it can find encode function which will be used to transform body into a http body.\n\nresponse$content_type #> \"text/plain\" response$encode\n#> NULL\n\nTwo immediate questions can arise:\n\n1. Why content_type is equal to text/plain?\n• This is because we can specify default content_type in Application constructor. It is text/plain by default, which means all the responses by default will have text/plain content type.\n2. How does application know how to encode text/plain? Can it encode any arbitrary content type?\n• Application by default is initialized with pre-defined ?EncodeDecodeMiddleware middleware. The logic on how to encode and decode request and response body is controlled by its ContentHandlers property. Out of the box it supports two content types - text/plain and application/json.\n\nFor instance app1 and app2 are equal:\n\nencode_decode_middleware = EncodeDecodeMiddleware$new() app1 = Application$new(middleware = list())\napp1$append_middleware(encode_decode_middleware) app2 = Application$new()\n\nHere is example on how you can get the actual function used for application/json encoding:\n\n\nFUN = encode_decode_middleware$ContentHandlers$get_encode('application/json')\nFUN\n#> function(x, unbox = TRUE) {\n#> res = jsonlite::toJSON(x, dataframe = 'columns', auto_unbox = unbox, null = 'null', na = 'null')\n#> unclass(res)\n#> }\n#> <bytecode: 0x7fdb7f31db98>\n#> <environment: namespace:RestRserve>\n\nWe can manually override application default content-type:\n\napplication$add_get(path = \"/factorial-json\", function(.req, .res) { x = as.integer(.req$get_param_query(\"x\"))\nresult = factorial(x)\n.res$set_body(list(result = result)) .res$set_content_type(\"application/json\")\n})\nrequest = Request$new( path = \"/factorial-json\", method = \"GET\", parameters_query = list(x = 10) ) response = application$process_request(request)\nresponse$body #> \"{\\\"result\\\":3628800}\" And here is a little bit more complex example where we store a binary object in the body. We will use R’s native serialization, but one can use protobuf, messagepack, etc. application$add_get(path = \"/factorial-rds\", function(.req, .res) {\nx = as.integer(.req$get_param_query(\"x\")) result = factorial(x) body_rds = serialize(list(result = result), connection = NULL) .res$set_body(body_rds)\n.res$set_content_type(\"application/x-rds\") }) However function above won’t work correctly. Out of the box ContentHndlers doesn’t know anything about application/x-rds: request = Request$new(\npath = \"/factorial-rds\",\nmethod = \"GET\",\nparameters_query = list(x = 10)\n)\nresponse = application$process_request(request) response$body\n#> \"500 Internal Server Error: can't encode body with content_type = 'application/x-rds'\"\n\nIn order to resolve problem above we would need to either register application/x-rds content handler with ContentHandlers$set_encode() or manually specify encode function (identity in our case): application$add_get(path = \"/factorial-rds2\", function(.req, .res) {\nx = as.integer(.req$get_param_query(\"x\")) result = factorial(x) body_rds = serialize(list(result = result), connection = NULL) .res$set_body(body_rds)\n.res$set_content_type(\"application/x-rds\") .res$encode = identity\n})\n\nrequest = Request$new( path = \"/factorial-rds2\", method = \"GET\", parameters_query = list(x = 10) ) response = application$process_request(request)\nunserialize(response$body) #>$result\n#> 3628800\n\n# Decoding\n\nRestRserve facilitates with parsing incoming request body as well. Consider a service which expects JSON POST requests:\n\napplication = Application$new(content_type = \"application/json\") application$add_post(\"/echo\", function(.req, .res) {\n.res$set_body(.req$body)\n})\n\nrequest = Request$new(path = \"/echo\", method = \"POST\", body = '{\"hello\":\"world\"}', content_type = \"application/json\") response = application$process_request(request)\nresponse$body #> \"{\\\"hello\\\":\\\"world\\\"}\" The logic behind decoding is also controlled by ?EncodeDecodeMiddleware and its ContentHandlers property. # Extending encoding and decoding Here is an example which demonstrates on how to extend ?EncodeDecodeMiddleware to handle additional content types: encode_decode_middleware = EncodeDecodeMiddleware$new()\n\nencode_decode_middleware$ContentHandlers$set_encode(\n\"text/csv\",\nfunction(x) {\ncon = rawConnection(raw(0), \"w\")\non.exit(close(con))\nwrite.csv(x, con, row.names = FALSE)\nrawConnectionValue(con)\n}\n)\n\nencode_decode_middleware$ContentHandlers$set_decode(\n\"text/csv\",\nfunction(x) {\nres = try({\ncon = textConnection(rawToChar(x), open = \"r\")\non.exit(close(con))\n}, silent = TRUE)\n\nif (inherits(res, \"try-error\")) {\nraise(HTTPError$bad_request(body = attributes(res)$condition$message)) } return(res) } ) Extended middleware needs to be provided to the application constructor: data(iris) app = Application$new(middleware = list(encode_decode_middleware))\n\nNow let’s test it:\n\napp$add_get(\"/iris\", FUN = function(.req, .res) { .res$set_content_type(\"text/csv\")\n.res$set_body(iris) }) req = Request$new(path = \"/iris\", method = \"GET\")\nres = app$process_request(req) iris_out = read.csv(textConnection(rawToChar(res$body)))\n#> Sepal.Length Sepal.Width Petal.Length Petal.Width Species\n#> 1 5.1 3.5 1.4 0.2 setosa\n#> 2 4.9 3.0 1.4 0.2 setosa\n#> 3 4.7 3.2 1.3 0.2 setosa\n#> 4 4.6 3.1 1.5 0.2 setosa\n#> 5 5.0 3.6 1.4 0.2 setosa\n#> 6 5.4 3.9 1.7 0.4 setosa\napp$add_post(\"/in\", FUN = function(.req, .res) { str(.req$body)\n})\nreq = Request$new(path = \"/in\", method = \"POST\", body = res$body, content_type = \"text/csv\")\napp$process_request(req) #> 'data.frame': 150 obs. of 5 variables: #>$ Sepal.Length: num 5.1 4.9 4.7 4.6 5 5.4 4.6 5 4.4 4.9 ...\n#> $Sepal.Width : num 3.5 3 3.2 3.1 3.6 3.9 3.4 3.4 2.9 3.1 ... #>$ Petal.Length: num 1.4 1.4 1.3 1.5 1.4 1.7 1.4 1.5 1.4 1.5 ...\n#> $Petal.Width : num 0.2 0.2 0.2 0.2 0.2 0.4 0.3 0.2 0.2 0.1 ... #>$ Species : chr \"setosa\" \"setosa\" \"setosa\" \"setosa\" ...\n#> <RestRserve Response>\n#> status code: 200 OK\n#> content-type: text/plain\n#> Server: RestRserve/0.4.0"
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https://numbermatics.com/n/460/ | [
"# 460\n\n## 460 is an even composite number composed of three prime numbers multiplied together.\n\nWhat does the number 460 look like?\n\nThis visualization shows the relationship between its 3 prime factors (large circles) and 12 divisors.\n\n460 is an even composite number. It is composed of three distinct prime numbers multiplied together. It has a total of twelve divisors.\n\n## Prime factorization of 460:\n\n### 22 × 5 × 23\n\n(2 × 2 × 5 × 23)\n\nSee below for interesting mathematical facts about the number 460 from the Numbermatics database.\n\n### Names of 460\n\n• Cardinal: 460 can be written as Four hundred sixty.\n\n### Scientific notation\n\n• Scientific notation: 4.6 × 102\n\n### Factors of 460\n\n• Number of distinct prime factors ω(n): 3\n• Total number of prime factors Ω(n): 4\n• Sum of prime factors: 30\n\n### Divisors of 460\n\n• Number of divisors d(n): 12\n• Complete list of divisors:\n• Sum of all divisors σ(n): 1008\n• Sum of proper divisors (its aliquot sum) s(n): 548\n• 460 is an abundant number, because the sum of its proper divisors (548) is greater than itself. Its abundance is 88\n\n### Bases of 460\n\n• Binary: 1110011002\n• Base-36: CS\n\n### Squares and roots of 460\n\n• 460 squared (4602) is 211600\n• 460 cubed (4603) is 97336000\n• The square root of 460 is 21.4476105895\n• The cube root of 460 is 7.7194426293\n\n### Scales and comparisons\n\nHow big is 460?\n• 460 seconds is equal to 7 minutes, 40 seconds.\n• To count from 1 to 460 would take you about three minutes.\n\nThis is a very rough estimate, based on a speaking rate of half a second every third order of magnitude. If you speak quickly, you could probably say any randomly-chosen number between one and a thousand in around half a second. Very big numbers obviously take longer to say, so we add half a second for every extra x1000. (We do not count involuntary pauses, bathroom breaks or the necessity of sleep in our calculation!)\n\n• A cube with a volume of 460 cubic inches would be around 0.6 feet tall.\n\n### Recreational maths with 460\n\n• 460 backwards is 064\n• 460 is a Harshad number.\n• The number of decimal digits it has is: 3\n• The sum of 460's digits is 10\n• More coming soon!"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.86606205,"math_prob":0.9825132,"size":3048,"snap":"2019-51-2020-05","text_gpt3_token_len":826,"char_repetition_ratio":0.1130092,"word_repetition_ratio":0.05027933,"special_character_ratio":0.31167978,"punctuation_ratio":0.14681892,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99452126,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-12-11T14:04:38Z\",\"WARC-Record-ID\":\"<urn:uuid:c1f33756-1888-4a7d-adec-31a04f7c7aa6>\",\"Content-Length\":\"16006\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:09c542ef-4b52-4cc9-b69c-e32267391224>\",\"WARC-Concurrent-To\":\"<urn:uuid:003d713f-340f-426e-9c97-090c6c5d622d>\",\"WARC-IP-Address\":\"72.44.94.106\",\"WARC-Target-URI\":\"https://numbermatics.com/n/460/\",\"WARC-Payload-Digest\":\"sha1:OQE7BSALF7EYFSSYMLQD3ZFSPSG3KWZO\",\"WARC-Block-Digest\":\"sha1:LQ6BDVDYNCETKFBFU43KN5K6GGTO6SXY\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-51/CC-MAIN-2019-51_segments_1575540531917.10_warc_CC-MAIN-20191211131640-20191211155640-00268.warc.gz\"}"} |
http://api.fmrchallenge.org/classintegrator__chains_1_1Polytope.html | [
"fmrbenchmark 0.0.4\nintegrator_chains::Polytope Class Reference\n\nBasic half-space representation of polytopes. More...\n\n`#include <polytope.hpp>`\n\nInheritance diagram for integrator_chains::Polytope:",
null,
"[legend]\n\n## Public Member Functions\n\nvoid dumpJSONcore (std::ostream &out) const\nOutput this polytope in JSON excluding opening { and closing }. More...\n\nbool is_consistent () const\nCheck that defining matrices have consistent dimensions. More...\n\nbool is_in (Eigen::VectorXd X) const\nIs X contained in this polytope? More...\n\nPolytope operator& (const Polytope &P2)\nIntersect two polytopes that are defined in the same dimension space. More...\n\nPolytope (Eigen::MatrixXd incoming_H, Eigen::VectorXd incoming_K)\n\nPolytope (const Polytope &other)\n\n## Static Public Member Functions\n\nstatic Polytopebox (const Eigen::VectorXd &bounds)\nConstruct Polytope that is an axis-aligned rectangle. More...\n\nstatic PolytoperandomH (int n)\nCreate random Polytope in R^n using Eigen::MatrixXd::Random(). More...\n\n## Friends\n\nstd::ostream & operator<< (std::ostream &out, const Polytope &P)\nOutput this polytope in JSON to given stream. More...\n\n## Detailed Description\n\nBasic half-space representation of polytopes.\n\n## Member Function Documentation\n\n Polytope * integrator_chains::Polytope::box ( const Eigen::VectorXd & bounds )\nstatic\n\nConstruct Polytope that is an axis-aligned rectangle.\n\nParameters\n bounds an array of the form [x1_min, x1_max, x2_min, x2_max, ..., xn_min, xn_max], which defines a polytope in terms of intervals along each axis in R^n. The interval along the first axis is [x1_min, x1_max], the interval along the second axis is [x2_min, x2_max], etc. Thus the length of the given array is 2n.\n\nE.g., a unit square in R^2 can be created using\n\nEigen::Vector4d bounds;\nbounds << 0, 1,\n0, 1;\nPolytope *square = Polytope::box( bounds );\n void integrator_chains::Polytope::dumpJSONcore ( std::ostream & out ) const\n\nOutput this polytope in JSON excluding opening { and closing }.\n\nThis method facilitates inheritance from Polytope without crowding the JSON representations of other classes.\n\n bool integrator_chains::Polytope::is_consistent ( ) const\n\nCheck that defining matrices have consistent dimensions.\n\nThe \"defining matrices\" are those involved in the inequality providing the half-space representation, i.e., H and K in {x | Hx <= K}. N.B., this check does not occur during instantiation of Polytope.\n\n bool integrator_chains::Polytope::is_in ( Eigen::VectorXd X ) const\n\nIs X contained in this polytope?\n\nThe polytope is a closed set. No numerical tolerance is used.\n\n Polytope integrator_chains::Polytope::operator& ( const Polytope & P2 )\n\nIntersect two polytopes that are defined in the same dimension space.\n\n Polytope * integrator_chains::Polytope::randomH ( int n )\nstatic\n\nCreate random Polytope in R^n using Eigen::MatrixXd::Random().\n\nParameters\n n dimension of the containing space.\n\nRandom matrices as provided by Eigen::MatrixXd::Random() are used to instantiate Polytope in half-space representation. The matrices have `n+1` rows, corresponding to `n+1` inequalities.\n\n## Friends And Related Function Documentation\n\n std::ostream& operator<< ( std::ostream & out, const Polytope & P )\nfriend\n\nOutput this polytope in JSON to given stream.\n\nThe documentation for this class was generated from the following file:\n• polytope.hpp"
]
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"http://api.fmrchallenge.org/classintegrator__chains_1_1Polytope__inherit__graph.png",
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https://www.codespeedy.com/difference-of-days-between-two-dates-in-python/ | [
"# How to find the difference or gap of days between two dates in python\n\nIn this tutorial, We will see How to find the difference or gap of days between two dates in python. So Guy’s, No need to fear about it that how we will solve this problem. Here, I am going to provide a simple solution to this problem in python by using datetime module. In order to solve this problem in python language, we have to know datetime module in python language.\n\nYou may also like to read:\n\nWhat is datetime module in python?\n\nPython provide inbuilt module datetime which allow us to solve various problem related to date and time.\n\n## To find the difference or gap of days between two dates in Python\n\nSo, let’s start to understand this problem in easy ways. We will follow these steps in python language:\n\n1. First of all, we will include the date in our python program from datetime module by using import function.\n\n`from datetime import date`\n\n2. We will take the starting date and the ending date of calendar between which you have to find the difference or gap of days.\n\n```Start=date(2019,7,1)\nEnd=date(2019,8,15)```\n\n3. Now, we will find the difference or gap of days between two dates as we have learned to Subtract two number by using minus sign (-) and print gap of days on output page.\n\n```Gap=(End-Start).days\nprint(\"Days gap:\")\nprint(Gap)```\n\n#### Python program to find difference or gap of days\n\nPython program:\n\n```from datetime import date\nStart=date(2019,7,1)\nEnd=date(2019,8,15)\nGap=(End-Start).days\nprint(\"Days gap:\")\nprint(Gap)```\n\nOutput of code:\n\n```Days gap:\n45```\n\nSo Guy’s, I hope you really enjoy this tutorial and feel free to leave a comment if you have any doubt.\n\n### One response to “How to find the difference or gap of days between two dates in python”\n\n1. Vishal says:\n\nHello,\nWhat if I want to create a code where the user can put in 2 dates?\nEverywhere I see, I see the dates are already a part of the code, is there a way to let a user “input” 2 dates?\nThanks!"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.88840854,"math_prob":0.8010707,"size":1820,"snap":"2020-45-2020-50","text_gpt3_token_len":435,"char_repetition_ratio":0.13381058,"word_repetition_ratio":0.10869565,"special_character_ratio":0.2434066,"punctuation_ratio":0.11278196,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9932301,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-10-27T11:38:59Z\",\"WARC-Record-ID\":\"<urn:uuid:974d5f50-621d-4394-a6d3-17f653d2be63>\",\"Content-Length\":\"25731\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:c1bc7dba-85f8-41cf-afb6-91dd5ebb2012>\",\"WARC-Concurrent-To\":\"<urn:uuid:41021375-ca18-4226-9c96-d0b572747671>\",\"WARC-IP-Address\":\"74.207.248.30\",\"WARC-Target-URI\":\"https://www.codespeedy.com/difference-of-days-between-two-dates-in-python/\",\"WARC-Payload-Digest\":\"sha1:4LJHA2AVZWO7A2MP4E6QWIVNFEJZ4YYW\",\"WARC-Block-Digest\":\"sha1:QHYN7YTIW5LRWGN2AACAMQXACQCDBIUD\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-45/CC-MAIN-2020-45_segments_1603107894175.55_warc_CC-MAIN-20201027111346-20201027141346-00195.warc.gz\"}"} |
https://www.exyb.cn/news/show-4555798.html | [
"## 分支语句(选择结构)——“C”\n\nnews/2023/6/6 4:26:01\n\n• 如果你在家,我去拜访你\n• 如果考试不及格,要补考\n• 如果遇到红灯,要停车等待\n\nC语言中有两种选择语句:\n\n• if语句,比较适合实现两个分支的选择结构(比如上课或者不上课,向左还是向右......)\n• switch语句,比较适合实现多分支的选择结构(比如从多个选修课中选择一门,选择一个最喜欢的科目)\n\nif(表达式)\n\n语句;\n\nif(表达式)\n\n语句1;\n\nelse\n\n语句2;\n\n//多分支\n\nif(表达式1)\n\n语句1;\n\nelse if(表达式2)\n\n语句2;\n\nelse\n\n语句3;\n\n例1:输入两个实数,按代数值由小到大的顺序输出这两个数\n\n解题思路:\n\n只需要做一次比较,然后进行一次交换即可\n\n用if语句实现条件决断\n\n想要实现两个变量值的互换,则要定义第三个变量\n\n这是这个题目的一段小代码,我们一起来看看\n\n``````#include<stdio.h>\nint main()\n{float a=0.0;float b=0.0;float tmp=0.0;scanf(\"%f %f\",&a,&b);if(a>b){tmp=a;a=b;b=tmp;}printf(\"%.2f,%.2f\\n\",a,b);return 0;\n}``````\n\n解题思路:可以先用伪代码写出算法\n\nif a>b,a和b对换 (a是a、b中的小者)\n\nif a>c,a和c对换 (a是三者中的最小者)\n\nif b>c,b和c对换 (b是三者中次小者)\n\n顺序输出a,b,c\n\n``````#include<stdio.h>\nint main()\n{int a=0;int b=0;int c=0;int tmp=0;scanf(\"%d %d %d\",&a,&b,&c);if(a>b){tmp=a; a=b;b=tmp;}if(a>c){tmp=a;a=c;c=tmp;}if(b>c){tmp=b;b=c;c=tmp;}printf(\"%d %d %d\",a,b,c);return 0;\n}``````\n\n当你写了这样一个具有迷惑性的代码:\n\n``````#include<stdio.h>\nint main()\n{int a=0;int b=2;if(a==1)if(b==2)printf(\"hehe\\n\");else printf(\"haha\\n\");return 0;\n}``````\n\n``````//适当地使用{}可以使代码的逻辑更加清楚\n//代码风格很重要\n#include<stdio.h>\nint main()\n{int a=0;int b=2;if(a==1){if(b==2){printf(\"hehe\\n\");}}else{printf(\"haha\\n\");}return 0;\n}``````\n\n哈哈,这个代码的输出结果就确确实实为haha了\n\nswitch是“开关”的意思,它也是一种选择语句,常常用于多分支的情况\n\nswitch和if\n\n从功能上说,switch语句和if语句完全可以相互替代。但从编程的角度,它们又各有各的特点,所以至今为止,也不能说谁可以完全取代谁。\n\n当嵌套的if比较少时(三个以内),用if编程程序会比较简洁。但是当选择的分支比较多时,嵌套的if语句层数就会很多,导致程序冗长,可读性下降。因此C语言提供switch语句来处理多分支选择。在很多大型的项目中,多分支选择的情况经常会遇到,所以switch语句用得还是比较多的。\n\nswitch语句说明\n\nswitch语句的作用是根据表达式的值,使流程跳转到不同的语句\n\n下面,来给大家举几个例子来深入说明一下switch语句\n\n解题思路:\n\n判断出这是一个多分支选择问题\n\n根据百分制分数将学生成绩分为4个等级\n\n如果用if语句,至少要用三层嵌套的if,进行3次检查判断\n\n用switch语句进行一次检查即可得到结果\n\n``````#include<stdio.h>\nint main()\n}``````\n\nbreak语句的实际效果是把语句列表划分为不同的分支部分。\n\n在最后一个 case 语句的后面加上一条 break语句。\n\n(之所以这么写是可以避免出现在以前的最后一个 case 语句后面忘了添加 break语句)\n\ndefault子句\n\n s<250 没有折扣 250==3000 15%折扣\n\n解题思路:\n\n设每吨每千米货物的基本运费为p,货物重量为w,距离为s,折扣为d\n\n总运费的计算公式为f=p*w*s*(1-d)\n\n计算等式中p、w、s为用户输入,所以关键是要找到折扣d的变化规律,由题可知折扣d与输入距离s有关,而且“变化点”都是250的倍数,故引入一折扣变量c,令c的值为s/250,即c代表250的倍数。\n\n即当c<1时,表示s<250,无折扣\n\n1=<c<2时,表示250=<s<500,折扣d=2%\n\n2=<c<4时,表示500=<s<1000,折扣d=5%\n\n4=<c<8时,表示1000=<s<2000,折扣d=8%\n\n8=<c<12时,表示2000=<s<3000,折扣d=10%\n\nc>=12时,表示s>=3000,折扣d=15%\n\n``````#include<stdio.h>\nint main()\n{int c=0;//倍数int s=0;//距离float p=0.0;//每吨每千米货物的基本运费float w=0.0;//货物的重量float d=0.0;//折扣float f=0.0;//总运费printf(\"please enter price,weight,distance:\");scanf(\"%f %f %d\",&p,&w,&s);if(s>=3000){c=12;}else {c=s/250;}switch(c){case 0:d=0;break;case 1:d=2;break;case 2:case 3:d=5;break;case 4:case 5:case 6:case 7:d=8;break;case 8:case 9:case 10:case 11:d=10;break;case 12:d=15;break;}f=p*w*s*(1-d/100);printf(\"freight=%10.2f\\n\",f);return 0;\n}``````\n\n### 运算放大器:运放的平衡电阻\n\n1.主要运放参数 集成运放的基本参数很多,包括静态技术指标(直流参数)和动态技术指标(交流参数)。。例如,输入失调电压、输入失调电流、输入偏置电流、输入失调电压温漂、最大差模输入电压、最大…"
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| {"ft_lang_label":"__label__zh","ft_lang_prob":0.8239567,"math_prob":0.9927211,"size":3900,"snap":"2023-14-2023-23","text_gpt3_token_len":2877,"char_repetition_ratio":0.11524641,"word_repetition_ratio":0.013953488,"special_character_ratio":0.30564103,"punctuation_ratio":0.1948718,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.95071197,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-06-05T20:26:01Z\",\"WARC-Record-ID\":\"<urn:uuid:3feaeb6e-a9e7-4d08-982b-b3093774d4b3>\",\"Content-Length\":\"30540\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:5f8cfcec-a6ba-40da-82c0-66e37a50d3cc>\",\"WARC-Concurrent-To\":\"<urn:uuid:4ae82759-21f3-4540-9c29-20f222d730b2>\",\"WARC-IP-Address\":\"43.154.132.222\",\"WARC-Target-URI\":\"https://www.exyb.cn/news/show-4555798.html\",\"WARC-Payload-Digest\":\"sha1:OQ65VXFUTYLKDLOOBJPKZ3WNTS75VOTI\",\"WARC-Block-Digest\":\"sha1:24MFO355XRGJHT3XLJIOAD3IFWXVV6HC\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-23/CC-MAIN-2023-23_segments_1685224652161.52_warc_CC-MAIN-20230605185809-20230605215809-00625.warc.gz\"}"} |
https://alb.codehs.com/info/standards/explore/OH-CTE | [
"# Ohio CTE Framework\n\n## Standards\n\nStandard Description\n2.3.1. Identify and explain coding information and representation of characters (e.g., American Standard Code for Information Interchange [ASCII], Extended Binary Coded Decimal Interchange Code [EBCDIC], Unicode). Lessons\n2.3.2. Convert between numbering systems (e.g., binary, hexadecimal, decimal). Lessons\n2.9.1. Identify and incorporate branding strategies. Lessons\n2.9.2. Determine the scope and purpose of the project. Lessons\n2.9.3. Determine the target audience, client needs, expected outcomes, objectives, and budget. Lessons\n2.9.4. Develop a conceptual model and design brief for the project. Lessons\n2.9.5. Develop a timeline, a communication plan, a task breakdown, costs (e.g., equipment, labor), deliverables, and responsibilities for completion. Lessons\n2.9.6. Develop and present a comprehensive proposal to stakeholders. Lessons\n2.11.1. Identify the problem. Lessons\n2.11.2. Select troubleshooting methodology (e.g., top down, bottom up, follow the path, spot the differences). Lessons\n2.11.3. Investigate symptoms based on the selected methodology. Lessons\n2.11.4. Gather and analyze data about the problem. Lessons\n2.11.5. Design a solution. Lessons\n2.11.6. Test a solution. Lessons\n2.11.7. Implement a solution. Lessons\n2.11.8. Document the problem and the verified solution. Lessons\n2.12.1. Create a written procedure agreed by the stakeholders and project team for determining the acceptability of the project deliverables. Lessons\n2.12.2. Develop a test system that accurately mimics external interfaces. Lessons\n2.12.3. Develop test cases that are realistic, compare with expected performance, and include targeted platforms and device types. Lessons\n2.12.4. Develop, perform, and document usability and testing integration. Lessons\n2.12.5. Make corrections indicated by test results. Lessons\n2.12.6. Seek stakeholder acceptance upon successful completion of the test plan. Lessons\n2.13.1. Include overall project goals and timelines in the rollout plan. Lessons\n2.13.2. Communicate rollout plans to key stakeholders in a timely manner. Lessons\n2.13.3. Conduct final review and approvals according to company standards. Lessons\n2.13.4. Identify support staff, training needs, and contingency plans in the rollout plan. Lessons\n2.13.5. Test delivered application to assure that it is fully functional for the customer or user and meets all requirements. Lessons\n2.13.6. Deliver support and training materials. Lessons\n5.1.1. Describe how computer programs and scripts can be used to solve problems (e.g., desktop, mobile, enterprise). Lessons\n5.1.2. Explain how algorithms and data structures are used in information processing. Lessons\n5.1.3. Model the solution using both graphic tools (e.g., flowcharts) and pseudocode techniques. Lessons\n5.1.4. Describe, compare, and contrast the basics of procedural, structured, object-oriented (OO), and event driven programming. Lessons\n5.1.5. Describe the concepts of data management through programming languages. Lessons\n5.1.6. Analyze the strengths and weaknesses of different languages for solving a specific problem. Lessons\n5.1.7. Compare the functions and operations of compilers and interpreters. Lessons\n5.1.8. Describe version control and the relevance of documentation. Lessons\n5.2.1. Compare primitive types of numeric and nonnumeric data (e.g., integers, floats, Boolean, strings). Lessons\n5.2.2. Identify the scope of data (e.g., global versus local, variables, constants, arrays). Lessons\n5.2.3. Write code that uses arithmetic operations. Lessons\n5.2.4. Write code that uses subtotals and final totals. Lessons\n5.2.5. Write code that applies string operations (e.g., concatenation, pattern matching, substring). Lessons\n5.3.1. Explain Boolean logic. Lessons\n5.3.2. Solve a truth table. Lessons\n5.3.3. Write code that uses logical operators (e.g., and, or, not). Lessons\n5.3.4. Write code that uses relational operators and compound conditions. Lessons\n5.3.5. Write code that uses conditional control structures (e.g., if, if-then-else). Lessons\n5.3.6. Write code that uses repetition control structures (e.g., while, for). Lessons\n5.3.7. Write code that uses selection control structures (e.g., case, switch). Lessons\n5.3.8. Write code that uses nested structures and recursion. Lessons\n5.3.9. Write code that creates and calls functions. Lessons\n5.3.10. Code error handling techniques. Lessons\n5.3.11. Write code to access data repositories. Lessons\n5.3.12. Write code to create classes, objects, and methods. Lessons\n5.4.1. Configure options, preferences, and tools. Lessons\n5.4.2. Write and edit code in the integrated development environment (IDE). Lessons\n5.4.3. Compile or interpret a working program. Lessons\n5.4.4. Define test cases. Lessons\n5.4.5. Test the program using defined test cases. Lessons\n5.4.6. Correct syntax and runtime errors. Lessons\n5.4.7. Debug logic errors. Lessons\n5.5.1. Develop programs using data validation techniques. Lessons\n5.5.2. Develop programs that use reuse libraries. Lessons\n5.5.3. Develop programs using operating system calls. Lessons\n5.5.4. Develop programs that call other programs. Lessons\n5.5.5. Use appropriate naming conventions and apply comments. Lessons\n5.5.6. Format output (e.g., desktop, mobile, enterprise, reports, data files). Lessons\n5.6.1. Determine requirements specification documentation. Lessons\n5.6.2. Identify constraints and system processing requirements. Lessons\n5.6.3. Develop and adhere to timelines. Lessons\n5.6.4. Identify a programming language, framework, and an integrated development environment (IDE). Lessons\n5.6.5. Identify input and output (I/O) requirements. Lessons\n5.6.6. Design system inputs, outputs, and processes. Lessons\n5.6.7. Document a design using the appropriate tools (e.g., program flowchart, dataflow diagrams, Unified Modeling Language [UML]). Lessons\n5.6.8. Create documentation (e.g., implementation plan, contingency plan, data dictionary, user help). Lessons\n5.6.9. Review the design (e.g., peer walkthrough). Lessons\n5.6.10. Present the system design to stakeholders. Lessons\n5.6.11. Develop the application. Lessons\n5.6.12. Compare software methodologies (e.g., agile, waterfall). Lessons\n5.6.13. Perform code reviews (e.g., peer walkthrough, static analysis). Lessons\n5.6.14. Ensure code quality by testing and debugging the application (e.g., system testing, user acceptance testing). Lessons\n5.6.15. Train stakeholders. Lessons\n5.6.16. Deploy the application. Lessons\n5.6.17. Collect application feedback and maintain the application. Lessons\n5.7.1. Explain version management and interface control. Lessons\n5.7.2. Explain baseline and software lifecycle phases. Lessons\n5.7.3. Analyze the impact of changes. Lessons\n6.3.1. Select and apply scripting languages used in web development. Lessons"
]
| [
null
]
| {"ft_lang_label":"__label__en","ft_lang_prob":0.6287717,"math_prob":0.7769306,"size":7132,"snap":"2022-27-2022-33","text_gpt3_token_len":2042,"char_repetition_ratio":0.23835579,"word_repetition_ratio":0.008088979,"special_character_ratio":0.29080203,"punctuation_ratio":0.29904762,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9695059,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2022-08-07T23:01:22Z\",\"WARC-Record-ID\":\"<urn:uuid:0eac5f73-6a8c-441f-989b-541720272a24>\",\"Content-Length\":\"191317\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:649e4a12-09aa-4f56-bf82-cbc9f51ba43c>\",\"WARC-Concurrent-To\":\"<urn:uuid:78a57bc5-8423-44f5-9b0b-519deb430a0a>\",\"WARC-IP-Address\":\"52.85.132.81\",\"WARC-Target-URI\":\"https://alb.codehs.com/info/standards/explore/OH-CTE\",\"WARC-Payload-Digest\":\"sha1:X7UIRPIXXXT6HKJVXV5Y3SIMYU2U2MXA\",\"WARC-Block-Digest\":\"sha1:KSRQ3RZZR3F2HTF6IONKPZ6NLXCBR6EC\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2022/CC-MAIN-2022-33/CC-MAIN-2022-33_segments_1659882570730.59_warc_CC-MAIN-20220807211157-20220808001157-00441.warc.gz\"}"} |
https://gis.stackexchange.com/questions/115822/calculate-fields-with-null-values-using-arcpy-da-updatecursor-of-arcgis-for-desk | [
"Calculate Fields with Null Values using arcpy.da.UpdateCursor of ArcGIS for Desktop?\n\nHow do you calculate fields with null values? I have multiple fields that may have null values, that aren't being calculated in the third field.",
null,
"import arcpy\nwith arcpy.da.UpdateCursor(r\"...gdb\\test.gdb\\test\",[\"A\", \"B\", \"C\"]) as cursor:\nfor row in cursor:\nrow = row + row\ncursor.updateRow(row)\n\nThe result of that calculation is this error:\n\nTraceback (most recent call last):\nFile \"C:\\Users\\Desktop\\updatecursor2.py\", line 4, in <module>\nrow = row + row\nTypeError: unsupported operand type(s) for +: 'NoneType' and 'float'\n\nThe result of the script are the same results when I try to use the field calculator:",
null,
"How do you use the data update cursor, or field calculator to calculate the sum of the values in a new field if you have null values?\n\nI'm using ArcGIS 10.1 SP1 for Desktop.\n\n• What are the data types of these fields? It looks like you are trying to set the value of field \"A\" (2) with the sum of the values from ObjectID (0), and Shape (1). I also don't think you are setting the values correctly. – jbchurchill Oct 1 '14 at 13:37\n• @jbchurchill The data type is Double. – user3767931 Oct 1 '14 at 13:38\n• @jbchurchill FYI, when using data access cursors, the index numbers correspond to the user-supplied attribute list (in this case [\"A\",\"B\",\"C\"]) and not the list of all fields in the table, so they were being referenced correctly. – nmpeterson Oct 1 '14 at 14:31\n• Ah I see that now. So those values are being set correctly after all. – jbchurchill Oct 1 '14 at 14:34\n• What do you want to do if A and/or B is Null? Give C the value of the non-Null field, if there is one, or skip it, leaving C Null? – recurvata Oct 1 '14 at 15:05\n\nHere's a way to replace all the nulls with zeroes:\n\nimport arcpy\nwith arcpy.da.UpdateCursor(r\"...gdb\\test.gdb\\test\",[\"A\", \"B\", \"C\"]) as cursor:\nfor row in cursor:\na_value = row if row else 0 # Use 0 when \"A\" is falsy\nb_value = row if row else 0 # Use 0 when \"B\" is falsy\nrow = a_value + b_value\ncursor.updateRow(row)\n\nNote: this doesn't actually update the null values in the table; it merely replaces them with zeroes during calculations. If you want to replace the nulls with zeroes permanently, you could change the penultimate line to row = [a_value, b_value, a_value + b_value].\n\n• You could take advantage of the way Python does boolean expressions and simply do a_value = row or 0 – Jason Scheirer Oct 3 '14 at 22:00\n\nLets start with the field calculator. it should look like these 2 screenshots.",
null,
"",
null,
"When I calculate fields inside of an Update cursor (update_cursor) it looks more like this. Here I have a SearchCursor (row is set to searchCursor.next) and an update Cursor (row2 is set to update_cursor.next). This is actually slightly different since I am using values in a different layer for the updates and a selection.\n\nwhile row:\nwhile row2:\ngrpnumValue = row2.getValue(\"A\")\nif (grpnumValue > 0):\nrow.setValue(\"MAILING_GROUP\", grpnumValue)\nrow2 = searchCursor.next\nrow = update_cursor.next()"
]
| [
null,
"https://i.stack.imgur.com/bWNCw.jpg",
null,
"https://i.stack.imgur.com/hZwOU.jpg",
null,
"https://i.stack.imgur.com/PXRUL.jpg",
null,
"https://i.stack.imgur.com/9H7sK.jpg",
null
]
| {"ft_lang_label":"__label__en","ft_lang_prob":0.816297,"math_prob":0.8318572,"size":932,"snap":"2019-43-2019-47","text_gpt3_token_len":255,"char_repetition_ratio":0.13038793,"word_repetition_ratio":0.013513514,"special_character_ratio":0.2832618,"punctuation_ratio":0.16256158,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.97314256,"pos_list":[0,1,2,3,4,5,6,7,8],"im_url_duplicate_count":[null,2,null,2,null,2,null,2,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-10-24T02:10:17Z\",\"WARC-Record-ID\":\"<urn:uuid:66a087ba-a10e-4595-a7c4-58b66f422934>\",\"Content-Length\":\"153831\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:9554e577-7ba9-43bd-9a85-50f540c783a3>\",\"WARC-Concurrent-To\":\"<urn:uuid:2e566a43-a811-4b52-80db-788a4b7d21b6>\",\"WARC-IP-Address\":\"151.101.193.69\",\"WARC-Target-URI\":\"https://gis.stackexchange.com/questions/115822/calculate-fields-with-null-values-using-arcpy-da-updatecursor-of-arcgis-for-desk\",\"WARC-Payload-Digest\":\"sha1:B3CGWBY7GHMIRJD3PVTF3BRUUZQB2EQF\",\"WARC-Block-Digest\":\"sha1:RL6KURMILABFXXSGXZB72IHYJFYQUSCY\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-43/CC-MAIN-2019-43_segments_1570987838289.72_warc_CC-MAIN-20191024012613-20191024040113-00521.warc.gz\"}"} |
https://www.thebalancesmb.com/liquidity-position-analysis-with-ratios-393233 | [
"# Analysis of Liquidity Position Using Financial Ratios\n\nIn this article, we will consider some commonly used liquidity ratios used in the financial analysis of a company. A balance sheet is provided as an example for calculating a company's financial position by measuring its liquidity, which is the ability to pay its current debt with its current assets. The information reflects two years of data for a hypothetical company.\n\nThe balance sheet data will also be used to calculate the current ratio, quick ratio, and net working capital, as well as provide an explanation of each as well as the meaning of changes from year to year. The results can be replicated for your own firm or one that you are interested in investing in.\n\n## Calculate the Company's Current Ratio\n\nThe first step in liquidity analysis is to calculate the company's current ratio. The current ratio shows how many times over the firm can pay its current debt obligations based on its assets. \"Current\" usually means a short time period of less than twelve months. The formula is:\n\nCurrent Ratio = Current Assets/Current Liabilities\n\nIn the balance sheet, you can see the highlighted numbers. Those are the ones you use for the calculation. For 2018, the calculation would be:\n\nCurrent Ratio = \\$708/\\$540 = 1.311 X\n\nThis means that the firm can meet its current short-term debt obligations 1.311 times over. In order to stay solvent, the firm must have a current ratio of at least 1.0 X, which means it can exactly meet its current debt obligations. So, this firm is solvent.\n\nHowever, in this case, the firm is a little more liquid than that. It can meet its current debt obligations and have a little left over. If you calculate the current ratio for 2017, you will see that the current ratio was 1.182 X. So, the firm improved its liquidity in 2018 which, in this case, is good as it is operating with relatively low liquidity.\n\n## Calculate the Company's Quick Ratio or Acid Test\n\nThe second step in liquidity analysis is to calculate the company's quick ratio or acid test. The quick ratio is a more stringent test of liquidity than the current ratio. It looks at how well the company can meet its short-term debt obligations without having to sell any of its inventory to do so.\n\nInventory is the least liquid of all the current assets because you have to find a buyer for your inventory. Finding a buyer, especially in a slow economy, is not always possible. Therefore, firms want to be able to meet their short-term debt obligations without having to rely on selling inventory. The formula is:\n\nQuick Ratio = Current Assets-Inventory/Current Liabilities.\n\nIn the balance sheet, you can see the highlighted numbers. Those are the ones you use for the calculation. For 2018, the calculation would be:\n\nQuick Ratio = \\$708-\\$422/\\$540 = 0.529 X.\n\nThis means that the firm cannot meet its current short-term debt obligations without selling inventory because the quick ratio is 0.529 X, which is less than 1.0 X. In order to stay solvent and pay its short-term debt without selling inventory, the quick ratio must be at least 1.0 X, which it is not.\n\nHowever, in this case, the firm will have to sell inventory to pay its short-term debt. If you calculate the quick ratio for 2017, you will see that it was 0.458 X. So, the firm improved its liquidity by 2018 which, in this case, is good, as it is operating with relatively low liquidity. It needs to improve its quick ratio to above 1.0 X so it won't have to sell inventory to meet its short-term debt obligations.\n\n## Calculate the Company's Net Working Capital\n\nA company's net working capital is the difference between its current assets and current liabilities:\n\nNet Working Capital = Current Assets - Current Liabilities\n\nFor 2018, this company's net working capital would be:\n\n\\$708 - 540 = \\$168\n\nFrom this calculation, you know you have positive net working capital with which to pay short-term debt obligations before you even calculate the current ratio. You should be able to see the relationship between the company's net working capital and its current ratio.\n\nFor 2017, the company's net working capital was \\$99, so its net working capital position, and, thus, its liquidity position, has improved from 2017 to 2018."
]
| [
null
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.9627623,"math_prob":0.9341934,"size":5181,"snap":"2021-31-2021-39","text_gpt3_token_len":1100,"char_repetition_ratio":0.15549546,"word_repetition_ratio":0.12429378,"special_character_ratio":0.22254391,"punctuation_ratio":0.10858835,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.98586506,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-09-22T13:29:46Z\",\"WARC-Record-ID\":\"<urn:uuid:c5b4890a-1bee-4aee-8040-f806dd1b84e3>\",\"Content-Length\":\"145193\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:02d46a1e-52dc-42cc-a4a6-f301acaf974b>\",\"WARC-Concurrent-To\":\"<urn:uuid:726f56c7-7fba-418a-b32c-4f101ceeb109>\",\"WARC-IP-Address\":\"199.232.66.137\",\"WARC-Target-URI\":\"https://www.thebalancesmb.com/liquidity-position-analysis-with-ratios-393233\",\"WARC-Payload-Digest\":\"sha1:VB7NSKMMIRI7GKRQZ4Y4AON4S4L47V2D\",\"WARC-Block-Digest\":\"sha1:KQCMWTIMRG7CWDEHB72PIVPIRKDQK3AN\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-39/CC-MAIN-2021-39_segments_1631780057366.40_warc_CC-MAIN-20210922132653-20210922162653-00641.warc.gz\"}"} |
https://www.intmath.com/blog/videos/friday-math-movie-how-to-use-the-quadratic-formula-by-hector-the-battle-droid-1248 | [
"Search IntMath\nClose\n\n# How To Use the Quadratic Formula by Hector the Battle Droid\n\nBy Murray Bourne, 20 Jun 2008\n\nThis week's math movie is fun.\n\nThe title says it all...\n\nIt's quite a clever compilation of social commentary with an important mathematical concept. The quadratic formula arises a lot when solving math problems, because the curve of a quadratic (a parabola) is an elegant simple shape, and can be used to model many real-life situations.\n\nWell anyway, the video is not a bad way to revise the quadratic formula.\n\nBe the first to comment below.\n\n### Comment Preview\n\nHTML: You can use simple tags like <b>, <a href=\"...\">, etc.\n\nTo enter math, you can can either:\n\n1. Use simple calculator-like input in the following format (surround your math in backticks, or qq on tablet or phone):\na^2 = sqrt(b^2 + c^2)\n(See more on ASCIIMath syntax); or\n2. Use simple LaTeX in the following format. Surround your math with $$ and $$.\n$$\\int g dx = \\sqrt{\\frac{a}{b}}$$\n(This is standard simple LaTeX.)\n\nNOTE: You can mix both types of math entry in your comment."
]
| [
null
]
| {"ft_lang_label":"__label__en","ft_lang_prob":0.87548465,"math_prob":0.97498626,"size":531,"snap":"2023-40-2023-50","text_gpt3_token_len":118,"char_repetition_ratio":0.121442124,"word_repetition_ratio":0.0,"special_character_ratio":0.21657251,"punctuation_ratio":0.11320755,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.995673,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-12-07T06:00:16Z\",\"WARC-Record-ID\":\"<urn:uuid:55a2166b-8bae-421f-af7c-c142ba50016c>\",\"Content-Length\":\"123023\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:4fb9ccb4-0d11-49f5-90d0-503d0a5aca0d>\",\"WARC-Concurrent-To\":\"<urn:uuid:c592aedc-c518-40b1-b883-236460ad0345>\",\"WARC-IP-Address\":\"104.26.13.103\",\"WARC-Target-URI\":\"https://www.intmath.com/blog/videos/friday-math-movie-how-to-use-the-quadratic-formula-by-hector-the-battle-droid-1248\",\"WARC-Payload-Digest\":\"sha1:QJDBCT3YTUPDUIHZIBQDS4HGCQ3P772Z\",\"WARC-Block-Digest\":\"sha1:43A6NE6Y7AV26ZFJHHLSTQVY4FQMUBBZ\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-50/CC-MAIN-2023-50_segments_1700679100650.21_warc_CC-MAIN-20231207054219-20231207084219-00572.warc.gz\"}"} |
https://theshippingforecastmusic.com/qa/is-ranking-categorical-or-quantitative.html | [
"",
null,
"# Is Ranking Categorical Or Quantitative?\n\n## Is rating categorical or quantitative?\n\nSatisfaction ratings on a scale from 1 to 5.\n\nAlthough these are represented by numbers, they do not represent a count or true measurement.\n\nSuch ratings are categorical..\n\n## Is height categorical or quantitative?\n\nIn our medical example, age is an example of a quantitative variable because it can take on multiple numerical values. It also makes sense to think about it in numerical form; that is, a person can be 18 years old or 80 years old. Weight and height are also examples of quantitative variables.\n\n## What are the 3 types of variables?\n\nA variable is any factor, trait, or condition that can exist in differing amounts or types. An experiment usually has three kinds of variables: independent, dependent, and controlled.\n\n## What are the two types of categorical data?\n\nThere are two types of categorical data, namely; the nominal and ordinal data. Nominal Data: This is a type of data used to name variables without providing any numerical value.\n\n## What is categorical data used for?\n\nCategorical data is a good way of collecting information that doesn’t present itself in the form of numbers or if the numbers needed to be grouped to analyze. Categorical data is data that is collected in groups or topics; the number of events in each group is counted numerically.\n\n## What is categorical data with examples?\n\nCategorical variables represent types of data which may be divided into groups. Examples of categorical variables are race, sex, age group, and educational level. There are 8 different event categories, with weight given as numeric data. …\n\n## Can time be a categorical variable?\n\nCategorical data might not have a logical order. For example, categorical predictors include gender, material type, and payment method. Discrete variables are numeric variables that have a countable number of values between any two values. … A continuous variable can be numeric or date/time.\n\n## What are the 5 types of variables?\n\nThere are six common variable types:DEPENDENT VARIABLES.INDEPENDENT VARIABLES.INTERVENING VARIABLES.MODERATOR VARIABLES.CONTROL VARIABLES.EXTRANEOUS VARIABLES.\n\n## Are yes or no questions categorical or quantitative?\n\nThe Categorical Variable Another instance of categorical variables is answers to yes and no questions.\n\n## What are the 4 types of data?\n\nIn statistics, there are four data measurement scales: nominal, ordinal, interval and ratio. These are simply ways to sub-categorize different types of data (here’s an overview of statistical data types) .\n\n## Is age categorical or continuous?\n\nMondal suggests that age can be viewed as a discrete variable because it is commonly expressed as an integer in units of years with no decimal to indicate days and presumably, hours, minutes, and seconds."
]
| [
null,
"https://mc.yandex.ru/watch/66677008",
null
]
| {"ft_lang_label":"__label__en","ft_lang_prob":0.8343634,"math_prob":0.9604684,"size":3179,"snap":"2020-45-2020-50","text_gpt3_token_len":638,"char_repetition_ratio":0.20409448,"word_repetition_ratio":0.11787819,"special_character_ratio":0.19723183,"punctuation_ratio":0.13559322,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9835442,"pos_list":[0,1,2],"im_url_duplicate_count":[null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-11-26T23:44:41Z\",\"WARC-Record-ID\":\"<urn:uuid:e1585146-6b4b-4759-8eec-722b7264bb9d>\",\"Content-Length\":\"34255\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:77dbde19-0db5-4ac3-9a03-c9733904971b>\",\"WARC-Concurrent-To\":\"<urn:uuid:f1b8a5bf-9d88-4dbf-ac76-b317cbccad73>\",\"WARC-IP-Address\":\"87.236.16.235\",\"WARC-Target-URI\":\"https://theshippingforecastmusic.com/qa/is-ranking-categorical-or-quantitative.html\",\"WARC-Payload-Digest\":\"sha1:R75JV7ZRRYLMDJ6VAGU2DD3VDQJSO7QG\",\"WARC-Block-Digest\":\"sha1:YEN3CYUZZS4OM5G33C7362AJ3UOD3SMS\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-50/CC-MAIN-2020-50_segments_1606141189030.27_warc_CC-MAIN-20201126230216-20201127020216-00593.warc.gz\"}"} |
https://www.analyticsvidhya.com/blog/2017/05/questions-python-for-data-science/ | [
"Faizan Shaikh — May 4, 2017\n\nPython is increasingly becoming popular among data science enthusiasts, and for right reasons. It brings the entire ecosystem of a general programming language. So you can not only transform and manipulate data, but you can also create strong pipelines and machine learning workflows in a single ecosystem.\n\nAt Analytics Vidhya, we love Python. Most of us use Python as our preferred tool for machine learning. Not only this, if you want to learn Deep Learning, Python clearly has the most mature ecosystem among all other languages.\n\nLearning Python is the first step in your Data Science Journey. Want to know what are the milestones in Data Science Journey and how to achieve them? Check out the complete Data Science Roadmap! Click here to Download.\n\nIf you are learning Python for Data Science, this test was created to help you assess your skill in Python. This test was conducted as part of DataFest 2017. Close to 1,300 people participated in the test with more than 300 people taking this test.\n\nBelow are the distribution scores of the people who took the test:",
null,
"You can access the final scores here. Here are a few statistics about the distribution.\n\nMean Score: 14.16\n\nMedian Score: 15\n\nMode Score: 0",
null,
"Question Context 1\n\nYou must have seen the show “How I met your mother”. Do you remember the game where they played, in which each person drinks a shot whenever someone says “but, um”. I thought of adding a twist to the game. What if you could use your technical skills to play this game?\n\nTo identify how many shots a person is having in the entire game, you are supposed to write a code.\n\nBelow is the subtitle sample script.\n\nNote: Python regular expression library has been imported as re.\n\n```txt = '''450\n00:17:53,457 --> 00:17:56,175\nOkay, but, um,\nthanks for being with us.\n\n451\n00:17:56,175 --> 00:17:58,616\nBut, um, if there's any\ncollege kids watching,\n\n452\n00:17:58,616 --> 00:18:01,610\nBut, um, but, um, but, um,\nbut, um, but, um,\n\n453\n00:18:01,610 --> 00:18:03,656\nWe have to drink, professor.```\n```454\n00:18:03,656 --> 00:18:07,507\nIt's the rules.\nShe said \"But, um\"\n\n455\n00:18:09,788 --> 00:18:12,515\nBut, um, but, um, but, um...\ngod help us all.\n'''```\n\n1) Which of the following codes would be appropriate for this task?\n\nA) len(re.findall(‘But, um’, txt))\n\nB) re.search(‘But, um’, txt).count()\n\nC) len(re.findall(‘[B,b]ut, um’, txt))\n\nD) re.search(‘[B,b]ut, um’, txt)).count()\n\nQuestion Context 2\n\nSuppose you are given the below string\n\n[email protected],aa,Owner,2014\n[email protected],bb,Member,2015\n[email protected],cc,Member,2017\n[email protected],dd,Member,2016\n[email protected],ee,Member,2020\n“””\n\nIn order to extract only the domain names from the email addresses from the above string (for eg. “aaa”, “bbb”..) you write the following code:\n\n```for i in re.finditer('([a-zA-Z]+)@([a-zA-Z]+).(com)', str):\nprint i.group(__)```\n\n2) What number should be mentioned instead of “__” to index only the domains?\n\nNote: Python regular expression library has been imported as re.\n\nA) 0\n\nB) 1\n\nC) 2\n\nD) 3\n\nQuestion Context 3\n\nYour friend has a hypothesis – “All those people who have names ending with the sound of “y” (Eg: Hollie) are intelligent people.” Please note: The name should end with the sound of ‘y’ but not end with alphabet ‘y’.\n\nNow you being a data freak, challenge the hypothesis by scraping data from your college’s website. Here’s data you have collected.\n\n Name Marks Andy 0 Mandi 10 Sandy 20 Hollie 18 Molly 19 Dollie 15\n\nYou want to make a list of all people who fall in this category. You write following code do to the same:\n\n```temp = []\nfor i in re.finditer(pattern, str):\ntemp.append(i.group(1))```\n\n3) What should be the value of “pattern” in regular expression?\n\nNote: Python regular expression library has been imported as re.\n\nA) pattern = ‘(i|ie)(,)’\n\nB) pattern = ‘(i\\$|ie\\$)(,)’\n\nC) pattern = ‘([a-zA-Z]+i|[a-zA-Z]+ie)(,)’\n\nD) None of these\n\nQuestion Context 4\n\nAssume, you are given two lists:\n\na = [1,2,3,4,5]\n\nb = [6,7,8,9]\n\nThe task is to create a list which has all the elements of a and b in one dimension.\n\nOutput:\n\na = [1,2,3,4,5,6,7,8,9]\n\n4) Which of the following option would you choose?\n\nA) a.append(b)\n\nB) a.extend(b)\n\nC) Any of the above\n\nD) None of these\n\n5) You have built a machine learning model which you wish to freeze now and use later. Which of the following command can perform this task for you?\n\nNote: Pickle library has been imported as pkl.\n\nA) push(model, “file”)\n\nB) save(model, “file”)\n\nC) dump(model, “file”)\n\nD) freeze(model, “file”)\n\nQuestion Context 6\n\nWe want to convert the below string in date-time value:\n\n```import time\nstr = '21/01/2017'\ndatetime_value = time.strptime(str,date_format)```\n\n6) To convert the above string, what should be written in place of date_format?\n\nA) “%d/%m/%y”\n\nB) “%D/%M/%Y”\n\nC) “%d/%M/%y”\n\nD) “%d/%m/%Y”\n\nSolution: (D)\n\nOption D is correct\n\nQuestion Context 7\n\nI have built a simple neural network for an image recognition problem. Now, I want to test if I have assigned the weights & biases for the hidden layer correctly. To perform this action, I am giving an identity matrix as input. Below is my identity matrix:\n\nA = [ 1, 0, 0\n0, 1, 0\n0, 0, 1]\n\n7) How would you create this identity matrix in python?\n\nNote: Library numpy has been imported as np.\n\nA) np.eye(3)\n\nB) identity(3)\n\nC) np.array([1, 0, 0], [0, 1, 0], [0, 0, 1])\n\nD) All of these\n\nSolution: (A)\n\nOption B does not exist (it should be np.identity()). And option C is wrong, because the syntax is incorrect. So the answer is option A\n\n8) To check whether the two arrays occupy same space, what would you do?\n\nI have two numpy arrays “e” and “f”.\n\nYou get the following output when you print “e” & “f”\n\n```print e\n[1, 2, 3, 2, 3, 4, 4, 5, 6]\nprint f\n[[1, 2, 3], [2, 3, 4], [4, 5, 6]]```\n\nWhen you change the values of the first array, the values for the second array also changes. This creates a problem while processing the data.\n\nFor example, if you set the first 5 values of e as 0; i.e.\n\n```print e[:5]\n\n0\n```\n\nthe final values of e and f are\n\n```print e\n\n[0, 0, 0, 0, 0, 4, 4, 5, 6]\n\nprint f\n\n[[0, 0, 0], [0, 0, 4], [4, 5, 6]]```\n\nYou surmise that the two arrays must have the same space allocated.\n\nA) Check memory of both arrays, if they match that means the arrays are same.\n\nB) Do “np.array_equal(e, f)” and if the output is “True” then they both are same\n\nC) Print flags of both arrays by e.flags and f.flags; check the flag “OWNDATA”. If one of them is False, then both the arrays have same space allocated.\n\nD) None of these\n\nSolution: (C)\n\nOption C is correct\n\nQuestion Context 9\n\nSuppose you want to join train and test dataset (both are two numpy arrays train_set and test_set) into a resulting array (resulting_set) to do data processing on it simultaneously. This is as follows:\n\n```train_set = np.array([1, 2, 3])\ntest_set = np.array([[0, 1, 2], [1, 2, 3]])\nresulting_set --> [[1, 2, 3], [0, 1, 2], [1, 2, 3]]```\n\n9) How would you join the two arrays?\n\nNote: Numpy library has been imported as np\n\nA) resulting_set = train_set.append(test_set)\n\nB) resulting_set = np.concatenate([train_set, test_set])\n\nC) resulting_set = np.vstack([train_set, test_set])\n\nD) None of these\n\nSolution: (C)\n\nBoth option A and B would do horizontal stacking, but we would like to have vertical stacking. So option C is correct\n\nQuestion Context 10\n\nSuppose you are tuning hyperparameters of a random forest classifier for the Iris dataset.\n\n Sepal_length Sepal_width Petal_length Petal_width Species 4.6 3.2 1.4 0.2 Iris-setosa 5.3 3.7 1.5 0.2 Iris-setosa 5.0 3.3 1.4 0.2 Iris-setosa 7.0 3.2 4.7 1.4 Iris-versicolor 6.4 3.2 4.5 1.5 Iris-versicolor\n\n10) What would be the best value for “random_state (Seed value)”?\n\nA) np.random.seed(1)\n\nB) np.random.seed(40)\n\nC) np.random.seed(32)\n\nD) Can’t say\n\nSolution: (D)\n\nThere is no best value for seed. It depends on the data.\n\nQuestion 11\n\nWhile reading a csv file with numpy, you want to automatically fill missing values of column “Date_Of_Joining” with date “01/01/2010”.\n\n Name Age Date_Of_Joining Total_Experience Andy 20 01/02/2013 0 Mandy 30 01/05/2014 10 Sandy 10 0 Bandy 40 01/10/2009 20\n\n11) Which command will be appropriate to fill missing value while reading the file with numpy?\n\nNote: numpy has been imported as np\n\nA) filling_values = (“-“, 0, 01/01/2010, 0)\ntemp = np.genfromtxt(filename, filling_values=filling_values)\n\nB) filling_values = (“-“, 0, 01/01/2010, 0)\n\nC) filling_values = (“-“, 0, 01/01/2010, 0)\ntemp = np.gentxt(filename, filling_values=filling_values)\n\nD) None of these\n\nSolution: (A)\n\nOption A is correct\n\n12) How would you import a decision tree classifier in sklearn?\n\nA) from sklearn.decision_tree import DecisionTreeClassifier\n\nB) from sklearn.ensemble import DecisionTreeClassifier\n\nC) from sklearn.tree import DecisionTreeClassifier\n\nD) None of these\n\nSolution: (C)\n\nOption C is correct\n\n13) You have uploaded the dataset in csv format on google spreadsheet and shared it publicly. You want to access it in python, how can you do this?\n\nNote: Library StringIO has been imported as StringIO.\n\n```A)\n```B)\n\n```\n\nC)\n\n```link = https://docs.google.com/spreadsheets/d/...source = StringIO(requests.get(link).content))\n\nD) None of these\n\nSolution: (A)\n\nOption A is correct\n\nQuestion Context 14\n\nImagine, you have a dataframe train file with 2 columns & 3 rows, which is loaded in pandas.\n\nimport pandas as pd\n\n`train = pd.DataFrame({'id':[1,2,4],'features':[[\"A\",\"B\",\"C\"],[\"A\",\"D\",\"E\"],[\"C\",\"D\",\"F\"]]})`\n\nNow you want to apply a lambda function on “features” column:\n\n`train['features_t'] = train[\"features\"].apply(lambda x: \" \".join([\"_\".join(i.split(\" \")) for i in x]))`\n\n14) What will be the output of following print command?\n\n`print train['features_t']`\n\nA)\n\n0 A B C\n1 A D E\n2 C D F\n\nB)\n\n0 AB\n\n2 CDF\n\nC) Error\nD) None of these\n\nSolution: (A)\n\nOption A is correct\n\nQuestion Context 15\n\nWe have a multi-class classification problem for predicting quality of wine on the basis of its attributes. The data is loaded in a dataframe “df”\n\n fixed acidity volatile acidity citric acid residual sugar chlorides free sulfur dioxide total sulfur dioxide density pH sulphates Alcohol quality 0 7.4 0.70 0.00 1.9 0.076 11 34 0.9978 3.51 0.56 9.4 5 1 7.8 0.88 0.00 2.6 0.098 25 67 0.9968 3.20 0.68 9.8 5 2 7.8 0.76 0.04 2.3 0.092 15 54 0.9970 3.26 0.65 9.8 5 3 11.2 0.28 0.56 1.9 0.075 17 60 0.9980 3.16 0.58 9.8 6 4 7.4 0.70 0.00 1.9 0.076 11 34 0.9978 3.51 0.56 9.4 5\n\nThe quality column currently has values 1 to 10, but we want to substitute this by a binary classification problem. You want to keep the threshold for classification to 5, such that if the class is greater than 5, the output should be 1, else output should be 0.\n\nNote: Numpy has been imported as np and dataframe is set as df.\n\nA)\n\n```Y = df[quality].values\nY = np.array([1 if y >= 6 else 0 for y in Y])```\n\nB)\n\n```Y = df[quality].values()\nY = np.array([0 if y >= 6 else 1 for y in Y])```\n\nC)\n\n```Y = df[quality]\nY = np.array([0 if y >= 6 else 1 for y in Y])```\n\nD)None of these\n\nSolution: (A)\n\nOption A is correct\n\nQuestion Context 16\n\nSuppose we make a dataframe as\n\n```df = pd.DataFrame(['ff', 'gg', 'hh', 'yy'],\n[24, 12, 48, 30],\ncolumns = ['Name', 'Age'])```\n\n16) What is the difference between the two data series given below?\n\n1. df[‘Name’] and\n2. df.loc[:, ‘Name’]\n\nNote: Pandas has been imported as pd\n\nA) 1 is view of original dataframe and 2 is a copy of original dataframe.\n\nB) 2 is view of original dataframe and 1 is a copy of original dataframe.\n\nC) Both are copies of original dataframe.\n\nD) Both are views of original dataframe\n\nSolution: (B)\n\nOption B is correct. Refer the official docs of pandas library.\n\nQuestion Context 17\n\nConsider a function “fun” which is defined below:\n\n```def fun(x):\nx = 5\nreturn x```\n\nNow you define a list which has three numbers in it.\n\ng = [10,11,12]\n\n17) Which of the following will be the output of the given print statement:\n\n`print fun(g), g`\n\nA) [5, 11, 12] [5, 11, 12]\n\nB) [5, 11, 12] [10, 11, 12]\n\nC) [10, 11, 12] [10, 11, 12]\n\nD) [10, 11, 12] [5, 11, 12]\n\nSolution: (A)\n\nOption A is correct\n\nQuestion Context 18\n\nSigmoid function is usually used for creating a neural network activation function. A sigmoid function is denoted as\n\n```def sigmoid(x):\nreturn (1 / (1 + math.exp(-x)))```\n\n18) It is necessary to know how to find the derivatives of sigmoid, as it would be essential for backpropagation. Select the option for finding derivative?\n\nA)\n\n```import scipy\n\nDv = scipy.misc.derive(sigmoid)```\n\nB)\n\n```from sympy import *\n\nx = symbol(x)\n\ny = sigmoid(x)\n\nDv = y.differentiate(x)```\n\nC)\n\n`Dv = sigmoid(x) * (1 - sigmoid(x))`\n\nD) None of these\n\nSolution: (C)\n\nOption C is correct\n\nQuestion Context 19\n\nSuppose you are given a monthly data and you have to convert it to daily data.\n\nFor example,",
null,
"For this, first you have to expand the data for every month (considering that every month has 30 days)\n\n19) Which of the following code would do this?\n\nNote: Numpy has been imported as np and dataframe is set as df.\n\nA) new_df = pd.concat([df]*30, index = False)\n\nB) new_df = pd.concat([df]*30, ignore_index=True)\n\nC) new_df = pd.concat([df]*30, ignore_index=False)\n\nD) None of these\n\nSolution: (B)\n\nOption B is correct\n\nContext: 20-22\n\nSuppose you are given a dataframe df.\n\n`df = pd.DataFrame({'Click_Id':['A','B','C','D','E'],'Count':[100,200,300,400,250]})`\n\n20) Now you want to change the name of the column ‘Count’ in df to ‘Click_Count’. So, for performing that action you have written the following code.\n\n`df.rename(columns = {'Count':'Click_Count'})`\n\nWhat will be the output of print statement below?\n\n`print df.columns`\n\nNote: Pandas library has been imported as pd.\n\nA) [‘Click_Id’, ‘Click_Count’]\n\nB) [‘Click_Id’, ‘Count’]\n\nC) Error\n\nD) None of these\n\nSolution: (B)\n\nOption B is correct\n\nContext: 20-22\n\nSuppose you are given a data frame df.\n\n`df = pd.DataFrame({'Click_Id':['A','B','C','D','E'],'Count':[100,200,300,400,250]})`\n\n21) In many data science projects, you are required to convert a dataframe into a dictionary. Suppose you want to convert “df” into a dictionary such that ‘Click_Id’ will be the key and ‘Count’ will be the value for each key. Which of the following options will give you the desired result?\n\nNote: Pandas library has been imported as pd\n\nA) set_index(‘Click_Id’)[‘Count’].to_dict()\n\nB) set_index(‘Count’)[‘Click_Id’].to_dict()\n\nC) We cannot perform this task since dataframe and dictionary are different data structures\n\nD) None of these\n\nSolution: (A)\n\nOption A is correct\n\n22) In above dataframe df. Suppose you want to assign a df to df1, so that you can recover original content of df in future using df1 as below.\n\n`df1 = df`\n\nNow you want to change some values of “Count” column in df.\n\n`df.loc[df.Click_Id == 'A', 'Count'] += 100`\n\nWhich of the following will be the right output for the below print statement?\n\n`print df.Count.values,df1.Count.values`\n\nNote: Pandas library has been imported as pd.\n\nA) [200 200 300 400 250] [200 200 300 400 250]\n\nB) [100 200 300 400 250] [100 200 300 400 250]\n\nC) [200 200 300 400 250] [100 200 300 400 250]\n\nD) None of these\n\nSolution: (A)\n\nOption A is correct\n\n23) You write a code for preprocessing data, and you notice it is taking a lot of time. To amend this, you put a bookmark in the code so that you come to know how much time is spent on each code line. To perform this task, which of the following actions you would take?\n\n1. You put bookmark as time.sleep() so that you would know how much the code has “slept” literally\n2. You put bookmark as time.time() and check how much time elapses in each code line\n3. You put bookmark as datetime.timedelta(), so that you would find out differences of execution times\n4. You copy whole code in an Ipython / Jupyter notebook, with each code line as a separate block and write magic function %%timeit in each block\n\nA) 1 & 2\n\nB) 1,2 & 3\n\nC) 1,2 & 4\n\nD) All of the above\n\nSolution: (C)\n\nOption C is correct\n\n24) How would you read data from the file using pandas by skipping the first three lines?\n\nNote: pandas library has been imported as pd In the given file (email.csv), the first three records are empty.\n\n```,,,\n\n,,,\n\n,,,\n\n[email protected],aa,Owner,2014\n\n[email protected],bb,Member,2015\n\n[email protected],cc,Member,2017\n\n[email protected],dd,Member,2016```\n\nD) None of these\n\nSolution: (B)\n\nOption B is correct\n\n25) What should be written in-place of “method” to produce the desired outcome?\n\nGiven below is dataframe “df”:",
null,
"Now, you want to know whether BMI and Gender would influence the sales.\n\nFor this, you want to plot a bar graph as shown below:",
null,
"The code for this is:\n\n```var = df.groupby(['BMI','Gender']).Sales.sum()\n\nvar.unstack().plot(kind='bar', method, color=['red','blue'], grid=False)```\n\nA) stacked=True\n\nB) stacked=False\n\nC) stack=False\n\nD) None of these\n\nSolution: (A)\n\nIt’s a stacked bar chart.\n\n26) Suppose, you are given 2 list – City_A and City_B.\n\nCity_A = [‘1′,’2′,’3′,’4’]\n\nCity_B = [‘2′,’3′,’4′,’5’]\n\nIn both cities, some values are common. Which of the following code will find the name of all cities which are present in “City_A” but not in “City_B”.\n\nA) [i for i in City_A if i not in City_B]\n\nB) [i for i in City_B if i not in City_A]\n\nC) [i for i in City_A if i in City_B]\n\nD) None of these\n\nSolution: (A)\n\nOption A is correct\n\nQuestion Context 27\n\nSuppose you are trying to read a file “temp.csv” using pandas and you get the following error.\n\n```Traceback (most recent call last):\nFile \"<input>\", line 1, in<module>\nUnicodeEncodeError: 'ascii' codec can't encode character.```\n\n27) Which of the following would likely correct this error?\n\nNote: pandas has been imported as pd\n\nD) None of these\n\nSolution: (C)\n\nOption C is correct, because encoding should be ‘utf-8’\n\n28) Suppose you are defining a tuple given below:\n\ntup = (1, 2, 3, 4, 5 )\n\nNow, you want to update the value of this tuple at 2nd index to 10. Which of the following option will you choose?\n\nA) tup(2) = 10\n\nB) tup = 10\n\nC) tup{2} = 10\n\nD) None of these\n\nSolution: (D)\n\nA tuple cannot be updated.\n\n29) You want to read a website which has url as “www.abcd.org”. Which of the following options will perform this task?\n\nA) urllib2.urlopen(www.abcd.org)\n\nB) requests.get(www.abcd.org)\n\nC) Both A and B\n\nD) None of these\n\nSolution: (C)\n\nOption C is correct\n\nQuestion Context 30\n\nSuppose you are given the below web page\n\n```html_doc = “””\n<!DOCTYPE html>\n<htmllang=\"en\">\n<metacharset=\"utf-8\">\n<metaname=\"viewport\" content=\"width=device-width\">\n<title>udacity/deep-learning: Repo for the Deep Learning Nanodegree Foundations program.</title>\n<metaproperty=\"fb:app_id\" content=\"1401488693436528\">\n...\n\n“””```\n\n30) To read the title of the webpage you are using BeautifulSoup. What is the code for this?\n\nHint: You have to extract text in title tag\n\n1. from bs4 import BeautifulSoup\nsoup =BeautifulSoup(html_doc,’html.parser’)\nprint soup.title.name\n2. from bs4 import BeautifulSoup\nsoup =BeautifulSoup(html_doc,’html.parser’)\nprint soup.title.string\n3. from bs4 import BeautifulSoup\nsoup=BeautifulSoup(html_doc,’html.parser’)\nprint soup.title.get_text\n4. None of these\n\nSolution: (B)\n\nOption B is correct\nQuestion Context 31\n\nImagine, you are given a list of items in a DataFrame as below.\n\nD = [‘A’,’B’,’C’,’D’,’E’,’AA’,’AB’]\n\nNow, you want to apply label encoding on this list for importing and transforming, using LabelEncoder.\n\n```from sklearn.preprocessing import LabelEncoder\n\nle = LabelEncoder()```\n\n31) What will be the output of the print statement below ?\n\n`print le.fit_transform(D)`\n1. array([0, 2, 3, 4, 5, 6, 1])\n2. array([0, 3, 4, 5, 6, 1, 2])\n3. array([0, 2, 3, 4, 5, 1, 6])\n4. Any of the above\n\nSolution: (D)\n\nOption D is correct\n\n32) Which of the following will be the output of the below print statement?\n\n`print df.val == np.nan`\n\nAssume, you have defined a data frame which has 2 columns.\n\n```import numpy as np\n\ndf = pd.DataFrame({'Id':[1,2,3,4],'val':[2,5,np.nan,6]})```\n\nA) 0 False\n1 False\n2 False\n3 False\n\nB) 0 False\n1 False\n2 True\n3 False\n\nC) 0 True\n1 True\n2 True\n3 True\n\nD) None of these\n\nSolution: (A)\n\nOption A is correct\n\n33) Suppose the data is stored in HDFS format and you want to find how the data is structured. For this, which of the following command would help you find out the names of HDFS keys?\n\nNote: HDFS file has been loaded by h5py as hf.\n\nA) hf.key()\n\nB) hf.key\n\nC) hf.keys()\n\nD) None of these\n\nSolution: (C)\n\nOption C is correct\n\nQuestion Context 34\n\nYou are given reviews for movies below:\n\nreviews = [‘movie is unwatchable no matter how decent the first half is . ‘, ‘somewhat funny and well paced action thriller that has jamie foxx as a hapless fast talking hoodlum who is chosen by an overly demanding’, ‘morse is okay as the agent who comes up with the ingenious plan to get whoever did it at all cost .’]\n\nYour task is to find sentiments from the review above. For this, you first write a code to find count of individual words in all the sentences.\n\n```counts = Counter()\n\nfor i in range(len(reviews)):\nfor word in reviews[i].split(value):\ncounts[word] += 1```\n\n34)What value should we split on to get individual words?\n\n1. ‘ ‘\n2. ‘,’\n3. ‘.’\n4. None of these\n\nSolution: (A)\n\nOption A is correct\n\n35) How to set a line width in the plot given below?",
null,
"For the above graph, the code for producing the plot was\n\n```import matplotlib.pyplot as plt\nplt.plot([1,2,3,4])\nplt.show()```\n1. In line two, write plt.plot([1,2,3,4], width=3)\n2. In line two, write plt.plot([1,2,3,4], line_width=3\n3. In line two, write plt.plot([1,2,3,4], lw=3)\n4. None of these\n\nSolution: (C)\n\nOption C is correct\n\n36) How would you reset the index of a dataframe to a given list? The new index is given as:\n\nnew_index=[‘Safari’,’Iceweasel’,’Comodo Dragon’,’IE10′,’Chrome’]\n\nNote: df is a pandas dataframe\n\n http_status response_time Firefox 200 0.04 Chrome 200 0.02 Safari 404 0.07 IE10 404 0.08 Konqueror 301 1.00\n\nA) df.reset_index(new_index,)\n\nB) df.reindex(new_index,)\n\nC) df.reindex_like(new_index,)\n\nD) None of these\n\nSolution: (A)\n\nOption A is correct\n\n37) Determine the proportion of passengers survived based on their passenger class.\n\n PassengerId Survived Pclass Name Sex Age SibSp Parch Ticket Fare Cabin Embarked 0 1 0 3 Braund, Mr. Owen Harris male 22.0 1 0 A/5 21171 7.2500 NaN S 1 2 1 1 Cumings, Mrs. John Bradley (Florence Briggs Th… female 38.0 1 0 PC 17599 71.2833 C85 C 2 3 1 3 Heikkinen, Miss. Laina female 26.0 0 0 STON/O2. 3101282 7.9250 NaN S 3 4 1 1 Futrelle, Mrs. Jacques Heath (Lily May Peel) female 35.0 1 0 113803 53.1000 C123 S 4 5 0 3 Allen, Mr. William Henry male 35.0 0 0 373450 8.0500 NaN S\n\n1. crosstab(df_train[‘Pclass’], df_train[‘Survived’])\n2. proportion(df_train[‘Pclass’], df_train[‘Survived’])\n3. crosstab(df_train[‘Survived’], df_train[‘Pclass’])\n4. None of these\n\nSolution: (A)\n\nOption A is correct\n\n38) You want to write a generic code to calculate n-gram of the text. The 2-gram of this sentence would be [[“this, “is”], [“is”, “a”], [“a, “sample”], [“sample”, “text”]]\n\nWhich of the following code would be correct?\n\nFor a given a sentence:\n‘this is a sample text’.\n\n1. def generate_ngrams(text, n):\nwords = text.split(‘\\n’)\noutput = [] for i in range(len(words)-n+1):\nappend(words[i+1:i+n])\nreturn output\n2. def generate_ngrams(text, n):\nwords = text.split()\noutput = [] for i in range(len(words)-n+1):\nappend(words[i:i+n])\nreturn output\n3. def generate_ngrams(text, n):\nwords = text.split()\noutput = [] for i in range(len(words)-n+1):\nappend(words[i+1:i+n])\nreturn output\n4. None of these\n\nSolution: (B)\n\nOption B is correct\n\n39) Which of the following code will export dataframe (df) in CSV file, encoded in UTF-8 after hiding index & header labels.\n\n4. None of these\n\nSolution: (C)\n\nOption C is correct\n\n40) Which of the following is a correct implementation of mean squared error (MSE) metric?\n\nNote: numpy library has been imported as np.\n\n1. def MSE(real_target, predicted_target):\nreturn np.mean((np.square(real_target) – np.square(predicted_target)))\n2. def MSE(real_target, predicted_target):\nreturn np.mean((real_target – predicted_target)**2)\n3. def MSE(real_target, predicted_target):\nreturn np.sqrt(np.mean((np.square(real_target) – np.square(predicted_target))))\n4. None of the above\n\nSolution: (B)\n\nOption B is correct\n\n### End Notes\n\nIf you are learning Python, make sure you go through the test above. It will not only help you assess your skill. You can also see where you stand among other people in the community. If you have any questions or doubts, feel free to post them below.\n\n### Learn, compete, hack and get hired!",
null,
"###### Faizan Shaikh\n\nFaizan is a Data Science enthusiast and a Deep learning rookie. A recent Comp. Sc. undergrad, he aims to utilize his skills to push the boundaries of AI research.\n\n## 4 thoughts on \"40 Questions to test your skill in Python for Data Science\"",
null,
"###### Lia says:May 07, 2017 at 10:39 am\nFor Question Context 7: np.identity(3), which is option (B) does exist: https://docs.scipy.org/doc/numpy/reference/generated/numpy.identity.html But option (A) seems to be incorrect as we've got to write np.eye(3), don't we? Reply",
null,
"###### Faizan Shaikh says:May 08, 2017 at 5:14 am\nThank you for letting us know the typo. Actually option B does not exist because it should have been np.identity(), whereas it should have been np.eye() in option A. Reply",
null,
"###### issac says:June 06, 2017 at 10:48 am\nFor Question Context 16: I found there is instruction in python documnet about this issue http://pandas.pydata.org/pandas-docs/stable/indexing.html#returning-a-view-versus-a-copy and I think it's a little different from your answer. Could you explain why option B is corret ? Thanks Reply",
null,
"###### Faizan Shaikh says:July 08, 2017 at 6:21 pm\nThanks for the feedback. I have updated the same Reply"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.78266305,"math_prob":0.86941147,"size":25783,"snap":"2021-43-2021-49","text_gpt3_token_len":7711,"char_repetition_ratio":0.12665348,"word_repetition_ratio":0.118395776,"special_character_ratio":0.3270372,"punctuation_ratio":0.17626588,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9855077,"pos_list":[0,1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22],"im_url_duplicate_count":[null,4,null,10,null,4,null,4,null,4,null,4,null,null,null,null,null,null,null,null,null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-10-26T21:52:02Z\",\"WARC-Record-ID\":\"<urn:uuid:8cdb2dee-4c2c-47f0-871a-dbab03722b04>\",\"Content-Length\":\"156155\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:7eb43d2d-d282-4433-88b3-8f057c780c55>\",\"WARC-Concurrent-To\":\"<urn:uuid:3e2d75c7-e7cd-4447-92c4-d67857e7ec2f>\",\"WARC-IP-Address\":\"104.22.54.101\",\"WARC-Target-URI\":\"https://www.analyticsvidhya.com/blog/2017/05/questions-python-for-data-science/\",\"WARC-Payload-Digest\":\"sha1:Z7IXCQFF2CHQFR4XFVP73MVEUYDAJOJD\",\"WARC-Block-Digest\":\"sha1:DA3VDSHZTJD2VQ5WHON4UKFI4XSO2LXM\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-43/CC-MAIN-2021-43_segments_1634323587926.9_warc_CC-MAIN-20211026200738-20211026230738-00663.warc.gz\"}"} |
https://www.fossilhunters.xyz/thermodynamics/info-fza.html | [
"## Info\n\nFor T > 423 K: use ideal-gas law for v h = 2783 + 1.62 x (T-423) + 3.33 x KM CP -4231) s = 8.69 + 1.62 x bi(T/423) + 6.65 x 104 (T-423)\n\nFor T > 573 K: use ideal gas law for v h = 3065 + 1.71 x (T - 573) + 2.94 x 10\" CP - 573») s = 7.71 + 1.71 x 111(7/573) + 5.87 x IQ-« (T-S13)\n\nFor T > 423 K: use ideal-gas law for v h = 2783 + 1.62 x (T-423) + 3.33 x KM CP -4231) s = 8.69 + 1.62 x bi(T/423) + 6.65 x 104 (T-423)\n\nFor T > 573 K: use ideal gas law for v h = 3065 + 1.71 x (T - 573) + 2.94 x 10\" CP - 573») s = 7.71 + 1.71 x 111(7/573) + 5.87 x IQ-« (T-S13)\n\nT, K\n\nv, m3/kg\n\nh, kj/kg\n\ns, kJ/kg-K\n\nT, K\n\nv, m3/kg\n\nh, kj/kg\n\ns, kJ/kg-K",
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"https://www.fossilhunters.xyz/images/downloads/eJw9yksKgCAQANDbuPQHagTSUWJSyaF0pAyvH23avNXLvbdZiIEHjrRJ6XghIh6oiEijngRxLVBhT5e4U4285bZA6EjVNwz9uRL7I0ZvrLITBKeM0Zplr41k4_MF7K0j-w.jpg",
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https://math.stackexchange.com/questions/3192319/what-is-the-characteristic-of-a-local-ring/3192449 | [
"What is the Characteristic of a local ring? [closed]\n\nWhat is the Characteristic of a local ring ?\n\nWe define Characteristic of a Commutative ring with $$1$$ say, $$A$$ in the following way: Define a ring homomorphism $$\\phi: \\mathbb{Z} \\to A$$ by $$\\phi(n)=n \\cdot 1.$$ Since $$\\mathbb{Z}$$ is a PID, $$\\text{ker}(\\phi)$$ is a principal ideal. If $$\\text{ker}(\\phi)=m\\mathbb{Z},$$ we define the Characteristic of the ring $$A$$ to be $$m.$$ We know that Characteristic of a domain is either $$0$$ or a prime $$p.$$\n\nHow do I classify the Characteristic of a local ring $$(A,m)$$\n\nclosed as unclear what you're asking by Arnaud D., max_zorn, Javi, José Carlos Santos, RamiroApr 19 at 16:25\n\nPlease clarify your specific problem or add additional details to highlight exactly what you need. As it's currently written, it’s hard to tell exactly what you're asking. See the How to Ask page for help clarifying this question. If this question can be reworded to fit the rules in the help center, please edit the question.\n\n• The characteristic of a ring need not be prime: for instance, the characteristic of $\\mathbb Z/(6)$ is $6$. It only needs to be a prime if the ring is an integral domain. – Claudius Apr 18 at 12:23\n• I don't really understand the question. You have the definition of the characteristic of a ring, so theoretically you now how to find it, right? – Arnaud D. Apr 18 at 12:28\n• It is not clear to me what you mean by “find the characteristic“. Are you asking about the definition of the characteristic of a local ring? – Claudius Apr 18 at 12:29\n• Like integral domain you can classify the characteristic of a local ring. – user371231 Apr 18 at 12:45\n• I much as I guess $6$ cannot be characteristic of a local ring – user371231 Apr 18 at 12:49\n\nThe characteristic of a local ring is a power of a prime or $$0$$, and any of these happens in some local rings.\n\nThat they all happen is easy : you may look at fields for characteristic $$0$$, and $$\\mathbb{Z}/p^n\\mathbb{Z}$$ for powers of primes.\n\nNow let $$(R,m)$$ be a local ring, and $$n$$ its characteristic, which we assume to be $$>0$$. Suppose $$n=ab, a\\land b = 1$$. Then the ideals $$I=\\{x\\in R, ax = 0\\}$$ and $$J=\\{x\\in R, bx=0\\}$$ are comaximal : indeed $$a\\in J, b\\in I$$ and there are $$u,v$$ with $$au+bv=1$$ so $$1\\in I+J$$.\n\nTherefore by locality, one of them is $$R$$ (otherwise they would both be $$\\subset m$$). If it is $$I$$, then $$a = 0$$ in $$R$$ and so $$R$$ has characteristic $$\\mid a$$ so $$b=1$$. If it's $$J$$, then $$a=1$$. In any case, $$a=1 \\lor b=1$$, so that $$n$$ is a power of a prime.\n\nIf you already know a local ring has only trivial idempotents, then you can reason this way:\n\nSuppose the characteristic of a ring $$R$$ is finite, say $$n$$, and is divisible by more than one prime. The ring contains a copy of $$\\mathbb Z/n\\mathbb Z$$. So to show $$R$$ isn't local, it suffices to show that $$\\mathbb Z/n\\mathbb Z$$ contains a nontrivial idempotent, so that $$R$$ will also contain a nontrivial idempotent.\n\nBy reasoning with the Chinese remainder theorem, you can quickly see that $$\\mathbb Z/n\\mathbb Z$$ is isomorphic to $$\\mathbb Z/p^k\\mathbb Z$$ for primes $$p$$ dividing $$n$$ and powers $$k$$ depending on $$p$$. Since there is more than one prime dividing $$n$$ (our assumption) there is at least one nontrivial idempotent splitting $$\\mathbb Z/n\\mathbb Z$$ into two pieces. This is clearly a nontrivial idempotent of $$R$$ too.\n\nSo by contrapositive, we have shown that a local ring $$R$$ must have either characteristic $$0$$, or else it has finite characteristic that is a power of a prime.\n\nSince we already have examples of such rings for every such finite characteristic, we can see these are precisely the characteristics that are possible."
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.73721415,"math_prob":0.9998975,"size":499,"snap":"2019-26-2019-30","text_gpt3_token_len":156,"char_repetition_ratio":0.18181819,"word_repetition_ratio":0.05,"special_character_ratio":0.3046092,"punctuation_ratio":0.10377359,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":1.0000027,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-06-17T19:21:28Z\",\"WARC-Record-ID\":\"<urn:uuid:60b0fa4e-8592-4c20-929f-ed7970222ac4>\",\"Content-Length\":\"133671\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:a74ef8f2-b99e-49be-802d-cd62079b87b1>\",\"WARC-Concurrent-To\":\"<urn:uuid:913fb40a-a8e1-41f8-97f7-66db343e057f>\",\"WARC-IP-Address\":\"151.101.65.69\",\"WARC-Target-URI\":\"https://math.stackexchange.com/questions/3192319/what-is-the-characteristic-of-a-local-ring/3192449\",\"WARC-Payload-Digest\":\"sha1:RQPP7RQDNDMIZB2XA2X7BSGBS27EY3TS\",\"WARC-Block-Digest\":\"sha1:WAPBJHNDIOMN2FL5WHYKJU2XXTTWQPOZ\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-26/CC-MAIN-2019-26_segments_1560627998558.51_warc_CC-MAIN-20190617183209-20190617205209-00447.warc.gz\"}"} |
https://www.lmfdb.org/EllipticCurve/Q/28611/g/4 | [
"Show commands for: Magma / SageMath / Pari/GP\n\n## Minimal Weierstrass equation\n\nmagma: E := EllipticCurve([1, -1, 1, 113089, -4911334]); // or\n\nmagma: E := EllipticCurve(\"28611u3\");\n\nsage: E = EllipticCurve([1, -1, 1, 113089, -4911334]) # or\n\nsage: E = EllipticCurve(\"28611u3\")\n\ngp: E = ellinit([1, -1, 1, 113089, -4911334]) \\\\ or\n\ngp: E = ellinit(\"28611u3\")\n\n$$y^2 + x y + y = x^{3} - x^{2} + 113089 x - 4911334$$\n\n## Mordell-Weil group structure\n\n$$\\Z\\times \\Z/{2}\\Z$$\n\n### Infinite order Mordell-Weil generator and height\n\nmagma: Generators(E);\n\nsage: E.gens()\n\n $$P$$ = $$\\left(\\frac{1327}{4}, \\frac{65139}{8}\\right)$$ $$\\hat{h}(P)$$ ≈ 4.87435501435\n\n## Torsion generators\n\nmagma: TorsionSubgroup(E);\n\nsage: E.torsion_subgroup().gens()\n\ngp: elltors(E)\n\n$$\\left(\\frac{171}{4}, -\\frac{175}{8}\\right)$$\n\n## Integral points\n\nmagma: IntegralPoints(E);\n\nsage: E.integral_points()\n\nNone\n\n## Invariants\n\n magma: Conductor(E); sage: E.conductor().factor() gp: ellglobalred(E) Conductor: $$28611$$ = $$3^{2} \\cdot 11 \\cdot 17^{2}$$ magma: Discriminant(E); sage: E.discriminant().factor() gp: E.disc Discriminant: $$-102865276637763651$$ = $$-1 \\cdot 3^{18} \\cdot 11 \\cdot 17^{6}$$ magma: jInvariant(E); sage: E.j_invariant().factor() gp: E.j j-invariant: $$\\frac{9090072503}{5845851}$$ = $$3^{-12} \\cdot 11^{-1} \\cdot 2087^{3}$$ Endomorphism ring: $$\\Z$$ (no Complex Multiplication) Sato-Tate Group: $\\mathrm{SU}(2)$\n\n## BSD invariants\n\n magma: Rank(E); sage: E.rank() Rank: $$1$$ magma: Regulator(E); sage: E.regulator() Regulator: $$4.87435501435$$ magma: RealPeriod(E); sage: E.period_lattice().omega() gp: E.omega Real period: $$0.192162771421$$ magma: TamagawaNumbers(E); sage: E.tamagawa_numbers() gp: gr=ellglobalred(E); [[gr[i,1],gr[i]] | i<-[1..#gr[,1]]] Tamagawa product: $$8$$ = $$2^{2}\\cdot1\\cdot2$$ magma: Order(TorsionSubgroup(E)); sage: E.torsion_order() gp: elltors(E) Torsion order: $$2$$ magma: MordellWeilShaInformation(E); sage: E.sha().an_numerical() Analytic order of Ш: $$1$$ (exact)\n\n## Modular invariants\n\n#### Modular form 28611.2.a.g\n\nmagma: ModularForm(E);\n\nsage: E.q_eigenform(20)\n\ngp: xy = elltaniyama(E);\n\ngp: x*deriv(xy)/(2*xy+E.a1*xy+E.a3)\n\n$$q - q^{2} - q^{4} - 2q^{5} - 4q^{7} + 3q^{8} + 2q^{10} + q^{11} - 2q^{13} + 4q^{14} - q^{16} + O(q^{20})$$\n\n magma: ModularDegree(E); sage: E.modular_degree() Modular degree: 245760 $$\\Gamma_0(N)$$-optimal: no Manin constant: 1\n\n#### Special L-value\n\nmagma: Lr1 where r,Lr1 := AnalyticRank(E: Precision:=12);\n\nsage: r = E.rank();\n\nsage: E.lseries().dokchitser().derivative(1,r)/r.factorial()\n\ngp: ar = ellanalyticrank(E);\n\ngp: ar/factorial(ar)\n\n$$L'(E,1)$$ ≈ $$1.87333913689$$\n\n## Local data\n\nThis elliptic curve is not semistable.\n\nmagma: [LocalInformation(E,p) : p in BadPrimes(E)];\n\nsage: E.local_data()\n\ngp: ellglobalred(E)\n\nprime Tamagawa number Kodaira symbol Reduction type Root number ord($$N$$) ord($$\\Delta$$) ord$$(j)_{-}$$\n$$3$$ $$4$$ $$I_12^{*}$$ Additive -1 2 18 12\n$$11$$ $$1$$ $$I_{1}$$ Split multiplicative -1 1 1 1\n$$17$$ $$2$$ $$I_0^{*}$$ Additive 1 2 6 0\n\n## Galois representations\n\nThe image of the 2-adic representation attached to this elliptic curve is the subgroup of $\\GL(2,\\Z_2)$ with Rouse label X13.\n\nThis subgroup is the pull-back of the subgroup of $\\GL(2,\\Z_2/2^2\\Z_2)$ generated by $\\left(\\begin{array}{rr} 3 & 0 \\\\ 0 & 1 \\end{array}\\right),\\left(\\begin{array}{rr} 1 & 1 \\\\ 0 & 1 \\end{array}\\right),\\left(\\begin{array}{rr} 3 & 0 \\\\ 0 & 3 \\end{array}\\right)$ and has index 6.\n\nmagma: [GaloisRepresentation(E,p): p in PrimesUpTo(20)];\n\nsage: rho = E.galois_representation();\n\nsage: [rho.image_type(p) for p in rho.non_surjective()]\n\nThe mod $$p$$ Galois representation has maximal image $$\\GL(2,\\F_p)$$ for all primes $$p$$ except those listed.\n\nprime Image of Galois representation\n$$2$$ B\n\n## $p$-adic data\n\n### $p$-adic regulators\n\nsage: [E.padic_regulator(p) for p in primes(3,20) if E.conductor().valuation(p)<2]\n\n$$p$$-adic regulators are not yet computed for curves that are not $$\\Gamma_0$$-optimal.\n\n## Iwasawa invariants\n\n $p$ Reduction type $\\lambda$-invariant(s) $\\mu$-invariant(s) 2 3 5 7 11 13 17 19 23 29 31 37 41 43 47 ordinary add ordinary ordinary split ordinary add ss ordinary ordinary ordinary ordinary ordinary ss ordinary 11 - 1 1 2 1 - 1,1 1 1 1 1 1 1,1 1 2 - 0 0 0 0 - 0,0 0 0 0 0 0 0,0 0\n\nAn entry - indicates that the invariants are not computed because the reduction is additive.\n\n## Isogenies\n\nThis curve has non-trivial cyclic isogenies of degree $$d$$ for $$d=$$ 2 and 4.\nIts isogeny class 28611.g consists of 4 curves linked by isogenies of degrees dividing 4.\n\n## Growth of torsion in number fields\n\nThe number fields $K$ of degree up to 7 such that $E(K)_{\\rm tors}$ is strictly larger than $E(\\Q)_{\\rm tors}$ $\\cong \\Z/{2}\\Z$ are as follows:\n\n$[K:\\Q]$ $K$ $E(K)_{\\rm tors}$ Base-change curve\n2 $$\\Q(\\sqrt{51})$$ $$\\Z/4\\Z$$ Not in database\n$$\\Q(\\sqrt{-561})$$ $$\\Z/4\\Z$$ Not in database\n$$\\Q(\\sqrt{-11})$$ $$\\Z/2\\Z \\times \\Z/2\\Z$$ Not in database\n4 $$\\Q(\\sqrt{-11}, \\sqrt{51})$$ $$\\Z/2\\Z \\times \\Z/4\\Z$$ Not in database\n\nWe only show fields where the torsion growth is primitive. For each field $K$ we either show its label, or a defining polynomial when $K$ is not in the database."
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https://occupychristmas.org/multiply-or-divide-two-quantities-by-the-same-number/ | [
"Ratios and also Proportions tantamount Ratios Proportion fixing Ratio and also ProportionRatios and also Proportions\n\nRatios are supplied to to compare quantities. Ratios aid us come compare quantities and also determine the relation between them. A proportion is a comparison of two similar quantities derived by splitting one quantity by the other. Due to the fact that a proportion is only a compare or relation between quantities, it is one abstract number. For instance, the proportion of 6 miles to 3 miles is just 2, not 2 miles. Ratios space written v the” : “symbol.\n\nYou are watching: Multiply or divide two quantities by the same number\n\nIf two amounts cannot it is in expressed in terms of the same unit, there cannot it is in a ratio in between them. Thus to compare two quantities, the units should be the same.\n\nConsider an example to discover the proportion of 3 kilometres to 300 m.First convert both the ranges to the exact same unit.\n\nSo, 3 km = 3 × 1000 m = 3000 m.\n\nThus, the required ratio, 3 km : 300 m is 3000 : 300 = 10 : 1\n\nEquivalent Ratios\n\nDifferent ratios can additionally be contrasted with each various other to know whether they are equivalent or not. To do this, we have to write the ratios in the form of fractions and then to compare them by converting them to choose fractions. If these choose fractions space equal, we say the given ratios are equivalent. Us can uncover equivalent ratios by multiplying or dividing the numerator and denominator by the exact same number. Consider an example to examine whether the ratios 1 : 2 and 2 : 3 equivalent.\n\nTo inspect this, we require to recognize whether",
null,
"We have,",
null,
"We uncover that",
null,
"which means that",
null,
"Therefore, the ratio 1 :2 is not indistinguishable to the ratio 2 : 3.\n\nProportion\n\nThe ratio of two quantities in the exact same unit is a fraction that mirrors how numerous times one quantity is better or smaller sized than the other. Four quantities are claimed to be in proportion, if the proportion of very first and second quantities is same to the ratio of third and fourth quantities. If 2 ratios room equal, then we say the they room in proportion and use the price ‘:: ’ or ‘=’ to equate the 2 ratios.\n\nSolving Ratio and also Proportion\n\nRatio and proportion troubles can be fixed by using two methods, the unitary method and also equating the ratios to make proportions, and then fixing the equation.\n\nFor example,\n\nTo examine whether 8, 22, 12, and 33 room in proportion or not, we have to find the ratio of 8 come 22 and also the proportion of 12 come 33.",
null,
"Therefore, 8, 22, 12, and 33 are in ratio as 8 : 22 and 12 : 33 room equal. When four terms room in proportion, the first and 4th terms are well-known as extreme terms and also the second and 3rd terms are recognized as middle terms. In the above example, 8, 22, 12, and also 33 were in proportion. Therefore, 8 and also 33 are known as too much terms while 22 and 12 are known as center terms.\n\nThe method in which we an initial find the value of one unit and then the value of the required variety of units is recognized as unitary method.\n\nConsider an instance to find the cost of 9 bananas if the expense of a dozen bananas is Rs 20.\n\n1 dozen = 12 units\n\nCost that 12 bananas = Rs 20\n\n∴ expense of 1 bananas = Rs",
null,
"∴ price of 9 bananas = Rs",
null,
"This technique is known as unitary method.\n\nSee more: Driving Directions To 150 Windermere Rd Winter Garden, Fl 34787, Usa\n\nSummary We have actually learnt, Ratios are provided to to compare quantities. Because a ratio is only a compare or relation in between quantities, that is an summary number. Ratios can be created as fractions. They also have every the nature of fractions. The proportion of 6 to 3 have to be proclaimed as 2 come 1, yet common usage has shortened the expression that ratios to be called simply 2. If two amounts cannot it is in expressed in terms of the same unit, over there cannot be a ratio between them. If any kind of three state in a proportion are given, the fourth may it is in found. The product that the way is same to the product of the extremes. It is vital to remember the to use the proportion; the ratios need to be same to each other and also must remain constant.\n\nCite this Simulator:\n\noccupychristmas.org,. (2013). Ratios and Proportions. Recall 18 September 2021, from occupychristmas.org/?sub=100&brch=300&sim=1556&cnt=3676"
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"https://occupychristmas.org/multiply-or-divide-two-quantities-by-the-same-number/\\\"https:/occupychristmas.org/multiply-or-divide-two-quantities-by-the-same-number/imager_4_3664_700.jpg\\\"",
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https://ask.sagemath.org/questions/10388/revisions/ | [
"# Revision history [back]\n\n### Testing inequalities in sage\n\nI wanted to show if: $$|a+b| \\leq |a| + |b|$$\n\nSo I wrote this in sage:\n\nvar('a','b')\neqn1=abs(a+b)\neqn2=abs(a)+abs(b)\nbool(eqn1<=eqn2)\n\n\nThe result is False.\n\nI had expected the result to be True. What is the correct way to test this in sage?\n\nThank you in advance for any help provided.",
null,
"2 retagged\n\n### Testing inequalities in sage\n\nI wanted to show if: $$|a+b| \\leq |a| + |b|$$\n\nSo I wrote this in sage:\n\nvar('a','b')\neqn1=abs(a+b)\neqn2=abs(a)+abs(b)\nbool(eqn1<=eqn2)\n\n\nThe result is False.\n\nI had expected the result to be True. What is the correct way to test this in sage?\n\nThank you in advance for any help provided.",
null,
"3 retagged\n\n### Testing inequalities in sage\n\nI wanted to show if: $$|a+b| \\leq |a| + |b|$$\n\nSo I wrote this in sage:\n\nvar('a','b')\neqn1=abs(a+b)\neqn2=abs(a)+abs(b)\nbool(eqn1<=eqn2)\n\n\nThe result is False.\n\nI had expected the result to be True. What is the correct way to test this in sage?\n\nThank you in advance for any help provided.",
null,
"4 retagged\n\n### Testing inequalities in sage\n\nI wanted to show if: $$|a+b| \\leq |a| + |b|$$\n\nSo I wrote this in sage:\n\nvar('a','b')\neqn1=abs(a+b)\neqn2=abs(a)+abs(b)\nbool(eqn1<=eqn2)\n\n\nThe result is False.\n\nI had expected the result to be True. What is the correct way to test this in sage?\n\nThank you in advance for any help provided."
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.9188352,"math_prob":0.7497649,"size":283,"snap":"2023-14-2023-23","text_gpt3_token_len":97,"char_repetition_ratio":0.11469534,"word_repetition_ratio":0.0,"special_character_ratio":0.33215547,"punctuation_ratio":0.10294118,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99849623,"pos_list":[0,1,2,3,4,5,6],"im_url_duplicate_count":[null,null,null,null,null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-03-21T00:43:55Z\",\"WARC-Record-ID\":\"<urn:uuid:b4238d28-7d4a-47a9-80f3-074fe25de419>\",\"Content-Length\":\"22193\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:19a6b0b2-fd92-421a-813c-593d124adabc>\",\"WARC-Concurrent-To\":\"<urn:uuid:687fb13a-72b0-4031-bcca-01971da786eb>\",\"WARC-IP-Address\":\"194.254.163.53\",\"WARC-Target-URI\":\"https://ask.sagemath.org/questions/10388/revisions/\",\"WARC-Payload-Digest\":\"sha1:UIQRVBJNMYPZCAHIKY2UO6DTSFVUEGCK\",\"WARC-Block-Digest\":\"sha1:BLEOAMXNSARIAL3OOX67BPMRJ2NNC6H3\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-14/CC-MAIN-2023-14_segments_1679296943589.10_warc_CC-MAIN-20230321002050-20230321032050-00532.warc.gz\"}"} |
http://bristolcrypto.blogspot.com/2013/03/study-group-new-approach-to-practical.html | [
"## Thursday, March 7, 2013\n\n### Study Group: A New Approach to Practical Active-Secure Two-Party Computation\n\nThis week's study group, given by Nigel, concerned the paper A New Approach to Practical Active-Secure Two-Party Computation (CRYPTO 2012) by J.B. Nielsen et al. In this paper the authors propose a 2-party UC protocol computational secure against a semi-honest adversary in the random oracle model, in which two parties, Alice and Bob, with some private input bits x and y, respectively, jointly compute a boolean function f(x,y). The main motivation for the paper is to give a PRACTICAL efficient 2-party protocol with the standard requirements of 1) Correctness (the output of the computation is correct) and 2) Privacy (the output is kept secret). To this purpose they use a new approach based on Oblivious Transfer (OT), actually getting efficiency from a highly inefficient tool. In particular they introduce a new way of extending OTs: from a small number of seed OTs they can derive, in an actively secure way, a large number of committed OT-like primitives.\n\nTheir approach is based on the passive-secure 2-party protocol of [GMW87], that extensively uses OT. The input bits x and y are secret shared in such a way that Alice holds xA, yA and Bob holds xB, yB, with x=xA xB, y = yAyB. Then the boolean circuit computing the function f(x,y) is evaluated gate-by gate. Suppose the parties want to compute an AND gate: they need to calculate a random sharing zA, zB of z= xy = xAyA ⊕ xA yB ⊕ xB yA ⊕ xB yB. So they locally compute tA=xAyAand tB=xByB, and then, using OT, they compute the cross products u=xAyB and v=xByA such that xy=tuv. To achieve active security the authors add information theoretic Message Authentication Code (MAC) to all the shares. The first step is the oblivious authentication of bits (aBit): A party (for example Bob) holds a global key Δ A ∈ {0,1}k , where k is the security parameter, and, for each of the Alice's bit x, a local key Kx ∈ {0,1}k . Alice inputs x in a OT and she receives the MAC Mx= Kxx Δ A. Notice that if y is another message and My=Kyy Δ A its corresponding MAC, then Alice can locally compute MxMy=(Kx Ky)⊕(x⊕y) Δ A. It is important to note that Bob has to use the same global key Δ A for each of the OT. To ensure this a cut-and-choose-like technique is proposed in which one authenticates twice as many bits as he needs and then he sacrifices half of them checking that they were done with the same global key. Using aBit, the authors describe Authenticated AND (aAnd) and Authenticated OT (aOT). If Alice holds authenticated random bits a,b,c, aAnd allows to compute c=ab and obtain an authentication of this result; aOT permits to perform OT of previously authenticated bits and produce an authentication on the result.\n\nSumming up the authors describe a secure 2-party protocol for boolean function in the preprocessing model. During the preprocessing phase they prepare random authenticated messages, random authenticated multiplication triples and random authenticated OTs, using aBit, aAnd and aOT. In particular aAnd is used to get a MAC on tA=aAbA and tB=aBbB and aOT to secure compute u=aAbB and v=aBbA (u,v are the cross products in c=ab=aAbA ⊕ aA bB ⊕ aB bA ⊕ aB bB), that will be used in the AND gates during the online phase, where the preprocessed data is used to actually evaluate the circuit. The efficiency is guaranteed by the OT-extension technique, that from a small number of long MACs on Bob 's random bits permits to derive many, short MACs on Alice's random bits. Intuitively the OT-extension works as follows:\n\n1) Long MAC for Bob: this first step consists in generating a few aBit using very long keys. Bob inputs some random bits yj, j=1, ..., h, in a OT and receives\nNj=Lj⊕ yjΓB\nfor j=1, ..., h and Nj, Lj, ΓB∈ {0,1}n, with h small (around 128) and n very big. This step is also called LaBit (Leacking Bits) as the key holder (Alice in this case) can learn a few of Bob's bits yj.\n\n2) Short MAC for Alice. This step consists in generating a lot of aBit with short keys:\n• Rewrite the MACs created in 1) in matrix form Nij=Lij⊕ yjΓBi , i=1,...,n and j=1,...,h:\n[ N1 | . . . | Nh ] = [ L1 | . . . | Lh ] ⊕ [ y1ΓB1 | . . . | yhΓBh].\n• Swap the position of the MACs and the keys:\n[ L1 | . . . | Lh ] = [ N1 | . . . | Nh ] ⊕ [ y1ΓB1 | . . . | yhΓBh].\n• Flip the values of columns and rows:\n[ L1j . . . Lnj ] = [ N1j . . . Nnj ] ⊕ [ yjB1 . . . ΓBn) ], j=1, . . ., h.\n• Rename Mij = Lji, Kij = Nji, xi ΓBi and ΓAj = yj, from which we get the n MACs\nMi=KixiΓA,\ni=1, ..., n and Mi, Ki, ΓA∈ {0,1}k.\nThis step is called WaBit (Weak Bits) as a few bit of the global key ΓA may leak to the MAC holder.\n\n3) Fix the problems obtaining a fully secure global key Δ A.\n\nUsing these ideas the authors obtain the first practical 2-party computation protocol based on OT at a rate of about 20000 gates for seconds."
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.8720813,"math_prob":0.94089293,"size":4820,"snap":"2023-14-2023-23","text_gpt3_token_len":1377,"char_repetition_ratio":0.113164455,"word_repetition_ratio":0.041666668,"special_character_ratio":0.26846474,"punctuation_ratio":0.15157293,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.97722113,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-06-01T03:16:09Z\",\"WARC-Record-ID\":\"<urn:uuid:54a7456f-ab6a-4581-a23d-2ca973a5df47>\",\"Content-Length\":\"96862\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:0b260033-2c3a-4242-8de5-5fbb828df6f0>\",\"WARC-Concurrent-To\":\"<urn:uuid:5d6abf4f-4e8c-4a4d-8c06-1baba1a97fb4>\",\"WARC-IP-Address\":\"172.253.122.132\",\"WARC-Target-URI\":\"http://bristolcrypto.blogspot.com/2013/03/study-group-new-approach-to-practical.html\",\"WARC-Payload-Digest\":\"sha1:PZ6SL6DXCJUVP5CORFFYMJIHRZUTKJVA\",\"WARC-Block-Digest\":\"sha1:HCZZCWNRAC5KOT66YR5QKZMVGBMKBQAK\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-23/CC-MAIN-2023-23_segments_1685224647525.11_warc_CC-MAIN-20230601010402-20230601040402-00574.warc.gz\"}"} |
https://www.jpost.com/breaking-news/article-750194 | [
"(function (a, d, o, r, i, c, u, p, w, m) { m = d.getElementsByTagName(o), a[c] = a[c] || {}, a[c].trigger = a[c].trigger || function () { (a[c].trigger.arg = a[c].trigger.arg || []).push(arguments)}, a[c].on = a[c].on || function () {(a[c].on.arg = a[c].on.arg || []).push(arguments)}, a[c].off = a[c].off || function () {(a[c].off.arg = a[c].off.arg || []).push(arguments) }, w = d.createElement(o), w.id = i, w.src = r, w.async = 1, w.setAttribute(p, u), m.parentNode.insertBefore(w, m), w = null} )(window, document, \"script\", \"https://95662602.adoric-om.com/adoric.js\", \"Adoric_Script\", \"adoric\",\"9cc40a7455aa779b8031bd738f77ccf1\", \"data-key\");\nvar domain=window.location.hostname; var params_totm = \"\"; (new URLSearchParams(window.location.search)).forEach(function(value, key) {if (key.startsWith('totm')) { params_totm = params_totm +\"&\"+key.replace('totm','')+\"=\"+value}}); var rand=Math.floor(10*Math.random()); var script=document.createElement(\"script\"); script.src=`https://stag-core.tfla.xyz/pre_onetag?pub_id=34&domain=\\${domain}&rand=\\${rand}&min_ugl=0\\${params_totm}`; document.head.append(script);"
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https://www.weegy.com/?ConversationId=1B69A694 | [
"how to multiply easily\nHere follows a short tutorial with simple calculations: 1. When calculating one bind numbers like in 8,9=89. 2. When adding and subtracting one go from left to right 16+17= (1+1) , (6+7) = 2,(13) =(2+1),3 =33. [ These steps are carried out mentally. Then with a simple subtraction we get 27-19= (2-1) ,(7-9) = 1,(-2) = 10-2=8 or mix (2-1),7 - 9 =17-9 =[ use all from 9 and the last from 10] = 7+1 =8. 3. the rule to check an addition or subtraction is the following, let the a, b be numbers that lie in Z+ , and S be an operator that sum the digits in the number representation. Then the rule\nS(S(a)+S(b))=S(a+b) can be used to check if it is correct. Example 27 +19 = 46 : check S(S(27) +S(19))=S(9+10)=S(19)=S(10)=1=S(46)=S(10)=1 , OK!. This also works with a multiplication : a*b=c with the check S(S(a)*S(b))=S(c) . 4. Square numbers with 5 : 75^2 = 7*(7+1), 25 = 5625 . 5. The multiplication method used in the thread with examples from cmd. This provides a fast way to expand your mental multiplication table with numbers like 14*17= (14+7), 4*7 = 21,28 = 238 and with squares that are easiest to remember mentally. There are a lot more methods but those have more conditions. Google Vedic mathematics to learn more. These methods are very useful with large numbers, but one can practice the ideas on small problems to get better faster. The source that I've used is an introduction by Kenneth Williams called 'The art of mental math ' or something similar. It covers the most basic methods, but I will eventually order 'the real deal' , I mean the books with the complete theory. ]\nQuestion\ns\nRating\n\n32,732,850\nGET\nGET THE APP.\nweegy*",
null,
"*\nGet answers from Weegy and a team of really smart live experts.\nPopular Conversations\nWhich set is an example of like fractions? A. 1/2 and 3/2 B. 7/4 and ...\nWeegy: The set which is an example of like fractions is: 10/10 and 5/5.\nVery light, thin lines that separate the colored areas or rock units ...\nWeegy: Very light, thin lines that separate the colored areas or rock units on a geologic map are called contact lines. ...\nA user can move to the end of a document by pressing what key ...\nWeegy: A user can easily move to the end of a document by pressing the Ctrl+Page Down key combination. User: What ...\nA galaxy that has a shape similar to a football is a(n) ____ galaxy. ...\nWeegy: A galaxy that has a shape similar to a football is an irregular galaxy.\nIn Asia, the Cold war led to\nWhich NIMS Management Characteristic refers to the number of ...\nWeegy: Manageable Span of Control refers to the number of subordinates that directly report to a supervisor. User: ...\nS\nL\nP\nR\nP\nR\nL\nP\nP\nC\nR\nP\nR\nL\nP\nR\nP\nR\nP\nR\nR\nPoints 1667 [Total 19103] Ratings 1 Comments 1347 Invitations 31 Offline\nS\nL\nL\n1\nP\n1\nL\nPoints 1473 [Total 10213] Ratings 14 Comments 1333 Invitations 0 Offline\nS\nL\nPoints 815 [Total 2097] Ratings 0 Comments 765 Invitations 5 Offline\nS\nL\nP\n1\nL\nPoints 579 [Total 6545] Ratings 7 Comments 509 Invitations 0 Offline\nS\nL\nP\nP\nP\n1\nP\nL\n1\nPoints 449 [Total 9101] Ratings 4 Comments 409 Invitations 0 Offline\nS\nL\nPoints 263 [Total 917] Ratings 19 Comments 73 Invitations 0 Offline\nS\nL\n1\n1\n1\n1\n1\n1\n1\n1\n1\n1\nPoints 189 [Total 2306] Ratings 18 Comments 9 Invitations 0 Offline\nS\nL\nPoints 152 [Total 3183] Ratings 4 Comments 112 Invitations 0 Offline\nS\nL\nPoints 143 [Total 340] Ratings 0 Comments 143 Invitations 0 Offline\nS\nL\nPoints 141 [Total 152] Ratings 0 Comments 141 Invitations 0 Offline\n* Excludes moderators and previous\nwinners (Include)\nHome | Contact | Blog | About | Terms | Privacy | © Purple Inc."
]
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"https://www.weegy.com/img/ad-appstore-4.png",
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https://answers.everydaycalculation.com/add-fractions/9-40-plus-10-20 | [
"Solutions by everydaycalculation.com\n\n9/40 + 10/20 is 29/40.\n\n1. Find the least common denominator or LCM of the two denominators:\nLCM of 40 and 20 is 40\n2. For the 1st fraction, since 40 × 1 = 40,\n9/40 = 9 × 1/40 × 1 = 9/40\n3. Likewise, for the 2nd fraction, since 20 × 2 = 40,\n10/20 = 10 × 2/20 × 2 = 20/40",
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"Download our mobile app and learn to work with fractions in your own time:"
]
| [
null,
"https://answers.everydaycalculation.com/mathstep-app-icon.png",
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.5421632,"math_prob":0.99534184,"size":330,"snap":"2019-43-2019-47","text_gpt3_token_len":133,"char_repetition_ratio":0.21779141,"word_repetition_ratio":0.0,"special_character_ratio":0.5030303,"punctuation_ratio":0.064935066,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99656934,"pos_list":[0,1,2],"im_url_duplicate_count":[null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-11-12T03:31:38Z\",\"WARC-Record-ID\":\"<urn:uuid:a98a2a2e-f46c-45fb-81e9-f5c7e48d7154>\",\"Content-Length\":\"7700\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:6e8c28f1-4ed6-4e7b-b44e-b6942c123e46>\",\"WARC-Concurrent-To\":\"<urn:uuid:5226c1b7-f672-41bf-af3e-2fc0c565e019>\",\"WARC-IP-Address\":\"96.126.107.130\",\"WARC-Target-URI\":\"https://answers.everydaycalculation.com/add-fractions/9-40-plus-10-20\",\"WARC-Payload-Digest\":\"sha1:325OO4Y43WNGXLCAAYWXSKPOAIRBUTKL\",\"WARC-Block-Digest\":\"sha1:XPBJLIPTF3SMR6F4IDNZDVENPGVZ7CUT\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-47/CC-MAIN-2019-47_segments_1573496664567.4_warc_CC-MAIN-20191112024224-20191112052224-00399.warc.gz\"}"} |
https://codereview.stackexchange.com/questions/100642/a-big-game-of-life | [
"# A big “Game of Life”\n\nOur quest: Create a big simulation for Conway's Game of Life, and record the entire simulation history.\n\nCurrent Approach: Cython is used for an iterate method. The history of life is placed in an HDF store, with help from pandas, and matplotlib is used to visually check results.\n\nWhat I could use help with: While I'd love advice on anything, I'm especially interested in improving the pandas implementation in this code. Also, how could I make this file easier for others to read?\n\nExplanation of definitions\n\n• Z (ndarray, int32): 2D array of life (1 or 0).\n• N (ndarray, int32): Temporary array used to tally the count of neighbors at each point on Z. N has the shape of Z minus one on each axis.\n• Z_chunk (DataFrame, int32): History of the past few iterations of Z\n\niterate.pyx\n\n#cython: wraparound=False, boundscheck=False, cdivision=True\n#cython: profile=False, nonecheck=False, overflowcheck=False\n#cython: cdivision_warnings=False, unraisable_tracebacks=False\nimport numpy as np\ncimport numpy as np\n\ncpdef iterate(Z, c):\n'''Element by elemenent iteration with optimized Cython.\n\nArgs:\nZ (ndarray - int32) - Represents 2D space\nc (namedtuple) - Container for constants\nReturns:\nZ (ndarray - int32)\n'''\n\nN = np.zeros((c.rows-1, c.cols-1), dtype=np.int32)\n\ncdef int rows = c.rows\ncdef int cols = c.cols\ncdef int [:, :] N_ = N\ncdef int [:, :] Z_ = Z\ncdef int x, y\n\nwith nogil:\n# Count neighbors\nfor x in range(1, rows-1):\nfor y in range(1, cols-1):\nN_[x, y] = (Z_[x-1, y-1] + Z_[x-1, y] + Z_[x-1, y+1] +\nZ_[x, y-1] + Z_[x, y+1] +\nZ_[x+1, y-1] + Z_[x+1, y] + Z_[x+1, y+1])\n# Apply rules\nfor x in range(1, rows-1):\nfor y in range(1, cols-1):\nif Z_[x, y] == 1 and (N_[x, y] < 2 or N_[x, y] > 3):\nZ_[x, y] = 0\nelif Z_[x, y] == 0 and N_[x, y] == 3:\nZ_[x, y] = 1\n\nreturn np.array(Z_)\n\n\nMain file\n\nimport time\nimport os, sys\nfrom matplotlib import pylab as plt\nimport numpy as np\nimport pandas as pd\nfrom pandas import Series, DataFrame\nfrom collections import namedtuple\nimport pyximport; pyximport.install()\nfrom iterate import iterate\n\n# Configure constants\n#####################\n\n# WARNING! Do not make these values large.\n# The pandas part of this code is poorly written and does not scale well.\nn_chunks = 3\nchunk_size = 10\nn_iterations = n_chunks * chunk_size\nrows = 128\ncols = 128\n\nlbls_row = ['row%05i'%(i) for i in range(rows)]\nlbls_col = ['col%05i'%(i) for i in range(cols)]\nlbls_iter_all = ['iter%05i'%(i) for i in range(n_iterations)]\n\n# c is passed to all functions\nConst = namedtuple('c', ['rows', 'cols', 'n_iterations', 'chunk_size', 'n_chunks',\n'store_path', 'save_path', 'lbls_row', 'lbls_col',\n'lbls_iter_all'])\nc = Const(rows=rows, cols=cols, n_iterations=n_iterations, chunk_size=chunk_size,\nn_chunks=n_chunks, store_path='life_store.h5', save_path='life_results',\nlbls_row=lbls_row, lbls_col=lbls_col, lbls_iter_all=lbls_iter_all)\n\n# Use m only for matplotlib parameters\ndpi = 72.0\nfigsize = c.cols / float(dpi), c.rows / float(dpi)\nConfig_mpl = namedtuple('m', ['figsize', 'dpi'])\nm = Config_mpl(figsize=figsize, dpi=dpi)\n\n# Run the game\n##############\n\nstart = time.time()\n\n# Clear previous results if they exist\nif os.path.exists(c.store_path):\nos.system('rm ' + c.store_path)\n# Create new store\nstore = pd.HDFStore(c.store_path)\n\n# Randomly place 1s throughout the map\nZ = np.random.randint(0, 2, (c.rows, c.cols)).astype(np.int32)\nZ[0, :] = 0 # Clear boarders-- will act as a boundary\nZ[-1, :] = 0\nZ[:, 0] = 0\nZ[:, -1] = 0\n\nfor i in range(c.n_chunks):\nprint 'Chunk', i\n\n# Initialize Z_chunk\nlbls_iter = ['iter%05i'%(k) for k in range(c.chunk_size * i,\nc.chunk_size * i + c.chunk_size)]\ncolumns = pd.MultiIndex.from_product([lbls_iter, c.lbls_col], names=['iter', 'col'])\nZ_chunk = DataFrame(index=c.lbls_row, columns=columns, dtype=np.int32)\n\nfor j in range(c.chunk_size):\nZ_chunk.loc[:, lbls_iter[j]] = iterate(Z, c)\n\nstore['chunk%03i'%i] = Z_chunk\n\nprint 'Life lasted: ', time.time() - start\n\n# View results\n##############\n\n# Create a folder in the current directory\nif not os.path.exists(c.save_path):\nos.makedirs(c.save_path)\nelse: # Clear previous images if the directory exists\ncmd = 'rm ./' + c.save_path + '/*.png'\nos.system(cmd)\n\n# Create figure\nfig = plt.figure(figsize=m.figsize, dpi=m.dpi, facecolor=\"white\")\n\nax = fig.add_axes([0.0, 0.0, 1.0, 1.0], frameon=False)\nax.get_xaxis().set_visible(False)\nax.get_yaxis().set_visible(False)\n\n# Because of my sloppy HDF writing, we will need nested for loops here\nfor i in range(c.n_chunks):\nZ_chunk = store['chunk%03i'%i]\nlbls_iter = ['iter%05i'%(k) for k in range(c.chunk_size * i,\nc.chunk_size * i + c.chunk_size)]\nfor j, lbl in enumerate(lbls_iter):\n# Extract\nZ = Z_chunk.loc[:, lbl]\n# Show\nax.imshow(Z, interpolation='nearest', cmap=plt.cm.gray_r)\n# Save\nfig.savefig('./{}/img_{}.png'.format(c.save_path, (1+i)*(j+1)))\n# Clear\nax.cla()\n\n# Close\nplt.close(fig)\nstore.close()\n\n\nReferences: Python Tutorial\n\nUpdate!\n\nAs suggested by Curt, h5py is used instead of pandas to remove index support, and NumPy is used instead of Cython for clarity.\n\nWith the following values\n\nn_chunks = 10\nchunk_size = 100\nn_iterations = n_chunks * chunk_size\nrows = 1024\ncols = 1024\n\n\nComparison:\n\n• Cython - 31.8s\n• scipy.signal.convolve - 229.5s\n• NumPy vectorization - 49.1s\n\n(Note: The NumPy vectorization method is from the NumPy Tutorial linked above in the reference. I don't understand the mathematics behind convolution well enough to explain why it's slower.)\n\nThe following code seems to work very well for big values. Even though the Cython version is slightly faster, both methods are plenty fast enough when compared to disk writing and image processing.\n\nimport time\nimport os, sys\nfrom matplotlib import pylab as plt\nimport numpy as np\nimport h5py\nfrom scipy.signal import convolve\nfrom collections import namedtuple\n\ndef iterate(Z):\n# Count neighbours\nN = (Z[0:-2,0:-2] + Z[0:-2,1:-1] + Z[0:-2,2:] +\nZ[1:-1,0:-2] + Z[1:-1,2:] +\nZ[2: ,0:-2] + Z[2: ,1:-1] + Z[2: ,2:])\n\n# Apply rules\nbirth = (N==3) & (Z[1:-1,1:-1]==0)\nsurvive = ((N==2) | (N==3)) & (Z[1:-1,1:-1]==1)\nZ[...] = 0\nZ[1:-1,1:-1][birth | survive] = 1\nreturn Z\n\n# Configure constants\n#####################\n\nn_chunks = 10\nchunk_size = 100\nn_iterations = n_chunks * chunk_size\nrows = 1024\ncols = 1024\n\n# c is passed to all functions\nConst = namedtuple('c', ['rows', 'cols', 'n_iterations', 'chunk_size', 'n_chunks',\n'h5_path', 'save_path'])\nc = Const(rows=rows, cols=cols, n_iterations=n_iterations, chunk_size=chunk_size,\nn_chunks=n_chunks, h5_path='life.hdf5', save_path='life_results')\n\n# Use m only for matplotlib parameters\ndpi = 72.0\nfigsize = c.cols / float(dpi), c.rows / float(dpi)\nConfig_mpl = namedtuple('m', ['figsize', 'dpi'])\nm = Config_mpl(figsize=figsize, dpi=dpi)\n\n# Run the game\n##############\n\nstart = time.time()\n\n# Clear previous results if they exist\nif os.path.exists(c.h5_path):\nos.system('rm ' + c.h5_path)\n# Create new store\nf = h5py.File(c.h5_path, 'w')\n\ndset = f.create_dataset(\"Results\", (c.rows, c.cols, c.n_iterations), dtype=np.int32,\nchunks=(c.rows, c.cols, c.chunk_size))\n\n# Randomly place 1s throughout the map\nZ = np.random.randint(0, 2, (c.rows, c.cols)).astype(np.int32)\nZ[0, :] = 0 # Clear boarders-- will act as a boundary\nZ[-1, :] = 0\nZ[:, 0] = 0\nZ[:, -1] = 0\n\nfor i in range(c.n_chunks):\nprint 'Chunk', i\n\n# Initialize Z_chunk\nZ_chunk = np.zeros((c.rows, c.cols, c.chunk_size), dtype=np.int32)\n\nfor j in range(c.chunk_size):\nZ_chunk[:, :, j] = iterate(Z)\n\ndset[:, :, i*c.chunk_size : i*c.chunk_size+chunk_size] = Z_chunk\n\nprint 'Time elapsed: ', time.time() - start\n\n# View the results\n##################\n\n# Create a folder in the current directory\nif not os.path.exists(c.h5_path):\nos.makedirs(c.h5_path)\nelse: # Clear previous images if the directory exists\ncmd = 'rm ./' + c.h5_path + '/*.png'\nos.system(cmd)\n\n# Create figure\nfig = plt.figure(figsize=m.figsize, dpi=m.dpi, facecolor=\"white\")\n\nax = fig.add_axes([0.0, 0.0, 1.0, 1.0], frameon=False)\nax.get_xaxis().set_visible(False)\nax.get_yaxis().set_visible(False)\n\n# Iterate through dset to create images\nfor i in range(c.n_iterations):\n\n# Extract\nZ = dset[:, :, i]\n# Show\nax.imshow(Z, cmap=plt.cm.gray_r)\n# Save\nfig.savefig('./{}/img_{}.png'.format(c.save_path, i))\n# Clear\nax.cla()\n\n# Close\nplt.close(fig)\n\n\nExample frame",
null,
"• Awesome update! BTW I did some more reading and convolve2d is way faster than the general convolve for the specific case of 2D data. It may still be slower than your NumPy or Cython versions, though. – Curt F. Aug 16 '15 at 4:46\n• Also, if you haven't seen it already, this post was pretty cool: jakevdp.github.io/blog/2013/08/07/conways-game-of-life – Curt F. Aug 16 '15 at 4:56\n\nDISCLAIMER: I don't know cython and have never used it, so if any of my advice doesn't apply because of cython limitations, feel free to disregard it.\n\n1. Counting neighbors in a game board is very easy to do via convolution with the proper kernel. Below, I used SciPy's convolve function, not the much faster fftconvolve, because the latter only works on floats and so rounding back to integers / bools would be required. Nonetheless, I suspect for large game boards, the FFT method and rounding may still be faster. I doubt that Cython would speed up NumPy very much, but I would love to be proven wrong! (A Cython guide for NumPy users says Typical Python numerical programs would tend to gain very little as most time is spent in lower-level C that is used in a high-level fashion.) Anyway, to my eye at least this function is a bit easier to read and interpret.\n\nimport numpy as np\nfrom scipy.signal import convolve\n\ndef iterate_game_of_life(board, neighbors_kernel=None):\n\"\"\"Performs one iteration of Conway's game of life on a 2d numpy array of bools\"\"\"\nif neighbors_kernel is None:\nneighbors_kernel = np.ones(shape=(3, 3), dtype='int')\nneighbors_kernel[1, 1] = 0\n\nneighbors_count = convolve(board, neighbors_kernel, mode='same')\nhas_three, has_two = neighbors_count == 3, neighbors_count == 2\nreturn np.logical_or(has_three, np.logical_and(board, has_two))\n\n1. Why do you need pandas at all? Are you using it just to store HDF5 files? If so, I'd recommend looking at h5py instead. You may have to learn a bit more about how HDF5 file formats work, but I think it would be more efficient than Pandas. In particular, in an application like this where the game board is naturally a matrix, Pandas' DataFrame model that rows and columns need to have labels seems like annoying overhead instead of a feature. You could even store the iterations of the game as a single datacube instead of as separate HDF5 datasets.\n\n2. Probably defining your own chunking will improve HDF5 performance at the largest sizes, but it depends on how you want to view the data. Do you want to view the entire board for a single iteration easily? Or do you want to view a small region of the board across multiple iterations easily? Unless you have particular views in mind, a good starting place would be to just use h5py's autochunking, i.e., don't define your own.\n\n3. This is minor, but why are you using any interpolation at all in ax.imshow(Z, interpolation='nearest', cmap=plt.cm.gray_r)? I'd recommend ax.imshow(Z, interpolation='none', cmap=plt.cm.gray_r)."
]
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null,
"https://i.stack.imgur.com/QZnkz.jpg",
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.52630097,"math_prob":0.9429752,"size":8393,"snap":"2020-45-2020-50","text_gpt3_token_len":2622,"char_repetition_ratio":0.12337585,"word_repetition_ratio":0.29197684,"special_character_ratio":0.34767067,"punctuation_ratio":0.23145072,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9921169,"pos_list":[0,1,2],"im_url_duplicate_count":[null,4,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-10-30T21:00:01Z\",\"WARC-Record-ID\":\"<urn:uuid:e2a72915-377e-470a-a09b-f82292d6c14c>\",\"Content-Length\":\"161747\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:07fe5295-6487-45e6-b091-c672e0fa0872>\",\"WARC-Concurrent-To\":\"<urn:uuid:13bb67e2-ce4d-4747-934a-ec0cf75e0f35>\",\"WARC-IP-Address\":\"151.101.129.69\",\"WARC-Target-URI\":\"https://codereview.stackexchange.com/questions/100642/a-big-game-of-life\",\"WARC-Payload-Digest\":\"sha1:RTE6WNI5U4JYJHHB4BP6U2KVYXGWCIIJ\",\"WARC-Block-Digest\":\"sha1:HSQYPHMBMXMCA4CXCHXXPAKVKAFY4PCT\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-45/CC-MAIN-2020-45_segments_1603107911229.96_warc_CC-MAIN-20201030182757-20201030212757-00096.warc.gz\"}"} |
https://www.percentagecal.com/answer/93-is-what-percent-of-152.4 | [
"Solution for 93 is what percent of 152.4:\n\n93:152.4*100 =\n\n(93*100):152.4 =\n\n9300:152.4 = 61.023622047244\n\nNow we have: 93 is what percent of 152.4 = 61.023622047244\n\nQuestion: 93 is what percent of 152.4?\n\nPercentage solution with steps:\n\nStep 1: We make the assumption that 152.4 is 100% since it is our output value.\n\nStep 2: We next represent the value we seek with {x}.\n\nStep 3: From step 1, it follows that {100\\%}={152.4}.\n\nStep 4: In the same vein, {x\\%}={93}.\n\nStep 5: This gives us a pair of simple equations:\n\n{100\\%}={152.4}(1).\n\n{x\\%}={93}(2).\n\nStep 6: By simply dividing equation 1 by equation 2 and taking note of the fact that both the LHS\n(left hand side) of both equations have the same unit (%); we have\n\n\\frac{100\\%}{x\\%}=\\frac{152.4}{93}\n\nStep 7: Taking the inverse (or reciprocal) of both sides yields\n\n\\frac{x\\%}{100\\%}=\\frac{93}{152.4}\n\n\\Rightarrow{x} = {61.023622047244\\%}\n\nTherefore, {93} is {61.023622047244\\%} of {152.4}.\n\nSolution for 152.4 is what percent of 93:\n\n152.4:93*100 =\n\n(152.4*100):93 =\n\n15240:93 = 163.87096774194\n\nNow we have: 152.4 is what percent of 93 = 163.87096774194\n\nQuestion: 152.4 is what percent of 93?\n\nPercentage solution with steps:\n\nStep 1: We make the assumption that 93 is 100% since it is our output value.\n\nStep 2: We next represent the value we seek with {x}.\n\nStep 3: From step 1, it follows that {100\\%}={93}.\n\nStep 4: In the same vein, {x\\%}={152.4}.\n\nStep 5: This gives us a pair of simple equations:\n\n{100\\%}={93}(1).\n\n{x\\%}={152.4}(2).\n\nStep 6: By simply dividing equation 1 by equation 2 and taking note of the fact that both the LHS\n(left hand side) of both equations have the same unit (%); we have\n\n\\frac{100\\%}{x\\%}=\\frac{93}{152.4}\n\nStep 7: Taking the inverse (or reciprocal) of both sides yields\n\n\\frac{x\\%}{100\\%}=\\frac{152.4}{93}\n\n\\Rightarrow{x} = {163.87096774194\\%}\n\nTherefore, {152.4} is {163.87096774194\\%} of {93}.\n\nCalculation Samples"
]
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null
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.8428846,"math_prob":0.99931645,"size":2251,"snap":"2022-05-2022-21","text_gpt3_token_len":803,"char_repetition_ratio":0.17935024,"word_repetition_ratio":0.42933333,"special_character_ratio":0.48556197,"punctuation_ratio":0.18317758,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99995315,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2022-01-19T02:21:50Z\",\"WARC-Record-ID\":\"<urn:uuid:42120cf8-3f8c-426a-ad1e-4e3b515bdf2e>\",\"Content-Length\":\"10459\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:d7bd77b1-bcf4-48ed-ab4c-b8fdfd850804>\",\"WARC-Concurrent-To\":\"<urn:uuid:cf9900fa-b1d2-4abf-b47c-c4af00a1b2f5>\",\"WARC-IP-Address\":\"217.23.5.136\",\"WARC-Target-URI\":\"https://www.percentagecal.com/answer/93-is-what-percent-of-152.4\",\"WARC-Payload-Digest\":\"sha1:FQHF2ZKVSFUASXBYDNGKJQ5DO4EWHQAE\",\"WARC-Block-Digest\":\"sha1:7VSVQK2UXHP375WAHBUQNKCVL432YG7F\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2022/CC-MAIN-2022-05/CC-MAIN-2022-05_segments_1642320301217.83_warc_CC-MAIN-20220119003144-20220119033144-00397.warc.gz\"}"} |
https://cs.stackexchange.com/questions/37450/three-languages-and-how-to-decide-if-they-are-regular?noredirect=1 | [
"# Three languages and how to decide if they are regular [closed]\n\nFrom following languages which one is regular and why others are not?And what is the regular expression for regular one.\n\n$L_1= \\{wxwy | x,y,w \\in (a+b)^+\\}$\n\n$L_2 = \\{xwyw | x,y,w \\in (a+b)^+\\}$\n\n$L_3 = \\{wxyw | x,y,w \\in (a+b)^+\\}$\n\nAlso where can I find these type of problems?\n\n## closed as unclear what you're asking by D.W.♦, Luke Mathieson, Juho, David Richerby, Ellen SpertusFeb 3 '15 at 0:29\n\nPlease clarify your specific problem or add additional details to highlight exactly what you need. As it's currently written, it’s hard to tell exactly what you're asking. See the How to Ask page for help clarifying this question. If this question can be reworded to fit the rules in the help center, please edit the question.\n\n• What have you tried and where did you get stuck? Please restrict yourself to one question per post. Where to find... why, via regular-languages of course! – Raphael Jan 22 '15 at 12:18\n• According to me regular expression for them are as follows-L1={{a(a+b)^+a(a+b)^+}+{b(a+b)^+b(a+b)^+}} L2={{(a+b)^+a(a+b)^+a}+{(a+b)^+b(a+b)^+b}} L3={{a(a+b)^+(a+b)^+a}+{b(a+b)^+(a+b)^+b}} So all should be regular?Am I right or wrong?@Raphael – user1917769 Jan 22 '15 at 16:05\n• What do you think? How did you get to these regular expressions? Have you tried formally proving correctness? – Raphael Jan 22 '15 at 16:13\n\n## 1 Answer\n\nThe first two are regular, because they can be written as $aA^*aA^*+bA^*bA^*$ and $A^*aA^*a+A^*bA^*b$ (where $A=a+b$). This is because it is enough to check them for $|w|=1$, as it is implied by longer $w$.\n\nThe last language is not regular, because its intersection with the regular language $a^+b^+aba^+b^+$ is $\\{a^nb^maba^nb^m| n,m\\geq 1\\}$ which is not regular (you can show this by pumping lemma).\n\n• +1 This paradigm is worth mentioning, since in my experience many beginners see the first $w$ and think that it has to match the second $w$ without realizing that the important thing is that you only have to match the first characters because of the arbitrary suffixes $x$ and $y$. Good job. – Rick Decker Jan 21 '15 at 20:20\n• I could not understand your explanation about L3.What are you assuming w,x and y as? And I think for L3 regular expression can be written as {a(a+b)^+(a+b)^+a}+{b(a+b)^+(a+b)^+b} So this should also be regular. – user1917769 Jan 22 '15 at 11:16\n• for $L3$ I use the fact that regular language are closed under intersection. So if I nteresect $L3$ with a regular language it should stay regular. I show it is not the case for this particular language. Your expression is not correct, because for instance $abab$ is not in it. – Denis Jan 22 '15 at 11:46\n• In abab what is w,x,y? And also remember x,y,w belong to (a+b)^+ so L3 length should be >=4.In abab w=a,x=b,y=a then w again can not be b – user1917769 Jan 22 '15 at 15:55\n• ah yes sorry, x and y have to be non empty, then say $ababab$ for instance, where $x=a$ and $y=b$. I edit the answer to correct this issue. – Denis Jan 22 '15 at 15:58"
]
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null
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.80849975,"math_prob":0.9699969,"size":276,"snap":"2019-35-2019-39","text_gpt3_token_len":98,"char_repetition_ratio":0.15441176,"word_repetition_ratio":0.0,"special_character_ratio":0.38043478,"punctuation_ratio":0.14285715,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9977803,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-08-24T20:01:00Z\",\"WARC-Record-ID\":\"<urn:uuid:eede7b43-5512-4d14-bbfa-8d24b298fbab>\",\"Content-Length\":\"129239\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:fb4c7946-ab62-4f93-a598-f1fa2c873ebf>\",\"WARC-Concurrent-To\":\"<urn:uuid:a5da5f42-bf8a-457b-a2c3-e47a7db7e904>\",\"WARC-IP-Address\":\"151.101.1.69\",\"WARC-Target-URI\":\"https://cs.stackexchange.com/questions/37450/three-languages-and-how-to-decide-if-they-are-regular?noredirect=1\",\"WARC-Payload-Digest\":\"sha1:ROACBEYEWYDMXE37JYQ3YH3K2A7EIK4R\",\"WARC-Block-Digest\":\"sha1:GZEBJLAPFZUB4E5H7MDM6HNJKA74HGVN\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-35/CC-MAIN-2019-35_segments_1566027321696.96_warc_CC-MAIN-20190824194521-20190824220521-00494.warc.gz\"}"} |
http://mathonline.wikidot.com/basic-operations-on-euclidean-n-space | [
"Basic Operations on Euclidean n-Space\n\n# Basic Operations on Euclidean n-Space\n\nRecall from the Euclidean n-Space page that for each positive integer $n$, the Euclidean n-space $\\mathbb{R}^n$ is the set of all points $\\mathbf{x} = (x_1, x_2, ..., x_n)$.\n\nIn a moment we will look at some operations defined on Euclidean n-space that the reader should already be familiar with. Before we do though, the reader should note that all of the operations defined below are in compliance to the field axioms of the real numbers in that all of the operations below are all in conjunction with the operations $+$ of addition and $\\cdot$ of multiplication of reals.\n\n Definition: if $\\mathbb{x} = (x_1, x_2, ..., x_n), \\mathbb{y} = (y_1, y_2, ..., y_n) \\in \\mathbb{R}^n$ then we define Equality $\\mathbf{x} = \\mathbf{y}$ if and only if $x_k = y_k$ for all $k \\in \\{ 1, 2, ..., n \\}$.\n\nFor example, if $\\mathbf{x} = (1, 4, 7)$ and $\\mathbf{y} = (1, 3, 7)$ then $\\mathbf{x} \\neq \\mathbf{y}$ since $4 \\neq 3$.\n\n Definition: If $\\mathbf{x} = (x_1, x_2, ..., x_n), \\mathbf{y} = (y_1, y_2, ..., y_n) \\in \\mathbb{R}^n$ then Addition is defined to be $\\mathbf{x} + \\mathbf{y} = (x_1 + y_1, x_2 + y_2, ..., x_n + y_n)$ and Subtraction is defined to be $\\mathbf{x} - \\mathbf{y} = (x_1 - y_1, x_2 - y_2, ..., x_n - y_n)$.\n\nFor example, consider the points $\\mathbf{x} = (1, 4, 2, 6), \\mathbf{y} = (3, -2, 0.5, \\pi) \\in \\mathbb{R}^4$. Then:\n\n(1)\n\\begin{align} \\quad \\mathbf{x} + \\mathbf{y} = (1+3, 4 +(-2), 2 + 0.5, 6 + \\pi) = (4, -2, 2.5, 6 + \\pi) \\end{align}\n\nAnd furthermore we have that:\n\n(2)\n\\begin{align} \\quad \\mathbf{x} - \\mathbf{y} = (1 - 3, 4 - (-2), 2 - 0.5, 6 - \\pi) = (-2, 6, 1.5, 6 -\\pi) \\end{align}\n\nNote that in general $\\mathbf{x} + \\mathbf{y} \\neq \\mathbf{y} + \\mathbf{x}$ which we are already familiar with in the case when $n = 1$.\n\n Definition: If $\\mathbf{x} = (x_1, x_2, ..., x_n) \\in \\mathbb{R}^n$ then Scalar Multiplication by the scalar $a \\in \\mathbb{R}$ is defined to be $a \\mathbf{x} = a(x_1, x_2, ..., x_n) = (ax_1, ax_2, ..., ax_n)$.\n\nFor example, consider the point $\\mathbf{x} = (1, 2, 3, 4, 5) \\in \\mathbb{R}^5$ and $a = 2 \\in \\mathbb{R}$. Then:\n\n(3)\n\\begin{align} \\quad a\\mathbf{x} = 2(1, 2, 3, 4, 5) = (2, 4, 6, 8, 10) \\end{align}"
]
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.61258364,"math_prob":1.0000094,"size":1892,"snap":"2023-40-2023-50","text_gpt3_token_len":719,"char_repetition_ratio":0.20603813,"word_repetition_ratio":0.064417176,"special_character_ratio":0.40591967,"punctuation_ratio":0.23972602,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":1.000009,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-09-30T06:03:20Z\",\"WARC-Record-ID\":\"<urn:uuid:5fbc0096-ef49-4140-9cc7-6ed9e7b1188c>\",\"Content-Length\":\"16445\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:bdbc5ece-856d-4b7f-9e76-fd3d240912ff>\",\"WARC-Concurrent-To\":\"<urn:uuid:2e046fe2-6a08-4e15-b1e6-48216e78d31a>\",\"WARC-IP-Address\":\"107.20.139.176\",\"WARC-Target-URI\":\"http://mathonline.wikidot.com/basic-operations-on-euclidean-n-space\",\"WARC-Payload-Digest\":\"sha1:LF67YBH2OKBTNSMTTL6EYHSCMVDMZVOY\",\"WARC-Block-Digest\":\"sha1:PBCQW3Z6Y3YT2IVI6IV2JR6NTFNK56EM\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-40/CC-MAIN-2023-40_segments_1695233510603.89_warc_CC-MAIN-20230930050118-20230930080118-00139.warc.gz\"}"} |
https://voer.edu.vn/c/the-first-law-of-thermodynamics/0e60bfc6/f28024af | [
"Giáo trình\n\n# College Physics\n\nScience and Technology\n\n## The First Law of Thermodynamics\n\nTác giả: OpenStaxCollege",
null,
"This boiling tea kettle represents energy in motion. The water in the kettle is turning to water vapor because heat is being transferred from the stove to the kettle. As the entire system gets hotter, work is done—from the evaporation of the water to the whistling of the kettle. (credit: Gina Hamilton)\n\nIf we are interested in how heat transfer is converted into doing work, then the conservation of energy principle is important. The first law of thermodynamics applies the conservation of energy principle to systems where heat transfer and doing work are the methods of transferring energy into and out of the system. The first law of thermodynamics states that the change in internal energy of a system equals the net heat transfer into the system minus the net work done by the system. In equation form, the first law of thermodynamics is\n\n$\\Delta U=Q-W\\text{.}$\n\nHere $\\Delta U$ is the change in internal energy $U$ of the system. $Q$ is the net heat transferred into the system—that is, $Q$ is the sum of all heat transfer into and out of the system. $W$ is the net work done by the system—that is, $W$ is the sum of all work done on or by the system. We use the following sign conventions: if $Q$ is positive, then there is a net heat transfer into the system; if $W$ is positive, then there is net work done by the system. So positive $Q$ adds energy to the system and positive $W$ takes energy from the system. Thus $\\Delta U=Q-W$. Note also that if more heat transfer into the system occurs than work done, the difference is stored as internal energy. Heat engines are a good example of this—heat transfer into them takes place so that they can do work. (See [link].) We will now examine $Q$, $W$, and $\\Delta U$ further.",
null,
"The first law of thermodynamics is the conservation-of-energy principle stated for a system where heat and work are the methods of transferring energy for a system in thermal equilibrium. Q size 12{Q} {} represents the net heat transfer—it is the sum of all heat transfers into and out of the system. Q size 12{Q} {} is positive for net heat transfer into the system. W size 12{W} {} is the total work done on and by the system. W size 12{W} {} is positive when more work is done by the system than on it. The change in the internal energy of the system, ΔU size 12{ΔU} {}, is related to heat and work by the first law of thermodynamics, ΔU=Q−W size 12{ΔU=Q - W} {}.\n\n# Heat Q and Work W\n\nHeat transfer ($Q$) and doing work ($W$) are the two everyday means of bringing energy into or taking energy out of a system. The processes are quite different. Heat transfer, a less organized process, is driven by temperature differences. Work, a quite organized process, involves a macroscopic force exerted through a distance. Nevertheless, heat and work can produce identical results.For example, both can cause a temperature increase. Heat transfer into a system, such as when the Sun warms the air in a bicycle tire, can increase its temperature, and so can work done on the system, as when the bicyclist pumps air into the tire. Once the temperature increase has occurred, it is impossible to tell whether it was caused by heat transfer or by doing work. This uncertainty is an important point. Heat transfer and work are both energy in transit—neither is stored as such in a system. However, both can change the internal energy $U$ of a system. Internal energy is a form of energy completely different from either heat or work.\n\n# Internal Energy U\n\nWe can think about the internal energy of a system in two different but consistent ways. The first is the atomic and molecular view, which examines the system on the atomic and molecular scale. The internal energy $U$ of a system is the sum of the kinetic and potential energies of its atoms and molecules. Recall that kinetic plus potential energy is called mechanical energy. Thus internal energy is the sum of atomic and molecular mechanical energy. Because it is impossible to keep track of all individual atoms and molecules, we must deal with averages and distributions. A second way to view the internal energy of a system is in terms of its macroscopic characteristics, which are very similar to atomic and molecular average values.\n\nMacroscopically, we define the change in internal energy $\\Delta U$ to be that given by the first law of thermodynamics:\n\n$\\Delta U=Q-W\\text{.}$\n\nMany detailed experiments have verified that $\\Delta U=Q-W$, where $\\Delta U$ is the change in total kinetic and potential energy of all atoms and molecules in a system. It has also been determined experimentally that the internal energy $U$ of a system depends only on the state of the system and not how it reached that state. More specifically, $U$ is found to be a function of a few macroscopic quantities (pressure, volume, and temperature, for example), independent of past history such as whether there has been heat transfer or work done. This independence means that if we know the state of a system, we can calculate changes in its internal energy $U$ from a few macroscopic variables.\n\nTo get a better idea of how to think about the internal energy of a system, let us examine a system going from State 1 to State 2. The system has internal energy ${U}_{1}$ in State 1, and it has internal energy ${U}_{2}$ in State 2, no matter how it got to either state. So the change in internal energy $\\Delta U={U}_{2}-{U}_{1}$ is independent of what caused the change. In other words, $\\Delta U$ is independent of path. By path, we mean the method of getting from the starting point to the ending point. Why is this independence important? Note that $\\Delta U=Q-W$. Both $Q$ and $W$depend on path, but $\\Delta U$ does not. This path independence means that internal energy $U$ is easier to consider than either heat transfer or work done.\n\nCalculating Change in Internal Energy: The Same Change in $U$ is Produced by Two Different Processes\n\n(a) Suppose there is heat transfer of 40.00 J to a system, while the system does 10.00 J of work. Later, there is heat transfer of 25.00 J out of the system while 4.00 J of work is done on the system. What is the net change in internal energy of the system?\n\n(b) What is the change in internal energy of a system when a total of 150.00 J of heat transfer occurs out of (from) the system and 159.00 J of work is done on the system? (See [link]).\n\nStrategy\n\nIn part (a), we must first find the net heat transfer and net work done from the given information. Then the first law of thermodynamics $\\left(\\Delta U=Q-W\\right)$ can be used to find the change in internal energy. In part (b), the net heat transfer and work done are given, so the equation can be used directly.\n\nSolution for (a)\n\nThe net heat transfer is the heat transfer into the system minus the heat transfer out of the system, or\n\n$Q=\\text{40}\\text{.}\\text{00}J-\\text{25}\\text{.}\\text{00 J}=\\text{15}\\text{.}\\text{00}\\phantom{\\rule{0.25em}{0ex}}J.$\n\nSimilarly, the total work is the work done by the system minus the work done on the system, or\n\n$W=\\text{10}\\text{.}\\text{00}J-4\\text{.}\\text{00}J=6\\text{.}\\text{00 J.}$\n\nThus the change in internal energy is given by the first law of thermodynamics:\n\n$\\Delta U=Q-W=\\text{15}\\text{.}\\text{00}J-6\\text{.}\\text{00}J=9\\text{.}\\text{00 J.}$\n\nWe can also find the change in internal energy for each of the two steps. First, consider 40.00 J of heat transfer in and 10.00 J of work out, or\n\n$\\Delta {U}_{1}={Q}_{1}-{W}_{1}=\\text{40}\\text{.}\\text{00}J-\\text{10}\\text{.}\\text{00}J=\\text{30}\\text{.}\\text{00 J.}$\n\nNow consider 25.00 J of heat transfer out and 4.00 J of work in, or\n\n$\\Delta {U}_{2}={Q}_{2}-{W}_{2}\\text{=}-\\text{25}\\text{.}\\text{00}J-\\left(-4\\text{.}\\text{00}J\\right)=\\text{–21.00 J.}$\n\nThe total change is the sum of these two steps, or\n\n$\\Delta U=\\Delta {U}_{1}+\\Delta {U}_{2}=\\text{30}\\text{.}\\text{00}J+\\left(-\\text{21}\\text{.}\\text{00}J\\right)=9\\text{.}\\text{00 J.}$\n\nDiscussion on (a)\n\nNo matter whether you look at the overall process or break it into steps, the change in internal energy is the same.\n\nSolution for (b)\n\nHere the net heat transfer and total work are given directly to be $Q=–\\text{150}\\text{.}\\text{00 J}$ and $W=–\\text{159}\\text{.}\\text{00 J}$, so that\n\n$\\Delta U=Q–W=–\\text{150}\\text{.}\\text{00 J}–\\left(-\\text{159}\\text{.}\\text{00 J}\\right)=9\\text{.}\\text{00 J.}$\n\nDiscussion on (b)\n\nA very different process in part (b) produces the same 9.00-J change in internal energy as in part (a). Note that the change in the system in both parts is related to $\\Delta U$ and not to the individual $Q$s or $W$s involved. The system ends up in the same state in both (a) and (b). Parts (a) and (b) present two different paths for the system to follow between the same starting and ending points, and the change in internal energy for each is the same—it is independent of path.",
null,
"Two different processes produce the same change in a system. (a) A total of 15.00 J of heat transfer occurs into the system, while work takes out a total of 6.00 J. The change in internal energy is ΔU=Q−W=9.00 J size 12{DU=Q-W=9 \".\" \"00\"\" J\"} {}. (b) Heat transfer removes 150.00 J from the system while work puts 159.00 J into it, producing an increase of 9.00 J in internal energy. If the system starts out in the same state in (a) and (b), it will end up in the same final state in either case—its final state is related to internal energy, not how that energy was acquired.\n\n## Human Metabolism and the First Law of Thermodynamics\n\nHuman metabolism is the conversion of food into heat transfer, work, and stored fat. Metabolism is an interesting example of the first law of thermodynamics in action. We now take another look at these topics via the first law of thermodynamics. Considering the body as the system of interest, we can use the first law to examine heat transfer, doing work, and internal energy in activities ranging from sleep to heavy exercise. What are some of the major characteristics of heat transfer, doing work, and energy in the body? For one, body temperature is normally kept constant by heat transfer to the surroundings. This means $Q$ is negative. Another fact is that the body usually does work on the outside world. This means $W$ is positive. In such situations, then, the body loses internal energy, since $\\Delta U=Q-W$ is negative.\n\nNow consider the effects of eating. Eating increases the internal energy of the body by adding chemical potential energy (this is an unromantic view of a good steak). The body metabolizes all the food we consume. Basically, metabolism is an oxidation process in which the chemical potential energy of food is released. This implies that food input is in the form of work. Food energy is reported in a special unit, known as the Calorie. This energy is measured by burning food in a calorimeter, which is how the units are determined.\n\nIn chemistry and biochemistry, one calorie (spelled with a lowercase c) is defined as the energy (or heat transfer) required to raise the temperature of one gram of pure water by one degree Celsius. Nutritionists and weight-watchers tend to use the dietary calorie, which is frequently called a Calorie (spelled with a capital C). One food Calorie is the energy needed to raise the temperature of one kilogram of water by one degree Celsius. This means that one dietary Calorie is equal to one kilocalorie for the chemist, and one must be careful to avoid confusion between the two.\n\nAgain, consider the internal energy the body has lost. There are three places this internal energy can go—to heat transfer, to doing work, and to stored fat (a tiny fraction also goes to cell repair and growth). Heat transfer and doing work take internal energy out of the body, and food puts it back. If you eat just the right amount of food, then your average internal energy remains constant. Whatever you lose to heat transfer and doing work is replaced by food, so that, in the long run, $\\Delta U=0$. If you overeat repeatedly, then $\\Delta U$ is always positive, and your body stores this extra internal energy as fat. The reverse is true if you eat too little. If $\\Delta U$ is negative for a few days, then the body metabolizes its own fat to maintain body temperature and do work that takes energy from the body. This process is how dieting produces weight loss.\n\nLife is not always this simple, as any dieter knows. The body stores fat or metabolizes it only if energy intake changes for a period of several days. Once you have been on a major diet, the next one is less successful because your body alters the way it responds to low energy intake. Your basal metabolic rate (BMR) is the rate at which food is converted into heat transfer and work done while the body is at complete rest. The body adjusts its basal metabolic rate to partially compensate for over-eating or under-eating. The body will decrease the metabolic rate rather than eliminate its own fat to replace lost food intake. You will chill more easily and feel less energetic as a result of the lower metabolic rate, and you will not lose weight as fast as before. Exercise helps to lose weight, because it produces both heat transfer from your body and work, and raises your metabolic rate even when you are at rest. Weight loss is also aided by the quite low efficiency of the body in converting internal energy to work, so that the loss of internal energy resulting from doing work is much greater than the work done.It should be noted, however, that living systems are not in thermalequilibrium.\n\nThe body provides us with an excellent indication that many thermodynamic processes are irreversible. An irreversible process can go in one direction but not the reverse, under a given set of conditions. For example, although body fat can be converted to do work and produce heat transfer, work done on the body and heat transfer into it cannot be converted to body fat. Otherwise, we could skip lunch by sunning ourselves or by walking down stairs. Another example of an irreversible thermodynamic process is photosynthesis. This process is the intake of one form of energy—light—by plants and its conversion to chemical potential energy. Both applications of the first law of thermodynamics are illustrated in [link]. One great advantage of conservation laws such as the first law of thermodynamics is that they accurately describe the beginning and ending points of complex processes, such as metabolism and photosynthesis, without regard to the complications in between. [link] presents a summary of terms relevant to the first law of thermodynamics.",
null,
"(a) The first law of thermodynamics applied to metabolism. Heat transferred out of the body (Q size 12{Q} {}) and work done by the body (W size 12{W} {}) remove internal energy, while food intake replaces it. (Food intake may be considered as work done on the body.) (b) Plants convert part of the radiant heat transfer in sunlight to stored chemical energy, a process called photosynthesis.\n Term Definition $U$ Internal energy—the sum of the kinetic and potential energies of a system’s atoms and molecules. Can be divided into many subcategories, such as thermal and chemical energy. Depends only on the state of a system (such as its $P$, $V$, and $T$), not on how the energy entered the system. Change in internal energy is path independent. $Q$ Heat—energy transferred because of a temperature difference. Characterized by random molecular motion. Highly dependent on path. $Q$ entering a system is positive. $W$ Work—energy transferred by a force moving through a distance. An organized, orderly process. Path dependent. $W$ done by a system (either against an external force or to increase the volume of the system) is positive.\n\n# Section Summary\n\n• The first law of thermodynamics is given as $\\Delta U=Q-W$, where $\\Delta U$ is the change in internal energy of a system, $Q$ is the net heat transfer (the sum of all heat transfer into and out of the system), and $W$ is the net work done (the sum of all work done on or by the system).\n• Both $Q$ and $W$ are energy in transit; only $\\Delta U$ represents an independent quantity capable of being stored.\n• The internal energy $U$ of a system depends only on the state of the system and not how it reached that state.\n• Metabolism of living organisms, and photosynthesis of plants, are specialized types of heat transfer, doing work, and internal energy of systems.\n\n# Conceptual Questions\n\nDescribe the photo of the tea kettle at the beginning of this section in terms of heat transfer, work done, and internal energy. How is heat being transferred? What is the work done and what is doing it? How does the kettle maintain its internal energy?\n\nThe first law of thermodynamics and the conservation of energy, as discussed in Conservation of Energy, are clearly related. How do they differ in the types of energy considered?\n\nHeat transfer $Q$ and work done $W$ are always energy in transit, whereas internal energy $U$ is energy stored in a system. Give an example of each type of energy, and state specifically how it is either in transit or resides in a system.\n\nHow do heat transfer and internal energy differ? In particular, which can be stored as such in a system and which cannot?\n\nIf you run down some stairs and stop, what happens to your kinetic energy and your initial gravitational potential energy?\n\nGive an explanation of how food energy (calories) can be viewed as molecular potential energy (consistent with the atomic and molecular definition of internal energy).\n\nIdentify the type of energy transferred to your body in each of the following as either internal energy, heat transfer, or doing work: (a) basking in sunlight; (b) eating food; (c) riding an elevator to a higher floor.\n\n# Problems & Exercises\n\nWhat is the change in internal energy of a car if you put 12.0 gal of gasoline into its tank? The energy content of gasoline is $1\\text{.}3×{\\text{10}}^{8}\\phantom{\\rule{0.25em}{0ex}}\\text{J/gal}$. All other factors, such as the car’s temperature, are constant.\n\n$1\\text{.}6×{\\text{10}}^{9}\\phantom{\\rule{0.25em}{0ex}}\\text{J}$\n\nHow much heat transfer occurs from a system, if its internal energy decreased by 150 J while it was doing 30.0 J of work?\n\nA system does $1\\text{.}\\text{80}×{\\text{10}}^{8}\\phantom{\\rule{0.25em}{0ex}}\\text{J}$ of work while $7\\text{.}\\text{50}×{\\text{10}}^{8}\\phantom{\\rule{0.25em}{0ex}}\\text{J}$ of heat transfer occurs to the environment. What is the change in internal energy of the system assuming no other changes (such as in temperature or by the addition of fuel)?\n\n$-9\\text{.}\\text{30}×{\\text{10}}^{8}\\phantom{\\rule{0.25em}{0ex}}\\text{J}$\n\nWhat is the change in internal energy of a system which does $4\\text{.}\\text{50}×{\\text{10}}^{5}\\phantom{\\rule{0.25em}{0ex}}\\text{J}$ of work while $3\\text{.}\\text{00}×{\\text{10}}^{6}\\phantom{\\rule{0.25em}{0ex}}\\text{J}$ of heat transfer occurs into the system, and $8\\text{.}\\text{00}×{\\text{10}}^{6}\\phantom{\\rule{0.25em}{0ex}}\\text{J}$ of heat transfer occurs to the environment?\n\nSuppose a woman does 500 J of work and 9500 J of heat transfer occurs into the environment in the process. (a) What is the decrease in her internal energy, assuming no change in temperature or consumption of food? (That is, there is no other energy transfer.) (b) What is her efficiency?\n\n(a) $-1\\text{.}0×{\\text{10}}^{4}\\phantom{\\rule{0.25em}{0ex}}\\text{J}$ , or $-2\\text{.}\\text{39 kcal}$\n\n(b) 5.00%\n\n(a) How much food energy will a man metabolize in the process of doing 35.0 kJ of work with an efficiency of 5.00%? (b) How much heat transfer occurs to the environment to keep his temperature constant? Explicitly show how you follow the steps in the Problem-Solving Strategy for thermodynamics found in Problem-Solving Strategies for Thermodynamics.\n\n(a) What is the average metabolic rate in watts of a man who metabolizes 10,500 kJ of food energy in one day? (b) What is the maximum amount of work in joules he can do without breaking down fat, assuming a maximum efficiency of 20.0%? (c) Compare his work output with the daily output of a 187-W (0.250-horsepower) motor.\n\n(a) 122 W\n\n(b) $2\\text{.}\\text{10}×{\\text{10}}^{6}\\phantom{\\rule{0.25em}{0ex}}\\text{J}$\n\n(c) Work done by the motor is $1\\text{.}\\text{61}×{\\text{10}}^{7}\\phantom{\\rule{0.25em}{0ex}}\\text{J}$ ;thus the motor produces 7.67 times the work done by the man\n\n(a) How long will the energy in a 1470-kJ (350-kcal) cup of yogurt last in a woman doing work at the rate of 150 W with an efficiency of 20.0% (such as in leisurely climbing stairs)? (b) Does the time found in part (a) imply that it is easy to consume more food energy than you can reasonably expect to work off with exercise?\n\n(a) A woman climbing the Washington Monument metabolizes $6\\text{.}\\text{00}×{\\text{10}}^{2}\\phantom{\\rule{0.25em}{0ex}}\\text{kJ}$ of food energy. If her efficiency is 18.0%, how much heat transfer occurs to the environment to keep her temperature constant? (b) Discuss the amount of heat transfer found in (a). Is it consistent with the fact that you quickly warm up when exercising?\n\n(a) 492 kJ\n\n(b) This amount of heat is consistent with the fact that you warm quickly when exercising. Since the body is inefficient, the excess heat produced must be dissipated through sweating, breathing, etc."
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https://codea.io/talk/discussion/12990/path-finder-again | [
"Howdy, Stranger!\n\nIt looks like you're new here. If you want to get involved, click one of these buttons!\n\nPath finder (again)\n\nPosts: 9,808\n\nHere’s another kind of useless program. I modified this from an earlier version I wrote. It finds the shortest path from a circle in the upper right corner to the lower left corner. There are red circle barriers that it has to go around. Tap the square to find the shortest path or no path, or tap the screen to add more barriers. Once the path is shown, tap the square to start another. Currently the size is 30, but it can be changed all the way to 1. If you’re below a size of maybe 10, depending on your device, it will be slow so you’ll have to be patient. I try to find the shortest path manually just to see if it agrees with me. Of course, once you get to a smaller size, it will be too small to try manually. At the lower sizes, it reminds me of a lightning bolt with the zig zags.\n\nviewer.mode=FULLSCREEN\n\nfunction setup()\nsize=30\n\nfontSize(25)\ninitializeVariables()\ninitializeTable()\nsetStartFinish()\nend\n\nfunction initializeVariables()\nmoveO={-1,1,0,1,1,0,0,-1,-1,-1,-1,0} -- odd line movement\nmoveE={0,1,1,1,1,0,1,-1,0,-1,-1,0} -- even line movement\nsq=math.sqrt(3)/2\nxSize=WIDTH//size-1\nySize=HEIGHT//size\nfind,showPath=false,false\ncount,pathPoints=0,0\npath,locTab={},{}\nend\n\nfunction initializeTable()\n-- fill table with 9999\ntab={}\nfor x=1,xSize do\ntab[x]={}\nfor y=1,ySize do\ntab[x][y]=9999\nend\nend\nend\n\n-- add barriers to table, set to 9998\nfor z=1,xSize*ySize/2 do\nx=math.random(xSize)\ny=math.random(ySize)\nif tab[x][y]~=9998 then\ntab[x][y]=9998\ncount=count+1\nend\nend\nend\n\nfunction setStartFinish()\nstart=vec2(3,3) -- starting x,y value\ntab[start.x][start.y]=0 -- set table start to 0\nfinish=vec2(xSize-2,ySize-2) -- ending x,y value\ntab[finish.x][finish.y]=9997 -- set table finist to 9997\nend\n\nfunction draw()\nbackground(0)\nfill(255)\nrect(WIDTH-60,HEIGHT-60,60,60)\nif not showPath then\ntext(\"Barriers \"..count,WIDTH/2,HEIGHT-35)\ntext(\"Tap screen for more barriers or tap square to find shortest path\",WIDTH/2,HEIGHT-75)\nelse\ntext(\"Tap screen for restart\",WIDTH/2,HEIGHT-75)\ntext(\"Path points \"..pathPoints,WIDTH/2,HEIGHT-35)\nend\nlocTab=tab\nfor x=1,xSize do\nfor y=1,ySize do\nfill(154, 213, 223, 163)\nif x==start.x and y==start.y or x==finish.x and y==finish.y then\nfill(234, 255, 0) -- set start and finish color\nelseif locTab[x][y]==9996 then\nfill(255) -- set path color\nelseif locTab[x][y]==9998 then\nfill(255,0,0) -- set barrier color\nend\nif y%2==0 then\nellipse(x*size+size/2,y*size*sq,size+2)\nelse\nellipse(x*size,y*size*sq,size+2)\nend\nend\nend\nfindPaths()\nshowPaths()\nend\n\nfunction findPaths()\nif find then\nfindAllPaths() -- returns a table of the path\nfindShortestPath()\nfind=false\nshowPath=true\nend\nend\n\nfunction showPaths()\nif showPath then -- show path\nif pathPoints==0 then\nfill(255)\ntext(\"NO PATH FOUND\",WIDTH/2,HEIGHT/2)\nelse\nfor zz=1,#path do\nlocTab[path[zz].x][path[zz].y]=9996\nend\nend\nend\nend\n\nfunction touched(t)\nif t.state==BEGAN then\nif not showPath then\nif t.x>WIDTH-60 and t.y>HEIGHT-60 then -- find path\nfind=true\nsetStartFinish()\nelse\nfor z=1,100 do -- add 100 extra barriers\nx=math.random(xSize)\ny=math.random(ySize)\nif tab[x][y]~=9998 then\ntab[x][y]=9998\ncount=count+1\nend\nsetStartFinish()\nend\nend\nelse\nviewer.restart() -- restart\nreturn\nend\nend\nend\n\nfunction findAllPaths()\nlocal v,c,val,x,y=0,0,0,0,0\n\n-- calculate all the path distances from start to finish\nlocal locTab1={vec2(start.x,start.y)}\nwhile find do\nlocal locTab2={}\nfor s=1,#locTab1 do\nfor z=1,12,2 do\nif locTab1[s].y%2==0 then\nmx=moveE[z]\nmy=moveE[z+1]\nelse\nmx=moveO[z]\nmy=moveO[z+1]\nend\nx=locTab1[s].x\ny=locTab1[s].y\nif x+mx>=1 and x+mx<=xSize and y+my>=1 and y+my<=ySize then\nif locTab[x+mx][y+my]==9999 then\nval=locTab[x][y]\nif val+1<locTab[x+mx][y+my] then\nlocTab[x+mx][y+my]=val+1\ntable.insert(locTab2,vec2(x+mx,y+my))\nend\nelseif locTab[x+mx][y+my]==9997 then\nfind=false\nend\nend\nend\nend\nlocTab1=locTab2\nif #locTab2==0 then\nfind=false\nreturn\nend\nend\nend\n\nfunction findShortestPath()\n-- find the shortest path distance from finish to start\nlocal ex1,ey1=finish.x,finish.y\nlocal xh,yh=ex1,ey1\nlocal c=0\nlocal find=true\nwhile find do\nval=locTab[ex1][ey1]\n-- move through moveO or moveE table by 2\nfor z=1,12,2 do\nif ey1%2==0 then\nx=ex1+moveE[z]\ny=ey1+moveE[z+1]\nelse\nx=ex1+moveO[z]\ny=ey1+moveO[z+1]\nend\nif x>=1 and x<=xSize and y>=1 and y<=ySize then\nv=locTab[x][y]\nif v<val then\nval=v\nxh=x\nyh=y\nend\nend\nend\nex1=xh\ney1=yh\n-- reached the start points\nif xh==start.x and yh==start.y then\npathPoints=#path\nreturn\nelse\ntable.insert(path,1,vec2(xh,yh))\nend\nc=c+1\nif c>2000 then -- prevent infinate while loop\nfind=false\nend\nend\nend\n\n• Posts: 18\n\nIs it a random method? I got rather satisfied with I think it is called the breath first search method and keep using that one. I have a a* one that I can port if needed.\n\nI did program a brute force pathfinder once. But this one gets slower with each additional step. That version just creates every possible path starting at one step and going up.\n\n• Posts: 9,808\n\n@Pakz This code finds every path from the start to the finish position. It also keeps track of how many steps it has to take for the paths. It then determines which of the 6 paths around the finish has the least amount of steps and follows that path back to the start. So it always finds the shortest path or one of them if several paths are equal. I have no use for this code other than it gave me a problem to solve and code to write.\n\n• Posts: 1,303\n\nHere's one I did. Tap once to choose starting pos, once to choose ending pos. Additional taps add obstacles where you tap.\n\nCell = class()\nCell.indices = { {-1,1}, {0,1}, {1,1}, {-1,0}, {1,0}, {-1,-1}, {0,-1}, {1, -1}}\nCell.indices = { {0,1}, {-1,0}, {1,0}, {0,-1} }\n\nfunction Cell:init(x,y,value)\nself.x = x\nself.y = y\nself.target = false\nself.obstacle = false\nself.path = false\nself.start = false\nself.distance = MaxDistance\nself.plaincolor = color(0,0,0)\nself.highlighted = false\nend\n\nfunction Cell:draw(grid)\nlocal step = grid.step\ndx = self.x * step\ndy = self.y * step\npushStyle()\nstrokeWidth(2)\nstroke(255,255,255)\nfill(self:color())\nrect(dx,dy, step,step)\nfill(255)\nif self.highlighted then fill(0) end\ntext(self.distance, dx+step/2, dy+step/2)\npopStyle()\nend\n\nfunction Cell:touched(grid, touch)\nif touch.state == BEGAN then\nlocal step = grid.step\nlowx = self.x*step\nlowy = self.y*step\nif ( touch.x > lowx and touch.y > lowy and touch.x < lowx + step and touch.y < lowy+step) then\nself:changeState()\nend\nend\nend\n\n-----\n\nfunction Cell:changeState()\nif State == \"start\" then Grid.start = self; self.start = true; State = \"target\"; return end\nif State == \"target\" then Grid.target = self; self.target = true; State = \"obstacle\" return end\nself.obstacle = not self.obstacle\nend\n\nfunction Cell:color()\nif self.start then return color(0,0,255) end\nif self.target then return color(0,255,0) end\nif self.obstacle then return color(255,0,0) end\nreturn self.plaincolor\nend\n\nfunction Cell:distanceFrom(c)\nif true then return 1 end\nlocal t = math.abs(c.x - self.x) + math.abs(c.y - self.y)\nif t == 1 then return 10 else return 14 end\nend\n\nfunction Cell:highlight()\nif self.highlighted or self.target or self.obstacle then return end\nself.highlighted = true\nself.plaincolor = color(255,255,0)\nGrid.highlightQueue:pushRight(self)\nend\n\nfunction Cell:highlightNeighbors()\nfunction compare(c1,c2)\nreturn Grid.target:vecDist(c1) < Grid.target:vecDist(c2)\nend\nif not self.distance then return end\nif self.obstacle then return end\nlocal ok = {}\nfor i,c in ipairs(self:neighbors()) do\nif c.distance < self.distance then\nif self.distance == 2 then\nprint(\"inserting\", self.x, self.y, self.distance, c.x, c.y, c.distance)\nend\ntable.insert(ok, c)\nend\nend\ntable.sort(ok,compare)\nlocal bestDistance = Grid.target:vecDist(ok)\nfor i,c in ipairs(ok) do\nif Grid.target:vecDist(c) == bestDistance then\nc:highlight()\nend\nend\nend\n\nfunction Cell:highlightPath()\nGrid:processHighlight(self)\nend\n\nfunction Cell:neighbors()\nlocal cells = {}\nfor i, p in ipairs(Cell.indices) do\nlocal cell = Grid:at(self.x + p, self.y + p)\ntable.insert(cells, cell)\nend\nreturn cells\nend\n\nfunction Cell:setDistance(dist)\nif self.obstacle then return end\nif self.distance > dist then\nself.distance = dist\nGrid.pathQueue:pushRight(self)\nend\nend\n\nfunction Cell:setNeighbors()\nif self.obstacle then return end\nfor i,c in ipairs(self:neighbors()) do\nc:setDistance(self.distance + self:distanceFrom(c))\nend\nend\n\nfunction Cell:setTarget()\nself.target = true\nself.distance = 0\nprint(\"i am target\", self.x, self.y)\nend\n\nfunction Cell:showPath()\nself.distance = 0\nGrid:processPath(self)\nend\n\nfunction Cell:vecDist(c)\nlocal s1 = vec2(self.x, self.y)\nlocal c1 = vec2(c.x,c.y)\nreturn s1:dist(c1)\nend"
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https://www.colorhexa.com/597a6c | [
"# #597a6c Color Information\n\nIn a RGB color space, hex #597a6c is composed of 34.9% red, 47.8% green and 42.4% blue. Whereas in a CMYK color space, it is composed of 27% cyan, 0% magenta, 11.5% yellow and 52.2% black. It has a hue angle of 154.5 degrees, a saturation of 15.6% and a lightness of 41.4%. #597a6c color hex could be obtained by blending #b2f4d8 with #000000. Closest websafe color is: #666666.\n\n• R 35\n• G 48\n• B 42\nRGB color chart\n• C 27\n• M 0\n• Y 11\n• K 52\nCMYK color chart\n\n#597a6c color description : Mostly desaturated dark cyan - lime green.\n\n# #597a6c Color Conversion\n\nThe hexadecimal color #597a6c has RGB values of R:89, G:122, B:108 and CMYK values of C:0.27, M:0, Y:0.11, K:0.52. Its decimal value is 5864044.\n\nHex triplet RGB Decimal 597a6c `#597a6c` 89, 122, 108 `rgb(89,122,108)` 34.9, 47.8, 42.4 `rgb(34.9%,47.8%,42.4%)` 27, 0, 11, 52 154.5°, 15.6, 41.4 `hsl(154.5,15.6%,41.4%)` 154.5°, 27, 47.8 666666 `#666666`\nCIE-LAB 48.417, -14.959, 3.867 13.785, 17.125, 16.766 0.289, 0.359, 17.125 48.417, 15.45, 165.505 48.417, -16.389, 7.47 41.383, -12.957, 4.947 01011001, 01111010, 01101100\n\n# Color Schemes with #597a6c\n\n• #597a6c\n``#597a6c` `rgb(89,122,108)``\n• #7a5967\n``#7a5967` `rgb(122,89,103)``\nComplementary Color\n• #597a5c\n``#597a5c` `rgb(89,122,92)``\n• #597a6c\n``#597a6c` `rgb(89,122,108)``\n• #59787a\n``#59787a` `rgb(89,120,122)``\nAnalogous Color\n• #7a5c59\n``#7a5c59` `rgb(122,92,89)``\n• #597a6c\n``#597a6c` `rgb(89,122,108)``\n• #7a5978\n``#7a5978` `rgb(122,89,120)``\nSplit Complementary Color\n• #7a6c59\n``#7a6c59` `rgb(122,108,89)``\n• #597a6c\n``#597a6c` `rgb(89,122,108)``\n• #6c597a\n``#6c597a` `rgb(108,89,122)``\n• #677a59\n``#677a59` `rgb(103,122,89)``\n• #597a6c\n``#597a6c` `rgb(89,122,108)``\n• #6c597a\n``#6c597a` `rgb(108,89,122)``\n• #7a5967\n``#7a5967` `rgb(122,89,103)``\n• #394e45\n``#394e45` `rgb(57,78,69)``\n• #435d52\n``#435d52` `rgb(67,93,82)``\n• #4e6b5f\n``#4e6b5f` `rgb(78,107,95)``\n• #597a6c\n``#597a6c` `rgb(89,122,108)``\n• #648979\n``#648979` `rgb(100,137,121)``\n• #709686\n``#709686` `rgb(112,150,134)``\n• #7ea192\n``#7ea192` `rgb(126,161,146)``\nMonochromatic Color\n\n# Alternatives to #597a6c\n\nBelow, you can see some colors close to #597a6c. Having a set of related colors can be useful if you need an inspirational alternative to your original color choice.\n\n• #597a64\n``#597a64` `rgb(89,122,100)``\n• #597a67\n``#597a67` `rgb(89,122,103)``\n• #597a69\n``#597a69` `rgb(89,122,105)``\n• #597a6c\n``#597a6c` `rgb(89,122,108)``\n• #597a6f\n``#597a6f` `rgb(89,122,111)``\n• #597a72\n``#597a72` `rgb(89,122,114)``\n• #597a74\n``#597a74` `rgb(89,122,116)``\nSimilar Colors\n\n# #597a6c Preview\n\nThis text has a font color of #597a6c.\n\n``<span style=\"color:#597a6c;\">Text here</span>``\n#597a6c background color\n\nThis paragraph has a background color of #597a6c.\n\n``<p style=\"background-color:#597a6c;\">Content here</p>``\n#597a6c border color\n\nThis element has a border color of #597a6c.\n\n``<div style=\"border:1px solid #597a6c;\">Content here</div>``\nCSS codes\n``.text {color:#597a6c;}``\n``.background {background-color:#597a6c;}``\n``.border {border:1px solid #597a6c;}``\n\n# Shades and Tints of #597a6c\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, #060908 is the darkest color, while #fcfdfd is the lightest one.\n\n• #060908\n``#060908` `rgb(6,9,8)``\n• #0f1412\n``#0f1412` `rgb(15,20,18)``\n• #171f1c\n``#171f1c` `rgb(23,31,28)``\n• #1f2b26\n``#1f2b26` `rgb(31,43,38)``\n• #273630\n``#273630` `rgb(39,54,48)``\n• #30413a\n``#30413a` `rgb(48,65,58)``\n• #384d44\n``#384d44` `rgb(56,77,68)``\n• #40584e\n``#40584e` `rgb(64,88,78)``\n• #486358\n``#486358` `rgb(72,99,88)``\n• #516f62\n``#516f62` `rgb(81,111,98)``\n• #597a6c\n``#597a6c` `rgb(89,122,108)``\n• #618576\n``#618576` `rgb(97,133,118)``\n• #6a9180\n``#6a9180` `rgb(106,145,128)``\n• #749a8a\n``#749a8a` `rgb(116,154,138)``\n• #7fa293\n``#7fa293` `rgb(127,162,147)``\n• #8baa9d\n``#8baa9d` `rgb(139,170,157)``\n• #96b3a6\n``#96b3a6` `rgb(150,179,166)``\n• #a2bbb0\n``#a2bbb0` `rgb(162,187,176)``\n``#adc3ba` `rgb(173,195,186)``\n• #b8cbc3\n``#b8cbc3` `rgb(184,203,195)``\n• #c4d4cd\n``#c4d4cd` `rgb(196,212,205)``\n• #cfdcd6\n``#cfdcd6` `rgb(207,220,214)``\n• #dae4e0\n``#dae4e0` `rgb(218,228,224)``\n• #e6ecea\n``#e6ecea` `rgb(230,236,234)``\n• #f1f5f3\n``#f1f5f3` `rgb(241,245,243)``\n• #fcfdfd\n``#fcfdfd` `rgb(252,253,253)``\nTint Color Variation\n\n# Tones of #597a6c\n\nA tone is produced by adding gray to any pure hue. In this case, #696a6a is the less saturated color, while #08cb78 is the most saturated one.\n\n• #696a6a\n``#696a6a` `rgb(105,106,106)``\n• #61726b\n``#61726b` `rgb(97,114,107)``\n• #597a6c\n``#597a6c` `rgb(89,122,108)``\n• #51826d\n``#51826d` `rgb(81,130,109)``\n• #498a6e\n``#498a6e` `rgb(73,138,110)``\n• #419270\n``#419270` `rgb(65,146,112)``\n• #399a71\n``#399a71` `rgb(57,154,113)``\n• #30a372\n``#30a372` `rgb(48,163,114)``\n• #28ab73\n``#28ab73` `rgb(40,171,115)``\n• #20b375\n``#20b375` `rgb(32,179,117)``\n• #18bb76\n``#18bb76` `rgb(24,187,118)``\n• #10c377\n``#10c377` `rgb(16,195,119)``\n• #08cb78\n``#08cb78` `rgb(8,203,120)``\nTone Color Variation\n\n# Color Blindness Simulator\n\nBelow, you can see how #597a6c 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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| {"ft_lang_label":"__label__en","ft_lang_prob":0.54585207,"math_prob":0.58134997,"size":3736,"snap":"2021-31-2021-39","text_gpt3_token_len":1653,"char_repetition_ratio":0.121918544,"word_repetition_ratio":0.011009174,"special_character_ratio":0.5596895,"punctuation_ratio":0.2358804,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99098366,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-09-18T08:25:48Z\",\"WARC-Record-ID\":\"<urn:uuid:2cda16e2-adef-407f-bbc9-6ba469f5fd4f>\",\"Content-Length\":\"36223\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:29b4d016-3550-4622-a361-a35140fc1345>\",\"WARC-Concurrent-To\":\"<urn:uuid:771fe0dd-c5f6-49a8-a409-7cfbc1d73401>\",\"WARC-IP-Address\":\"178.32.117.56\",\"WARC-Target-URI\":\"https://www.colorhexa.com/597a6c\",\"WARC-Payload-Digest\":\"sha1:C5H7TY6AGPS3NXHLHBFY3FM7N2WOMW5E\",\"WARC-Block-Digest\":\"sha1:YJ3YLIZAESNXOHESO7QPGLXDBHNE5KVP\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-39/CC-MAIN-2021-39_segments_1631780056348.59_warc_CC-MAIN-20210918062845-20210918092845-00469.warc.gz\"}"} |
https://tangerinedev.com/play/cat-watching-spider | [
"Close\n\n## Simone Seagle\n\nIndependent Web and Educational Software Developer\n\n# Tangerine Development\n\nPlay\n\n### Cat Watching a Spider\n\nMouse-over or touch/drag to interact with the spider. He'll follow your finger if you hover over the bottom part of the image. Or, view fullscreen.\n\n## About the Art\n\nCat Watching a Spider is a Japanese ink painting by Ōide Tōkō on silk from the 1890s. The Met doesn't have too much information about this piece for me to talk about, however. I was inspired by National Cat Day on Twitter to do a cat interactive, and the Japanese have a flair for depicting them. I wish I had more to say on the subject, but that's about it.\n\n## About the Programming\n\nThis works in a similar way to the Portrait Gallery interactive, where the eyes are a separate png behind the heads that follows something around. It uses pretty simple math to work:\n\n`````` var dy = spider.y - (eyeLocations.y*scale);\nvar dx = spider.x - (eyeLocations.x*scale);\n\nvar angle = Math.atan2( dy, dx);\n\nvar x = scale *(eyeLocations.x + 4 * Math.cos(angle));\nvar y = scale *(eyeLocations.y + 2 * Math.sin(angle));\n\ncatEyes.x = x;\ncatEyes.y = y;``````\n\nI do the same thing for the cat heads on the right and the left, and I show or hide one of the heads depending on which side of the cat the spider is on.\n\nThe spider moves by finding goal points and then trying to race to them, and for some reason it often overshoots. It's probably going too fast or something. Anyway, here's how I decide where the spider goes:\n\n`````` function newSpiderPt() {\n\nif (trackLoc.y < 1416 * scale || spider.y < 1400 * scale) {\n// If the tracking location or the spider is out of bounds, get a random point in the box\nvar x = Math.random() * size.width;\nvar y = Math.random() * (size.height\n- 1416 * scale) + 1416 * scale;\n\n} else {\n// It goes to the tracking location if in bounds\n//console.log(\"tracking!\", trackLoc);\nvar x= trackLoc.x;\nvar y = trackLoc.y;\n}\n\nspiderGoalPt = {x: x, y:y};\n\nvar angle = Math.atan2(y - spider.y,\nx - spider.x);\n\nvar vx = (Math.random() + 0.7) *\n4 * Math.cos(angle);\nvar vy = (Math.random() + 0.7) *\n4 * Math.sin(angle);\n\nspiderVelocity = {x:vx, y:vy};\n\nif (spiderVelocity.x < 0) {\nspider.scale.set(scale);\n} else {\nspider.scale.set(scale * -1, scale);\n}\n}``````\n\nAnd then I just update the spider with the given velocity."
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https://www.britannica.com/science/potential-energy/images-videos | [
"# Potential energy\n\nphysics\nMedia (4 Images and 3 Videos)",
null,
"Changes in potential and kinetic energy as a pendulum swings. (02:16)",
null,
"Conservation of energy (02:55) Explanation of the principle of the conservation of energy.",
null,
"Conservation of energy: proof (02:45) Learn how the lack of an “absolute” time implies the conservation of energy.",
null,
"Figure 5: Potential energy landscape. (A) Potential energy of a positive charge near a second positive charge. (B)…",
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"Figure 10: Potential energy for a positive charge (see text).",
null,
"Figure 2: The potential energy as a function of elongation of a fissioning nucleus. G is the ground state…",
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"Potential-energy curve. The activation energy represents the minimum amount of energy required to transform reactants into…\nVIEW MORE in these related Britannica articles:\n×\nBritannica Examines Earth's Greatest Challenges",
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https://physics.stackexchange.com/questions/278137/why-is-imposing-a-symmetry-on-a-theory-considered-more-natural-than-fine-tunin | [
"# Why is imposing a symmetry on a theory considered more “natural” than fine-tuning its couplings?\n\nTheories whose behavior would qualitatively change if their couplings were not fine-tuned to particular values are often dismissed as \"unnatural\" (in high-energy physics) or \"unrealistic\" (in condensed-matter physics), while theories whose couplings are constrained by symmetry requirements are happily accepted. Why is this? A symmetry constraint can be thought of as just a collection of fine-tunings that has some unifying pattern.\n\nFor example, a complex scalar field Lagrangian $$\\mathcal{L}_1 = \\partial_\\mu \\varphi^\\dagger \\partial^\\mu \\varphi - m^2 \\varphi^\\dagger \\varphi - \\lambda \\left( \\varphi^\\dagger \\right)^2 \\varphi^2 \\tag{1}$$ with a global $U(1)$-symmetry $$\\varphi \\to e^{i \\theta} \\varphi$$ can be thought of as a general Lagrangian $$\\mathcal{L}_2 = \\partial_\\mu \\varphi^\\dagger \\partial^\\mu \\varphi - m^2 \\varphi^\\dagger \\varphi - m'^2 \\left( \\left( \\varphi^\\dagger \\right)^2 + \\varphi^2 \\right) - \\lambda \\left( \\varphi^\\dagger \\right)^2 \\varphi^2 - \\lambda' \\left( \\left( \\varphi^\\dagger \\right)^4 + \\varphi^4 \\right) - \\dots\\tag{2}$$ in which the primed couplings have all been fine-tuned to zero. (Things are admittedly more complicated in the case of gauge quantum field theories, because in that case the gauge symmetry requires you to modify your quantization procedure as well). This kind of \"fine-tuning\" is a little less arbitrary than the usual kind, but arguably it's not much less arbitrary.\n\n• Fun fact, the second lagrangian is also \"fine-tuned\", due to the presence of the symmetry $\\varphi\\leftrightarrow\\varphi^\\dagger$. – Adam Sep 4 '16 at 8:53\n• Fine tuning requires order by order matching of loop corrections coming to m in terms of $\\lambda$ (which gets correction itself). A symmetry group which can handle a proper cancellation for both fermionic and bosonic loop to every order must show this symmetry. This strong condition requires odd graded elements in your symmetry algebra which requires an extension of symmetry to supersymmetry to avoid fine tuning. – ved Sep 4 '16 at 14:16\n• @Adam No, I think that symmetry comes from the requirement that the Lagrangian be real/the Hamiltonian be Hermitian. – tparker Sep 4 '16 at 16:53\n• @tparker: isn't that some fine tuning too ? ;-) – Adam Sep 4 '16 at 17:22\n• @Adam I would consider the unitarity of the theory to be a fundamental postulate of quantum mechanics, necessary for Born's probabilistic interpretation to make any sense. – tparker Sep 4 '16 at 17:57\n\n1. If one has a theory $S[\\alpha]$ that depends on some parameters $\\alpha$, one can always introduce new artificial parameters $\\beta$, and claim for free that the theory $S[\\alpha,\\beta]:=S[\\alpha]$ has a symmetry $\\beta\\to \\beta+ b$. This is of course not a very interesting symmetry.\n\n2. A symmetry, say $\\alpha \\to\\alpha + a$, is only interesting if different values of $\\alpha$ are physically meaningful/realizable/accessible. In contrast, if there is a physical principle/superselection rule that completely fix $\\alpha$ to a certain value, then we are essentially back to pt. 1.\n\n3. How do we quantify naturalness? It seems relevant to mention 't Hooft's definition of technical naturalness, cf. Refs. 1 & 2. At energy scale $\\mu$, two small parameters of the form $$m^{\\prime 2}~\\sim~ \\varepsilon^{\\prime} \\mu^2 , \\qquad \\lambda^{\\prime}~\\sim~ \\varepsilon^{\\prime}, \\qquad|\\varepsilon^{\\prime}|~\\ll~ 1,$$\nin the Lagrangian density $${\\cal L}_2~=~{\\cal L}_1 - m^{\\prime 2} \\left( \\left( \\varphi^{\\dagger} \\right)^2 + \\varphi^2 \\right) - \\lambda^{\\prime} \\left( \\left( \\varphi^{\\dagger} \\right)^4 + \\varphi^4 \\right)$$ is technical natural, since the replacement $\\varepsilon^{\\prime}=0$ would increase the symmetry of the system, namely it would restore the $U(1)$-symmetry $\\varphi \\to e^{i \\theta} \\varphi$, cf. the Lagrangian density ${\\cal L}_1$.\n\n4. Similarly, at energy scale $\\mu$, two small parameters of the form $$m^2~\\sim~ \\varepsilon \\mu^2 , \\qquad \\lambda ~\\sim~ \\varepsilon , \\qquad|\\varepsilon |~\\ll~ 1,$$\nin the Lagrangian density $${\\cal L}_1~=~ \\partial_{\\nu}\\varphi^{\\dagger} \\partial^{\\nu} \\varphi - m^2 \\varphi^{\\dagger} \\varphi - \\lambda \\left( \\varphi^{\\dagger} \\varphi \\right)^2$$ is technical natural, since the replacement $\\varepsilon=0$ would increase the symmetry of the system, namely it would restore the translation symmetry $\\varphi \\to \\varphi+a$.\n\nReferences:\n\n1. G. 't Hooft, Naturalness, Chiral Symmetry, and Spontaneous Chiral Symmetry Breaking, NATO ASI Series B59 (1980) 135. (PDF)\n\n2. P. Horava, Surprises with Nonrelativistic Naturalness, arXiv:1608.06287; p.2.\n\n• What do you think of fine-tuning/naturalness arguments in physics? – innisfree Sep 20 '16 at 14:33\n\nI would argue exactly the opposite : picking a symmetry requires much less fine-tuning.\n\nIndeed, when picking a symmetry, your are fine-tuning one \"parameter\", the fact that the model has a given symmetry, but effectively killing an infinite number of coupling in one sweep.\n\nOn the other end, standard fine-tuning forces you to put an infinite number of of coupling constants to zero. Since one is much smaller than infinity, I think that choosing a symmetry amounts to much less fine-tuning.\n\n• Well in field theories (other than ones that are being explicitly considered as effective theories with a known energy cutoff), we generally only consider renormalizable couplings, so fine-tuning actually only eliminates a finite number of couplings. I would argue that whether that finite number is \"much\" greater than one is largely a matter of opinion. – tparker Sep 4 '16 at 16:58\n• @tparker: you can require (old school) renormalizability, but that's not necessary for this discussion. Especially in a condensed matter context, where there are generically an infinite number of coupling constants (even in presence of symmetries). – Adam Sep 4 '16 at 17:25\n• In condensed matter, the microscopic lattice Hamiltonian may have an infinite number of couplings, but once you coarse-grain to a continuum theory all but a finite number are irrelevant under RG, so there are only a finite number of important couplings for explaining the low-energy physics. – tparker Sep 4 '16 at 18:01\n• @tparker: Not necessarily, if the system is not close to a fixed point (which is generically not the case, unless you fine tune the system ;-) ). And anyway, in a Wilsonian point of view, all (allowed) coupling constants are finite at a non-trivial fixed point. – Adam Sep 4 '16 at 18:10\n\nWhy is imposing a symmetry on a theory considered more “natural” than fine-tuning its couplings?\n\nTake a one carat diamond (200 milligrams ofcarbon). It can be described by a simple symmetry",
null,
"Unit cell of the diamond cubic crystal structure\n\nWhich is \"simpler\" : imagining the build up of the crystal by using the symmetry or listing all the (x,y,z,t) coordinates of the atoms, even the few ones in this unit cell?\n\nSymmetries \"simplify\" concepts. Even your argument about \"fine tuning of the primed couplings\" falls into the category of simplification. One does not have to impose it to each of them, the symmetry does it.\n\nI suppose if we were computers it would make no difference, but man is a pattern recognition animal, and finding patterns and repetitions of patterns is inherent in our tools of accumulation of knowledge, but this is outside physics.\n\n• How is fine-tuning related to a symmetric unit cell? – Statics Sep 4 '16 at 13:01\n• @Statics The \"discovery\" that a unit cell repeated described crystal symmetries is an analogue of symmetriew reducing fine tuning; if one sees the infinity coupling constants as uncorrelated as individual atom position might be seen as uncorrelated and needing individual determination of coordinate. It is an analogy. – anna v Sep 4 '16 at 13:53\n• I certainly agree that imposing a symmetry is simpler than fine-tuning many couplings in that you need to specify less information, but without explaining a physical mechanism that imposes the symmetry, it doesn't really seem much more natural to me. It just shifts the question from \"why are the couplings fine-tuned to certain values?\" to \"why do the couplings have this funny symmetry pattern?\" – tparker Sep 4 '16 at 17:03\n• @tparker Yes. You must have realized by now that ultimately physics does not answer \"why\" questions. Rather it answers \"why\" questions by pushing them to postulates and laws in as series of \"whys\". Naturalness is one of those traits, imo. It is, like Ocams razor, a preference we have as analyzers of nature. – anna v Sep 4 '16 at 17:24"
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https://scienceofdoom.com/2011/08/10/statistics-and-climate-%E2%80%93-part-four-%E2%80%93-autocorrelation/ | [
"Feeds:\nPosts\nComments\n\n## Statistics and Climate – Part Four – Autocorrelation\n\nIn Part Three we started looking at time-series that are autocorrelated, which means each value has a relationship to one or more previous values in the time-series. This is unlike the simple statistical models of independent events.\n\nAnd in Part Two we have seen how to test whether a sample comes from a population of a stated mean value. The ability to run this test is important and in Part Two the test took place for a population of independent events.\n\nThe theory that allows us to accept or reject hypotheses to a certain statistical significance does not work properly with serially correlated data (not without modification).\n\nHere is a nice example from Wilks:\n\nFigure 1\n\nRemember that (usually) with statistical test we don’t actually know the whole population – that’s what we want to find out about. Instead, we take a sample and attempt to find out information about the population.\n\nTake a look at figure 1 – the lighter short horizontal lines are the means (the “averages”) of a number of samples. If you compare the top and bottom graphs you see that the distribution of the means of samples is larger in the bottom graph. This bottom graph is the timeseries with autocorrelation.\n\nWhat this means is that if we take a sample from a time-series and apply the standard Student-t test to find out whether it came from a population of mean = μ, we will calculate that it didn’t come from a mean that it actually did come from too many times. So a 95% test will incorrectly reject the hypothesis a lot more than 5%.\n\nTo demonstrate this, here is the % of false rejections (“Type I errors”) as the autocorrelation parameter increases, when a standard Student-t test is applied:",
null,
"Figure 2\n\nThe test was done with Matlab, with a time-series population of 100,000, Gaussian (“normal distribution”) errors, and samples of 100 taken 10,000 times (in each case a random start point was chosen then the next 100 points were taken as a sample – this was repeated 10,000 times). When the time-series is generated with no serial correlation, the hypothesis test works just fine. As the autocorrelation increases (as we move to the right of the graph), the hypothesis test starts creating more false fails.\n\nWith AR(1) autocorrelation – the simplest model of autocorrelation – there is a simple correction that we can apply. This goes under different names like effective sample size and variance inflation factor.\n\nFor those who like details, instead of the standard deviation of the sample means:\n\ns = σ/√n\n\nwe derive:\n\ns = σ.√[(1+ρ)/n.(1-ρ)], where ρ = autocorrelation parameter.\n\nRepeating the same test with the adjusted value:",
null,
"Figure 3\n\nWe see that Type I errors start to get above our expected values at higher values of autocorrelation. (I’m not sure whether that actually happens with an infinite number of tests and true random samples).\n\nNote as well that the tests above were done using the known value of the autocorrelation parameter (this is like having secret information which we don’t normally have).\n\nSo I re-ran the tests using the derived autocorrelation parameter from the sample data (regressing the time-series against the same time-series with a one time step lag) – and got similar, but not identical results and apparently more false fails.\n\nCuriosity made me continue (tempered by the knowledge of the large time-wasting exercise I had previously engaged in because of a misplaced bracket in one equation), so I rewrote the Matlab program to allow me to test some ideas a little further. It was good to rewrite because I was also wondering whether having one (long) time-series generated with lots of tests against it was as good as repeatedly generating a time-series and carrying out lots of tests each time.\n\nSo this following comparison had a time-series population of 100,000 events, samples of 100 items for each test, repeated for 100 tests, then the time-series regenerated – and this done 100 times. So 10,000 tests across 100 different populations – first with the known autoregression parameter, then with the estimated value of this parameter from the sample in question:",
null,
"Figure 4 – Each sample size = 100\n\nThe correct value of rejected tests should be 5% no matter what the autoregression parameter.\n\nThe rewritten program allows us to test for the effect of sample size. The following graph uses the known value of autogression parameter in the test, a time-series population of 100,000, drawing samples out 1000 times from each population, and repeating through 10 populations in total:",
null,
"Figure 5 – Using known value of autoregression parameter in Student T-test\n\nRemembering that all of the lines should be horizontal on 5%, we can see that the largest sample population of 1000 is the most resistant to higher autoregression parameters.\n\nThis reminded me that the equation for the variance inflation factor (shown earlier) is in fact an approximation. The correct formula (for those who like to see such things):\n\nFigure 6\n\nSo I adjusted the variance inflation factor in the program and reran.\n\nI’m really starting to slow things down now – because in each single hypothesis test we are estimating the autoregression parameter, ρ, by a lag-1 correlation, then with this estimate we have to calculate the above circled formula, which requires summing the equation from 1 through to the number of samples. So in the case of n=1000 that’s 1000 calculations, all summed, then used in a Student-t test. And this is done in each case for 1000 tests per population x 10 populations.. thank goodness for Matlab which did it in 18 minutes. (And apologies to readers trying to follow the detail – in the graphics I show the autoregression parameter as φ, when I meant to use ρ, no idea why..)\n\nFortunately, the result turns out almost identical to using the approximation (the graph using the approximation is not shown):",
null,
"Figure 7 – Using estimated autoregression parameter\n\nSo unless I have made some kind of mistake (quite possible), I take this to mean that the sampling uncertainty in the autoregression parameter adds uncertainty to the Student T-test, which can’t be corrected for easily.\n\nWith large samples, like 1000, it appears to work just fine. With time-series data from the climate system we have to take what we can get and mostly it’s not 1000 points.\n\nWe are still considering a very basic model – AR(1) with normally-distributed noise.\n\nIn the next article I hope to cover some more complex models, as well as the results from this kind of significance test if we assume AR(1) with normally-distributed noise yet actually have a different model in operation..\n\n### References\n\nStatistical Methods in the Atmospheric Sciences, 3rd edition, Daniel Wilks, Academic Press (2011)\n\nTaking Serial Correlation into Account in Tests of the Mean, Zwiers & von Storch, Journal of Climate (1995)\n\n### 6 Responses\n\n1. on August 11, 2011 at 4:39 pm | Reply",
null,
"Carrick\n\nI could be mistaken, but I believe the breakdown in your analytic equations is do to a bias error in the estimation of the standard deviation that depends on N. (For large N your Monte Carlo results should converge asymptotically to the analytic formulae.) IMO, this is a good motivation for going away from the formulae in computing the confidence interval, and using a Monte Carlo based approach instead. That and with a Monte Carlo, you aren’t locked into normal distributions (or stationary noise, etc.)\n\nWikipedia’s article on error of the mean has a reference to Bence that relates to this, which I downloaded and briefly read over.\n\nJames R. Bence (1995) Analysis of short time series: Correcting for autocorrelation. Ecology 76(2): 628 – 639\n\nHe does similar comparisons to what you did. I didn’t look at the article closely to see how much agreement there was being your results and his, but it might be a good article to look at to track down the breakdown of the formal results for small N.\n\n• on August 14, 2011 at 9:12 am | Reply",
null,
"scienceofdoom\n\nThanks for the article – I’ve had a read and very interesting. I’ll try his revised calculation out. This is the “bias-corrected estimator suggested by Doran et al (1992)”.\n\nFor the standard deviation of the sample I am using the 1/(N-1) version, i.e. Bessel’s correction. In Matlab this is simply the function std().\n\n• on August 20, 2011 at 2:26 pm",
null,
"Carrick\n\nI was meaning to comment on this earlier and got side tracked by RL.\n\nTake home part:\n\nThe use of n − 1 instead of n in the formula for the sample variance is known as Bessel’s correction, which corrects the bias in the estimation of the sample variance, and some, but not all of the bias in the estimation of the sample standard deviation.\n\nThe problem arises because of taking the square-root of a random variable, and it is that which introduces the bias. Since the square-root is a “compressive nonlinearity”, that causes the square-root of an unbiased estimator of variance (Bessel’s variance) to be biased low.\n\nIt is this which leads to an underestimation of the true error of the mean, and in turn to a too-high of a false rejection rate.\n\n2. on August 13, 2011 at 1:20 am | Reply",
null,
"Jeff Id\n\nSOD,\n\nYou once wrote, why did the editor post an article at tAV? You may remember that it was an obviously confused individual with a post that would be shredded by the readers. I think you may have answered your own question with these baby step posts into stats.\n\nThe fun is in the puzzle and the intent is for clarity to those who don’t have the backgrounds to find it.\n\n3. on August 28, 2011 at 10:47 am | Reply",
null,
"Statistics and Climate – Part Five – AR(n) « The Science of Doom\n\n[…] the last article we saw some testing of the simplest autoregressive model AR(1). I still have an outstanding issue raised by one commenter relating to the hypothesis testing that was introduced, and I hope to come […]\n\n4. on May 15, 2014 at 6:19 am | Reply",
null,
"aura cacia oils\n\nI’ll right away snatch your rss as I can’t to find your e-mail subscription hyperlink or\nnewsletter service. Do you’ve any? Kindly allow me understand in order that\nI could subscribe. Thanks."
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.9278294,"math_prob":0.89404166,"size":9508,"snap":"2021-04-2021-17","text_gpt3_token_len":2057,"char_repetition_ratio":0.13425925,"word_repetition_ratio":0.0037151703,"special_character_ratio":0.2181321,"punctuation_ratio":0.08158765,"nsfw_num_words":1,"has_unicode_error":false,"math_prob_llama3":0.9853848,"pos_list":[0,1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22],"im_url_duplicate_count":[null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-04-14T07:56:14Z\",\"WARC-Record-ID\":\"<urn:uuid:1c671d21-5301-4e9e-81da-0afed724cb08>\",\"Content-Length\":\"129820\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:4905f52f-2c4a-46aa-9a86-518a6792e333>\",\"WARC-Concurrent-To\":\"<urn:uuid:dd73dfb3-a930-4069-ac97-4e20a3badae3>\",\"WARC-IP-Address\":\"192.0.78.25\",\"WARC-Target-URI\":\"https://scienceofdoom.com/2011/08/10/statistics-and-climate-%E2%80%93-part-four-%E2%80%93-autocorrelation/\",\"WARC-Payload-Digest\":\"sha1:FCVY35MJFTV5KCPYD3JLXPZN3X3PIB5Q\",\"WARC-Block-Digest\":\"sha1:TEHERKOBFR2CN5SEIZIYIUOR5KIIVAXK\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-17/CC-MAIN-2021-17_segments_1618038077336.28_warc_CC-MAIN-20210414064832-20210414094832-00369.warc.gz\"}"} |
http://www.bondeconomics.com/2017/09/calculating-initial-steady-state-in.html | [
"## Wednesday, September 6, 2017\n\n### Calculating An Initial Steady State In sfc_models\n\nOne typical task in SFC modelling is examining the effect of a policy change. We assume that a model starts in a steady state at k=0, the policy change hits at some later time, and we then examine the solution. This yields more plausible scenarios than starting with stock variables equal to zero. However, the difficulty with this task is that we need to set the initial conditions of the variables to equal the initial steady state.\n\nThis article is an unedited excerpt from my manuscript on stock-flow consistent (SFC) modelling in Python. It describes how the sfc_models framework determines an initial steady state for a model. For readers who are unfamiliar with the notion of the steady state within the context of SFC models, I have this primer on the concepts of steady state and equilibrium.\n\nDetermining the initial steady state is particularly difficult if there are multiple types of financial assets within the model. All need to be set at levels that match asset allocation functions, and we must ensure that all balance sheets balance. (At present, the framework does not attempt to force balance sheets into balance; unbalanced initial conditions result in the creation of “ghost asset balances” that are implied but not explicitly held within the model.)\n\nThe EquationSolver class has the capacity to solve for an initial steady state (if it exists). By setting ParameterSolveInitialSteadyState to True, the solver will starts a new simulation, starting at k=-200 (by default), and then simulating from that point until k=0. The solver will then restart from k=0 from that steady state value normally. (The starting time is set by ParameterInitialSteadyStateMaxTime, which has a default of 200.)\n\nImportantly, if this option is chosen, the initial conditions are applied to the starting state in negative time; the values at k=0 are just the calculated steady state values. By default, all financial stock variables start at zero, and therefore balance sheets balance. Therefore, the resulting steady state (if it exists) will obey accounting rules. (If the user hardcodes an initial condition, it is up to the user to validate that accounting consistency holds.) It is not possible to solve for a steady state and then specify different initial conditions for k=0. That is, you would not be able to apply a shock to the steady state until k=1.\n\nIt would be more elegant to solve for the steady state explicitly (as is done in the text Monetary Economics by Godley and Lavoie). In principle, it looks straightforward: we just leave the equations unchanged, except for lag conditions: in a steady state, x[k-1] = x[k]. That is, we replace lag relationships with an equality. However, when this was tested for simple models, there was no convergence to a solution. It is a future research project to re-examine this, and see whether it is possible to solve for the steady state in this fashion.\n\nThe framework currently supports the notion of a constant steady state: (almost) all variables are assumed to converge to constant values. (Exceptions are discussed below.) Presumably, we need exogenous variables to be constant as well. As a result, we use the value of exogenous variables at k=0 for all negative times. This technique will not work for variables that are viewed as “exogenous” from the point of view of economics, but are not explicitly defined as such. For example, we might think of government consumption as exogenous, and we want to see what happens if it increases linearly. If we specify spending as a function (for example, G = 20 * k) government spending will be calculated as such during negative time. As a result, we would not expect a steady state solution to exist. However, if we define G as an exogenous variable, equal to a Python list ([0.0, 20.0, 40.0, …]), the government spending will be held flat at 0 for all negative time. If you want to avoid using a list, you could define the variable to be equal to a custom function (Section 7.3). You just need to ensure that the custom function returns a constant value for negative time values.\n\nIn this case, we could use:\n\ndef gov_spending(k):\n\"\"\"\nGovernment spending function that respects negative time.\n\"\"\"\nif k < 0:\n# We are in the initial steady state calculation\nreturn 0.0\nelse:\nreturn 20.0*k\n\nThe calculated time series are associated with the ‘steadystate_0’ log, which is output to the “_steadystate.txt” log when RegisterStandardLogs (Section 3.3) is called. These series will need to be examined to see which ones do not reach steady state if the framework throws an error when trying to calculate the steady state.\n\nThe framework just looks at the last values, to see whether they are (roughly) constant. The criterion may be changed in the future; it presently just looks at the last two value, and checks whether the percentage change is less than ParameterInitialSteadyStateErrorToler (default is now 1e-4). The exception is when the last value is small in absolute terms (hardcoded threshold of 1e-4). In this case, the algorithm just validates that the previous value has a similarly low absolute value. This needs to be done, as series that are close to zero can have quite large percentage changes when solved numerically.\n\nHowever, some variables are expected to change, even in a steady state. The most obvious example being the custom time axis t. (Within sfc_models, there are two variables associated with the time axis; the discrete time k which always matches the iteration step number, and the custom time axis which can be a function of k. This allows us to define a time axis that goes up by 0.25 increments to match quarterly data, while still having access to the current time step.) The parameter ParameterInitialSteadyStateExcludedVariables is a parameter that is a list of variables to exclude (by default, just 't'). (The time axis k is always excluded.) The user can add more variables to exclude in order to proceed to solving in positive time.\n\nA planned extension will be to allow a “steady state” where variables are growing at a steady rate. Unfortunately, the growth rate of variables depends upon the variables’ classification. For example, nominal variables will grow at a nominal growth rate, real variables at a real growth rate, and price variables the rate of inflation. Meanwhile, parameters will still be constants, with a nominal growth rate of zero. The complexity of determining whether the solution is a legitimate steady state explains why this implementation has been pushed back.\n\n(c) Brian Romanchuk 2017"
]
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.9025418,"math_prob":0.9658034,"size":6880,"snap":"2020-34-2020-40","text_gpt3_token_len":1465,"char_repetition_ratio":0.12579988,"word_repetition_ratio":0.005291005,"special_character_ratio":0.20901163,"punctuation_ratio":0.11008468,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.97542524,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-09-27T09:53:31Z\",\"WARC-Record-ID\":\"<urn:uuid:c28e1f0b-0719-4f9d-b553-48e216e26964>\",\"Content-Length\":\"105070\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:cc81e656-778e-4a2f-abfd-00521860b693>\",\"WARC-Concurrent-To\":\"<urn:uuid:2d11a110-f913-4698-b495-2a6751d3395f>\",\"WARC-IP-Address\":\"172.217.2.115\",\"WARC-Target-URI\":\"http://www.bondeconomics.com/2017/09/calculating-initial-steady-state-in.html\",\"WARC-Payload-Digest\":\"sha1:LFYMOXCRG35A7HVDGPUKI2MRTGXKY7TH\",\"WARC-Block-Digest\":\"sha1:3KZWSUBO55UH3ZOFFEKDVJB3SMGL35DP\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-40/CC-MAIN-2020-40_segments_1600400274441.60_warc_CC-MAIN-20200927085848-20200927115848-00660.warc.gz\"}"} |
https://tw.dictionary.search.yahoo.com/search?p=calculate&nojs=1&ei=UTF-8&context=gsmcontext%3A%3Alimlangpair%3A%3Aen_en | [
"# Yahoo奇摩字典 網頁搜尋\n\n### calculate\n\n• IPA[ˈkalkyəˌlāt]\n\n美式\n\n• determine (the amount or number of something) mathematically;determine by reasoning, experience, or common sense; reckon or judge\n\n• 釋義\n• 相關詞\n\n### 動詞\n\n• 1. determine (the amount or number of something) mathematically Japanese land value was calculated at 2.5 times that of the U.S he calculated that Texas would gain four new seats in the House of Representatives 同義詞\n• determine by reasoning, experience, or common sense; reckon or judge I was bright enough to calculate that she had been on vacation\n• include as an essential element in one's plans he may have calculated on maximizing pressure for policy revision 同義詞 rely, ... 更多\n• 2. intend (an action) to have a particular effect his last words were calculated to wound her 同義詞\n• 3. US dialect suppose or believe.\n\n### calculated\n\n• (of an action) done with full awareness of the likely consequences: victims of vicious and calculated assaults a calculated decision\n\n### calculating\n\n• acting in a scheming and ruthlessly determined way: he was a coolly calculating, ruthless man\n\n### calculated\n\n• (of an action) done with full awareness of the likely consequences: victims of vicious and calculated assaults\n\n### calculating\n\n• acting in a scheming and ruthlessly determined way: he was a coolly calculating, ruthless man\n\n• 更多解釋\n\n### calculate\n\n• IPA[ˈkalkjʊleɪt]\n\n英式\n\n• determine (the amount or number of something) mathematically: the program can calculate the number of words that will fit in the space available local authorities have calculated that full training would cost around £5,000 per teacher\n\n2. ### 知識+\n\n• #### calculate和count有何差別?用法時機為何?\n\n...一個蠻有難度的問題 本人意見如下 1.兩者雖然都有計算的意義 但calculate它還有事前估算的意義count則否 也就是說calculate應比count更有縝密之...網站上計算 瀏覽人數的東東 叫counter不叫caculator 由這可體會count與calculate之差別\n\n• #### Calculated risks怎麼翻成什麼比較好?\n\nCALCULATED RISK 計畫風險 在評估過可能的影響之後,採取或被接受去完成特殊目的的一種行為。計畫風險(時常被稱為殘餘風險)是在計畫性作業經周詳考量後,可以接受風險稱之計畫風險。\n\n• #### [英翻中] to Calculate the First and Last Day of the Month?\n\n[英翻中] to Calculate the First and Last Day of the Month (X..."
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.8747744,"math_prob":0.9510156,"size":2164,"snap":"2020-45-2020-50","text_gpt3_token_len":765,"char_repetition_ratio":0.14675926,"word_repetition_ratio":0.2724359,"special_character_ratio":0.19547135,"punctuation_ratio":0.12112676,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.96703756,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-10-23T01:01:59Z\",\"WARC-Record-ID\":\"<urn:uuid:a944c160-4765-4f62-b934-e79b9dbd4bc5>\",\"Content-Length\":\"58119\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:c7b381e7-5278-4496-92fb-2b5e358cbfcf>\",\"WARC-Concurrent-To\":\"<urn:uuid:db49b4e1-3f29-4435-a53a-3eb14c2f19c5>\",\"WARC-IP-Address\":\"66.218.84.137\",\"WARC-Target-URI\":\"https://tw.dictionary.search.yahoo.com/search?p=calculate&nojs=1&ei=UTF-8&context=gsmcontext%3A%3Alimlangpair%3A%3Aen_en\",\"WARC-Payload-Digest\":\"sha1:BYBLVNG5KO635RSMFCPV7KVBMZCN56UF\",\"WARC-Block-Digest\":\"sha1:7EOUBBMIFLIEWQ6Q64GLV3IWZO7R7YL6\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-45/CC-MAIN-2020-45_segments_1603107880401.35_warc_CC-MAIN-20201022225046-20201023015046-00679.warc.gz\"}"} |
https://socratic.org/questions/a-model-train-with-a-mass-of-6-kg-is-moving-on-a-circular-track-with-a-radius-of-6 | [
"# A model train, with a mass of 6 kg, is moving on a circular track with a radius of 7 m. If the train's rate of revolution changes from 4 Hz to 2 Hz, by how much will the centripetal force applied by the tracks change by?\n\nJun 15, 2017\n\nThe centripetal force changes by $= 6632.4 N$\n\n#### Explanation:\n\nThe centripetal force is\n\n$F = m r {\\omega}^{2}$\n\nThe mass is $m = 6 k g$\n\nThe radius $r = 7 m$\n\nThe change in the angular velocity is\n\n$\\Delta \\omega = \\left(4 - 2\\right) \\cdot 2 \\pi = \\left(4 \\pi\\right) r a {\\mathrm{ds}}^{-} 1$\n\nThe variation in centripetal force is\n\n$\\Delta F = m r {\\left(\\Delta \\omega\\right)}^{2}$\n\n$= 6 \\cdot 7 \\cdot {\\left(4 \\pi\\right)}^{2}$\n\n$= 6632.4 N$"
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http://talkstats.com/threads/normal-distribution-help.2149/ | [
"# Normal Distribution Help\n\n#### Bishop\n\n##### New Member\nQuestion:\nThe probability that a person has an unlisted telephone number is 0.15. The district manager of a political action group is phoning people urging them to vote. In a district with 416 households, all households have phones. What is the probability that the district manger will find that:\n\n(a) 50 or fewer households in the district will have unlisted numbers?\n\nI'm having trouble finding out what to do here because there is no standard deviation or means they supply with the problem. This is what I did so far using the normal approximation to the binomial distribution. I'm not sure if I'm using the right formula to calculate this problem.\n\npopulation means = n*p and o(standard deviation)= square root n*p*q\n\nX<=50\nN = 50 P = .15\nU = np = 50(.15) = 7.5\nStd dev = sqrt50(.15)(.85) = 2.52\nAnswer: 50-7.5/2.52 = 16.87\n\nLast edited:\n\n#### vinaitheerthan\n\n##### New Member\nHi,\n\nHere n should be 416 not 50 and your p=0.15 and q = 0.85\nyou will have to calculate the probability\nP(x <= 50)\n\nRegards,\nRe.Vinaitheerthan\n\n#### Bishop\n\n##### New Member\nthank you",
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https://www.rdocumentation.org/packages/spatstat/versions/1.29-0/topics/rotate.owin | [
"# rotate.owin\n\n0th\n\nPercentile\n\nRotates a window\n\nKeywords\nspatial, math\n##### Usage\n## S3 method for class 'owin':\nrotate(X, angle=pi/2, \\dots, rescue=TRUE)\n##### Arguments\nX\nA window (object of class \"owin\").\nangle\nAngle of rotation.\nrescue\nLogical. If TRUE, the rotated window will be processed by rescue.rectangle.\n...\nOptional arguments passed to as.mask controlling the resolution of the rotated window, if X is a binary pixel mask. Ignored if X is not a binary mask.\n##### Details\n\nRotates the window by the specified angle. Angles are measured in radians, anticlockwise. The default is to rotate the window 90 degrees anticlockwise. The centre of rotation is the origin.\n\n##### Value\n\n• Another object of class \"owin\" representing the rotated window.\n\nowin.object\n\n• rotate.owin\n##### Examples\nw <- owin(c(0,1),c(0,1))\nv <- rotate(w, pi/3)\nplot(v)\ndata(letterR)\nv <- rotate(w, pi/5)"
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https://smallsats.org/2013/03/24/fundamental-constants/ | [
"Home » Useful Engineering » Fundamental constants\n\n# Fundamental constants\n\n```c = 2.9979E8; %[m/s] Speed of light\nmu0 = 4*pi*1E-7; %[V*s/(A*m)] Permeability\neps0 = 8.8542E-12; %[A*s/(V*m)] Permittivity\nG = 6.672E11; %[N*m2/kg2] Gravitation constant\nme = 9.109E-31; %[kg] Electron rest mass\nmp = 1.673E-27; %[kg] Proton rest mass\ne = 1.602E-19; %[C] Elementary charge\nk = 1.381E-23; %[J/K] Boltzmann constant\nh = 6.626E-34; %[J*s] Planck’s constant\nMe = 5.98E24; %[kg] Earth’s mass\nRe = 6.37E6; %[m] Earth’s radius\nMs = 1.989E30; %[kg] Solar mass\nRs = 6.966E8; %[m] Solar radius\nMd = 8E15; %[T*m3] Earth’s magnetic dipole moment\nR = 1.985E-3; %[kcal/(mole*K)]Gas constant```"
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http://arcmaildefenderaws.com/books/analysis-leicht-gemacht | [
"# Read e-book online Analysis leicht gemacht PDF",
null,
"By Silvanus P. Thompson\n\nISBN-10: 3871447390\n\nISBN-13: 9783871447396\n\nBest analysis books\n\nAlan Agresti(auth.)'s Analysis of Ordinal Categorical Data, Second Edition PDF\n\nStatistical science’s first coordinated guide of equipment for interpreting ordered express info, now absolutely revised and up to date, keeps to give purposes and case experiences in fields as diversified as sociology, public well-being, ecology, advertising, and pharmacy. research of Ordinal express information, moment version presents an creation to simple descriptive and inferential equipment for express information, giving thorough assurance of recent advancements and up to date tools.\n\nDownload e-book for iPad: The Capitalistic Cost-Benefit Structure of Money: An by Dieter Suhr\n\nThis examine is worried with the widely used challenge of the switch that's prompted whilst funds enters into the financial system. way back to Aristotle (Politics, pp. 1135-1143) the still-unanswered query concerning the dichotomy of the real-exchange and the financial economic system was once raised. He contrasted Oeconomic, the place humans try to procure genuine utilities (household management), to Chrematistic, the place they use funds to make more cash (art of wealth-acquisition): the real wealth involves such values in use; for the volume of ownership of this sort, in a position to making existence friendly, isn't really limitless.\n\nExtra resources for Analysis leicht gemacht\n\nSample text\n\nThe prefix 'iso' means same in Greek. Today an isoperimetric inequality refers to an inequality obtained when we optimize some domain dependent functional keeping some geometric parameter (like the measure, for instance) of the domain fixed. 1) are available. We refer the reader to the survey article of [Osserman (1978)] for a nice proof. The inequality can also easily be proved using Fourier series. We will defer a proof of this inequality to later in this section, when we will give a simple proof (at least for smooth domains) in all space dimensions.\n\nWe now prove another particular case of the co-area formula. 2 Let Q C RN be an open set and let u £ £>(fi). 9) J where M = max a . G ^u(x). 10) Proof: Step 1. Since u is smooth, by Sard's thoerem, for almost every t in the range of u, we have that |Vu| ^ 0 on the level set {« = £}. Thus, {u = t} will be an (N — 1) - dimensional surface and, further {u = t} = d{u > t). Also, \\{u* = t}\\ = |{w = t}| = 0. Step 2. Let 2 < p < oo. Define f = -div{\\Vu\\p~2Vu). Vvdx Jo, = J fvdx. 11) Let t > 0. Set v = (u-1)+ € WQ'P{Q).\n\nFinally, we consider the rearrangement u* of u. Let R be the radius of Q*. Let us write (by abuse of notation) u*(x) = u*(\\x\\) and thus consider it as a function of a single variable, for convenience. dx = / * \\u*'(r)\\pNu>NrN-1dr = Jo* \\u*' {r^N^r\"'1^™*' (r))dr"
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"https://images-na.ssl-images-amazon.com/images/I/51jRcjNzDXL._SX351_BO1,204,203,200_.jpg",
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https://encyclopediaofmath.org/wiki/Birkhoff-Witt_theorem | [
"# Birkhoff-Witt theorem\n\nPoincaré–Birkhoff–Witt theorem\n\nA theorem about the representability of Lie algebras in associative algebras. Let $G$ be a Lie algebra over a field $k$, let $U(G)$ be its universal enveloping algebra, and let $B = \\{ {b _ {i} } : {i \\in I } \\}$ be a basis of the algebra $G$ which is totally ordered in some way. All the possible finite products $b _ {\\alpha _ {1} } \\dots b _ {\\alpha _ {r} }$, where $\\alpha _ {1} \\leq \\dots \\leq \\alpha _ {r}$, then form a basis of the algebra $U(G)$, and it thus follows that the canonical homomorphism $G \\rightarrow U(G)$ is a monomorphism.\n\nIt is possible to construct a Lie algebra $L(R)$ for any associative algebra $R$ by replacing the operation of multiplication in $R$ with the commutator operation\n\n$$[xy] = xy - yx .$$\n\nThe Birkhoff–Witt theorem is sometimes formulated as follows: For any Lie algebra $G$ over any field $k$ there exists an associative algebra $R$ over this field such that $G$ is isomorphically imbeddable in $L(R)$.\n\nThe first variant of this theorem was obtained by H. Poincaré ; the theorem was subsequently completely demonstrated by E. Witt and G.D. Birkhoff . The theorem remains valid if $k$ is a principal ideal domain , in particular for Lie rings without operators, i.e. over $\\mathbf Z$, but in the general case of Lie algebras over an arbitrary domain of operators the theorem is not valid .\n\nHow to Cite This Entry:\nBirkhoff-Witt theorem. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Birkhoff-Witt_theorem&oldid=46072\nThis article was adapted from an original article by T.S. Fofanova (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article"
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https://www.pinayhomeschooler.com/2018/02/montessori-addition-and-subtraction-of.html | [
"## Friday, February 2, 2018\n\nSharing some updates with regard to my elementary boy. Though it may seem that I’m posting a lot about preschool activities, in the background my 9 years old is doing a lot of work too in math, geography/history, and science. Now, one of the things he worked on last year was his fractions. After working fractions and fraction equivalence, Mavi worked on addition and subtraction of fractions. He did very well on this. With one simple presentation, he grasped the concept right away, and after which he did a lot of practise using our fraction cut-outs. Somehow, I find this straightforward, meaning if your child knows about their basic addition and subtraction they can breezily work on this and move on to multiplication of fractions or working with unlike fractions.\n\n## Addition and Subtraction with Same Denominator\n\nNote that you only work on this once the child has a good grasp of the basic concept of fractions.\n\n1. Using the ticket, take three 1/6 cut-outs and say “This is three 1/6 or 3/6”.\n2. Place two 1/6 and place them next (to the right) of the 3/6 and explain that you need to add all the fraction cut-outs. Place the addition sign (or just write this on paper) in between the two fraction cut-outs to form the equation.\n3. Combine the two groups of fraction cut-outs, and count the total fraction cut-outs. Say 3/6 plus 2/6 is (or equals) 5/6.\n4. You can reduce the sum to it’s equivalence. In our case 5/6 is already in its reduced form.\n\n### Subtraction:\n\n1. Place five 1/8 cut-outs and have the child take away two 1/8 cut-outs. For the sake of presentation, Mavi showed me what’s 2/8 thus, he placed two 1/8 cut-outs on the rug on the right of the first set of fraction (5/8). Place a minus symbol or you can just write it in a piece of paper instead\n2. Once you have removed two 1/8 cut-outs from the first fraction, ask the child what’s left. Reduce the fraction if needed.\nNOTE: In most homeschool and Montessori schools, they write tickets and place them underneath the fraction (see a sample of it here). We didn’t do this at home because Mavi used the answer sheets in our Fraction printable instead.\n\n## Mixed Fractions\n\nThis is the case when the sum is more than one whole. For example, in 3/4 + 2/4 = 5/4, Mavi replaced the 4/4 with 1 to reduce the fraction to 1 and 1/4. The same happens to the second set of equation, replacing the answer to 1 and 4/10.\n\n## Subtraction involving Whole Numbers\n\nNow when you encounter a problem like this, the first thing to do is to convert the whole number to its equivalent fraction. In the first equation, we replaced 1 whole to four 1/4 cut-outs, and removed two 1/4 cut-outs from it.\n\nSimilarly, replace 1 in 1 and 4/7 to seven 1/7 cut-outs so you can subtract six 1/7 cut-outs from the total number of 1/7 cut-outs in the equation.\n\nThe method of using fraction cut-outs is undeniably effective in making the child understand how to manipulate fractions by using concrete materials. Through first hand experience of how these fractions work, how they are added and subtracted, the child can easily retain the concepts of fraction operations. And they can easily master reducing fractions as the cut-outs can provide a visual demonstration of the operation. We worked on these materials for two months (since December)and just last week Mavi started abstract work (working with worksheets). This is the second series of my elementary fraction posts (see first part here - Hands-on Learning of Equivalent Fractions), and hopefully we’ll get to work on other equations too so I can share them with you.\n\nMore learning materials at Pinay Homeschooler Shop."
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https://tex.stackexchange.com/questions/130586/vim-nice-folding-function | [
"# vim: nice folding function\n\nI use Latex-Box but I really like vim-latex (a.k.a Latex-Suite) folding. I tried to copy Latex-Suite's folding.vim file to my ftplugin/tex folder but cannot make it work. Has anyone written a nice folding function or uses Latex-Suite one without Latex-Suite full plugin?\n\n• I use Latex-Suite pretty much only for the folding, so I would really like to see an answer. – Kallus Aug 29 '13 at 2:26\n• Untested: You could install latex-suite and then edit ftplugin/latex-suite/main.vim and start deleting stuff from line 810 onwards (except, of course, line 824 that sources folding.vim). – Aditya Aug 29 '13 at 2:55\n\nI've modified Latex-Box (excellent) folding in two ways: i) since I only like to fold sections (parts, chapters, etc), the abstract environment and frames (in beamer class) I've added a new variable g:LatexBox_folded_environments that controls which environments are folded ii) I changed the LatexBox_FoldText() to resemble Latex-Suite.\n\nYou should save this file as ftplugin/tex/folding.vim and it should work out of the box.\n\n\" Initialization {{{\n\nfinish\nendif\n\n\" }}}\n\" Set options {{{\n\nsetlocal foldmethod=expr\nsetlocal foldexpr=LatexBox_FoldLevel(v:lnum)\nsetlocal foldtext=LatexBox_FoldText()\n\nif !exists('g:LatexBox_fold_preamble')\nlet g:LatexBox_fold_preamble=1\nendif\n\nif !exists('g:LatexBox_fold_parts')\nlet g:LatexBox_fold_parts=[\n\\ \"appendix\",\n\\ \"frontmatter\",\n\\ \"mainmatter\",\n\\ \"backmatter\"\n\\ ]\nendif\n\nif !exists('g:LatexBox_fold_sections')\nlet g:LatexBox_fold_sections=[\n\\ \"part\",\n\\ \"chapter\",\n\\ \"section\",\n\\ \"subsection\",\n\\ \"subsubsection\"\n\\ ]\nendif\n\nif !exists('g:LatexBox_fold_envs')\nlet g:LatexBox_fold_envs=1\nendif\nif !exists('g:LatexBox_folded_environments')\nlet g:LatexBox_folded_environments = [\n\\ \"abstract\",\n\\ \"frame\"\n\\ ]\nendif\n\n\" }}}\n\" LatexBox_FoldLevel helper functions {{{\n\n\" This function parses the tex file to find the sections that are to be folded\n\" and their levels, and then predefines the patterns for optimized folding.\nfunction! s:FoldSectionLevels()\n\" Initialize\nlet level = 1\nlet foldsections = []\n\n\" If we use two or more of the *matter commands, we need one more foldlevel\nlet nparts = 0\nfor part in g:LatexBox_fold_parts\nlet i = 1\nwhile i < line(\"$\") if getline(i) =~ '^\\s*\\\\' . part . '\\>' let nparts += 1 break endif let i += 1 endwhile if nparts > 1 let level = 2 break endif endfor \" Combine sections and levels, but ignore unused section commands: If we \" don't use the part command, then chapter should have the highest \" level. If we don't use the chapter command, then section should be the \" highest level. And so on. let ignore = 1 for part in g:LatexBox_fold_sections \" For each part, check if it is used in the file. We start adding the \" part patterns to the fold sections array whenever we find one. let partpattern = '^\\s*$$\\\\\\|% Fake$$' . part . '\\>' if ignore let i = 1 while i < line(\"$\")\nif getline(i) =~# partpattern\ncall insert(foldsections, [partpattern, level])\nlet level += 1\nlet ignore = 0\nbreak\nendif\nlet i += 1\nendwhile\nelse\ncall insert(foldsections, [partpattern, level])\nlet level += 1\nendif\nendfor\n\nreturn foldsections\nendfunction\n\n\" }}}\n\" LatexBox_FoldLevel {{{\n\n\" Parse file to dynamically set the sectioning fold levels\nlet b:LatexBox_FoldSections = s:FoldSectionLevels()\n\n\" Optimize by predefine common patterns\nlet s:foldparts = '^\\s*\\\\\\%(' . join(g:LatexBox_fold_parts, '\\|') . '\\)'\nlet s:folded = '$$% Fake\\|\\\\\\(document\\|begin\\|end\\|' \\ . 'front\\|main\\|back\\|app\\|sub\\|section\\|chapter\\|part$$\\)'\n\n\" Fold certain selected environments\nlet s:notbslash = '\\%(\\\\\\@<!\\%(\\\\\\\\\\)*\\)\\@<='\nlet s:notcomment = '\\%(\\%(\\\\\\@<!\\%(\\\\\\\\\\)*\\)\\@<=%.*\\)\\@<!'\nlet s:envbeginpattern = s:notcomment . s:notbslash .\n\\ '\\\\begin\\s*{$$'. join(g:LatexBox_folded_environments, '\\|') .'$$}'\nlet s:envendpattern = s:notcomment . s:notbslash .\n\\ '\\\\end\\s*{$$'. join(g:LatexBox_folded_environments, '\\|') . '$$}'\n\nfunction! LatexBox_FoldLevel(lnum)\n\" Check for normal lines first (optimization)\nlet line = getline(a:lnum)\nif line !~ s:folded\nreturn \"=\"\nendif\n\n\" Fold preamble\nif g:LatexBox_fold_preamble == 1\nif line =~# '\\s*\\\\documentclass'\nreturn \">1\"\nelseif line =~# '^\\s*\\\\begin\\s*{\\s*document\\s*}'\nreturn \"0\"\nendif\nendif\n\n\" Fold parts (\\frontmatter, \\mainmatter, \\backmatter, and \\appendix)\nif line =~# s:foldparts\nreturn \">1\"\nendif\n\n\" Fold chapters and sections\nfor [part, level] in b:LatexBox_FoldSections\nif line =~# part\nreturn \">\" . level\nendif\nendfor\n\n\" Fold environments\nif g:LatexBox_fold_envs == 1\nif line =~# s:envbeginpattern\nreturn \"a1\"\nelseif line =~# '^\\s*\\\\end{document}'\n\" Never fold \\end{document}\nreturn 0\nelseif line =~# s:envendpattern\nreturn \"s1\"\nendif\nendif\n\n\" Return foldlevel of previous line\nreturn \"=\"\nendfunction\n\n\" }}}\n\" LatexBox_FoldText helper functions {{{\n\nfunction! s:CaptionFrame(line)\n\" Test simple variants first\nlet caption1 = matchstr(a:line,'\\\\begin\\*\\?{.*}{\\zs.\\+\\ze}')\nlet caption2 = matchstr(a:line,'\\\\begin\\*\\?{.*}{\\zs.\\+')\n\nif len(caption1) > 0\nreturn caption1\nelseif len(caption2) > 0\nreturn caption2\nelse\nlet i = v:foldstart\nwhile i <= v:foldend\nif getline(i) =~ '^\\s*\\\\frametitle'\nreturn matchstr(getline(i),\n\\ '^\\s*\\\\frametitle$$$.*$$$\\?{\\zs.\\+')\nend\nlet i += 1\nendwhile\n\nreturn \"\"\nendif\nendfunction\n\n\" }}}\n\" LatexBox_FoldText {{{\n\nfunction! LatexBox_FoldText()\n\" Initialize\nlet line = getline(v:foldstart)\nlet nlines = v:foldend - v:foldstart + 1\nlet level = ''\nlet title = 'Not defined'\n\n\" Fold level and number of lines\nlet level = '+-' . repeat('-', v:foldlevel-1) . ' '\nlet alignlnr = repeat(' ', 6-(v:foldlevel-1)-len(nlines))\nlet lineinfo = nlines . ' lines: '\n\n\" Preamble\nif line =~ '\\s*\\\\documentclass'\nlet title = \"Preamble\"\nendif\n\n\" Parts, sections and fakesections\nlet sections = '$$\\(sub$$*section\\|part\\|chapter\\)'\nlet secpat1 = '^\\s*\\\\' . sections . '\\*\\?\\s*{'\nlet secpat2 = '^\\s*\\\\' . sections . '\\*\\?\\s*$' if line =~ '\\\\frontmatter' let title = \"Frontmatter\" elseif line =~ '\\\\mainmatter' let title = \"Mainmatter\" elseif line =~ '\\\\backmatter' let title = \"Backmatter\" elseif line =~ '\\\\appendix' let title = \"Appendix\" elseif line =~ secpat1 . '.*}' let title = line elseif line =~ secpat1 let title = line elseif line =~ secpat2 . '.*$'\nlet title = line\nelseif line =~ secpat2\nlet title = line\nelseif line =~ 'Fake' . sections . ':'\nlet title = matchstr(line,'Fake' . sections . ':\\s*\\zs.*')\nelseif line =~ 'Fake' . sections\nlet title = matchstr(line, 'Fake' . sections)\nendif\n\n\" Environments\nif line =~ '\\\\begin'\n\" Capture environment name\nlet env = matchstr(line,'\\\\begin\\*\\?{\\zs\\w*\\*\\?\\ze}')\nif env == 'abstract'\nlet title = 'Abstract'\nelseif env == 'frame'\nlet caption = s:CaptionFrame(line)\nlet title = 'Frame - ' . substitute(caption, '}\\s*\\$', '','')\nendif\nendif\n\nreturn level . alignlnr . lineinfo . title . ' '\nendfunction\n\n\" }}}\n\n\nIf you want to fold figures, tables and other environments you should add the functions LabelEnv(), CaptionEnv() and CaptionTable() from LaTeX-Box/ftplugin/latex-box/folding.vim and modify the LatexBox_FoldText() function to include the mentioned functions as its done in Latex-Box folding (but changing the format to the format that suits your needs).\n\n• Works like a charm (even in 2017 ;)). Why don't you put it in a tiny github repo like latex-folding.vim? EDIT: ok, there is already github.com/matze/vim-tex-fold – bijancn Feb 20 '17 at 13:23\n• @bijancn That github folding isn't that good. – Mahbub Alam Mar 12 '18 at 16:37\n• Hey, @petobens I was thinking of uploading .vimrc and related files to GitHub. May I upload your folding as well mentioning that its yours? I'll provide a link to your answer here, if you allow. – Mahbub Alam May 30 '18 at 0:04\n• Go ahead. I have it already on Github: github.com/petobens/dotfiles/blob/master/vim/ftplugin/tex/… – petobens Jun 8 '18 at 17:15\n• I have lots of keybindings in vim for latex, and when I use this folding method it takes much longer to load any keybinding. After I removed this folding method it was working fine. I am also not sure whether this folding method is what's causing this problem, but it does go away if I remove this. – Mahbub Alam Oct 31 '18 at 0:10"
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https://byjus.com/question-answer/the-intensity-of-sound-from-a-point-source-is-1-0-times-10-6-m-1/ | [
"",
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"",
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"Question\n\n# The intensity of sound from a point source is 1.0 × 10−6m−2 at a distance of 5.0 m from the source. What will be the intensity at a distance of 25 m from the source?",
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"",
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"",
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"Solution\n\n## The correct option is A",
null,
"The power of the sound wave is intensity × surface area power =1 × 108 × 4π × 25 =100π 10−8 = 10−6π W Intensity at 25m =powersurfacearea =10−6π4π(25)2 =10−6625 × 4 =10−62500 =0.04 × 10−8 Wm−2",
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"",
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"Suggest corrections",
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"data:image/svg+xml;base64,PHN2ZyB3aWR0aD0iNDQiIGhlaWdodD0iNDQiIHhtbG5zPSJodHRwOi8vd3d3LnczLm9yZy8yMDAwL3N2ZyIgdmVyc2lvbj0iMS4xIi8+",
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"data:image/gif;base64,R0lGODlhAQABAIAAAAAAAP///yH5BAEAAAAALAAAAAABAAEAAAIBRAA7",
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"https://search-static.byjusweb.com/question-images/byjus/581804_c0947db96d0333e2f19c31779381fe48b9cc52f220160907-19040-1fmfzb4.png",
null,
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http://www.wordsearchfun.com/197164_Tale_wordsearch.html?r=1582846940 | [
"Tale\nSoek die woorde wat onderaan die bladsy staan.\n\nLogin to be the first to rate this puzzle!\nBEWONDERAARS\nBLOUBLASIES\nBOUKONTRAKTEUR\nBRANDERPLANK\nBRANDERS\nDUBBELTJIE\nGROOTOUERS\nOUTOMATIESE\nROEISPANE\nSEESTROME\nSKOOLVAKANSIE\nSNORKEL\nSONBRANDMIDDEL\nSTRANDHANDDOEK\nSTRANDSAMBREEL\nTOEPASLIKE\n B O U K O N T R A K T E U R M K B R A N D E R P L A N K L I E I L E M O R T S E E S E C X O U T O M A T I E S E E N D B D V K R U X S C W J R E A U E D I Q J N B I X Q B L F P B W N M Q S D L L K M B J C S B O A S K O O L V A K A N S I E N H U V X K P S U S R L H E L D D B R A N D E R S I G O O T E N V I F N M P T B R E O R J R A E H A J L E K R O N S I I A R G R O O T O U E R S B A E A T T O E P A S L I K E Z Z Q R S O N B R A N D M I D D E L S"
]
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https://www.shaalaa.com/online-tests/cbse-psychology-term-1-exam-2021-22-official-sample-question-paper-01_273 | [
"Online Test - CBSE Psychology Term 1 Exam 2021-22 Official Sample Question Paper 01\n\n1. The Question Paper contains three sections. 2. Section A has 24 questions. Attempt any 20 questions. 3. Section B has 24 questions. Attempt any 20 questions. 4. Section C has 12 questions. Attempt any 10 questions. 5. All questions carry equal marks. 6. There is no negative marking.\nThe final score will be adjusted from 50 to 35\n\nThis test has 3 sections.\nSection - A\nSection A has 24 questions from question no. 1 to 24. Answer any 20 questions from this section.\nQuestions: 24\nDuration: 00:36:00\nThe maximum score for this section is 20\n\nSection - B\nSection B has 24 questions from question no. 25 to 48. Answer any 20 questions from this section.\nQuestions: 24\nDuration: 00:36:00\nThe maximum score for this section is 20\n\nSection - C\nSection C has 12 questions from question no. 49 to 60. A total of 10 questions are to be answered in this section.\nQuestions: 12\nDuration: 00:18:00\nThe maximum score for this section is 10"
]
| [
null
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https://peterdaugaardrasmussen.com/2023/01/21/mssql-how-to-add-to-a-date-or-time-in-mssql/ | [
" MSSQL - How to add years, days, months etc. to a date\n\nIn SQL Server, you can use the DATEADD function to add a specified time interval to a given date. The syntax for the `DATEADD` function is as follows:\n\n``````DATEADD(datepart, number, date)\n``````\n\nThe three parameters are:\n\n• datepart is the part of the date you want to add the interval to (e.g. day, month, year)\n• number is the number of intervals to add\n• date is the date you want to add the interval to\n\nFor example, to add three months to the current date:\n\n``````SELECT DATEADD(month, 3, GETDATE())\n``````\n\nTo add 30 days to a specific date, you can use the following:\n\n``````DECLARE @date DATE = '2022-01-01'\nYou can use different date parts like `'year'`, `'month'`, `'day'`, `'hour'`, `'minute'`, `'second'`, `'millisecond'` to add to those parts of the date.\nYou can also use `DATEADD` in a update statement in order to add days to a column in a table, like below:\n``````UPDATE myTable"
]
| [
null
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https://search.r-project.org/CRAN/refmans/BMAmevt/html/expfunction.nl.html | [
"expfunction.nl {BMAmevt} R Documentation\n\n## Exponent function in the NL model.\n\n### Description\n\nThe exponent function V for a max-stable variable M is such that P(M<x) = exp(-V(x))\n\n### Usage\n\n```expfunction.nl(par = c(0.3, 0.4, 0.5, 0.6), x = 10 * rep(1, 3))\n```\n\n### Arguments\n\n `par` The parameter for the NL distribution, respectively of length two or four. `x` A vector of three extended positive real numbers\n\n### Value\n\nthe value of V(x) for x=thres.\n\n[Package BMAmevt version 1.0.4 Index]"
]
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null
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http://dudui.club/what-is-two-step-math/ | [
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.7650391,"math_prob":0.99709195,"size":2512,"snap":"2019-51-2020-05","text_gpt3_token_len":487,"char_repetition_ratio":0.3740032,"word_repetition_ratio":0.27816093,"special_character_ratio":0.19307324,"punctuation_ratio":0.051835854,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":1.0000098,"pos_list":[0,1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48],"im_url_duplicate_count":[null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null,2,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-01-24T21:33:55Z\",\"WARC-Record-ID\":\"<urn:uuid:33341f67-df82-4cdb-8706-3520a7bb103a>\",\"Content-Length\":\"33758\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:db822561-8b28-45c1-b898-3bbabde19da9>\",\"WARC-Concurrent-To\":\"<urn:uuid:8b04c61b-4a71-44e2-ba1b-eaca9f14cf7c>\",\"WARC-IP-Address\":\"104.27.138.25\",\"WARC-Target-URI\":\"http://dudui.club/what-is-two-step-math/\",\"WARC-Payload-Digest\":\"sha1:UWXOSSFL34WXFZ3T7RXCPJPK25WYM3MQ\",\"WARC-Block-Digest\":\"sha1:KVHL45MUYD35YKC32QNZSZOQH4YAGN3J\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-05/CC-MAIN-2020-05_segments_1579250625097.75_warc_CC-MAIN-20200124191133-20200124220133-00146.warc.gz\"}"} |
https://it.mathworks.com/matlabcentral/cody/problems/43115-annoying-population/solutions/1698271 | [
"Cody\n\n# Problem 43115. Annoying population\n\nSolution 1698271\n\nSubmitted on 21 Dec 2018 by Athi\nThis solution is locked. To view this solution, you need to provide a solution of the same size or smaller.\n\n### Test Suite\n\nTest Status Code Input and Output\n1 Pass\nx = 4; y = 3; y_correct = 108; assert(isequal(findAnnoyingPopulation(x,y),y_correct))\n\n2 Pass\nx = 6; y = 2; y_correct = 54; assert(isequal(findAnnoyingPopulation(x,y),y_correct))\n\n3 Pass\nx = 7; y = 5; y_correct = 1701; assert(isequal(findAnnoyingPopulation(x,y),y_correct))"
]
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null
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.5613863,"math_prob":0.9858134,"size":496,"snap":"2019-51-2020-05","text_gpt3_token_len":161,"char_repetition_ratio":0.15447155,"word_repetition_ratio":0.0,"special_character_ratio":0.34475806,"punctuation_ratio":0.1875,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.98120034,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-01-21T16:10:31Z\",\"WARC-Record-ID\":\"<urn:uuid:6f29d1b2-9dc4-469c-b27f-3d2c5373210e>\",\"Content-Length\":\"72947\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:5ad566c5-cf54-4aad-bf8e-0e5c8d5a3190>\",\"WARC-Concurrent-To\":\"<urn:uuid:0eaa2e49-2ce0-4393-ba5c-f712b2b9df51>\",\"WARC-IP-Address\":\"104.96.217.125\",\"WARC-Target-URI\":\"https://it.mathworks.com/matlabcentral/cody/problems/43115-annoying-population/solutions/1698271\",\"WARC-Payload-Digest\":\"sha1:QFBA5SD5UCIWBKURA26VAJ2L24VOMSQC\",\"WARC-Block-Digest\":\"sha1:LSHBICJTJK3EKNWBS2CNINMNCFUHMKKE\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-05/CC-MAIN-2020-05_segments_1579250604397.40_warc_CC-MAIN-20200121132900-20200121161900-00311.warc.gz\"}"} |
https://convertoctopus.com/1169-meters-per-second-to-miles-per-hour | [
"## Conversion formula\n\nThe conversion factor from meters per second to miles per hour is 2.2369362920544, which means that 1 meter per second is equal to 2.2369362920544 miles per hour:\n\n1 m/s = 2.2369362920544 mph\n\nTo convert 1169 meters per second into miles per hour we have to multiply 1169 by the conversion factor in order to get the velocity amount from meters per second to miles per hour. We can also form a simple proportion to calculate the result:\n\n1 m/s → 2.2369362920544 mph\n\n1169 m/s → V(mph)\n\nSolve the above proportion to obtain the velocity V in miles per hour:\n\nV(mph) = 1169 m/s × 2.2369362920544 mph\n\nV(mph) = 2614.9785254116 mph\n\nThe final result is:\n\n1169 m/s → 2614.9785254116 mph\n\nWe conclude that 1169 meters per second is equivalent to 2614.9785254116 miles per hour:\n\n1169 meters per second = 2614.9785254116 miles per hour\n\n## Alternative conversion\n\nWe can also convert by utilizing the inverse value of the conversion factor. In this case 1 mile per hour is equal to 0.0003824123182207 × 1169 meters per second.\n\nAnother way is saying that 1169 meters per second is equal to 1 ÷ 0.0003824123182207 miles per hour.\n\n## Approximate result\n\nFor practical purposes we can round our final result to an approximate numerical value. We can say that one thousand one hundred sixty-nine meters per second is approximately two thousand six hundred fourteen point nine seven nine miles per hour:\n\n1169 m/s ≅ 2614.979 mph\n\nAn alternative is also that one mile per hour is approximately zero times one thousand one hundred sixty-nine meters per second.\n\n## Conversion table\n\n### meters per second to miles per hour chart\n\nFor quick reference purposes, below is the conversion table you can use to convert from meters per second to miles per hour\n\nmeters per second (m/s) miles per hour (mph)\n1170 meters per second 2617.215 miles per hour\n1171 meters per second 2619.452 miles per hour\n1172 meters per second 2621.689 miles per hour\n1173 meters per second 2623.926 miles per hour\n1174 meters per second 2626.163 miles per hour\n1175 meters per second 2628.4 miles per hour\n1176 meters per second 2630.637 miles per hour\n1177 meters per second 2632.874 miles per hour\n1178 meters per second 2635.111 miles per hour\n1179 meters per second 2637.348 miles per hour"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.7313279,"math_prob":0.9782301,"size":2275,"snap":"2020-45-2020-50","text_gpt3_token_len":604,"char_repetition_ratio":0.29062086,"word_repetition_ratio":0.068601586,"special_character_ratio":0.34681317,"punctuation_ratio":0.08144797,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99857205,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-10-28T08:14:44Z\",\"WARC-Record-ID\":\"<urn:uuid:11240bc9-7549-4708-8674-0283c6247ee6>\",\"Content-Length\":\"30523\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:fe808c5c-a623-4731-8a3a-904921b88e65>\",\"WARC-Concurrent-To\":\"<urn:uuid:27862299-988a-47e1-948e-f8c3b3458aa4>\",\"WARC-IP-Address\":\"104.27.143.66\",\"WARC-Target-URI\":\"https://convertoctopus.com/1169-meters-per-second-to-miles-per-hour\",\"WARC-Payload-Digest\":\"sha1:7EE6TTKL7AY7UMWAIQ36EDUED2VCRF2R\",\"WARC-Block-Digest\":\"sha1:VGCECU5NUZ2DIHQQSV2PWGCF3VFKGJLN\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-45/CC-MAIN-2020-45_segments_1603107897022.61_warc_CC-MAIN-20201028073614-20201028103614-00501.warc.gz\"}"} |
https://www.swie.io/pcb-assembly/tools/pages/n-way-power-divider-calculator/ | [
"This calculator determines the total path loss provided by an RF n-way power splitter.\n\n(dB)\n\n(dB)\n\n### Overview\n\nAn N-way power divider, also known as a Wilkinson power divider, has become very popular in the RF engineering world because it allows isolation between the output ports while maintaining a matched condition on all ports. This tool will compute for the total loss in an N-way power divider given the total number of ports and the path loss. You can compute for up to 16 paths. Note that the path loss and total loss are presented in decibels (dB).",
null,
"### Equations\n\n$Loss_{total} = -10log_{10}(\\frac{1}{N}) + Loss_{path}$\n\nWhere:\n\n$N$ = number of ports\n\n### Applications\n\nThe Wilkinson power divider has many uses, particularly in RF technology. When you feed power to one port of a power divider, the power divides equally between all ports. The bidirectional nature of power dividers means you can also use them as power combiners.\n\nWilkinson power dividers are mostly seen in I/Q modulators & demodulators, high power transmission systems, and signal mixers. For example, a 5-way power divider can be used in multiple-channel superheterodyne receivers, to distribute the local oscillator signal to all channels at one time from a single source. The Wilkinson power divider can also be used in high power amplifiers and T/R modules for power combining."
]
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null,
"https://www.swie.io/pcb-assembly/tools/images/content/Power-Divider-Calculator.png",
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]
| {"ft_lang_label":"__label__en","ft_lang_prob":0.9076388,"math_prob":0.9400134,"size":1371,"snap":"2019-26-2019-30","text_gpt3_token_len":299,"char_repetition_ratio":0.15801024,"word_repetition_ratio":0.0,"special_character_ratio":0.20714806,"punctuation_ratio":0.07936508,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99042207,"pos_list":[0,1,2],"im_url_duplicate_count":[null,1,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-07-17T05:18:09Z\",\"WARC-Record-ID\":\"<urn:uuid:07697df7-a4eb-4d3a-af64-0d8ba578f3a0>\",\"Content-Length\":\"11855\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:879ebef5-0fdf-47d2-b058-f04b0ca29dc1>\",\"WARC-Concurrent-To\":\"<urn:uuid:c9775bc7-b310-43ad-ad34-bcd9e2509750>\",\"WARC-IP-Address\":\"18.196.95.104\",\"WARC-Target-URI\":\"https://www.swie.io/pcb-assembly/tools/pages/n-way-power-divider-calculator/\",\"WARC-Payload-Digest\":\"sha1:CDA3YIE5NFRSWKSFQETPK5B6HU7E35IR\",\"WARC-Block-Digest\":\"sha1:5WQOHB3H6M6SJA4HVAS5DYDGJ2QGA6HS\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-30/CC-MAIN-2019-30_segments_1563195525046.5_warc_CC-MAIN-20190717041500-20190717063500-00028.warc.gz\"}"} |
https://studylib.net/doc/18522908/capacitance | [
"CAPACITANCE",
null,
"```C H A P T E R\nLearning Objectives\n➣ Capacitor\n➣ Capacitance\n➣ Capacitance of an Isolated\nSphere\n➣ Spherical Capacitor\n➣ Parallel-plate Capacitor\n➣ Special Cases of Parallelplate Capacitor\n➣ Multiple and Variable\nCapacitors\n➣ Cylindrical Capacitor\nCylindrical Capacitor\n➣ Capacitance Between two\nParallel Wires\n➣ Capacitors in Series\n➣ Capacitors in Parallel\n➣ Cylindrical Capacitor with\nCompound Dielectric\n➣ Insulation Resistance of a\nCable Capacitor\n➣ Energy Stored in a Capacitor\n➣ Force of Attraction Between\nOppositely-charged Plates\n➣ Current-Voltage\nRelationships in a Capacitor\n➣ Charging of a Capacitor\n➣ Time Constant\n➣ Discharging of a Capacitor\n➣ Transient Relations during\nCapacitor Charging Cycle\n➣ Transient Relations during\nCapacitor Discharging Cycle\n➣ Charging and Discharging of\na Capacitor with Initial\nCharge\n5\nCAPACITANCE\nThe above figure shows a variable\ncapacitor. A capacitor stores electric\ncharge and acts a small reservoir of\nenergy\n214\nElectrical Technology\n5.1. Capacitor\nA capacitor essentially consists of two conducting surfaces separated\nby a layer of an insulating medium called dielectric. The conducting surfaces may be in the form of either circular (or rectangular) plates or be of\nspherical or cylindrical shape. The purpose of a capacitor is to store electrical energy by electrostatic stress in the dielectric (the word ‘condenser’\nis a misnomer since a capacitor does not ‘condense’ electricity as such, it\nmerely stores it).\nA parallel-plate capacitor is shown in Fig. 5.1. One plate is joined to\nthe positive end of the supply and the other to the negative end or is earthed.\nIt is experimentally found that in the presence of an earthed plate B, plate\nA is capable of withholding more charge than when B is not there. When\nsuch a capacitor is put across a battery, there is a momentary flow of\nelectrons from A to B. As negatively-charged electrons are withdrawn\nfrom A, it becomes positive and as these electrons collect on B, it becomes\nFig. 5.1\nnegative. Hence, a p.d. is established between plates A and B. The transient\nflow of electrons gives rise to charging current. The strength of the charging\ncurrent is maximum when the two plates are uncharged but it then decreases and finally ceases when\np.d. across the plates becomes slowly and slowly equal and opposite to the battery e.m.f.\n5.2. Capacitance\nThe property of a capacitor to ‘store electricity’ may be called\nits capacitance.\nAs we may measure the capacity of a tank, not by the total\nmass or volume of water it can hold, but by the mass in kg of\nwater required to raise its level by one metre, similarly, the\ncapacitance of a capacitor is defined as “the amount of charge\nrequired to create a unit p.d. between its plates.”\nSuppose we give Q coulomb of charge to one of the two plate\nof capacitor and if a p.d. of V volts is established between the two,\nthen its capacitance is\ncharge\nQ\nC=\n=\nA capacitor stores electricity\nV potential differnce\nHence, capacitance is the charge required per unit potential difference.\nBy definition, the unit of capacitance is coulomb/volt which is also called farad (in honour of\n∴\nOne farad is defined as the capacitance of a capacitor which requires a charge of one coulomb\nto establish a p.d. of one volt between its plates.\nOne farad is actually too large for practical purposes. Hence, much smaller units like microfarad\n1 μF = 10−9 F; 1 nF = 10−9 F ; 1 μμF or pF = 10−12F\nIncidentally, capacitance is that property of a capacitor which delays and change of voltage\nacross it.\n5.3. Capacitance of an Isolated Sphere\nConsider a charged sphere of radius r metres having a charge of Q coulomb placed in a medium\nCapacitance\nof relative permittivity ε r as shown in Fig. 5.2.\nIt has been proved in Art 4.13 that the free surface potential V\nof such a sphere with respect to infinity (in practice, earth) is given by\nQ\nQ =4πε ε r\nV =\n∴\n0 r\n4 π ε0 εr r\nV\nBy definition, Q/V = capacitance C\n∴\n= 4 π ε0 εr r F\n– in a medium\n= 4 π ε0 r F\n– in air\n215\nFig. 5.2\nNote : It is sometimes felt surprising that an isolated sphere can act as a capacitor because, at first sight, it\nappears to have one plate only. The question arises as to which is the second surface. But if we remember that\nthe surface potential V is with reference to infinity (actually earth) then it is obvious that the other surface is\nearth. The capacitance 4 π ε0 r exists between the surface of the sphere and earth.\n5.4. Spherical Capacitor\n(a) When outer sphere is earthed\nConsider a spherical capacitor consisting of two concentric spheres of radii ‘a’ and ‘b’ metres as\nshown in Fig. 5.3. Suppose, the inner sphere is given a charge of + Q\ncoulombs. It will induce a charge of −Q coulombs on the inner surfaces\nwhich will go to earth. If the dielectric medium between the two spheres\nhas a relative permittivity of ε r, then the free surface potential of the inner\nsphere due to its own charge Q/4 π ε 0 ε r a volts. The potential of the\ninner sphere due to − Q charge on the outer sphere is − Q/4 π ε 0 ε r b\n(remembering that potential anywhere inside a sphere is the same as that\nits surface).\nFig. 5.3\n∴\nTotal potential difference between two surfaces is\nQ\nQ\n−\nV =\n4 π ε0 ε r a 4 π ε0 ε r b\n(\n)\nQ\nQ\n⎛b − a⎞\n1−1 =\n⎜\n⎟\n4 π ε0 εr a b\n4 π ε0 εr ⎝ ab ⎠\n4 π ε0 ε r ab\nQ\n=\n∴ C = 4 π ε 0 ε r ab F\nb−a\nV\nb−a\n=\nFig. 5.4\n(b) When inner sphere is earthed\nSuch a capacitor is shown in Fig. 5.4. If a charge of + Q coulombs is given to the outer sphere A,\nit will distribute itself over both its inner and outer surfaces. Some charge Q2 coulomb will remain on\nthe outer surface of A because it is surrounded by earth all around. Also, some charge\n+ Q1 coulombs will shift to its inner side because there is an earthed sphere B inside A.\nObviously,\nQ = Q1 + Q2\nThe inner charge + Q1 coulomb on A induces −Q1 coulomb on B but the other induced charge of\n+ Q1 coulomb goes to earth.\nNow, there are two capacitors connected in parallel :\n(i) One capacitor consists of the inner surface of A and the outer surface of B. Its capacitance,\nas found earlier, is\nab\nC1 = 4 π ε0 ε r\nb−a\n(ii) The second capacitor consists of outer surfaces of B and earth. Its capacitance is C2 = 4 π ε0\nb −if surrounding medium is air. Total capacitance C = C1 + C2.\n216\nElectrical Technology\n5.5. Parallel-plate Capacitor\nVacuum\nDielectric\n–Q\n(i) Uniform Dielectric-Medium\nQ –Q\nQ\nA parallel-plate capacitor consisting of two plates M and\nN each of area A m2 separated by a thickness d metres of a\nmedium of relative permittivity ε r\n←V ←\n←V←\n0\nis shown in Fig. 5.5. If a charge\nof + Q coulomb is given to plate\nM, then flux passing through the\nmedium is ψ = Q coulomb. Flux\nElectrometer\nElectrometer\ndensity in the medium is\n(b)\n(a)\nThe figure shows how the\nψ Q\nD= =\ncapacitance changes when\nA A\ndielectric constant is changed\nElectric intensity E = V/d and\nD=ε E\nFig. 5.5\nV\nQ\n= ε\n∴ Q = εA\nor\nd\nA\nV\nd\nε0 ε r A\n∴\nC=\n– in a medium\n...(i)\nd\nε0 A\n=\n– with air as medium\nd\n(ii) Medium Partly Air\nAs shown in Fig. 5.6, the medium consists partly of air and partly\nof parallel-sided dielectric slab of thickness t and relative permittivity\nε r. The electric flux density D = Q/A is the same in both media. But\nelectric intensities are different.\n... in the medium\nE1 = D\nε0 ε r\nD\nE2 =\n... in air\nε0\nV = E1 . t + E2 (d −t)\nD t + D (d − t ) = D ⎛ t + d − t ⎞\n=\n⎟\nFig. 5.6\nε0 ε r\nε0\nε0 ⎜⎝ ε r\n⎠\nQ\n[d − (t − t / ε r )]\n=\nε0 A\nε0 A\nε0 A\nQ\nor\n=\nor C =\n...(ii)\nd\n−\nt\n−\nt\nε\nd\n−\nt − t / εr )]\n[\n(\n/\n)]\n[\n(\nV\nr\nIf the medium were totally air, then capacitance would have been\nC = ε 0 A/d\nFrom (ii) and (iii), it is obvious that when a dielectric slab of thickness t and relative permittivity\nε r is introduced between the plates of an air capacitor, then its capacitance increases because as seen\nfrom (ii), the denominator decreases. The distance between the plates is effectively reduces by\n(t −t/ε r). To bring the capacitance back to its original value, the capacitor plates will have to be\nfurther separated by that much distance in air. Hence, the new separation between the two plates\nwould be\n= [d + (t −t / εr)]\nε A\nThe expression given in (i) above can be written as C = 0\nd / εr\np.d. between plates,\n217\nCapacitance\nIf the space between the plates is filled with slabs of different thickness and relative permittivities,\nε0 A\nthen the above expression can be generalized into C =\nΣ d / εr\nThe capacitance of the capacitor shown in Fig. 5.7 can be written as\nε0 A\nC =\nd3 ⎞\n⎛ d1 d 2\n⎜ε + ε + ε ⎟\nr2\nr3 ⎠\n⎝ r1\n(iii) Composite Medium\nThe above expression may be derived independently as given under :\nIf V is the total potential difference across the capacitor plates and V1, V2, V3, the potential\ndifferences across the three dielectric slabs, then\nV = V1 + V2 + V3 = E1t1 + E2t2 + E3t3\n∴\nFig. 5.7\n=\nD .t + D .t + D .t\nε0 ε r1 1 ε0 ε r 2 2 ε0 εr 3 3\n=\nD\nε0\nC =\nt2\nt3 ⎞\nt2\nt3 ⎞\n⎛ t1\nQ ⎛ t1\n⎜ε + ε + ε ⎟= ε A ⎜ε + ε + ε ⎟\nr2\nr3 ⎠\n0\nr2\nr3 ⎠\n⎝ r1\n⎝ r1\nε0 A\nQ\n=\nV ⎛ t1\nt3 ⎞\nt2\n⎜ε + ε + ε ⎟\nr2\nr3 ⎠\n⎝ r1\n5.6. Special Cases of Parallel-plate Capacitor\nConsider the cases illustrated in Fig. 5.8.\n(i) As shown in Fig. 5.8 (a), the dielectric is of\nthickness d but occupies only a part of the area. This\narrangement is equal to two capacitors in parallel. Their\ncapacitances are\nε A\nε ε A\nC1 = 0 1 and C2 = 0 r 2\nd\nd\nTotal capacitance of the parallel-plate capacitor is\nε0 A1 ε0 ε r A2\n+\nd\nd\n(ii) The arrangement shown in Fig. 5.8 (b) consists of two capacitors connected in parallel.\nC = C1 + C2 =\n(a)\n(b)\nFig. 5.8\nε0 A1\nd\n(b) the other capacitor has dielectric partly air and partly some other medium. Its capacitance is\nε0 A2\n[Art 5.5 (ii)]. C2 =\n. Total capacitance is C = C1 + C2\n[d − (t − t / ε r )\n(a) one capacitor having plate area A1 and air as dielectric. Its capacitance is C1 =\n5.7. Multiple and Variable Capacitors\nMultiple capacitors are shown in Fig. 5.9 and Fig. 5.10.\nThe arrangement of Fig. 5.9. is equivalent to two capacitors joined in parallel. Hence, its\ncapacitance is double that of a single capacitor. Similarly, the arrangement of Fig. 5.10 has four times\nthe capacitance of single capacitor.\n218\nElectrical Technology\n(a)\n(b)\nFig. 5.9\nFig. 5.10\nIf one set of plates is fixed and the other is capable of rotation, then\ncapacitance of such a multiplate capacitor can be varied. Such variablecapacitance air capacitors are widely used in radio work (Fig. 5.11). The\nset of fixed plates F is insulated from the other set R which can be rotated\nby turning the knob K. The common area between the two sets is varied\nby rotating K, hence the capacitance between the two is altered. Minimum\ncapacitance is obtained when R is completely rotated out of F and maximum\nwhen R is completely rotated in i.e. when the two sets of plates completely\noverlap each other.\nThe capacitance of such a capacitor is\n(n − 1) . ε0 ε r A\n=\nd\nwhere n is the number of plates which means that (n −1) is the number of\ncapacitors.\nExample 5.1. The voltage applied across a capacitor having a\nFig. 5.11\ncapacitance of 10 μ F is varied thus :\nThe p.d. is increased uniformly from 0 to 600 V in seconds. It\nis then maintained constant at 600 V for 1 second and subsequently decreased uniformly to zero in five seconds. Plot a\ngraph showing the variation of current during these 8 seconds. Calculate (a) the charge (b) the energy stored in the\ncapacitor when the terminal voltage is 600.\n(Principles of Elect. Engg.-I, Jadavpur Univ.)\nSolution. The variation of voltage across the capacitor is as\nshown in Fig. 5.12 (a).\nThe charging current is given by\ndq d\n= (Cv) = C . dv\ni =\ndt dt\ndt\nCharging current during the first stage\n−6\n−3\n= 10 × 10 × (600/2) = 3 × 10 A = 3 mA\nCharging current during the second stage is zero because\ndv/dt = 0 as the voltage remains constant.\nCharging current through the third stage\n⎛ 0 − 600 ⎞\n−6\n−3\nFig. 5.12\n= 10 × 10 × ⎜\n⎟ = −1.2 × 10 A = −1.2 mA\n⎝ 5 ⎠\nThe waveform of the charging current or capacitor current is shown in Fig. 5.12 (b).\n−3\n−6\n(a) Charge when a steady voltage of 600 V is applied is = 600 × 10 × 10 = 6 × 10 C\n2\n−\n5\n2\n(b) Energy stored = 12 C V = 12 × 10 × 600 = 1.8 J\nExample 5.2. A voltage of V is applied to the inner sphere of a spherical capacitor, whereas the\nouter sphere is earthed. The inner sphere has a radius of a and the outer one of b. If b is fixed and a may\nbe varied, prove that the maximum stress in the dielectric cannot be reduced below a value of 4 V/b.\nCapacitance\nSolution. As seen from Art. 5.4,\n(\n219\n)\nQ\n1−1\n...(i)\n4 π ε0 ε r a b\nAs per Art. 4.15, the value of electric intensity at any radius x between the two spheres is given\nQ\n2\nby E =\nor Q = 4 π ε0 ε r x E\n2\n4 π ε0 εr x\nSubstituting this value in (i) above, we get\n4 π ε0 ε r x 2 E 1 1\nV\n−\nor E =\nV =\n4 π ε0 ε r\na b\n(1/ a − 1/ b) x 2\nAs per Art. 5.9, the maximum value of E occurs as the surface of inner sphere i.e. when x = a\nFor E to be maximum or minimum, dE/da = 0.\nd 1 − 1 a2 = 0 or d (a −a2/b) = 0\n∴\nda a b\nda\nor\n1 − 2 a/b = 0 or a = b/2\nV\nV\nV\nNow,\nE =\n∴Emax =\n=\n2\n(1/ a − 1/ b) x\n(1/ a − 1/ b) a 2\n(a − a 2 / b)\n4 bV\n4V\nV\n4bV\nSince, a = b/2\n∴ Emax =\n=\n=\n2\n2 =\n2\nb\n(b / 2 − b2 / 4b)\n2b − b\nb\nExample 5.3. A capacitor consists of two similar square aluminium plates, each 10 cm × 10 cm\nmounted parallel and opposite to each other. What is their capacitance in μμ F when distance\nbetween them is 1 cm and the dielectric is air ? If the capacitor is given a charge of 500 μμ C, what\nwill be the difference of potential between plates ? How will this be affected if the space between the\nplates is filled with wax which has a relative permittivity of 4 ?\nV =\n(\n(\n)\n)\nC = ε 0 A/d farad\n−12\n2\n−2 2\nε0 = 8.854 × 10 F/m ; A = 10 × 10 = 100 cm = 10 m\n−2\nd = 1 cm = 10 m\n−12\n−2\n8.854 × 10 × 10\n∴\nC =\n= 8.854 × 10−12 F = 8.854 μμ\nμμF\n−2\n10\n−12\nQ\nQ\n500 × 10\nC = 56.5 volts.\nNow\nC =\n∴ V=\nor V =\n−12 F\nC\nV\n8.854 × 10\nWhen wax is introduced, their capacitance is increased four times because\nC = ε 0 ε r A/d F = 4 × 8.854 = 35.4 μμ F\nThe p.d. will obviously decrease to one fourth value because charge remains constant.\n∴\nV = 56.5/4 = 14.1 volts.\nExample 5.4. The capacitance of a capacitor formed by two parallel metal plates each\n200 cm2 in area separated by a dielectric 4 mm thick is 0.0004 microfarads. A p.d. of 20,000 V is\napplied. Calculate (a) the total charge on the plates (b) the potential gradient in V/m (c) relative\npermittivity of the dielectric (d) the electric flux density.\n(Elect. Engg. I Osmaina Univ.)\n−4\n4\nSolution.\nC = 4 × 10 μF ; V = 2 × 10 V\n−6\n−4\n4\n(a) ∴ Total charge\nQ = CV = 4 × 10 × 2 × 10 μC = 8 μC = 8 × 10 C\n4\n2 × 10\n6\n= dV =\n= 5 × 10 V/m\ndx 4 × 10−3\n−\nD = Q/A = 8 × 10−6/200 × 10−4 = 4 × 10 4 C/m2\n(c)\n6\n(d)\nE = 5 × 10 V/m\n−4\n4 × 10\nD =\nSince D = ε 0 ε r E ∴\nεr =\n=9\n−\n12\nε0 × E 8.854 × 10 × 5 × 106\nSolution.\nHere\n220\nElectrical Technology\nExample 5.5. A parallel plate capacitor has 3 dielectrics with relative permittivities of 5.5, 2.2\nand 1.5 respectively. The area of each plate is 100 cm2 and thickness of each dielectric 1 mm.\nCalculate the stored charge in the capacitor when a potential difference of 5,000 V is applied across\nthe composite capacitor so formed. Calculate the potential gradient developed in each dielectric of\nthe capacitor.\n(Elect. Engg. A.M.Ae.S.I.)\nSolution. As seen from Art. 5.5,\n−12\n−4\n−14\nε0 A\n8.854 × 10 × (100 × 10 ) 8.854 × 10\n= 292 pF\nC =\n=\n=\n−\n3\nd3 ⎞\n⎛ d1 d 2\n⎛ 10−3 10−3 10−3 ⎞\n10\n0.303\n×\n+\n+\n⎜ε + ε + ε ⎟\n⎜\n2.2\n1.5 ⎠⎟\nr2\nr3 ⎠\n⎝ r1\n⎝ 5.5\nQ\nD\ng1\ng2\n=\n=\n=\n=\nCV =292 × 10−12 × 5000 = 146 × 10−8 coulomb\n−8\n−4\n−6\n2\nQ/A = 146 × 10 /(100 × 10 ) = 146 × 10 C/m\n−6\n-12\nE1 = D/ε 0 ε r1 = 146 × 10 /8.854 × 10 × 5.5 = 3 × 106 V/m\n6\n6\nE2 = D/ε 0 ε r2 = 7.5 × 10 V/m; g3 = D/ε 0 ε r3 = 11 × 10 V/m\nExample 5.6. An air capacitor has two parallel plates 10 cm2 in area and 0.5 cm apart. When\n2\na dielectric slab of area 10 cm and thickness 0.4 cm was inserted between the plates, one of the\nplates has to be moved by 0.4 cm to restore the capacitance. What is the dielectric constant of the\nslab ?\n(Elect. Technology, Hyderabad Univ. 1992 )\nSolution. The capacitance in the first case is\nε A ε × 10 × 10−4 ε0\nCa = 0 = 0\n=\nd\n5\n0.5 × 10−2\nThe capacitor, as it becomes in the second case, is shown in Fig.\n5.13. The capacitance is\n−3\nε0 A\nε0 × 10\nε0\nCm =\n=\n=\nΣ d / ε r ⎛ 0.5 × 10−3 ⎞ ⎛ 5 + 4 ⎞\n⎟\n⎜\n⎟ ⎜ε\n⎠\nεr\n⎝\n⎠ ⎝ r\nε0\nε\nSince,\nCa = Cm ∴ 0 =\n∴ εr = 5\n(5 / εr + 4)\n5\nFig. 5.13\nNote. We may use the relation derived in Art. 5.5 (ii)\nSeparation = (t − t/ε 1)\n∴ 0.4 = (0.5 − 0.5/ε r)\nor\nεr = 5\nExample 5.7. A parallel plate capacitor of area, A, and plate separation, d, has a voltage, V0,\napplied by a battery. The battery is then disconnected and a dielectric slab of permittivity ε 1 and\nthickness, d1, (d1 < d) is inserted. (a) Find the new voltage V1 across the capacitor, (b) Find the\ncapacitance C0 before and its value C1 after the slab is introduced. (c) Find the ratio V1/V0 and the\nratio C1/C0 when d1 = d/2 and ε 1 = 4 ε 0.\n(Electromagnetic Fields and Waves AMIETE (New Scheme) June 1990)\nε0 A\nA\nSolution. (b)\nC0 =\n; C1 =\nd\n⎛ (d − d1) d1 ⎞\n+ ⎟\n⎜ ε\nε1 ⎠\n0\n⎝\n8ε A\nA\n= 0\n5d\n⎛ d\n⎞\nd\n⎜ 2ε + 2 × 4 ε ⎟\n0⎠\n⎝ 0\n(a) Since the capacitor charge remains the same\nC\nε A\n5V\n5d\nQ = C0 V0 = C1 V1 ∴ V1 = V0 0 = V0 × 0 ×\n= 0\nC1\nd\n8 ε0 A\n8\nSince d1 = d/2 and ε 1 = 4 ε 0 ∴ C1 =\nCapacitance\n(c) As seen from above, V1 = V0 5/8 ; C1 C0 =\n221\n8 ε0 A\n× d =5\n5d\nε0 A 8\nTutorial Problems No. 5.1\n1. Two parallel plate capacitors have plates of an equal area, dielectrics of relative permittivities ε r1 and\nε r2 and plate spacing of d1 and d2. Find the ratio of their capacitances if εr1/ε r2 = 2 and d1/d2 = 0.25.\n[C1/C2 = 8]\n2. A capacitor is made of two plates with an area of 11 cm2 which are separated by a mica sheet 2 mm\nthick. If for mica ε r = 6, find its capacitance. If, now, one plate of the capacitor is moved further to give an air\ngap 0.5 mm wide between the plates and mica, find the change in capacitance.\n[29.19 pF, 11.6 pF]\n3. A parallel-plate capacitor is made of two plane circular plates separated by d cm of air. When a\nparallel-faced plane sheet of glass 2 mm thick is placed between the plates, the capacitance of the system is\nincreased by 50% of its initial value. What is the distance between the plates if the dielectric constant of the\nglass is 6 ?\n−\n[0.5 × 10 3 m]\n4. A p.d. of 10 kV is applied to the terminals of a capacitor consisting of two circular plates, each\nhaving an area of 100 cm2 separated by a dielectric 1 mm thick. If the capacitance is 3 × 10−4 μ F, calculate\n(a) the total electric flux in coulomb\n(b) the electric flux density and\n(c) the relative permittivity of the dielectric.\n−\n−\n[(a) 3 × 10 6C (b) 3 × 10 4 μ C/m2 (c) 3.39]\n5. Two slabs of material of dielectric strength 4 and 6 and of thickness 2 mm and 5 mm respectively are\ninserted between the plates of a parallel-plate capacitor. Find by how much the distance between the plates\nshould be changed so as to restore the potential of the capacitor to its original value.\n[5.67 mm]\n6. The oil dielectric to be used in a parallel-plate capacitor has a relative permittivity of 2.3 and the\nmaximum working potential gradient in the oil is not to exceed 106 V/m. Calculate the approximate plate area\nrequired for a capacitance of 0.0003 μ F, the maximum working voltage being 10,000 V.\n−\n[147 × 10 3 m2]\n7. A capacitor consist of two metal plates, each 10 cm square placed parallel and 3 mm apart. The\nspace between the plates is occupied by a plate of insulating material 3 mm thick. The capacitor is charged to\n300 V.\n(a) the metal plates are isolated from the 300 V supply and the insulating plate is removed. What is\nexpected to happen to the voltage between the plates ?\n(b) if the metal plates are moved to a distance of 6 mm apart, what is the further effect on the voltage\nbetween them. Assume throughout that the insulation is perfect.\n[300 ε r ; 600 ε r ; where ε r is the relative permittivity of the insulating material]\n2\n8. A parallel-plate capacitor has an effecting plate area of 100 cm (each plate) separated by a dielectric\n0.5 mm thick. Its capacitance is 442 μμ F and it is raised to a potential differences of 10 kV. Calculate from\nfirst principles\n(a) potential gradient in the dielectric (b) electric flux density in the dielectric\n(c) the relative permittivity of the dielectric material.\n2\n[(a) 20 kV/mm (b) 442 μC/m (c) 2.5]\n9. A parallel-plate capacitor with fixed dimensions has air as dielectric. It is connected to supply of p.d.\nV volts and then isolated. The air is then replaced by a dielectric medium of relative permittivity 6. Calculate\nthe change in magnitude of each of the following quantities.\n(a) the capacitance (b) the charge (c) the p.d. between the plates\n(d) the displacement in the dielectric (e) the potential gradient in the dielectric.\n[(a) 6 : 1 increase (b) no change (c) 6 : 1 decrease (d) no change (e) 6 : 1 decrease]\n222\nElectrical Technology\n5.8. Cylindrical Capacitor\nA single-core cable or cylindrical capacitor consisting two\nco-axial cylinders of radii a and b metres, is shown in Fig. 5.14.\nLet the charge per metre length of the cable on the outer surface\nof the inner cylinder be + Q coulomb and on the inner surface of\nthe outer cylinder be −Q coulomb. For all practical purposes,\nthe charge + Q coulomb/metre on the surface of the inner cylinder can be supposed to be located along its axis. Let ε r be the\nrelative permittivity of the medium between the two cylinders.\nThe outer cylinder is earthed.\nNow, let us find the value of electric intensity at any point\ndistant x metres from the axis of the inner cylinder. As shown in\nFig. 5.15, consider an imaginary co-axial cylinder of radius x\nmetres and length one metre between the two given cylinders.\nThe electric field between the two cylinders is radial as shown.\nTotal flux coming out radially from the curved surface of this\nimaginary cylinder is Q coulomb. Area of the curved surface = 2\nπ x × 1 = 2 π x m2.\nHence, the value of electric flux density on the surface of the\nimaginary cylinder is\nQ\nflux in coulomb = ψ = Q\n2\n2\nD=\nC/m ∴D =\nC/m\n2\nA\nA\n2\nπ\nx\narea in metre\nThe value of electric intensity is\nQ\nE = D\nor E =\nV/m\nε0 ε r\n2π ε0 εr x\nNow,\ndV = − E dx\na\na\nQ dx\nor\nV =\n− E . dx = −\n2 πε0 εr x\nb\nb\n∫\nFig. 5.14\n∫\na\n−Q\na\ndx = − Q\nlog x b\n2 π ε0 ε r b x 2 π ε0 ε r\n−Q\n−Q\nQ\n=\n(log e a − log e b) =\nlog e a =\nlog e a\nb\n2 π ε0 ε r\n2 π ε0 ε r\n2 π ε0 εr\nb\n2\nπ\nε\nε\n2\nπ\nε\nε\nQ\n0 r\n0 r\nF/m ⎛⎜ log e b = 2.3 log10 b ⎞⎟\n=\n∴ C =\nb\na\na ⎠\nb\nV\n⎝\n2.3 log10\nlog e\na\na\n2 πε0 εr l\nThe capacitance of l metre length of this cable is C =\nF\n2.3 log10 b\na\nIn case the capacitor has compound dielectric, the relation becomes\n2 πε0 l\nC =\nF\nΣ log e b / ε r\na\nThe capacitance of 1 km length of the cable in μ F can be found by putting l = 1 km in the above\nexpression.\n−12\n2 π × 8.854 × 10 × εr × 1000\n0.024 εr\nC =\nF/km =\nμ F/km\n2.3 log10 b\nlog10 b\na\na\n∫\n=\n()\n()\n()\n()\n()\n()\n()\n()\n()\n()\nCapacitance\n223\n5.9. Potential Gradient in a Cylindrical Capacitor\nIt is seen from Art. 5.8 that in a cable capacitor\nQ\nE =\nV/m\n2 π ε0 ε r x\nwhere x is the distance from cylinder axis to the point under consideration.\nQ\nV/m\n...(i)\nNow\nE = g ∴ g =\n2 π ε0 ε r x\n2 πε0 ε r V\nQ\nlog e b\nFrom Art. 5.8, we find that V =\nor Q =\n2 π ε0 εr\na\nFig. 5.15\nloge b\na\nSubstituting this value of Q in (i) above, we get\n()\ng=\n2 π ε0 ε r V\nV\nV/m or g =\nV/m\nb\nx log e b\nlog e\n× 2 π ε0 ε r x\na\na\n()\n()\nor g =\nV\n()\n2.3 x log10 b\na\nObviously, potential gradient varies inversely as x.\nMinimum value of x = a, hence maximum value of potential gradient is\nV\nV/m\ngmax =\n2.3 a log10 b\na\nV\nSimilarly,\ngmax =\nV/m\n2.3 b log10 b\na\n()\n()\n()\nvolt/metre\n...(ii)\nNote. The above relation may be used to obtain most economical dimension while designing a cable. As\nseen, greater the value of permissible maximum stress Emax, smaller the cable may be for given value of V.\nHowever, Emax is dependent on the dielectric strength of the insulating material used.\nIf V and Emax are fixed, then Eq. (ii) above may be written as\nV ∴ b\nb\nV\nk/a\nk/a\nEmax =\nor a logh\n=\n= e or b = a e\nEmax\na\na\nb\na logh e\na\nFor most economical cable db/da = 0\ndb = 0 = ek/a + a (−k/a2)ek/a or a = k = V/E\n∴\nmax and b = ae = 2.718 a\nda\n()\n()\nExample 5.8. A cable is 300 km long and has a conductor of 0.5 cm in diameter with an\ninsulation covering of 0.4 cm thickness. Calculate the capacitance of the cable if relative permittivity of insulation is 4.5.\n(Elect. Engg. A.M.Ae. S.I.)\n0.024 εr\nSolution. Capacitance of a cable is C =\nμ F/km\nlog10 b\na\n2.6\nHere, a = 0.5/2 = 0.25 cm ; b = 0.25 + 0.4 = 0.65 cm ; b/a = 0.65/0.25 = 2.6 ; log10 = 0.415\n0.024 × 4.5\n= 0.26\n∴\nC =\n0.415\nTotal capacitance for 300 km is = 300 × 0.26 = 78 μ F.\nExample 5.9. In a concentric cable capacitor, the diameters of the inner and outer cylinders\nare 3 and 10 mm respectively. If ε r for insulation is 3, find its capacitance per metre.\nA p.d. of 600 volts is applied between the two conductors. Calculate the values of the electric\nforce and electric flux density : (a) at the surface of inner conductor (b) at the inner surface of outer\nconductor.\n()\n224\nElectrical Technology\n( )\n∴b/a = 5/1.5 = 10/3 ; log10 10 = 0.523\n3\nSolution. a = 1.5 mm ; b = 5 mm ;\nC =\n(a)\nNow\nD\nQ\nD\nE\n=\n=\n=\n=\n(b)\nD =\n−12\n2 π ε0 ε r l\n2π × 8.854 × 10 × 3 × 1\n−12\n= 138.8 × 10 F = 138.8 pF\n=\nb\n2.3\n×\n0.523\n2.3 log10\na\nQ/2π a\n−12\n−9\nCV = 138.8 × 10 × 600 = 8.33 × 10 C\n−8\n−3\n8.33 × 10 /2π × 1.5 × 10 = 8.835 μ C/m2\nD/ε 0 ε r = 332.6 V/m\n()\n−8\n8.33 × 10\n2\n2\nC/m = 2.65 μ C/m ; E = D/ε 0 ε r = 99.82 V/m.\n−3\n2π × 5 × 10\nExample 5.10. The radius of the copper core of a single-core rubber-insulated cable is 2.25\nmm. Calculate the radius of the lead sheath which covers the rubber insulation and the cable\ncapacitance per metre. A voltage of 10 kV may be applied between the core and the lead sheath with\na safety factor of 3. The rubber insulation has a relative permittivity of 4 and breakdown field\n6\nstrength of 18 × 10 V/m.\nV\nSolution. As shown in Art. 5.9, gmax =\n2.3 a log10 b\na\n6\nNow, gmax = Emax = 18 × 10 V/m ; V = breakdown voltage x\n4\nSafety factor = 10 × 3 = 30,000 V\n30, 000\n6\n∴ b = 2.1 or b = 2.1 × 2.25 = 4.72 mm\n∴8 × 10 =\n−3\nb\na\n2.3 × 2.25 × 10 × log10\na\n− 12\n2π ε0 εr l\n2π × 8.854 × 10 × 4 × 1\n=\n= 3 × 10–9 F\nC =\nb\n2.3\nlog\n(2.1)\n10\n2.3 log10\na\n()\n()\n()\n5.10. Capacitance Between Two Parallel Wires\nThis case is of practical importance in overhead transmission lines. The simplest system is 2-wire system (either\nd.c. or a.c.). In the case of a.c. system, if the transmission\nline is long and voltage high, the charging current drawn by\nthe line due to the capacitance between conductors is appreciable and affects its performance considerably.\nWith reference to Fig. 5.16, let\nd = distance between centres of the wires A and B\nr = radius of each wire (≤d)\nQ = charge in coulomb/metre of each wire*\nNow, let us consider electric intensity at any point P\nbetween conductors A and B.\nElectric intensity at P* due to charge + Q coulomb/metre\non A is\nA capictor can be charged by\nconnecting it to a battery\nFig. 5.16\n*\nIf charge on A is + Q, then on B will be −Q.\nCapacitance\n=\nQ\nV/m\n2 π ε0 ε r x\n225\n... towards B.\nElectric intesity at P due to charge −Q coulomb/metre on B is\nQ\nV/m\n=\n2 π ε0 ε r (d − x)\n... towards B.\nQ\n⎛1\n⎞\n+ 1\n2 π ε0 ε r ⎜⎝ x d − x ⎟⎠\nHence, potential difference between the two wires is\nd −r\nd −r ⎛\nQ\n1\n1 ⎞\nE.dx =\nV =\n⎜ x + d − x ⎟ dx\n2 π ε0 ε r r\nr\n⎝\n⎠\nd −r\nQ\nQ\nd −r\n| log e x − log e (d − x) |r =\nlog\nV =\n2 π ε0 ε r\nπ ε0 εr e r\nTotal electric intensity at P, E =\n∫\nNow C = Q/V ∴ C =\n∫\nπ ε0 εr\nπ ε0 ε r\nπ ε0 εr\nF/m (approx.)\n=\n=\n(d − r )\n(d − r )\n2.3 log10 d\nlog e\n2.3 log10\nr\nr\nr\n()\nThe capacitance for a length of l metres C =\nπ ε0 ε r\n()\n2.3 log10 d\nr\nF\nThe capacitance per kilometre is\n− 12\n6\nπ × 8.854 × 10 × εr × 100 × 10\n= μ F/km\nC =\n0.0121 ε r\n2.3 log10 d =\nr\nlog10 d\nr\n()\n()\nExample 5.11. The conductors of a two-wire transmission line (4 km long) are spaced 45 cm\nbetween centre. If each conductor has a diameter of 1.5 cm, calculate the capacitance of the line.\nπ ε0 ε r\nSolution. Formula used\nC =\nF\n2.3 log10 d\nr\n45 × 2\nHere l = 4000 metres ; r = 1.5/2 cm ; d = 45 cm ; ε r = 1−for air ∴ d =\n= 60\nr\n1.5\n()\n[or\n− 12\nπ × 8.854 × 10 × 4000\n= 0.0272 × 10–6 F\n2.3 log10 60\n0.0121\nμF]\nC = 4\n0.0272μ\nlog10 60\nC =\n5.11. Capacitors in Series\nWith reference of Fig. 5.17, let\nC1, C2, C3 = Capacitances of three capacitors\nV1, V2, V3 = p.ds. across three capacitors.\nV = applied voltage across combination\nC = combined or equivalent or joining capacitance.\nIn series combination, charge on all capacitors is the same but p.d. across each is different.\n226\n∴\nor\nor\nElectrical Technology\nV = V1 + V2 + V3\nQ\nQ\nQ\nQ\n+\n+\n=\nC\nC\nC\nC\n1\n2\n3\n1 + 1 + 1\n1\n=\nC1 C2 C3\nC\nFor a changing applied voltage,\ndV1 dV2 dV3\ndV\n+\n+\n=\ndt\ndt\ndt\ndt\nFig. 5.17\nWe can also find values of V1, V2 and\nV3 in terms of V. Now, Q = C1 V1 = C2V2 = C3V3 = CV\nC1 C2 C3\nCC C\n= 1 2 3\nwhere\nC =\nC1C2 + C2C3 + C3C1 Σ C1C2\nC C\n∴\nC1V1 = C V or V1 = V C = V . 2 3\nC1\nΣ C1C2\nC1 C3\nC C\nand V3 = V ⋅ 1 2\nSimilarly,\nV2 = V ⋅\nΣ C1 C2\nΣ C1 C2\nFig. 5.18\n5.12. Capacitors in Parallel\nIn this case, p.d. across each is the same but charge on each is different (Fig. 5.18).\n∴ Q = Q1 + Q2 + Q3 or CV = C1V + C2V + C3V or C = C1 + C2 + C3\nFor such a combination, dV/dt is the same for all capacitors.\nExample 5.12. Find the Ceq of the circuit shown in Fig. 5.19. All capacitances are in μ F.\n(Basic Circuit Analysis Osmania Univ. Jan./Feb. 1992)\nSolution. Capacitance between C and D = 4 + 1 || 2 = 14/3 μ F.\nCapacitance between A and B i.e. Ceq = 3 + 2 ||\n14/3 = 4.4 μ F\nExample 5.13. Two capacitors of a capacitance\n4 μF and 2 μF respectively, are joined in series\nwith a battery of e.m.f. 100 V. The connections\nare broken and the like terminals of the capacitors are then joined. Find the final charge on\nFig. 5.19\neach capacitor.\nSolution. When joined in series, let V1 and V2 be the voltages across the capacitors. Then as\ncharge across each is the same.\n∴ 4 × V1 = 2V2\n∴ V2 = 2V1 Also V1 + V2 = 100\n∴ V1 + 2V1 = 100\n∴ V1 = 100/3 V and V2 = 200/3 V\n∴ Q1 = Q2 = (200/3) × 2 = (400/3) μ C\n∴ Total charge on both capacitors = 800/3 μ C\nWhen joined in parallel, a redistribution of charge takes place because both capacitors are reduced to a common potential V.\nTotal charge = 800/3 μ C; total capacitance = 4 + 2 = 6 μ F\n800 = 400 volts\n∴\nV =\n3× 6\n9\nCapacitance\n227\nQ1 = (400/9) × 4 = 1600/9 = 178 μ C\nQ2 = (400/9) × 2 = 800/9 = 89 μ C (approx.)\nHence\nExample 5.14. Three capacitors A, B, C have capacitances 10, 50 and 25 μF respectively.\nCalculate (i) charge on each when connected in parallel to a 250 V\nsupply (ii) total capacitance and (iii) p.d. across each when connected in series.\n(Elect. Technology, Gwalior Univ.)\nFig. 5.20\nSolution. (i) Parallel connection is shown in Fig. 5.20 (a).\nEach capacitor has a p.d. of 250 V across it.\nQ1 = C1V = 10 × 250 = 2500 μ C; Q2 = 50 × 250 = 12,500 μC\nQ3 = 25 × 250 = 6,750 μ C.\n(ii) C = C1 + C2 + C3 = 10 + 50 + 25 = 85 μF\n(iii) Series connection is shown in Fig. 5.20 (b). Here charge on\neach capacitor is the same and is equal to that on the equivalent\nsingle capacitor.\n1/C = 1/C1 + 1/C2 + 1/C3 ; C = 25/4 μ F\nQ = CV = 25 × 250/4 = 1562.5 μ F\nQ = C1V1 ; V1 = 1562.5/10 = 156.25 V\nV2 = 1562.5/25 = 62.5 V; V3 = 1562.5/50 = 31.25 V.\nExample 5.15. Find the charges on capacitors in Fig. 5.21 and the p.d. across them.\nSolution. Equivalent capacitance between points A and B is\nC2 + C3 = 5 + 3 = 8 μ F\nCapacitance of the whole combination (Fig. 5.21)\n8× 2\n1.6 μ F\nC =\n8+2\nCharge on the combination is\nQ1 = CV = 100 × 1.6 = 160 μC\nQ 160\n= 80 V ; V2 = 100 − 80 = 20 V\nV1 = 1 =\n2\nC1\nFig. 5.21\n−6\nQ1 = C2V2 = 3 × 10 × 20 = 60 μC\nQ3 = C3V2 = 5 × 10−6 × 20 = 100 μC\nExample 5.16. Two capacitors A and B are connected in series across a 100 V supply and it is\nobserved that the p.d.s. across them are 60 V and 40 V respectively. A capacitor of 2 μF capacitance\nis now connected in parallel with A and the p.d. across B rises to 90 volts. Calculate the capacitance\nof A and B in microfarads.\nSolution. Let C1 and C2 μ F be the capacitances of the two capacitors. Since they are connected\nin series [Fig. 5.22 (a)], the charge across each is the same.\n∴ 60 C1 = 40 C2 or C1/C2 = 2/3\n...(i)\nIn Fig. 5.22 (b) is shown a capacitor of 2 μ F connected across capacitor A. Their combined\ncapacitance = (C1 + 2) μ F\n...(ii)\n∴\n(C1 + 2) 10 = 90 C2 or C1/C2 = 2/3\nPutting the value of C2 = 3C1/2 from (i) in (ii) we get\nC1 + 2\n∴ C1 + 2 = 13.5 C1\n3C1/2 = 9\n228\nElectrical Technology\nC1 = 2/12.4 = 0.16 μ F and\nC2 = (3/2) × 0.16 = 0.24 μ F\nor\n(b)\n(a)\nFig. 5.22\nExample 5.17. Three capacitors of 2 μ F, 5 μ F and 10 μ F have breakdown voltage of 200 V,\n500 V and 100 V respectively. The capacitors are connected in series and the applied direct voltage\nto the circuit is gradually increased. Which capacitor will breakdown first ? Determine the total\n[Bombay Univeristy 2001]\napplied voltage and total energy stored at the point of breakdown.\nSolution. C1 of 2 μF, C2 of 5 μ F, and C3 of 10 μF are connected\nin series. If the equivalent single capacitor is C,\n1/C = 1/C1 + 1/C2 + 1/C3, which gives C = 1.25 μ F\nIf V is the applied voltage,\nV1 = V × C/C1 = V × (1.25 / 2)\n= 62.5 % of V\nV2 = V × (C/C2) = C × (1.25/5) = 25 % of V\nFig. 5.23\nV3 = V × (C/C3) = V × (1.25/10) = 12.5 % of V\nIf V1= 200 volts, V = 320 volts and V2 = 80 volts, V3 = 40 volts.\nIt means that, first capacitor C1 will breakdown first.\n2\n−6\nEnergy stored = 1/2 CV = 1/2 × 1.25 × 10 × 320 × 320 = 0.064 Joule\nExample 5.18. A multiple plate capacitor has 10 plates, each of area 10 square cm and separation\nbetween 2 plates is 1 mm with air as dielectric. Determine the energy stored when voltage of 100\nvolts is applied across the capacitor.\n[Bombay University 2001]\nSolution. Number of plates, n = 10\n(n − 1) ∈0 9 × 8.854 × 10− 12 × 10 × 10− 4\n=\n= 79.7 pF\n−3\nd\n1 × 10\n−12\n= 1/2 × 79.7 × 10 × 100 × 100 = 0.3985 μJ\nC =\nEnergy stored\nExample 5.19. Determine the capacitance between the points A and B in figure 5.24 (a). All\ncapacitor values are in μF.\nFig. 5.24 (a)\nCapacitance\n229\nSolution. Capacitances are being dealt with in this case. For simplifying this, Delta to star\ntransformation is necessary. Formulae for this transformation are known if we are dealing with resistors\nor impedances. Same formulae are applicable to capacitors provided we are aware that capacitive\nreactance is dependent on reciprocal of capacitance.\nFurther steps are given below :\nFig. 5.24 (b)\nFig. 5.24 (c)\nReciprocals of capacitances taken first :\nBetween B-C ⎯\n⎯ 0.05, Between B-D ⎯\n⎯ 0.10\n⎯ 0.05, Sum of these three = 0.20\nBetween C-D ⎯\nFor this delta, star-transformation is done :\nBetween N-C : 0.05 × 0.05/0.20 = 0.0125, its reciprocal = 80 μ F\nBetween N-B : 0.05 × 0.10/0.20 = 0.025, its reciprocal = 40 μ F\nBetween N-D : 0.05 × 0.10/0.20 = 0.025, its reciprocal = 40 μ F\nThis is marked on Fig. 5.24 (c).\nWith series-parallel combination of capacitances, further simplification gives the final result.\nCAB = 16.13 μ F\nNote : Alternatively, with ADB as the vertices and C treated as the star point, star to delta transformation\ncan be done. The results so obtained agree with previous effective capacitance of 16.14 μ F.\nExample 5.20. (a) A capacitor of 10 pF is connected to a voltage source of 100 V. If the\ndistance between the capacitor plates is reduced to 50 % while it remains, connected to the 100 V\nsupply. Find the new values of charge, energy stored and potential as well as potential gradient.\nWhich of these quantities increased by reducing the distance and why ?\n[Bombay University 2000]\nSolution.\n(ii) C = 20 pF, distance halved\n(i) C = 10 pF\nCharge = 1000 p Coul\nCharge = 2000 p-coul\n2\nEnergy = 1/2 CV = 0.05 μ J\nEnergy = 0.10 μ J\nPotential gradient in the second case will be twice of earlier value.\nExample 5.20 (b). A capacitor 5 μ F charged to 10 V is connected with another capacitor of\n10 μ F charged to 50 V, so that the capacitors have one and the same voltage after connection. What\nare the possible values of this common voltage ?\n[Bombay University 2000]\nSolution. The clearer procedure is discussed here.\nInitial charges held by the capacitors are represented by equivalent voltage sources in Fig. 5.25\n(b). The circuit is simplified to that in Fig. 5.25 (c). This is the case of C1 and C2 connected in series\nand excited by a 40-V source. If C is the equivalent capacitance of this series-combination,\n1/C = 1/C1 + C2\n230\nElectrical Technology\nFig. 5.25 (a)\nFig. 5.25 (c) Simplification\nFig. 5.25 (b). Initial charge represented by equiv-source\nFig. 5.25 (d). Final condition\nThis gives C = 3.33 μF\nIn Fig. (c),\nVC1 = 40 × C/C1 = 40 × 3.33/5 = 26.67 volts\nVS1 and VS2 are integral parts of C1 and C2 in Fig. 5.25 (c),\nVoltage across C1 = 10 + 26.67 = 36.67 (A w.r. to 0)\nVoltage acorss C2 = 50 −13.33 = 36.67, (B w.r. to 0)\nThus, the final voltage across the capacitor is 36.67 volts.\nNote : If one of the initial voltages on the capacitors happens to be the opposite to the single equivalent\nsource voltage in Fig. 5.25 (c) will be 60 volts. Proceeding similarly, with proper care about signs, the final\nsituation will be the common voltage will be 30 volts.\n5.13. Cylindrical Capacitor with Compound Dielectric\nSuch a capacitor is shown in Fig. 5.26\nLet\nr1 = radius of the core\nr2 = radius of inner dielectric ε r1\nr3 = radius of outer dielectric ε r2\nObviously, there are two capacitors joined in series.\nNow\n0.024 εr1\n0.024 εr 2\nμF/km and C2 =\nμF/M\nC1 =\nlog10 (r2 /r1)\nlog10 (r3/r2 )\nTotal capacitance of the cable is C =\nC1C2\nC1 + C2\nA cyclindrical\nCapacitor\n231\nCapacitance\nNow for capacitors joined in series, charge is the same.\n∴\nQ = C1V1 = C2V2\nV2\nV1\nor\n=\nC1 ε r1 log10 (r3/r2 )\n=\nC2 ε r1 log10 (r2 / r1)\nFrom this relation, V2 and V1 can be found,\ngmax in inner capacitor\nV1\n2, 3 r1 log10(r2 /r1)\n(Art. 5.9)\nSimilarly, gmax for outer capacitor =\ng max\nV1\nV2\n=\n÷\ng max 2.3 r1 log10(r2 /r1) 2, 3 r2 log10(r3/r2 )\n∴\n=\nV2\n2, 3 r2 log10(r3/r2 )\nV1r2 log10 (r3/r2 ) C2r2 log10 (r3/r2 ) ⎛ V1 C2 ⎞\n×\n=\n×\n∴ =\nV2 r1 log10 (r2 /r1) C1r1 log10 (r2 /r1) ⎜⎝ V2 C1 ⎟⎠\nPutting the values of C1 and C2, we get\ng max 1\ng max 2\n=\nFig. 5.26\ng max 1\n0.024 ε r 2 log10 (r3/r2 ) r2 log10 (r2 /r1)\nε .r\n×\n= ×\n∴\n= r2 2\nlog10 (r3/r2 )\n0.024 εr1\nr1 log10 (r2 /r1)\ng max 2 εr1 . r1\nHence, voltage gradient is inversely proportional to the permittivity and the inner radius of the\ninsulating material.\nExample 5.21. A single-core lead-sheathed cable, with a conductor diameter of 2 cm is designed\nto withstand 66 kV. The dielectric consists of two layers A and B having relative permittivities of 3.5\nand 3 respectively. The corresponding maximum permissible electrostatic stresses are 72 and\n60 kV/cm. Find the thicknesses of the two layers.\n(Power Systems-I, M.S. Univ. Baroda)\nSolution. As seen from Art. 5.13.\ng max 1\n3 × r2\nε r 2 . r2\nor 72 =\nor r2 = 1.4 cm\ng max 2 = ε r1 . r1\n60 3.5 × 1\nV1 × 2\nNow,\ngmax =\n2.3 r1 log10 r2 /r1\nwhere V1 is the r.m.s. values of the voltage across the first dielectric.\nV1 × 2\nor V1 = 17.1 kV\n2.3 × 1 × log10 1.4\n∴\n72 =\nObviously,\nV2 = 60 −17.1= 48.9 kV\nNow,\n∴\n...Art. 5.9\nV2 × 2\n48.9\n∴ 60 =\n2.3 r2 log10 (r3/r2 )\n2.3 × 1.4 log10 (r3/r2 )\nr\nlog10 (r3/r2) = 0.2531 = log10 (1.79) ∴ 3 = 1.79 or r3 = 2.5 cm\nr2\ngmax 2 =\n232\nElectrical Technology\nThickness of first dielectric layer = 1.4 −1.0 = 0.4 cm.\nThickness of second layer = 2.5 −1.4 = 1.1 cm.\n5.14. Insulation Resistance of a Cable Capacitor\nIn a cable capacitor, useful current flows along the axis of the core but there is always present\nsome leakage of current. This leakage is radial i.e. at right angles to the flow of useful current. The\nresistance offered to this radial leakage of current is called\ninsulation resistance of the cable. If cable length is greater,\nthen leakage is also greater. It means that more current will\nleak. In other words, insulation resistance is decreased.\nHence, we find that insulation resistance is inversely\nproportional to the cable length. This insulation resistance\nis not to be confused with conductor resistance which is\ndirectly proportional to the cable length.\nConsider i metre of a single-core cable of inner-radius r1\nand outer radius r2 (Fig. 5.27). Imagine an annular ring of\nIf resistivity of insulating material is ρ, then resistance of\nρ dr\nρdr\n=\n∴Insulation\nthe this narrow ring is dR =\n2πr × l 2πrl\nresistance of l metre length of cable is\nr 2 ρdr\nr2\nρ\nFig. 5.27\ndR =\nor R =\nlog e (r ) r1\n2π rl\nr1 2π rl\n2.3 ρ\nρ\nlog e (r2 /r1) =\nlog10 (r2 /r1) Ω\nR =\n2 πl\n2πl\n∫\n∫\nIt should be noted\n(i) that R is inversely proportional to the cable length\n(ii) that R depends upon the ratio r2/r1 and NOT on the thickness of insulator itself.\nExample 5.22. A liquid resistor consists of two concentric metal cylinders of diameters D = 35\ncm and d = 20 cm respectively with water of specific resistance ρ = 8000 Ω cm between them. The\nlength of both cylinders is 60 cm. Calculate the resistance of the liquid resistor.\n(Elect. Engg. Aligarh Univ.,)\nSolution. r1 = 10 cm ; r2\n= 17.5 cm; log10 (1.75) = 0.243\n3\nρ = 8 × 10 Ω− cm; l = 60 cm.\n3\nResistance of the liquid resistor R = 2.3 × 8 × 10 × 0.243 = 11.85 Ω.\n2π × 60\nExample 5.23. Two underground cables having conductor resistances of 0.7 Ω and 0.5 and\ninsulation resistance of 300 M Ω respectively are joind (i) in series (ii) in parallel. Find the resultant\nconductor and insulation resistance.\n(Elect. Engineering, Calcutta Univ.)\nSolution. (i) The conductor resistance will add like resistances in series. However, the leakage\nresistances will decrease and would be given by the reciprocal relation.\nTotal conductor resistance = 0.7 + 0.5 = 1.2 Ω\nIf R is the combined leakage resistance, then\n1 = 1 + 1\n∴ R = 200 M Ω\nR 300 600\nCapacitance\n233\n(ii) In this case, conductor resistance is = 0.7 × 0.5/(0.7 + 0.5) = 0.3. Ω (approx)\nInsulation resistance = 300 + 600 = 900 M Ω\nExample 5.24. The insulation resistance of a kilometre of the cable having a conductor diameter\nof 1.5 cm and an insulation thickness of 1.5 cm is 500 M Ω. What would be the insulation resistance\nif the thickness of the insulation were increased to 2.5 cm ?\nSolution. The insulation resistance of a cable is\n2.3 ρ\nFirst Case\nR = 2π l log10 (r2 /r1)\nr1 = 1.5/2 = 0.75 cm ; r2 = 0.75 + 1.5 = 2.25 cm\n∴ r2/r1 = 2.25/0.75 = 3 ; log10 (3) = 0.4771 ∴ 500 = 2.3 ρ × 0.4771\n2πl\nSecond Case\nr1 = 0.75 cm −as before r2 = 0.75 + 2.5 = 3.25 cm\n2.4 ρ\n× 0.6368\nr2/r1 = 3.25/0.75 = 4.333 ; log10 (4.333) = 0.6368 ∴ R =\n2πl\nDividing Eq. (ii) by Eq. (i), we get\nR = 0.6368 ; R = 500 × 0.6368 / 0.4771 = 667.4 Μ Ω\n500 0.4771\n5.15. Energy Stored in a Capacitor\nCharging of a capacitor always involves some expenditure of energy by the charging agency. This energy\nis stored up in the electrostatic field set up in the dielectric medium. On discharging the capacitor, the field collapses and the stored energy is released.\nTo begin with, when the capacitor is uncharged, little\nwork is done in transferring charge from one plate to\nanother. But further instalments of charge have to be\ncarried against the repulsive force due to the charge\nalready collected on the capacitor plates. Let us find the\nenergy spent in charging a capacitor of capacitance C to\na voltage V.\nSuppose at any stage of charging, the p.d. across the\nplates is v. By definition, it is equal to the work done in\nshifting one coulomb from one plate to another. If ‘dq’\nis charge next transferred, the work done is\ndW = v.dq\nNow\nq = Cv ∴ dq = C.dv ∴ dW = Cv.dv\nTotal work done in giving V units of potential is\nW =\n∫\nv\n0\n2\nCv.dv = C v\n2\nv\n0\nCapacitors on a motherboard\n∴ W = 1 CV\n2\n2\nQ2\nIf C is in farads and V is in volts, then W = 1 CV 2 joules = 1 QV joules =\njoules\n2C\n2\n2\nIf Q is in coulombs and C is in farads, the energy stored is given in joules.\n...(i)\n...(ii)\n234\nElectrical Technology\nNote : As seen from above, energy stored in a capacitor is E = 1 CV 2\n2\n2\nNow, for a capacitor of plate area A m and dielectric of thickness d metre, energy per unit volume of\ndielectric medium.\n2\n1 CV 2 1 A . V 2 1\nV\n1 E 2 1 DE D 2 / 2 joules/m3 *\nd\n2\n2\nIt will be noted that the formula 12 DE is similar to the expression 12 stress × strain which is used for\ncalculating the mechanical energy stored per unit volume of a body subjected to elastic stress.\nExample 5.25. Since a capacitor can store charge just like a lead-acid battery, it can be used at\nleast theoretically as an electrostatic battery. Calculate the capacitance of 12-V electrostatic battery\nwhich the same capacity as a 40 Ah, 12 V lead-acid battery.\nSolution. Capacity of the lead-acid battery = 40 Ah = 40 × 36 As = 144000 Coulomb\n6\nEnergy stored in the battery = QV = 144000 × 12 = 1.728 × 10 J\n2\n1\nEnergy stored in an electrostatic battery = CV\n2\n∴ 1 × C × 122 = 1.728 × 106 ∴ C = 2.4 × 104 F = 24 kF\n2\nExample 5.26. A capacitor-type stored-energy welder is to deliver the same heat to a single\nweld as a conventional welder that draws 20 kVA at 0.8 pf for 0.0625 second/weld. If C = 2000 μF,\nfind the voltage to which it is charged.\n(Power Electronics, A.M.I.E. Sec B, 1993)\nSolution. The energy supplied per weld in a conventional welder is\nW = VA × cos φ × time = 20,000 × 0.8 × 0.0625 = 1000 J\n2\nNow, energy stored in a capacitor is (1/2) CV\n2 × 1000\n1 CV 2 or V = 2 W =\n= 1000 V\n∴\nW =\n−6\n2\nC\n2000 × 10\nExample 5.27. A parallel-plate capacitor is charged to 50 μC at 150 V. It is then connected to\nanother capacitor of capacitance 4 times the capacitance of the first capacitor. Find the loss of\nenergy.\n(Elect. Engg. Aligarh Univ.)\nSolution. C1 = 50/150 = 1/3 μF ; C2 = 4 × 1/3 = 4/3 μF\nBefore Joining\n1 C V 2 = 1 × ⎛ 1 ⎞ 10− 6 × 1502 = 37.5 × 10− 4 J ; E = 0\nE1 =\n2\n2 1 1 2 ⎜⎝ 3 ⎟⎠\nTotal energy = 37.5 × 10−4 J\nAfter Joining\nWhen the two capacitors are connected in parallel, the charge of 50 μ C gets redistributed and the\ntwo capacitors come to a common potential V.\ntotal charge\n50 μC\n=\n= 30 V\nV =\ntotal capacitance [(1/ 3) + (4 / 3)] μ F\n1 × (1/3) × 10− 6 × 302 = 1.5 × 10− 4 J\nE1 =\n2\n1 × (4/3) × 10− 6 × 302 = 6.0 × 10 − 4 J\nE2 =\n2\n−2\n−4\n−4\nTotal energy\n= 7.5 × 10 J ; Loss of energy = (37.5 −7.5) × 10 = 3 × 10 J\nThe energy is wasted away as heat in the conductor connecting the two capacitors.\n*\nIt is similar to the expression for the energy stored per unit volume of a magnetic field.\nCapacitance\n235\nExample 5.28. An air-capacitor of capacitance 0.005 μ F is connected to a direct voltage of\n500 V, is disconnected and then immersed in oil with a relative permittivity of 2.5. Find the energy\nstored in the capacitor before and after immersion.\n(Elect. Technology : London Univ.)\nSolution. Energy before immersion is\n1 CV 2 = 1 × 0.005 × 10− 6 × 5002 =\n–6\nE1 =\n625 × 10 J\n2\n2\nWhen immersed in oil, its capacitance is increased 2.5 times. Since charge is constant, voltage\nmust become 2.5 times. Hence, new capacitances is 2.5 × 0.005 = 0.0125 μF and new voltage is\n500/2.5 = 200 V.\n1 × 0.0125 × 10− 6 × (200) 2 =\n250 × 10–6 J\nE2 =\n2\nExample 5.29. A parallel-plate air capacitor is charged to 100 V. Its plate separation is 2 mm\nand the area of each of its plate is 120 cm2.\nCalculate and account for the increase or decrease of stored energy when plate separation is\nreduced to 1 mm\n(a) at constant voltage (b) at constant charge.\nSolution. Capacitance is the first case\nε A 8.854 × 10− 12 × 120 × 10− 4\n= 53.1 × 10− 12 F\nC1 = 0 =\n−3\nd\n2 × 10\nCapacitance in the second case i.e. with reduced spacing\nC2 =\n− 12\n8.854 × 10 × 120 × 10\n−3\n1 × 10\n−4\n= 106.2 × 10− 12 F\n(a) When Voltage is Constant\n1\n2\n1\n2\nCV\nCV\n2 2\n2 1\n1 × 1002 × (106.2 − 53.1) × 10−12 =\n=\n26.55 × 10–8 J\n2\nThis represents an increase in the energy of the capacitor. This extra work has been done by the\nexternal supply source because charge has to be given to the capacitor when its capacitance increases,\nvoltage remaining constant.\n(b) When Charge Remains Constant\nChange in stored energy\ndE =\nEnergy in the first case\nE1 =\n2\n1Q ;\nQ2\nEnergy in the second case, E2 = 1\n2 C1\n2 C2\n∴ change in energy is\ndE =\n1 Q 2 ⎛ 1 − 1 ⎞ × 1012 J\n⎜ 53.1 106.2 ⎟\n2\n⎝\n⎠\n1 (C V )2 ⎛ 1 − 1 ⎞ × 1012 J\n2 1 1 ⎜⎝ 53.1 106.2 ⎟⎠\n= 1 (53.1 × 10− 12 ) 2 × 104 × 0.0094 × 1012\n2\n−8\n= 13.3 × 10 joules\nHence, there is a decrease in the stored energy. The reason is that charge remaining constant,\nwhen the capacitance is increased, then voltage must fall with a consequent decrease in stored energy\n(E = 1 QV )\n2\n=\n236\nElectrical Technology\nExample 5.30. A point charge of 100 μC is embedded in an extensive mass of bakelite which\nhas a relative permittivity of 5. Calculate the total energy contained in the electric field outside a\nradial distance of (i) 100 m (ii) 10 m (iii) 1 m and (iv) 1 cm.\nSolution. As per the Coulomb’s law, the electric field intensity at any distance x from the point\n2\ncharge is given by E = Q/4 π ε x . Let us draw a spherical shell of radius x as shown in Fig. Another\nspherical shell of radius (x + dx) has also been drawn. A differential volume of the space enclosed\n2\nbetween the two shells is dv = 4 π x dx. As per Art. 5.15, the energy stored per unit volume of the\nelectric field is (1/2) DE. Hence, differential energy contained in the small volume is\n2\n2\n1 DE d ν = 1 ε E 2 d ν = 1 ε ⎛ Q ⎞ 4 π x 2 dx = Q . dx\n⎜⎜\n⎟\ndW =\n2\n2\n2 ⎝ 4 π ε x 2 ⎟⎠\n8 π ε x2\nTotal energy of the electric field extending from x = R to x = ∞ is\nW =\nQ2\n8πε\n∫\n∞\nR\nx\n−2\ndx =\nQ2\nQ2\n=\n8 π ε R 8 π ε0 ε r R\n(i) The energy contained in the electic field lying outside a radius of R = 100 m is\n−6 2\nW =\n(100 × 10 )\n= 0.90 J\n− 12\n8 π × 8.854 × 10 × 5 × 100\n(ii) For R = 10 m, W = 10 × 0.09 = 0.09 J\n(iii) For R = 1 m, W = 100 × 0.09 = 9 J\n(iv) For R = 1 cm, W = 10,000 × 0.09 = 900 J\nExample 5.31. Calculate the change in the stored energy of a parallel-plate capacitor if a\ndielectric slab of relative permittivity 5 is introduced between its two plates.\nSolution. Let A be the plate area, d the plate separation, E the electric field intensity and D the\nelectric flux density of the capacitor. As per Art. 5.15, energy stored per unit volume of the field is\n= (1/2) DE. Since the space volume is d × A, hence,\n⎛V ⎞\n2\nW1 = 1 D1E1 × dA = 1 ε0 E1 × dA = 1 ε0 dA ⎜ 1 ⎟\n2\n2\n2\n⎝d⎠\nWhen the dielectric slab is introduced,\nW2\n2\n1 D E × dA = 1 ε E 2 × dA = 1 ε ε dA ⎛ V2 ⎞\n=\n2\n⎜d ⎟\n2 2 2\n2\n2 0 r\n⎝ ⎠\n2\n2\n2\n1 ε ε dA ⎛ V2 ⎞ = 1 ε dA ⎛ V1 ⎞ 1 ∴ W = W1\n=\n⎜ε d ⎟\n2\n⎜d⎟ ε\n2 0 r\n2 0\nεr\n⎝ ⎠ r\n⎝ r ⎠\nIt is seen that the stored energy is reduced by a factor of ε r. Hence, change in energy is\n1\ndW = W1 − W2 = W1 ⎛⎜ 1 − 1 ⎞⎟ = W1 ⎛⎜1 − ⎞⎟ = W1 × 4 ∴ dW = 0.8\n5⎠\n5\nεr ⎠\nW1\n⎝\n⎝\nExample 5.32. When a capacitor C charges through a resistor R from a d.c. source voltage E,\ndetermine the energy appearing as heat.\n[Bombay University, 2000]\nSolution. R-C series ciruit switched on to a d.c. source of voltage E, at t = 0, results into a\ncurrent i (t), given by\n−t/τ\ni (t) = (E/R) e\nwhere\nt = RC\nΔ WR = Energy appearing as heat in time Δt\n237\nCapacitance\n2\nΔ WR\n= i R Δt\n= Energy appearing as heat in time Δt\n2\n= i R Δt\nWR = R\n∫\n∞\n0\n2\ni dt\n= R (E/R)\n2\n∫\n∞\n0\n(ε\n2\n) = 1 CE\n2\n− t/τ 2\nNote : Energy stored by the capacitor at the end of charging process = 1/2 CE2\nHence, energy received from the source = CF.\n5.16. Force of Attraction Between Oppositely-charged Plates\nIn Fig. 5.28 are shown two parallel conducting plates A and B\ncarrying constant charges of + Q and −Q coulombs respectively. Let\nthe force of attraction between the two be F newtons. If one of the\nplates is pulled apart by distance dx, then work done is\n= F × dx joules\n...(i)\nSince the plate charges remain constant, no electrical energy comes\ninto the arrangement during the movement dx.\n∴ Work done = change in stored energy\n1 Q2 joules\nInitial stored energy =\n2 C\nFig. 5.28\nIf capacitance becomes (C −dC) due to the movement dx, then\n2\n2\nQ2\n1.Q\n1\n1 Q 1 dC if dC\nFinal stored energy 1\n2 (C dC ) 2 C\n2 C\nC\n1 dC\nC\n2\n2\nQ2 ⎛\ndC ⎞ − 1 Q = 1 Q . dC\n∴ Change in stored energy = 1\n1\n+\n2 C ⎝⎜\n2 C2\nC ⎠⎟ 2 C\n2\n1 Q . dC\nEquating Eq. (i) and (ii), we have F.dx =\n2 C2\n2\n1 Q . dC = 1 V 2 . dC\nF =\n2 C 2 dx 2\ndx\nNow\n∴\nC =\nC\n...(ii)\n(ä V = Q/C)\nεA\nεA\n∴ dC = − 2\nx\ndx\nx\n( ) newtons = − 12 ε A E\n1 2 εA\n1\nV\nF = − V . 2 =− ε A\n2\n2\nx\nx\n2\n2\nnewtons\nThis represents the force between the plates of a parallel-plate capacitor charged to a p.d. of V\nvolts. The negative sign shows that it is a force of attraction.\nExample 5.33. A parallel-plate capacitor is made of plates 1 m square and has a separation of\n1 mm. The space between the plates is filled with dielectric of ε r = 25.0. If 1 k V potential difference\nis applied to the plates, find the force squeezing the plates together.\n(Electromagnetic Theory, A.M.I.E. Sec B, 1993)\n2\nSolution. As seen from Art. 5.16, F = −(1/2) ε 0 ε r AE newton\n−3\n−6\nNow E = V/d = 1000/1 × 10 = 10 V/m\n238\nElectrical Technology\n∴\n2\n− 12\n6 2\n−4\nF = − 1 ε0 εr AE = − 1 × 8.854 × 10 × 25 × 1 × (10 ) = − 1.1 × 10 N\n2\n2\nTutorial Porblems No. 5.2\n1. Find the capacitance per unit length of a cylindrical capacitor of which the two conductors have radii\n2.5 and 4.5 cm and dielectric consists of two layers whose cylinder of contact is 3.5 cm in radius, the\ninner layer having a dielectric constant of 4 and the outer one of 6.\n[440 pF/m]\n2\n2. A parallel-plate capacitor, having plates 100 cm area, has three dielectrics 1 mm each and of\npermittivities 3, 4 and 6. If a peak voltage of 2,000 V is applied to the plates, calculate :\n(a) potential gradient across each dielectric\n(b) energy stored in each dielectric.\n−7\n[8.89 kV/cm; 6.67 kV/cm ; 4.44 kV/cm ; 1047, 786, 524 × 10 joule]\n3. The core and lead-sheath of a single-core cable are separated by a rubber covering. The crosssectional area of the core is 16 mm2. A voltage of 10 kV is applied to the cable. What must be the\nthickness of the rubber insulation if the electric field strength in it is not to exceed 6 × 106 V/m ?\n[2.5 mm (approx)]\n4. A circular conductor of 1 cm diameter is surrounded by a concentric conducting cylinder having an\ninner diameter of 2.5 cm. If the maximum electric stress in the dielectric is 40 kV/cm, calculate the\npotential difference between the conductors and also the minimum value of the electric stress.\n[18.4 kV ; 16 kV/cm]\n5. A multiple capacitor has parallel plates each of area 12 cm2 and each separated by a mica sheet\n0.2 mm thick. If dielectric constant for mica is 5, calculate the capacitance.\n[265.6 μμ\nμμF]\n6. A p.d. of 10 kV is applied to the terminals of a capacitor of two circular plates each having an area of\n100 sq. cm. separated by a dielectric 1 mm thick. If the capacitance is 3 × 10−4 microfarad, calculate\nthe electric flux density and the relative permittivity of the dielectric.\n−\n[D = 3 × 10 4 C/m2, ε r= 3.39] (City & Guilds, London)\n7. Each electrode of a capacitor of the electrolytic type has an area of 0.02 sq. metre. The relative\npermittivity of the dielectric film is 2.8. If the capacitor has a capacitance of 10 μF, estimate the\n−\nthickness of the dielectric film.\n[4.95 × 10 8 m] (I.E.E. London)\n5.17. Current-Voltage Relationships in a Capacitor\nget\nThe charge on a capacitor is given by the expression Q = CV. By differentiating this relation, we\ni =\ndQ d\n= (CV ) = C dV\ndt dt\ndt\nFollowing important facts can be deduced from the above relations :\n(i) since Q = CV, it means that the voltage across a capacitor is proportional to charge, not the\ncurrent.\n(ii) a capacitor has the ability to store charge and hence to provide a short of memory.\n(iii) a capacitor can have a voltage across it even when there is no current flowing.\n(iv) from i = c dV/dt, it is clear that current in the capacitor is present only when voltage on it\nchanges with time. If dV/dt = 0 i.e. when its voltage is constant or for d.c. voltage, i = 0.\nHence, the capacitor behaves like an open circuit.\nCapacitance\n239\n(v) from i = C dV/dt, we have dV/dt = i/C. It shows that for a given value of (charge or discharge) current i, rate of change in voltage is inversely proportional to capacitance. Larger\nthe value of C, slower the rate of change in capacitive voltage. Also, capacitor voltage\ncannot change instantaneously.\n(vi) the above equation can be put as dv = i . dt\nC\nt\nIntegrating the above, we get dv = 1 i . dt or dv = 1 i dt\nC\nC 0\n∫\n∫\n∫\nExample 5.34. The voltage across a 5 μF capacitor changes uniformly from 10 to 70 V in 5 ms.\nCalculate (i) change in capacitor charge (ii) charging current.\nQ = CV ∴dQ = C . dV and i = C dV/dt\ndV = 70 −10 = 60 V, ∴ dQ = 5 × 60 = 300 μ C.\ni = C . dV/dt = 5 × 60/5 = 60 mA\nSolution.\n(i)\n(ii)\nExample 5.35. An uncharged capacitor of 0.01 F is charged first by a current of 2 mA for 30\nseconds and then by a current of 4 mA for 30 seconds. Find the final voltage in it.\nSolution. Since the capacitor is initially uncharged, we will use the principle of Superposition.\n1\n0.01\n1\nV2 =\n0.01\nV1 =\n∫\n∫\n30\n0\n30\n0\n2 × 10\n−3\n. dt = 100 × 2 × 10\n−3\n. dt = 100 × 4 × 10\n4 × 10\n−3\n× 30 = 6 V\n−3\n× 30 = 12 V ; ∴ V = V1 + V2 = 6 + 12 = 18 V\nExample 5.36. The voltage across two series-connected 10 μ F capacitors changes uniformly\nfrom 30 to 150 V in 1 ms. Calculate the rate of change of voltage for (i) each capacitor and\n(ii) combination.\nSolution. For series combination\nC2\nC1\nV1 = V\n= V and V2 = V .\n= 2V\n3\nC1 + C2 3\nC1 + C2\nWhen V = 30 V V1 = V/3 = 30/3 = 10 V ; V2 = 2V/3 = 2 × 30/3 = 20 V\nWhen V = 150 V V1 = 150/3 = 50 V and V2 = 2 × 150/3 = 100 V\ndV1\ndV\n(50 − 10)\n(100 − 20) V\n= 40 kV/s ; 2 =\n= 80 kV/s\n(i) ∴\n=\ndt\n1 ms\ndt\n1 ms\n(150 − 30)\ndV\n= 120 kV/s\n(ii)\n=\n1 ms\ndt\nIt is seen that dV/dt = dV1/dt + dV2/dt.\n5.18. Charging of a Capacitor\nIn Fig. 5.29. (a) is shown an arrangement by which a capacitor C may be charged through a high\nresistance R from a battery of V volts. The voltage across C can be measured by a suitable voltmeter.\nWhen switch S is connected to terminal (a), C is charged but when it is connected to b, C is short\ncircuited through R and is thus discharged. As shown in Fig. 5.29. (b), switch S is shifted to a for\ncharging the capacitor for the battery. The voltage across C does not rise to V instantaneously but\nbuilds up slowly i.e. exponentially and not linearly. Charging current ic is maximum at the start i.e.\nwhen C is uncharged, then it decreases exponentially and finally ceases when p.d. across capacitor\nplates becomes equal and opposite to the battery voltage V. At any instant during charging, let\nvc = p.d. across C; ic = charging current\nq = charge on capacitor plates\n240\nElectrical Technology\nFig. 5.29\nThe applied voltage V is always equal to the sum of :\n(i) resistive drop (ic R) and (ii) voltage across capacitor (vc)\n∴\nV = ic R + vc\nNow\nic =\nor\nIntegrating both sides, we get\n...(i)\ndv\ndv\ndq d\n= (Cvc ) = C c ∴ V = vc + CR c\ndt dt\ndt\ndt\ndvc\n−\n= − dt\nV − vc\nCR\n− d Vc\n∫V − v\nc\n= − 1 dt ; ∴ log c (V − vc ) = − t +K\nCR\nCR\n∫\n...(ii)\n...(iii)\nwhere K is the constant of integration whose value can be found from initial known conditions. We\nknow that at the start of charging when t = 0, vc = 0.\nSubstituting these values in (iii), we get logc V = K\nHence, Eq. (iii) becomes loge (V −vc) =\nV − vc\nV\n−t\n+ log e V\nCR\n−t\n= − 1 where λ = CR = time constant\nCR\nλ\nV − vc\n− t/λ\n− t /λ\n=e\nor vc = V (1 − e )\n∴\n...(iv)\nV\nThis gives variation with time of voltage across the capacitor plates and is shown in Fig. 5.27.(a)\nor\nlog c\n=\nCapacitance\n241\nFig. 5.30\nNow\nvc = q/C and V = Q/C\nEquation (iv) becomes q = Q (1 − e− t /λ ) ∴ q = Q (1 − e− t/λ )\n...(v)\nc c\nWe find that increase of charge, like growth of potential, follows an exponential law in which the\nsteady value is reached after infinite time (Fig. 5.30 b). Now, ic = dq/dt.\nDifferentiating both sides of Eq. (v), we get\ndq\n⎛ 1 − t/λ ⎞\n− t/λ\nd\n= ic = Q (1 − e ) = Q ⎜ + e\n⎟\ndt\ndt\n⎝ λ\n⎠\nQ − t/λ CV − t/λ\n=\ne\ne\n=\n(ä Q = CV and λ = CR)\nλ\nCR\nV . e − t/λ or i = I e − t/λ\n∴\nic =\n...(vi)\nc\no\nR\nwhere I0 = maximum current = V/R\nExponentially rising curves for vc and q are shown in Fig. 5.30 (a) and (b) respectively.\nFig. 5.30 (c) shows the curve for exponentially decreasing charging current. It should be particularly\nnoted that ic decreases in magnitude only but its direction of flow remains the same i.e. positive.\nAs charging continues, charging current decreases according to equation (vi) as shown in Fig.\n5.30 (c). It becomes zero when t = ∞ (though it is almost zero in about 5 time constants). Under\nsteady-state conditions, the circuit appears only as a capacitor which means it acts as an open-circuit.\nSimilarly, it can be proved that vR decreases from its initial maximum value of V to zero exponentially\nas given by the relation vR = V e−t/λ.\n5.19. Time Constant\n(a) Just at the start of charging, p.d. across capacitor is zero, hence from (ii) putting vc = 0, we get\ndv\nV = CR c\ndt\n⎛ dv ⎞\n∴ initial rate of rise of voltage across the capacitor is* = ⎜ c ⎟\n= V = V volt/second\n⎝ dt ⎠t = 0 CR λ\nIf this rate of rise were maintained, then time taken to reach voltage V would have been\nV + V/CR = CR. This time is known as time constant (λ) of the circuit.\n*\nIt can also be found by differentiating Eq. (iv) with respect to time and then putting t = 0.\n242\nElectrical Technology\nHence, time constant of an R-C circuit is defined as the time during which voltage across capacitor would have reached its maximum value V had it maintained its initial rate of rise.\n(b) In equation (iv) if t = λ, then\n1 ⎞\n⎛ 1⎞\n⎛\nvc = V (1 − e − t/λ ) = V (1 − e− t/λ ) = V (1 − e − 1) = V ⎜1 − ⎟ = V ⎜ 1 −\n⎟ = 0.632 V\ne\n2.718\n⎝\n⎠\n⎝\n⎠\nHence, time constant may be defined as the time during which capacitor voltage actually rises\nto 0.632 of its final steady value.\n(c) From equaiton (vi), by putting t = λ, we get\n−λ/λ\n−1\nic = I0 e\n= I0 e = I0/2.718 ≅ 0.37 I0\nHence, the constant of a circuit is also the time during which the charging current falls to 0.37\nof its initial maximum value (or falls by 0.632 of its initial value).\n5.20. Discharging of a Capacitor\nAs shown in Fig. 5.31 (a), when S is shifted to b, C is discharged through R. It will be seen that\nthe discharging current flows in a direction opposite to that the charging current as shown in Fig.\n5.31(b). Hence, if the direction of the charging current is taken positive, then that of the discharging\ncurrent will be taken as negative. To begin with, the discharge current is maximum but then decreases\nexponentially till it ceases when capacitor is fully discharged.\n(b)\n(a)\nFig. 5.31\nSince battery is cut of the circuit, therefore, by putting V = 0 in equation (ii) of Art. 5.18, we get\ndvc ⎞\n⎛\ndv\ndv\n0 = CR c vc or vc\nCR c\n⎜ ic = C dt ⎟\ndt\ndt\n⎝\n⎠\ndvc\n1 dt\ndt or dvc\nt\nlog e ve\nvc = CR\nvc\nCR\nCR\nAt the start of discharge, when t = 0, vc = V ∴loge V = 0 + K ; or loge V = K\nPutting this value above, we get\n∴\nloge\nor\nSimilarly,\nIt can be proved that\nk\nt\nvc = − + log e V or log e vc /V = − t/λ\nλ\nvc\nV\n= e−t/λ\n− t/λ\nq = Qe\nor vc = Ve−t/λ\nand\nic = − I0 e\n− t/λ\nvR = − V e− t/λ\nThe fall of capacitor potential and its discharging current are shown in Fig. 5.32 (b).\nOne practical application of the above charging and discharging of a capacitor is found in digital\nCapacitance\n243\ncontrol circuits where a square-wave input is applied across an\nR-C circuit as shown in Fig. 5.32 (a). The different waveforms\nof the current and voltages are shown in Fig. 5.32 (b), (c), (d),\n(e). The sharp voltage pulses of VR are used for control\ncircuits.\nExample 5.37. Calculate the current in and voltage drop\nacross each element of the circuit shown in Fig. 5.33 (a) after\nswitch S has been closed long enough for steady-state\nconditions to prevail.\nAlso, calculate voltage drop across the capacitor and the\ndischarge current at the instant when S is opened.\nSolution. Under steady-state conditions, the capacitor becomes fully charged and draws no current. In fact, it acts like\nan open circuit with the result that no current flows through the\n1-Ω resistor. The steady state current ISS flows through loop\nABCD only.\nHence,\nISS = 100/(6 + 4) = 10 A\nDrop\nV6 = 100 × 6/(6 + 4) = 60 V\nV4 = 100 × 4/10 = 40 V\nV1 = 0 × 2 = 0 V\nVoltage across the capacitor = drop across B −C = 40 V\nFig. 5.32\nFig. 5.33\nSwitch Open\nWhen S is opened, the charged capacitor discharges through the loop BCFE as shown in Fig.\n5.33 (b). The discharge current is given by\nID = 40/(4 + 1) = 8 A\nAs seen, it flows in a direction opposite to that of ISS.\nExample 5.38. (a) A capacitor is charged through a large non-reactive resistance by a battery\nof constant voltage V. Derive an expression for the instantaneous charge on the capacitor.\n(b) For the above arrangement, if the capacitor has a capacitance of 10 μ F and the resistance\nis 1 M Ω, calculate the time taken for the capacitor to receive 90% of its final charge. Also, draw the\ncharge/time curve.\nSolution. (a) For this part, please refer to Art. 5.18.\n−6\n6\n(b) λ = CR = 10 × 10 × 1 × 10 = 10 s ; q = 0.9 Q\n− t/l\n− t/10\nt/10\nNow, q = Q (1 − e ) ∴ 0.9 Q = Q (1 − e\n) or e = 10\n∴ 0.1 t loge e = loge 10 or 0.1 t = 2.3 log10 10 = 2.3 or t = 23 s\n244\nElectrical Technology\nThe charge/time curve is similar to that shown in Fig. 5.27 (b).\nExample 5.39. A resistance R and a 4 μF capacitor are connected in series across a 200 V. d.c.\nsupply. Across the capacitor is a neon lamp that strikes (glows) at 120 V. Calculate the value of R to\nmake the lamp strike (glow) 5 seconds after the switch has been closed.\n(Electrotechnics-I.M.S. Univ. Baroda)\nSolution. Obviously, the capacitor voltage has to rise 120 V in 5 seconds.\n∴ 120 = 200 (1 −e−5/λ) or e5/λ = 2.5 or λ = 5.464 second.\n−6\nΩ\nNow, λ = CR ∴ R = 5.464/4 × 10 = 1.366 MΩ\nExample 5.40. A capacitor of 0.1 μF is charged from a 100-V battery through a series resistance of 1,000 ohms. Find\n(a) the time for the capacitor to receive 63.2 % of its final charge.\n(b) the charge received in this time (c) the final rate of charging.\n(d) the rate of charging when the charge is 63.2% of the final charge.\n(Elect. Engineering, Bombay Univ.)\nSolution. (a) As seen from Art. 5.18 (b), 63.2% of charge is received in a time equal to the time\nconstant of the circuit.\n−4\n−6\n−3\nTime required = λ = CR = 0.1 × 10 × 1000 = 0.1 × 10 = 10 second\n(b) Final charge, Q = CV = 0.1 × 100 = 10 μC\nCharge received during this time is = 0.632 × 10 = 6.32 μ C\n(c) The rate of charging at any time is given by Eq. (ii) of Art. 5.18.\nV −v\ndv\n=\nCR\ndt\ndv\nV =\n100\n= 106 V/s\nInitially\nv = 0, Hence\n=\nCR 0.1 × 10− 6 × 103\ndt\n(d) Here\nv = 0.632 V = 0.632 × 100 = 63.2 volts\n100 − 63.2\ndv\n= 368 kV/s\n=\n∴\ndt\n10 − 4\nExample 5.41. A series combination having R = 2 M Ω and C = 0.01 μF is connected across a\nd.c. voltage source of 50 V. Determine\n(a) capacitor voltage after 0.02 s, 0.04 s, 0.06 s and 1 hour\n(b) charging current after 0.02 s, 0.04 s, 0.06 s and 0.1 s.\n6\n−6\nλ = CR = 2 × 10 × 0.01 × 10 = 0.02 second\n6\nIm = V/R = 50/2 × 10 = 25 μA.\nWhile solving this question, it should be remembered that (i) in each time constant, vc increases\nfurther by 63.2% of its balance value and (ii) in each constant, ic decreases to 37% its previous value.\n(a) (i) t = 0.02 s\nSince, initially at\nt = 0, vc = 0 V and Ve = 50 V, hence, in one time constant\nvc = 0.632 (50 −0) = 31.6 V\n(ii) t = 0.04 s\nThis time equals two time-constants.\n∴\nvc = 31.6 + 0.632 (50 −31.6) = 43.2 V\n(iii) t = 0.06 s\nThis time equals three time-constants.\n∴\nvc = 43.2 + 0.632 (50 −43.2) = 47. 5 V\nSolution.\nCapacitance\n245\nSince in one hour, steady-state conditions would be established, vc would have achieved its\nmaximum possible value of 50 V.\n(b) (i) t = 0.02 s,\nic = 0.37 × 25 = 9.25 μA\n(ii) t = 0.4 s,\nic = 0.37 × 9.25 = 3.4 μA\n(iii) t = 0.06 s,\nic = 0.37 × 3.4 = 1.26 μA\n(iv) t = 0.1 s, This time equals 5 time constants. In this time, current falls almost to zero\nvalue.\nExample 5.42. A voltage as shown in Fig. 5.43 (a) is applied to a series circuit consisting of a\nresistance of 2 Ω in series with a pure capacitor of 100 μF. Determine the voltage across the capacitor\nat t = 0.5 millisecond.\n[Bombay University, 2000]\nFig. 5.34 (a)\nSolution.\nFig. 5.34 (b)\nτ = RC = 0.2 milli-second\nBetween 0 and 0.2 m sec;\nv (t) = 10 [1 −exp (−t/τ )]\nAt t = 0.2, v (t) = 6.32 volts\nBetween 0.2 and 0.4 m Sec, counting time from A indicating it as t1\nv (t1) = 6.32 exp (t1/τ )\nAt point B, t1 = 0.2, V = 2.325\nBetween 0.4 and 0.6 m Sec, time is counted from β with variable as t2,\nv (t2) = 2.325 + (10 − 2.325) [1 − exp (− t2/τ )]\nAt C,\nt2 = 0.2, V = 7.716 volts.\n5.21. Transient Relations During Capacitor Charging Cycle\nWhenever a circuit goes from one steady-state condition to another steady-state condition, it\npasses through a transient state which is of short duration. The first steady-state condition is called\nthe initial condition and the second steady-state condition is called the final condition. In fact,\ntransient condition lies in between the initial and final conditions. For example, when switch S in Fig.\n5.35 (a) is not connected either to a or b, the RC circuit is in its initial steady state with no current and\n246\nElectrical Technology\nhence no voltage drops. When S is shifted to point a, current starts flowing through R and hence,\ntransient voltages are developed across R and C till they achieve their final steady values. The period\nduring which current and voltage changes take place is called transient condition.\nThe moment switch S is shifted to point ‘a’ as shown in Fig. 5.35 (b), a charging current ic is set\nup which starts charging C that is initially uncharged. At the beginning of the transient state, ic is\nmaximum because there is no potential across C to oppose the applied voltage V. It has maximum\nvalue = V/R = I0. It produces maximum voltage drop across R = ic R = I0R. Also, initially, vc = 0, but\nas time passes, ic decreases gradually so does vR but vc increases exponentially till it reaches the final\nsteady value of V. Although V is constant, vR and vc are variable. However, at any time V = vR + vc =\nicR + vc.\nAt the beginning of the transient state, ic = I0, vc = 0 but vR = V. At the end of the transient state,\nic = 0 hence, vR = 0 but vc = V.\n(a)\nby\n(b)\nThe initial rates of change of vc, vR and ic are given\n⎛ dvc ⎞\nV volt/second,\n=\n⎜ dt ⎟\nλ\n⎝\n⎠t = 0\nI R\n⎛ dvR ⎞\nV\n= 0 = − volt/second\n⎜ dt ⎟\nλ\nλ\n⎝\n⎠t = 0\n⎛ dic ⎞\nI\nV\n= 0 where I 0 =\n⎜ dt ⎟\nλ\nR\n⎝\n⎠t = 0\nThese are the initial rates of change. However, their\n(c)\nrate of change at any time during the charging transient\nFig. 5.35\nare given as under :\ndvc\nV e− t/λ ; dic = − dvR = − V e − t/λ\n=\ndt\ndt\ndt\nλ\nλ\nIt is shown in Fig. 5.35 (c).\nIt should be clearly understood that a negative rate of change means a decreasing rate of change.\nIt does not mean that the concerned quantity has reversed its direction.\n5.22. Transient Relations During Capacitor Discharging Cycle\nAs shown in Fig. 5.36 (b), switch S has been shifted to b. Hence, the capacitor undergoes the\ndischarge cycle. Just before the transient state starts, ic = 0, vR = 0 and vc = V. The moment transient\nCapacitance\n247\nstate begins, ic has maximum value and decreases exponentially to zero at the end of the transient\nstate. So does vc. However, during discharge, all rates of change have polarity opposite to that during\ncharge. For example, dvc/dt has a positive rate of change during charging and negative rate of change\nduring discharging.\nFig. 5.36\nAlso, it should be noted that during discharge, vc maintains its original polarity whereas ic reverses\nits direction of flow. Consequently, during capacitor discharge, vR also reverses its direction.\nThe various rates of change at any time during the discharge transients are as given in Art.\ndvc\nV − t/λ ; dic = I 0 e − t/λ ; dvR = V e− t/λ\n= − e\ndt\ndt\ndt\nλ\nλ\nλ\nThese are represented by the curves of Fig. 5.32.\n5.23. Charging and Discharging of a capacitor with Initial Charge\nIn Art. 5.18, we considered the case when the capacitor was initially uncharged and hence, had\nno voltage across it. Let us now consider the case, when the capacitor has an initial potential of V0\n(less than V) which opposes the applied battery voltage V as shown in Fig. 5.37 (a).\nAs seen from Fig. 5.37 (b), the initial rate of rise of vc is now somewhat less than when the\ncapacitor is initially uncharged. Since the capacitor voltage rises from an initial value of v0 to the\nfinal value of V in one time constant, its initial rate of rise is given by\nV − V0 V − V0\n⎛ dvc ⎞\n=\n=\n⎜ dt ⎟\nλ\nRC\n⎝\n⎠t = 0\n248\nElectrical Technology\nFig. 5.37\nThe value of the capacitor voltage at any time during the charging cycle is given by\nvc = (V − V0)(1− e− t/λ) + V0\nFig. 5.38\nHowever, as shown in Fig. 5.38 (a), if the initial capacitor voltage is negative with respect to the\nbattery voltage i.e. the capacitor voltage is series aiding the battery voltage, rate of change of vc is\nsteeper than in the previous case. It is so because as shown in Fig. 5.38 (b), in one time period, the\nvoltage change = V −(−V0) = (V + V0). Hence, the initial rate of change of voltage is given by\nV + V0 V + V0\n⎛ dvc ⎞\n=\n=\n⎜ dt ⎟\nλ\nRC\n⎝\n⎠t = 0\nThe value of capacitor voltage at any time during the charging cycle is given by\n− t/λ\nvc = (V + V0) (1 − e ) − V0\nThe time required for the capacitor voltage to attain any value of vc during the charging cycle is\ngiven by\n⎛ V − V0 ⎞\n⎛ V − V0 ⎞\nt = λ ln ⎜\n= RC ln ⎜\n⎟\n⎜ V − v c ⎟⎟\n⎝ V − vc ⎠\n⎝\n⎠\n⎛ V + V0 ⎞\n⎛ V + V0 ⎞\nt = λ ln ⎜\n⎟ = RC ln ⎜⎜ V − v ⎟⎟\nV\nv\n−\nc ⎠\nc⎠\n⎝\n⎝\n... when V0 is positive\n... when V0 is negative\nExample 5.43. In Fig. 5.39, the capacitor is initially uncharged and the switch S is then closed.\nFind the values of I, I1, I2 and the voltage at the point A at the start and finish of the transient state.\nCapacitance\n249\nSolution. At the moment of closing the\nswitch i.e. at the start of the transient state, the\ncapacitor acts as a short-circuit. Hence, there\nis only a resistance of 2 Ω in the circuit because\n1 Ω resistance is shorted out thereby grounding\npoint A. Hence, I1 = 0; I = I2 = 12/2 = 6A.\nObviously, VA = 0 V.\nAt the end of the transient state, the capacitor acts as an open-circuit. Hence,\nFig. 5.39\nI2 = 0 and I = I1 = 12/(2 + 1)\n= 4 A. VA = 6 V.\nExample 5.44. Calculate the values of i2, i3, v2, v3, va, vc and vL of the network shown in Fig.\n5.40 at the following times :\n(i) At time, t = 0 + immediately after the switch S is closed ;\n(ii) At time, t →∞ i.e. in the steady state. (Network Analysis AMIE Sec. B Winter 1990)\nSolution. (i) In this case the coil acts as an open\ncircuit, hence i2 = 0 ; v2 = 0 and vL = 20 V.\nSince a capacitor acts as a short circuit i3 = 20/(5 + 4)\n= 9 = 20/9 A. Hence, v3 = (20/9) × 4 = 80/9 V and vc = 0.\n(ii) Under steady state conditions, capacitor acts as\nan open circuit and coil as a short circuit. Hence, i2 = 20/\n(5 + 7) = 20/12 = 5/3 A; v2 = 7 × 5/3 = 35/3 V; vL = 0.\nAlso i3 = 0, v3 = 0 but vc = 20 V.\nExample 5.45. If in the RC circuit of Fig. 5.36;\nR = 2 M Ω, C = 5 m F and V = 100 V, calculate\n(a) initial rate of change of capacitor voltage\nFig. 5.40\n(b) initial rate of change of capacitor current\n(c) initial rate of change of voltage across the 2 M Ω resistor\n(d) all of the above at t = 80 s.\nSolution. (a)\n(b)\n(c)\n⎛ dvc ⎞\nV\n100\n100\n=\n⎜ dt ⎟\n6\n6\n10\n⎝\n⎠t = 0\n2 10 5 10\n6\n⎛ dic ⎞\nI0\n100/2 10\nV/R\n=\n⎜ dt ⎟\n10\n⎝\n⎠t = 0\ndv\n⎛ R⎞\nV\n100\n=\n–10 V/s\n⎜ dt ⎟\n10\n⎝\n⎠t = 0\n10 V/s\n–5μ\nμA/s\n(d) All the above rates of change would be zero because the transient disappears after about\n5 λ = 5 × 10 = 50 s.\nExample 5.46. In Fig. 5.41 (a), the capacitor C is fully discharged, since the switch is in\nposition 2. At time t = 0, the switch is shifted to position 1 for 2 seconds. It is then returned to\nposition 2 where it remains indefinitely. Calculate\n(a) the maximum voltage to which the capacitor is charged when in position 1.\n(b) charging time constant λ1 in position 1.\n(c) discharging time constant λ2 in position 2.\n(d) vc and ic at the end of 1 second in position 1.\n250\nElectrical Technology\n(e) vc and ic at the instant the switch is shifted to positon 2 at t = 1 second.\n(f) vc and ic after a lapse of 1 second when in position 2.\n(g) sketch the waveforms for vc and ic for the first 2 seconds of the above switching sequence.\nSolution. (a) We will first find the voltage available at terminal 1. As seen the net battery\nvoltage around the circuit = 40 −10 = 30 V. Drop across 30 K resistor = 30 × 30/(30 + 60) = 10 V.\nHence, potential of terminal 1 with respect to ground G = 40 −10 = 30 V. Hence, capacitor will\ncharge to a maximum voltage of 30 V when in position 1.\n(b) Total resistance, R = [(30 K || 60 K) + 10 K] = 30 K\n∴ λ1 = RC = 30 K × 10 μF = 0.3 s\n(c) λ2 = 10 K × 10 μ F = 0.1 s\n−t/λ1\n−1/0.3\n(d) vC = V (1 −e\n) = 30 (1 −e\n) = 28.9 V\niC = V e\nR\n− t/λ 1\n=\n30 V − 1/0.03\ne\n= 1 × 0.0361 = 0.036 mA\n30 K\n+\n+\n(e) vC = 28.9 V at t = 1 S at position 2 but iC = −28.9 V/10 K = −2/89 mA at t = 1 s in position 2.\n− t/λ 2\n= 28.9 e − 1/0.1 = 0.0013 V = 0 V.\n− t /λ 2\n= − 2.89 e − 1/0.1 = 0.00013 mA ≅ 0.\n(f) vC = 28.9 e\niC = 28.9 e\nThe waveform of the capacitor voltage and charging current are sketched in Fig. 5.41 (b).\nFig. 5.41\nExample 5.47. In the RC circuit of Fig. 5.42, R = 2 M Ω and C = 5 μ F, the capacitor is charged\n+\nto an initial potential of 50 V. When the switch is closed at t = 0 , calculate\n(a) initial rate of change of capacitor voltage and\n(b) capacitor voltage after a lapse of 5 times the time constant i.e. 5λ.\nCapacitance\n251\nIf the polarity of capacitor voltage is reversed,\ncalculate\n(c) the values of the above quantities and\n(d) time for vc to reach −10 V, 0 V and 95 V.\nSolution. (a)\n⎛ dvc ⎞\nV − V0\n=\n⎜ dt ⎟\nλ\n⎝\n⎠t = 0\nV − V0 100 − 50\n=\n= 5 V/s\nRC\n10\n− t/λ\nFig. 5.42\n(b) vC = (V −V0) (1 −e ) + V0\n−5 λ / λ\n= (100 −50) (1−e\n) = 50 = 49.7 + 50 = 99.7 V\nV − (− V0 ) V + V0 150\n⎛ dv ⎞\n=\n=\n=\n= 15 V/s\n(c) When\nV0 = − 50 V, ⎜ c ⎟\ndt\nλ\nλ\n10\n⎝\n⎠t = 0\n=\n(d)\nvC = (V − V0) (1 − e− t/λ) + V0 = [100 − (− 50)] (1 − e− 5) + (− 50)\n−5\n= 150 (1 − e ) − 50 = 99 V.\n⎛ V − V0 ⎞\n⎡100 − (− 50) ⎤\n⎛ 150 ⎞\nt = λ ln ⎜\n⎟ = 10 ln ⎢ 100 − (− 10) ⎥ = 10 ln ⎜ 110 ⎟ = 3.1 s\n−\nV\nv\n⎝\n⎠\n⎣\n⎦\nc ⎠\n⎝\n⎡100 − (− 50) ⎤\n⎛ 150 ⎞\nt = 10 ln ⎢\n⎥ = 10 ln ⎜ 100 ⎟ = 4.055 s\n−\n100\n(0)\n⎣\n⎦\n⎝\n⎠\n⎡100 − (− 50) ⎤\n⎛ 150 ⎞\nt = 10 ln ⎢\n⎥ = 10 ln ⎜ 5 ⎟ = 34 s\n⎣ 100 − 95 ⎦\n⎝\n⎠\nExample 5.48. The uncharged capacitor, if it is\ninitially switched to position 1 of the switch for 2 sec\nand then switched to position 2 for the next two seconds. What will be the voltage on the capacitor at\nthe end of this period ? Sketch the variation of voltage across the capacitor.[Bombay University 2001]\nSolution. Uncharged capacitor is switched to\nposition 1 for 2 seconds. It will be charged to 100\nvolts instantaneously since resistance is not present\nin the charging circuit. After 2 seconds, the capacitor\ncharged to 100 volts will get discharged through R-C\nFig. 5.43\ncircuit with a time constant of\n−3\nτ = RC = 1500 × 10 = 1.5 sec.\nCounting time from instant of switching over to positon 2, the expression for voltage across the\ncapacitor is V (t) = 100 exp (−t/τ )\nAfter 2 seconds in this position,\nv (t) = 100 exp (−2/1.5) = 26/36 Volts.\nExample 5.49. There are three passive elements in the circuit below and a voltage and a current are defined for each. Find the values of these six qualities at both t = 0− and t = 0+.\n[Bombay University, 2001]\nSolution. Current source 4 u (t) means a step function of 4 amp applied at t = 0. Other current\nsource of 5 amp is operative throughout.\n–\nAt t = 0 , 5 amp source is operative. This unidirectional constant current establishes a steady\ncurrent of 5 amp through 30-ohm resistor and 3-H inductor. Note that positive VR means a rise from\nright to left.\n252\nAt\nElectrical Technology\nt\nVR\niL\nVL\niC\nVC\n=\n=\n=\n=\n=\n=\n=\n0\n− 150 Volts (Since right-terminal of Resistor is + ve)\n5 amp\n0, it represents the voltage between B and O.\n0\n150 volts = VBO + (Voltage between A and B with due regards to sign).\n0 − (− 150) = + 150 volts\nFig. 5.44 (a)\nAt t = O+, 4 amp step function becomes operative. Capacitive-voltage and Inductance-current\ncannot change abruptly.\nHence iL (0+) = 5 amp\nVC(O+) = 150 amp\nVC(O+) = 150 volts, with node A positive with respect to 0.\nWith these two values known, the waveforms for current sources are drawn in Fig. 5.44 (b).\nFig. 5.44 (b)\nFig. 5.44 (c)\nRemaining four parameters are evaluated from Fig. 5.44 (c).\nVL = VB = VA −(30 × 1) = 120 Volts\niR = 1 amp, VR = − 30 Volts\niC = 4 amp in downward direction.\nAdditional Observation. After 4 amp source is operative, final conditions (at t tending to\ninfinity) are as follows.\nInductance carries a total direct current of 9 amp, with VL = 0.\nHence,\nVB = 0.\niR = 5 amp, VR = − 150 volts\nVC = 150 volts, iC = 0\nExample 5.50. The voltage as shown in Fig. 5.45 (a) is applied across −(i) A resistor of 2 ohms\n(ii) A capacitor of 2 F. Find and sketch the current in each case up to 6 seconds.\nCapacitance\n253\nFig. 5.45 (a)\n[Bombay University 1998]\nSolution.\nFig. 5.45 (b) Current in a Resistor of 2 ohms iR = V (t)/2 amp\nFig. 5.45 (c) Current thro 2-F capacitor, iC = C (dv/dt)\nExample 5.51. Three capacitors 2 μF, 3 μF, and 5 μF are connected in series and charged from\na 900 V d.c. supply. Find the voltage across condensers. They are then disconnected from the\nsupply and reconnected with all the + ve plates connected together and all the −ve plates connected\ntogether. Find the voltages across the combinations and the charge on each capacitor after\nreconnections. Assume perfect insulation.\n[Bombay University, 1998]\nSolution. The capacitors are connected in series. If C is the resultant capacitance.\nI/C = I/C1 + I/C2 = I/C3, which gives C = (30/31) μF\nV1 = 900 × (30/31)/2 = 435.5 volts\nV2 = 900 × (30/31)/3 = 290.3 volts\nV3 = 900 × (30/31)/5 = 174.2 volts\n254\nElectrical Technology\nFig. 5.46\nIn series connection, charge held by each capacitor is same. If it is denoted by Q.\n−6\nQ = 435 × 2 × 10 = 871 μ coulombs\nThree capacitors hold a total charge of (3 × 871) = 2613 μ coulombs\nWith parallel connection of these three capacitors, equivalent capacitance, C’= C1 + C2 + C3 = 10μF\n−6\n−6\nSince,\nQ’ = C’, 2613 × 10 = 10 × 10 × V’\nor\nV’ = 261 volts.\nCharge on each capacitor after reconnection is as follows :\n−6\nQ1’ = C1 V1 = 2 × 10 × 261 = 522 μ-coulombs\n−6\nQ2’ = C2 V1 = 3 × 10 × 261 = 783 μ-coulombs\n−6\nQ3’ = C3 V2 = 5 × 10 × 261 = 1305 μ-coulombs\nTutorial Problems No. 5.3\n1. For the circuit shown in Fig. 5.47 calculate (i) equivalent capacitance and (ii) voltage drop across\neach capacitor. All capacitance values are in μF.\n[(i) 6 μF (ii) VAB = 50 V, VBC = 40 V]\n2. In the circuit of Fig. 5.48 find (i) equivalent capacitance (ii) drop across each capacitor and\n(iii) charge on each capacitor. All capacitance values are in μF.\n[(i) 1.82 μF (ii) V1 = 50 V; V2 = V3 = 20 V; V4 = 40 V\n(iii) Q1 = 200 μC; Q2 = 160 μC; Q3 = 40 μC; Q4 = 200 μC]\nFig. 5.47\nFig. 5.48\nFig. 5.49\nFig. 5.50\n3. With switch in Fig. 5.49 closed and steady-state conditions established, calculate (i) steady-state\ncurrent (ii) voltage and charge across capacitor (iii) what would be the discharge current at the instant\nof opening the switch ?\n[(i) 1.5 mA (ii) 9V; 270 μC (iii) 1.5 mA]\n4. When the circuit of Fig. 5.50 is in steady state, what would be the p.d. across the capacitor ? Also,\nfind the discharge current at the instant S is opened.\n[8 V; 1.8 A]\nCapacitance\n255\n5. Find the time constant of the circuit shown in Fig. 5.51.\n[200 μS]\n6. A capacitor of capacitance 0.01 μF is being charged by 1000 V d.c.\nsupply through a resistor of 0.01 megaohm. Determine the voltage\nto which the capacitor has been charged when the charging current\nhas decreased to 90 % of its initial value. Find also the time taken\nfor the current to decrease to 90% of its initial value.\n[100 V, 0.1056 ms]\nFig. 5.51\n7. An 8 μF capacitor is being charged by a 400 V supply through 0.1\nmega-ohm resistor. How long will it take the capacitor to develop a p.d. of 300 V ? Also what\n[1.11 Second, 56.3% of full energy]\nfraction of the final energy is stored in the capacitor ?\n8. An 10 μF capacitor is charged from a 200 V battery 250 times/second and completely discharged\nthrough a 5 Ω resistor during the interval between charges. Determine\n(a) the power taken from the battery.\n(b) the average value of the current in 5 Ω resistor.\n[(a) 50 W (b) 0.5 A]\n9. When a capacitor, charged to a p.d. of 400 V, is connected to a voltmeter having a resistance of\n25 MΩ, the voltmeter reading is observed to have fallen to 50 V at the end of an interval of 2 minutes.\nFind the capacitance of the capacitor.\n[2.31 μF] (App. Elect. London Univ.)\n10. A capacitor and a resistor are connected in series with a d.c. source of V volts. Derive an expression\nfor the voltage across the capacitor after ‘t’ seconds during discharging.\n(Gujrat University, Summer 2003)\n11. Derive an expression for the equivalent capacitance of a group of capacitors when they are connected\n(Gujrat University, Summer 2003)\n(i) in parallel (ii) in series.\n12. The total capacitance of two capacitors is 0.03 μF when joined in series and 0.16 μF when connected\nin parallel. Calculate the capacitance of each capacitor.\n(Gujrat University, Summer 2003)\n13. In a capacitor with two plates separated by an insulator 3mm thick and of relative permittivity of\n4, the distance between the plates is increased to allow the insertion of a second insulator 5mm\nthick and relative permittivity E. If the capacitance so formed is one third of the original capacitance,\nfind E.\n(V.TU., Belgaum Karnataka University, February 2002)\n14. Derive an expression for the capacitance of a parallel plate capacitor.\n(V.TU., Belgaum Karnataka University, Summer 2002)\n15. Three capacitors A, B and C are charged as follows\nA = 10μF, 100 V\nB = 15μF, 150 V\nC = 25μF, 200 V\nThey are connected in parallel with terminals of like polarities together. Find the voltage across\nthe combination.\n(V.TU., Belgaum Karnataka University, Summer 2002)\n16. Prove that average power consumed by a pure capacitance is zero.\n(V.TU., Belgaum Karnataka University, Summer 2002)\n17. Current drawn by a pure capacitor of 20μF is 1.382A from 220V AC supply. What is the supply\nfrequency?\n(V.TU., Belgaum Karnataka University, Summer 2003)\n18. Find the equivalent capacitance between the points A and B of the network shown in fig. 1.\n(V.TU., Belgaum Karnataka University, Summer 2003)\nFig. 5.52\n19. Three capacitors of 1, 2 and 3 micro farads are connected in series across a supply voltage of 100V.\nFind the equivalent capacitance of the combination and energy stored in each capacitor.\n(Mumbai University 2003) (V.T.U. Belgaum Karnataka University, Wimter 2003)\n20. Consider a parallel plate capacitor, the space between which is filled by two dielectric of thickness\nd1 and d2 with relative permittivities ∈1 and ∈2 respectively. Derive an expression for the capacitance\nbetween the plates.\n(V.T.U. Belgaum Karnataka University, Wimter 2004)\n256\nElectrical Technology\n21. A capacitor consists of two plates of area 0.16m2 spaced 6mm apart. This space is filled with a\nlayer of 1mm thick paper of relative permittivity 2, and remaining space with glass of relative\npermittivity 5. A dc voltage of 10kV is applied between the plates. Determine the electric field\nstrength in each dielectric.\n(V.T.U. Belgaum Karnataka University, Wimter2004)\n22. In a give R-L circuit, R = 35Ω and L = 0.1H. Find (i) current through the circuit (ii) power factor\nif a 50 Hz frequency, voltage V = 220∠30° is applied across the circuit.\n(RGPV Bhopal 2001)\n23. Three voltage represented by e1 = 20 sin ω t, e2 = 30 sin (ω t = 45°) and e3 = sin (ω t + 30°)\nare connected in series and then connected to a load of impedance (2 + j 3) Ω. Find the resultant\ncurrent and power factor of the circuit. Draw the phasor diagram.\n(Mumbai University, 2002) (RGPV Bhopal 2001)\nOBJECTIVE TESTS – 5\n1. A capacitor consists of two\n(a) insulation separated by a dielectric\n(b) conductors separated by an insulator\n(c) ceramic plates and one mica disc\n(d) silver-coated insulators\n2. The capacitance of a capacitor is NOT\ninfluenced by\n(a) plate thickness\n(b) plate area\n(c) plate separation\n(d) nature of the dielectric\n3. A capacitor that stores a charge of 0.5 C at\n10 volts has a capacitance of .....farad.\n(a) 5\n(b) 20\n(c) 10\n(d) 0.05\n4. If dielectric slab of thickness 5 mm and\nε r = 6 is inserted between the plates of an air\ncapacitor with plate separation of 8 mm, its\ncapacitance is\n(a) decreased\n(b) almost doubled\n(c) almost halved\n(d)unaffected\n5. For the circuit shown in the given figure,\nthe current through L and the voltage across\nC2 are respectively\n(a) zero and RI\n(b) I and zero\n(c) zero and zero\n(d) I and RI\n(ESE 2001)\n6. A parallel plate capacitor has an electrode\narea of 100 mm2, with a spacing of 0.1 mm\nbetween the electrodes. The dielectric\nbetween the plates is air with a permittivity\nof 8.85 × 10–12 F/m. The charge on the\ncapacitor is 100 V. the stored energy in the\ncapacitor is\n(a) 8.85 pJ\n(b) 440 pJ\n(c) 22.1 nJ\n(d) 44.3 nJ\n(GATE 2003)\n7. A composite parallel plate capacitor is made\nup of two different dielectric materials with\ndifferent thicknesses (t1 and t2) as shown in\nFig.5.54. The two different dielectric\nmaterials are separates by a conducting foil\nF. The voltage of the conducting foil is\nFig. 5.54\n(a) 52 V\n(c) 67 V\nFig. 5.53"
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https://www.nag.com/numeric/nl/nagdoc_28.5/clhtml/f11/f11jcc.html | [
"# NAG CL Interfacef11jcc (real_symm_solve_ichol)\n\nSettings help\n\nCL Name Style:\n\n## 1Purpose\n\nf11jcc solves a real sparse symmetric system of linear equations, represented in symmetric coordinate storage format, using a conjugate gradient or Lanczos method, with incomplete Cholesky preconditioning.\n\n## 2Specification\n\n #include\n void f11jcc (Nag_SparseSym_Method method, Integer n, Integer nnz, const double a[], Integer la, const Integer irow[], const Integer icol[], const Integer ipiv[], const Integer istr[], const double b[], double tol, Integer maxitn, double x[], double *rnorm, Integer *itn, Nag_Sparse_Comm *comm, NagError *fail)\nThe function may be called by the names: f11jcc, nag_sparse_real_symm_solve_ichol or nag_sparse_sym_chol_sol.\n\n## 3Description\n\nf11jcc solves a real sparse symmetric linear system of equations:\n $Ax = b ,$\nusing a preconditioned conjugate gradient method (Meijerink and Van der Vorst (1977)), or a preconditioned Lanczos method based on the algorithm SYMMLQ (Paige and Saunders (1975)). The conjugate gradient method is more efficient if $A$ is positive definite, but may fail to converge for indefinite matrices. In this case the Lanczos method should be used instead. For further details see Barrett et al. (1994).\nf11jcc uses the incomplete Cholesky factorization determined by f11jac as the preconditioning matrix. A call to f11jcc must always be preceded by a call to f11jac. Alternative preconditioners for the same storage scheme are available by calling f11jec.\nThe matrix $A$, and the preconditioning matrix $M$, are represented in symmetric coordinate storage (SCS) format (see the F11 Chapter Introduction) in the arrays a, irow and icol, as returned from f11jac. The array a holds the nonzero entries in the lower triangular parts of these matrices, while irow and icol hold the corresponding row and column indices.\nBarrett R, Berry M, Chan T F, Demmel J, Donato J, Dongarra J, Eijkhout V, Pozo R, Romine C and Van der Vorst H (1994) Templates for the Solution of Linear Systems: Building Blocks for Iterative Methods SIAM, Philadelphia\nMeijerink J and Van der Vorst H (1977) An iterative solution method for linear systems of which the coefficient matrix is a symmetric M-matrix Math. Comput. 31 148–162\nPaige C C and Saunders M A (1975) Solution of sparse indefinite systems of linear equations SIAM J. Numer. Anal. 12 617–629\nSalvini S A and Shaw G J (1995) An evaluation of new NAG Library solvers for large sparse symmetric linear systems NAG Technical Report TR1/95\n\n## 5Arguments\n\n1: $\\mathbf{method}$Nag_SparseSym_Method Input\nOn entry: specifies the iterative method to be used.\n${\\mathbf{method}}=\\mathrm{Nag_SparseSym_CG}$\nThe conjugate gradient method is used.\n${\\mathbf{method}}=\\mathrm{Nag_SparseSym_Lanczos}$\nThe Lanczos method, SYMMLQ is used.\nConstraint: ${\\mathbf{method}}=\\mathrm{Nag_SparseSym_CG}$ or $\\mathrm{Nag_SparseSym_Lanczos}$.\n2: $\\mathbf{n}$Integer Input\nOn entry: the order of the matrix $A$. This must be the same value as was supplied in the preceding call to f11jac.\nConstraint: ${\\mathbf{n}}\\ge 1$.\n3: $\\mathbf{nnz}$Integer Input\nOn entry: the number of nonzero elements in the lower triangular part of the matrix $A$. This must be the same value as was supplied in the preceding call to f11jac.\nConstraint: $1\\le {\\mathbf{nnz}}\\le {\\mathbf{n}}×\\left({\\mathbf{n}}+1\\right)/2$.\n4: $\\mathbf{a}\\left[{\\mathbf{la}}\\right]$const double Input\nOn entry: the values returned in array a by a previous call to f11jac.\n5: $\\mathbf{la}$Integer Input\nOn entry: the second dimension of the arrays a, irow and icol.This must be the same value as returned by a previous call to f11jac.\nConstraint: ${\\mathbf{la}}\\ge 2×{\\mathbf{nnz}}$.\n6: $\\mathbf{irow}\\left[{\\mathbf{la}}\\right]$const Integer Input\n7: $\\mathbf{icol}\\left[{\\mathbf{la}}\\right]$const Integer Input\n8: $\\mathbf{ipiv}\\left[{\\mathbf{n}}\\right]$const Integer Input\n9: $\\mathbf{istr}\\left[{\\mathbf{n}}+1\\right]$const Integer Input\nOn entry: the values returned in the arrays irow, icol, ipiv and istr by a previous call to f11jac.\n10: $\\mathbf{b}\\left[{\\mathbf{n}}\\right]$const double Input\nOn entry: the right-hand side vector $b$.\n11: $\\mathbf{tol}$double Input\nOn entry: the required tolerance. Let ${x}_{k}$ denote the approximate solution at iteration $k$, and ${r}_{k}$ the corresponding residual. The algorithm is considered to have converged at iteration $k$ if:\n $‖ r k ‖ ∞ ≤ τ × ( ‖b‖ ∞ + ‖A‖ ∞ ‖ x k ‖ ∞ ) .$\nIf ${\\mathbf{tol}}\\le 0.0$, $\\tau =\\mathrm{max}\\phantom{\\rule{0.125em}{0ex}}\\left(\\sqrt{\\epsilon },\\sqrt{{\\mathbf{n}}}\\epsilon \\right)$ is used, where $\\epsilon$ is the machine precision. Otherwise $\\tau =\\mathrm{max}\\phantom{\\rule{0.125em}{0ex}}\\left({\\mathbf{tol}},10\\epsilon ,\\sqrt{{\\mathbf{n}}},\\epsilon \\right)$ is used.\nConstraint: ${\\mathbf{tol}}<1.0$.\n12: $\\mathbf{maxitn}$Integer Input\nOn entry: the maximum number of iterations allowed.\nConstraint: ${\\mathbf{maxitn}}\\ge 1$.\n13: $\\mathbf{x}\\left[{\\mathbf{n}}\\right]$double Input/Output\nOn entry: an initial approximation to the solution vector $x$.\nOn exit: an improved approximation to the solution vector $x$.\n14: $\\mathbf{rnorm}$double * Output\nOn exit: the final value of the residual norm ${‖{r}_{k}‖}_{\\infty }$, where $k$ is the output value of itn.\n15: $\\mathbf{itn}$Integer * Output\nOn exit: the number of iterations carried out.\n16: $\\mathbf{comm}$Nag_Sparse_Comm * Input/Output\nOn entry/exit: a pointer to a structure of type Nag_Sparse_Comm whose members are used by the iterative solver.\n17: $\\mathbf{fail}$NagError * Input/Output\nThe NAG error argument (see Section 7 in the Introduction to the NAG Library CL Interface).\n\n## 6Error Indicators and Warnings\n\nNE_2_INT_ARG_LT\nOn entry, ${\\mathbf{la}}=⟨\\mathit{\\text{value}}⟩$ while ${\\mathbf{nnz}}=⟨\\mathit{\\text{value}}⟩$. These arguments must satisfy ${\\mathbf{la}}\\ge 2×{\\mathbf{nnz}}$.\nNE_ACC_LIMIT\nThe required accuracy could not be obtained. However, a reasonable accuracy has been obtained and further iterations cannot improve the result.\nNE_ALLOC_FAIL\nDynamic memory allocation failed.\nOn entry, argument method had an illegal value.\nNE_COEFF_NOT_POS_DEF\nThe matrix of coefficients appears not to be positive definite.\nNE_INT_2\nOn entry, ${\\mathbf{nnz}}=⟨\\mathit{\\text{value}}⟩$, ${\\mathbf{n}}=⟨\\mathit{\\text{value}}⟩$.\nConstraint: $1\\le {\\mathbf{nnz}}\\le {\\mathbf{n}}×\\left({\\mathbf{n}}+1\\right)/2$.\nNE_INT_ARG_LT\nOn entry, ${\\mathbf{maxitn}}=⟨\\mathit{\\text{value}}⟩$.\nConstraint: ${\\mathbf{maxitn}}\\ge 1$.\nOn entry, ${\\mathbf{n}}=⟨\\mathit{\\text{value}}⟩$.\nConstraint: ${\\mathbf{n}}\\ge 1$.\nNE_INTERNAL_ERROR\nAn internal error has occurred in this function. Check the function call and any array sizes. If the call is correct then please contact NAG for assistance.\nNE_INVALID_SCS\nThe SCS representation of the matrix $A$ is invalid. Check that the call to f11jcc has been preceded by a valid call to f11jac, and that the arrays a, irow and icol have not been corrupted between the two calls.\nNE_INVALID_SCS_PRECOND\nThe SCS representation of the preconditioning matrix $M$ is invalid. Check that the call to f11jcc has been preceded by a valid call to f11jac, and that the arrays a, irow, icol, ipiv and istr have not been corrupted between the two calls.\nNE_NOT_REQ_ACC\nThe required accuracy has not been obtained in maxitn iterations.\nNE_PRECOND_NOT_POS_DEF\nThe preconditioner appears not to be positive definite.\nNE_REAL_ARG_GE\nOn entry, tol must not be greater than or equal to 1.0: ${\\mathbf{tol}}=⟨\\mathit{\\text{value}}⟩$.\n\n## 7Accuracy\n\nOn successful termination, the final residual ${r}_{k}={b-Ax}_{k}$, where $k={\\mathbf{itn}}$, satisfies the termination criterion\n $‖ r k ‖ ∞ ≤ τ × ( ‖b‖ ∞ + ‖A‖ ∞ ‖ x k ‖ ∞ ) .$\nThe value of the final residual norm is returned in rnorm.\n\n## 8Parallelism and Performance\n\nf11jcc is threaded by NAG for parallel execution in multithreaded implementations of the NAG Library.\nf11jcc makes calls to BLAS and/or LAPACK routines, which may be threaded within the vendor library used by this implementation. Consult the documentation for the vendor library for further information.\nPlease consult the X06 Chapter Introduction for information on how to control and interrogate the OpenMP environment used within this function. Please also consult the Users' Note for your implementation for any additional implementation-specific information.\n\nThe time taken by f11jcc for each iteration is roughly proportional to the value of nnzc returned from the preceding call to f11jac. One iteration with the Lanczos method (SYMMLQ) requires a slightly larger number of operations than one iteration with the conjugate gradient method.\nThe number of iterations required to achieve a prescribed accuracy cannot be easily determined a priori, as it can depend dramatically on the conditioning and spectrum of the preconditioned matrix of the coefficients $\\overline{A}={M}^{-1}A$.\nSome illustrations of the application of f11jcc to linear systems arising from the discretization of two-dimensional elliptic partial differential equations, and to random-valued randomly structured symmetric positive definite linear systems, can be found in Salvini and Shaw (1995).\n\n## 10Example\n\nThis example program solves a symmetric positive definite system of equations using the conjugate gradient method, with incomplete Cholesky preconditioning.\n\n### 10.1Program Text\n\nProgram Text (f11jcce.c)\n\n### 10.2Program Data\n\nProgram Data (f11jcce.d)\n\n### 10.3Program Results\n\nProgram Results (f11jcce.r)"
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https://docs.microsoft.com/en-us/archive/blogs/research/wtf-using-f-to-calculate-ballistics | [
"# WTF: Using F# to calculate ballistics\n\nIn building software, it is important to have the background, the algorithm and test data.\n\nBackground:\n\nUgh, what a weekend, a teenager was walking around in the roof of our condo with an Airsoft Pellet gun, with the orange tip covered so it looked like an assault rifle. Needless to say it was an interesting afternoon with six cop cars and the police helicopter paying our quiet neighborhood a visit. We were fortunate that the local news agencies have an office window policy, that is: if it isn’t viewable from their office windows, they don’t report on it. Can’t blame the news agencies for that with the current advertisement prices dropping. Now let’s take a look at computing a simple ballistic example, in this case, an Airsoft Pellet is fired straight up, we will assume that it is in a vacuum.\n\nAlso, do not attempt this at home, the teenager and his father had a very bad afternoon explaining all of this to the police and their neighbors. You might consider just throwing a ball in the air instead.\n\nPhysics problem/algorithm development\n\nThe muzzle velocity for an Airsoft Pellet gun is around 300 ft/sec to 400 ft/sec, but let’s be like the rest of the world and use meters, so it is reasonable that the muzzle velocity could be around 100 m/s (from the Airsoft web page).\n\nTo calculate the velocity of the pellet at the time that it’s velocity or speed is equal to zero, the derived calculations would be (since there is no x or horizontal velocity, and the mass is a “unit” mass):\n\n• y= ((Final velocity)^2 - (Initial Velocity)^2/(-2 * gravitational force)\n\nThe final velocity in this case is equal to zero so our equation becomes:\n\n• y= (-Initial Velocity)^2/(-2*gravitational force) or by multiplying by –1/-1 I get the equation:\n• y = (Initial Velocity)^2/(2*gravitational force)\n\nWhich is a fairly simple equation, as long as you are able to shoot the pellet at exactly normal to the local gravitational field in a vacuum, and since it is an air rifle that could be hard to do. In this case let’s go with it.\n\nBack to Background\n\nLet’s use the teenager running around on my condo’s roof on Saturday, his muzzle velocity is 100 m/s and he fires the pellet directly normal or 90 degrees to the ground surface, using a plumb bob he could determine the correct angle.\n\nPhysics/algorithm again\n\nThen the absolute highest the pellet could go is y=(100 m/s)^2/(2*9.8 m/s^2).\n\nNow units become an important part of this equation, in the upper part the equation becomes (100 m^2)/s^2/(19.6 m/s^2), which becomes about 5 meters around 510 meters above the barrel of the Airsoft pellet rifle.\n\nOne of the problems we might encounter is that the Airsoft rifle is manually pumped and may have a tendency to vary the projectile velocity out of the barrel. Let’s say that there is a 10% variation, and we might need to calculate this variation. Before we write the F# code, it is important to have a way to insure your programming work is correct.\n\nTest Data\n\nI use Excel to get an idea of what the actual output of the F# program should be, and in this case I used a 10% variation in muzzle velocity. You could use a graphing calculator to create the test data.\n\nNow I look at the calculation, I have to ask myself is this correct? Ok, let’s go with it.\n\nThe equation that I used in Excel is: Attitude Earth =Cellvalue^2/(2*9.8), where cellvalue is the cell coordinate, and I use a range of 90 to 110 in steps of 1 for the maximum attitude attained by the projectile in a vacuum and a perfect center of gravity.\n\nBefore writing my code, I usually make every attempt to create a simulation that I can use to check my programming. I usually turn to Excel to do the initial calculation. This gives a way to make sure I don’t make mistakes in programming and I am able to determine the form of the algorithm.\n\n Attitude Earth Muzzle Velocity 413 90 423 91 432 92 441 93 451 94 460 95 470 96 480 97 490 98 500 99 510 100 520 101 531 102 541 103 552 104 563 105 573 106 584 107 595 108 606 109 617 110\n\nNext we will write the F# that will solve the simulated equation."
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https://tools.carboncollective.co/future-value/43-in-49-years/ | [
"# Future Value of $43 in 49 Years Calculating the future value of$43 over the next 49 years allows you to see how much your principal will grow based on the compounding interest.\n\nSo if you want to save $43 for 49 years, you would want to know approximately how much that investment would be worth at the end of the period. To do this, we can use the future value formula below: $$FV = PV \\times (1 + r)^{n}$$ We already have two of the three required variables to calculate this: • Present Value (FV): This is the original$43 to be invested\n• n: This is the number of periods, which is 49 years\n\nThe final variable we need to do this calculation is r, which is the rate of return for the investment. With some investments, the interest rate might be given up front, while others could depend on performance (at which point you might want to look at a range of future values to assess whether the investment is a good option).\n\nIn the table below, we have calculated the future value (FV) of $43 over 49 years for expected rates of return from 2% to 30%. The table below shows the present value (PV) of$43 in 49 years for interest rates from 2% to 30%.\n\nAs you will see, the future value of $43 over 49 years can range from$113.47 to $16,469,966.61. Discount Rate Present Value Future Value 2%$43 $113.47 3%$43 $183.02 4%$43 $293.83 5%$43 $469.62 6%$43 $747.23 7%$43 $1,183.79 8%$43 $1,867.38 9%$43 $2,933.37 10%$43 $4,588.92 11%$43 $7,149.81 12%$43 $11,095.62 13%$43 $17,151.90 14%$43 $26,412.30 15%$43 $40,519.37 16%$43 $61,931.26 17%$43 $94,313.90 18%$43 $143,115.55 19%$43 $216,406.13 20%$43 $326,099.03 21%$43 $489,724.24 22%$43 $732,993.56 23%$43 $1,093,500.32 24%$43 $1,626,039.26 25%$43 $2,410,233.36 26%$43 $3,561,436.18 27%$43 $5,246,271.75 28%$43 $7,704,721.91 29%$43 $11,281,432.79 30%$43 \\$16,469,966.61\n\nThis is the most commonly used FV formula which calculates the compound interest on the new balance at the end of the period. Some investments will add interest at the beginning of the new period, while some might have continuous compounding, which again would require a slightly different formula.\n\nHopefully this article has helped you to understand how to make future value calculations yourself. You can also use our quick future value calculator for specific numbers."
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https://www.thestudentroom.co.uk/showthread.php?t=2231299 | [
"# OCR Physics Unit 2 - G482 - (June Exams Preparation)\n\nWatch\nAnnouncements\n#1\nI have made this thread for the June Unit 2 Physics exam for anyone interested in starting the revising process early and so that we can help eachother with what we're learning as we go. I started Unit 2 last week (an hour after my last exam, slightly brain dead).\n\nI'm glad to hear some people thinking it would be a good idea, I haven't encountered all of this content but luckily I did a Lvl 3 VRQ in Electrical Engineering last year so hopefully I can help us quite a bit ^.^ Once I finished compiling my class notes I'll pop 'em up on this thread!\n\nEdit: Would have finished typing up my notes tonight but got a bit distracted having my birthday, sorry will try to get everything done before the weekend's over.\n5\n#2\nPART 1/5\n\nElectrons drift slowly through a circuit carrying an electric current. As the electrons move they create a shift in the electrons pushing the electrons in front of them down the circuit; therefore despite the slow speed the moment an electrical circuit is switched on each of the electrical components (e.g. an LED or a resistor) receives current.\n\nElectric Current is defined as the flow of charge through a conductive material. There are two types of electrical current:\nConventional Current is where current is considered to be the flow of positive charge from positive (e.g. 5V) to negative (0V) due to the negative electrons traveling in the opposite direction.\nElectron Flow is the movement of electrons carrying a negative charge from negative to positive.\n\nWhen there is no current electrons move randomly about the material causing no net drift.\nWhen current is present (despite still moving randomly) the general drift of electrons is in a specific direction (towards negative).\n\nAmperes (Amps) - Current is measured in Amperes (A) measuring the amount of electric current through a point per unit of time. 1A=1Cs-1\n\nElectric Charge is the total amount of current that is supplied over a certain period of time. It can be defined with the following equation:\nQ=It (charge = current x time)\n\nCoulombs - Charge is measured in coulombs (C) - 1C if the total charge supplied by a current of 1A in a time of 1s.\n\nKirchhoff's Law: \"The sum of the currents entering any junction is always equal to the sum of the currents leaving the junction.\"\nNote: Charge will be conserved throughout the circuit.\n\nAmmeters are used to measure electric current. A digital multimeter is more often used - they're a multifunctional piece of equipment that allows you to measure current, voltage and resistance. Theoretically an ammeter should have negligible resistance. In a circuit they need to be connected in series, not in parallel, otherwise the electrical current will pass through the ammeter, limiting or stopping the current from passing through the component it is connected in parallel to (should that component present any form of resistance).\n\nMean Drift Velocity is the average velocity that an electron attains when an electric current flows. Mean drift velocity is directly proportional to current. It is given by the equation:\nI=nAve\nWhere: I = current\nn = number density of electrons (electrons per unit volume)\nA = cross-sectional area\nv = mean drift velocity\ne= electron charge (1.6x10-19C)*\n\n*1.6x10-19C is the negative charge of an electron; this is the number you need to know - like remembering 9.81ms-2 was the magnitude of acceleration due to gravity in the last unit\n\nMaterial Categories\nConductors contain a high number density of conducting electrons e.g. a copper wire.\nInsulators contain very few or no conducting electrons e.g. rubber.\nSemiconductors have properties that lie between those of conductors and insulators e.g. silicon. The conductivity of a semiconductor increases with increasing temperature, behavior opposite to that of a metal.\n\nTHE END OF PART 1/5\n3\n8 years ago\n#3\n(Original post by Shinusuke_Akki)\nKnowledge Update 01\n\nElectrons drift slowly through a circuit carrying an electric current. As the electrons move they create a shift in the electrons pushing the electrons in front of them down the circuit; therefore despite the slow speed the moment an electrical circuit is switched on each of the electrical components (e.g. an LED or a resistor) receives current.\n\nElectric Current is defined as the flow of charge through a conductive material. There are two types of electrical current:\nConventional Current is where current is considered to be the flow of positive charge from positive (e.g. 5V) to negative (0V) due to the negative electrons traveling in the opposite direction.\nElectron Flow is the movement of electrons carrying a negative charge from negative to positive.\n\nWhen there is no current electrons move randomly about the material causing no net drift.\nWhen current is present (despite still moving randomly) the general drift of electrons is in a specific direction (towards negative).\n\nAmperes (Amps) - Current is measured in Amperes (A) measuring the amount of electric current through a point per unit of time. 1A=1Cs-1\n\nElectric Charge is the total amount of current that is supplied over a certain period of time. It can be defined with the following equation:\n[B]Q=It[B] (charge = current x time)\n\nCoulombs - Charge is measured in coulombs (C) - 1C if the total charge supplied by a current of 1A in a time of 1s.\n\nKirchhoff's Law: \"The sum of the currents entering any junction is always equal to the sum of the currents leaving the junction.\"\n\nAmmeters are used to measure electric current. A digital multimeter is more often used - they're a multifunctional piece of equipment that allows you to measure current, voltage and resistance. Theoretically an ammeter should have negligible resistance. In a circuit they need to be connected in series, not in parallel, otherwise the electrical current will pass through the ammeter, limiting or stopping the current from passing through the component it is connected in parallel to (should that component present any form of resistance).\n\nMean Drift Velocity is the average velocity that an electron attains when an electric current flows. Mean drift velocity is directly proportional to current. It is given by the equation:\nI=nAve\nWhere: I = current\nn = number density of electrons (electrons per unit volume)\nA = cross-sectional area\ne= electron charge (1.6x10-19C)*\n\n*1.6x10-19C is the negative charge of an electron; this is the number you need to know - like remembering 9.81ms-2 was the magnitude of acceleration due to gravity in the last unit\nThanks for this, it's really helpful",
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"0\n#4\n(Original post by Gotzz)\nThanks for this, it's really helpful",
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"Thank-you I'm glad that it is, will try to get the next one up when I've compiled a good enough note collection. If you have any questions or feel I've missed something, please do say ^^\n0\n#5\nI'm about ready to start my write ups for part 2 of 5, I should be finishing up my topic on resistance and will write up notes and post them hopefully by this weekend if not sooner (sorry for the delay I've had some personal issues which have delayed my work temporarily but everything should be okie-dokie-lokie now) :3\n0\n7 years ago\n#6\nWhy isn't there this for Unit 5 arghhhhhhhhhhhhh\n0\n#7\n(Original post by Better)\nWhy isn't there this for Unit 5 arghhhhhhhhhhhhh\nWell apparently there is a thread... Yours by the looks of it... http://www.thestudentroom.co.uk/show....php?t=2244676 :P\n0\n#8\n(Original post by Law-Hopeful)\nI'm really lost on emf and polarisation. Anyone care to help?",
null,
"",
null,
"Will post about E.M.F by this weekend not sure about polarisation yet tho, sorry. If the E.M.F is urgent I can try to post my notes before I've finished them for you?\n0\n7 years ago\n#9\nI love this Unit so much it is the best! Much better than Unit 1",
null,
". I sat this exam in Jan so if anyone is unsure of anything just ask me",
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"0\n7 years ago\n#10\n(Original post by Law-Hopeful)\nI'm really lost on emf and polarisation. Anyone care to help?",
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"",
null,
"Definition for E.m.f is the energy transfer per unit charge when other forms of energy is transferred into electrical energy denoted by the equation V = W/Q.\n\nThere is also another equation for Emf which combines Kirchoff's Second Law have you reached to that stage yet?\n\nFor polarization what you need to know is that when light passes through a polarizing filter it will become partially polarized meaning the polarizing filter will only let through light which is acting in the same plane, all other planes of light will be blocked up.\n\nHowever when you pass partially polarized light through a second polarizing filter, the intensity of light will depend on the angle the second filter is rotated. It is denoted by equation I = Io + cos^2(pheta)\nWhere:\n- Io is the initial intensity (after passing through the first filter)\n- I is the final intensity (after passing through the second filter)\n- Pheta is the angle of rotation of the second filter.\n\nHere you would note that if 2nd filter isn't rotated, such that the angle is 0 degrees light would have full intensity. Since cos 0 = 1. 1 squared = 1.\n\nIf the 2nd filter is rotated perpendicular to the first filter, such that the angle is 90 degrees no light will pass through. Since cos 90 = 0. 0 square = 0.\n\nAlso if the 2nd filter is parallel to the first filter, such that the angle is 180 degrees the light would have full intensity. Since cos 180 = -1. And -1 squared = 1.\n\nHope this helps",
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"1\n7 years ago\n#11\nI understand the\ncurrents but not the answers to the voltages.\n\na) 5.0V, 0A\nb)0V, 1.1mA\n0\n7 years ago\n#12\nThe resistance between PQ can be regarded as very high(infinite) when the switch S is open. So pd across PQ = 5 x infinite/(infinite + 4.7kohm) = 5V\nWhen the switch is closed the resistance between PQ is zero. Hence pd across PQ = 5 x zero/(zero+ 4.7kohm) = 0V\n0\n7 years ago\n#13\n(Original post by gunner18)\nThe resistance between PQ can be regarded as very high(infinite) when the switch S is open. So pd across PQ = 5 x infinite/(infinite + 4.7kohm) = 5V\nWhen the switch is closed the resistance between PQ is zero. Hence pd across PQ = 5 x zero/(zero+ 4.7kohm) = 0V\nGot it! Thanks.\n\nhttp://www.cyberphysics.co.uk/topics...sistivityQ.htm\n\nI found this pretty useful.",
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"0\n7 years ago\n#14\nAnybody does the physics practical courseworks? Could do with some tips.\n0\n7 years ago\n#15\nI had my first physics practical before the half term, it was was the one out of 20 marks. Not sure how I did, will find out tomorrow, I think",
null,
"ETA: I got 19/20! SO happy!",
null,
"3\n7 years ago\n#16\n(Original post by Gotzz)\nI had my first physics practical before the half term, it was was the one out of 20 marks. Not sure how I did, will find out tomorrow, I think",
null,
"Was it to do with amps and resistivity?\n0\n7 years ago\n#17\n(Original post by Loiks94)\nWas it to do with amps and resistivity?\nNope\n0\n7 years ago\n#18\nHas anyone started doing past exam papers? How are you finding it relative to the work you were given in class? The questions considerably harder or about the same?\n0\n7 years ago\n#19\n(Original post by brawlerpit)\nHas anyone started doing past exam papers? How are you finding it relative to the work you were given in class? The questions considerably harder or about the same?\nCan't start doing exam papers as we've nowhere near covered all the content yet. Nerve-racking, really.\n0\n7 years ago\n#20\n(Original post by Dusky Mauve)\nCan't start doing exam papers as we've nowhere near covered all the content yet. Nerve-racking, really.\nMaybe someone who did it as an AS last year could shine some light; are you understanding the topics well?\n0\nX\n\nnew posts",
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"Back\nto top\nLatest\nMy Feed\n\n### Oops, nobody has postedin the last few hours.\n\nWhy not re-start the conversation?\n\nsee more\n\n### See more of what you like onThe Student Room\n\nYou can personalise what you see on TSR. Tell us a little about yourself to get started.\n\n### Poll\n\nJoin the discussion\n\n#### Do you have the space and resources you need to succeed in home learning?\n\nYes I have everything I need (331)\n55.72%\nI don't have everything I need (263)\n44.28%"
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http://www.cs.uu.nl/groups/ST/Software/UU_AG/index.html | [
"# Simple, Functional Attribute Grammars\n\n(Updated: 24-Oct--1999)\n\nClick here to return to the main page.\n\nTable of Contents\n\n### Why these Combinators?\n\nHave you always been intrigued by Attribute Grammars because they allow you to:\n\n• write language processors in a compositional way in which\n• the different aspects of a language may be textually separated\n\nbut you do not like:\n\n• to write code for constructing and inspecting intermediate data structures\n• the often verbose notation used by other systems\n• to learn a new language for describing semantic functions\n• the often limited expressibility of these languages\n• the sheer size of existing systems\n• the absence of any higher-order facilities\n\nthen why not use my simple attribute grammar system?\n\nThe UU_AG system is a very simple program that reads a set of files containing an attribute grammar, in which semantic functions are described through Haskell expressions. Out of this description catamorphisms and data type definitions are generated.\n\nI hope this software is useful to you. If you have any comments do not hesitate to contact me.\n\nDoaitse Swierstra\n\n### Change Log\n\n• 1999/09/05 Slightly different syntax for attribute definitions. Especially the types are enforced to be present.\n• 1999/10/24 Better error messages\n\nIf you want to stay informed about changes and corrections you should send me an email.\n\n### Where to get software\n\nYou need the following file:\n\nFurthermore you may be interested in the additional files, that are imported by the system:\n\n### Conditions for use\n\nI have been asked about any copyright associated with these files. Since I do not want to get too deeply involved in all kinds of legalese I have included a slightly adapted version of the artistic license that came with my version of Hugs. It seems to capture nicely what is my intent with this package.\n\nI would be happy it you would let me know:\n\n• whether you are using the package and what for\n• what modifications you are interested in\n• what modifications you have made yourself\n• whether you think the package is useful (visiting committees have called the construction of such packages \"not useful\"; once they show up again it would be nice if I could present proof of the contrary)\n\n### The Attribute Grammar Language\n\nBefore looking at the grammar you might want to first look at the example session.\n\n#### The Main Structure of the Input\n\nWe start with providing the full grammar of the accepted input, as expressed by the parsing part of the UU_AG file:\n\n`parser = parse pAG`\n\nThe input consists of a list of separate textual elements, each representing a small contribution to the complete grammar. Such grammar fragments may even be distributed over several files, according to the conventions stemming from the use of the standard UU scanning library\n\n```pAG = foldl sem_Elems_One_Elem sem_Elems_No_Elem\n<\\$> pList pElem\n```\n\nEach element in this list:\n\npElem =\n\neither represents:\n\n• a grammar rule definition. Since each production will lead to one more alternative in the data type describing the abstract syntax tree we have chosen the keyword \"DATA\" to start such an element with:\n``` sem_Elem_Data <\\$ pKey \"DATA\"\n<*> pConid <*> pAttrs\n<*> pAlts sem_Alt```\n• the definition of some attributes belonging to certain nonterminals\n``` <|> sem_Elem_AttrsDef <\\$ pKey \"ATTR\"\n<*> pList pConid <*> pAttrs ```\n• the definition of semantic functions, describing how to compute a specific attribute out of other attributes:\n``` <|> sem_Elem_Rules <\\$ pKey \"SEM\"\n<*> pConid <*> pAttrs\n<*> pAltRules```\n• an extension with extra elements of a earlier introduced right hand side of a production.\n``` <|> sem_Elem_Data <\\$ pKey \"EXT\"\n<*> pConid <*> pAttrs\n<*> pAlts sem_Alt'```\n• a specification of the prefix that the generated semantic functions should have\n` <|> sem_Elem_Pre <\\$ pKey \"PRE\" <*> pVarid`\n• the description of a named piece of input text, that is to be included in the generated attribute grammar evaluator\n` <|> sem_Elem_Txt <\\$> pTextnm <*> pList pTextln`\n\n#### Defining Grammar Rules\n\n`pAlts sem = applyall <\\$> pListPrefixed (pSpec '|') (sem <\\$> pConid <*> pFields)`\n\n#### Defining Attributes\n\n```pAttrs\n= pBracks ((,,) <\\$> pAttrNames\n<* pSpec '|' <*> pAttrNames\n<* pSpec '|' <*> pAttrNames\n) `opt` ([], [], [])\n\npAttrNames\n= concat <\\$> pList (\nsem_Attrs <\\$> pCommas pNameDef\n<*> (( (,) <\\$ pKey \"USE\" <*> pString <*> pString) `opt` (\"\",\"\"))\n<*> ( pKey \":\" *> pConid)\n) ```\n\n#### Defining Semantic Functions\n\n```pFields = applyall <\\$> pList pField\n\npField = sem_Field <\\$> pCommas pVarid <* pKey \":\" <*> pConid\n<|> (\\s -> sem_Field [(mklower s)] s) <\\$> pConid\n\npAltRules = pFoldrPrefixed compose_alg (pSpec '|') pAltRule\npAltRule = sem_AltRule <\\$> pConid <*> pFieldRules\n\npFieldRules\n= pFoldr compose_alg\n( sem_FieldRule <\\$> (pVarid\n<|> pKey \"LHS\") <*> pAttrRules (Ident <\\$> pVarid)\n<|> sem_FieldRule <\\$> pKey \"LOC\" <*> pAttrRules pNameDef\n)\n\npAttrRules pname = pFoldrPrefixed compose_alg (pSpec '.') (pAttrRule pname)\n\npAttrRule pname = sem_AttrRule <\\$> pname <*> (pKey \"=\" <|> pKey \":=\") <*> pAttrExpr\n\npAttrExpr = (((\\s-> \"(\"++s++\")\") <\\$> pString) <|> pVarid <|> pConid)\n\npNameDef = LocalDef <\\$> pVarid <*> ( pSpec '@' *> pPattern `opt` NoPat )\n<|> LocalDef <\\$> pSucceed \"\" <*> pPattern\n\npPattern = Product <\\$> pParens (pListSep (pSpec ',') pSimplePattern)\npSimplePattern = Var <\\$> pVarid\n<|> Constr <\\$> pConid <*> pList pSimplePattern\n<|> pPattern\n<|> Underscore <\\$ pSpec '_'```\n\n### An Example Session.\n\nAs a first example we take the well known RepMin problem. The input of the program is a binary tree, and it produces a binary tree of the same shape. In the new tree however all values in the leaves are equal to the minimum of the values in the leafs in the original tree. We will show two versions: the full version in which all semantic functions made explicit, and one in which many shorthand notation is used.\n\n#### The Full Version\n\nThe full code of this example is given in RepMin1.ag. We start by defining the structure of the tree. One might look at this both as a piece of abstract grammar, with two nonterminals, or as two data type definitions. The difference with a Haskell data type definition is that the fields are associated with a name, and not only by position.\n\n```\\BC -- we start each piece of attribute grammar code with \\BC since the system works in literate mode\nDATA Tree\n| Leaf int: Int\n| Bin left, right: Tree\n\nDATA Root | Root tree: Tree```\n\nWe split the computation to be performed into three different aspects:\n\n• the computation of the minimal value\n• making the minimal value available at the leaves\n• constructing the final result\n\nFor the computation of the minimal value we introduce one synthesised attribute m:\n\n`ATTR Tree [ | | m: Int ]`\n\nThat this is an synthesised attribute follows from the fact that the attribute specification is located after the second vertical bar |. Next we specify the computation of the minimum value by providing semantic rules. Such rules may be grouped by non-terminal and by production. In the next two rules we see the non-terminal that applies (Tree), the alternative for which the rule is defined (Leaf or Bin), the element of the alternative to which the attribute that is being defined is associated (in this case the left hand side of the production that is always called LHS), the attribute that is being defined (m), and the Haskell expression that describes the computation . This Haskell expression is either a complicated expression, in which case we represent is as a string (\"left_m `min` right_m\"), or a simple identifier (int).\n\n```SEM Tree\n| Leaf LHS .m = int\n| Bin LHS .m = \"left_m `min` right_m\"```\n\nNext we introduce an inherited attribute (minval) that describes how the computed minimal value is passed from the root of the tree to the leaves. That this is an inherited attribute stems from the fact that its definition occurs before the first vertical bar. In the Haskell expression we may refer to other accessible attributes by mean's of the identifier <element name>_<attribute name>. In order to refer to the inherited attributes of the right hand side we prefix the name of the attribute by lhs_.\n\n```ATTR Tree [ minval: Int ||]\nSEM Tree\n| Bin left .minval = lhs_minval\nright.minval = lhs_minval\n```\n\nThe third step concerns the computation of the resulting tree, which follows the computation of the minimum value:\n\n```ATTR Tree [ | | res: Tree ]\nSEM Tree\n| Leaf LHS .res = \"Tree_Leaf lhs_minval\"\n| Bin LHS .res = \"Tree_Bin left_res right_res\"\n```\n\nFinally we have to tie the knot at the root of the problem: the value that is computed as the minimum value is the value that should be passed down the tree, and as a result we are only interested in the constructed tree, and not in that minimum value.\n\n```ATTR Root [|| res: Tree ]\nSEM Root\n| Root tree .minval = tree_m\nLHS .res = tree_res\n\\EC -- we end each piece of attribute grammar code with \\EC since the system works in literate mode```\n\nThis input can be compiled as in the following session:\n\n```UU_AG> compile \"Repmin1\" allc\nRepmin1.hs generated\n(159277 reductions, 321908 cells)\nUU_AG>\n```\n\nThe value allc has been defined as:\n\n`allc = \"mdcs\"`\n\nin which the meaning of the characters is:\n\n• m : generate a module header\n• d : generate data type definitions\n• c : generate catamorphisms\n• s : generate signatures for semantic functions\n\nThe code generated by the attribute grammar system, with all options enabled is:\n\n```-- The module header : RepMin1 ----------------------------\nmodule RepMin1 where\n-- The data type definition: Tree -------------------------\ndata Tree = Tree_Leaf Int| Tree_Bin Tree Tree\nderiving Show\n-- The signatures for the semantic functions --------------\ntype T_Tree = Int ->(Tree,Int)\n-- The semantic functions (which are always generated) ----\nsem_Tree_Leaf ::Int -> T_Tree\nsem_Tree_Leaf int lhs_minval = ( (Tree_Leaf lhs_minval), int )\nsem_Tree_Bin :: T_Tree -> T_Tree -> T_Tree\nsem_Tree_Bin left right lhs_minval\n= let{ ( left_res, left_m ) = left lhs_minval\n; ( right_res, right_m ) = right lhs_minval\n}\nin ( (Tree_Bin left_res right_res), (left_m `min` right_m) )\n-- The data type definition: Root -------------------------\ndata Root = Root_Root Tree\nderiving Show\n-- The signatures for the semantic functions --------------\ntype T_Root = Tree\n-- The semantic functions (which are always generated) ----\nsem_Root_Root :: T_Tree -> T_Root\nsem_Root_Root tree = let{ ( tree_res, tree_m ) = tree tree_m}in tree_res\n```\n\n#### Shorthand Notation\n\nThe shorthand version of the above program is:\n\n```\\BC\nDATA Tree\n| Leaf Int\n| Bin left, right: Tree\n\nSEM Tree [ minval: Int || m: Int res: Tree ]\n| Leaf LHS.m = int\n.res = \"Tree_Leaf lhs_minval\"\n| Bin LHS.m = \"left_m `min` righth_m\"\n.res = \"Tree_Bin left_res right_res\"\n\nDATA Root [|| res: Tree ]\n| Root Tree\nSEM Root\n| Root tree.minval = tree_m\n\\EC```\n\nIn this completely equivalent program we can notice the following abbreviations:\n\n• The field Int in the production Leaf has not been explicitly named (nor the field Tree in the production Root or nonterminal Root). If this is the case its name is the same as the name of the non-terminal corresponding to that field, however with its first letter replaced by the lower case equivalent (i.e. int and tree).\n• If a child has an inherited attribute with the same name as its father, and no semantic function has been specified, a so-called copy rule is generated by the system that corresponds to the identity function applied to the inherited attribute of the father. This makes the value minval being automatically passed down to the leaves of the tree (this is an instance of a more general rule for generating copy rules that will be explained later).\n• If a father node has a synthesised attribute for which no rule is given, and there is a child which also has a synthesised attribute with the same name a copy rule is generated (this is an instance of a more general rule for generating copy rules that will be explained later).\n• Attributes may not only be defined by a special ATTR construct, but also after the non-terminal occurring in a DATA section or a SEM section.\n\n### Copy Rule Generation\n\nIn case no definition was given for a specific atribute the system will try the following strategy in generating a definition:\n\n1. If there exists a local attribute, or an elememnt in the pattern of a local attribute that has the same name as the attribute for which the definition is missing, a rule is geneated through which that elemnet is referred.\n2. If the previous rule does not solve the problem, and there exists a filed in the production for which no attributes have been specified, and this field has the same name as the attribute for which the definition is missing, this filed is taken as the value to be usedfor thi attribute.\n3.\n\n### An Example Language\n\nWe have developed a compiler for a small language in a stepwise fashion. You can find the description of the language and the associated files at the Implementation of Programming Languages course.\n\n### Errors\n\nThe error messages are generated in a rather generic way. We hope they are self-explaining. Some further work needs to be done on making the system continue once an error was reported.\n\n### Tips\n\n• none thus far\n\n### Still to do\n\n• make extensive documentation\n• make system always continue after reporting an error\n• extend the formalism so it has more facilities for handling modular descriptions\n• bootstrap the system"
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https://de.scribd.com/document/153934134/Work-Energy-and-Power | [
"Sie sind auf Seite 1von 6\n\n# Work, Power, Energy Multiple Choice PSI Physics Multiple Choice Questions Name____________________________________\n\n1.\n\nA block of mass m is pulled over a distance d by an applied force F which is directed in parallel to the displacement. How much work is done on the block by the force F? A. mFd B. zero C. Fd D. E. Fd\n\n2.\n\nA block of mass m is moved over a distance d. An applied force F is directed perpendicularly to the blocks displacement. How much work is done on the block by the force F? A. mFd B. zero C. Fd D. E. Fd\n\n3.\n\nA block of mass m is moved over a distance d. An applied force F is opposite to the blocks displacement. How much work is done on the block by the force F? A. mFd B. zero C. Fd D. E. Fd\n\n4.\n\nA truck driver is trying to push a loaded truck with an applied force. Unfortunately, his attempt was unsuccessful the truck stays stationary no matter how hard the driver pushes. How much work is done by the driver? A. Fd B. Fd C. D. E. Zero\n\n5.\n\nA spacecraft moves around Earth in a circular orbit with a constant radius. How much work is done by the gravitational force on the spacecraft during one revolution? A. FGd B. - FGd C. mgh D. mv2 E. zero\n\n6.\n\n7.\n\nA construction worker holds a heavy tool box. How much work is done by the worker? A. FGd B. - FGd C. mgh D. mv2 E. zero A container with a mass of 5 kg is lifted to a height of 8 m. How much work is done by the gravitational force? A. 400 J B. -400 J C. zero D. 50 J E. -50J A container with a mass of 5 kg is lifted to a height of 8 m. How much work is done by the external force? A. 400 J B. -400 J C. zero D. 50 J E. -50J A container with a mass of 5 kg is lifted to a height of 8 m and then returned back to the ground level. How much work is done by the gravitational force? A. 400 J B. -400 J C. zero D. 50 J E. -50J\n\n8.\n\n9.\n\n10. An object is thrown straight up. Which of the following is true about the sign of work done by the gravitational force while the object moves up and then down? A. Work is positive on the way up, work is positive on the way down B. Work is negative on the way up, work is negative on the way down C. Work is negative on the way up, work is positive on the way down D. Work is positive on the way up, work is negative on the way down E. Work is zero the way up, work is zero on the way down\n\n11. The force as a function of displacement of a moving object is presented by the graph. How much work is done when the object moves from 0 m to 8 m? A. 40 J B. 20 J C. 0 J D. 10 J E. 5 J\n\n12. The force as a function of displacement of a moving object is presented by the graph. How much work is done when the object moves from 0 m to 5 m? A. 30 J B. 12.5 J C. 18 J D. 9 J E. 24 J\n\n13. The force as a function of displacement of a moving object is presented by the graph. How much work is done when the object moves from 5 m to 8 m? A. 30 J B. 15 J C. 18 J D. 7.5 J E. 24 J\n\n14. The force as a function of displacement of a moving object is presented by the graph. How much work is done when the object moves from 0 m to 8 m? A. 30 J B. 15 J C. 18 J D. 5 J E. 20 J\n\n15. An applied force F accelerates an object from rest to a velocity v. How much work is done by the applied force F? A. mv2 B. mgh C. kx2 D. mFd E. Zero\n\n16. What happens to the kinetic energy of a moving object if the net work done is positive? A. The kinetic energy increases B. The kinetic energy decreases C. The kinetic energy remains the same D. The kinetic energy is zero E. The kinetic energy becomes negative\n\n17. A block of mass m = 50 kg moves on a rough horizontal surface with a coefficient of kinetic friction = 0.5. The traveled distance is 20 m. How much work is done by the friction force? A. 1000 J B. 2000 J C. 3000 J D. 4000 J E. -5000 J\n\n18. An object I with a mass of 4 kg is lifted vertically 3 m from the ground level; another object II with a mass of 2 kg is lifted 6 m up. Which of the following statements is true? I. Object I has greater potential energy since it is heavier II. Object II has greater potential energy since it is lifted to a higher position III. Two objects have the same potential energy A. I B. II C. III D. I and II E. II and III\n\n19. A 4 kg block is attached to a vertical spring with a spring constant 800 N/m. The spring stretches 5 cm down. How much elastic potential energy is stored in the system? A. 1.0 J B. 0.5 J C. 1.5 J D. 2.0 J E. 2.5 J\n\n20. A heavy block is suspended from a vertical spring. The elastic potential energy is stored in the spring is 2 J. What is the spring constant if the elongation of the spring is 10 cm? A. 400 N/m B. 300 N/m C. 200 N/m D. 100 N/m E. 50 N/m\n\n21. A heavy block is suspended from a vertical spring. The elastic potential energy is stored in the spring is 0.8 J. What is the elongation of the spring if the spring constant is 100 N/m? A. 2 cm B. 4 cm C. 8 cm D. 10 cm E. 13 cm\n\n22. The elastic force as a function of displacement presented by the graph. How much elastic potential energy is stored in the spring when it is stretched by 10 cm? A. 0.1 J B. 0.2 J C. 0.3 J D. 0.4 J E. 0.5 J\n\n23. A bullet penetrates a wooden block and loses its velocity by a half. What is the ration between the initial kinetic energy of the bullet and kinetic energy when the bullet leaves the block? A. = B. = C. = D. = E. = 24. A truck drives slams on the brakes of a moving truck with a constant velocity v, as a result of his action the truck stops after traveling a distance d. If the driver had been traveling with twice the velocity, what would be the stopping distance compared to the distance in the first trial? A. Two times greater B. Four times greater C. The same D. Half as much E. One-quarter as much 25. What happens to the total energy of a moving object if all the applied forces are conserved? A. It increases B. It decreases C. It remains constant D. The velocity is required to answer this question E. The altitude is required to answer this question 26. A machine does 2500 J of work in 1 min. What is the power developed by the machine? A. 21 W B. 42 W C. 150 W D. 2500 W E. 150000 W 27. A car travels with a constant speed of 15 m/s. The cars engine produces a 4000 N pushing force in order to keep the speed constant. How much power is developed by the engine? A. 60 W B. 600 W C. 6000 W D. 60000 W E. 600000W\n\n28. A block with a mass of m crosses a rough horizontal surface at a constant speed of v. The coefficient of kinetic friction between the block and the surface is . How much power must be produced in order to overcome the friction force? A. mg B. mg C. zero D. g E. mgv 29. A motorbike engine can develop a power of 90000 W in order to keep a constant velocity of 30 m/s. What is the pushing force? A. 3000 N B. 30000 N C. 300000 N D. 300 N E. 30 N\n\nAnswers 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. 16. 17. 18. 19. 20. 21. 22. 23. 24. 25. 26. 27. 28. 29. C B E E E E B A C C A B D E A A E C A A E C D B C B D E A"
]
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https://shardbox.org/shards/hashdiff/releases/1.0.0 | [
"# hashdiff\n\nHashdiff is a crystal library to compute the smallest difference between two hashes. It was translated from the hashdiff ruby gem\n1.0.0 released\n\n# hashdiff\n\nHashdiff is a crystal library to compute the smallest difference between two hashes. It was translated from the hashdiff ruby gem.\n\nIt also supports comparing two arrays.\n\nHashdiff does not monkey-patch any existing class. All features are contained inside the `Hashdiff` module.\n\n## Why Hashdiff?\n\nGiven two Hashes A and B, sometimes you face the question: what's the smallest modification that can be made to change A into B?\n\nAn algorithm that responds to this question has to do following:\n\n• Generate a list of additions, deletions and changes, so that `A + ChangeSet = B` and `B - ChangeSet = A`.\n• Compute recursively -- Arrays and Hashes may be nested arbitrarily in A or B.\n• Compute the smallest change -- it should recognize similar child Hashes or child Arrays between A and B.\n\nHashdiff answers the question above using an opinionated approach:\n\n• Hash can be represented as a list of (dot-syntax-path, value) pairs. For example, `{a: [{c: 2}]}` can be represented as `[\"a.c\", 2]`.\n• The change set can be represented using the dot-syntax representation. For example, `[{\"-\", \"b.x\", 3}, {\"~\", \"b.z\", 45, 30}, {\"+\", \"b.y\", 3}]`.\n• It compares Arrays using the LCS(longest common subsequence) algorithm.\n• It recognizes similar Hashes in an Array using a similarity value (0 < similarity <= 1).\n\n## Installation\n\n1. Add the dependency to your `shard.yml`:\n\n``````dependencies:\nhashdiff:\ngithub: spoved/hashdiff.cr\n``````\n2. Run `shards install`\n\n## Usage\n\n``````require \"hashdiff\"\n``````\n\n### Diff\n\nTwo simple hashes:\n\n``````a = {a: 3, b: 2}\nb = {}\n\ndiff = Hashdiff.diff(a, b)\ndiff.should == [{\"-\", \"a\", 3}, {\"-\", \"b\", 2}]\n``````\n\nMore complex hashes:\n\n``````a = {a: {x: 2, y: 3, z: 4}, b: {x: 3, z: 45}}\nb = {a: {y: 3}, b: {y: 3, z: 30}}\n\ndiff = Hashdiff.diff(a, b)\ndiff.should == [{\"-\", \"a.x\", 2}, {\"-\", \"a.z\", 4}, {\"-\", \"b.x\", 3}, {\"~\", \"b.z\", 45, 30}, {\"+\", \"b.y\", 3}]\n``````\n\nArrays in hashes:\n\n``````a = {a: [{x: 2, y: 3, z: 4}, {x: 11, y: 22, z: 33}], b: {x: 3, z: 45}}\nb = {a: [{y: 3}, {x: 11, z: 33}], b: {y: 22}}\n\ndiff = Hashdiff.best_diff(a, b)\ndiff.should == [{\"-\", \"a.x\", 2}, {\"-\", \"a.z\", 4}, {\"-\", \"a.y\", 22}, {\"-\", \"b.x\", 3}, {\"-\", \"b.z\", 45}, {\"+\", \"b.y\", 22}]\n``````\n\n### Patch\n\npatch example:\n\n``````a = {\"a\" => 3}\nb = {\"a\" => {\"a1\" => 1, \"a2\" => 2}}\n\ndiff = Hashdiff.diff(a, b)\nHashdiff.patch!(a, diff).should == b\n``````\n\nunpatch example:\n\n``````a = [{\"a\" => 1, \"b\" => 2, \"c\" => 3, \"d\" => 4, \"e\" => 5}, {\"x\" => 5, \"y\" => 6, \"z\" => 3}, 1]\nb = [1, {\"a\" => 1, \"b\" => 2, \"c\" => 3, \"e\" => 5}]\n\ndiff = Hashdiff.diff(a, b) # diff two array is OK\nHashdiff.unpatch!(b, diff).should == a\n``````\n\n### Options\n\nThere are eight options available: `:delimiter`, `:similarity`, `:strict`, `:indifferent`, `:numeric_tolerance`, `:strip`, `:case_insensitive`, `:array_path` and `:use_lcs`\n\n#### `:delimiter`\n\nYou can specify `:delimiter` to be something other than the default dot. For example:\n\n``````a = {a: {x: 2, y: 3, z: 4}, b: {x: 3, z: 45}}\nb = {a: {y: 3}, b: {y: 3, z: 30}}\n\ndiff = Hashdiff.diff(a, b, delimiter: \"\\t\")\ndiff.should == [{\"-\", \"a\\tx\", 2}, {\"-\", \"a\\tz\", 4}, {\"-\", \"b\\tx\", 3}, {\"~\", \"b\\tz\", 45, 30}, {\"+\", \"b\\ty\", 3}]\n``````\n\n#### `:similarity`\n\nIn cases where you have similar hash objects in arrays, you can pass a custom value for `:similarity` instead of the default `0.8`. This is interpreted as a ratio of similarity (default is 80% similar, whereas `:similarity => 0.5` would look for at least a 50% similarity).\n\n#### `:strict`\n\nThe `:strict` option, which defaults to `true`, specifies whether numeric types are compared on type as well as value. By default, an Integer will never be equal to a Float (e.g. 4 != 4.0). Setting `:strict` to false makes the comparison looser (e.g. 4 == 4.0).\n\n#### `:indifferent`\n\nThe `:indifferent` option, which defaults to `false`, specifies whether to treat hash keys indifferently. Setting `:indifferent` to true has the effect of ignoring differences between symbol keys (ie. {a: 1} ~= {\"a\" => 1})\n\n#### `:numeric_tolerance`\n\nThe :numeric_tolerance option allows for a small numeric tolerance.\n\n``````a = {x: 5, y: 3.75, z: 7}\nb = {x: 6, y: 3.76, z: 7}\n\ndiff = Hashdiff.diff(a, b, numeric_tolerance: 0.1)\ndiff.should == [{\"~\", \"x\", 5, 6}]\n``````\n\n#### `:strip`\n\nThe :strip option strips all strings before comparing.\n\n``````a = {x: 5, s: \"foo \"}\nb = {x: 6, s: \"foo\"}\n\ndiff = Hashdiff.diff(a, b, numeric_tolerance: 0.1, strip: true)\ndiff.should == [{\"~\", \"x\", 5, 6}]\n``````\n\n#### `:case_insensitive`\n\nThe :case_insensitive option makes string comparisons ignore case.\n\n``````a = {x: 5, s: \"FooBar\"}\nb = {x: 6, s: \"foobar\"}\n\ndiff = Hashdiff.diff(a, b, numeric_tolerance: 0.1, case_insensitive: true)\ndiff.should == [{\"~\", \"x\", 5, 6}]\n``````\n\n#### `:array_path`\n\nThe :array_path option represents the path of the diff in an array rather than a string. This can be used to show differences in between hash key types and is useful for `patch!` when used on hashes without string keys.\n\n``````a = {x: 5}\nb = {\"x\" => 6}\n\ndiff = Hashdiff.diff(a, b, array_path: true)\ndiff.should == [{\"-\", [:x], 5}, {\"+\", [\"x\"], 6}]\n``````\n\nFor cases where there are arrays in paths their index will be added to the path.\n\n``````a = {x: [0,1]}\nb = {x: [0,2]}\n\ndiff = Hashdiff.diff(a, b, array_path: true)\ndiff.should == [{\"-\", [:x, 1], 1}, {\"+\", [:x, 1], 2}]\n``````\n\nThis shouldn't cause problems if you are comparing an array with a hash:\n\n``````a = {x: {0=>1}}\nb = {x: }\n\ndiff = Hashdiff.diff(a, b, array_path: true)\ndiff.should == [{\"~\", [:x], {0=>1}, }]\n``````\n\n#### `:use_lcs`\n\nThe :use_lcs option is used to specify whether a Longest common subsequence (LCS) algorithm is used to determine differences in arrays. This defaults to `true` but can be changed to `false` for significantly faster array comparisons (O(n) complexity rather than O(n2) for LCS).\n\nWhen :use_lcs is false the results of array comparisons have a tendency to show changes at indexes rather than additions and subtractions when :use_lcs is true.\n\nNote, currently the :similarity option has no effect when :use_lcs is false.\n\n``````a = {x: [0, 1, 2]}\nb = {x: [0, 2, 2, 3]}\n\ndiff = Hashdiff.diff(a, b, use_lcs: false)\ndiff.should == [{\"~\", \"x\", 1, 2}, {\"+\", \"x\", 3}]\n``````\n\n#### Specifying a custom comparison method\n\nIt's possible to specify how the values of a key should be compared.\n\n``````a = {a: \"car\", b: \"boat\", c: \"plane\"}\nb = {a: \"bus\", b: \"truck\", c: \" plan\"}\n\ndiff = Hashdiff.diff(a, b) do |path, obj1, obj2|\ncase path\nwhen /a|b|c/\nobj1.length == obj2.length\nend\nend\n\ndiff.should == [{\"~\", \"b\", \"boat\", \"truck\"}]\n``````\n\nThe yielded params of the comparison block is `|path, obj1, obj2|`, in which path is the key (or delimited compound key) to the value being compared. When comparing elements in array, the path is with the format `array[*]`. For example:\n\n``````a = {a: \"car\", b: [\"boat\", \"plane\"] }\nb = {a: \"bus\", b: [\"truck\", \" plan\"] }\n\ndiff = Hashdiff.diff(a, b) do |path, obj1, obj2|\ncase path\nwhen \"b[*]\"\nobj1.length == obj2.length\nend\nend\n\ndiff.should == [{\"~\", \"a\", \"car\", \"bus\"}, {\"~\", \"b\", \"plane\", \" plan\"}, {\"-\", \"b\", \"boat\"}, {\"+\", \"b\", \"truck\"}]\n``````\n\nWhen a comparison block is given, it'll be given priority over other specified options. If the block returns value other than `true` or `false`, then the two values will be compared with other specified options.\n\nWhen used in conjunction with the `array_path` option, the path passed in as an argument will be an array. When determining the ordering of an array a key of `\"*\"` will be used in place of the `key[*]` field. It is possible, if you have hashes with integer or `\"*\"` keys, to have problems distinguishing between arrays and hashes - although this shouldn't be an issue unless your data is very difficult to predict and/or your custom rules are very specific.\n\n#### Sorting arrays before comparison\n\nAn order difference alone between two arrays can create too many diffs to be useful. Consider sorting them prior to diffing.\n\n``````a = {a: \"car\", b: [\"boat\", \"plane\"] }\nb = {a: \"car\", b: [\"plane\", \"boat\"] }\n\nHashdiff.diff(a, b).should == [{\"+\", \"b\", \"plane\"}, {\"-\", \"b\", \"plane\"}]\n\nb[:b].sort!\n\nHashdiff.diff(a, b).should == []\n``````\n\n## Contributing\n\n1. Fork it (https://github.com/spoved/hashdiff.cr/fork)\n2. Create your feature branch (`git checkout -b my-new-feature`)\n3. Commit your changes (`git commit -am 'Add some feature'`)\n4. Push to the branch (`git push origin my-new-feature`)\n5. Create a new Pull Request\n\n## Contributors\n\n```hashdiff:\ngithub: spoved/hashdiff.cr\nversion: ~> 1.0.0```\nCrystal >= 1.2.2, < 2.0.0\n\n### Development Dependencies 1\n\n• spectator ~> 0.10.1\n`{'gitlab' => 'arctic-fox/spectator', 'version' => '~> 0.10.1'}`\n\nLast synced ."
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https://www.bartleby.com/solution-answer/chapter-143-problem-13e-mathematical-applications-for-the-management-life-and-social-sciences-11th-edition/9781305108042/13-suppose-that-the-production-function-for-a-product-is-where-x-represents-the-number-of-work-/20cad41d-6041-11e9-8385-02ee952b546e | [
"",
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"Chapter 14.3, Problem 13E",
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"Mathematical Applications for the ...\n\n11th Edition\nRonald J. Harshbarger + 1 other\nISBN: 9781305108042\n\nSolutions\n\nChapter\nSection",
null,
"Mathematical Applications for the ...\n\n11th Edition\nRonald J. Harshbarger + 1 other\nISBN: 9781305108042\nTextbook Problem\n\nSuppose that the production function for a product is z = 4 x y , where x represents the number of work- hours per month and y is the number of available machines. Determine the marginal productivity of (a) x. (b) y.\n\n(a)\n\nTo determine\n\nTo calculate: The marginal productivity of x if the production function for a product is z=4xy, where x represents the number of work-hours per month and y is the number of available machines.\n\nExplanation\n\nGiven Information:\n\nThe production function for a product is z=4xy, where x represents the number of work-hours per month and y is the number of available machines.\n\nFormula used:\n\nFor a production function of the form z=f(x,y), the marginal productivity of x is given by zx and the marginal productivity of y is given by zy.\n\nFor a function f(x,y), the partial derivative of f with respect to x is calculated by taking the derivative of f(x,y) with respect to x and keeping the other variable y constant. The partial derivative of f with respect to x is denoted by fx.\n\nPower of x rule for a real number n is such that, if f(x)=xn then f(x)=nxn1.\n\nChain rule for the function f(x)=u(v(x)) is f(x)=u(v(x))v(x).\n\nConstant function rule for a constant c is such that, if f(x)=c then f(x)=0.\n\nThe coefficient rule for a constant c is such that, if f(x)=cu(x), where u(x) is a differentiable function of x, then f(x)=cu(x)\n\n(b)\n\nTo determine\n\nTo calculate: The marginal productivity of y if the production function for a product is z=4xy, where x represents the number of work-hours per month and y is the number of available machines.\n\nStill sussing out bartleby?\n\nCheck out a sample textbook solution.\n\nSee a sample solution\n\nThe 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\nIn Exercises 6372, evaluate the expression. 65. 12+41612\n\nApplied Calculus for the Managerial, Life, and Social Sciences: A Brief Approach\n\nUse the guidelines of this section to sketch the curve. y=x213\n\nSingle Variable Calculus: Early Transcendentals, Volume I\n\nUse two disjoint sets to show that 0+2=0.\n\nMathematical Excursions (MindTap Course List)\n\nFor\n\nStudy Guide for Stewart's Multivariable Calculus, 8th",
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.64643615,"math_prob":0.99599004,"size":1931,"snap":"2019-43-2019-47","text_gpt3_token_len":408,"char_repetition_ratio":0.17021276,"word_repetition_ratio":0.12890625,"special_character_ratio":0.16053858,"punctuation_ratio":0.075,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9998635,"pos_list":[0,1,2,3,4,5,6,7,8,9,10,11,12],"im_url_duplicate_count":[null,null,null,null,null,null,null,null,null,null,null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-10-14T03:24:42Z\",\"WARC-Record-ID\":\"<urn:uuid:1cfdf402-5f7b-41d6-b949-f3cb6d8b9596>\",\"Content-Length\":\"455163\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:00f6540d-bb0a-4962-aa7e-61df11b4edb7>\",\"WARC-Concurrent-To\":\"<urn:uuid:5f6a2057-ece2-4750-841e-689d19a008fe>\",\"WARC-IP-Address\":\"99.84.104.2\",\"WARC-Target-URI\":\"https://www.bartleby.com/solution-answer/chapter-143-problem-13e-mathematical-applications-for-the-management-life-and-social-sciences-11th-edition/9781305108042/13-suppose-that-the-production-function-for-a-product-is-where-x-represents-the-number-of-work-/20cad41d-6041-11e9-8385-02ee952b546e\",\"WARC-Payload-Digest\":\"sha1:JDQVXJNDEGRROA53HYA2PATQTD3B3ORU\",\"WARC-Block-Digest\":\"sha1:PT72ODHIOPN5IDMW3OQGECXCYSNQK2HD\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-43/CC-MAIN-2019-43_segments_1570986649035.4_warc_CC-MAIN-20191014025508-20191014052508-00010.warc.gz\"}"} |
https://discourse.matplotlib.org/t/incremental-colors-for-lines/15417 | [
"",
null,
"# incremental colors for lines\n\nI have been trying to assign different colors for each line I plot, where the colors are incrementally darkened (or lightened), or selected from a colorbar (e.g. rainbow).\nAny ideas?\n\n···\n\nView this message in context: incremental colors for lines\n\nSent from the matplotlib - users mailing list archive at Nabble.com.\n\n(Sorry for sending this twice, Pythonified, but I forgot to copy the list)\n\nI have been trying to assign different colors for each line I plot, where the colors are incrementally darkened (or lightened), or selected from a colorbar (e.g. rainbow).\nAny ideas?\n\nI posted some code awhile back to do what you’re looking for (see: http://old.nabble.com/Where-to-post-examples-%28specifically,-one-that-may-be-useful-for-time-evolution-plots%29-td23901837.html).\n\nI’m copying the code below again because it’s evolved a bit (I really need to start posting code to github). Anyway, if you copy the attached code to a module, you should be able to call the “cycle_cmap” function to change the cmap globally, or the “cycle_cmap_axes” function to create an axes with the specified cmap.\n\nBest,\n-Tony\n\n#---- start of code\n\nimport matplotlib.pyplot as plt\nimport numpy as np\n\n# reverse these colormaps so that it goes from light to dark\n\nREVERSE_CMAP = [‘summer’, ‘autumn’, ‘winter’, ‘spring’, ‘copper’]\n\n# clip some colormaps so the colors aren’t too light\n\nCMAP_RANGE = dict(gray={‘start’:200, ‘stop’:0},\nBlues={‘start’:60, ‘stop’:255},\nOranges={‘start’:100, ‘stop’:255},\n\n`````` OrRd={'start':60, 'stop':255},\nBuGn={'start':60, 'stop':255},\nPuRd={'start':60, 'stop':255},\nYlGn={'start':60, 'stop':255},\n\nYlGnBu={'start':60, 'stop':255},\nYlOrBr={'start':60, 'stop':255},\nYlOrRd={'start':60, 'stop':255},\nhot={'start':230, 'stop':0},\n\nbone={'start':200, 'stop':0},\npink={'start':160, 'stop':0})\n``````\n\ndef cmap_intervals(length=50, cmap=‘YlOrBr’, start=None, stop=None):\n“”\"Return evenly spaced intervals of a given colormap `cmap`.\n\n``````Colormaps listed in REVERSE_CMAP will be cycled in reverse order. Certain\ncolormaps have pre-specified color ranges in CMAP_RANGE. These module\nvariables ensure that colors cycle from light to dark and light colors are\n\nnot too close to white.\n\nParameters\n``````\n···\n\nOn Wed, May 4, 2011 at 9:51 PM, Pythonified <netdriveremail@…287…> wrote:\n----------\nlength : int\nthe number of colors used before cycling back to first color. When\n`length` is large (> ~10), it is difficult to distinguish between\n\n`````` successive lines because successive colors are very similar.\ncmap : str\nname of a matplotlib colormap (see [matplotlib.pyplot.cm](http://matplotlib.pyplot.cm/))\n\"\"\"\n\ncm = getattr([plt.cm](http://plt.cm/), cmap)\ncrange = CMAP_RANGE.get(cmap, dict(start=0, stop=255))\nif cmap in REVERSE_CMAP:\ncrange = dict(start=crange['stop'], stop=crange['start'])\n\nif start is not None:\ncrange['start'] = start\nif stop is not None:\ncrange['stop'] = stop\n\nif length > abs(crange['start'] - crange['stop']):\n\nprint ('Warning: the input length is greater than the number of ' +\n'colors in the colormap; some colors will be repeated')\nidx = np.linspace(crange['start'], crange['stop'], length).astype([np.int](http://np.int/))\n\nreturn cm(idx)\n``````\n\ndef cycle_cmap(length=50, cmap=‘YlOrBr’, start=None, stop=None):\n“”\"Set default color cycle of matplotlib to a given colormap `cmap`.\n\n``````The default color cycle of matplotlib is set to evenly distribute colors in\n\ncolor cycle over specified colormap.\n\nNote: this function must be called before *any* plot commands because it\nchanges the default color cycle.\n\nSee ``cmap_intervals`` for input details.\n\n\"\"\"\ncolor_cycle = cmap_intervals(length, cmap, start, stop)\n# set_default_color_cycle doesn't play nice with numpy arrays\nplt.rc('axes', color_cycle=color_cycle.tolist())\n``````\n\ndef cycle_cmap_axes(length=50, cmap=‘YlOrBr’, start=None, stop=None):\n“”\"Return axes with color cycle set to a given colormap `cmap`.\n\n``````The color cycle of the axes is set to evenly distribute colors in color\n\ncycle over specified colormap.\n\nSee ``cmap_intervals`` for input details.\n\"\"\"\ncolor_cycle = cmap_intervals(length, cmap, start, stop)\n# set_default_color_cycle doesn't play nice with numpy arrays\n\nax = plt.gca()\nax.set_color_cycle(color_cycle)\nreturn ax\n``````\n\nif name == ‘main’:\nn_lines = 10\nx = np.linspace(0, n_lines)\n\n``````# change the global cmap\ncycle_cmap(n_lines, 'Oranges')\n\nfor shift in np.linspace(0, np.pi, n_lines):\nplt.plot(x, np.sin(x - shift))\n\nplt.figure()\n# create an axes that is set to desired cmap\nax = cycle_cmap_axes(n_lines, 'Blues')\n\nfor shift in np.linspace(0, np.pi, n_lines):\nax.plot(x, np.sin(x - shift))\n\nplt.show()\n``````\n\nPythonified wrote:\n\nI have been trying to assign different colors for each line I plot, where\nthe colors are incrementally darkened (or lightened), or selected from a\ncolorbar (e.g. rainbow).\n\nAny ideas?\n\nI have found a simple and better way. One can chose from colors from a color\nmap:\n\nimport pylab as pl\nimport matplotlib.cm as cm\nxval = pl.arange(0, 20, 0.2)\nfor i in range(256):\n\n... pl.plot(xval, pl.sin(xval)+i, c=cm.hot(i), lw=5)\n\nThis one if, for instance, picking from a color map called \"hot\". If one\nwants to the colors to fade away, or darken, the \"alpha\" option can be\nutilized or another color map in which colors darken or fade into another\ncolor.\n\nThere is no need for a long sophisticated script.\n\nEnjoy,\nPythonified\n\n···\n\n--\nView this message in context: http://old.nabble.com/incremental-colors-for-lines-tp31546719p31581404.html\nSent from the matplotlib - users mailing list archive at Nabble.com.\n\nNice trick. This can go into the gallery or somewhere else in scipy cookbook.\n\n···\n\nOn Mon, May 9, 2011 at 5:11 PM, Pythonified <netdriveremail@…287…> wrote:\n\nPythonified wrote:\n\nI have been trying to assign different colors for each line I plot, where\n\nthe colors are incrementally darkened (or lightened), or selected from a\n\ncolorbar (e.g. rainbow).\n\nAny ideas?\n\nI have found a simple and better way. One can chose from colors from a color\n\nmap:\n\nimport pylab as pl\n\nimport matplotlib.cm as cm\n\nxval = pl.arange(0, 20, 0.2)\n\nfor i in range(256):\n\n`````` ... pl.plot(xval, pl.sin(xval)+i, c=cm.hot(i), lw=5)\n``````\n\nThis one if, for instance, picking from a color map called “hot”. If one\n\nwants to the colors to fade away, or darken, the “alpha” option can be\n\nutilized or another color map in which colors darken or fade into another\n\ncolor.\n\nThere is no need for a long sophisticated script.\n\nEnjoy,\n\nPythonified\n\nGökhan\n\nHi, I like this, too.\n\nHowever, I don't understand why it works at all. Usually, when I apply\na colormap, I need to take care about the scaling myself, i.e. divide\nthe range up into the number of elements to plot:\n\nimport pylab as pl\nimport matplotlib.cm as cm\n\nxval = pl.arange(0, 20, 0.2)\nn = 256\nfor i in range(n):\n# pl.plot(xval, pl.sin(xval)+i, c=cm.hot(i), lw=5)\npl.plot(xval, pl.sin(xval)+i, c=cm.hot(1.*i/n), lw=5)\n\nCan anyone tell me why this is not necessary here but essential for\nexample here:\n\nfor i,infile in enumerate(infiles):\n## title for plot\ntname = os.path.splitext(infile)\n\nf = FileHelpers.BlockedFile(infile)\n\nalldata = scipy.array([[],[]])\nfor ii in ['+', '2', 'x', '1']: # use for markers, too\n# for ii in [4,3,2,1]: # use for markers, too\ntry:\nf.next_block()\nalldata = scipy.concatenate((alldata, data), axis=1)\n# ax.plot(data,data, '%s'%ii,\ncolor=cm.hot(1.*i/len(infiles)), mew=1.5 )\nax.plot(data,data, '%s'%ii, c=cm.hot(i), mew=1.5 )\nexcept Exception, e:\nprint e\nbreak\n\nDaniel\n\n···\n\nI have found a simple and better way. One can chose from colors from a\ncolor\nmap:\n\n>>import pylab as pl\n>>import matplotlib.cm as cm\n>>xval = pl.arange(0, 20, 0.2)\n>>for i in range(256):\n... pl.plot(xval, pl.sin(xval)+i, c=cm.hot(i), lw=5)\n\nThis one if, for instance, picking from a color map called \"hot\". If one\nwants to the colors to fade away, or darken, the \"alpha\" option can be\nutilized or another color map in which colors darken or fade into another\ncolor.\n\nThere is no need for a long sophisticated script."
]
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"https://discourse.matplotlib.org/uploads/default/original/1X/226e21a6b2d1e1ae3ffbb5d50c20c828692648a1.png",
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https://tools.carboncollective.co/inflation/us/1950/81197/2003/ | [
"# $81,197 in 1950 is worth$619,927.30 in 2003\n\n$81,197 in 1950 has the same purchasing power as$619,927.30 in 2003. Over the 53 years this is a change of $538,730.30. The average inflation rate of the dollar between 1950 and 2003 was 3.90% per year. The cumulative price increase of the dollar over this time was 663.49%. ## The value of$81,197 from 1950 to 2003\n\nSo what does this data mean? It means that the prices in 2003 are 6,199.27 higher than the average prices since 1950. A dollar in 2003 can buy 13.10% of what it could buy in 1950.\n\nWe can look at the buying power equivalent for $81,197 in 1950 to see how much you would need to adjust for in order to beat inflation. For 1950 to 2003, if you started with$81,197 in 1950, you would need to have $619,927.30 in 1950 to keep up with inflation rates. So if we are saying that$81,197 is equivalent to $619,927.30 over time, you can see the core concept of inflation in action. The \"real value\" of a single dollar decreases over time. It will pay for fewer items at the store than it did previously. In the chart below you can see how the value of the dollar is worth less over 53 years. ## Value of$81,197 Over Time\n\nIn the table below we can see the value of the US Dollar over time. According to the BLS, each of these amounts are equivalent in terms of what that amount could purchase at the time.\n\nYear Dollar Value Inflation Rate\n1950 $81,197.00 1.26% 1951$87,598.42 7.88%\n1952 $89,283.01 1.92% 1953$89,956.84 0.75%\n1954 $90,630.68 0.75% 1955$90,293.76 -0.37%\n1956 $91,641.43 1.49% 1957$94,673.68 3.31%\n1958 $97,369.02 2.85% 1959$98,042.85 0.69%\n1960 $99,727.44 1.72% 1961$100,738.19 1.01%\n1962 $101,748.94 1.00% 1963$103,096.61 1.32%\n1964 $104,444.27 1.31% 1965$106,128.86 1.61%\n1966 $109,161.11 2.86% 1967$112,530.28 3.09%\n1968 $117,247.12 4.19% 1969$123,648.54 5.46%\n1970 $130,723.80 5.72% 1971$136,451.39 4.38%\n1972 $140,831.31 3.21% 1973$149,591.15 6.22%\n1974 $166,100.09 11.04% 1975$181,261.35 9.13%\n1976 $191,705.78 5.76% 1977$204,171.71 6.50%\n1978 $219,669.89 7.59% 1979$244,601.75 11.35%\n1980 $277,619.62 13.50% 1981$306,257.56 10.32%\n1982 $325,124.92 6.16% 1983$335,569.34 3.21%\n1984 $350,056.78 4.32% 1985$362,522.71 3.56%\n1986 $369,261.05 1.86% 1987$382,737.73 3.65%\n1988 $398,572.83 4.14% 1989$417,777.10 4.82%\n1990 $440,350.54 5.40% 1991$458,880.97 4.21%\n1992 $472,694.57 3.01% 1993$486,845.08 2.99%\n1994 $499,311.01 2.56% 1995$513,461.53 2.83%\n1996 $528,622.79 2.95% 1997$540,751.80 2.29%\n1998 $549,174.73 1.56% 1999$561,303.74 2.21%\n2000 $580,171.10 3.36% 2001$596,680.03 2.85%\n2002 $606,113.71 1.58% 2003$619,927.30 2.28%\n\n## US Dollar Inflation Conversion\n\nIf you're interested to see the effect of inflation on various 1950 amounts, the table below shows how much each amount would be worth today based on the price increase of 663.49%.\n\nInitial Value Equivalent Value\n$1.00 in 1950$7.63 in 2003\n$5.00 in 1950$38.17 in 2003\n$10.00 in 1950$76.35 in 2003\n$50.00 in 1950$381.74 in 2003\n$100.00 in 1950$763.49 in 2003\n$500.00 in 1950$3,817.43 in 2003\n$1,000.00 in 1950$7,634.85 in 2003\n$5,000.00 in 1950$38,174.27 in 2003\n$10,000.00 in 1950$76,348.55 in 2003\n$50,000.00 in 1950$381,742.74 in 2003\n$100,000.00 in 1950$763,485.48 in 2003\n$500,000.00 in 1950$3,817,427.39 in 2003\n$1,000,000.00 in 1950$7,634,854.77 in 2003\n\n## Calculate Inflation Rate for $81,197 from 1950 to 2003 To calculate the inflation rate of$81,197 from 1950 to 2003, we use the following formula:\n\n$$\\dfrac{ 1950\\; USD\\; value \\times CPI\\; in\\; 2003 }{ CPI\\; in\\; 1950 } = 2003\\; USD\\; value$$\n\nWe then replace the variables with the historical CPI values. The CPI in 1950 was 24.1 and 184 in 2003.\n\n$$\\dfrac{ \\81,197 \\times 184 }{ 24.1 } = \\text{ \\619,927.30 }$$\n\n$81,197 in 1950 has the same purchasing power as$619,927.30 in 2003.\n\nTo work out the total inflation rate for the 53 years between 1950 and 2003, we can use a different formula:\n\n$$\\dfrac{\\text{CPI in 2003 } - \\text{ CPI in 1950 } }{\\text{CPI in 1950 }} \\times 100 = \\text{Cumulative rate for 53 years}$$\n\nAgain, we can replace those variables with the correct Consumer Price Index values to work out the cumulativate rate:\n\n$$\\dfrac{\\text{ 184 } - \\text{ 24.1 } }{\\text{ 24.1 }} \\times 100 = \\text{ 663.49\\% }$$\n\n## Inflation Rate Definition\n\nThe inflation rate is the percentage increase in the average level of prices of a basket of selected goods over time. It indicates a decrease in the purchasing power of currency and results in an increased consumer price index (CPI). Put simply, the inflation rate is the rate at which the general prices of consumer goods increases when the currency purchase power is falling.\n\nThe most common cause of inflation is an increase in the money supply, though it can be caused by many different circumstances and events. The value of the floating currency starts to decline when it becomes abundant. What this means is that the currency is not as scarce and, as a result, not as valuable.\n\nBy comparing a list of standard products (the CPI), the change in price over time will be measured by the inflation rate. The prices of products such as milk, bread, and gas will be tracked over time after they are grouped together. Inflation shows that the money used to buy these products is not worth as much as it used to be when there is an increase in these products’ prices over time.\n\nThe inflation rate is basically the rate at which money loses its value when compared to the basket of selected goods – which is a fixed set of consumer products and services that are valued on an annual basis."
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https://answers.everydaycalculation.com/gcf/1617-1890 | [
"Solutions by everydaycalculation.com\n\n## What is the GCF of 1617 and 1890?\n\nThe gcf of 1617 and 1890 is 21.\n\n#### Steps to find GCF\n\n1. Find the prime factorization of 1617\n1617 = 3 × 7 × 7 × 11\n2. Find the prime factorization of 1890\n1890 = 2 × 3 × 3 × 3 × 5 × 7\n3. To find the gcf, multiply all the prime factors common to both numbers:\n\nTherefore, GCF = 3 × 7\n4. GCF = 21\n\nMathStep (Works offline)",
null,
"Download our mobile app and learn how to find GCF of upto four numbers in your own time:"
]
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"https://answers.everydaycalculation.com/mathstep-app-icon.png",
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.81498706,"math_prob":0.9959424,"size":573,"snap":"2020-24-2020-29","text_gpt3_token_len":185,"char_repetition_ratio":0.1142355,"word_repetition_ratio":0.0,"special_character_ratio":0.40314135,"punctuation_ratio":0.08411215,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9963126,"pos_list":[0,1,2],"im_url_duplicate_count":[null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-06-07T10:27:56Z\",\"WARC-Record-ID\":\"<urn:uuid:f8f22ca3-c5af-4ccb-b366-ffcc5b311ce3>\",\"Content-Length\":\"5838\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:034dbf94-f03b-42de-9816-b191a174f349>\",\"WARC-Concurrent-To\":\"<urn:uuid:55a1f021-39ac-4b43-96f5-e37b6ae725ed>\",\"WARC-IP-Address\":\"96.126.107.130\",\"WARC-Target-URI\":\"https://answers.everydaycalculation.com/gcf/1617-1890\",\"WARC-Payload-Digest\":\"sha1:QGEZHLC4WBNPVB4O5WNEDO3UOI5MWFSM\",\"WARC-Block-Digest\":\"sha1:NZVSMX2LTEUTOAMINOK6MYZWYZLHWDPX\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-24/CC-MAIN-2020-24_segments_1590348526471.98_warc_CC-MAIN-20200607075929-20200607105929-00142.warc.gz\"}"} |
http://hafen.github.io/taxi/ | [
"Exploration of NYC Taxi Data\n\n### Background\n\nThis is a simple document outlining some initial exploratory analysis of the NYC taxi data.\n\n### Getting the data\n\nThere are a few sources. I got it from here.\n\nThere are of course plenty of ways to get the data into shape. I chose whatever I could think of most quickly. There is probably an awk one-liner or more efficient way to do it, but it's not very much data and these steps didn't take long.\n\nThere are two sets of files - one for trip data and one for fare data. This site has them broken down into 12 files for each set.\n\nIn a bash shell, you can download and unzip the data with the following:\n\nfor i in {1..12}; do\necho \"$i\" wget \"https://nyctaxitrips.blob.core.windows.net/data/trip_data_$i.csv.zip\"\nwget \"https://nyctaxitrips.blob.core.windows.net/data/trip_fare_$i.csv.zip\" done for f in *.zip; do echo \"$f\"\nunzip $f done rm *.zip It turns out the files have CRLF endings... file * # trip_data_1.csv: ASCII text, with CRLF line terminators # trip_data_10.csv: ASCII text, with CRLF line terminators No good. I converted them to unix format with dos2unix, which may not be installed on all linux flavors, but it's easy to install or there are other ways to deal with it. for f in *.csv; do echo \"$f\"\ndos2unix $f done Looking at the files, it turns out that the number of lines match for each numbered trip and fare file. It would be nice to merge these, but we should make sure before merging that the rows match. Each record seems to be able to be uniquely defined by the medallion, hack_license, and pickup_datetime, which are present in both the trip and fare files. We can run a simple awk command to make sure each these match for each row. # for i in {1..12}; do # echo \"$i\"\n# awk -F',' 'NR==FNR { a[$1,$2,$6]; next } ($1,$2,$4) in a { c++ } END { print c }' \"trip_data_$i.csv\" \"trip_fare_$i.csv\"\n# done\n\n\nThe code is commented out because we have already verified this so no need to re-run unless you really want to. Everything matches, except some header lines have spaces and therefore don't match.\n\n#### Merge trip and fare\n\nNow let's merge the data/fare file pairs only using non-reduncant columns\n\nfor i in {1..12}; do\necho \"$i\" paste -d, \"trip_data_$i.csv\" <(cut -d',' -f5-11 \"trip_fare_$i.csv\") > \"trip_$i.csv\"\ndone\n\n\nThis gives us 12 merged files: trip_1.csv, etc.\n\nFinally, we can remove the original files.\n\nrm trip_data*\nrm trip_fare*\n\n\nThe final data is about 31GB.\n\nReading in the raw data to R is as simple as calling drRead.csv(). However, some initial exploration revealed some transformations that would be good to first apply.\n\n#### Initial transformations\n\nThe first transformation is simply that we want to parse the pickup and dropoff times as POSIXct.\n\nSecond, there are some very large outliers in the pickup and dropoff latitude and longitude that are not plausible and will hinder our analysis. We could deal with this later, but might as well take care of it up front.\n\nFor an idea of what the raw lat/lon data looks like, here are some quantile plots for the dropoff lat/lon, for example:",
null,
"Note that these quantiles have been computed at intervals of 0, 0.005, 0.01, ..., 0.995, 1, so there are more outlying points than those shown in the plot.\n\nAccording to this, the bounding box of NYC city limits is latitude=40.917577, longitude=-74.259090 at the northwest corner, and latitude=40.477399, longitude=-73.700272 at the southeast corner. So we have some very egregious outliers.\n\nWe will set any coordinates outside of this bounding box to NA in our initial transformation. We don't want to remove them altogether as they may contain other interesting information that may be valid.\n\nWe are just looking at the first csv file and using the \"local disk\" back end.\n\nlibrary(datadr)\nlibrary(parallel) # needed for multicore MapReduce\n# set the default backend to be R multicore with 4 cores\noptions(defaultLocalDiskControl = localDiskControl(makeCluster(4)))\n\nnw <- list(lat = 40.917577, lon = -74.259090)\nse <- list(lat = 40.477399, lon = -73.700272)\n\ntrans <- function(x) {\n# convert to POSIXct time\nx$pickup_datetime <- fast_strptime(as.character(x$pickup_datetime), format = \"%Y-%m-%d %H:%M:%S\", tz = \"EST\")\nx$dropoff_datetime <- fast_strptime(as.character(x$dropoff_datetime), format = \"%Y-%m-%d %H:%M:%S\", tz = \"EST\")\n\n# set coordinates outside of NYC bounding box to NA\nind <- which(x$dropoff_longitude < nw$lon | x$dropoff_longitude > se$lon)\nx$dropoff_longitude[ind] <- NA ind <- which(x$pickup_longitude < nw$lon | x$pickup_longitude > se$lon) x$pickup_longitude[ind] <- NA\nind <- which(x$dropoff_latitude < se$lat | x$dropoff_latitude > nw$lat)\nx$dropoff_latitude[ind] <- NA ind <- which(x$pickup_latitude < se$lat | x$pickup_latitude > nw$lat) x$pickup_latitude[ind] <- NA\nx\n}\n\nraw <- drRead.csv(\"data/raw_csv/trip_1.csv\", rowsPerBlock = 300000,\npostTransFn = trans, output = localDiskConn(\"data/raw\"))\n\nraw <- updateAttributes(raw)\n\n\n### Initial Exploration\n\nHere are some simple quick summaries to help us start to get a feel for the data and where we might want to start taking a deeper look. There's a lot more to look at, this is just a quick start.\n\nHere we make use of some of datadr's division-indpendent summary methods that operate over the entire data set and do not care about how it is divided.\n\n#### Connecting to raw data\n\nWe can reconnect to the ddf we read in with the following:\n\nraw <- ddf(localDiskConn(\"data/raw\"))\nraw\n\n\nDistributed data frame backed by 'kvLocalDisk' connection\n\nattribute | value\n----------------+-----------------------------------------------------------\nnames | medallion(cha), hack_license(cha), and 19 more\nnrow | 14776615\nsize (stored) | 844.42 MB\nsize (object) | 2.24 GB\n# subsets | 50\n\n* Other attributes: getKeys(), splitSizeDistn(), splitRowDistn(), summary()\n\n\nWe see that this ddf contains ~14.8 million taxi trips and is split into 50 arbitrary subsets.\n\n#### Summaries\n\nWhen we read in the data, since it is a ddf, summary statistics were computed for each variable:\n\nsummary(raw)\n\n medallion\n---------------------------------------\nlevels : 10000+\nmissing : 0\n7E1346F23960CC18D7D129FA28B63A75 : 2137\n6FFCF7A4F34BA44239636028E680E438 : 2112\nA979CDA04CFB8BA3D3ACBA7E8D7F0661 : 2039\nD5C7CD37EA4D372D00F0A681CDC93F11 : 1959\n---------------------------------------\n--------------------------------------- ------------------\nlevels : 10000+ levels : 2\nmissing : 0 missing : 0\n00B7691D86D96AEBD21DD9E138F90840 : 1933 CMT : 7450899\nF49FD0D84449AE7F72F3BC492CD6C754 : 1616 VTS : 7325716\n847349F8845A667D9AC7CDEDD1C873CB : 1570\n--------------------------------------- ------------------\nrate_code store_and_fwd_flag pickup_datetime\n-------------------- ------------------ ------------------------\nmissing : 0 levels : 3 missing : 0\nmin : 0 missing : 0 min : 12-12-31 16:00\nmax : 210 > freqTable head < max : 13-01-31 15:59\nmean : 1.034273 : 7326207\nstd dev : 0.3387715 N : 7285231\nskewness : 195.5337 Y : 165177\nkurtosis : 113263.8\n-------------------- ------------------ ------------------------\ndropoff_datetime passenger_count trip_time_in_secs\n------------------------ ------------------- -------------------\nmissing : 0 missing : 0 missing : 0\nmin : 12-12-31 16:00 min : 0 min : 0\nmax : 13-02-01 02:33 max : 255 max : 10800\nmean : 1.697372 mean : 683.4236\nstd dev : 1.365396 std dev : 494.4063\nskewness : 2.681262 skewness : 2.27493\nkurtosis : 121.2664 kurtosis : 13.97751\n------------------------ ------------------- -------------------\ntrip_distance pickup_longitude pickup_latitude\n------------------- --------------------- ---------------------\nmissing : 0 missing : 271114 missing : 267926\nmin : 0 min : -74.25858 min : 40.47757\nmax : 100 max : -73.70029 max : 40.91757\nmean : 2.770976 mean : -73.97533 mean : 40.75106\nstd dev : 3.305923 std dev : 0.03428528 std dev : 0.02674132\nskewness : 3.836538 skewness : 3.407925 skewness : -0.9979193\nkurtosis : 32.05707 kurtosis : 18.54463 kurtosis : 6.431953\n------------------- --------------------- ---------------------\ndropoff_longitude dropoff_latitude payment_type\n--------------------- --------------------- ------------------\nmissing : 282583 missing : 278369 levels : 5\nmin : -74.2589 min : 40.47763 missing : 0\nmax : -73.70029 max : 40.91752 > freqTable head <\nmean : -73.97497 mean : 40.75154 CRD : 7743844\nstd dev : 0.03235445 std dev : 0.03000986 CSH : 6982383\nskewness : 2.510542 skewness : -0.5599866 NOC : 32783\nkurtosis : 18.01025 kurtosis : 6.503353 DIS : 11171\n--------------------- --------------------- ------------------\nfare_amount surcharge mta_tax\n------------------- -------------------- ---------------------\nmissing : 0 missing : 0 missing : 0\nmin : 2.5 min : 0 min : 0\nmax : 500 max : 12.5 max : 0.5\nmean : 11.66472 mean : 0.3204904 mean : 0.498397\nstd dev : 9.639219 std dev : 0.3675741 std dev : 0.02826541\nskewness : 4.072831 skewness : 0.6875023 skewness : -17.57604\nkurtosis : 51.30727 kurtosis : 2.39267 kurtosis : 309.9172\n------------------- -------------------- ---------------------\ntip_amount tolls_amount total_amount\n------------------- ------------------- -------------------\nmissing : 0 missing : 0 missing : 0\nmin : 0 min : 0 min : 2.5\nmax : 200 max : 20 max : 650\nmean : 1.267509 mean : 0.201867 mean : 13.95298\nstd dev : 2.046084 std dev : 1.035481 std dev : 11.46469\nskewness : 6.081281 skewness : 5.859475 skewness : 3.887555\nkurtosis : 180.7268 kurtosis : 46.02757 kurtosis : 39.25815\n------------------- ------------------- -------------------\n\n\nThis gives us some initial interesting insight. This data pretty much spans January 2013, credit card and cash are used nearly in equal proportion, the average total fare is $13.95, etc. Let's visualize some of these summaries. Looking at medallion and hack_license, we see that it says there are \"10000+\" levels. The ddf summary method has a cutoff for how many unique levels of a variable to tabulate (to avoid tail cases where there might be millions of unique values). In this case, the top 5000 and bottom 5000 medallions and hack licenses are reported. We can plot the distribution of these by extracting them from the summaries. # medallion frequency table mft <- summary(raw)$medallion$freqTable plot(sort(mft$Freq),\nylab = \"Medallion frequency (top/bottom 5000)\")\nabline(v = 5000, lty = 2, col = \"gray\")",
null,
"This is an interesting distribution - many mediallions were hardly used, while some were used over 2000 times (~65x per day).\n\n# hack_license frequency table\nhft <- summary(raw)$hack_license$freqTable\n\nplot(sort(hft$Freq), ylab = \"Hack frequency (top/bottom 5000)\") abline(v = 5000, lty = 2, col = \"gray\")",
null,
"This is also interesting. Some hacks have driven over 1500 trips - some up to an average of over 50 trips a day, while we know the bottom 5000 of the hacks were involved in 125 or fewer trips (~4 trips or less per day). #### Quantile plots For some of the quantitative variables, we want to look at more than just some summary statistics. We can compute and look at quantile plots for these using drQuantile(). pc_quant <- drQuantile(raw, var = \"passenger_count\", tails = 1) triptime_quant <- drQuantile(raw, var = \"trip_time_in_secs\", tails = 1) tripdist_quant <- drQuantile(raw, var = \"trip_distance\", tails = 1) tot_quant <- drQuantile(raw, var = \"total_amount\", tails = 1) tip_quant <- drQuantile(raw, var = \"tip_amount\", by = \"payment_type\", tails = 1) plat_quant <- drQuantile(raw, var = \"pickup_latitude\", tails = 1) plon_quant <- drQuantile(raw, var = \"pickup_longitude\", tails = 1) dlat_quant <- drQuantile(raw, var = \"dropoff_latitude\", tails = 1) dlon_quant <- drQuantile(raw, var = \"dropoff_longitude\", tails = 1) The tails = 1 argument tells it to only compute 1 exact value at each tail (min and max) - by default it gets all First, passenger count: library(latticeExtra) p1 <- xyplot(q ~ fval, pc_quant, xlab = \"Proportion\", ylab = \"# Passengers\", type = c(\"p\", \"g\")) p2 <- xyplot(q ~ fval, pc_quant, subset = q < 200, xlab = \"Proportion\", ylab = \"# Passengers\", type = c(\"p\", \"g\")) c(p1, p2)",
null,
"The plot on the left shows everything, while the plot on the right truncates the highest outlying percentiles. The max number of passengers is 255 - this is surely an invalid value. It looks like ~70\\% of cab rides have a single passenger, and zero passengers was also reported. Now trip time: p1 <- xyplot(q / 60 ~ fval, triptime_quant, xlab = \"Proportion\", ylab = \"Trip Duration (minutes)\", type = c(\"p\", \"g\")) p2 <- xyplot(q / 60 ~ fval, triptime_quant, xlab = \"Proportion\", ylab = \"Trip Duration (minutes)\", type = c(\"p\", \"g\"), subset = q / 60 < 100) c(p1, p2)",
null,
"Half of cab rides are 10 minutes or less, nearly all are less than an hour. The maximum is 180 minutes. It looks like there is some rounding going on in some cases, not in others. Now trip distance: xyplot(q ~ fval, tripdist_quant, xlab = \"Proportion\", ylab = \"Trip Distance (miles)\", type = c(\"p\", \"g\"), subset = q < 40)",
null,
"Almost 90\\% of cab rides are 5 miles or less. I'm not sure how trip distance is calculated. p1 <- xyplot(q ~ fval, tot_quant, xlab = \"Proportion\", ylab = \"Total Payment (dollars)\", type = c(\"p\", \"g\")) p2 <- xyplot(q ~ fval, tot_quant, xlab = \"Proportion\", ylab = \"Total Payment (dollars)\", type = c(\"p\", \"g\"), subset = q < 200) c(p1, p2)",
null,
"The median cab fare is about$10.\n\nNow for tips. We calculated tip quantiles by payment_type since we were under the suspicion that tips are zero for cash payments.\n\np1 <- xyplot(q ~ fval, tip_quant, groups = payment_type,\nxlab = \"Proportion\", ylab = \"Tip Amount (dollars)\",\ntype = c(\"p\", \"g\"), auto.key = TRUE)\np2 <- xyplot(q ~ fval, tip_quant, groups = payment_type,\nxlab = \"Proportion\", ylab = \"Tip Amount (dollars)\",\ntype = c(\"p\", \"g\"), auto.key = TRUE, subset = q < 25)\nc(p1, p2)",
null,
"Other than CRD and UNK, tip amounts are zero. Although every category has at least some positive tip amount (see the highest quantiles on the left plot).\n\n#### Some bivariate relationships\n\nWe can look at high-level summaries of some bivariate relationships with drHexbin(), which computes hexagon-binned counts across the entire data set.\n\nFirst, let's look at pickup_latitude vs pickup_latitude:\n\npickup_latlon <- drHexbin(\"pickup_longitude\", \"pickup_latitude\", data = raw, xbins = 300, shape = 1.4)\n\nlibrary(hexbin)\nplot(pickup_latlon, trans = log, inv = exp, style = \"centroids\", xlab = \"longitude\", ylab = \"latitude\", legend = FALSE)",
null,
"With a different color ramp:\n\nplot(pickup_latlon, trans = log, inv = exp, style = \"colorscale\", xlab = \"longitude\", ylab = \"latitude\", colramp = LinOCS)",
null,
"Zooming in on Manhattan:\n\nxRange <- c(-74.03, -73.92)\nyRange <- c(40.7, 40.82)\nsubset(x, pickup_longitude < -73.92 & pickup_longitude > -74.03 &\npickup_latitude > 40.7 & pickup_latitude < 40.82)\n})\npickup_latlon_manhat <- drHexbin(\"pickup_longitude\", \"pickup_latitude\", data = tmp, xbins = 300, shape = 1.4, xRange = xRange, yRange = yRange)\n\nplot(pickup_latlon_manhat, trans = log, inv = exp, style = \"centroids\", xlab = \"longitude\", ylab = \"latitude\", legend = FALSE)",
null,
"plot(pickup_latlon_manhat, trans = log, inv = exp, style = \"colorscale\", xlab = \"longitude\", ylab = \"latitude\", colramp = LinOCS)",
null,
"Total amount vs. trip distance:\n\ntrns <- function(x) log2(x + 1)\namount_vs_dist <- drHexbin(\"trip_distance\", \"total_amount\", data = raw, xbins = 150, shape = 1, xTransFn = trns, yTransFn = trns)\n\nplot(amount_vs_dist, trans = log, inv = exp, style = \"colorscale\", colramp = LinOCS, xlab = \"Distance (log2 miles)\", ylab = \"Total Amount Paid (log2 dollars)\")",
null,
"There appears to be two major trajectories, as well as a fixed distance-independent flat rate around 26=\\$64. There is also obviously some garbage going on here.\n\nTrip time vs. trip distance:\n\ntrns2 <- function(x) log2(x / 60 + 1)\ntime_vs_dist <- drHexbin(\"trip_distance\", \"trip_time_in_secs\", data = raw, xbins = 150, shape = 1, xTransFn = trns, yTransFn = trns2)\n\nplot(time_vs_dist, trans = log, inv = exp, style = \"colorscale\", colramp = LinOCS, xlab = \"Distance (log2 miles)\", ylab = \"Trip Time (log2 minutes)\")",
null,
""
]
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"http://hafen.github.io/taxi/figures/knitr/unnamed-chunk-3-1.png",
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.7145742,"math_prob":0.9647866,"size":16282,"snap":"2020-10-2020-16","text_gpt3_token_len":4760,"char_repetition_ratio":0.15524021,"word_repetition_ratio":0.13780919,"special_character_ratio":0.38932565,"punctuation_ratio":0.19401479,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9912871,"pos_list":[0,1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28],"im_url_duplicate_count":[null,1,null,1,null,1,null,1,null,1,null,1,null,1,null,1,null,1,null,1,null,1,null,1,null,1,null,1,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-02-19T03:18:11Z\",\"WARC-Record-ID\":\"<urn:uuid:5c863377-cb58-4a02-ba5f-2cdc5a2652ac>\",\"Content-Length\":\"27418\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:ee1cd58f-adcd-4e6e-9a73-28d4032ec801>\",\"WARC-Concurrent-To\":\"<urn:uuid:0e535f9e-1f6d-46a1-b61a-3524a63b3c32>\",\"WARC-IP-Address\":\"185.199.110.153\",\"WARC-Target-URI\":\"http://hafen.github.io/taxi/\",\"WARC-Payload-Digest\":\"sha1:IQF5WYJKBAVWZNZVHSHLKBDEZABBU5VQ\",\"WARC-Block-Digest\":\"sha1:XPNSHPWNQ6NVHLTHFSUE5UJU7PURRGCD\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-10/CC-MAIN-2020-10_segments_1581875144027.33_warc_CC-MAIN-20200219030731-20200219060731-00330.warc.gz\"}"} |
https://bestbinaryqkxba.netlify.app/manteca82257goqo/growth-percent-in-excel-328.html | [
"## Growth percent in excel\n\nIf you need to increase a number by a certain percentage, you can use a simple formula that multiplies the number times the percent + 1. How this formula works If want to calculate a percentage increase in Excel (i.e. increase a number by a specified percentage), this can be done by simply multiply the number by 1 + the To calculate the percentage increase in Excel which must have at least two values. For example, if we have 2 numbers, then to find the percentage increase we\n\nExcel: Increase Excel Values by Percentage (%), Multiply, Add, Subtract or Divide . Current Special! Complete Excel Excel Training Course for Excel 97 - Excel From a chart in Excel I need to automatically calculate what the annual percentage growth rate is of a trend line. Does anyone know how to automate this in 8 Oct 2019 This tutorial teaches you everything about percentages in Excel. Learn to convert decimals to percentages, calculate percentage change, and In the example, when you enter the formula, Excel displays \"12.67605634\" meaning you have a 12.67 percent increase. Show Comments CAGR stands for Compound Annual Growth Rate. CAGR is the year-over-year average growth rate I am trying to calculate percentage growth in excel with a positive and negative number. This Year's value: 2434 Last Year's value: -2. formula I'm\n\n## 10 Nov 2018 Divide the difference by the previous year's total sales. Convert the value to percentages. Let's take a look at the following example.\n\nIf want to calculate a percentage increase in Excel (i.e. increase a number by a specified percentage), this can be done by simply multiply the number by 1 + the To calculate the percentage increase in Excel which must have at least two values. For example, if we have 2 numbers, then to find the percentage increase we Excel Growth Rates. How to Calculate BOTH Types of Compound Growth Rates in Excel. To calculate the correct growth rate you need to be clear about what 12 Nov 2013 Paolo Lenotti of Excel with Business is on hand to show you how. Average percentage growth is not an official accounting or bookkeeping term,\n\n### 25 Feb 2017 This example looks at calculating average trends using percentages a percentage growth factor to 2010's number but rather a value growth\n\nStep 6: The resultant will be the annual growth rate. Examples of Growth Rate Calculation. You can download this Growth Rate Formula Excel Template here – Will someone help me in calculating Compound Growth Rate (CGR) in MS Excel ? I have mentioned the formula of it along with attached a paper using the The Microsoft Excel program allows you to work quickly with the percent's: find them, summarize them, add them to the number, calculate the % increase, the 25 Feb 2017 This example looks at calculating average trends using percentages a percentage growth factor to 2010's number but rather a value growth\n\n### If want to calculate a percentage increase in Excel (i.e. increase a number by a specified percentage), this can be done by simply multiply the number by 1 + the\n\n18 Sep 2014 To get your profit percentage, enter the percentage formula for Excel “=a2-b2” into the c2 Profit cell. Once you have calculated the profit amount, 4 Aug 2017 Let Excel do the work for you – simple formulas can help you find the percentage of a total, for example, or the percentage difference between\n\n## 12 Nov 2013 Paolo Lenotti of Excel with Business is on hand to show you how. Average percentage growth is not an official accounting or bookkeeping term,\n\nThe Microsoft Excel program allows you to work quickly with the percent's: find them, summarize them, add them to the number, calculate the % increase, the 25 Feb 2017 This example looks at calculating average trends using percentages a percentage growth factor to 2010's number but rather a value growth Quickly learn to calculate the increase or decrease in percentage terms. Formula, real-life examples and percentage change calculator.\n\nLet Excel do the work for you – simple formulas can help you find the percentage of a total, for example, or the percentage difference between two numbers. The percent change formula is used very often in Excel. For example, to calculate the Monthly Change and Total Change. Now the percentage difference between two given numbers is calculated. The Best Office Productivity Tools. Kutools for Excel Solves Most of Your Problems, and"
]
| [
null
]
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https://www.mathworks.com/matlabcentral/cody/problems/43294-can-we-make-a-triangle/solutions/1885246 | [
"Cody\n\n# Problem 43294. Can we make a triangle?\n\nSolution 1885246\n\nSubmitted on 26 Jul 2019 by Christian Schröder\nThis solution is locked. To view this solution, you need to provide a solution of the same size or smaller.\n\n### Test Suite\n\nTest Status Code Input and Output\n1 Pass\nassert(isequal(Is_Triangle(3,4,6),true))\n\n2 Pass\nassert(isequal(Is_Triangle(6,4,3),true))\n\n3 Pass\nassert(isequal(Is_Triangle(3,7,4),false))\n\n4 Pass\nassert(isequal(Is_Triangle(4,3,7),false))\n\n5 Pass\nassert(isequal(Is_Triangle(3,3,4),true))\n\n### Community Treasure Hunt\n\nFind the treasures in MATLAB Central and discover how the community can help you!\n\nStart Hunting!"
]
| [
null
]
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http://www.talks.cam.ac.uk/talk/index/119449 | [
"# Statistical analysis of a non-linear inverse problem for an elliptic PDE\n\n•",
null,
"Sven Wang, University of Cambridge\n•",
null,
"Wednesday 30 January 2019, 16:00-17:00\n•",
null,
"MR14, Centre for Mathematical Sciences.\n\nThe talk will be about some statistical inverse problems arising in the context of second order elliptic PDEs. Concretely, suppose $f$ is the unknown coefficient function of a second order elliptic partial differential operator $L_f$ on some bounded domain $\\mathcal O\\subseteq \\R^d$, and the unique solution $u_f$ of a corresponding boundary value problem is observed, corrupted by additive Gaussian white noise. Concrete examples include $L_fu=\\Delta u-2fu$ (Schr\\”odinger equation with attenuation potential $f$) and $L_fu=\\text{div} (f\\nabla u)$ (divergence form equation with conductivity $f$). I will present some recent results on the convergence rates for Tikhonov-type penalised least squares estimators $\\hat f$ for $f$ in these contexts. The penalty functionals are of squared Sobolev-norm type and thus $\\hat f$ can also be interpreted as a Bayesian `MAP’-estimator corresponding to some Gaussian process prior. We derive rates of convergence of $\\hat f$ and of $u_{\\hat f}$, to $f, u_f$, respectively. The rates obtained are minimax-optimal in prediction loss.\n\nThis talk is part of the Cambridge Analysts' Knowledge Exchange series."
]
| [
null,
"http://talks.cam.ac.uk/images/user.jpg",
null,
"http://talks.cam.ac.uk/images/clock.jpg",
null,
"http://talks.cam.ac.uk/images/house.jpg",
null
]
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https://homework.cpm.org/category/CCI_CT/textbook/PC3/chapter/Ch8/lesson/8.3.3/problem/8-125 | [
"",
null,
"",
null,
"### Home > PC3 > Chapter Ch8 > Lesson 8.3.3 > Problem8-125\n\n8-125.\n\nThe graph of $y = -2\\left(x + 1\\right)^{3} - 5$ is to be shifted $4$ units to the left and $7$ units down. Write the equation of the new graph.\n\nWrite your equation for the new graph. Then use a graphing calculator to graph the original equation and your shifted equation. Check your work, identifying and correcting any mistakes."
]
| [
null,
"https://homework.cpm.org/dist/7d633b3a30200de4995665c02bdda1b8.png",
null,
"data:image/png;base64,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",
null
]
| {"ft_lang_label":"__label__en","ft_lang_prob":0.8440507,"math_prob":0.9993661,"size":261,"snap":"2020-34-2020-40","text_gpt3_token_len":65,"char_repetition_ratio":0.15953307,"word_repetition_ratio":0.0,"special_character_ratio":0.26819924,"punctuation_ratio":0.13461539,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99314666,"pos_list":[0,1,2,3,4],"im_url_duplicate_count":[null,null,null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-08-06T22:58:52Z\",\"WARC-Record-ID\":\"<urn:uuid:d5ae2268-49e1-4c03-bf2f-01258f1f37df>\",\"Content-Length\":\"34043\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:1acf0f21-aa6a-4274-9d66-cea7191c575a>\",\"WARC-Concurrent-To\":\"<urn:uuid:cf1a4092-398f-44b9-b976-4d7d3a799ec2>\",\"WARC-IP-Address\":\"104.26.6.16\",\"WARC-Target-URI\":\"https://homework.cpm.org/category/CCI_CT/textbook/PC3/chapter/Ch8/lesson/8.3.3/problem/8-125\",\"WARC-Payload-Digest\":\"sha1:DTY3DG5MCMNU7HMXWOM6W262KUDLHYB6\",\"WARC-Block-Digest\":\"sha1:JRUCZRHXP2GHHGYAR44GBEVOKYSGPNAJ\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-34/CC-MAIN-2020-34_segments_1596439737039.58_warc_CC-MAIN-20200806210649-20200807000649-00459.warc.gz\"}"} |
http://www.numbersaplenty.com/612216 | [
"Search a number\nBaseRepresentation\nbin10010101011101111000\n31011002210200\n42111131320\n5124042331\n621042200\n75126613\noct2253570\n91132720\n10612216\n11388a70\n12256360\n13185877\n1411d17a\n15c15e6\nhex95778\n\n612216 has 48 divisors (see below), whose sum is σ = 1811160. Its totient is φ = 185280.\n\nThe previous prime is 612193. The next prime is 612217.\n\nIt can be divided in two parts, 612 and 216, that added together give a palindrome (828).\n\nIt is a happy number.\n\n612216 is nontrivially palindromic in base 10.\n\nIt is a Harshad number since it is a multiple of its sum of digits (18).\n\nIt is a nude number because it is divisible by every one of its digits.\n\nIt is a congruent number.\n\nIt is not an unprimeable number, because it can be changed into a prime (612217) by changing a digit.\n\nIt is a pernicious number, because its binary representation contains a prime number (11) of ones.\n\nIt is a polite number, since it can be written in 11 ways as a sum of consecutive naturals, for example, 406 + ... + 1178.\n\n2612216 is an apocalyptic number.\n\n612216 is a gapful number since it is divisible by the number (66) formed by its first and last digit.\n\nIt is an amenable number.\n\nIt is a practical number, because each smaller number is the sum of distinct divisors of 612216, and also a Zumkeller number, because its divisors can be partitioned in two sets with the same sum (905580).\n\n612216 is an abundant number, since it is smaller than the sum of its proper divisors (1198944).\n\nIt is a pseudoperfect number, because it is the sum of a subset of its proper divisors.\n\n612216 is a wasteful number, since it uses less digits than its factorization.\n\n612216 is an odious number, because the sum of its binary digits is odd.\n\nThe sum of its prime factors is 796 (or 789 counting only the distinct ones).\n\nThe product of its digits is 144, while the sum is 18.\n\nThe square root of 612216 is about 782.4423301433. The cubic root of 612216 is about 84.9118347655.\n\nThe spelling of 612216 in words is \"six hundred twelve thousand, two hundred sixteen\"."
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.932484,"math_prob":0.9920994,"size":1919,"snap":"2020-24-2020-29","text_gpt3_token_len":506,"char_repetition_ratio":0.18224543,"word_repetition_ratio":0.0056980057,"special_character_ratio":0.32152164,"punctuation_ratio":0.12935324,"nsfw_num_words":1,"has_unicode_error":false,"math_prob_llama3":0.99747396,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-06-02T20:30:38Z\",\"WARC-Record-ID\":\"<urn:uuid:c4fa317d-a289-4081-bbea-ec973d279202>\",\"Content-Length\":\"10359\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:727dd3fe-824b-4a16-9b1f-a88623f7fe5b>\",\"WARC-Concurrent-To\":\"<urn:uuid:f123437c-5337-42c5-84cf-f58f004eb54e>\",\"WARC-IP-Address\":\"62.149.142.170\",\"WARC-Target-URI\":\"http://www.numbersaplenty.com/612216\",\"WARC-Payload-Digest\":\"sha1:URW327J54UDTJJ44RZUURKYYG7TEXMHZ\",\"WARC-Block-Digest\":\"sha1:K7RTHZ3CO6FBNHCRFVF2KBK3OK5H7SR3\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-24/CC-MAIN-2020-24_segments_1590347426801.75_warc_CC-MAIN-20200602193431-20200602223431-00595.warc.gz\"}"} |
https://www.jpost.com/breaking-news/molotov-cocktails-thrown-at-car-near-nablus-no-injuries-reported | [
"(function (a, d, o, r, i, c, u, p, w, m) { m = d.getElementsByTagName(o), a[c] = a[c] || {}, a[c].trigger = a[c].trigger || function () { (a[c].trigger.arg = a[c].trigger.arg || []).push(arguments)}, a[c].on = a[c].on || function () {(a[c].on.arg = a[c].on.arg || []).push(arguments)}, a[c].off = a[c].off || function () {(a[c].off.arg = a[c].off.arg || []).push(arguments) }, w = d.createElement(o), w.id = i, w.src = r, w.async = 1, w.setAttribute(p, u), m.parentNode.insertBefore(w, m), w = null} )(window, document, \"script\", \"https://95662602.adoric-om.com/adoric.js\", \"Adoric_Script\", \"adoric\",\"9cc40a7455aa779b8031bd738f77ccf1\", \"data-key\");\nvar domain=window.location.hostname; var params_totm = \"\"; (new URLSearchParams(window.location.search)).forEach(function(value, key) {if (key.startsWith('totm')) { params_totm = params_totm +\"&\"+key.replace('totm','')+\"=\"+value}}); var rand=Math.floor(10*Math.random()); var script=document.createElement(\"script\"); script.src=`https://stag-core.tfla.xyz/pre_onetag?pub_id=34&domain=\\${domain}&rand=\\${rand}&min_ugl=0\\${params_totm}`; document.head.append(script);"
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https://visualfractions.com/calculator/factors/factors-of-466/ | [
"# Factors of 466\n\nSo you need to find the factors of 466 do you? In this quick guide we'll describe what the factors of 466 are, how you find them and list out the factor pairs of 466 for you to prove the calculation works. Let's dive in!\n\nWant to quickly learn or show students how to find the factors of 466? Play this very quick and fun video now!\n\n## Factors of 466 Definition\n\nWhen we talk about the factors of 466, what we really mean is all of the positive and negative integers (whole numbers) that can be evenly divided into 466. If you were to take 466 and divide it by one of its factors, the answer would be another factor of 466.\n\nLet's look at how to find all of the factors of 466 and list them out.\n\n## How to Find the Factors of 466\n\nWe just said that a factor is a number that can be divided equally into 466. So the way you find and list all of the factors of 466 is to go through every number up to and including 466 and check which numbers result in an even quotient (which means no decimal place).\n\nDoing this by hand for large numbers can be time consuming, but it's relatively easy for a computer program to do it. Our calculator has worked this out for you. Here are all of the factors of 466:\n\n• 466 ÷ 1 = 466\n• 466 ÷ 2 = 233\n• 466 ÷ 233 = 2\n• 466 ÷ 466 = 1\n\nAll of these factors can be used to divide 466 by and get a whole number. The full list of positive factors for 466 are:\n\n1, 2, 233, and 466\n\n## Negative Factors of 466\n\nTechnically, in math you can also have negative factors of 466. If you are looking to calculate the factors of a number for homework or a test, most often the teacher or exam will be looking for specifically positive numbers.\n\nHowever, we can just flip the positive numbers into negatives and those negative numbers would also be factors of 466:\n\n-1, -2, -233, and -466\n\n## How Many Factors of 466 Are There?\n\nAs we can see from the calculations above there are a total of 4 positive factors for 466 and 4 negative factors for 466 for a total of 8 factors for the number 466.\n\nThere are 4 positive factors of 466 and 4 negative factors of 466. Wht are there negative numbers that can be a factor of 466?\n\n## Factor Pairs of 466\n\nA factor pair is a combination of two factors which can be multiplied together to equal 466. For 466, all of the possible factor pairs are listed below:\n\n• 1 x 466 = 466\n• 2 x 233 = 466\n\nWe have also written a guide that goes into a little more detail about the factor pairs for 466 in case you are interested!\n\nJust like before, we can also list out all of the negative factor pairs for 466:\n\n• -1 x -466 = 466\n• -2 x -233 = 466\n\nNotice in the negative factor pairs that because we are multiplying a minus with a minus, the result is a positive number.\n\nSo there you have it. A complete guide to the factors of 466. You should now have the knowledge and skills to go out and calculate your own factors and factor pairs for any number you like.\n\nFeel free to try the calculator below to check another number or, if you're feeling fancy, grab a pencil and paper and try and do it by hand. Just make sure to pick small numbers!\n\nIf you found this content useful in your research, please do us a great favor and use the tool below to make sure you properly reference us wherever you use it. We really appreciate your support!\n\n• \"Factors of 466\". VisualFractions.com. Accessed on September 29, 2023. http://visualfractions.com/calculator/factors/factors-of-466/.\n\n• \"Factors of 466\". VisualFractions.com, http://visualfractions.com/calculator/factors/factors-of-466/. Accessed 29 September, 2023."
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.9197191,"math_prob":0.9458651,"size":3875,"snap":"2023-40-2023-50","text_gpt3_token_len":965,"char_repetition_ratio":0.20253165,"word_repetition_ratio":0.012784091,"special_character_ratio":0.27974194,"punctuation_ratio":0.100871734,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99526936,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-09-29T19:56:57Z\",\"WARC-Record-ID\":\"<urn:uuid:a9a01cf6-7003-4211-8693-d131d4ca4280>\",\"Content-Length\":\"28357\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:aa4209c2-fb1b-4bfb-81b2-de8eccd944fb>\",\"WARC-Concurrent-To\":\"<urn:uuid:83bf6947-9082-4409-a29a-0a678256882c>\",\"WARC-IP-Address\":\"104.21.46.54\",\"WARC-Target-URI\":\"https://visualfractions.com/calculator/factors/factors-of-466/\",\"WARC-Payload-Digest\":\"sha1:4DTI5XLIV7ANRVADDRYGRLNCIA6L3JC4\",\"WARC-Block-Digest\":\"sha1:UEQDRY4J4NXX2E2JKVJEBPR4Q2BLAQCY\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-40/CC-MAIN-2023-40_segments_1695233510528.86_warc_CC-MAIN-20230929190403-20230929220403-00411.warc.gz\"}"} |
https://rasterio.groups.io/g/main/topic/save/31667785?p=,,,20,0,0,0::recentpostdate/sticky,,,20,2,220,31667785,previd%3D1567021737651489178,nextid%3D1557253771674814696&previd=1567021737651489178&nextid=1557253771674814696 | [
"#### save\n\nGabriel Cotlier\n\nAfter following the steps in the tutorial of the Planet website (https://developers.planet.com/tutorials/convert-planetscope-imagery-from-radiance-to-reflectance/), I want to save each individual band of a RapidEye image Level 3B as a separate GeoTIFF layer file to be able to open it in any other GIS-software such as QGIS, ArcGIS other. I could not succeed in saving each band separately as GeoTIFF layer file. Here is the code:\n\n```\n#!/usr/bin/env python\n# coding: utf-8\n\nimport rasterio\nimport numpy as np\n\nfilename = \"20180308_133037_1024_3B_AnalyticMS.tif\"\n\n# Load red and NIR bands - note all PlanetScope 4-band images have band order BGRN\nwith rasterio.open(filename) as src:\n\nwith rasterio.open(filename) as src:\n\nwith rasterio.open(filename) as src:\n\nwith rasterio.open(filename) as src:\n\nfrom xml.dom import minidom\n\n# XML parser refers to bands by numbers 1-4\ncoeffs = {}\nfor node in nodes:\nbn = node.getElementsByTagName(\"ps:bandNumber\").firstChild.data\nif bn in ['1', '2', '3', '4']:\ni = int(bn)\nvalue = node.getElementsByTagName(\"ps:reflectanceCoefficient\").firstChild.data\ncoeffs[i] = float(value)\n\nprint \"Conversion coefficients:\", coeffs\n\n# Multiply the Digital Number (DN) values in each band by the TOA reflectance coefficients\n\nimport numpy as np\nprint \"Red band reflectance is from {} to {}\".format(np.amin(band_red_reflectance), np.amax(band_red_reflectance))\n\nprint \"Before Scaling, red band reflectance is from {} to {}\".format(np.amin(band_red_reflectance), np.amax(band_red_reflectance))\n\n# Here we include a fixed scaling factor. This is common practice.\nscale = 10000\nblue_ref_scaled = scale * band_blue_reflectance\ngreen_ref_scaled = scale * band_green_reflectance\nred_ref_scaled = scale * band_red_reflectance\nnir_ref_scaled = scale * band_nir_reflectance\n\nprint \"After Scaling, red band reflectance is from {} to {}\".format(np.amin(red_ref_scaled), np.amax(red_ref_scaled))\n```\nHere I tried unsuccessfully to save each individual band as GeotiFF file.\n\nI have tried, any idea how to do the save of each band correctly to further open in QGIS orArGIS for calculating NDVI there?\n\n```\ndst_crs='EPSG:32720'\n\n## saving bands individualy\nnew_dataset = rasterio.open(\n'ReflectanceB1.tif',\n'w',\ndriver='GTiff',\nheight=band_blue_reflectance.shape,\nwidth=band_blue_reflectance.shape,\ncount=1,\ndtype=band_blue_reflectance.dtype,\ncrs=dst_crs,\n)\n\nnew_dataset.write(band_blue_reflectance, 1)\nnew_dataset.close()\n\nnew_dataset = rasterio.open(\n'ReflectanceB2.tif',\n'w',\ndriver='GTiff',\nheight=band_red_reflectance.shape,\nwidth=band_red_reflectance.shape,\ncount=1,\ndtype=band_red_reflectance.dtype,\ncrs=dst_crs,\n)\n\nnew_dataset.write(band_red_reflectance, 1)\nnew_dataset.close()\n\nnew_dataset = rasterio.open(\n'ReflectanceB3.tif',\n'w',\ndriver='GTiff',\nheight=band_red_reflectance.shape,\nwidth=band_red_reflectance.shape,\ncount=1,\ndtype=band_red_reflectance.dtype,\ncrs=dst_crs,\n)\n\nnew_dataset.write(band_red_reflectance, 1)\nnew_dataset.close()\n\nnew_dataset = rasterio.open(\n'ReflectanceB4.tif',\n'w',\ndriver='GTiff',\nheight=band_red_reflectance.shape,\nwidth=band_red_reflectance.shape,\ncount=1,\ndtype=band_red_reflectance.dtype,\ncrs=dst_crs,\n)\n\nnew_dataset.write(band_red_reflectance, 1)\nnew_dataset.close()\n```\nI'm using as input image \"20180308_133037_1024_3B_AnalyticMS.tif\" instead of \"20180308_133037_1024_3B_AnalyticMS_SR.tif\" don't know if is the problem\n\nI'm getting resulting GeoTIFF file but when I open it in ArcMap I get this error\n\n[![enter image description here]]\n\n: https://i.stack.imgur.com/zJ73V.jpg\n\nThe GeoTIFF band are there and can be seen at ArcMap screen... but the error appear anyway... might be related to coordinate systems to be defined possibly while saving in rasterio? And need to have it correctly projected for clipping with shapefiles.\n\n 1 - 1 of 1"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.66081816,"math_prob":0.8382073,"size":4449,"snap":"2022-27-2022-33","text_gpt3_token_len":1259,"char_repetition_ratio":0.18672666,"word_repetition_ratio":0.09406953,"special_character_ratio":0.27197123,"punctuation_ratio":0.20027064,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9820176,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2022-08-10T04:25:39Z\",\"WARC-Record-ID\":\"<urn:uuid:ba0a4512-4125-4f9e-9753-6f4a12931d69>\",\"Content-Length\":\"88341\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:24c0bac7-ada0-4dc6-8c3c-1a76b5cdcaf0>\",\"WARC-Concurrent-To\":\"<urn:uuid:61d31a5b-61fb-41fd-9cb6-59bb8360ac62>\",\"WARC-IP-Address\":\"45.79.81.153\",\"WARC-Target-URI\":\"https://rasterio.groups.io/g/main/topic/save/31667785?p=,,,20,0,0,0::recentpostdate/sticky,,,20,2,220,31667785,previd%3D1567021737651489178,nextid%3D1557253771674814696&previd=1567021737651489178&nextid=1557253771674814696\",\"WARC-Payload-Digest\":\"sha1:CR47QJQ4A7VM3EBNABMUKKEFRJNWM5XB\",\"WARC-Block-Digest\":\"sha1:FS7IG5DRNVMQWIRL2H6QQHTQ4JUBNFU3\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2022/CC-MAIN-2022-33/CC-MAIN-2022-33_segments_1659882571147.84_warc_CC-MAIN-20220810040253-20220810070253-00635.warc.gz\"}"} |
https://www.numbers.education/26137.html | [
"Is 26137 a prime number? What are the divisors of 26137?\n\n## Parity of 26 137\n\n26 137 is an odd number, because it is not evenly divisible by 2.\n\nFind out more:\n\n## Is 26 137 a perfect square number?\n\nA number is a perfect square (or a square number) if its square root is an integer; that is to say, it is the product of an integer with itself. Here, the square root of 26 137 is about 161.669.\n\nThus, the square root of 26 137 is not an integer, and therefore 26 137 is not a square number.\n\n## What is the square number of 26 137?\n\nThe square of a number (here 26 137) is the result of the product of this number (26 137) by itself (i.e., 26 137 × 26 137); the square of 26 137 is sometimes called \"raising 26 137 to the power 2\", or \"26 137 squared\".\n\nThe square of 26 137 is 683 142 769 because 26 137 × 26 137 = 26 1372 = 683 142 769.\n\nAs a consequence, 26 137 is the square root of 683 142 769.\n\n## Number of digits of 26 137\n\n26 137 is a number with 5 digits.\n\n## What are the multiples of 26 137?\n\nThe multiples of 26 137 are all integers evenly divisible by 26 137, that is all numbers such that the remainder of the division by 26 137 is zero. There are infinitely many multiples of 26 137. The smallest multiples of 26 137 are:\n\n## Numbers near 26 137\n\n### Nearest numbers from 26 137\n\nFind out whether some integer is a prime number"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.86712015,"math_prob":0.99800456,"size":354,"snap":"2021-43-2021-49","text_gpt3_token_len":104,"char_repetition_ratio":0.19428572,"word_repetition_ratio":0.0,"special_character_ratio":0.35875705,"punctuation_ratio":0.16091955,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9988846,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-10-19T23:48:42Z\",\"WARC-Record-ID\":\"<urn:uuid:c9e5d407-f5fd-4fab-a532-b69c4cfe8d54>\",\"Content-Length\":\"18699\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:e377c499-2761-492e-89b0-30d93064f9ec>\",\"WARC-Concurrent-To\":\"<urn:uuid:94780f2b-00b8-4724-aca0-aba7282a468d>\",\"WARC-IP-Address\":\"213.186.33.19\",\"WARC-Target-URI\":\"https://www.numbers.education/26137.html\",\"WARC-Payload-Digest\":\"sha1:FSOJ4QYFGEYUAHVHSJTKIYKDBLZ4ISLY\",\"WARC-Block-Digest\":\"sha1:6F7HCTNIPIDPMIVPW3O2OEN5VOTO7F2G\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-43/CC-MAIN-2021-43_segments_1634323585290.83_warc_CC-MAIN-20211019233130-20211020023130-00682.warc.gz\"}"} |
https://socratic.org/questions/how-do-you-solve-frac-x-2-3x-28-x-x-7 | [
"# How do you solve \\frac{x^{2}-3x-28}{x}=x-7?\n\nOct 16, 2017\n\n$x = 7$\n\n#### Explanation:\n\nMultiply both sides by $x$ so you get rid of it as a denominator.\n\nThis will give you:\n${x}^{2} - 3 x - 28 = x \\left(x - 7\\right)$\n${x}^{2} - 3 x - 28 = {x}^{2} - 7 x$\n\nMove all the unknowns to one side and solve for $x$.\n${x}^{2} - {x}^{2} - 3 x + 7 x = 28$\n$\\cancel{{x}^{2}} - \\cancel{{x}^{2}} - 3 x + 7 x = 28$\n$4 x = 28$\n$\\therefore x = 7$"
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null
]
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