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https://www.bosssealing.com/rubber-tensile-strength-at-break/
[ "# Rubber tensile strength at break\n\nIn a tensile test, the maximum tensile stress of the sample until it breaks is the tensile strength, which is called tensile strength in academia, and the result is expressed in MPa.\n\nCalculation formula:\nDuring the tensile process of the sample, the material passes through the yield stage and enters the strengthening stage. After the transverse section size is significantly reduced, the maximum force (Fb) that it bears when it breaks is divided by the original cross-sectional area (So) of the sample. Stress (σ) is called tensile strength or strength limit (σb), and the unit is N/(MPa). It represents the maximum ability of a metal material to resist damage under tensile force. The calculation formula is:\nσ=Fb/So\nIn the formula: Fb–the maximum force that the sample bears when it is broken, N (Newton); So–the original cross-sectional area of the sample, mm².\n\n(1) When using the instrument to test the tensile strength of the sample, the tensile breaking stress, tensile yield stress, elongation at break and other data can be obtained together.\n(2) In the stress-strain curve, the point where the elongation will rise even if the load does not increase is usually called the yield point, the stress at this time is called the yield strength, and the deformation rate at this time is called the yield elongation; In the same way, the stress and deformation rate at the breaking point are called tensile strength at break and elongation at break, respectively.\n\nThe main factors affecting resistance are:\n1. Uncertainty of material performance\nMainly refers to the variability of material properties (such as strength, elastic modulus) in the structure or component caused by material factors, process, loading, environment, size and other factors;\n\n2. Uncertainty of component geometric parameters\nMainly refers to the variability of the geometrical dimensions of components caused by dimensional deviation and installation errors;\n\n3. Uncertainty of calculation model\n\nMainly refers to the variability caused by the basic assumptions and calculation formulas used in the calculation of resistance." ]
[ null ]
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https://nanohub.org/resources/comphe/about
[ "## Computational Helium\n\n1. Purdue University\n\nThis notebook solves the ground state for the helium atom computationally within the mean field approximation using four Gaussian functions as the basis set.\n\nYou must login before you can run this tool.\n\nVersion 1.0 - published on 07 Jul 2017\n\ndoi:10.4231/D32R3NZ97 cite this\n\n#### Abstract\n\nSummary. This notebook solves the ground state for the helium atom computationally within the mean field approximation using four Gaussian functions as the basis set. Assuming the two-electron wavefunction to be the product of two like orbitals, the two-particle Schrodinger equation reduces to single particle one but the effective Hamiltonian depends on the orbital one is trying to find (to describe electron-electron repulsion within mean field). This equation can be solved iteratively using self-consistent field (SCF) approach.\nThe initial part of the notebook go over the initial step in the SCF calculation starting from a guess wave function. All steps are described in detail. The second part performs the iterative SCF calculation until convergence is achieved.\n\n#### Cite this work\n\nResearchers should cite this work as follows:\n\n• Alejandro Strachan (2017), \"Computational Helium,\" https://nanohub.org/resources/comphe. (DOI: 10.4231/D32R3NZ97).\n\n#### Submitter\n\nMartin Hunt\n\nPurdue University" ]
[ null ]
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https://community.articulate.com/discussions/articulate-storyline/how-do-i-assign-points-to-options-for-questions-how-do-i-add-up-all-the-points
[ "# How do I assign points to options (for questions)? How do I add up all the points?\n\nHi Everyone! I'd like to build an assessment/survey with 10 questions. Each question would have 5 options (never, almost never, sometimes, fairly often, often). And, each option would be assigned a point (a.=1, b.=2, c. = 3, ...) At the end of the test, I want to add up all the points. Depending on the total points, users would get different feedback (e.g., 0-5 points show a green slide, 6-15 points show a red slide, 16-25 points show a yellow slide...) How do I start? Can I use regular test questions or am I building custom questions? I haven't used number variables but this might be the time? Let me know! Thanks.\n\n###### 5 Replies", null, "1. You need to use variables. If you don't know how, let us know and we can point you to some training webinars we've done.\n2. Assign a value to a variable when a decision is made. For example, you could have one total points variable and just keep adding to it.\n3. At the end have triggers that say, go to X if the value is between these values, got to y if the value is between these values, etc" ]
[ null, "https://api.articulate.com/id/v1/avatars/auth0|55ff0860-b37f-0131-2ee8-22000b2f96a1", null ]
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https://www.judicialwatch.org/document-archive/naomi-r-buchwald-2012/
[ "DONATE\n\nJudicial Watch • Naomi R. Buchwald – 2012\n\n# Naomi R. Buchwald – 2012", null, "Category:Federal Judges\n\nNumber of Pages:28\n\nDate Created:January 3, 2014\n\nDate Uploaded to the Library:May 22, 2014", null, "Donate now to keep these documents public!\n\nSee Generated Text   ∨\n\nAutogenerated text from PDF\n\n```Rev. 112013\nFOR CALENDAR YEAR 2012 U.S.C. app. 101-111) Person Reporting (last name, first, middle initial) Buchwald, Naomi Court Organization SOUTHERN DISTRICT NEW YORK Date Report 0510412013 Title (Article Ill judges indicate active senior status; magistrate judges indicate full-or part-time) U.S. District Judge (Senior) Sa. Report Type (check appropriate type) Nomination Date Initial Annual Sb. Amended Report Final Reporting Period 01/01/2012 12/31/2012 Chambers Office Address\nDaniel Patrick Moynihan Courthouse 500 Pearl Street --ROOM 2270 New York, 10007\n/MPO ANT NOTES: The instructions accompanying this form must followed. Complete all parts, checking the NONE box for each part where you have reportable information. POSITIONS. (Reporting individual only; see pp. 9-13 filing instructions.) NONE (No reportable positions.)\n\nNAME ORGANIZATION/ENTITY POA: Accounts 1-7\n\nII. AGREEMENTS. (Reporting individual only; see pp. 14-16 filing instructions.)\n[{] NONE (No reportable agreements.)\n\nPARTIES AND TERMS\n\nBuchwald, Naomi\n05/04/2013\nIll. 0N-INVESTMENT ME. (Reporting individual and spouse; see pp. 17-24 filing instructions.) Filer's Non-Investment Income [{] NONE (No reportable non-investment income.)\nSOURCE AND TYPE INCOME (yours, not spouse's) Spouse's Non-Investment Income -If you were married during any portion the reporting year, complete this section.\n(Dollar amount not required except for honoraria.) NONE (No reportable non-investment income.)\nSOURCE AND TYPE\n\nPartner law firm Kelley, Drye Warren LLP\n\nIV REIMBURSEMENTS -transportation, lodging, food, entertainmenL (Includes those spouse and dependent children; see pp. 25-27 filing instructions.)\n[{] NONE (No reportable reimbursements.) SOURCE DATES LOCATION PURPOSE ITEMS PAID PROVIDED\n\nBuchwald, Naomi\n05/04/2013 GIFTS. (Includes those spouse and dependent children; see pp. 28-31 filing instructions.)\nSOURCE DESCRIPTION VALUE\n\nVI. LIABILITIES. (Includes those spouse and dependent children; see pp. 32-33 filing instructions.)\n[{] NONE (No reportable liabilities.)\nCREDITOR DESCRIPTION VALUE CODE\n\nBuchwald, Naomi\n05/04/2013\nVII. INVESTMENTS and -income, value, transactions (Includes those spouse and dependent children; see PP 34-60 filing instructions.) NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period\n(including trust assets) reporting period reporting period\n\n(I) (2) (2) (3) (4) (5)\nPlace \"(X)\" after each asset\nAmount Type (e.g., Value Value Type (e.g., Date Value\nGain Identity\nexempt from prior disclosure Code (A-H) div., rent, int.) Code (J-P) Method Code (Q-W) buy, sell, redemption) mm/dd/yy Code (J-P) Code (A-H) buyer/seller (if private transaction) Citibank Accounts Interest Vanguard Voyager (IRA) Dividend Income Gain Codes: =\\$1 .000 less =\\$1.00 \\$2.500 =\\$2.501 -\\$5.000 =\\$5.001 -\\$15.000 =\\$15.001 -\\$50.000\n(Sec Columns and 04) =\\$50.001 -\\$!00.000 =\\$I 00.00 -\\$1.000.000 fl] =\\$1 .000.00 -\\$5.000.000 =More than \\$5.000.000 Value Codes =\\$1 5.000 less =\\$15.001 -\\$50.000 =\\$50.001 -\\$I 00.000 I00.00 -\\$250.000\n(See Columns and 03) =\\$250.001 -\\$500.000 =\\$500.00 -\\$1.000.000 =\\$1.000.001 -\\$5.000.000 =\\$5.000.00 -\\$25.000.000 =\\$25.000.001 -\\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(See Column C2) =Book Value V=Othcr =Estimated\n\nVII. INVESTMENTS and TRUSTS -income, value, transactions r1nc1udes those spouse and dependent children; see PP 34-60 filing instructions.) NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period\n(including trust assets) reporting period ofreporting period\n\n(I) (I) (2) (I) (4) Income Gain Codes: 41.000 less =\\$1.001 -\\$2.500 c=\\$2.501 -\\$5.000 0=\\$5.001 -\\$15.000 E=\\$15.00 -\\$50.000\n(Sec Columns and 04) F=\\$50.001 -\\$100.000 =\\$!00.001 -\\$1.000.000 =\\$1.000.001 -\\$5.000.000 112 =More than \\$5.000.000 Value Codes J=\\$15.000 less K=\\$15.001 -\\$50.000 =\\$50.00I -\\$I 00.000 =\\$100.001 -\\$250,000\n{Sec Columns and D3) =\\$250.001 -\\$500.000 0=\\$500.00I -\\$1.000.000 =\\$1.000.001 -\\$5.000.000 =\\$5.000.001 -\\$25.000.000 =\\$25.000.001 -\\$50.000.000 P4=More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment T=Cash Market\n(Sec Column C2) U=Book Value =Other =Estimated\n\nBuchwald, Naomi\n05/04/2013\nVII. INVESTMENTS and TRUSTS -income, value, transactions r1nc1udes those spouse and dependent children; see PP 34-60 instructions.; NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period\n(including trust assets) reporting period ofreporting period\nPlace \"(X)\" after each asset exempt from prior disclosure (I) Amount Code (2) Type (e.g., div., rent, (I) Value Code (2) Value Method (I) Type (e.g., buy, sell, (2) Date mm/dd/yy (3) Value Code (4) Gain Code (5) Identity buyer/seller\n(A-H) int.) (J-P) Code redemption) (J-P) (A-H) (if private\n(Q-W) transaction)\nSold 12/6/12\n36.\n--International Rectifier (Common)\n\nNone Sold 917112\n37.\n\n--Amazon (Common) None Buy 01/3/12 Income Gain Codes: .000 less =\\$1.001 -\\$2.500 =\\$2.501 -\\$5.000 D=\\$5,00I -\\$15.000 =\\$15.001 -\\$50.000\n(Sec Columns and D4) =\\$50.00 -\\$I 00.000 =\\$I 00.00 -\\$1 .000.000 =\\$1 .000 .001 -\\$5.000.000 =More than \\$5.000.000 Value Codes =\\$1 5.000 Jess =\\$15.001 -\\$50.000 =\\$50.00 J00.000 =\\$I 00.00 -\\$250.000\n(Sec Columns and D3) =\\$250.00 -\\$500.000 =\\$500.00 -\\$1 .000.000 =\\$1.000.001 -\\$5.000.000 =\\$5.000.001 -\\$25.000.000 =\\$25.000.001 -\\$50,000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(Sec Column C2) =Book Value V=Othcr =Estimated\n\nBuchwald, Naomi\n05/04/2013\nVII. INVESTMENTS and TRUSTS -income, vatue, transactions r1nctudes those spouse and dependent children; see PP 34-60 filing instructions.) NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period (including trust assets) reporting period reporting period\n(2) (2) (3) (4) (5) Place \"(X)\" after each asset Amount Type (e.g., Value Value Type (e.g., Date Value Gain Identity\nexempt from prior disclosure Code (A-H) div., rent, int.) Code (J-P) Method Code (Q-W) buy, sell, redemption) mm/dd/yy Code (J-P) Code (A-H) buyer/seller (if private transaction)\n52. Sold 11/15/12\n\n--Valero (Common) Dividend\nSold 2/8/12\n55.\nBuy 3/3/12 Income Gain Codes: =\\$1.000 less =\\$1,001 -\\$2.500 =\\$2.501 -\\$5,000 0=\\$5.001 -\\$1 5.000 =\\$15.001 -\\$50.000\n(Sec Columns and 04) =\\$50.00 -\\$I 00.000 100.00 -\\$1.000.000 =\\$1 .000.001 -\\$5.000.000 =More than \\$5.000.000 Value Codes =\\$1 5.000 less K=\\$15.00I \\$50.000 =\\$50.001 -\\$100.000 100.00 -\\$250.000\n(See Columns and 03) =\\$250.001 -\\$500.000 =\\$500,00I -\\$1.000.000 Pl =\\$1,000.001 -\\$5,000.000 =\\$5.000.001 -\\$25.000.000 =\\$25.000.001 -\\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(See Column C2) =Book Value V=Other =Estimated\n\nBuchwald, Naomi\n05/04/2013\nVII. INVESTMENTS and TRUSTS -income, value, transactions r1nc1udes those spouse and dependent children; see PP 34-60 filing instructions.J NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end\n(including trust assets) reporting period ofreporting period\n\nTransactions during reporting period\n(I) (I)\n(2) (I) (2) (3) (4) (5)\nPlace \"(X)\" after each asset exempt from prior disclosure Amount Code (A-H) Type (e.g., div., rent, int.) Value Code (J-P) Value Method Code (Q-W) Type (e.g., buy, sell, redemption) Date mm/dd/yy Value Code (J-P) Gain Code (A-H) Identity buyer/seller (if private transaction)\n\nSold 08/6/12\n71.\nBuy 0817/12 Income Gain Codes: =\\$1 .000 less 41.001 -\\$2.500 =\\$2.501 -\\$5.000 0=\\$5.001 -\\$15.000 E=\\$1 5.001 -\\$50.000\n(Sec Columns and 04) F=\\$50.00l -\\$100.000 =\\$I 00.00 -\\$1.000.000 =\\$1.000.001 -\\$5.000.000 112 =More than \\$5.000.000 Value Codes =\\$15.000 less =\\$15,001 -\\$50.000 =\\$50.001 -\\$100.000 =\\$!00.001 -\\$250.000\n(Sec Columns and 03) =\\$250.001 -\\$500.000 =\\$500,00 -\\$1.000.000 =\\$1.000.001 -\\$5,000.000 =\\$5.000.001 -\\$25.000.000 =\\$25.000.001 -\\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(Sec Column C2) =Book Value V=Other =Estimated\n\nVII. INVESTMENTS and TRUSTS -income, value, transactions (lnc/11des those spouse and dependent children; see PP 34-60 filing instructions.) NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period\n(including trust assets) reporting period reporting period\n\n(I) (I) (I) (3) (4) (5)\nPlace \"(X)\" after each asset exempt from prior disclosure Amount Code (A-H) Type (e.g., div., rent, int.) Value Code (J-P) Value Method Code (Q-W) Type (e.g., buy, sell, redemption) Date mm/dd/yy Value Code (J-P) Gain Code (A-H) Identity buyer/seller (if private transaction)\n87. Sold 2/29/12\n\n90.\n91.\n92.\n93. Sold 1111 5/12\n\n--M icrosoft (Common) Dividend Buy 3/20/12\nSold 8/17/12 (part)\nSold 8/26/12 (part)\n99.\nSold 8/27/12\n\n100.\n--Research Motion (Common) None Buy 09115112\n\nIOI. Sold 12/16/12\n102. JPMorgan Chase Accounts Interest Income Gain Codes: =\\$1.000 less =\\$1.001 -\\$2.500\n(See Colmnns and 04) =\\$50.00 -\\$100.000 =\\$100.00 I.000.000 Value Codes =\\$1 5.000 less =\\$15.001 -\\$50.000\n(See Columns and 03) =\\$250.00 -\\$500.000 =\\$500.00 I.000.000 =\\$25.000.00! -\\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only)\n(Sec Column C2) =Book Value V=Othcr =\\$2.501 -\\$5.000 Ill =\\$!.000.001 -\\$5.000.000 =\\$50.00 -\\$100.000 =\\$1.000.001 -\\$5.000.000 =More than \\$50.000.000 =Assessment =Estimated 0=\\$5.001-\\$1 5.000 =More than \\$5.000.000 =\\$100.00 -\\$250.000 =\\$5.000.001 -\\$25.000.000 =Cash Market =\\$15.001 -\\$50.000\n\nBuchwald, Naomi\n0510412013\nVII. INVESTMENTS and TRUSTS -income, value, transactions r1nc1udes those spouse and dependent children; see PP 14-60 filing instructions.) NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period (including trust assets) reporting period reporting period\n(2) (2) (I) (2) (4)\n\nPlace \"{X)\" after each asset exempt from prior disclosure Amount Code (A-H) Type (e.g., div., rent, int.) Value Code2 (J-P) Value Method Code (Q-W) Type (e.g., buy, sell, redemption) Date mm/dd/yy Value Code (J-P) Gain Code (A-H) Identity buyer/seller (if private transaction)\n!03. Schwab Account --NY Muni Money Mkt Int./Div.\n104. 105. Merrill Lynch Cash Ace-formerly America cash reserve Treasury Direct Dividend Interest 06. Time Warner Common Stock Dividend Buy 7/13/12\n107. 108. Sold (part) Buy 7/17/I2 9126112\n109. IO. Applied Materials mmon Stock (IRA) Dividend Sold (part) Buy I/20/I2 1112 Sold 8/16/12 I2. Blount Common Stock None\n113. Intel mmon Stock (IRA) Dividend Buy 01/17/12 Buy 01/18/12 Sold 01/18/12\n118. Sold 3/2/12 Buy 3/5/12 Income Gain Codes: =\\$1.000 less =\\$1 .001 -\\$2.500 =\\$2.501 -\\$5.000 0=\\$5.001 -\\$15.000 =\\$15.001 -\\$50.000\n(Sec Columns and 04) F=\\$50,00l -\\$100.000 =\\$I 00.00 -\\$1.000.000 =\\$1.000.001 -\\$5.000.000 =More than \\$5.000.000 Value Codes J=\\$15.000 lcss =\\$15,001 -\\$50.000 =\\$50.00 -\\$I 00.000 100.00 -\\$250.000\n(Sec Columns and 03) =\\$250.00 -\\$500.000 =\\$500.00 -\\$I .000.000 =\\$1.000.001 -\\$5.000.000 =\\$5.000.001 -\\$25.000.000 =\\$25.000.001 -\\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(Sec Column C2) =Book Value V=Othcr =Estimated\n\nBuchwald, Naomi\n05/04/2013\nVII. INVESTMENTS and TRUSTS -income, vatue, transactions r1nc1udes those spouse and dependent children; see PP 34-60 filing instmctions.J NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period (including trust assets) reporting period ofreporting period\n\n(2) (l) (2) (3) (4) (5) Place \"(X)\" after each asset\nAmount Type (e.g., Value Value Type (e.g., Date Value Gain Identity exempt from prior disclosure\n(A-H) int.) (J-P) \tCode redemption) (J-P) (A-H) (if private (Q-W) transaction)\n120.\n121.\nSold 3/9/12 (part) Income Gain Codes: =\\$1.000 less =\\$1 .00 -\\$2.500 =\\$2.501 -\\$5.000 =\\$5.001 -\\$15.000 =\\$15.00 -\\$50,000\n(Sec Colunms and 04) =\\$50.00I -\\$I 00.000 =\\$100,001 -\\$1.000.000 =\\$1.000.001 -\\$5.000.000 112 =More than \\$5.000.000 Value Codes J=\\$15.000 less K=\\$15.00l -\\$50.000 =\\$50.00I -\\$I 00.000 I00.00 -\\$250.000\n(Sec Columns and D3) =\\$250,00 -\\$500.000 =\\$500,00 -\\$1.000.000 =\\$1 .000.001 -\\$5.000.000 =\\$5.000.001 -\\$25,000.000 =\\$25.000.00 -\\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(See Column C2) =Book Value V=Othcr =Estimated\n\nBuchwald, Naomi\n05/04/2013\n\nVII. INVESTMENTS and -income, value, transactions (Includes those spouse and dependent children; see PP 34-60 filing instructions.) NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period\n(including trust assets) reporting period reporting period\n\n(I) (2) (I) (I) (3) (4) (5)\nPlace \"(X)\" after each asset exempt from prior disclosure Amount Code (A-H) Type (e.g., div., rent, int.) Value Code (J-P) Value Method Code (Q-W) Type (e.g., buy, sell, redemption) Date mm/dd/yy Value Code (J-P) Gain Code (A-H) Identity buyer/seller (if private transaction)\n137. Buy 5/2/12 Income Gain Codes: 41,000 less =\\$1 ,001 -\\$2.500 =\\$2.501 -\\$5.000 0=\\$5,001 -\\$15.000 =\\$15.00I -\\$50.000\n(Sec Columns and 04) =\\$50.001 -\\$100.000 =\\$100.001 -\\$1.000.000 =\\$1.000.001 -\\$5.000.000 =More than \\$5.000.000 Value Codes =\\$15.000 less =\\$15.001 -\\$50.000 =\\$50.001 -\\$1 00.000 =\\$100.001 -\\$250.000\n(Sec Columns and 03) =\\$250.001 -\\$500.000 =\\$500.001 -\\$1 .000.000 =\\$1 .000.001 -\\$5,000.000 =\\$5.000.001 -\\$25.000.000 =\\$25.000.001 -\\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(Sec Column C2) =Book Value V=Othcr =Estimated\n\nBuchwald, Naomi\n05/04/20\nVII. INVESTMENTS and TRUSTS -income, value, transactions r1nc1udes those spouse and dependent children; see pp. 34-60 filing instructions.) NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period (including trust assets) reporting period reporting period\n\n(2) (I) (2) (I) (2) (3) (4) (5)\nPlace \"(X)\" after each asset Amount Type (e.g., Value Value Type (e.g., Date Value Gain Identity\nexempt from prior disclosure Code div., rent, Code Method buy, sell, mm/dd/yy Code Code buyer/seller\n(A-H) int.) (J-P) Code redemption) (J-P) (A-H) (if private\n\ntransaction)\n154.\nSold 3/26/12\n\n155.\n\n156.\nSold 04/18/12 (part)\n\n157.\nSold 4/19/12 (part) Income Gain Codes: 41.000 less ,001 -\\$2,500 =\\$2.501 -\\$5.000 =\\$5.001 -\\$15.000 =\\$15.00 -\\$50.000\n(Sec Columns and D4) F=\\$50.00l -\\$100.000 =\\$100.00 -\\$1 .000.000 =\\$1.000.001 -\\$5.000.000 =More than \\$5.000.000 Value Codes =\\$15.000 less K=\\$15,00l -\\$50.000 =\\$50.001 100.000 =\\$100.001 -\\$250.000\n(Sec Columns and 03) =\\$250.00 -\\$500.000 =\\$500.00 -\\$1 .000.000 =\\$1.000.001 -\\$5,000.000 =\\$5.000.001 -\\$25,000.000 =\\$25.000.001 -\\$50.000.000 =More than \\$50.000.000 Value Method Coctcs =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(Sec Column C2) =Book Value V=Othcr =Estimated\n\nBuchwald, Naomi\n05/04/2013\n\nVII. INVESTMENTS and TRUSTS -income, value, transactions r1nc1udes those spouse and dependent children; see PP 34-60 offiling instructions.) NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period\n(including trust assets) reporting period reporting period\n\n(2) (I) (2) (3) (4)\nPlace \"(X)\" after each asset Amount Type (e.g., Value Value Type (e.g., Date Value Gain Identity\nexempt from prior disclosure Code div., rent, Code Method buy, sell, mm/dd/yy Code Code buyer/seller\n(A-H) int.) (J-P) Code redemption) (J-P) (A-H) (if private\n\ntransaction)\n171.\n172.\nSold 3/8/12\n173.\n\n174.\nSold 3/14/12\n\n175.\n\n176.\n\n178. 179. Sold (part) Buy 3/26/12 3/29/12\n180. Sold (part) 4/3/12\n181. Sold (part) 4/12/12\n182. 183. 184. Sold (part) Sold (part) Sold (part) 4/18/12 4/24/12 4/25/\n185. Sold 4/30/12\n187. Buy 5/2/12 Income Gain Codes: =\\$1 .000 less =\\$1.00 -\\$2.500 =\\$2.501 -\\$5.000 D45.00t 15.000 =\\$15.001 -\\$50.000\n(See Columns and D4) =\\$50.00 -\\$I 00.000 =\\$100.001 -\\$1 .000.000 =\\$1 .000.001 -\\$5.000.000 112 =More than \\$5.000.000 Value Codes =\\$15.000 less =\\$15.001 -\\$50.000 =\\$50.00 -\\$1 00.000 =\\$100.00 -\\$250.000\n(See Columns and DJ) =\\$250.00 -\\$500.000 =\\$500.00 -\\$1 .000.000 =\\$1.000.001 -\\$5.000.000 =\\$5.000.001 -\\$25.000.000 =\\$25.000.001 -\\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(Sec Column C2) =Book Value V=Othcr =Estimated\n\nBuchwald, Naomi\n05/04/2013\n\nVII. INVESTMENTS and TRUSTS --income, vatue, transactions r1nc1udes those spouse and dependent children; see PP 34-60 offiting instructions.J NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period\n(including trust assets) reporting period reporting period\n\n(1) (2)\n(2) (3) (4) (5)\nPlace \"(X)\" after each asset exempt from prior disclosure Amount Code (A-H) Type (e.g., div., rent, int.) Value Code (J-P) Value Method Code (Q-W) Type (e.g., buy, sell, redemption) Date mm/dd/yy Value Code (J-P) Gain Code (A-H) Identity buyer/seller (if private transaction)\n188. Buy 515112 Income Gain Codes: =\\$1.000 less 41.001 -\\$2.500 c=\\$2.501 -\\$5.000 045,001 -\\$15.000 =\\$15,001 -\\$50,000\n(See Columns and 04) =\\$50.001 -\\$1 00.000 =\\$100.00 -\\$1 .000.000 Ill =\\$1.000.001 -\\$5.000.000 112 =More than \\$5.000.000 Value Codes J=\\$1 5.000 less =\\$1 5.001 -\\$50.000 L=\\$50.00 -\\$100.000 I00.00 -\\$250.000\n(See Columns and DJ) N=\\$250.001 -\\$500.000 0=\\$500.00 -\\$1.000.000 =\\$1 .000.001 -\\$5.000.000 =\\$5.000.001 -\\$25,000.000 =\\$25.000.001 -\\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment T=Cash Market\n(Sec Column C2) U=Book Value V=Othcr W=Estimated\n\nBuchwald, Naomi\n05/04/2013\nVII. INVESTMENTS and TRUSTS -income, vatue, transactions r1nc1udes those spouse and dependent children; see PP 34-60 filing instructions.) NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period (including trust assets) reporting period ofreporting period\n(I) (2) (I) (2) (I) (2) (3) (4) (5) Place \"(X)\" after each asset\nAmount Type (e.g., Value Value Type (e.g., Date Value Gain Identity exempt from prior disclosure\nCode\n(A-H) int.) (J-P) \tCode redemption) (J-P) (A-H) (if private (Q-W) transaction)\n205.\nSold 7112112 (part)\n206.\n207.\nSold Jncomc Gain Codes: =\\$1.000 less 641.001 -\\$2.500 =\\$2.501 \\$5.000 D=\\$5.001 \\$15.000 =\\$15.001 -\\$50.000\n(See Columns and 04) F=\\$50.001 -\\$1 00.000 =\\$I 00.00 -\\$1 .000.000 =\\$1 .000.001 \\$5.000.000 fl2 =More than \\$5.000.000 Value Codes J=\\$15.000 less =\\$15.001 -\\$50.000 L=\\$50.00 \\$100.000 =\\$100.00 -\\$250.000\n(Sec Columns and D3) =\\$250.001 -\\$500.000 =\\$500.00 .000.000 =\\$1.000.00 -\\$5.000.000 =\\$5.000.001 \\$25.000.000 =\\$25.000.001 \\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(Sec Column C2) =Book Value V=Othcr W=Estimated\n\nBuchwald, Naomi\n05/04/2013\nVII. INVESTMENTS and TRUSTS -income, value, transactions r1nc1udes those spouse and dependent children; see PP 34-60 offilinc instructions.J NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period\n(including trust assets) reporting period reporting period\n\n(I) (2) (l) (l) (3) (4)\nPlace \"(X)\" after each asset exempt from prior disclosure Amount Code (A-H) Type (e.g., div., rent, int.) Value Code (J-P) Value Method Code (Q-W) Type (e.g., buy, sell, redemption) Date mm/dd/yy Value Code (J-P) Gain Code (A-H) Identity buyer/seller (if private transaction)\n222. Sold (part) 12112\n\n223.\nBuy 1117/12 Income Gain Codes: I.000 less =\\$1,001 -\\$2.500 c=\\$2.501 -\\$5.000 D=\\$5.001 -\\$15.000 =\\$15.001 -\\$50.000 (Sec Columns and 04) =\\$50.00 -\\$I 00.000 =\\$100.001 -\\$1.000.000 =\\$1.000.001-\\$5.000.000 fl2 =More than \\$5.000.000\nValue Codes J=\\$15.000 less K=\\$15.00l -\\$50.000 L=\\$50.00 -\\$I 00.000 =\\$100.00 -\\$250.000\n\n(Sec Columns and 03) \tN=\\$250.001 -\\$500.000 0=\\$500.00 -\\$1.000.000 =\\$1.000.001 -\\$5.000.000 P2=\\$5.000.00 -\\$25.000.000 =\\$25.000.001 -\\$50.000.000 =More than \\$50.000.000\nValue Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market (Sec Colunm C2) =Book Value =Other W=Estimated\n\nBuchwald, Naomi\n0510412013\nVII. INVESTMENTS and TRUSTS -income, vatue, transactions r1nc1udes those spouse and dependent children; see pp. 34-60 filing instructions.) NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period (including trust assets) reporting period ofreporting period\n(2) (I) (2) (2) (3) (4)\nPlace \"(X)\" after each asset\nAmount Type (e.g., Value Value Type (e.g., Date Value Gain Identity\nCode\nexempt from prior disclosure\n(A-H) int.) Code redemption) (J-P) (A-H) (if private (Q-W) transaction) Jncomc Gain Codes: =\\$1.000 less =\\$1 .00 -\\$2.500 =\\$2.501 -\\$5.000 D=\\$5.001 -\\$15.000 =\\$15.00 -\\$50.000\n(See Columns and 04) =\\$50.00 -\\$I 00.000 =\\$I 00.00 -\\$1 .000.000 =\\$1.000.001 -\\$5.000.000 =More than \\$5,000.000 Value Codes J=\\$1 5,000 less =\\$15,001 -\\$50.000 =\\$50.00I -\\$I 00.000 =\\$100.001 -\\$250,000\n(See Columns and 03) =\\$250.001 -\\$500.000 0=\\$500.001 -\\$1 .000.000 =\\$1.000.001 -\\$5.000.000 =\\$5.000.001 -\\$25.000.000 =\\$25.000.001 -\\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(Sec Column C2) U=Book Value V=Othcr W=Estimated\n\nBuchwald, Naomi\n05/04/20\nVII. INVESTMENTS and TRUSTS -income, vatue, transactions r1nc1udes those spouse and dependent children; see PP 34-60 filing instructions.; NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period\n(including trust assets) reporting period reporting period\n\n(I) (I) (2) (2) (3) (4) (5)\nPlace \"(X)\" after each asset Amount Type (e.g., Value Value Type (e.g., Date Value Gain Identity\nexempt from prior disclosure Code div., rent, Code Method buy, sell, mm/dd/yy Code Code buyer/seller\n(A-H) int.) (J-P) Code redemption) (J-P) (A-H) (if private\n\ntransaction)\n256.\n257.\n\nSold 10/15/12\n258.\nBuy 1117/12 Income Gain Codes: A=\\$1,000or lcss =\\$1 ,00 -\\$2,500 =\\$2.501 -\\$5,000 =\\$5.001 -\\$1 5,000 =\\$15.001 -\\$50.000\n(Sec Columns and 04) =\\$50,001 -\\$100.000 I00,00 -\\$1 ,000.000 =\\$1.000.001 -\\$5.000.000 =More than \\$5.000.000 Value Codes =\\$15.000 less =\\$15.001 -\\$50.000 =\\$50.00 -\\$I 00.000 I00.00 -\\$250.000\n(See Columns and 03) =\\$250.001 -\\$500.000 0=\\$500,00 -\\$1.000.000 =\\$1.000.001 -\\$5,000.000 =\\$5.000.00 -\\$25,000.000 =\\$25.000.001 -\\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(Sec Column C2) =Book Value V=Othcr =Estimated\n\nBuchwald, Naomi\n05/04/2013\nVII. INVESTMENTS and TRUSTS -income, value, transactions r1nc1udes those spouse and dependent children; see PP 34-60 filing instructions.) NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period\n(including trust assets) reporting period ofreporting period\n\n(1) (2) (1) (2)\n(2) (4) (5)\nPlace \"(X)\" after each asset Amount Type (e.g., Value Value Type (e.g., Date Value Gain Identity\nexempt from prior disclosure Code div., rent, Code Method buy, sell, mm/dd/yy Code Code buyer/seller\n(A-H) int.) (J-P) Code redemption) (J-P) (A-H) (if private\n\ntransaction)\n273. Sold 2/28/12 Income Gain Codes: =\\$1.000 less =\\$1 ,00 -\\$2,500 =\\$2.501 -\\$5.000 0=\\$5.001 -\\$1 5.000 =\\$1 5.00 -\\$50.000\n(See Columns and 04) F=\\$50,001 -\\$100.000 =\\$I 00.00 -\\$1 .000.000 =\\$1 .000.001 -\\$5.000.000 ll2 =More than \\$5.000.000 Value Codes =\\$15,000 less =\\$15,001 -\\$50.000 =\\$50.00 100.000 100.00 -\\$250.000\n(Sec Columns and D3) =\\$250.001 -\\$500.000 0=\\$500.001 1,000.000 =\\$1,000.001 -\\$5.000.000 =\\$5.000.001 -\\$25,000.000 =\\$25.000.001 -\\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) \"\"Assessment ==Cash Market\n(See Column C2) =Book Value =Other =Estimated\n\nBuchwald, Naomi\n05/04/2013\nVII. INVESTMENTS and TRUSTS -income, value, transactions r1nc1udes those spouse and dependent children; see PP 34-60 filing instructions.; NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end\n(including trust assets) reporting period reporting period\n\nTransactions during reporting period\n(I) (2) (2) (I) (2) (4) (5)\nPlace \"(X)\" after each asset\nAmount Type (e.g., Value Value Type (e.g., Date Value Gain Identity\nCode\nexempt from prior disclosure\n(A-H) int.)\nCode redemption) (J-P) (A-H) (if private\ntransaction) Income Gain Codes: =\\$1.000 lcss =\\$1,001 -\\$2.500 =\\$2.501 -\\$5.000 =\\$5.001 -\\$15,000 =\\$15.001 -\\$50.000\n(See Columns and D4) 450.001 -\\$100.000 =\\$1 00.001 -\\$1 .000.000 Ill =\\$1 .000.001 -\\$5.000.000 =More than \\$5.000.000 Value Codes =\\$15.000 less K=\\$1 5,00I -\\$50.000 =\\$50.00 -\\$I 00.000 =\\$100.00 -\\$250.000\n(See Columns and D3) =\\$250.00 -\\$500.000 =\\$500.00 -\\$1 .000.000 =\\$1.000.001 -\\$5.000.000 =\\$5.000.001 -\\$25.000.000 =\\$25.000.001 -\\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(See Column C2) =Book Value V=Othcr =Estimated\n\nBuchwald, Naomi\n05/04/2013\nVII. INVESTMENTS and TRUSTS -income, value, transactions r1nc1udes those spouse and dependent children; see PP 34-60 filing instructions.J NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period (including trust assets) reporting period ofreporting period\n(2) (2) (4) (5)\nPlace \"(X)\" after each asset exempt from prior disclosure Amount Code (A-H) Type (e.g., div., rent, int.) Value Code (J-P) Value Method Code (Q-W) Type (e.g., buy, sell, redemption) Date mm/dd/yy Value Code (J-P) Gain Code (A-H) Identity buyer/seller (if private transaction)\n308. Buy 4/8/12 Income Gain Codes: =\\$1 .000 less =\\$1.001 -\\$2.500 =\\$2.501 -\\$5,000 =\\$5.001 -\\$15.000 =\\$15.001 -\\$50.000\n(Sec Columns and 04) =\\$50.001 -\\$100.000 =\\$100.00 -\\$1.000.000 =\\$1 .000.001 -\\$5.000.000 =More than \\$5.000.000 Value Codes =\\$1 5.000 less =\\$15.001 -\\$50,000 =\\$50.001 -\\$100.000 I00.00 -\\$250.000\n(Sec Columns and 03) =\\$250.001 -\\$500.000 =\\$500.00 -\\$1 .000.000 =\\$1.000.001 -\\$5,000.000 =\\$5.000.001 -\\$25.000.000\n1'3 =\\$25.000.00 -\\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(Sec Column C2) =Book Value V=Othcr =Estimated\n\nVII. INVESTMENTS and TRUSTS -income, vatue, transactions r1nc1udes those ofspo11se and dependent children; see pp. 34-60 filing instr11c1ions.J NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period\n{including trust assets) reporting period reporting period\n\n(I) (2) (I) (2) (I) (2) (4) (5)\nPlace \"(X)\" after each asset\nAmount Type (e.g., Value Value Type (e.g., Date Value Gain Identity\nCode\nexempt from prior disclosure\ndiv., rent, Code Method buy, sell, mm/dd/yy Code Code buyer/seller Jncomc Gain Codes: =\\$1.000 Jess =\\$1,00 -\\$2.500 =\\$2.501 -\\$5.000 =\\$5.001 -\\$15.000 =\\$15,001 -\\$50.000\n(Sec Columns and 04) F=\\$50.001 -\\$100.000 =\\$I 00.00 -\\$1 .000.000 Ill =\\$1.000.001 -\\$5.000.000 =More than \\$5.000.000 Value Codes =\\$15.000 less =\\$15.001 -\\$50.000 =\\$50.001 -\\$1 00.000 I00.00 -\\$250.000\n(See Columns and 03) =\\$250.00 -\\$500.000 0=\\$500,001 -\\$1.000.000 =\\$1.000.001 -\\$5.000.000 =\\$5.000.001 -\\$25,000.000 =\\$25.000.001 -\\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(Sec Column C2) =Book Value V=Other =Estimated\n\nBuchwald, Naomi\n05/04/2013\nVII. INVESTMENTS and TRUSTS -income, value, transactions (Includes those spouse and dependent children; see PP 34-60 filing instructions.) NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end\n(including trust assets) reporting period reporting period\n\nTransactions during reporting period\n(I) (2)\n(I)\n(2) (3) (5)\nPlace \"(X)\" after each asset\nAmount Type (e.g., Value Value Type (e.g., Date Value Gain Identity\nCode\nexempt from prior disclosure\n(A-H) int.) Code redemption) (J-P) (A-H) (if private (Q-W) transaction)\n341.\n\nSold 8/24/12\n342.\nTime Warner Cable Common Dividend Buy 7/13/12 Income Gain Codes: =\\$1 ,000 Jess =\\$1,001 -\\$2.500 =\\$2.501 -\\$5.000 =\\$5.001 -\\$15.000 =\\$15.001 -\\$50.000\n(See Columns and 04) F=\\$50.00I -\\$1 00.000 =\\$100.001 -\\$1.000.000 =\\$1 .000.001 -\\$5.000.000 =More lhan \\$5.000.000 Value Codes =\\$15.000 less =\\$15.001 -\\$50.000 =\\$50.001 -\\$100.000 =\\$100.001 -\\$250,000\n(Sec Columns and 03) =\\$250.00 -\\$500.000 =\\$500.00 -\\$1.000.000 =\\$1.000.001 -\\$5.000.000 =\\$5.000.001 -\\$25.000.000 =\\$25.000.001 -\\$50.000.000 =More 1han \\$50.000.000 Value Method Codes =Appraisal =Cos1 (Real Es1a1c Only) =Assessment =Cash Market\n(Sec Column C2) =Book Value V=01hcr =Estimated\n\n.VII. INVESTMENTS and TRUSTS -income, value, transactions r1nc1udes those spouse and dependent chitdren; see PP 34-60 offiting instructions.) NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end Transactions during reporting period\n(including trust assets) reporting period reporting period\n\n(I) (I) (2) (3) (4) (5)\nPlace \"(X)\" after each asset Amount Type (e.g., Value Value Type (e.g., Date Value Gain Identity\nexempt from prior disclosure Code div., rent, Code Method buy, sell, mm/dd/yy Code Code buyer/seller\n(A-H) int.) (J-P) Code redemption) (J-P) (A-H) (if private\n\ntransaction) Income Gain Codes: A=\\$1.000or less =\\$1,001 -\\$2,500 c=\\$2.501 -\\$5.000 =\\$5.001 -\\$15.000\n(Sec Columns and 04) F=\\$50.00l -\\$100.000 =\\$100.001 -\\$1 .000.000 =\\$1 .000.001 -\\$5.000.000 =More than \\$5.000.000 Value Codes J=\\$1 5.000 lcss K=SIS,001 -\\$50.000 L=\\$50.00 -\\$I 00.000 =\\$100.00 -\\$250.000\n(Sec Columns and 03) N=\\$250.00 -\\$500.000 0=\\$500.00 \\$1.000.000 =Sl.000.001 -\\$5.000.000 =\\$5.000.001 -\\$25,000.000 =\\$25.000.001 \\$50.000.000 =More than \\$50.000.000 Value Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(Sec Column C2) U=Book Value V=Othcr W=Estimated =\\$15.001 -\\$50.000\n\nBuchwald, Naomi\n05/04/2013\nVII. INVESTMENTS and TRUSTS -income, value, transactions r1nc111des those spouse and dependent children; see PP 34-60 filing instructions.J NONE (No reportable income, assets, transactions.)\nDescription Assets Income during Gross value end\nTransactions during reporting period\n(including trust assets) reporting period reporting period\n(I) (2) (I) (2) (I) (2) (4) (5)\nPlace \"(X)\" after each asset\nAmount Type (e.g., Value Value Type (e.g., Date Value Gain Identity\nCode\nexempt from prior disclosure\n(A-H) int.)\nCode redemption) (J-P) (A-H) (if private (Q-W) transaction)\n375.\n\n376.\n-JP Morgan Mid Cap Value Fund\n\n377.\n-Growth Fund America\n\n378.\n-Invesco Van Kampen Senior. Loan Fund\n\n-Touchtone Mid Cap Growth Fund\n380.\n-Escrow Leiner Health Products exchanged for Lehman\n\n381.\n-Express Scripts Holding Co. Common Stock (X) Income Gain Codes: =\\$1.000 less =\\$1.001 -\\$2.500 =\\$2.501 -\\$5.000 0=\\$5.001 \\$15.000 E=\\$15.00I -\\$50,000 (Se Columns and 04) =\\$50.001 -\\$100.000 =\\$100.00I -\\$1.000.000 =\\$1 .000.001 \\$5.000.000 112 =More than \\$5.000.000\nValue Codes =\\$15.000 less =\\$15.001 \\$50.000 =\\$50.00 I00.000 =\\$100.001 -\\$250.000\n\n(Sec Columns and D3) =\\$250.00 -\\$500.000 =\\$500,00 -\\$1,000.000 =\\$1,000.001 \\$5.000.000 =\\$5.000.001 -\\$25.000.000 =\\$25.000.001 -\\$50.000.000 =More than \\$50.000.000\nValue Method Codes =Appraisal =Cost (Real Estate Only) =Assessment =Cash Market\n(See Column C2) =Book Value V=Othcr =Estimated\n\nName Person Reporting\nDate Report\nBuchwald, Naomi\n05/04/2013\n\nVIII. ADDITIONAL INFORMATION EXPLANATIONS. (lndicate part ofreport.)\n\n05104120\nBuchwald, Naomi\nIX. CERTIFICATION. certify that all information given above (including information pertaining spouse and minor dependent children, any) accurate, true, and complete the best knowledge and belief, and that any information not reported was withheld because met applicable statutory provisions permitting non-disclosure. further certify that earned income from outside employment and honoraria and the acceptance gifts which have been reported are compliance with the provisions U.S.C. app. 501 et. seq., U.S.C. 7353, and Judicial Conference regulations.\nSignature: Naomi Buchwald\n\nNOTE: ANY INDIVIDUAL WHO KNOWINGLY AND WILLFULLY FALSIFIES FAILS FILE THIS REPORT MAY SUBJECT CIVIL AND CRIMINAL SANCTIONS U.S.C. app. 104)\n\nCommittee Financial Disclosure Administrative Office the United States Courts Suite 2-301 One Columbus Circle, N.E. Washington, D.C. 20544```\n\nWWW.JUDICIALWATCH.ORG\n\nJudicial Watch is a 501(c)(3) nonprofit organization. Contributions are received from individuals, foundations, and corporations and are tax-deductible to the extent allowed by law.\n\n425 Third Street SW, Suite 800\nWashington, DC 20024\n888-593-8442" ]
[ null, "https://www.judicialwatch.org/wp-content/uploads/2014/05/Naomi_R_Buchwald-2012.jpg", null, "https://www.judicialwatch.org/t/images/da/security-checked.png", null ]
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https://www.colorhexa.com/00e02e
[ "# #00e02e Color Information\n\nIn a RGB color space, hex #00e02e is composed of 0% red, 87.8% green and 18% blue. Whereas in a CMYK color space, it is composed of 100% cyan, 0% magenta, 79.5% yellow and 12.2% black. It has a hue angle of 132.3 degrees, a saturation of 100% and a lightness of 43.9%. #00e02e color hex could be obtained by blending #00ff5c with #00c100. Closest websafe color is: #00cc33.\n\n• R 0\n• G 88\n• B 18\nRGB color chart\n• C 100\n• M 0\n• Y 79\n• K 12\nCMYK color chart\n\n#00e02e color description : Pure (or mostly pure) lime green.\n\n# #00e02e Color Conversion\n\nThe hexadecimal color #00e02e has RGB values of R:0, G:224, B:46 and CMYK values of C:1, M:0, Y:0.79, K:0.12. Its decimal value is 57390.\n\nHex triplet RGB Decimal 00e02e `#00e02e` 0, 224, 46 `rgb(0,224,46)` 0, 87.8, 18 `rgb(0%,87.8%,18%)` 100, 0, 79, 12 132.3°, 100, 43.9 `hsl(132.3,100%,43.9%)` 132.3°, 100, 87.8 00cc33 `#00cc33`\nCIE-LAB 78.172, -76.636, 67.879 27.147, 53.505, 11.481 0.295, 0.581, 53.505 78.172, 102.375, 138.468 78.172, -73.356, 90.344 73.147, -61.761, 41.897 00000000, 11100000, 00101110\n\n# Color Schemes with #00e02e\n\n• #00e02e\n``#00e02e` `rgb(0,224,46)``\n• #e000b2\n``#e000b2` `rgb(224,0,178)``\nComplementary Color\n• #42e000\n``#42e000` `rgb(66,224,0)``\n• #00e02e\n``#00e02e` `rgb(0,224,46)``\n• #00e09e\n``#00e09e` `rgb(0,224,158)``\nAnalogous Color\n• #e00042\n``#e00042` `rgb(224,0,66)``\n• #00e02e\n``#00e02e` `rgb(0,224,46)``\n• #9e00e0\n``#9e00e0` `rgb(158,0,224)``\nSplit Complementary Color\n• #e02e00\n``#e02e00` `rgb(224,46,0)``\n• #00e02e\n``#00e02e` `rgb(0,224,46)``\n• #2e00e0\n``#2e00e0` `rgb(46,0,224)``\n• #b2e000\n``#b2e000` `rgb(178,224,0)``\n• #00e02e\n``#00e02e` `rgb(0,224,46)``\n• #2e00e0\n``#2e00e0` `rgb(46,0,224)``\n• #e000b2\n``#e000b2` `rgb(224,0,178)``\n• #00941e\n``#00941e` `rgb(0,148,30)``\n``#00ad24` `rgb(0,173,36)``\n• #00c729\n``#00c729` `rgb(0,199,41)``\n• #00e02e\n``#00e02e` `rgb(0,224,46)``\n• #00fa33\n``#00fa33` `rgb(0,250,51)``\n• #14ff44\n``#14ff44` `rgb(20,255,68)``\n• #2eff59\n``#2eff59` `rgb(46,255,89)``\nMonochromatic Color\n\n# Alternatives to #00e02e\n\nBelow, you can see some colors close to #00e02e. Having a set of related colors can be useful if you need an inspirational alternative to your original color choice.\n\n• #0ae000\n``#0ae000` `rgb(10,224,0)``\n• #00e009\n``#00e009` `rgb(0,224,9)``\n• #00e01b\n``#00e01b` `rgb(0,224,27)``\n• #00e02e\n``#00e02e` `rgb(0,224,46)``\n• #00e041\n``#00e041` `rgb(0,224,65)``\n• #00e053\n``#00e053` `rgb(0,224,83)``\n• #00e066\n``#00e066` `rgb(0,224,102)``\nSimilar Colors\n\n# #00e02e Preview\n\nText with hexadecimal color #00e02e\n\nThis text has a font color of #00e02e.\n\n``<span style=\"color:#00e02e;\">Text here</span>``\n#00e02e background color\n\nThis paragraph has a background color of #00e02e.\n\n``<p style=\"background-color:#00e02e;\">Content here</p>``\n#00e02e border color\n\nThis element has a border color of #00e02e.\n\n``<div style=\"border:1px solid #00e02e;\">Content here</div>``\nCSS codes\n``.text {color:#00e02e;}``\n``.background {background-color:#00e02e;}``\n``.border {border:1px solid #00e02e;}``\n\n# Shades and Tints of #00e02e\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, #000802 is the darkest color, while #f4fff6 is the lightest one.\n\n• #000802\n``#000802` `rgb(0,8,2)``\n• #001c06\n``#001c06` `rgb(0,28,6)``\n• #002f0a\n``#002f0a` `rgb(0,47,10)``\n• #00430e\n``#00430e` `rgb(0,67,14)``\n• #005712\n``#005712` `rgb(0,87,18)``\n• #006a16\n``#006a16` `rgb(0,106,22)``\n• #007e1a\n``#007e1a` `rgb(0,126,26)``\n• #00921e\n``#00921e` `rgb(0,146,30)``\n• #00a522\n``#00a522` `rgb(0,165,34)``\n• #00b926\n``#00b926` `rgb(0,185,38)``\n• #00cc2a\n``#00cc2a` `rgb(0,204,42)``\n• #00e02e\n``#00e02e` `rgb(0,224,46)``\n• #00f432\n``#00f432` `rgb(0,244,50)``\n• #08ff3b\n``#08ff3b` `rgb(8,255,59)``\n• #1cff4a\n``#1cff4a` `rgb(28,255,74)``\n• #2fff5a\n``#2fff5a` `rgb(47,255,90)``\n• #43ff6a\n``#43ff6a` `rgb(67,255,106)``\n• #57ff79\n``#57ff79` `rgb(87,255,121)``\n• #6aff89\n``#6aff89` `rgb(106,255,137)``\n• #7eff98\n``#7eff98` `rgb(126,255,152)``\n• #92ffa8\n``#92ffa8` `rgb(146,255,168)``\n• #a5ffb8\n``#a5ffb8` `rgb(165,255,184)``\n• #b9ffc7\n``#b9ffc7` `rgb(185,255,199)``\n• #ccffd7\n``#ccffd7` `rgb(204,255,215)``\n• #e0ffe6\n``#e0ffe6` `rgb(224,255,230)``\n• #f4fff6\n``#f4fff6` `rgb(244,255,246)``\nTint Color Variation\n\n# Tones of #00e02e\n\nA tone is produced by adding gray to any pure hue. In this case, #67796b is the less saturated color, while #00e02e is the most saturated one.\n\n• #67796b\n``#67796b` `rgb(103,121,107)``\n• #5f8166\n``#5f8166` `rgb(95,129,102)``\n• #568a61\n``#568a61` `rgb(86,138,97)``\n• #4e925c\n``#4e925c` `rgb(78,146,92)``\n• #459b57\n``#459b57` `rgb(69,155,87)``\n• #3ca452\n``#3ca452` `rgb(60,164,82)``\n• #34ac4c\n``#34ac4c` `rgb(52,172,76)``\n• #2bb547\n``#2bb547` `rgb(43,181,71)``\n• #22be42\n``#22be42` `rgb(34,190,66)``\n• #1ac63d\n``#1ac63d` `rgb(26,198,61)``\n• #11cf38\n``#11cf38` `rgb(17,207,56)``\n• #09d733\n``#09d733` `rgb(9,215,51)``\n• #00e02e\n``#00e02e` `rgb(0,224,46)``\nTone Color Variation\n\n# Color Blindness Simulator\n\nBelow, you can see how #00e02e is perceived by people affected by a color vision deficiency. This can be useful if you need to ensure your color combinations are accessible to color-blind users.\n\nMonochromacy\n• Achromatopsia 0.005% of the population\n• Atypical Achromatopsia 0.001% of the population\nDichromacy\n• Protanopia 1% of men\n• Deuteranopia 1% of men\n• Tritanopia 0.001% of the population\nTrichromacy\n• Protanomaly 1% of men, 0.01% of women\n• Deuteranomaly 6% of men, 0.4% of women\n• Tritanomaly 0.01% of the population" ]
[ null ]
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http://www.mock4exam.org/quiz-mixture-and-alligation-set-3/
[ "# Quiz: Mixture and Alligation Set 3\n\n1. The average weekly salary per head of the entire staff of a factory consisting ofsupervisors and the labourers is Rs. 55. The average salary per head of the supervisors is Rs. 300 and that of the labourers is Rs. 40. Given that the number of supervisors is 10, find the number of labourers in the factory.\nA.160\nB.120\nC.155\nD.143\nE.None of these\n\nSolution:\n40…………………………………..300\n………………….55…………………….\n245…………………………………15\n(Number of labourers)/(Number of supervisors) = 245/15 = 16.33/1 = 16/1\n16:1 = 160:10\n2. A man travelled a distance of 40 km. in 5 hours partly on foot at the rate of 7 km per hour and partly on bicycle at 12 km. per hour. Find the distance travelled on foot ?\nA.36km\nB.24km\nC.32km\nD.28km\nE.None of these\n\nSolution:\n7……………………………………….12\n…………………..40/5=8………………..\n4………………………………………..1\nTime taken on foot /Time taken on bicycle = 4:1\nDistance travelled on foot = 4*7 = 28km\n3. Milk contains 15% water. What quantity of pure milk should be added to 50 litres of milk to reduce the quantity of water to 12% ?\nA.16litres\nB.14litres\nC.12.5litres\nD.17litres\nE.None of these\n\nSolution:\nAns: 50*15/100 = (50+x)*12/100\n7.5 *100 = 600+12x\n12x = 150\nX = 150/12 = 12.5litre\n4. Dhal worth Rs. 110 per kg and Rs. 95 per kg are mixed with a third variety in the ratio 1:1:2. If the mixture is worth Rs. 115 per kg, the price of the third variety per kg will be\nA.Rs.127.5\nB.Rs.115.75\nC.Rs.125\nD.Rs.117.5\nE.None of these\n\nSolution:\n1st two type of Dhal = 110+95/2 = 102.5\n102.5…………………………………..X\n……………..115……………………….\nx-115……………………………………12.5\nx-115 = 12.5\nx = 127.5\n5. A zookeeper counted the heads of the animals in a zoo and found it to be 100. When he counted the legs of the animals he found it to be 340. If the zoo had either pigeons or elephants, how many pigeons were there in the zoo?\nA.45\nB.30\nC.70\nD.50\nE.None of these\n\nSolution:\ntotal number of legs = 4x + 2(100-x) = 340\n4x + 200 – 2x = 340\n2x = 140\nx = 70\nP = 100-70 =30\n6. In a 70 litres mixture of milk and water, % of water is 30%. The milkman gave 20 litres of this mixture to a customer and then added 20 litres of water to the remaining mixture. What is the % of milk in the final mixture ?\nA.48%\nB.50%\nC.40%\nD.53%\nE.None of these\n\nSolution:\n20litre given remaining = 70-20 = 50litre\nQuantity of milk = 50*70/100 = 35litre\nQuantity of water = 50-35 = 15litre\n20litres of water added = 50+20 = 70\n% of milk = 35*100/70 =50%\n7. A company is creating a new signature drink. They are using two alcoholic ingredients in the drink vodka and gin. They are using two non-alcoholic ingredients in the drink: orange juice and cranberry juice. The alcoholic ingredients contain 50% alcohol. The non-alcoholic ingredients contain no alcohol. How many litres of non-alcoholic ingredients must be added to 5 litres of alcoholic ingredients to produce a mixture that is 20% alcohol?\nA.8\nB.6.5\nC.7.5\nD.9\nE.None of these\n\nSolution:\n(5+x) (20%) = 5(50%) + x(0%)\n(5+x) 0.2 = 5(0.5) + 0\n1+0.2x = 2.5\nX = 2.5-1/0.2 = 1.5/0.2 = 7.5\n8. A can contains 30liter of juice, from this container 5litres of juice was taken out and replaced by water. This process was repeated further two times. How much juice is now contained by the container?\nA.21\nB.13\nC.15\nD.17\nE.None of these\n\nSolution:\nQuantity of milk in the final mixture = 30[1-(5/30)]3\n= 30*(5/6) 3\n= 30*125/216 = 17.36 liter = 17\n9. Rani mixes 70kg of sugar worth Rs.28.50 per kg with 100kg of sugar worth Rs.30.50 per kg. At what rate shall he sell the mixture to gain 10% ?\nA.Rs.32.64\nB.Rs.31.50\nC.Rs.30.46\nD.Rs.29.75\nE.None of these\n\nSolution:\n70/100 = 100x – 30.50(110)/28.50(110)-100x\n0.7 = 100x-3355/3135-100x\n2194.5 – 70x =  100x-3355\n170x = 5549.5\nX = 32.64\n10. 90 litres of a mixture of milk and water contains 20% water. How much water should be added so that the mixture has 28% water ?\nA.18litres\nB.12litres\nC.10litres\nD.8litres\nE.None of these" ]
[ null ]
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https://planspace.org/20150417-negative_r_squared/
[ "# R Squared Can Be Negative\n\nFriday April 17, 2015\n\nLet's do a little linear regression in Python with scikit-learn:\n\n``````import numpy as np\nfrom sklearn.linear_model import LinearRegression\nfrom sklearn.cross_validation import train_test_split\n\nX, y = np.random.randn(100, 20), np.random.randn(100)\nX_train, X_test, y_train, y_test = train_test_split(X, y)\n\nmodel = LinearRegression()\nmodel.fit(X_train, y_train)``````\n\nIt is a property of ordinary least squares regression that for the training data we fit on, the coefficient of determination R2 and the square of the correlation coefficient r2 of the model's predictions with the actual data are equal.\n\n``````# coefficient of determination R^2\nprint model.score(X_train, y_train)\n## 0.203942898079\n\n# squared correlation coefficient r^2\nprint np.corrcoef(model.predict(X_train), y_train)[0, 1]**2\n## 0.203942898079``````\n\nThis does not hold for new data, and if our model is sufficiently bad the coefficient of determination can be negative. The squared correlation coefficient is never negative but can be quite low.\n\n``````# coefficient of determination R^2\nprint model.score(X_test, y_test)\n## -0.277742673311\n\n# squared correlation coefficient r^2\nprint np.corrcoef(model.predict(X_test), y_test)[0, 1]**2\n## 0.0266856746214``````\n\nThese declines in performance worsen with overfitting." ]
[ null ]
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https://books.google.gr/books?id=BMc2AAAAMAAJ&pg=PA198&vq=%22How+many+bricks+8+inches+long,+4+inches+wide,+and+2+inches+thick,%22&dq=editions:HARVARD32044096994090&lr=&hl=el&output=html_text
[ "Ĺéęüíĺň óĺëßäáň PDF Çëĺęôń. Ýęäďóç\n .flow { margin: 0; font-size: 1em; } .flow .pagebreak { page-break-before: always; } .flow p { text-align: left; text-indent: 0; margin-top: 0; margin-bottom: 0.5em; } .flow .gstxt_sup { font-size: 75%; position: relative; bottom: 0.5em; } .flow .gstxt_sub { font-size: 75%; position: relative; top: 0.3em; } .flow .gstxt_hlt { background-color: yellow; } .flow div.gtxt_inset_box { padding: 0.5em 0.5em 0.5em 0.5em; margin: 1em 1em 1em 1em; border: 1px black solid; } .flow div.gtxt_footnote { padding: 0 0.5em 0 0.5em; border: 1px black dotted; } .flow .gstxt_underline { text-decoration: underline; } .flow .gtxt_heading { text-align: center; margin-bottom: 1em; font-size: 150%; font-weight: bold; font-variant: small-caps; } .flow .gtxt_h1_heading { text-align: center; font-size: 120%; font-weight: bold; } .flow .gtxt_h2_heading { font-size: 110%; font-weight: bold; } .flow .gtxt_h3_heading { font-weight: bold; } .flow .gtxt_lineated { margin-left: 2em; margin-top: 1em; margin-bottom: 1em; white-space: pre-wrap; } .flow .gtxt_lineated_code { margin-left: 2em; margin-top: 1em; margin-bottom: 1em; white-space: pre-wrap; font-family: monospace; } .flow .gtxt_quote { margin-left: 2em; margin-right: 2em; margin-top: 1em; margin-bottom: 1em; } .flow .gtxt_list_entry { margin-left: 2ex; text-indent: -2ex; } .flow .gimg_graphic { margin-top: 1em; margin-bottom: 1em; } .flow .gimg_table { margin-top: 1em; margin-bottom: 1em; } .flow { font-family: serif; } .flow span,p { font-family: inherit; } .flow-top-div {font-size:83%;} 29. At \\$2.67\\$ per yard, what will 400 yards of cloth cost? 30. At \\$54 per barrel, what will 1560 barrels of flour cost? DIVISION OF FEDERAL MONEY. Ex. 1. A man bought 6 hats for \\$25.68: how much did they cost apiece ? Operation. If 6 hats cost \\$25.68, 1 hat will cost 6)25.68 one sixth of \\$25.68. Divide as in sim\\$4.28 Ans, ple numbers, and point off two decimal figures in the quotient. (Art. 194.) Proof. \\$4.28 If i hat costs \\$4.28, 6 hats will cost 6 times 6 as much ; and \\$4.28 x6=\\$25.68, which is the cost. Hence, \\$25.68 217. When the number of articles, pounds, yards, &c., and the cost of the whole are given, to find the price of one article, pound, &c. Divide the whole cost by the whole number of articles, fc., and point off the quotient as in division of decimal fractions. (Art. 194.) 2. How many yards of cloth, at \\$3.13 per yard, can be bought for \\$20.345 ? Operation. Since \\$3.13 will buy 1 yard, 3.13)20.345(6.5 Ans. \\$20.345 will buy as many yards 18 78 as \\$3.13 is contained times in \\$20.345. Divide as in simple 1 565 1 565 numbers, and point off one decimal figure in the quotient. (Art. 194.) Proof.—\\$3.13 X 6.5=20.345. Hence, , QUEST.-217. When the number of articles, pounds, &c., and the cost of the whole, are given, how is the cost of one article found ? 218. When the price of one article, pound, yard, &c., and the cost of the whole are given, to find the number of articles, &c. Divide the whole cost by the price of one, and point of the quotient as in Art. 217. 3. Divide \\$149.625 by \\$2.375. Ans. 63 cents. 4. If \\$75 are divided equally among 18 men, how much will each receive ? Operation. 18)75(\\$4.16 6 Ans. 72 3000 18 120 108 120 108 After dividing the \\$75 by 18, there is a remainder of 3 dollars, which must be reduced to cents and mills, (Art. 208,) and then be divided as before. The ciphers thus annexed must be regarded as decimals; consequently there will be three decimal figures in the quotient. 12 rem. 219. From the preceding illustrations we derive the following GENERAL RULE. Divide as in simple numbers, and point of the quotient as in division of decimal fractions. (Art. 194.) Obs. After all the figures of the dividend are divided, if there is a remainder, ciphers may be annexed to it, and the operation may be continued as in division of decimals. (Art. 194. Obs. 3.) The ciphers thus annexed must be regarded as decimal places of the dividend. 5. How many pounds of cheese, 'at 7 cts. a pound, can you buy for \\$1.47? QUEST.-218. When the price of 1 article, 1 pound, &c., and the cost of the whole, are given, how is the number of articles found? 219. What is the rule for Division of Federal Money? Obs. When there is a remainder after all the figures of the dividend are divided, how proceed? 6. A man paid \\$0.75 for the use of a horse and buggy to go 8 miles : how much was that per mile? 7. How many quarts of cherries, at 7 cents a quart, can you buy for \\$1.12? 8. How many pounds of figs, at 14 cents a pound, can you buy for \\$3.57 ? 9. How many watermelons, at 12 cts. apiece, can be bought for \\$3 ? 10. How many pen-knives, at 20 cts. apiece, can be bought for \\$7.20 ? 11. At 174 cts. a quart, how many quarts of molasses can be bought for \\$4.40 ? 12. A man bought 50 pair of thick boots for \\$175 : how much did he give a pair ? 13. A man paid \\$485.50 for 260 sheep: how much did he give per head ? 14. At \\$2.50 a cord, how many cords of wood can I buy for \\$165 ? 15. At \\$4.75 per barrel, how many barrels of flour can I buy for \\$8.50 ? 16. If a man's income is \\$1.68 per day, how much is it per hour ? 17. If a man pays \\$3.62} per week for board, how long can he board for \\$188.50 ? 18. Suppose a man's income is \\$500 a year, how much is that per day? 19. Suppose a man's interest money is \\$28.80 per day, how much is it per minute ? 20. A mason received \\$94.375 for doing a job, which took him 75} days : how much did he receive per day? 21. At \\$1.123 per bushel, how many bushels of wheat can be bought for \\$523.75 ? 22. If \\$1285.20 were divided equally among 125 men, what would each receive ? 23. If \\$1637.10 were divided equally among 150 men, what would each receive ? 24. The salary of the President of the United States is \\$25000 a year: how much does he receive per day? APPLICATIONS OF FEDERAL MONEY. BILLS, ACCOUNTS, &C. 220. A Bill, in mercantile operations, is a written paper, containing a statement of particulars, or amount of goods sold. Ex. 1. What is the cost of the several articles, and what the amount, of the following bill ? at · Boston, May 25th, 1845. James Brown, Esq. Bought of Fairfield f Lincoln, 5 yds. of Broadcloth, \\$3.25 3 yds. of Cambric, .12) 3 doz. Buttons, .15 6 skeins Sewing Silk, .06 4 yds. Wadding, .08 Amount, \\$17.77. Received Pay't, Fairfield f Lincoln. ( 2.)", null, "NEW HAVEN, Sept.20, 1845. Hon. R. S. Baldwin, Bought of Durrie of Peck, 4 Lovell's Young Speaker, at \\$ .621 5 Olmsted's Rudiments, .58 6 Morse's Geography, .50 8 Webster's Spelling Book, .10 3 Day's Algebra, 1.25 What was the cost of the several articles, and what the amount of his bill ? (3.) NEW YORK, Aug. 18th, 1845. John Jacob Astor, Esq. Bought of G. W. Lewis of Co. 25 lbs. Sugar, at \\$.09 50 lbs. Coffee, .11 12 lbs. Tea, .75 14 lbs. Raisins, .14 9 doz. Eggs, .10 15 lbs. Butter, .125 What was the cost of the several articles, and what the amount of his bill ? ( 4.) PHILADELPHIA, June 30, 1845. W. A. Sandford, Esq. To James Conrad, Dr. For 28 yds. Silk, at \\$1.25 “ 22 yds. Muslin, .56 “ 16 pair Cotton Hose, .37) Silk 1.10 66 25 \" Shoes, 1.25 What was the cost of the several articles, and how much is due on his account? 66 35 ( 5.) CINCINNATI, July 4th, 1845. Messrs. Holmes f Homer, To H. W. Morgan f Co. Dr. For 100 bls. Flour, at \\$4.50 50 8.25 25 Beef, 9.75 “ 112 kegs of Lard, 3.25 25 bush. of Corn, .34 What was the cost of the several articles, and how much is due on his account? “ Pork,", null, "66", null, "« ĐńďçăďýěĺíçÓőíÝ÷ĺéá »" ]
[ null, "https://books.google.gr/books/content", null, "https://books.google.gr/books/content", null, "https://books.google.gr/books/content", null ]
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https://cran.microsoft.com/snapshot/2017-02-25/web/packages/RcppShark/vignettes/RcppShark.html
[ "# Tutorial\n\nRcppShark is basically a bridge to allow creating packages based on Shark. It also allows for rapid prototyping using Shark as the underlying machine learning library. Therefore, the most important part is to understand how to use RcppShark in your own packages. For this reason, RcppShark contains (the usual) package skeleton creator. To develop your own package using RcppShark, you simply call after installing RcppShark\n\nlibrary (RcppShark)\n\nRcppShark.package.skeleton (“myOwnPackage”)\n\n(make sure your own name is valid). This will create a empty package structure where you can freely use Shark in the C++ part. Let us wrap the KMeans algorithm, following the tutorial from the Shark homepage (http://image.diku.dk/shark/sphinx_pages/build/html/rest_sources/tutorials/algorithms/kmeans.html).\n\nFor this we want basically two functions: One that will ‘learn’ the clustering and cluster the given training data, and one that will ‘predict’ the clustering to new data. Let us start with the first part. We start with the C++ code, and will only add R code, if it is necessary. Rcpp will export our C++ function to R in a very nice fashion, so it is not always necessary to add R code, at least not for our little tutorial.\n\nNow we can write the corresponding C++ function. For this we follow the Shark tutorial by creating a new file in the src folder of our new package, called KMeans.cpp, and importing all the headers we need:\n\n#include <shark/Algorithms/KMeans.h> //k-means algorithm\n#include <shark/Models/Clustering/Centroids.h>//model performing hard clustering of points\n#include <shark/Models/Clustering/HardClusteringModel.h>//model performing hard clustering of points\n\n#include <Rcpp.h>\n#include \"utils.h\" // some conversion helpers\n\nusing namespace shark;\nusing namespace std;\n\nusing namespace Rcpp;\n\nNote that we have skipped the CSV and normalizer header, as we have full control over both in R, and added Rcpp as well as our small utils.h header which contains some code to convert from the Shark to the Rcpp data format (and back). Lets continue with the main routine. This will take a matrix, the number of clusters $$k$$ to find and will return a list with the following two information: The final clustering in form of a model consisting of the centroids and a vector with the cluster assignments. So we start with the header:\n\n//' Simple KMeans Train\n//'\n//' @export\n//'\n// [[Rcpp::depends(BH)]]\n// [[Rcpp::export]]\nList SharkKMeansTrain (NumericMatrix X, ssize_t k) {\n\nThe first thing to do is to convert the given data in form of a matrix into an object, Shark can work with. For this, we call the corresponding function from the utils.h class:\n\n // convert data\nUnlabeledData<RealVector> data = NumericMatrixToUnlabeledData(X);\nstd::size_t elements = data.numberOfElements();\n\nNow comes the Shark code. For more details on this, please consult the Shark tutorial. We drop here everything that we do not need, e.g. printing information.\n\n // compute centroids using k-means clustering\nCentroids centroids;\nkMeans (data, k, centroids);\n\n// convert cluster centers/centroids\nData<RealVector> const& c = centroids.centroids();\nNumericMatrix cM = DataRealVectorToNumericMatrix (c);\n\n// cluster training data we are given and convert to Rcpp object\nHardClusteringModel<RealVector> model(&centroids);\nData<unsigned> clusters = model(data);\nNumericVector labels = LabelsToNumericVector (clusters);\n\nFinally we just need to put all the bits into a list and return it to R:\n\n // return solution found\nRcpp::List rl = R_NilValue;\nrl = Rcpp::List::create(\nRcpp::Named(\"labels\") = labels,\nRcpp::Named(\"centroids\") = cM );\nreturn (rl);\n\nPlease note that for sake of brevity we dropped all kind of checks. For production code such checks obviously should be done.\n\nBefore we test this code, let us quickly write the corresponding predict function (which is more or less already part of the training function, so we could drop that there):\n\n//' Simple KMeans Predict\n//'\n//' @export\n//'\n// [[Rcpp::depends(BH)]]\n// [[Rcpp::export]]\nList SharkKMeansPredict (NumericMatrix X, NumericMatrix centroids) {\n\n// convert data\nUnlabeledData<RealVector> data = NumericMatrixToUnlabeledData (X);\nstd::size_t elements = data.numberOfElements();\n\n// convert centroids\nCentroids c (NumericMatrixToDataRealVector (centroids));\n\n// cluster data we are given and convert to Rcpp object\nHardClusteringModel<RealVector> model (&c);\nData<unsigned> clusters = model (data);\nNumericVector labels = LabelsToNumericVector (clusters);\n\n// return solution found\nrl = Rcpp::List::create(Rcpp::Named(\"labels\") = labels);\nreturn (rl);\n}\n\nRunning this code is now easy, as by Rcpp::export tag, Rcpp will automatically create a wrapper to be called from R. This is good enough for us, though usually you really want to wrap the C++ function in a nice R routine. So we can now write a small function that will use our KMeans routine by creating first some example data and then calling our KMeans:\n\nlibrary (devtools)\n\n# convert iris to matrix\ndata = as.matrix(iris[,1:4])\n\nmodel = SharkKMeansTrain (data, 3)\nlabels = SharkKMeansPredict (data, model$centroids) Note that we need the devtools package, as we develop a new package. The output should be look similar to this: > model$labels\n 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0\n 0 0 0 0 0 0 0 0 0 0 0 0 0 1 1 2 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1\n 1 1 1 2 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 1 2 2 2 2 1 2 2 2 2\n 2 2 1 1 2 2 2 2 1 2 1 2 1 2 2 1 1 2 2 2 2 2 1 2 2 2 2 1 2 2 2 1 2 2 2 1 2\n 2 1\n\n$centroids [,1] [,2] [,3] [,4] [1,] 5.006000 3.428000 1.462000 0.246000 [2,] 5.901613 2.748387 4.393548 1.433871 [3,] 6.850000 3.073684 5.742105 2.071053 > labels$labels\n 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0\n 0 0 0 0 0 0 0 0 0 0 0 0 0 1 1 2 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1\n 1 1 1 2 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 1 2 2 2 2 1 2 2 2 2\n 2 2 1 1 2 2 2 2 1 2 1 2 1 2 2 1 1 2 2 2 2 2 1 2 2 2 2 1 2 2 2 1 2 2 2 1 2\n 2 1\n\nFor convenience every new created skeleton contains the above KMeans example." ]
[ null ]
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https://www.ams.org/journals/tran/1974-193-00/S0002-9947-1974-0352427-3/
[ "", null, "", null, "", null, "ISSN 1088-6850(online) ISSN 0002-9947(print)\n\nInequalities for polynomials with a prescribed zero\n\nAuthors: A. Giroux and Q. I. Rahman\nJournal: Trans. Amer. Math. Soc. 193 (1974), 67-98\nMSC: Primary 30A06\nDOI: https://doi.org/10.1090/S0002-9947-1974-0352427-3\nMathSciNet review: 0352427\nFull-text PDF Free Access\n\nAbstract: Inequalities for the derivative and for the maximum modulus on a larger circle of a polynomial with a given zero on the unit circle are obtained in terms of its degree and maximum modulus on the unit circle; examples are given to show that these are sharp with respect to the degree (best constants are not known). Inequalities for \\${L^p}\\$ norms, in particular \\${L^2}\\$ norms, are also derived. Also certain functions of exponential type are considered and similar inequalities are obtained for them. Finally, the problem of estimating \\${P_n}(r)\\$ (with \\$0 < r < 1\\$) given \\${P_n}(1) = 0\\$ is taken up.\n\n[Enhancements On Off] (What's this?)\n\nRetrieve articles in Transactions of the American Mathematical Society with MSC: 30A06\n\nRetrieve articles in all journals with MSC: 30A06\n\nAdditional Information\n\nKeywords: Derivative of a polynomial, Bernstein’s inequality, growth of maximum modulus, problem of Hal&#225;sz, <IMG WIDTH=\"29\" HEIGHT=\"20\" ALIGN=\"BOTTOM\" BORDER=\"0\" SRC=\"images/img1.gif\" ALT=\"\\${L^p}\\$\"> norm of a polynomial, trigonometric polynomial, entire function of exponential type, interpolation formula\nArticle copyright: © Copyright 1974 American Mathematical Society" ]
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https://jneuroinflammation.biomedcentral.com/articles/10.1186/s12974-020-01808-2/tables/2
[ "# Table 2 The number and distribution of the animals included for the present study\n\nGroups (n) Mortality (n)\nTime course study WB (6, 12, 24, and 72 h post-ROSC) Sham (n = 4) 0\nACA (6 h, 12 h, 24 h, 72 h) (n = 16) 3 (1 died at 12 h, 1 died at 15 h, and 1 died at 22 h post-ROSC)\nCellular localization (24 h post-ROSC) Sham (n = 1), ACA (n = 1) 0\nToluidine blue staining (24 h post-ROSC) Sham (n = 1) 0\nACA (n = 1) 0\nShort-term outcome study (up to 7-day post ROSC) Fluoro-Jade C staining Sham (n = 6) 0\nACA + vehicle (n = 6) 2 (1 at 24 h post-ROSC, 1 died at 48 h post-ROSC)\nACA + APC366 (50 μg) (n = 6) 2 (1 died at 48 h post-ROSC, 1 died at 70 h post-ROSC)\nACA + APC366 (150) (n = 6) 1 (died at 6 h post-ROSC)\nACA + AC55541 (30 μg) (n = 6) 2 (1 died on 5th day post-ROSC, 1 died on 6th post-ROSC)\nLong-term outcome study (30-day post-ROSC) Fluoro-Jade C staining Sham (n = 6) 0\nACA + vehicle (n = 6) 0\nACA + APC366 (50 μg) (n = 6) 0\nMechanism study (24 h post-ROSC) Western blot Sham (n = 6) 0\nACA + vehicle (n = 6) 0\nACA + APC366 (50 μg) (n = 6) 0\nACA + AC55541 (30 μg) (n = 6) 0\nACA + APC366 (50 μg) + AC55541 (30 μg) (n = 6) 1 (died at 8 h post-ROSC)\nACA + AC55541 (30 μg) + SB203580 (300 μg) (n = 6) 0\nMass spectrometry APC366 (n = 1) 0\nTotal 120 109 11\n1. ACA asphyxial cardiac arrest, h hours, ROSC return of spontaneous circulation", null, "" ]
[ null, "https://jneuroinflammation.biomedcentral.com/track/article/10.1186/s12974-020-01808-2", null ]
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https://demonstrations.wolfram.com/EulersGeneratingFunctionForThePartitionNumbers/
[ "", null, "# Euler's Generating Function for the Partition Numbers\n\nInitializing live version", null, "Requires a Wolfram Notebook System\n\nInteract on desktop, mobile and cloud with the free Wolfram Player or other Wolfram Language products.\n\nThis Demonstration shows the partition numbers", null, "up to", null, "as the coefficients of", null, "in the polynomial on the right.\n\n[more]\n\nThe partition numbers", null, "are 1, 1, 2, 3, 5, 7, 11, 15, 22, 30, 42, 56, 77, 101, 135, 176, 231, 297, 385, 490, 627, …. They count the number of ways of splitting an integer", null, "into a sum of positive integers, without regard to order. For instance,", null, ", the number of ways to partition 4, is 5 because there are 5 possible sums that add to 4: 4, 1+3, 2+2, 1+1+2, 1+1+1+1. By convention,", null, ".\n\nThe left-hand side of the identity shows the product of geometric series", null, "with common ratios", null, ",", null, ",", null, ",…,", null, ", each truncated to", null, "terms. The right-hand side multiplies them out and collects terms.\n\nAs an example, let", null, "; the term", null, "on the right is the sum of the five products", null, ",", null, ",", null, ",", null, ",", null, ", where the factors in each product are in the order of the series they come from. These products correspond to the partitions 4, 1+3, 2+2, 1+1+2, 1+1+1+1.\n\nIn general, an uncollected term in the expansion of the left side is of the form", null, ". The factor", null, "comes from the", null, "term of the", null, "truncated series", null, "and contributes", null, "(", null, "times) in the corresponding partition. Collecting terms amounts to counting the number of ways", null, "can be partitioned.\n\nThe generating function for", null, "is thus", null, ".\n\n[less]\n\nContributed by: George Beck (March 2011)\nOpen content licensed under CC BY-NC-SA\n\n## Snapshots", null, "", null, "", null, "## Permanent Citation\n\nGeorge Beck\n\n Feedback (field required) Email (field required) Name Occupation Organization Note: Your message & contact information may be shared with the author of any specific Demonstration for which you give feedback. Send" ]
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https://www.colorhexa.com/00d55b
[ "# #00d55b Color Information\n\nIn a RGB color space, hex #00d55b is composed of 0% red, 83.5% green and 35.7% blue. Whereas in a CMYK color space, it is composed of 100% cyan, 0% magenta, 57.3% yellow and 16.5% black. It has a hue angle of 145.6 degrees, a saturation of 100% and a lightness of 41.8%. #00d55b color hex could be obtained by blending #00ffb6 with #00ab00. Closest websafe color is: #00cc66.\n\n• R 0\n• G 84\n• B 36\nRGB color chart\n• C 100\n• M 0\n• Y 57\n• K 16\nCMYK color chart\n\n#00d55b color description : Strong cyan - lime green.\n\n# #00d55b Color Conversion\n\nThe hexadecimal color #00d55b has RGB values of R:0, G:213, B:91 and CMYK values of C:1, M:0, Y:0.57, K:0.16. Its decimal value is 54619.\n\nHex triplet RGB Decimal 00d55b `#00d55b` 0, 213, 91 `rgb(0,213,91)` 0, 83.5, 35.7 `rgb(0%,83.5%,35.7%)` 100, 0, 57, 16 145.6°, 100, 41.8 `hsl(145.6,100%,41.8%)` 145.6°, 100, 83.5 00cc66 `#00cc66`\nCIE-LAB 75.039, -69.17, 47.455 25.681, 48.341, 17.874 0.279, 0.526, 48.341 75.039, 83.884, 145.547 75.039, -68.423, 70.737 69.528, -55.742, 33.427 00000000, 11010101, 01011011\n\n# Color Schemes with #00d55b\n\n• #00d55b\n``#00d55b` `rgb(0,213,91)``\n• #d5007a\n``#d5007a` `rgb(213,0,122)``\nComplementary Color\n• #0fd500\n``#0fd500` `rgb(15,213,0)``\n• #00d55b\n``#00d55b` `rgb(0,213,91)``\n• #00d5c6\n``#00d5c6` `rgb(0,213,198)``\nAnalogous Color\n• #d5000f\n``#d5000f` `rgb(213,0,15)``\n• #00d55b\n``#00d55b` `rgb(0,213,91)``\n• #c600d5\n``#c600d5` `rgb(198,0,213)``\nSplit Complementary Color\n• #d55b00\n``#d55b00` `rgb(213,91,0)``\n• #00d55b\n``#00d55b` `rgb(0,213,91)``\n• #5b00d5\n``#5b00d5` `rgb(91,0,213)``\n``#7ad500` `rgb(122,213,0)``\n• #00d55b\n``#00d55b` `rgb(0,213,91)``\n• #5b00d5\n``#5b00d5` `rgb(91,0,213)``\n• #d5007a\n``#d5007a` `rgb(213,0,122)``\n• #00893a\n``#00893a` `rgb(0,137,58)``\n• #00a245\n``#00a245` `rgb(0,162,69)``\n• #00bc50\n``#00bc50` `rgb(0,188,80)``\n• #00d55b\n``#00d55b` `rgb(0,213,91)``\n• #00ef66\n``#00ef66` `rgb(0,239,102)``\n• #09ff72\n``#09ff72` `rgb(9,255,114)``\n• #23ff81\n``#23ff81` `rgb(35,255,129)``\nMonochromatic Color\n\n# Alternatives to #00d55b\n\nBelow, you can see some colors close to #00d55b. Having a set of related colors can be useful if you need an inspirational alternative to your original color choice.\n\n• #00d526\n``#00d526` `rgb(0,213,38)``\n• #00d538\n``#00d538` `rgb(0,213,56)``\n• #00d549\n``#00d549` `rgb(0,213,73)``\n• #00d55b\n``#00d55b` `rgb(0,213,91)``\n• #00d56d\n``#00d56d` `rgb(0,213,109)``\n• #00d57f\n``#00d57f` `rgb(0,213,127)``\n• #00d590\n``#00d590` `rgb(0,213,144)``\nSimilar Colors\n\n# #00d55b Preview\n\nThis text has a font color of #00d55b.\n\n``<span style=\"color:#00d55b;\">Text here</span>``\n#00d55b background color\n\nThis paragraph has a background color of #00d55b.\n\n``<p style=\"background-color:#00d55b;\">Content here</p>``\n#00d55b border color\n\nThis element has a border color of #00d55b.\n\n``<div style=\"border:1px solid #00d55b;\">Content here</div>``\nCSS codes\n``.text {color:#00d55b;}``\n``.background {background-color:#00d55b;}``\n``.border {border:1px solid #00d55b;}``\n\n# Shades and Tints of #00d55b\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, #001107 is the darkest color, while #fcfffd is the lightest one.\n\n• #001107\n``#001107` `rgb(0,17,7)``\n• #002410\n``#002410` `rgb(0,36,16)``\n• #003818\n``#003818` `rgb(0,56,24)``\n• #004c20\n``#004c20` `rgb(0,76,32)``\n• #005f29\n``#005f29` `rgb(0,95,41)``\n• #007331\n``#007331` `rgb(0,115,49)``\n• #008739\n``#008739` `rgb(0,135,57)``\n• #009a42\n``#009a42` `rgb(0,154,66)``\n• #00ae4a\n``#00ae4a` `rgb(0,174,74)``\n• #00c153\n``#00c153` `rgb(0,193,83)``\n• #00d55b\n``#00d55b` `rgb(0,213,91)``\n• #00e963\n``#00e963` `rgb(0,233,99)``\n• #00fc6c\n``#00fc6c` `rgb(0,252,108)``\n• #11ff77\n``#11ff77` `rgb(17,255,119)``\n• #24ff82\n``#24ff82` `rgb(36,255,130)``\n• #38ff8d\n``#38ff8d` `rgb(56,255,141)``\n• #4cff98\n``#4cff98` `rgb(76,255,152)``\n• #5fffa4\n``#5fffa4` `rgb(95,255,164)``\n• #73ffaf\n``#73ffaf` `rgb(115,255,175)``\n• #87ffba\n``#87ffba` `rgb(135,255,186)``\n• #9affc5\n``#9affc5` `rgb(154,255,197)``\n• #aeffd0\n``#aeffd0` `rgb(174,255,208)``\n• #c1ffdc\n``#c1ffdc` `rgb(193,255,220)``\n• #d5ffe7\n``#d5ffe7` `rgb(213,255,231)``\n• #e9fff2\n``#e9fff2` `rgb(233,255,242)``\n• #fcfffd\n``#fcfffd` `rgb(252,255,253)``\nTint Color Variation\n\n# Tones of #00d55b\n\nA tone is produced by adding gray to any pure hue. In this case, #627369 is the less saturated color, while #00d55b is the most saturated one.\n\n• #627369\n``#627369` `rgb(98,115,105)``\n• #5a7b68\n``#5a7b68` `rgb(90,123,104)``\n• #528367\n``#528367` `rgb(82,131,103)``\n• #4a8b66\n``#4a8b66` `rgb(74,139,102)``\n• #429365\n``#429365` `rgb(66,147,101)``\n• #399c63\n``#399c63` `rgb(57,156,99)``\n• #31a462\n``#31a462` `rgb(49,164,98)``\n• #29ac61\n``#29ac61` `rgb(41,172,97)``\n• #21b460\n``#21b460` `rgb(33,180,96)``\n• #19bc5f\n``#19bc5f` `rgb(25,188,95)``\n• #10c55d\n``#10c55d` `rgb(16,197,93)``\n• #08cd5c\n``#08cd5c` `rgb(8,205,92)``\n• #00d55b\n``#00d55b` `rgb(0,213,91)``\nTone Color Variation\n\n# Color Blindness Simulator\n\nBelow, you can see how #00d55b is perceived by people affected by a color vision deficiency. This can be useful if you need to ensure your color combinations are accessible to color-blind users.\n\nMonochromacy\n• Achromatopsia 0.005% of the population\n• Atypical Achromatopsia 0.001% of the population\nDichromacy\n• Protanopia 1% of men\n• Deuteranopia 1% of men\n• Tritanopia 0.001% of the population\nTrichromacy\n• Protanomaly 1% of men, 0.01% of women\n• Deuteranomaly 6% of men, 0.4% of women\n• Tritanomaly 0.01% of the population" ]
[ null ]
{"ft_lang_label":"__label__en","ft_lang_prob":0.5080168,"math_prob":0.86883485,"size":3678,"snap":"2023-40-2023-50","text_gpt3_token_len":1644,"char_repetition_ratio":0.133914,"word_repetition_ratio":0.0073664826,"special_character_ratio":0.5541055,"punctuation_ratio":0.23224352,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9887068,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-12-07T14:15:42Z\",\"WARC-Record-ID\":\"<urn:uuid:5cb6f384-e2f5-4aa6-9172-ae88e85808d8>\",\"Content-Length\":\"36181\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:5e86c6c1-14fc-40e8-b781-2abb2051afb0>\",\"WARC-Concurrent-To\":\"<urn:uuid:e732371f-5ff7-4754-b881-499e9ce3461b>\",\"WARC-IP-Address\":\"178.32.117.56\",\"WARC-Target-URI\":\"https://www.colorhexa.com/00d55b\",\"WARC-Payload-Digest\":\"sha1:LKTA7M55RKWGMU7VQWTO5AE6UIYVSAB4\",\"WARC-Block-Digest\":\"sha1:WKYSJ6PBBA7IVHAX2DPEDIXWTJKSZUZQ\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-50/CC-MAIN-2023-50_segments_1700679100674.56_warc_CC-MAIN-20231207121942-20231207151942-00364.warc.gz\"}"}
https://markupuk.org/webhelp/ar08s02s02.html
[ "### Showing linked changes to JSON Structure in diff3x\n\nFor JSON, the issue of handling curly braces (for objects) and square brackets (for arrays) is similar to XML start and end tags. Again, some representation of connected change is needed to maintain syntactic correctness.\n\nObject members and array members are comma separated and this is tricky to get right in some situations. The syntax is shown below.\n\n```object = begin-object [ member *( value-separator member ) ]\nend-object\narray = begin-array [ value *( value-separator value ) ] end-array\n\nThese are the six structural characters:\nbegin-array = ws %x5B ws ; [ left square bracket\nbegin-object = ws %x7B ws ; { left curly bracket\nend-array = ws %x5D ws ; ] right square bracket\nend-object = ws %x7D ws ; } right curly bracket\nname-separator = ws %x3A ws ; : colon\nvalue-separator = ws %x2C ws ; , comma\n\nInsignificant whitespace is allowed before or after any of the six\nstructural characters.\nws = *(\n%x20 / ; Space\n%x09 / ; Horizontal tab\n%x0A / ; Line feed or New line\n%x0D ) ; Carriage return```\n\nHere is an example of a change to an array of strings.\n\nTable 3. JSON structural change\n\nA.txtO.txtB.txt\n`[[12,13,14],20,21,22]`\n`[12,13,14,20,21,22]`\n`[[12,13,14,20,21,22]]`\n\nThis could be represented in the diff3 format as shown below, but note that this is not how diff3 would process the above files which each have a single line. However the result below could be generated by careful use of line breaks in the input files.\n\n```[\n<<<<<<<< A.txt\n[\n||||||| O.txt\n\n=======\n\n>>>>>>> B.txt\n\n<<<<<<<< A.txt\n\n||||||| O.txt\n\n=======\n[\n>>>>>>> B.txt\n12,13,14\n<<<<<<<< A.txt\n]\n||||||| O.txt\n\n=======\n\n>>>>>>> B.txt\n,20,21,22\n<<<<<<<< A.txt\n\n||||||| O.txt\n\n=======\n]\n>>>>>>> B.txt\n]```\n\nThe above will only produce syntactically correct results if the correct choices are made, which is not easy. It is also not easy to see what is going on in the diff3 file because of the extra whitespace lines that have to be inserted to make this work.\n\nWe introduce here a way to connect the relevant consistent choices so that if the '[' is selected then the appropriate choice of the end ']' is also made automatically.\n\nA choice consists of one or more options. An option may have an id. An option may also have a select attribute which provides a boolean value made up of one or a combination of other ids and if these are 'true', i.e. have been chosen to be included, then this option is selected automatically.\n\nThis could be represented in diff3x as shown below. We show here the id attribute on an option to identify it uniquely within the file. We then use that id to reference that option where another option needs to be linked to it. In this case, the '[' in the A.txt has `id=\"a42\"` and this is then referenced in the select attribute of the corresponding ']' option later in the file. Similarly the pair of square brackets in B.txt are linked with the id \"b44\".\n\n```<diff3x a=\"A.txt\" b=\"B.txt\" o=\"O.txt\">\n[\n<choice2>\n<a id=\"a42\">[</a>\n<ob/></choice2>\n<choice2>\n<b id=\"b44\">[</b>\n<ao/></choice2>\n12,13,14\n<choice2>\n<a select=\"a42\">]</a>\n<ob/></choice2>\n,20,21,22\n<choice2>\n<b select=\"b44\">]</b>\n<ao/></choice2>\n]</diff3x>```\n\nNote that the '[' in A could be selected either instead of or as well as the '[' in B even though they are at the same position in the array. Whichever choice is made, the other choices with a select attribute identifying the same id are chosen and the result is syntactically correct. This is a powerful way to represent connected choices." ]
[ null ]
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https://www.numbers.education/2683.html
[ "Is 2683 a prime number? What are the divisors of 2683?\n\n## Is 2683 a prime number?\n\nYes, 2683 is a prime number.\n\nIndeed, the definition of a prime numbers is to have only two distinct positive divisors, 1 and itself. A number is a divisor of another number when the remainder of Euclid’s division of the second one by the first one is zero. Concerning the number 2683, the only two divisors are 1 and 2683. Therefore 2683 is a prime number.\n\nAs a consequence, 2683 is only a multiple of 1 and 2683.\n\nSince 2683 is a prime number, 2683 is also a deficient number, that is to say 2683 is a natural integer that is strictly larger than the sum of its proper divisors, i.e., the divisors of 2683 without 2683 itself (that is 1, by definition!).\n\n## Parity of 2683\n\n2683 is an odd number, because it is not evenly divisible by 2.\n\n## Is 2683 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 2683 is about 51.798.\n\nThus, the square root of 2683 is not an integer, and therefore 2683 is not a square number.\n\nAnyway, 2683 is a prime number, and a prime number cannot be a perfect square.\n\n## What is the square number of 2683?\n\nThe square of a number (here 2683) is the result of the product of this number (2683) by itself (i.e., 2683 × 2683); the square of 2683 is sometimes called \"raising 2683 to the power 2\", or \"2683 squared\".\n\nThe square of 2683 is 7 198 489 because 2683 × 2683 = 26832 = 7 198 489.\n\nAs a consequence, 2683 is the square root of 7 198 489.\n\n## Number of digits of 2683\n\n2683 is a number with 4 digits.\n\n## What are the multiples of 2683?\n\nThe multiples of 2683 are all integers evenly divisible by 2683, that is all numbers such that the remainder of the division by 2683 is zero. There are infinitely many multiples of 2683. The smallest multiples of 2683 are:\n\n• 0: indeed, 0 is divisible by any natural number, and it is thus a multiple of 2683 too, since 0 × 2683 = 0\n• 2683: indeed, 2683 is a multiple of itself, since 2683 is evenly divisible by 2683 (we have 2683 / 2683 = 1, so the remainder of this division is indeed zero)\n• 5 366: indeed, 5 366 = 2683 × 2\n• 8 049: indeed, 8 049 = 2683 × 3\n• 10 732: indeed, 10 732 = 2683 × 4\n• 13 415: indeed, 13 415 = 2683 × 5\n• etc.\n\n## Nearest numbers from 2683\n\nFind out whether some integer is a prime number" ]
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http://ltcconline.net/greenl/courses/106/explogtrig/arcsechPrime.htm
[ "Derivative of sech-1(x) We use the fact from the definition of the inverse that      sech(sech-1(x))  =  x and the fact that      sech'(x)  =  -tanh(x)sech(x) Now take the derivative of both sides (using the chain rule on the left hand side) to get     -tanh(sech-1x)sech(sech-1(x))(sech-1(x))'  =  1 or   **      -x tanh(sech-1x)(sech-1(x))'  =  1 We know that          cosh2(x) - sinh2(x)  =  1 Dividing by the cosh2(x) gives         1 - tanh2(x)  =  sech2(x) or", null, "so that", null, "Finally substituting into **  gives", null, "Back to the Page on Hyperbolic Trig Back to Math 105 Home Page Back to the Math Department Home e-mail Questions and Suggestions" ]
[ null, "http://ltcconline.net/greenl/courses/106/explogtrig/arcsec1.gif", null, "http://ltcconline.net/greenl/courses/106/explogtrig/arcsec2.gif", null, "http://ltcconline.net/greenl/courses/106/explogtrig/arcsec3.gif", null ]
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https://simple-accounting.org/how-to-calculate-straight-line-depreciation/
[ "# How To Calculate Straight Line Depreciation Formula\n\nThese accounts have credit balance (when an asset has a credit balance, it’s like it has a ‘negative’ balance) meaning that they decrease the value of your assets as they increase. Straight-line depreciation is a simple method for calculating how much a particular fixed asset depreciates over time. Understanding asset depreciation is an important part of running any business. When you’re able to accurately determine the condition of your assets as well as its current depreciation rate, you’ll improve your overall efficiency.\n\nMost tax systems provide different rules for real property (buildings, etc.) and personal property (equipment, etc.). The carrying value would be \\$200 on the balance sheet at the end of three years. The depreciation expense would be completed under the straight line depreciation method, and management would retire the asset. Any gain or loss above or below the estimated salvage value would be recorded, and there would no longer be any carrying value under the fixed asset line of the balance sheet.\n\n• However, when using the double-declining balance method of depreciation, an entity is not required to only accelerate depreciation by two.\n• To evaluate the lease classification, we used the capital vs. operating lease criteria test.\n• Office furniture, for example, is an appropriate asset for straight line depreciation.\n• Although, all the amount is paid for the machine at the time of purchase, however, the expense is charged over a period of time.\n• With the double-declining balance method, higher depreciation is posted at the beginning of the useful life of the asset, with lower depreciation expenses coming later.\n• It is calculated for intangible assets as the actual cost less amortization expense/impairments.\n\nHowever, in most countries the life is based on business experience, and the method may be chosen from one of several acceptable methods. The straight line depreciation calculation should make it clear how much leeway management has in managing reported earnings in any given period. It might seem that management has a lot of discretion in determining how high or low reported earnings are in any given period, and that’s correct.\n\nOr you can also come up with an estimation of how many units the asset can produce during its useful life. Straight-line depreciation has advantages and disadvantages, and is only one of many other methods used to calculate depreciation.\n\nA company may also choose to go with this method if it offers them tax or cash flow advantages. Four standard types of calculationsare used to determine depreciation expenses. The most common methods are straight-line depreciation, double declining balance depreciation, units of production depreciation, and sum of years digits depreciation. With the double-declining balance method, higher depreciation is posted at the beginning of the useful life of the asset, with lower depreciation expenses coming later. This method is an accelerated depreciation method because more expenses are posted in an asset’s early years, with fewer expenses being posted in later years. This approach works by calculating depreciation as a percentage and then depreciating the asset at twice the percentage rate. Accumulated depreciation is the associated balance sheet line item for depreciation expense.\n\n## Other Methods Of Calculating Depreciation\n\nTo calculate composite depreciation rate, divide depreciation per year by total historical cost. To calculate depreciation expense, multiply straight line depreciation the result by the same total historical cost. The result, not surprisingly, will equal the total depreciation per year again.\n\nHowever, the straight line method does not accurately reflect the difference in usage of an asset and may not be the most appropriate value calculation method for some depreciable assets. This method is regarded as the most accurate representation of devaluation, as it more closely reflects the actual wear and tear that assets go through. When using the units of production method, more resources are needed to collect enough data over long periods of time. Because of additional efforts required for this method, it is typically used for higher-value equipment. Besides capital expenditures, businesses also incur operating expenditures.\n\n## Retiring Assets\n\nWe discuss these briefly in the last section of our Beginners Guide to Depreciation. After an asset has been fully depreciated, it can remain in use as long as it is needed and is in good working order. To learn how to handle the retiring of assets, please see last section of our tutorial Beginner’s Guide to Depreciation. They have estimated the useful life of the machine to be 8 years with a salvage value of \\$ 2,000. Here, we are simply taking an average of the useful value of the asset over its useful life.\n\nFurther, the full value of the asset resides in the accumulated depreciation account as a credit. Combining the total asset and accumulated depreciation amounts equals a net book value of \\$0. Using the facts and circumstances presented, we can use LeaseQuery’s present value calculator to calculate the present value of the lease payments.\n\n## Accountingtools\n\nThe straight-line method of depreciation assumes a constant rate of depreciation. It calculates how much a specific asset depreciates in one year, and then depreciates the asset by that amount every year after that. As buildings, tools and equipment wear out over time, they depreciate in value. Being able to calculate depreciation is crucial for writing off the cost of expensive purchases, and for doing your taxes properly.\n\nEach of those \\$1,600 charges would be balanced against a contra account under property, plant, and equipment on the balance sheet. This is known as accumulated depreciation, which effectively reduces the carrying value of the asset. For example, the balance sheet would show a \\$5,000 computer offset by a \\$1,600 accumulated depreciation contra account after the first year, so the net carrying value would be \\$3,400. Straight-line depreciation is a method used to calculate the decline in value of fixed assets, such as vehicles or office equipment. If your company uses a piece of equipment, you should see more depreciation when you use the machinery to produce more units of a commodity. If production declines, this method lowers the depreciation expenses from one year to the next. The straight-line method of depreciation isn’t the only way businesses can calculate the value of their depreciable assets.\n\nWe’ll do one month of your bookkeeping and prepare a set of financial statements for you to keep. You can’t get a good grasp of the total value of your assets unless you figure out how much they’ve depreciated. This is especially important for businesses that own a lot of expensive, long-term assets that have long useful lives. Compared to the other three methods, straight line depreciation is by far the simplest. Learn accounting fundamentals and how to read financial statements with CFI’s free online accounting classes. Note how the book value of the machine at the end of year 5 is the same as the salvage value.\n\nOne method is called partial year depreciation, where depreciation is calculated exactly at when assets start service. Simply select “Yes” as an input in order to use partial year depreciation when using the calculator. You will find the depreciation expense used for each period until the value of the asset declines to its salvage value. Even if you’re still struggling with understanding some accounting terms, fortunately, straight line depreciation is pretty straightforward.\n\nThe total cost of the furniture and fixtures, including tax and delivery, was \\$9,000. Sally estimates the furniture will be worth around \\$1,500 at the end of its useful life, which, according to the chart above, is seven years. The final cost of the tractor, including tax and delivery, is \\$25,000, and the expected salvage value is \\$6,000. According to the table above, Jim can depreciate the tractor over a three-year period. In the last line of the chart, notice that 25% of \\$3,797 is \\$949, not the \\$797 that’s listed. However, the total depreciation allowed is equal to the initial cost minus the salvage value, which is \\$9,000.\n\n## The Best Method Of Calculating Depreciation For Tax Reporting Purposes\n\nContra AccountContra Account is an opposite entry passed to offset its related original account balances in the ledger. It helps a business retrieve the actual capital amount & amount of decrease in the value, hence representing the account’s net balances. As can be seen from the above table – At the end of 8 years, i.e., after its useful life is over, the machine has depreciated to its salvage value. Cost Of SalesThe costs directly attributable to the production of the goods that are sold in the firm or organization are referred to as the cost of sales.\n\nBut keep in mind this opens up the risk of overestimating the asset’s value. Reed, Inc. also evaluates the incremental borrowing rate for the lease to be 4%. For this example we will assume no other lease incentives, accruals, or initial direct costs are applicable for this lease. A depreciation schedule that treats all property acquired during the year as being acquired exactly in the middle of the year. But the IRS uses the accelerated/MACRS or Section 179 for certain assets, including intangible assets like copyrights, patents and trademarks.\n\nAs such, the income statement is expensed evenly, so is the value of the asset on the balance sheet. The carrying amount of the asset on the balance sheet reduces by the same amount. There are many methods of distributing depreciation amount over its useful life. The total amount of depreciation for any asset will be identical in the end no matter which method of depreciation is chosen; only the timing of depreciation will be altered. There are a lot of reasons businesses choose to use the straight line depreciation method. The straight-line depreciation method is one of the most popular depreciation methods used to charge depreciation expenses from fixed assets equally period assets’ useful life.\n\n### How do you record adjusting entries for depreciation?\n\nHow to Record Depreciation Expense. Depreciation is recorded by debiting Depreciation Expense and crediting Accumulated Depreciation. This is recorded at the end of the period (usually, at the end of every month, quarter, or year). Depreciation Expense: An expense account; hence, it is presented in the income statement …\n\nThe declining balance method calculates more depreciation expense initially, and uses a percentage of the asset’s current book value, as opposed to its initial cost. So, the amount of depreciation declines over time, and continues until the salvage value is reached. The most common types of depreciation methods include straight-line, double declining balance, units of production, and sum of years digits. Straight-line depreciation is the most common method of allocating the cost of a plant asset to expense in the accounting periods during which the asset is used. With the straight-line method of depreciation, each full accounting year will report the same amount of depreciation. The total amount of depreciation over the years of the asset’s useful life will be the asset’s cost minus any expected or assumed salvage value. Four types of depreciation systems are commonly available within accounting.\n\n## Step 4: Divide 1 By The Number Of Years Of Useful Life To Determine Annual Depreciation Rate\n\nThe annual depreciation expense is a measure of the loss of value of the item. In the article, we have seen how the straight line depreciation method can be used to depreciate the value of the asset over the useful life of the asset. It is the easiest and simplest method of depreciation where the cost of the asset is depreciated uniformly over its useful life. The depreciation rate is the rate an asset is depreciated each period.\n\nIn our example, the title transfers, which means at the end of the lease term the lessee will own the asset and continue depreciating it. However, the useful life of the equipment in this example equals the lease term so at the end of the lease, the asset will be depreciated to \\$0. Now, let’s consider a full example of a finance lease to illustrate straight-line depreciation expense. Below we will describe each method and provide the formula used to calculate the periodic depreciation expense. Depreciation is an accounting method of allocating the cost of a tangible asset over its useful life and is used to account for declines in value over time. To calculate depreciation using a straight line basis, simply divide net price by the number of useful years of life the asset has. Straight line basis is calculated by dividing the difference between an asset’s cost and its expected salvage value by the number of years it is expected to be used.\n\nDouble declining balance is the most widely used declining balance depreciation method, which has a depreciation rate that is twice the value of straight line depreciation for the first year. Use a depreciation factor of two when doing calculations for double declining balance depreciation. Regarding this method, salvage values are not included in the calculation for annual depreciation. For accounting, in particular, depreciation concerns allocating the cost of an asset over a period of time, usually its useful life. When a company purchases an asset, such as a piece of equipment, such large purchases can skewer the income statement confusingly. Instead of appearing as a sharp jump in the accounting books, this can be smoothed by expensing the asset over its useful life.\n\nWhile operating expenditures are tax-deductible during the year they are incurred, capital expenditures are not. Businesses may be able to use these two accounting categories to their advantage if they have particular challenges.\n\nAny smaller expenses that are incurred and used in a single accounting period cannot be depreciated. Instead these expenses are considered operating expenditures and can be taxed deducted in the same fiscal year when they were incurred. Typical expenses that cannot be depreciated include things like office supplies, rent and utilities, taxes, and labor expenses. Just about any major piece of tangible property as well as some intangible propertycan be depreciated over time. Examples of tangible property may include buildings, production machinery, computer and technology systems, transportation vehicles, and furniture. According to the Internal Revenue Service, businesses may also depreciate particular intangible assets like copyrights, computer software, and patents. And to calculate the annual depreciation rate, we need to divide one by the number of useful life." ]
[ null ]
{"ft_lang_label":"__label__en","ft_lang_prob":0.9314696,"math_prob":0.93497896,"size":15844,"snap":"2022-27-2022-33","text_gpt3_token_len":3017,"char_repetition_ratio":0.19968434,"word_repetition_ratio":0.031126872,"special_character_ratio":0.18783136,"punctuation_ratio":0.096448466,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.98975986,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2022-06-30T13:35:57Z\",\"WARC-Record-ID\":\"<urn:uuid:27a5dbc2-0ba4-47ba-bb53-6ad9a78b1ceb>\",\"Content-Length\":\"136227\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:acc3c894-f271-4e15-ae77-d5c75cab594d>\",\"WARC-Concurrent-To\":\"<urn:uuid:a565627c-ef72-4854-8e4c-44f8404b30bd>\",\"WARC-IP-Address\":\"104.21.25.133\",\"WARC-Target-URI\":\"https://simple-accounting.org/how-to-calculate-straight-line-depreciation/\",\"WARC-Payload-Digest\":\"sha1:IAHXFDRLLRGXHHU36LCSJWFOQQT4EC2O\",\"WARC-Block-Digest\":\"sha1:U7CAUM2BFOYGG3KI2FGUFPYMVOUVW3VH\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2022/CC-MAIN-2022-27/CC-MAIN-2022-27_segments_1656103821173.44_warc_CC-MAIN-20220630122857-20220630152857-00185.warc.gz\"}"}
https://statsidea.com/a-easy-rationalization-of-numpy-axes-with-examples/
[ "# A Easy Rationalization of NumPy Axes (With Examples)\n\nMany purposes in NumPy require that you simply specify an axis alongside which to use a definite calculation.\n\nUsually refer to rule of thumb applies:\n\n• axis=0: Follow the calculation “column-wise”\n• axis=1: Follow the calculation “row-wise”\n\nPlease see symbol presentations a ocular illustration of the axes on a NumPy matrix with 2 rows and four columns:", null, "Please see examples display methods to importance the axis argument in numerous eventualities with refer to NumPy matrix:\n\n```import numpy as np\n\n#assemble NumPy matrix\nmy_matrix = np.matrix([[1, 4, 7, 8], [5, 10, 12, 14]])\n\n#view NumPy matrix\nmy_matrix\n\nmatrix([[ 1, 4, 7, 8],\n[ 5, 10, 12, 14]])\n```\n\n## Instance 1: In finding Cruel Alongside Other Axes\n\nWe will importance axis=0 to seek out the ruthless of every column within the NumPy matrix:\n\n```#to find ruthless of every column in matrix\nnp.ruthless(my_matrix, axis=0)\n\nmatrix([[ 3. , 7. , 9.5, 11. ]])\n```\n\nThe output presentations the ruthless worth of every column within the matrix.\n\nFor instance:\n\n• The ruthless worth of the primary column is (1 + 5) / 2 = 3.\n• The ruthless worth of the second one column is (4 + 10) / 2 = 7.\n\nAnd so forth.\n\nWe will additionally importance axis=1 to seek out the ruthless of every row within the matrix:\n\n```#to find ruthless of every row in matrix\nnp.ruthless(my_matrix, axis=1)\n\nmatrix([[ 5. ],\n[10.25]])```\n\nThe output presentations the ruthless worth of every row within the matrix.\n\nFor instance:\n\n• The ruthless worth within the first row is (1+4+7+8) / 4 = 5.\n• The ruthless worth in the second one row is (5+10+12+14) / 4 = 10.25.\n\n## Instance 2: In finding Sum Alongside Other Axes\n\nWe will importance axis=0 to seek out the sum of every column within the matrix:\n\n```#to find sum of every column in matrix\nnp.sum(my_matrix, axis=0)\n\nmatrix([[ 6, 14, 19, 22]])\n```\n\nThe output presentations the sum of every column within the matrix.\n\nFor instance:\n\n• The sum of the primary column is 1 + 5 = 6.\n• The sum of the second one column is 4 + 10 = 14.\n\nAnd so forth.\n\nWe will additionally importance axis=1 to seek out the sum of every row within the matrix:\n\n```#to find sum of every row in matrix\nnp.sum(my_matrix, axis=1)\n\nmatrix([,\n])```\n\nThe output presentations the sum of every row within the matrix.\n\nFor instance:\n\n• The sum of the primary row is 1+4+7+8 = 20.\n• The sum of the second one row is 5+10+12+14 = 41.\n\n## Extra Sources\n\nPlease see tutorials give an explanation for methods to carry out alternative regular operations in NumPy:\n\nThe best way to Build a NumPy Matrix with Random Numbers\nThe best way to Normalize a NumPy Matrix\nThe best way to Upload Row to Matrix in NumPy" ]
[ null, "https://www.statology.org/wp-content/uploads/2022/06/numpyaxis1.jpg", null ]
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https://easystats.github.io/insight/reference/is_gam_model.html
[ "Small helper that checks if a model is a generalized additive model.\n\n## Usage\n\nis_gam_model(x)\n\nx\n\nA model object.\n\n## Value\n\nA logical, TRUE if x is a generalized additive model and has smooth-terms\n\n## Note\n\nThis function only returns TRUE when the model inherits from a typical GAM model class and when smooth terms are present in the model formula. If model has no smooth terms or is not from a typical gam class, FALSE is returned.\n\n## Examples\n\nif (require(\"mgcv\")) {\ndata(iris)\nmodel1 <- lm(Petal.Length ~ Petal.Width + Sepal.Length, data = iris)\nmodel2 <- gam(Petal.Length ~ Petal.Width + s(Sepal.Length), data = iris)\nis_gam_model(model1)\nis_gam_model(model2)\n}\n#> TRUE" ]
[ null ]
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https://www.electronics-tutorial.net/lab-test-and-measurement/Circuit-simulation-and-Tools/exp-3/
[ "EXPERIMENT NO.3\n\nTITLE: COMPUTE AUTO CORRELATION AND CROSS CORRELATION OF TWO SEQUENCES\n\nTHEORY:-\n\nAuto-correlation:-\n\nCorrelation is a mathematical tool used frequently in signal processing for analyzing function or series of values such as time domain signals correlation is mutual relationship between two or more random variables. Auto-correlation is correlation of signal with itself. This is unlike of two different signals.\n\nAuto-correlation is useful for finding repeating patterns in a signal such as determining presence of periodic signal which has been buried under noise or identifying fundamental frequency of signal which doesn’t actually contains that frequency components but implies it with many harmonic frequency.\n\nDifferent definitions of auto-correlation are in us depending on field of study which is being considered and not all of them are equivalent. In some fields the term is used interchangeability with auto covariance.\n\nIn signal processing given signal f(t), the continues auto-correlation Rf(t) is the continues cross-correlation of f(t) with itself.\n\nThe auto-correlation of a periodic function is itself periodic with the very same period.\n\nThe auto-correlation of sum of two completely uncorrelated functions is the sum of auto-correlation each function separately.\n\nSince auto-correlation is specific type of cross-correlation, it maintains all properties of cross-correlation.\n\nThe auto-correlation of a white noise signal will have strong peak at t=0 & will be close for all other T. This shows that a sampled instance of white noise signal is not statically correlated to sampled instance of same white noise signal at another time.\n\nThe Wiener-khinchin theorem relates the auto-correlation function to power spectral density via Fourier transform.\n\nCross-correlation:-\n\nIn signal processing cross-correlation is a measure of similarities of two waveforms as function of time lag applied to one of them. This is also known as a sliding dot product or inner product. It is commonly used for searching a long duration signal for a shorter known feature. It also has applications in pattern recognition, single practical analysis & neurophysiology.\n\nThe cross-correlation is similar in nature to convolution of two functions. Whereas convolution involves reversing signal & then shifting it & multiplying by another signal, correlation only involves shifting it & multiplying (no reversing).\n\nIn an auto-correlation, which is the cross-correlation of signal with itself, there will always be a peak at lag of zero.\n\nIf x & y are two independent random variables with probability distribution f & q respectively, then probability distribution of difference y - x is given by cross-correlation f * q . In contrast the convolution f *q gives probability distribution of the sum x + y.\n\nIn probability theorems & statistics the term cross-correlation us also sometimes used to referred to the convenience conv(x,y) between two random variables x & y in order to distinguish that concept from “Covariance” of a random variable x, which is understood to be matrix of covariance between the scalar components of x.\n\nProperties:-\n\nThe cross-correlation of function f(t) & g(t) is equivalent to the convolution of f*(-t) & g(t)\n\ni.e.f*g=(t ->f*(-t))*g\n\nIf either for g is hermitical then:\n\nF * g= f * g\n\n(f * g) * (f * g) = (f * f) * (g * g)\n\nAnalysis to convolution theorem\n\nThe cross-correlation satisfies,\n\nF{ f * g} = ( F {f} )* F{g} ,\n\nWhere F denotes Fourier transform & an asterisk again indicates complex conjugates coupled with fast Fourier transform algorithms, this property is often explained for the efficiency numerical computation of cross-correlation.\n\nThe cross-correlation is related to the spectral density.\n\nThe cross-correlation of a convolution of f & h with function g is convolution of the correlation of f & g with kernel h:\n\n(f * h) * g = h -> * (f * g)\n\nMATLAB CODE\n\nAuto and Cross Correlation\n\ndisp('autocorrelation and crosscorelation of sequences');\n\ndisp('4 autocorrelation 5 crosscorelation');\n\nchoice=input('enter the choice of corelation=');\n\nswitch(choice)\n\ncase{4}\n\nx=input('enter the input seqence for auto,x=');\n\ny=fliplr(x);\n\nr=conv(x,y);\n\nsubplot(3,1,1);\n\nstem(x);\n\nsubplot(3,1,2);\n\nstem(y);\n\nsubplot(3,1,3);\n\nstem(r);\n\nxlabel('input bit sequence');\n\nylabel('amplitude');\n\ntitle('autocorrelation');\n\ncase{5}\n\nd=input('enter input sequence for cross,d=');\n\ny=input('enter input sequence for cross,y=');\n\nz=conv(d,y);\n\nsubplot(4,1,1);\n\nstem(d);\n\nsubplot(4,1,2);\n\nstem(y);\n\nsubplot(4,1,3);\n\nstem(z);\n\nxlabel('input bit sequence');\n\nylabel('amplitude');\n\ntitle('crosscorelation');\n\nend;\n\nOUTPUT:-\n\nautocorrelation and crosscorelation of sequences\n\n4 autocorrelation 5 crosscorelation\n\nenter the choice of corelation=5\n\nenter input sequence for cross,d=[7 8 9]\n\nenter input sequence for cross,y=[4 5 6]", null, "CONCLUSION" ]
[ null, "https://www.electronics-tutorial.net/lab-test-and-measurement/Circuit-simulation-and-Tools/exp-3/clip_image002.gif", null ]
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https://questions.llc/questions/1112138/if-x-represents-the-present-age-of-father-and-y-represents-the-present-age-of-son-then
[ "# if x represents the present age of father and y represents the present age of son,then what will be the equation of the statement \"present age of father is 5 times more than 6 times the age of son\"\n\n1. 👍\n2. 👎\n3. 👁\n4. ℹ️\n5. 🚩\n1. present age of father = x\n6 times the age of son = 6y\nso, we have\n\nx = 6y+5y\n\nI suspect you meant\n\nfive more than\n\nIf so, x=6y+5\n\nIf you meant\n\nfive times as much as, then x=5*6y\n\n1. 👍\n2. 👎\n3. ℹ️\n4. 🚩\n2. Blah\n\n1. 👍\n2. 👎\n3. ℹ️\n4. 🚩" ]
[ null ]
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https://number.academy/36368
[ "# Number 36368\n\nNumber 36,368 spell 🔊, write in words: thirty-six thousand, three hundred and sixty-eight . Ordinal number 36368th is said 🔊 and write: thirty-six thousand, three hundred and sixty-eighth. The meaning of number 36368 in Maths: Is Prime? Factorization and prime factors tree. The square root and cube root of 36368. What is 36368 in computer science, numerology, codes and images, writing and naming in other languages. Other interesting facts related to 36368.\n\n## What is 36,368 in other units\n\nThe decimal (Arabic) number 36368 converted to a Roman number is (X)(X)(X)(V)MCCCLXVIII. Roman and decimal number conversions.\n\n#### Weight conversion\n\n36368 kilograms (kg) = 80176.9 pounds (lbs)\n36368 pounds (lbs) = 16496.4 kilograms (kg)\n\n#### Length conversion\n\n36368 kilometers (km) equals to 22599 miles (mi).\n36368 miles (mi) equals to 58529 kilometers (km).\n36368 meters (m) equals to 119317 feet (ft).\n36368 feet (ft) equals 11086 meters (m).\n36368 centimeters (cm) equals to 14318.1 inches (in).\n36368 inches (in) equals to 92374.7 centimeters (cm).\n\n#### Temperature conversion\n\n36368° Fahrenheit (°F) equals to 20186.7° Celsius (°C)\n36368° Celsius (°C) equals to 65494.4° Fahrenheit (°F)\n\n#### Time conversion\n\n(hours, minutes, seconds, days, weeks)\n36368 seconds equals to 10 hours, 6 minutes, 8 seconds\n36368 minutes equals to 3 weeks, 4 days, 6 hours, 8 minutes\n\n### Codes and images of the number 36368\n\nNumber 36368 morse code: ...-- -.... ...-- -.... ---..\nSign language for number 36368:", null, "", null, "", null, "", null, "", null, "Number 36368 in braille:", null, "Images of the number\nImage (1) of the numberImage (2) of the number", null, "", null, "More images, other sizes, codes and colors ...\n\n#### Number 36368 infographic", null, "## Share in social networks", null, "## Mathematics of no. 36368\n\n### Multiplications\n\n#### Multiplication table of 36368\n\n36368 multiplied by two equals 72736 (36368 x 2 = 72736).\n36368 multiplied by three equals 109104 (36368 x 3 = 109104).\n36368 multiplied by four equals 145472 (36368 x 4 = 145472).\n36368 multiplied by five equals 181840 (36368 x 5 = 181840).\n36368 multiplied by six equals 218208 (36368 x 6 = 218208).\n36368 multiplied by seven equals 254576 (36368 x 7 = 254576).\n36368 multiplied by eight equals 290944 (36368 x 8 = 290944).\n36368 multiplied by nine equals 327312 (36368 x 9 = 327312).\nshow multiplications by 6, 7, 8, 9 ...\n\n### Fractions: decimal fraction and common fraction\n\n#### Fraction table of 36368\n\nHalf of 36368 is 18184 (36368 / 2 = 18184).\nOne third of 36368 is 12122,6667 (36368 / 3 = 12122,6667 = 12122 2/3).\nOne quarter of 36368 is 9092 (36368 / 4 = 9092).\nOne fifth of 36368 is 7273,6 (36368 / 5 = 7273,6 = 7273 3/5).\nOne sixth of 36368 is 6061,3333 (36368 / 6 = 6061,3333 = 6061 1/3).\nOne seventh of 36368 is 5195,4286 (36368 / 7 = 5195,4286 = 5195 3/7).\nOne eighth of 36368 is 4546 (36368 / 8 = 4546).\nOne ninth of 36368 is 4040,8889 (36368 / 9 = 4040,8889 = 4040 8/9).\nshow fractions by 6, 7, 8, 9 ...\n\n### Calculator\n\n 36368\n\n#### Is Prime?\n\nThe number 36368 is not a prime number. The closest prime numbers are 36353, 36373.\n\n#### Factorization and factors (dividers)\n\nThe prime factors of 36368 are 2 * 2 * 2 * 2 * 2273\nThe factors of 36368 are 1 , 2 , 4 , 8 , 16 , 2273 , 4546 , 9092 , 18184 , 36368\nTotal factors 10.\nSum of factors 70494 (34126).\n\n#### Powers\n\nThe second power of 363682 is 1.322.631.424.\nThe third power of 363683 is 48.101.459.628.032.\n\n#### Roots\n\nThe square root √36368 is 190,703959.\nThe cube root of 336368 is 33,131401.\n\n#### Logarithms\n\nThe natural logarithm of No. ln 36368 = loge 36368 = 10,501445.\nThe logarithm to base 10 of No. log10 36368 = 4,560719.\nThe Napierian logarithm of No. log1/e 36368 = -10,501445.\n\n### Trigonometric functions\n\nThe cosine of 36368 is 0,603078.\nThe sine of 36368 is 0,797682.\nThe tangent of 36368 is 1,322685.\n\n### Properties of the number 36368\n\nIs a Friedman number: No\nIs a Fibonacci number: No\nIs a Bell number: No\nIs a palindromic number: No\nIs a pentagonal number: No\nIs a perfect number: No\n\n## Number 36368 in Computer Science\n\nCode typeCode value\n36368 Number of bytes35.5KB\nUnix timeUnix time 36368 is equal to Thursday Jan. 1, 1970, 10:06:08 a.m. GMT\nIPv4, IPv6Number 36368 internet address in dotted format v4 0.0.142.16, v6 ::8e10\n36368 Decimal = 1000111000010000 Binary\n36368 Decimal = 1211212222 Ternary\n36368 Decimal = 107020 Octal\n36368 Decimal = 8E10 Hexadecimal (0x8e10 hex)\n36368 BASE64MzYzNjg=\n36368 MD5e60af3c102de8282382170efa4972471\n36368 SHA1b18fae2c5b80cbb9166979e9291170a91810486a\n36368 SHA224f91354585218076a29cb628e08af020f732097d8b4e674dcfc85b1c7\n36368 SHA2567f67a5f99444c06499cfd205c1d251d1a92fb701c16f16c86d8c530d79939644\n36368 SHA384a1468a17b66ca76abc99b02cb87abd2f0f4bd49a978b3b75a16370a5cc70a5b20351f9f404d90af323c9d8075a8249bd\nMore SHA codes related to the number 36368 ...\n\nIf you know something interesting about the 36368 number that you did not find on this page, do not hesitate to write us here.\n\n## Numerology 36368\n\n### Character frequency in number 36368\n\nCharacter (importance) frequency for numerology.\n Character: Frequency: 3 2 6 2 8 1\n\n### Classical numerology\n\nAccording to classical numerology, to know what each number means, you have to reduce it to a single figure, with the number 36368, the numbers 3+6+3+6+8 = 2+6 = 8 are added and the meaning of the number 8 is sought.\n\n## Interesting facts about the number 36368\n\n### Asteroids\n\n• (36368) 2000 OG12 is asteroid number 36368. It was discovered by LINEAR, Lincoln Near-Earth Asteroid Research from Lincoln Laboratory, Socorro on 7/23/2000.\n\n## Number 36,368 in other languages\n\nHow to say or write the number thirty-six thousand, three hundred and sixty-eight in Spanish, German, French and other languages. The character used as the thousands separator.\n Spanish: 🔊 (número 36.368) treinta y seis mil trescientos sesenta y ocho German: 🔊 (Anzahl 36.368) sechsunddreißigtausenddreihundertachtundsechzig French: 🔊 (nombre 36 368) trente-six mille trois cent soixante-huit Portuguese: 🔊 (número 36 368) trinta e seis mil, trezentos e sessenta e oito Chinese: 🔊 (数 36 368) 三万六千三百六十八 Arabian: 🔊 (عدد 36,368) ستة و ثلاثون ألفاً و ثلاثمائةثمانية و ستون Czech: 🔊 (číslo 36 368) třicet šest tisíc třista šedesát osm Korean: 🔊 (번호 36,368) 삼만 육천삼백육십팔 Danish: 🔊 (nummer 36 368) seksogtredivetusinde og trehundrede og otteogtreds Dutch: 🔊 (nummer 36 368) zesendertigduizenddriehonderdachtenzestig Japanese: 🔊 (数 36,368) 三万六千三百六十八 Indonesian: 🔊 (jumlah 36.368) tiga puluh enam ribu tiga ratus enam puluh delapan Italian: 🔊 (numero 36 368) trentaseimilatrecentosessantotto Norwegian: 🔊 (nummer 36 368) tretti-seks tusen, tre hundre og seksti-åtte Polish: 🔊 (liczba 36 368) trzydzieści sześć tysięcy trzysta sześćdziesiąt osiem Russian: 🔊 (номер 36 368) тридцать шесть тысяч триста шестьдесят восемь Turkish: 🔊 (numara 36,368) otuzaltıbinüçyüzaltmışsekiz Thai: 🔊 (จำนวน 36 368) สามหมื่นหกพันสามร้อยหกสิบแปด Ukrainian: 🔊 (номер 36 368) тридцять шiсть тисяч триста шiстдесят вiсiм Vietnamese: 🔊 (con số 36.368) ba mươi sáu nghìn ba trăm sáu mươi tám Other languages ...\n\n## News to email\n\nPrivacy Policy.\n\n## Comment\n\nIf you know something interesting about the number 36368 or any natural number (positive integer) please write us here or on facebook." ]
[ null, "https://numero.wiki/s/senas/lenguaje-de-senas-numero-3.png", null, "https://numero.wiki/s/senas/lenguaje-de-senas-numero-6.png", null, "https://numero.wiki/s/senas/lenguaje-de-senas-numero-3.png", null, "https://numero.wiki/s/senas/lenguaje-de-senas-numero-6.png", null, "https://numero.wiki/s/senas/lenguaje-de-senas-numero-8.png", null, "https://number.academy/img/braille-36368.svg", null, "https://numero.wiki/img/a-36368.jpg", null, "https://numero.wiki/img/b-36368.jpg", null, "https://number.academy/i/infographics/8/number-36368-infographic.png", null, "https://numero.wiki/s/share-desktop.png", null ]
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https://www.colorhexa.com/0354e7
[ "# #0354e7 Color Information\n\nIn a RGB color space, hex #0354e7 is composed of 1.2% red, 32.9% green and 90.6% blue. Whereas in a CMYK color space, it is composed of 98.7% cyan, 63.6% magenta, 0% yellow and 9.4% black. It has a hue angle of 218.7 degrees, a saturation of 97.4% and a lightness of 45.9%. #0354e7 color hex could be obtained by blending #06a8ff with #0000cf. Closest websafe color is: #0066ff.\n\n• R 1\n• G 33\n• B 91\nRGB color chart\n• C 99\n• M 64\n• Y 0\n• K 9\nCMYK color chart\n\n#0354e7 color description : Vivid blue.\n\n# #0354e7 Color Conversion\n\nThe hexadecimal color #0354e7 has RGB values of R:3, G:84, B:231 and CMYK values of C:0.99, M:0.64, Y:0, K:0.09. Its decimal value is 218343.\n\nHex triplet RGB Decimal 0354e7 `#0354e7` 3, 84, 231 `rgb(3,84,231)` 1.2, 32.9, 90.6 `rgb(1.2%,32.9%,90.6%)` 99, 64, 0, 9 218.7°, 97.4, 45.9 `hsl(218.7,97.4%,45.9%)` 218.7°, 98.7, 90.6 0066ff `#0066ff`\nCIE-LAB 41.419, 37.648, -79.195 17.629, 12.128, 77.009 0.165, 0.114, 12.128 41.419, 87.688, 295.426 41.419, -18.346, -115.676 34.825, 29.413, -106.729 00000011, 01010100, 11100111\n\n# Color Schemes with #0354e7\n\n• #0354e7\n``#0354e7` `rgb(3,84,231)``\n• #e79603\n``#e79603` `rgb(231,150,3)``\nComplementary Color\n• #03c6e7\n``#03c6e7` `rgb(3,198,231)``\n• #0354e7\n``#0354e7` `rgb(3,84,231)``\n• #2403e7\n``#2403e7` `rgb(36,3,231)``\nAnalogous Color\n• #c6e703\n``#c6e703` `rgb(198,231,3)``\n• #0354e7\n``#0354e7` `rgb(3,84,231)``\n• #e72403\n``#e72403` `rgb(231,36,3)``\nSplit Complementary Color\n• #54e703\n``#54e703` `rgb(84,231,3)``\n• #0354e7\n``#0354e7` `rgb(3,84,231)``\n• #e70354\n``#e70354` `rgb(231,3,84)``\n• #03e796\n``#03e796` `rgb(3,231,150)``\n• #0354e7\n``#0354e7` `rgb(3,84,231)``\n• #e70354\n``#e70354` `rgb(231,3,84)``\n• #e79603\n``#e79603` `rgb(231,150,3)``\n• #02399b\n``#02399b` `rgb(2,57,155)``\n• #0242b5\n``#0242b5` `rgb(2,66,181)``\n• #034bce\n``#034bce` `rgb(3,75,206)``\n• #0354e7\n``#0354e7` `rgb(3,84,231)``\n• #085efc\n``#085efc` `rgb(8,94,252)``\n• #216ffc\n``#216ffc` `rgb(33,111,252)``\n• #3a7ffc\n``#3a7ffc` `rgb(58,127,252)``\nMonochromatic Color\n\n# Alternatives to #0354e7\n\nBelow, you can see some colors close to #0354e7. Having a set of related colors can be useful if you need an inspirational alternative to your original color choice.\n\n• #038de7\n``#038de7` `rgb(3,141,231)``\n• #037ae7\n``#037ae7` `rgb(3,122,231)``\n• #0367e7\n``#0367e7` `rgb(3,103,231)``\n• #0354e7\n``#0354e7` `rgb(3,84,231)``\n• #0341e7\n``#0341e7` `rgb(3,65,231)``\n• #032ee7\n``#032ee7` `rgb(3,46,231)``\n• #031be7\n``#031be7` `rgb(3,27,231)``\nSimilar Colors\n\n# #0354e7 Preview\n\nText with hexadecimal color #0354e7\n\nThis text has a font color of #0354e7.\n\n``<span style=\"color:#0354e7;\">Text here</span>``\n#0354e7 background color\n\nThis paragraph has a background color of #0354e7.\n\n``<p style=\"background-color:#0354e7;\">Content here</p>``\n#0354e7 border color\n\nThis element has a border color of #0354e7.\n\n``<div style=\"border:1px solid #0354e7;\">Content here</div>``\nCSS codes\n``.text {color:#0354e7;}``\n``.background {background-color:#0354e7;}``\n``.border {border:1px solid #0354e7;}``\n\n# Shades and Tints of #0354e7\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, #000712 is the darkest color, while #fefeff is the lightest one.\n\n• #000712\n``#000712` `rgb(0,7,18)``\n• #000e25\n``#000e25` `rgb(0,14,37)``\n• #011539\n``#011539` `rgb(1,21,57)``\n• #011c4c\n``#011c4c` `rgb(1,28,76)``\n• #01235f\n``#01235f` `rgb(1,35,95)``\n• #012a73\n``#012a73` `rgb(1,42,115)``\n• #023186\n``#023186` `rgb(2,49,134)``\n• #02389a\n``#02389a` `rgb(2,56,154)``\n``#023fad` `rgb(2,63,173)``\n• #0246c0\n``#0246c0` `rgb(2,70,192)``\n• #034dd4\n``#034dd4` `rgb(3,77,212)``\n• #0354e7\n``#0354e7` `rgb(3,84,231)``\n• #035bfa\n``#035bfa` `rgb(3,91,250)``\n• #1567fc\n``#1567fc` `rgb(21,103,252)``\n• #2974fc\n``#2974fc` `rgb(41,116,252)``\n• #3c80fc\n``#3c80fc` `rgb(60,128,252)``\n• #4f8dfd\n``#4f8dfd` `rgb(79,141,253)``\n• #639afd\n``#639afd` `rgb(99,154,253)``\n• #76a6fd\n``#76a6fd` `rgb(118,166,253)``\n• #89b3fd\n``#89b3fd` `rgb(137,179,253)``\n• #9dbffe\n``#9dbffe` `rgb(157,191,254)``\n• #b0ccfe\n``#b0ccfe` `rgb(176,204,254)``\n• #c4d8fe\n``#c4d8fe` `rgb(196,216,254)``\n• #d7e5fe\n``#d7e5fe` `rgb(215,229,254)``\n• #eaf2ff\n``#eaf2ff` `rgb(234,242,255)``\n• #fefeff\n``#fefeff` `rgb(254,254,255)``\nTint Color Variation\n\n# Tones of #0354e7\n\nA tone is produced by adding gray to any pure hue. In this case, #6f737b is the less saturated color, while #0354e7 is the most saturated one.\n\n• #6f737b\n``#6f737b` `rgb(111,115,123)``\n• #667184\n``#667184` `rgb(102,113,132)``\n• #5d6e8d\n``#5d6e8d` `rgb(93,110,141)``\n• #546b96\n``#546b96` `rgb(84,107,150)``\n• #4b699f\n``#4b699f` `rgb(75,105,159)``\n• #4266a8\n``#4266a8` `rgb(66,102,168)``\n• #3964b1\n``#3964b1` `rgb(57,100,177)``\n• #3061ba\n``#3061ba` `rgb(48,97,186)``\n• #275ec3\n``#275ec3` `rgb(39,94,195)``\n• #1e5ccc\n``#1e5ccc` `rgb(30,92,204)``\n• #1559d5\n``#1559d5` `rgb(21,89,213)``\n• #0c57de\n``#0c57de` `rgb(12,87,222)``\n• #0354e7\n``#0354e7` `rgb(3,84,231)``\nTone Color Variation\n\n# Color Blindness Simulator\n\nBelow, you can see how #0354e7 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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https://stats.stackexchange.com/questions/30002/mad-equivalent-for-standard-error
[ "# MAD equivalent for standard error\n\nAs far as I know, one can calculate the relative standard error from the standard deviation of a data sample. I am looking for the Median Absolute Deviation equivalent for standard error.\n\nDoes one exist? Also which methods exist to calculate the relative standard error, that do not require the standard deviation?\n\n• What properties do you want of a \"standard error\" (of the mean, presumably) that is a \"MAD equivalent\"? – whuber Jun 7 '12 at 16:53\n• What do you mean by equivalent? Are you looking for a formula that applies generally for distributions that relates MAD to se? – Michael R. Chernick Jun 7 '12 at 16:54\n• The goal is to find the statistical significance of a certain metric. Lots of data is involved, so best to come up with an efficient method. I started looking into MAD, because of possible outliers due to data problems ... – Navi Jun 7 '12 at 20:25\n\nWhen you say standard error, you should be talking about the standard error of something, such as the standard error of the sample mean.\n\nSimilarly you could for example talk about the median absolute deviation of the sample median. It is possible to calculate this, at least as an approximation for large samples.\n\nIt is well known that for a continuous random variable with population median $m$, continuous probability density of the median $f(m)$ and a large odd sample size $n$, the sample median is approximately normally distributed with median $m$ and variance $\\frac{1}{4 n f(m)^2}$, i.e. with median absolute deviation approximately $\\dfrac{\\Phi^{-1}\\left(\\frac34 \\right)}{2 \\sqrt{n} f(m)}$ where $\\frac{\\Phi^{-1}\\left(\\frac34 \\right)}{2} \\approx 0.337$.\n\nIf you want to have this as a relative median absolute deviation of the sample median, then presumably you divide by $m$.\n\n• Did you notice that \"MAD\" is a median absolute deviation? It is used as a robust statistic. Its utility in the role of a putative SE is something to be doubted because it does not enjoy the asymptotic properties of a standard error, nor does it have a comparable interpretation. – whuber Jun 7 '12 at 20:04\n• @whuber: I had typed mean absolute deviation when I meant median absolute deviation. The median absolute deviation of the sample median has the asymptotic property of being roughly proportional to $\\frac{1}{\\sqrt{n}}$, similar to the standard error of the sample mean. – Henry Jun 8 '12 at 6:22\n• @whuber: For large samples the absolute difference between the population median and the sample median has a roughly 95% chance of being less than 2.906 times the expression I gave, similar to the 1.96 property of the standard error. – Henry Jun 8 '12 at 6:30\n• @whuber: though I accept the point that the median absolute deviation of the sample median depends on the underlying population distribution near the median, and this may not be so immediately easy to estimate from the sample. – Henry Jun 8 '12 at 8:17\n• Thanks for the extended analysis--clear and to the point. (+1) – whuber Jun 8 '12 at 12:29\n\nAn alternative approach is to look at the quantiles of the the sample: order the observations so $x_1 \\le x_2 \\le x_3 \\le \\cdots \\le x_n$ and (for reasonably large samples from a continuous distribution) there is a 95% probability that the interval $$\\left[x_{\\frac{n}{2} - 0.98 \\sqrt{n}}, x_{\\frac{n}{2} + 0.98 \\sqrt{n}}\\right]$$ contains the population median.\n\nClearly ${\\frac{n}{2} \\pm 0.98 \\sqrt{n}}$ may not be an integer: you can round outwards to be conservative or use one of the many possibilities for interpolating quantiles: you are now looking for $Q_p$ where $p = {\\frac{1}{2} \\pm 0.98 /\\sqrt{n}}$.\n\nAgain for relative, you can divide by the median." ]
[ null ]
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https://web2.0calc.com/questions/algebra_25180
[ "+0\n\n# Algebra\n\n0\n232\n1\n\n(a) Let f : R -> R be defined by f(x) = x^2.  Show that f(x) has no inverse function.\n\n(b) Let g : (0,inf) -> R be defined by g(x) = x^2.  Show that g(x) has an inverse function.\n\nJun 18, 2021\n\n#1\n+2\n\nA function does not have an inverse function when 2 different x values can produce the same y value.\n\nf(-3) = 9\n\nf(3) = 9\n\nSo if we were to inverse it, f(9) could be 3 or -3, making it not a function.\n\nThink about why g(x) has an inverese.\n\nCan 2 different x in the domain produce the same y?\n\n=^._.^=\n\nJun 18, 2021" ]
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https://www.tutorialsteacher.com/python/getattr-method
[ "# Python getattr() Method\n\nThe `getattr()` method returns the value of the attribute of an object. If the named attribute does not exist, default is returned if provided, otherwise `AttributeError` is raised.\n\n### Syntax:\n\n``getattr(object, name, default)``\n\n#### Parameters:\n\n1. object: An object of the class whose attribute value needs to be returned.\n2. name: The string name of the attribute.\n3. default. (Optional) A value to be returned if the attribute is not found.\n\n#### Return Value:\n\n• Returns value of the attribute of the given object.\n• If the default value not specified, then throws `AttributeError`.\n\nThe following example demonstrates the `getattr()` method.\n\nExample: getattr()\n``````class student:\nname = 'John'\nage = 18\n\nstd = student() # creating object\n\nprint('student name is ', getattr(std, 'name'))\n\nstd.name = 'Bill' # updating value\nprint('student name changed to ', getattr(std, 'name'))\n``````\nOutput\n``````student name is John\nstudent name changed to Bill\n``````\n\nAbove, `getattr(std, 'name')` returns the value of the `name` property of the `std` object, which is `John`. It always returns the latest value even after updating a property value.\n\nIf the attribute specified in the argument is not found, an `AttributeError` exception is thrown.\n\nExample: getattr()\n``````class student:\nname = 'John'\nage = '18'\n\nstd = student()\nattr = getattr(std, 'subject')\n``````\nOutput\n``````Traceback (most recent call last):\nattr = getattr(std, 'subject')\nAttributeError: type object 'student' has no attribute 'subject'\n``````\n\nThe default parameter can be passed to avoid the above error, which returns the default value if the attribute is not found.\n\nExample: getattr()\n``````class student:\nname = 'John'\nage = '18'\n\nstd = student()\nsubject = getattr(std, 'subject', 'Not supported')\nprint(\"student's subject: \", subject)\n``````\nOutput\n``````student's subject: Not supported\n``````\n\nInstead of `getattr()` method, the `.` operator can also be used to access the attribute value if you are sure that an object has that attribute.\n\nExample: getattr()\n``````class student:\nname = 'John'\nage = '18'\n\nstd = student()\nprint('student name is ', std.name)\n``````\nOutput\n``````student name is John\n``````\n\nThe following get's the method of the built-in list object.\n\nExample: getattr()\n``````nums= [1, 2, 3, 4, 5]\nrev = getattr(nums, 'reverse')\nrev()\nprint(nums)\n``````\nOutput\n``````[5, 4, 3, 2, 1]\n``````\nWant to check how much you know Python?" ]
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https://convertoctopus.com/601-cubic-centimeters-to-tablespoons
[ "## Conversion formula\n\nThe conversion factor from cubic centimeters to tablespoons is 0.06762804511761, which means that 1 cubic centimeter is equal to 0.06762804511761 tablespoons:\n\n1 cm3 = 0.06762804511761 tbsp\n\nTo convert 601 cubic centimeters into tablespoons we have to multiply 601 by the conversion factor in order to get the volume amount from cubic centimeters to tablespoons. We can also form a simple proportion to calculate the result:\n\n1 cm3 → 0.06762804511761 tbsp\n\n601 cm3 → V(tbsp)\n\nSolve the above proportion to obtain the volume V in tablespoons:\n\nV(tbsp) = 601 cm3 × 0.06762804511761 tbsp\n\nV(tbsp) = 40.644455115684 tbsp\n\nThe final result is:\n\n601 cm3 → 40.644455115684 tbsp\n\nWe conclude that 601 cubic centimeters is equivalent to 40.644455115684 tablespoons:\n\n601 cubic centimeters = 40.644455115684 tablespoons\n\n## Alternative conversion\n\nWe can also convert by utilizing the inverse value of the conversion factor. In this case 1 tablespoon is equal to 0.024603602069551 × 601 cubic centimeters.\n\nAnother way is saying that 601 cubic centimeters is equal to 1 ÷ 0.024603602069551 tablespoons.\n\n## Approximate result\n\nFor practical purposes we can round our final result to an approximate numerical value. We can say that six hundred one cubic centimeters is approximately forty point six four four tablespoons:\n\n601 cm3 ≅ 40.644 tbsp\n\nAn alternative is also that one tablespoon is approximately zero point zero two five times six hundred one cubic centimeters.\n\n## Conversion table\n\n### cubic centimeters to tablespoons chart\n\nFor quick reference purposes, below is the conversion table you can use to convert from cubic centimeters to tablespoons\n\ncubic centimeters (cm3) tablespoons (tbsp)\n602 cubic centimeters 40.712 tablespoons\n603 cubic centimeters 40.78 tablespoons\n604 cubic centimeters 40.847 tablespoons\n605 cubic centimeters 40.915 tablespoons\n606 cubic centimeters 40.983 tablespoons\n607 cubic centimeters 41.05 tablespoons\n608 cubic centimeters 41.118 tablespoons\n609 cubic centimeters 41.185 tablespoons\n610 cubic centimeters 41.253 tablespoons\n611 cubic centimeters 41.321 tablespoons" ]
[ null ]
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https://hal.archives-ouvertes.fr/hal-01735374
[ "# Surface derivatives computation using Fourier Transform\n\n1 GeoMod - Modélisation Géométrique, Géométrie Algorithmique, Fractales\nLIRIS - Laboratoire d'InfoRmatique en Image et Systèmes d'information\nAbstract : We present a method for computing high order derivatives on a smooth surface S at a point p by analyzing the vibrations of the surface along circles in the tangent plane, centered at p. By computing the Discrete Fourier Transform of the deviation of S from the tangent plane restricted to those circles, a linear relation between the Fourier coefficients and the derivatives can be expressed. Thus, given a smooth scalar field defined on the surface, all its derivatives at p can be computed simultaneously. The originality of this method is that no direct derivation process is applied to the data. Instead, integration is performed through the Discrete Fourier Transform, and the result is expressed as a one dimensional polynomial. We derive two applications of our framework namely normal correction and curvature estimation which we demonstrate on synthetic and real data.\nDocument type :\nConference papers\nDomain :\n\nCited literature [10 references]\n\nhttps://hal.archives-ouvertes.fr/hal-01735374\nContributor : Julie Digne <>\nSubmitted on : Friday, March 16, 2018 - 1:57:18 PM\nLast modification on : Saturday, February 29, 2020 - 1:34:43 AM\nDocument(s) archivé(s) le : Monday, September 10, 2018 - 9:31:23 PM\n\n### File\n\nafig_2016.pdf\nFiles produced by the author(s)\n\n### Identifiers\n\n• HAL Id : hal-01735374, version 1\n\n### Citation\n\nYohann Béarzi, Julie Digne. Surface derivatives computation using Fourier Transform. JFIG 2016, Nov 2016, Grenoble, France. ⟨hal-01735374⟩\n\nRecord views" ]
[ null ]
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http://wikip.com/sotaychame.com/duoi-3-tuoi/
[ "## (605) 682-3465\n\nFasttrees provides a Fast-and-Frugal Tree classifier for Python.\n\nFast-and-frugal trees are classification trees that are especially useful for making decisions under uncertainty.\nDue their simplicity and transparency they are very robust against noise and errors in data.\nThey are one of the heuristics proposed by Gerd Gigerenzer in 4807866776. This particular implementation is based on on the R package 8333675197, developed by Phillips, Neth, Woike and Grassmaier.\n\nFirst, let’s install it. This can be done from the command line using pip:\n\n``````pip install fasttrees\n``````\n\nOnce it’s installed, let’s import the Fast-and-Frugal Tree classifier.\n\n``````from fasttrees.fasttrees import FastFrugalTreeClassifier\n``````\n\nNow let’s get some data to fit our classifier to. Fast-and-Frugal Trees tend to do well on real-world data prone to (human) error, as they disregard information that doesn’t seem very predictive of the outcome. A typical use case is in an operational setting where humans quickly have to take decisions. You could then fit a fast-and-frugal tree to the data in advance, and use the simple resulting tree to quickly make decisions.\n\nAs an example of this, let’s have a look at credit decisions. UCI provides a credit approval dataset. Download the `crx.data` file from the data folder.\n\nLet’s load the data as CSV to a Pandas dataframe:\n\n``````import pandas as pd\n``````\n\nAs there is no header, the columns are simply numbered 1, 2, 3 etc. Let’s make clear they’re attributes by naming them A1, A2, A3 etc.\n\n``````data.columns = ['A{}'.format(nr) for nr in data.columns]\n``````\n\nThe fasttrees implementation of fast-and-frugal trees can only work with categorical and numerical columns, so let’s assign the appropriate dtype to each column:\n\n``````import numpy as np\n\ncat_columns = ['A0', 'A3', 'A4', 'A5', 'A6', 'A8', 'A9', 'A11', 'A12']\nnr_columns = ['A1', 'A2', 'A7', 'A10', 'A13', 'A14']\n\nfor col in cat_columns:\ndata[col] = data[col].astype('category')\n\nfor col in nr_columns:\n# only recast columns that have not been correctly inferred\nif data[col].dtype != 'float' and data[col].dtype != 'int':\n# change the '?' placeholder to a nan\ndata.loc[data[col] == '?', col] = np.nan\ndata[col] = data[col].astype('float')\n``````\n\nThe last column is the variable we want to predict, the credit decision. It’s denoted by `+` or `-`. For our FastFrugalTreeClassifier to work we need to convert this to boolean:\n\n``````data['A15'] = data['A15'].apply(lambda x: True if x=='+' else False).astype(bool)\n``````\n\nYour data should now look something like this:\n\nA0 A1 A2 A3 A4 A5 A6 A7 A8 A9 A10 A11 A12 A13 A14 A15\n0 b 30.83 0 u g w v 1.25 t t 1 f g 202 0 True\n1 a 58.67 4.46 u g q h 3.04 t t 6 f g 43 560 True\n2 a 24.5 0.5 u g q h 1.5 t f 0 f g 280 824 True\n3 b 27.83 1.54 u g w v 3.75 t t 5 t g 100 3 True\n4 b 20.17 5.625 u g w v 1.71 t f 0 f s 120 0 True\n\nNow let’s do a train test split (we use two thirds of the data to train on):\n\n``````from sklearn.model_selection import train_test_split\n\nX_train, X_test, y_train, y_test = train_test_split(data.drop(columns='A15'), data['A15'], test_size=0.33, random_state=0)\n``````\n\nWe can now finally instantiate our fast-and-frugal tree classifier. Let’s use the default parameters:\n\n``````fc = FastFrugalTreeClassifier()\n``````\n\nLet’s fit the classifier to our training data (this can take a few seconds):\n\n``````fc.fit(X_train, y_train)\n``````\n\nWe can take a look at the resulting tree, which can be used for decision making:\n\n``````fc.get_tree()\n``````\nIF NO feature direction threshold IF YES\n0 decide NO A8 in (‘t’,) ↓\n1 ↓ A10 > 1 decide YES\n2 ↓ A9 in (‘t’,) decide YES\n3 decide NO A7 > 1.25 decide YES\n\nNow somebody making a decision can simply look at the 3 central columns, which read, for example `A8 in ('t',)` and have a look whether this is the case. If it isn’t, they take the action in `IF NO`, which would be to decide NO (in this case that would mean not to grant this specific person a credit). If it is, they take the action in `IF YES`, which is to look at the next feature, for which they then repeat the process.\n\nHow well does this simple tree classifier perform? Let’s score it against the test data. By default the balanced accuracy score is used:\n\n``````fc.score(X_test, y_test)\n``````\n\nThis returns a balanced accuracy of 0.86, pretty good!\n\nWe can also have a look at how much information it actually used to make its decisions:\n\n``````fc.get_tree(decision_view=False)\n``````\nfeature direction threshold type balanced_accuracy_score fraction_used exit\n0 A8 in (‘t’,) categorical 0.852438 1 0\n1 A10 > 1 numerical 0.852438 0.528139 1\n2 A9 in (‘t’,) categorical 0.852438 0.238095 1\n3 A7 > 1.25 numerical 0.852438 0.192641 0.5\n\nWhile the first cue is used for all decisions, the second is only used for 52% of all decisions. This means that 48% of decisions could be made by just looking at one single feature.\n\nHence, fast and frugal trees provide a very easy way to generate simple decision criteria from a large dataset, which often perform better than more advanced machine learning algorithms, and are much more transparent." ]
[ null ]
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https://socratic.org/questions/5862800eb72cff63940728e3
[ "# Question #728e3\n\nJan 2, 2017\n\nAlkali earth metals have a valance configuration of ${s}^{2}$\nHalogens have a valance configuration of ${s}^{2} {p}^{5}$\nBoth families of elements are chemically active.\n\n#### Explanation:\n\nAlkali Earth metals with a valance configuration of ${s}^{2}$ can most easily become stable by sharing these valance electrons with an element that is electrophilic. This leaves the Alkali Earth metals with the outside valance electron structure of a noble gas of the next lower electron shell.\n\nHalogens with a valance configuration of ${s}^{2} {p}^{5}$ can most easily become stable by acquiring an electron from another element. This leaves the Halogens with the outside valance electron structure of a noble gas in the same period.\n\nBoth of these families of elements are very active chemically.\n\nJan 25, 2017\n\nHere's what I get.\n\n#### Explanation:\n\n$\\boldsymbol{\\text{Alkaline Earth\"color(white)(ml)\"Halogen}}$\n${\\text{Be\"color(white)(m)[\"He\"] \"2s\"^2color(white)(mmmm)\"F\"color(white)(m)[\"He\"] \"2s\"^2 \"2p}}^{5}$\n${\\text{Mg\"color(white)(ll)[\"Ne\"] \"3s\"^2color(white)(m)color(white)(mmm)\"Cl\"color(white)(ll)[\"Ne\"] \"3s\"^2 \"3p}}^{5}$\n\n${\\text{Ca\"color(white)(m)[\"Ar\"] \"4s\"^2color(white)(m)color(white)(mmm)\"Br\"color(white)(ll)[\"Ar\"]\"4s\"^2 \"3d\"^10 \"4p}}^{5}$\n${\\text{Sr\"color(white)(ml)[\"Kr\"] \"5s\"^2color(white)(m)color(white)(mmm)\"I\"color(white)(ml)[\"Kr\"] \"5s\"^2 \"4d\"^10 \"5p}}^{5}$\n\n${\\text{Ba\"color(white)(m)[\"Xe\"] \"6s\"^2color(white)(m)color(white)(mmm)\"At\"color(white)(ll)[\"Xe\"]\"6s\"^2 \"4f\"^14 \"5d\"^10 \"6p}}^{5}$\n${\\text{Ra\"color(white)(m)[\"Rn\"] \"7s\"^2color(white)(m)color(white)(mmll)\"Ts\"color(white)(m)[\"Rn\"] \"7s\"^2 \"5f\"^14 \"6d\"^10 \"7p}}^{5}$\n\nThe alkaline earth metals have a electron configuration ending in $n {\\text{s}}^{2}$.\n\nThey can get a noble gas configuration by losing their two $\\text{s}$ electrons.\n\nThe halogens have an electron configuration ending in $n {\\text{s\"^2 n\"p}}^{5}$.\n\nThey can get a noble gas configuration by gaining one electron to complete their octet.\n\nThus, an alkali metal $\\text{M}$ will react by donating an electron to each of two halogen $\\text{X}$ atoms.\n\nThe metal will become a metal cation $\\text{M\"^\"2+}$ and the halogen will become an anion $\\text{X\"^\"-}$.\n\n$\\text{M + 2X\" → \"M\"^\"2+\", \"2X\"^\"-}$" ]
[ null ]
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https://www.nature.com/articles/s41598-018-34443-2?error=cookies_not_supported
[ "## Introduction\n\nDevelopment of method for determining crystal and magnetic structure is an important issue1,2,3. The magnetic structure of a compound is directly related to the microscopic origins of various intriguing magnetic phenomena observed in physics, chemistry, biology and geology4,5,6,7,8,9,10,11. Accurate information on the experimentally determined magnetic structures can be potentially used to effectively design functional materials and opens multiple opportunities for utilizing advanced first-principle calculations and informatics approaches. Furthermore, the responses of the analysed magnetic structure to external factors such as temperature, pressure, electromagnetic field, light and environment are usually related to the corresponding changes in the macroscopic properties of minerals and biomolecules.\n\nSince the pioneering work of Shull et al. published in 19511, many studies on the determination of the magnetic structures of various materials by neutron diffraction have been performed. Thus, Izymov, Kovalev and Bertaut developed the irreducible representation (IR) theory, which successfully classified magnetic structures by their magnetic point symmetries obtained through the analysis of neutron diffraction data12,13,14. Moreover, the modern neutron diffractometers exhibit relatively high statistical accuracy and resolution15,16. However, analysing neutron diffraction data to determine the correct magnetic structure represents a challenging task. The major issue here is the existence of so-called local solutions to the optimization problem (Fig. 1A). The analysis procedure is mathematically categorized as the nonlinear optimization, in which the obtained diffraction data points are fitted with the function of neutron scattering cross-section characterized by high-dimensional nonlinear parameters such as magnetic moment vectors17. After performing nonlinear optimization, it is very difficult to prove that the best solution obtained via various numerical models is the global one. Furthermore, multiple or many solutions are hidden in some cases, and no solutions exist in other cases. To mitigate these issues, global optimization techniques including a simulated annealing method, the Monte Carlo method and genetic algorithms can be used18,19,20,21,22,23. However, none of these approaches can determine the global solution(s) with 100% probability.\n\nIn this study, a new analytical method for the determination of magnetic structure is proposed, which allows (i) judging whether the obtained solution is a truly global one; (ii) evaluating the uniqueness of the solution obtained for a given set of experimental data; and (iii) completing the global optimization procedure in a very short time (typically, less than several seconds). Furthermore, the applicability of the proposed method is demonstrated using polarized-neutron powder diffraction data.\n\n## Mathematical Formulation for Applications of Semidefinite Relaxation Method\n\nRelaxation techniques have been previously developed in the field of mathematical programming. In particular, semidefinite relaxation (SDR) combined with semidefinite programming (SDP) has found many applications in applied mathematics and engineering (for example, see Chapter 2.2 in ref.24). SDR is an efficient technique for solving nonlinear optimization problems, such as quadratic programs (QPs), namely the minimization of multivariate quadratic polynomials under constraints. It should be noted that SDR could provide both fast convergence and a numerical proof of the global optimality of the obtained solutions using the global convergence property and duality theorem of the convex programming methods, as schematically shown in Fig. 1(B,C).\n\nIn the field of optical imaging, Candès et al. published a pioneering work (called the PhaseLift method), in which a sparse modelling approach was adopted for general phase retrieval25. Furthermore, one of the authors (ROT) developed an SDR-based mathematical approach to investigate whether a crystal structure could be uniquely identified using only diffraction data and independent atomic model26.\n\nIn this study, this method was applied to magnetic structure analysis by replacing the optimized parameters with magnetic moments. The problem of magnetic structure determination can be mathematically described by the following set of N quadratic equations:\n\n$${I}_{{\\rm{mag}},{\\rm{obs}}}({Q}_{k})\\approx {I}_{{\\rm{mag}},{\\rm{cal}}}({Q}_{k})={{\\boldsymbol{x}}}^{{\\rm{T}}}{S}_{k}{\\boldsymbol{x}}=\\sum _{1\\le i,j\\le n}{S}_{k}(i,j){x}_{i}{x}_{j}\\,(1\\,\\le \\,k\\,\\le N),$$\n(1)\n\nwhere $${I}_{\\mathrm{mag},\\mathrm{obs}}({Q}_{k})\\,$$and $${I}_{\\mathrm{mag},\\mathrm{cal}}({Q}_{k})$$ denote the observed and calculated integrated magnetic diffraction intensities at the magnetic reflection $${Q}_{k}={h}_{{\\rm{mag}}}\\,{k}_{{\\rm{mag}}}\\,{l}_{{\\rm{mag}}}$$, respectively; x = (x1, …, xn)T and $${S}_{k}$$ represents the coefficient matrix numerically obtained using the scattering cross-section formula for each $${Q}_{k}$$, which consists of the absolute intensity scale factor, magnetic form factor, Lorentz factor, multiplicity and structural weight factor (the details of this formula are summarized in Supplementary Information).\n\nThe symbol $$\\approx$$ indicates that each $${I}_{{\\rm{mag}},{\\rm{obs}}}({Q}_{k})$$ value includes an experimental error. In order to incorporate all errors, the following optimization problem is solved:\n\n$$\\{\\begin{array}{c}{\\rm{Minimize}}\\sum _{k=1}^{N}\\frac{|{I}_{{\\rm{mag}},{\\rm{obs}}}({Q}_{k})-{{\\boldsymbol{x}}}^{{\\rm{T}}}S{\\boldsymbol{x}}|}{{\\rm{Err}}[{I}_{{\\rm{mag}},{\\rm{obs}}}({Q}_{k})]},\\\\ {\\rm{subject}}\\,{\\rm{to}}:|{x}_{i}|\\le {R}_{i}(1\\le i\\le n).\\end{array}$$\n(2)\n\nThe inequality $$|{x}_{i}|\\le {R}_{i}$$ can be also removed if the permitted range of $$|{x}_{i}|$$ ($${R}_{i}$$, for example, the upper limit of magnetic moment) is uncertain while maintaining the validity of the subsequent discussion of the SDR and SDP techniques.\n\nEquation (2) is classified as a so-called l1-norm minimization problem, which is equivalent to the following form of the quadratic programming problem:\n\n$$\\{\\begin{array}{c}{\\rm{Minimize}}\\,\\sum _{k=1}^{N}\\,\\frac{{\\eta }_{k}^{+}+{\\eta }_{k}^{-}}{2}\\\\ {\\rm{subject}}\\,{\\rm{to}}:\\frac{{I}_{{\\rm{mag}},{\\rm{obs}}}({Q}_{k})-{{\\boldsymbol{x}}}^{{\\rm{T}}}{S}_{k}{\\boldsymbol{x}}}{{\\rm{Err}}[{I}_{\\mathrm{mag},\\mathrm{obs}}({Q}_{k})]}=\\frac{{\\eta }_{k}^{+}-{\\eta }_{k}^{-}}{2}(1\\le k\\le N),\\\\ {{x}_{i}}^{2}+{y}_{i}={{R}_{i}}^{2},\\,{y}_{k}\\ge 0\\,(1\\le i\\le n),\\\\ {\\eta }_{k}^{+}\\ge 0,{\\eta }_{k}^{-}\\ge 0\\,(1\\le k\\le N).\\end{array}$$\n(3)\n\nThe problems described by equations (2) and (3) are equivalent since they have the same set of solutions x and the minimized values of the objective functions (more details are provided in Supplementary Information). The basic strategy utilized in this work is to apply SDR to equation (3) in order to solve equation (2) and then provide a computational proof on the global convergence property of the solution. The least-squares minimization of the $$\\,\\sum _{k=1}^{N}{|({I}_{\\mathrm{mag},\\mathrm{obs}}({Q}_{k})-{{\\boldsymbol{x}}}^{T}S{\\boldsymbol{x}})/{\\rm{Err}}[{I}_{\\mathrm{mag},\\mathrm{obs}}({Q}_{k})]|}^{2}$$ function is avoided because a small increase in the polynomial degree considerably magnifies the size of the SDR problem (it increases proportionally to the power of N). Thus, it is possible to locate the global optimum by performing l1-norm minimization, which can be subsequently used as the initial parameter of the normal least-squares method to calculate the refined parameters and then compare them with literature data.\n\n## Application to Experimental Data Analysis\n\n### Experimental results\n\nThe developed SDR method was verified by applying it to the experimental data obtained for pyrochlore Nd2Ir2O7, which served as a proximate material for a three-dimensional Weyl semimetal and a component of spintronic devices on the basis of its geometrically frustrated magnetism and 5d-electron configuration27,28,29,30,31,32. This state theoretically corresponds to the all-in all-out type of magnetic structure described by the magnetic propagation vector kmag = (0, 0, 0), in which all the magnetic moments are oriented either towards the centre of the participating tetrahedron or in the opposite direction30,32. This prediction was experimentally confirmed in previous unpolarized neutron diffraction studies33,34. However, the superposition of the nuclear and magnetic reflections observed for the magnetic structures with kmag = (0, 0, 0) produces ambiguous results during their separation. Furthermore, it is not possible to mathematically prove with 100% certainty the absence of other acceptable solutions to the problem of magnetic structure determination. Thus, in this work, polarized neutron diffraction studies were performed for this material, and the obtained magnetic structure was verified mathematically.\n\nFigure 2 shows the representative neutron diffraction data obtained for Nd2Ir2O7 at the minimum temperature T = 1.4 K. The non-spin-flip and spin-flip parameters IOFF and ION roughly correspond to the nuclear and magnetic reflection components Inuc and Imag, respectively. The magnitude of IOFF is systematically larger than ION at all temperatures, thus confirming the necessity of conducting polarized neutron diffraction experiments. For ION, the intensity of the 113 reflection increases with decreasing temperature, indicating the existence of strong temperature dependence for this reflection, which is not observed for the 222 reflection. Moreover, as the flipping ratio of the neutron beam in the actual experiments is finite, the magnitudes of ION and IOFF can be expressed by the following formulas:\n\n$$\\{\\begin{array}{c}{I}_{{\\rm{OFF}}}=(1-{r}_{{\\rm{mix}}}){I}_{{\\rm{nuc}}}+\\,{r}_{{\\rm{mix}}}{I}_{{\\rm{mag}}},\\,\\\\ {I}_{{\\rm{ON}}}={r}_{{\\rm{mix}}}{I}_{{\\rm{nuc}}}+\\,(1-{r}_{{\\rm{mix}}}){I}_{{\\rm{mag}}},\\,\\end{array}$$\n\nwhere rmix = N/(N+ + N) is the mixing rate, and N+ (N) denotes the number of majority-spin (minority-spin) neutrons. The value of rmix is selected to satisfy the condition Imag = 0; hence, ION = rmix·Inuc at the paramagnetic T = 40 K. As a result, the pure magnetic intensity Imag can be determined by combining IOFF and ION. A more detailed explanation and data obtained for other reflections are presented in Supplementary Information, while the calculated Imag,obs values are listed in Table 1.\n\n### Magnetic structure analysis results\n\nThe arbitrary magnetic structure with kmag = (0, 0, 0) in the space group $$Fd\\bar{3}m$$ is described as the function of xarb = (m(Nd)1, , m(Nd)12, m(Ir)1, , m(Ir)12) containing narb = 24 variables generated by the eight magnetic atoms of the unit cell and three Cartesian coordinates. Here, the magnetic symmetry was classified by performing IR analysis (this procedure is generally not required for the proposed method; however, it may be potentially useful because of the reduction of the number of variables if the number of observed reflection points is limited). The possible magnetic structures are described by the representations ΓNd = Γ3 + 2Γ5 + 3Γ7 + 6Γ9 and ΓIr = Γ3 + 2Γ5 + 3Γ7 + 6Γ9, where Γ3 corresponds to the all-in all-out type of the magnetic structure, and the coefficients denote the numbers of basis vectors summarized in Table 218,35. Hence, the total numbers of variables are reduced to nΓ3 = 2, nΓ5 = 4, nΓ7 = 6 and nΓ9 = 12. Furthermore, representation Γ9 includes six ferromagnetic basis vectors. However, the Nd2Ir2O7 structure exhibits only extremely weak spontaneous magnetization (around 10−4μB/formula unit)29, which is significantly below the detection limit of the neutron diffraction technique. Therefore, the ferromagnetic basis vectors are precluded and the value of nΓ9 is further reduced from 12 to 6 during the analysis of the neutron diffraction data.\n\nThus, the variables used for the magnetic structure analysis in this work are defined as follows: xΓ3 = (m(Γ3,Nd)1, m(Γ3,Ir)1), xΓ5 = (m(Γ5,Nd)1, m(Γ5,Nd)2, m(Γ5,Ir)1, m(Γ5,Ir)2), xΓ7 = (m(Γ7,Nd)1, m(Γ7,Nd)2, m(Γ7,Nd)3, m(Γ7,Ir)1, m(Γ7,Ir)2, m(Γ7,Ir)3) and xΓ9 = (m(Γ9,Nd)1, m(Γ9,Nd)2, m(Γ9,Nd)3, m(Γ9,Ir)1, m(Γ9,Ir)2, m(Γ9,Ir)3). The goal is to determine the globally optimal solutions x for representations Γ3, Γ5, Γ7 and Γ9 using the Imag,obs magnitudes listed in Table 1. After that, the solution characterized by the best fit can be selected.\n\nThe output values produced by the SDP solver are as follows.\n\n1. (1)\n\nThe convergence procedure results in the following coefficients:\n\n$$\\begin{array}{c}{{X}_{{\\rm{\\Gamma }}3}}^{({\\rm{opt}})}\\approx {{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}3}}^{({\\rm{opt}}1)}{{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}3}}^{({\\rm{opt}}1)T};\\\\ {{X}_{{\\rm{\\Gamma }}5}}^{({\\rm{opt}})}\\approx ({{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}5}}^{({\\rm{opt}}1)}{{x}_{{\\rm{\\Gamma }}5}}^{({\\rm{opt}}1)T}+{{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}5}}^{({\\rm{opt}}2)}{{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}5}}^{({\\rm{opt}}2)T})/2;\\\\ {{X}_{{\\rm{\\Gamma }}7}}^{({\\rm{opt}})}\\approx 0;\\\\ {{X}_{{\\rm{\\Gamma }}9}}^{({\\rm{opt}})}\\approx ({{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}9}}^{({\\rm{opt}}1)}{{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}9}}^{({\\rm{opt}}1)T}+{{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}9}}^{({\\rm{opt}}2)}{{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}9}}^{({\\rm{opt}}2)T}+{{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}9}}^{({\\rm{opt}}3)}{{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}9}}^{({\\rm{opt}}3)T})/3;\\end{array}$$\n\nand\n\n$$\\begin{array}{c}{{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}3}}^{({\\rm{opt}})}=(-\\,1.20,\\,0.19);\\\\ {{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}5}}^{({\\rm{opt}}1)}=(0.55,\\,0.,\\,0.48,\\,0.),\\,{{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}5}}^{({\\rm{opt}}2)}=(0.,\\,0.55,\\,0.,\\,0.48);\\\\ {{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}7}}^{(opt)}=(0.,\\,0.,\\,0.,\\,0.,\\,0.,\\,0.);\\\\ {{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}9}}^{({\\rm{opt}}1)}=(0.55,\\,0.,\\,0.,\\,-\\,0.52,\\,0.,\\,0.),\\,{{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}9}}^{({\\rm{opt}}2)}=(0.,\\,0.55,\\,0.,\\,0.,\\,-\\,0.52,\\,0.),\\\\ {{{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}9}}^{({\\rm{opt}}3)}=(0.,\\,0.,\\,0.55,\\,0.,\\,0.,\\,-\\,0.52);\\end{array}$$\n\nwhere the values of x are expressed the μB units, and the negative sign indicates the nearest ferromagnetic Nd–Ir correlation. While a single optimum solution is determined for representation Γ3, multiple solutions are obtained for Γ5 and Γ9, respectively, in accordance with the rank values of XΓ5(opt) and XΓ9(opt), which indicate the existence of an infinite number of solutions with the same objective functions $${{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}5}^{({\\rm{opt}})}=\\,\\cos \\,\\theta {{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}5}^{({\\rm{opt}}1)}+\\,\\sin \\,\\theta {{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}5}^{({\\rm{opt}}2)}$$ and $${{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}9}^{({\\rm{opt}})}=\\,\\cos \\,\\theta {{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}9}^{({\\rm{opt}}1)}+\\,\\sin \\,\\theta \\,\\cos \\,\\varphi {{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}9}^{({\\rm{opt}}2)}+\\,\\sin \\,\\theta \\,\\sin \\,\\varphi {{\\boldsymbol{x}}}_{{\\rm{\\Gamma }}9}^{({\\rm{opt}}3)}$$, where $$\\theta$$ and $$\\varphi$$ are arbitrary. Without SDR, it is difficult to find the optimum solutions for this type of problems and prove that better solutions do not exist. Furthermore, the zero magnitude of xΓ7(opt) is obtained for representation Γ7. Indeed, when xΓ7 values are finite (non-zero), the $${I}_{{\\rm{mag}},{\\rm{cal}}}$$ values for $${I}_{{\\rm{mag}},{\\rm{obs}}}=0$$ indices increase more rapidly than those for $${I}_{{\\rm{mag}},{\\rm{obs}}}\\ne 0$$ indices. Thus, the SDR method automatically overcomes these issues.\n\n2. (2)\n\nThe obtained indicator values for representations Γ3, Γ5, Γ7 and Γ9 are as follows.\n\n1. a)\n\nThe corresponding duality gaps determined by the SDP solver are equal to $${\\rm{\\Delta }}f=2.1\\times {10}^{-7}$$, $$1.4\\times {10}^{-6}$$, $$3.1\\times {10}^{-6}$$ and $$8.0\\times {10}^{-7}$$, respectively. Their magnitudes are close to zero, indicating that the convergence to the global optimums is achieved.\n\n2. b)\n\nThe minimized objective function $${f}^{({\\rm{gl}})}\\underline{\\underline{{\\rm{def}}}}\\,\\sum _{k=1}^{N}\\,|{I}_{{\\rm{mag}},{\\rm{obs}}}({Q}_{k})-{I}_{{\\rm{mag}},{\\rm{cal}}}({Q}_{k})|/{\\rm{Err}}[{I}_{{\\rm{mag}},{\\rm{obs}}}({Q}_{k})]$$ = 4.5, 19, 32 and 27, and the more familiar R-factor, $${R}_{{\\rm{Bragg}}}\\underline{\\underline{{\\rm{def}}}}\\,(\\sum _{k=1}^{N}|{I}_{\\mathrm{mag},\\mathrm{obs}}({Q}_{k})-{I}_{\\mathrm{mag},\\mathrm{cal}}({Q}_{k})|)/(\\sum _{k=1}^{N}\\,{I}_{\\mathrm{mag},\\mathrm{obs}}({Q}_{k}))$$ = 0.13, 0.63, 1.0 and 0.81, respectively. These results show that the smallest values are obtained for representation Γ3.\n\n3. c)\n\nThe goodness of the fit $${\\chi }^{2}\\underline{\\underline{{\\rm{def}}}}\\,(\\sum _{k=1}^{N}{|{I}_{{\\rm{mag}},{\\rm{obs}}}({Q}_{k})-{I}_{{\\rm{mag}},{\\rm{cal}}}({Q}_{k})|}^{2}\\,/\\,\\,{\\rm{Err}}{[{I}_{{\\rm{mag}},{\\rm{obs}}}({Q}_{k})]}^{2})/(N-{n}_{{\\rm{\\Gamma }}})$$ = 2.6, 14, 25 and 20, and the related statistical parameter $${f}^{({\\rm{gl}})}/(N-{n}_{{\\rm{\\Gamma }}})=0.75$$, 4.8, 16 and 14, respectively. The value closest to the expected value (1 for $${\\chi }^{2}$$; $$\\sqrt{2/\\pi }\\approx 0.798$$ for the latter parameter) is obtained for Γ3.\n\nAll these facts suggest that Γ3 represents the best solution, whereas representations Γ5, Γ7 and Γ9 are excluded for the first time. For clarity, the values of Imag,cal are listed in Table 2 and also shown in Fig. 3. The magnitude of Imag,cal-Γ3 matches Imag,obs very well, whereas the globally optimal Imag,cal-Γ5, Imag,cal-Γ7 and Imag,cal-Γ9 parameters substantially differ from the corresponding Imag,obs values.\n\nAfter proving mathematically the uniqueness of representation Γ3, the refined values mNd = −1.22(5)μB and mIr = 0.14(5)μB are obtained using the xΓ3(opt) values as the initial parameters in the normal least-squares method. These results are comparable with the reported values of mNd = −1.27(1)μB and mIr = 0.34(1)μB34.\n\n## Discussion\n\nRepresentation Γ9 (the only IR containing ferromagnetic basis vectors35) is rejected as the optimal solution despite the existence of weak ferromagnetism29. The observed inconsistency suggests that this ferromagnetism is symmetrically decoupled from the bulk magnetic structure (for example, as a surface or interface-protected property). In fact, by performing careful measurements of the macroscopic magnetization and electrical resistivity of isomorphic Cd2Os2O7, it was found that the surface ferromagnetism coupled with novel spin-polarized conductivity emerged on the walls between the all-in all-out and all-out all-in antiferromagnetic domains36. The macroscopic observation is consistent with the findings of this study verified both microscopically and mathematically, indicating their potential applicability in domain wall spin electronics.\n\nWe discuss the expected application scope of the SDR method. After determining the list of (hmag, kmag, lmag, Imag,obs) values, the described SDR method can be used to find the corresponding magnetic structures as the global solutions. First, the configurations with kmag = (0, 0, 0) are considered, indicating their high potential applicability in various fields (including magnet materials). Second, this method is not restricted to polarized neutron diffraction experiments, but can be also used in studies involving unpolarized neutrons when the magnetic structure is characterized by kmag ≠ (0, 0, 0) or kmag = (0, 0, 0) with detectable magnetic moment. Both the magnetic and crystallographic structures can be simultaneously refined by the normal least-squares method, in which the obtained SDR solutions are utilized as the initial values of the magnetic structural parameters. Third, the SDR technique is able to easily process thousands of independent variables. Therefore, magnetic structures of arbitrary types can be theoretically determined using the advanced diffractometers that provide a relatively large number of reflection points (even for the target materials with complex compositions).\n\nThe diffraction intensities are not represented by quadratic functions of the atomic positions rj; hence, the SDR technique seems to be inapplicable for determining the values of rj (crystal structure). However, the neutron and X-ray diffraction intensities are represented by those of the nuclear and electron densities (generalized crystal structure), respectively. Likewise, a magnetic structure is also generalized to the magnetic moment density. Thus, the SDR technique is expected to enable analysing the global solutions of the generalized structures together with the aforementioned high-volume processing ability, such as protonic/ionic distributions in the conductors and electronic spin-orbital distributions.\n\n## Materials and Methods\n\n### Calculations\n\nThe system of quadratic equations was solved using the SDP solver SDPA37. To find the global optima of SDP problems, interior point methods were efficiently used38.\n\n### Experiments\n\nThe polarized neutron elastic scattering experiments were performed using the HB1 thermal neutron three-axis spectrometer located at the High Flux Isotope Reactor (HFIR) of the Oak Ridge National Laboratory (ORNL). Heusler alloy 111 reflection crystals were utilized as the monochromator and analyser. The flipping ratio R = 10 was obtained using the nuclear 222 reflection at a paramagnetic temperature of 40 K corresponding to the beam polarization P = 0.82. The polarization vector was set parallel to the scattering vector (P//Q). The incident energy of neutrons was Ei = 13.5 meV. The horizontal collimator sequence was 48′(open)–80′–80′–240′. A pyrolytic graphite Bragg-reflection filter was used to efficiently eliminate the contamination caused by higher-order wavelengths.\n\nA powder Nd2Ir2O7 sample was synthesized by a solid-state reaction method inside a quartz tube. About 4.8 g of the sample was wrapped in thin aluminium foil and shaped to a hollow cylinder with a thickness of 0.8 mm and diameter of 20 mm to mitigate the effect of the strong neutron absorption of Ir nuclei. The cylinder was stored in an aluminium container filled with He gas and placed under the cold heads of a He-closed-cycle (Displex) or liquid-He-type (Orange) cryostat." ]
[ null ]
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http://mymathforum.com/calculus/343053-lnx-e-x.html
[ "Calculus Calculus Math Forum\n\n December 11th, 2017, 09:18 AM #1 Banned Camp   Joined: Mar 2015 From: New Jersey Posts: 1,720 Thanks: 126 lnx and e^x $\\displaystyle \\ln x$ and e$\\displaystyle ^{x}$ are inverse functions: $\\displaystyle e^{\\ln x}=x$ and $\\displaystyle \\ln e^{x}=x$ But what are $\\displaystyle \\ln x$ and $\\displaystyle e^{x}$? Options: 1) Define $\\displaystyle e^{x}$ and $\\displaystyle \\ln x$ independently: $\\displaystyle e^{x} = 1+{}\\sum_{n=1}^{\\infty}\\frac{x^{n}}{n!}$ $\\displaystyle \\ln x=\\int_{1}^{x}\\frac{dx}{x}$ Then show they are inverses and derive the usual properties. 2) Choose either series or integral definition as fundamental, and define the other as inverse. If you choose integral definition, the series for $\\displaystyle e^{x}$ is easily derived: By definition $\\displaystyle e^{x}$ is the inverse function of $\\displaystyle \\ln x$. If $\\displaystyle y=\\ln^{-1}x. x=\\ln y$ and $\\displaystyle dx=\\frac{1}{y}dy$ so that $\\displaystyle \\frac{dy}{dx}= y =\\ln^{-1}(x)$, and $\\displaystyle \\frac{d^{2}y}{dx^{2}}=\\ln^{-1}(x)$,..... In general $\\displaystyle \\frac{d^{n}y}{dx^{n}}=\\ln^{-1}(x)$ and $\\displaystyle \\frac{d^{n}y}{dx^{n}}|_{x=0}=1$ from which Taylor series for $\\displaystyle e^x = \\ln^{-1}(x)$ follows. But I do have a question (surprise): Show, $\\displaystyle \\ln ab = \\ln a + \\ln b$ from the lntegral definition, i.e., Show $\\displaystyle \\int_{1}^{ab}\\frac{dx}{x}= \\int_{1}^{a}\\frac{dx}{x}+\\int_{1}^{b}\\frac{dx}{x}$ ------------------------------------------------------------------------------- skipjack has a way of editing typography so that text and equations are uniform. How? Last edited by skipjack; December 11th, 2017 at 02:44 PM.", null, "December 11th, 2017, 09:30 AM #2 Math Team   Joined: Dec 2013 From: Colombia Posts: 7,700 Thanks: 2682 Math Focus: Mainly analysis and algebra \\begin{align*} \\int_1^{ab}\\frac1t\\,\\mathrm dt &= \\int_1^{a}\\frac1t\\,\\mathrm dt + \\int_a^{ab}\\frac1t\\,\\mathrm dt \\\\ &= \\int_1^{a}\\frac1t\\,\\mathrm dt + \\int_1^{b}\\frac1u\\,\\mathrm du & \\text{(where $u=at$)} \\end{align*} Thanks from Maschke and zylo", null, "December 11th, 2017, 10:11 AM #3 Banned Camp   Joined: Mar 2015 From: New Jersey Posts: 1,720 Thanks: 126 Actually, u=t/a, but it's the thought that counts. 10/10, no deduction for typo. Many thanks.", null, "December 11th, 2017, 01:30 PM #4 Math Team   Joined: Dec 2013 From: Colombia Posts: 7,700 Thanks: 2682 Math Focus: Mainly analysis and algebra Oh, well perhaps some admin can correct it.", null, "December 11th, 2017, 02:14 PM #5 Banned Camp   Joined: Mar 2015 From: New Jersey Posts: 1,720 Thanks: 126 Exponents from scratch based on above. (till now, e$\\displaystyle ^{x}$ is not an exponential, it is just symbol for inverse of $\\ln x$ which is defined by integral.) $\\displaystyle a^{x} = e^{a\\ln x}$, which is a definition in terms of known, calculable, quantities. Otherwise, what is .8375^{4.2319}? Usual laws of exponents should follow. $\\displaystyle \\ln_{a}a^{x}=x$ is definition of inverse function ln$\\displaystyle _{a}$. (Since $\\displaystyle \\ln e^{x}-x, \\ln \\equiv \\ln_{e}$). $\\displaystyle a^{\\ln_{a}x}=x$, and take ln of both sides. $\\displaystyle \\ln_{a}x(\\ln a)=\\ln x$, and $\\displaystyle \\ln_{10}x=\\ln x/\\ln10$. Last edited by skipjack; December 11th, 2017 at 02:26 PM.", null, "December 11th, 2017, 02:49 PM #6 Global Moderator   Joined: Dec 2006 Posts: 21,128 Thanks: 2337 Obviously, $\\displaystyle a^{x} = e^{a\\ln x}$ is wrong. I assume you meant $\\displaystyle a^{x} = e^{x\\ln a}\\!$. Thanks from zylo", null, "December 11th, 2017, 04:03 PM   #7\nBanned Camp\n\nJoined: Mar 2015\nFrom: New Jersey\n\nPosts: 1,720\nThanks: 126\n\nQuote:\n Originally Posted by skipjack", null, "Obviously, $\\displaystyle a^{x} = e^{a\\ln x}$ is wrong. I assume you meant $\\displaystyle a^{x} = e^{x\\ln a}\\!$.\nIndeed. Thanks for catching that.\n\nAmazingly, if you calculate $\\displaystyle 3^{2}=e^{2\\ln3}$ on a simple TI calculator, it comes up with 9. Didn't expect that, after all the ten place intermediate decimals. Guess it was just a matter of rounding up the final number to ten places, which was 9.", null, "December 11th, 2017, 06:00 PM #8 Banned Camp   Joined: Mar 2015 From: New Jersey Posts: 1,720 Thanks: 126 On the other hand, consider the function $\\displaystyle f(x)=x^{a}$ with definition: $\\displaystyle f(x)=x^{a}=e^{a\\ln x}$ What is $\\displaystyle f^{-1}(f(x))=x$? $\\displaystyle f^{-1}(x) = x^{\\frac{1}{a}}$ $\\displaystyle f^{-1}(x^{a})= (x^{a})^{\\frac{1}{a}}=(e^{a\\ln x})^{\\frac{1}{a}}=x$ To summarize, $\\displaystyle a^{x}$ and $\\displaystyle x^{a}$ are different functions of x with different inverses.", null, "December 11th, 2017, 06:13 PM   #9\nMath Team\n\nJoined: Dec 2013\nFrom: Colombia\n\nPosts: 7,700\nThanks: 2682\n\nMath Focus: Mainly analysis and algebra\nQuote:\n Originally Posted by zylo", null, "To summarize, $\\displaystyle a^{x}$ and $\\displaystyle x^{a}$ are different functions of x with different inverses.\nPure genius. Who'd've thought it?", null, "December 12th, 2017, 08:23 AM #10 Banned Camp   Joined: Mar 2015 From: New Jersey Posts: 1,720 Thanks: 126 Two ways of looking at $\\displaystyle \\ln_{a}x$ 1) Def: $\\displaystyle \\ln_{a}x$ is the power you have to raise a to to get x: $\\displaystyle a^{\\ln_{a}x}=x$ $\\displaystyle \\ln_{a}(a^{x}) = x$, power you have to raise a to to get a$\\displaystyle ^{x}$. 2) Def: $\\displaystyle \\ln_{a}x = f^{-1}(a^{x})$ $\\displaystyle \\ln_{a}(a^{x}) = x, f^{-1}(f(x))=x$ $\\displaystyle a^{\\ln_{a}x}=x, f(f^{-1}(x))=x$ Def 1 is what I will remember a week from now because that's what I learned. I like Def 2 as a development from first principles as in this thread.", null, "Tags lnx", null, "Thread Tools", null, "Show Printable Version", null, "Email this Page Display Modes", null, "Linear Mode", null, "Switch to Hybrid Mode", null, "Switch to Threaded Mode\n\n Contact - Home - Forums - Cryptocurrency Forum - Top", null, "", null, "", null, "", null, "", null, "", null, "", null, "" ]
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https://planetmath.org/algebraicsumandproduct
[ "# algebraic sum and product\n\nLet $\\alpha,\\,\\beta$ be two elements of an extension field", null, "", null, "of a given field $K$.  Both these elements are algebraic over $K$ if and only if both $\\alpha\\!+\\!\\beta$ and $\\alpha\\beta$ are algebraic over $K$.\n\nProof.  Assume first that $\\alpha$ and $\\beta$ are algebraic", null, "", null, ".  Because\n\n $[K(\\alpha,\\,\\beta):K]=[K(\\alpha,\\,\\beta):K(\\alpha)]\\,[K(\\alpha):K]$\n\nand both here are finite (http://planetmath.org/ExtendedRealNumbers), then $[K(\\alpha,\\,\\beta):K]$ is finite.  So we have a finite field extension $K(\\alpha,\\,\\beta)/K$ which thus is also algebraic, and therefore the elements $\\alpha\\!+\\!\\beta$ and $\\alpha\\beta$ of $K(\\alpha,\\,\\beta)$ are algebraic over $K$.  Secondly suppose that $\\alpha\\!+\\!\\beta$ and $\\alpha\\beta$ are algebraic over $K$.  The elements $\\alpha$ and $\\beta$ are the roots of the quadratic equation$x^{2}-(\\alpha\\!+\\!\\beta)x+\\alpha\\beta=0$  (cf. properties of quadratic equation) with the coefficients in $K(\\alpha\\!+\\!\\beta,\\,\\alpha\\beta)$.  Thus\n\n $[K(\\alpha,\\,\\beta):K]=[K(\\alpha,\\,\\beta):K(\\alpha\\!+\\!\\beta,\\,\\alpha\\beta)]\\,[% K(\\alpha\\!+\\!\\beta,\\,\\alpha\\beta):K]\\leqq 2[K(\\alpha\\!+\\!\\beta,\\,\\alpha\\beta):% K].$\n\nSince  $[K(\\alpha\\!+\\!\\beta,\\,\\alpha\\beta):K]$  is finite,  then also  $[K(\\alpha,\\,\\beta):K]$ is, and in the finite extension (http://planetmath.org/FiniteExtension)  $K(\\alpha,\\,\\beta)/K$  the elements $\\alpha$ and $\\beta$ must be algebraic over $K$.\n\n Title algebraic sum and product Canonical name AlgebraicSumAndProduct Date of creation 2013-03-22 15:28:03 Last modified on 2013-03-22 15:28:03 Owner pahio (2872) Last modified by pahio (2872) Numerical id 8 Author pahio (2872) Entry type Theorem Classification msc 11R32 Classification msc 11R04 Classification msc 13B05 Synonym sum and product algebraic Related topic FiniteExtension Related topic TheoryOfAlgebraicNumbers Related topic FieldOfAlgebraicNumbers" ]
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https://www.gradesaver.com/textbooks/math/geometry/CLONE-68e52840-b25a-488c-a775-8f1d0bdf0669/chapter-4-section-4-1-properties-of-a-parallelogram-exercises-page-176/5
[ "## Elementary Geometry for College Students (6th Edition)\n\n(a) $QR = 6.4$ (b) $MP = 10.6$\n(a) The diagonals of a parallelogram bisect each other. Therefore the point R is the midpoint of $\\overline{QN}$ We can find $QR$: $QR = \\frac{QN}{2} = \\frac{12.8}{2} = 6.4$ (b) The diagonals of a parallelogram bisect each other. Therefore the point R is the midpoint of $\\overline{MP}$ We can find $MP$: $MP = 2\\times MR = (2)(5.3) = 10.6$" ]
[ null ]
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https://wiki.workxpress.com/doku.php?id=expression%20function%20-%20hyperbolic%20sine&rev=1473877160&do=diff
[ "", null, "# Differences\n\nThis shows you the differences between two versions of the page.\n\n — expression function - hyperbolic sine [2016/09/14 14:19] (current) Line 1: Line 1: + ====== Hyperbolic Sine (Expression Function) ====== + ===== Purpose ===== + The **Hyperbolic Sine** function (SINH) is used to calculate the hyperbolic sine of an angle given in radians, degrees, or gradians. ​ + + {{::​sinh_initial.png?​direct&​600|}} + + ===== Parameters ===== + The **Hyperbolic Sine** function has two parameters, the first of which is required: + + ==== Radians ==== + + Allowed Inputs: [[Field|field]] value or number + + The first required parameter is the angle that the hyperbolic sine will be obtained from either use the use the [[Query Builder]] to choose a field that contains the value or use type a value to enter a number. + + ==== Angle Unit ==== + + Allowed Inputs: omitted, '​d',​ '​g' ​ + + The second parameter of the **Hyperbolic Sine** function is the unit the angle is provided in. If the angle unit is omitted or not recognized then radians will be be used.  For an angle provided in degrees use '​d'​. ​ For an angle provided in gradians use '​g'​. ​ If the angle unit needs to be dynamically stored in a field then the advanced expression builder will need to be used. + + + ===== Output ===== + + The output of the **Hyperbolic Sine** function is a number representing the horizontal run of an angle where in intersects with the unit hyperbola. + + ===== Example ===== + + For example SINH(0.5235987755983),​ SINH(30,'​d'​),​ and SINH(33.3333333333,'​g'​) would result in \"​0.547853473888\"​.\nexpression function - hyperbolic sine.txt · Last modified: 2016/09/14 14:19 (external edit)", null, "", null, "", null, "" ]
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https://www.colorhexa.com/0d07d3
[ "# #0d07d3 Color Information\n\nIn a RGB color space, hex #0d07d3 is composed of 5.1% red, 2.7% green and 82.7% blue. Whereas in a CMYK color space, it is composed of 93.8% cyan, 96.7% magenta, 0% yellow and 17.3% black. It has a hue angle of 241.8 degrees, a saturation of 93.6% and a lightness of 42.7%. #0d07d3 color hex could be obtained by blending #1a0eff with #0000a7. Closest websafe color is: #0000cc.\n\n• R 5\n• G 3\n• B 83\nRGB color chart\n• C 94\n• M 97\n• Y 0\n• K 17\nCMYK color chart\n\n#0d07d3 color description : Strong blue.\n\n# #0d07d3 Color Conversion\n\nThe hexadecimal color #0d07d3 has RGB values of R:13, G:7, B:211 and CMYK values of C:0.94, M:0.97, Y:0, K:0.17. Its decimal value is 853971.\n\nHex triplet RGB Decimal 0d07d3 `#0d07d3` 13, 7, 211 `rgb(13,7,211)` 5.1, 2.7, 82.7 `rgb(5.1%,2.7%,82.7%)` 94, 97, 0, 17 241.8°, 93.6, 42.7 `hsl(241.8,93.6%,42.7%)` 241.8°, 96.7, 82.7 0000cc `#0000cc`\nCIE-LAB 26.562, 67.357, -92.338 11.997, 4.94, 61.946 0.152, 0.063, 4.94 26.562, 114.295, 306.109 26.562, -7.376, -105.267 22.226, 57.461, -149.691 00001101, 00000111, 11010011\n\n# Color Schemes with #0d07d3\n\n• #0d07d3\n``#0d07d3` `rgb(13,7,211)``\n• #cdd307\n``#cdd307` `rgb(205,211,7)``\nComplementary Color\n• #0767d3\n``#0767d3` `rgb(7,103,211)``\n• #0d07d3\n``#0d07d3` `rgb(13,7,211)``\n• #7307d3\n``#7307d3` `rgb(115,7,211)``\nAnalogous Color\n• #67d307\n``#67d307` `rgb(103,211,7)``\n• #0d07d3\n``#0d07d3` `rgb(13,7,211)``\n• #d37307\n``#d37307` `rgb(211,115,7)``\nSplit Complementary Color\n• #07d30d\n``#07d30d` `rgb(7,211,13)``\n• #0d07d3\n``#0d07d3` `rgb(13,7,211)``\n• #d30d07\n``#d30d07` `rgb(211,13,7)``\n• #07cdd3\n``#07cdd3` `rgb(7,205,211)``\n• #0d07d3\n``#0d07d3` `rgb(13,7,211)``\n• #d30d07\n``#d30d07` `rgb(211,13,7)``\n• #cdd307\n``#cdd307` `rgb(205,211,7)``\n• #080589\n``#080589` `rgb(8,5,137)``\n• #0a05a2\n``#0a05a2` `rgb(10,5,162)``\n• #0b06ba\n``#0b06ba` `rgb(11,6,186)``\n• #0d07d3\n``#0d07d3` `rgb(13,7,211)``\n• #0f08ec\n``#0f08ec` `rgb(15,8,236)``\n• #1c16f7\n``#1c16f7` `rgb(28,22,247)``\n• #342ef8\n``#342ef8` `rgb(52,46,248)``\nMonochromatic Color\n\n# Alternatives to #0d07d3\n\nBelow, you can see some colors close to #0d07d3. Having a set of related colors can be useful if you need an inspirational alternative to your original color choice.\n\n• #0734d3\n``#0734d3` `rgb(7,52,211)``\n• #0723d3\n``#0723d3` `rgb(7,35,211)``\n• #0712d3\n``#0712d3` `rgb(7,18,211)``\n• #0d07d3\n``#0d07d3` `rgb(13,7,211)``\n• #1e07d3\n``#1e07d3` `rgb(30,7,211)``\n• #2f07d3\n``#2f07d3` `rgb(47,7,211)``\n• #4007d3\n``#4007d3` `rgb(64,7,211)``\nSimilar Colors\n\n# #0d07d3 Preview\n\nThis text has a font color of #0d07d3.\n\n``<span style=\"color:#0d07d3;\">Text here</span>``\n#0d07d3 background color\n\nThis paragraph has a background color of #0d07d3.\n\n``<p style=\"background-color:#0d07d3;\">Content here</p>``\n#0d07d3 border color\n\nThis element has a border color of #0d07d3.\n\n``<div style=\"border:1px solid #0d07d3;\">Content here</div>``\nCSS codes\n``.text {color:#0d07d3;}``\n``.background {background-color:#0d07d3;}``\n``.border {border:1px solid #0d07d3;}``\n\n# Shades and Tints of #0d07d3\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, #000002 is the darkest color, while #efeefe is the lightest one.\n\n• #000002\n``#000002` `rgb(0,0,2)``\n• #010115\n``#010115` `rgb(1,1,21)``\n• #020128\n``#020128` `rgb(2,1,40)``\n• #04023b\n``#04023b` `rgb(4,2,59)``\n• #05034e\n``#05034e` `rgb(5,3,78)``\n• #060361\n``#060361` `rgb(6,3,97)``\n• #070474\n``#070474` `rgb(7,4,116)``\n• #080487\n``#080487` `rgb(8,4,135)``\n• #09059a\n``#09059a` `rgb(9,5,154)``\n``#0b06ad` `rgb(11,6,173)``\n• #0c06c0\n``#0c06c0` `rgb(12,6,192)``\n• #0d07d3\n``#0d07d3` `rgb(13,7,211)``\n• #0e08e6\n``#0e08e6` `rgb(14,8,230)``\n• #110af7\n``#110af7` `rgb(17,10,247)``\n• #241df8\n``#241df8` `rgb(36,29,248)``\n• #3630f8\n``#3630f8` `rgb(54,48,248)``\n• #4943f9\n``#4943f9` `rgb(73,67,249)``\n• #5b56f9\n``#5b56f9` `rgb(91,86,249)``\n• #6e69fa\n``#6e69fa` `rgb(110,105,250)``\n• #807cfb\n``#807cfb` `rgb(128,124,251)``\n• #928ffb\n``#928ffb` `rgb(146,143,251)``\n• #a5a2fc\n``#a5a2fc` `rgb(165,162,252)``\n• #b7b5fd\n``#b7b5fd` `rgb(183,181,253)``\n• #cac8fd\n``#cac8fd` `rgb(202,200,253)``\n• #dcdbfe\n``#dcdbfe` `rgb(220,219,254)``\n• #efeefe\n``#efeefe` `rgb(239,238,254)``\nTint Color Variation\n\n# Tones of #0d07d3\n\nA tone is produced by adding gray to any pure hue. In this case, #6c6c6e is the less saturated color, while #0d07d3 is the most saturated one.\n\n• #6c6c6e\n``#6c6c6e` `rgb(108,108,110)``\n• #646377\n``#646377` `rgb(100,99,119)``\n• #5c5b7f\n``#5c5b7f` `rgb(92,91,127)``\n• #545288\n``#545288` `rgb(84,82,136)``\n• #4c4a90\n``#4c4a90` `rgb(76,74,144)``\n• #444298\n``#444298` `rgb(68,66,152)``\n• #3c39a1\n``#3c39a1` `rgb(60,57,161)``\n• #3431a9\n``#3431a9` `rgb(52,49,169)``\n• #2d29b1\n``#2d29b1` `rgb(45,41,177)``\n• #2520ba\n``#2520ba` `rgb(37,32,186)``\n• #1d18c2\n``#1d18c2` `rgb(29,24,194)``\n• #150fcb\n``#150fcb` `rgb(21,15,203)``\n• #0d07d3\n``#0d07d3` `rgb(13,7,211)``\nTone Color Variation\n\n# Color Blindness Simulator\n\nBelow, you can see how #0d07d3 is perceived by people affected by a color vision deficiency. This can be useful if you need to ensure your color combinations are accessible to color-blind users.\n\nMonochromacy\n• Achromatopsia 0.005% of the population\n• Atypical Achromatopsia 0.001% of the population\nDichromacy\n• Protanopia 1% of men\n• Deuteranopia 1% of men\n• Tritanopia 0.001% of the population\nTrichromacy\n• Protanomaly 1% of men, 0.01% of women\n• Deuteranomaly 6% of men, 0.4% of women\n• Tritanomaly 0.01% of the population" ]
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http://icpc.njust.edu.cn/Problem/Hdu/5937/
[ "# Equation\n\nTime Limit: 2000/1000 MS (Java/Others)\n\nMemory Limit: 65536/32768 K (Java/Others)\n\n## Description\n\nLittle Ruins is a studious boy, recently he learned addition operation! He was rewarded some number bricks of $1$ to $9$ and infinity bricks of addition mark '+' and equal mark '='.\n\nNow little Ruins is puzzled by those bricks because he wants to put those bricks into as many different addition equations form $x + y = z$ as possible. Each brick can be used at most once and x, y, z are one digit integer.\n\nAs Ruins is a beginer of addition operation, $x$, $y$ and $z$ will be single digit number.\n\nTwo addition equations are different if any number of $x$, $y$ and $z$ is different.\n\n## Input\n\nFirst line contains an integer $T$, which indicates the number of test cases.\n\nEvery test case contains one line with nine integers, the $i^{th}$ integer indicates the number of bricks of $i$.\n\nLimits\n$1 \\leq T \\leq 30$\n$0 \\leq \\text{bricks number of each type} \\leq 100$\n\n## Output\n\nFor every test case, you should output 'Case #x: y', where x indicates the case number and counts from 1 and y is the result.\n\n## Sample Input\n\n3\n1 1 1 1 1 1 1 1 1\n2 2 2 2 2 2 2 2 2\n0 3 3 0 3 0 0 0 0\n\n## Sample Output\n\nCase #1: 2\nCase #2: 6\nCase #3: 2\n\nliuyiding\n\n## Source\n\n2016年中国大学生程序设计竞赛(杭州)" ]
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https://or.stackexchange.com/questions/4374/linearization-of-the-shifted-copy-of-a-function
[ "# Linearization of the shifted copy of a function\n\nSuppose in a model I have the expression $$y_{1}(x) = 10 + 5 x^2$$ where $$x \\in [0,20]$$ is a continuous variable. In order to be able to use an MILP solver, I piecewise linearise $$z_{1} = x^2$$, by choosing $$\\{0,5,10,20\\}$$ as arbitrary values for $$x$$, as follows:\n\n$$x = 0 \\lambda_{1} + 5 \\lambda_{2} + 10 \\lambda_{3} + 20 \\lambda_{4} \\\\ z_{1} =0 \\lambda_{1} + 25 \\lambda_{2} + 100 \\lambda_{3} + 400 \\lambda_{4} \\\\ \\lambda_{1} + \\lambda_{2} + \\lambda_{3} + \\lambda_{4} = 1$$\n\nIn the same model, I have to deal with the function:\n\n$$y_{2}(x,d) = 20 + 5 (x-d)^2, d \\ge 0$$, $$d$$ is a variable\n\nIs there a way to express $$(x-d)^2$$ in a linearised form in terms of $$\\lambda_{1}, \\lambda_{2}, \\lambda_{3}, \\lambda_{4}$$?\n\nPlease consider that $$y_{1}(x)$$ could be any nonlinear function, the quadratic form stated here is just an example.\n\n• Is $d$ really a variable of the whole model, and not a parameter? (Asking as the function is $y_2(x)$ and not $y_2(x, d)$) Jun 13 '20 at 15:42\n• d is a decision variable. $y_{2}(x)$ should be written $y_{2}(x,d)$, you are right. Jun 13 '20 at 17:08\n• First, is $x$ constrained to $\\lbrace 0, 5, 10, 20\\rbrace$ in the model? (Your constraints imply this.) Next, is $d$ discrete, and if so can you enumerate the possible values of $d$. Jun 13 '20 at 21:23\n• The three equations $x= ...$ , $z_{1} = ...$ , $\\lambda_{1} + ...$ are supposed to piecewise linear approximate $x^2$ within [0,20]. The points $x=0$, $x=5$, $x=10$, $x=20$ are chosen arbitrarily for this example. $d$ is not discrete. The only constraint imposed on $d$ is $x-d \\ge 0.0$. Jun 13 '20 at 22:44\n• $(x-d)^2=x^2 - 2xd + d^2$ and then you can look at or.stackexchange.com/questions/180/… for the middle term.\n– PSLP\nJun 15 '20 at 6:53" ]
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https://www.comsol.com/blogs/solving-shallow-water-equations-with-equation-based-modeling/?setlang=1
[ "", null, "", null, "# Solving Shallow Water Equations with Equation-Based Modeling\n\nFebruary 21, 2017\n\nThe COMSOL Multiphysics® software includes many built-in physics equations and interfaces, but there may be times when you need to implement physics that aren’t part of the software to solve your modeling problem. You can use the flexibility of the COMSOL® software to add user-defined equations via equation-based modeling. Today, we discuss using equation-based modeling to solve a shallow water equation, which can be used to analyze coastal erosion.\n\n### Analyzing Coastal Erosion with Shallow Water Equations\n\nOn the shoreline, crashing waves and the continuous movement of the tides cause coastal erosion, a phenomenon that removes sediment from beaches and wears away land.", null, "A rock formation affected by coastal erosion. Image by John Nuttall — Own work. Licensed under CC BY 2.0, via Flickr Creative Commons.\n\nAlthough coastal erosion has benefits, such as creating sand for beaches, it also causes damage to seaside property and habitats. To help predict this damage, researchers can use shallow water equations to learn more about coastal erosion. These equations enable scientists to model oceanographic and atmospheric fluid flow, thereby predicting what areas will be affected by coastal erosion and other issues, such as polar ice cap melting and pollution.\n\nShallow water equations are beneficial compared to the Navier-Stokes equations, which may be problematic depending on how free surfaces are resolved and the scale of the modeling domain. Today, we highlight a tutorial that showcases how to solve shallow water equations using the power of equation-based modeling.\n\n### Solving Shallow Water Equations in COMSOL Multiphysics®\n\nIn this shallow water equation model, we can describe the physics by adding our own equations — a feature called equation-based modeling. We use the General Form PDE interface and two dependent variables to ensure that the modeling process is straightforward. This way, we can easily define expressions as model variables, which comes in handy when defining the initial wave profile.\n\nThis simple 1D model uses the Saint-Venant shallow water equations to study a wave settling over a variable bed as a function of time.\n\nThe 1D model featured here would require substantial work to convert into a 2D model for solving typical applications. This tutorial is therefore most useful as an example of the benefits of equation-based modeling.", null, "A vertical section of the fluid domain. Here, zf is the analytical expression for the seabed profile and zs is the water surface profile.\n\nThe model, which investigates shallow water in a channel, has constraints at both ends and uses a wave profile as the initial condition. In order to easily alter parameters like the wave amplitude and bed shape, we can use mathematical relations to represent the initial wave and bed shapes. Please note that the model has a difference in scale between the x– and y-directions, as seen in the plots below.\n\nPlots of the seabed profile (left) and a comparison of the initial water surface profile with the seabed profile (right).\n\nWe see that the flow develops hydraulic jump discontinuities over time, which can cause instability in the solution. To stabilize the solution, we can add an artificial viscosity that makes the cell Reynolds number of order unity. The hydraulic jumps are replaced with steep fronts that can be resolved on a grid.\n\nSwitching gears, let’s take a look at our results. After running the simulation for 60 seconds, we see results that show the water surface and seabed slope at 6 different times, from the start of the simulation to 15 seconds later.", null, "Plots of the seabed profile and water surface level at 3-second increments.\n\nThese results clearly indicate that the seabed topography influences the water surface elevation. This, in turn, affects the impact of coastal erosion.\n\nWe can share these custom results with others by creating and exporting an animation to help visualize our findings — something that is easy to do in COMSOL Multiphysics.\n\nAn animation of the simulation results.\n\nAs a next step, try this tutorial yourself by clicking on the button below." ]
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https://www.physicsforums.com/threads/stress-tensor.90636/
[ "# Stress Tensor\n\nHello,\n\nPlease help me out here as I self study fluid mechanics. I ran into what they are calling a second order tensor quantity, which seems to be fancy words for a 3x3 matrix of sigmas and rhos, for shear and normal stress. They have a picture of a cube, with all the positive stresses indicated on it. Now they have a convention like sigma_xx or sigma_xy. I get that. I dont get the picture of the cube, though. Is it merely an illustration? See they start with the premise that you are looking locally at point C in space. And you make a plane of area deltaA, perpendicular to the x axis, then you find the shear and normal stress to the unit normal. Then they repeat for the other two orthogonal planes. Thats fine. Then the say there are an infinte number of planes that can pass through point C and have different shear values, FINE! Then they say that any stress can be found for any plane provided that you now know these three mutually perpendicular stress planes.......ok i kinda see what they mean, but im not tooo sure.....I could use some explaining on that point. Also, this damn box!? Is point C somewhere inside this box of dimensions dx,dy,dz?? Why is this thing now a box, I thought we just cared about flat planar areas that passed through point c? Is point C now surrounded by this box? Or is the box there just to explain to my stupid self the purpose of the x,y subsripts, becuase I have a feeling its going to be used as a local control surface for some reason.\n\n(This stuffs still great fun so far!", null, "Im just annoyed at the unclarity)\n\nAstronuc\nStaff Emeritus\nWell, stress (like pressure) is force/unit area, and one has three dimensions.\n\nWith three dimensions mutually orthogonal, each direction (dimension) has a surface associated with it formed by the other two dimensions. Thus the y,z-plane is perpendicular to x-direction, the x,z-plane to the y-direction, and the x,y-plane to the z-direction (in Cartesian cooridates). So with three dimensions there is an incremental volume (cube) with 6 faces (surface areas, planes) associated with the volume.\n\nThere are normal stress $\\sigma_{xx}, \\sigma_{yy}, and \\sigma_{zz}$ which act normal to a plane (surface) in tension or compression, and there are shear stress, e.g. $\\sigma_{xy} = \\tau_{xy}$ which acts parallel to a plane (surface). The $\\sigma_{xx}$ stress acts in the x-direction on the y,z plane (surface).\n\nI realize that astronuc, but my question was why the cube? I already know what the stresses and planes represnt, but im asking WHY are there 6 of them constructed the way they are?\n\nPerennialII\nGold Member\nTo satisfy the balance and equilibrium equations continuum mechanics is build upon in a 3D spatial description. That accounts for the 6 planes, the cube is a differential geometrical element.\n\nOk, and it is dx,dy,dz in dimension, but is it always true that dx,dy,dz are equal in magnitude? I dont see why they have to be, I have yet to run into a definition stating that they are.\n\nAstronuc\nStaff Emeritus\ncyrusabdollahi said:\nI realize that astronuc, but my question was why the cube? I already know what the stresses and planes represnt, but im asking WHY are there 6 of them constructed the way they are?\nAs PerennialII pointed out, a cube is an element in differential geometry, and it is the simplest volume element in Cartesian coordinates. What other volume element geometry would one propose?\n\nIf one used cylindrical or spherical coordinates (geometry) then one could use an annular or spherical volume segment.\n\nThe cube has 6 faces in 3D. In a static system, equal an opposing forces are applied on opposite faces of a volume element.\n\nPerennialII\nGold Member\nFollowing a typical differential geometric treatment their size is really not that much of an issue, the differential element under question being the smallest element in the continuum treatment's \"radar\", \"resolution\" etc. But if you think about the sizing of the different axes, nothing is gained by making them different sizes since it does not increase the \"information content\" of the solution of the problem (or its formulation)(ok, I'd say you could do it, but can't really see for what reason unless you'd be doing something really exotic, anisotropic, mixing different equilibrium concepts, material models etc., and even in such cases the basic formulation can be retained & formulated in a \"simple\" differential cube).\n\nVector base continuum non-cauchian theorem\n\nSymmetry of stress tensor ( ) is the start point of this survey. As we know in non-magnetic fields this symmetry is always valid and everybody has been accepting that for 200 years after Cauchy.\nWhile in quantum or discrete mechanics (statistical mechanics) it’s not evident. Also there are some continua situations, in them, that symmetry isn’t valid. So what is the reason of this difference? What is the problem?\n\nWhy a differential tetrahedron element is used? Nobody cares. But it’s the point because this element just differentiate the position not the orientation!\nAnd this result is not valid for any arbitrary volume, we will show the Cauchy principle is just a approximate solution of sigma. However we don’t know the exact one but it doesn’t matter.\n\nIn next we will try to find the most general shape for the relation. It’s just a claim to say vector form of equations is a valid shape for Cauchy–Riemann rules and we can’t prove it yet.\nWe will generate the conservative rule equations without assumption of linear mapping. And we show the computational cost advantages of vector base continuum in compare whit tensor.\nSome constitutive equations will be written in vector base form and we regenerate some well-known deformation such as navier-stockse\n\n#### Attachments\n\n• presentation.pdf\n1.7 MB · Views: 224" ]
[ null, "data:image/gif;base64,R0lGODlhAQABAIAAAAAAAP///yH5BAEAAAAALAAAAAABAAEAAAIBRAA7", null ]
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https://socratic.org/questions/what-is-1-600-4
[ "# What is 1,600 -: 4?\n\nMar 11, 2018\n\n$400$\n\n#### Explanation:\n\n$1600$ is the same as $16 \\times 100$\n\nSo we have $16 \\times 100 \\div 4$\n\nThe order we do this in does not matter so lets swap a bit of it around.\n\n$16 \\div 4 \\times 100$\n\n$4 \\times 100 = 400$" ]
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http://www.britishorigami.org.uk/0b87d9a4ad3430086afda5f06a9b9621
[ "# Review Stoichiometry Section 1 And 2 Answers\n\nreview stoichiometry section 1 and 2 answers\n\nMolar masses: H 2 O = 18.02 g/mole O 2 = 32.00 g/mole C 4 H 10 = 58.12 g/mole Stoichiometry Review Answers 1. a. Na3PO4 b. Ca(NO3)2 Na = 3 mol x 22.99 g/mol = 68.97 g Ca = 1 mol x 40.08 g/mol = 40.08 g\n\nCHAPTER 9 REVIEW Stoichiometry - manasquanschools.org\n\nStoichiometry. SECTION 1. SHORT ANSWER Answer the following questions in the space provided. 1. _____ The coefficients in a chemical equation represent the (a) masses in grams of all reactants and products. (b) relative number of moles of reactants and products. (c) number of atoms of each element in each compound in a reaction.\n\n[DOC] Chapter 9 Section 1 Review Stoichiometry Answers\n\nthe book. chapter 9 section 1 review stoichiometry answers really offers what everybody wants. The choices of the words, dictions, and how the author conveys the notice and lesson to the readers are enormously easy to understand. So, like you environment bad, you may not think fittingly difficult roughly this\n\nModern Chemistry Stoichiometry Section 1 Review Answers Modern Chemistry Stoichiometry Section 1 Right here, we have countless books Modern Chemistry Stoichiometry Section 1 Review Answers and collections to check out. We additionally come up with the money for variant types and moreover type of the books to browse. The normal book, fiction,\n\nCHAPTER 9 REVIEW Stoichiometry MIXED REVIEW SHORT ANSWER Answer the following questions in the space provided. 1. Given the following equation: C 3H 4(g) + xO 2(g) → 3CO 2(g) + 2H 2O(g) 4 a. What is the value of the coefficient x in this equation? 40.07 g/mol b. What is the molar mass of C 3H 4? 2 mol O 2:1 mol H 2O c. What is the mole ratio ...\n\nStoichiometry (Chapter 11) Flashcards | Quizlet\n\nChemistry: Stoichiometry – Problem Sheet 2 KEY 9) 2 24 2 2 23 2 2 2 2 4.63 x 10molecules I 1 mol I 6.02 x 10 moleculesI 1 mol Cl 1mol 71 g Cl Cl x 546 g Cl 10) 292 g Ag 1 mol Ag 108 g Ag 1 mol Cu 1 mol Ag 63.5 g Cu\n\nCHAPTER 9 REVIEW\n\n1 mol CO2 2 mol O2 1 mol O2 22.4 L O2 22.4 L CO2 1 mol CO2 Sometimes information you read is easier to remember if you write it in a different format. For example, the paragraph on page 363 and Figure 12.8 both explain how to solve stoichiometric problems. Use these explanations to make a diagram or flow chart for solving a particle–mass\n\nChapter 11: Stoichiometry\n\n17.16MB REVIEW STOICHIOMETRY SECTION 1 SHORT ANSWER As Pdf, 1 ANSWER STOICHIOMETRY SECTION REVIEW SHORT As Docx, 1 ANSWER SECTION REVIEW SHORT STOICHIOMETRY As Pptx REVIEW STOICHIOMETRY SECTION 1 SHORT ANSWER How easy reading concept can improve to be an effective person? REVIEW STOICHIOMETRY SECTION 1 SHORT ANSWER review is a very simple task.\n\nWorksheet for Basic Stoichiometry. Part 1: Mole ←→ Mass Conversions. Convert the following number of moles of chemical into its corresponding mass in grams. 1. 0.436 moles of ammonium chloride. 2. 2.360 moles of lead (II) oxide. 3. 0.031 moles of aluminum iodide. 4. 1.077 moles of magnesium phosphate. 5. 0.50 moles of calcium nitrate\n\nCHAPTER 11: STOICHIOMETRY\n\nChemistry (12th Edition) answers to Chapter 12 - Stoichiometry - 12.2 Chemical Calculations - Sample Problem 12.3 - Page 391 12 including work step by step written by community members like you. Textbook Authors: Wilbraham, ISBN-10: 0132525763, ISBN-13: 978-0-13252-576-3, Publisher: Prentice Hall\n\nchemistry chapter 12 stoichiometry Flashcards and Study ...\n\nStoichiometry b. Theoretically, how many moles of NH3 will be produced? PROBLEMS Write the answer on the line to the left, Show all your work in the space provided. 1 88% The actual yield of a reaction is 22 g and the theoretical yield is 25 g. Calculate the percentage yield. 2. 6.0 mol of N2 are mixed with 12.0 mol of H2 according to the ...\n\nCrown Publishing Group - #1 Books Space\n\nThe test covers section 4.1, 4.2, enthalpy notation in 4.4 (recognizing whether a reaction is exothermic or endothermic from the energy term associated with the reaction or from the classification of the reaction, as well as defining the two terms), 4.5, and 4.6.\n\nChapter 12 REVIEW: Stoichiometry, Theoretical, Actual & Percent yield Part I. Stoichiometry 1. 1 ZnI2 → 1 Zn + 1 I2 How many grams of iodine will you produce if you begin your rxn with 56.7g of zinc iodide? 56.7 g 1 mole 1 mole 253.8 g 319.19 g 1 mole 1 mole = 45.08 grams of Iodine 2. 1 Pb2(CO3)3 + 6 K → 2 Pb + 3 K2CO3\n\nmc06se cFMsr i-vi\n\n2 1 mol CS 2/76.15 g CS 2 2 mol SO 2/1 mol CS 2 22.4 L SO 2/1 mol SO 2 74.1 L SO 2 74.01 L SO 2 1 mol CO 2/2 mol SO 2 37.1 L CO 2 Concept Review: Limiting Reactants and Percentage Yield 1. excess 2. limiting, product 3. limiting ... Holt Chemistry 86 Stoichiometry Answer Key TEACHER RESOURCE PAGE.\n\nSECTION 9.1 Introduction to Stoichiometry\n\nCHAPTER 9 REVIEW. Stoichiometry. SECTION 9.2. PROBLEMS Write the answer on the line to the left. Show all your work in the space provided. 1. The following equation represents a laboratory preparation for oxygen gas: 2KClO3(s) ( 2KCl(s) + 3O2(g) How many grams of O2 form if 3.0 mol of KClO3 are totally consumed? 2. Given the following equation ...\n\nchapter 9 review stoichiometry section 2 answers - Bing\n\nChapter 12 Stoichiometry Pearson Answers. ... Chapter 12 Stoichiometry 127 SECTION 12.1 THE ARITHMETIC OF EQUATIONS (pages 353-358) This section explains how to calculate the amount of reactants required or product formed in a nonchemical process. ... Prentice hall chemistry chapter 12 review answers bing, prentice hall chemistry chapter 12 ...\n\nSection 9.1 - 9.2 Complete the following assignment in ...\n\nChapter 9 focuses on reaction stoichiometry: using a balanced chemical equation to calculate the number of grams, moles, or particles of reactants/products involved in a chemical reaction. Students had an introduction to composition stoichiometry in Chapter 3 and will now move on to some more difficult problems.\n\nto Stoichiometry sect~on9 ReVIew • 1\n\nStoichiometry Review Worksheet Answers Along with Balance the Following Equations Worksheet Image Collections. It should be no surprise to you that the third piece of information you will need to complete this course is the Stoichiometry Review Worksheet Answers, which you can find out about at the website of the KKSB (the governing body that runs the KKSB) which you can find below.\n\nchapter 9 review stoichiometry answers section 9 1 - Bing\n\n1 Chapter 9 - Stoichiometry Section 9.1 – Introduction to Stoichiometry Types of Stoichiometry Problems Given is in moles and unknown is in moles. o Given is in moles and unknown is in mass (grams). o Given is in mass and unknown is in moles. o Given is in mass and unknown is in mass. o\n\nReview Stoichiometry Section 3 Answers - Free PDF File Sharing\n\n2 1.1 mol O 2 in excess Practice Problems 12 Section 12.1 1. 10A 2C Ci y A 10C 2Ci 2. 2KClO 3(s) y 2KCl(s) 3O 2(g) 12 mol KClO 3 18 mol O 2 3 mol O 2 2 mol KClO 3 25 A 10C 2Ci A 1 1 0C 0A 2Ci 250 apples 3.1 mol SO 2 2 mol SO 3 2 mol SO 2 3.1 mol SO 2 2 1 m m o o l l S O O 2 2 2.1 1024 molecules O 2 4 7 m m o o l l N O H 2 3 1 7 m.0 o g lN N H H ...\n\nUnit 9: Stoichiometry - Mrs. Langman's Chemistry Classes\n\nstoichiometry Ask A Question . 241 Answered Questions for the topic stoichiometry ... Answers · 1. what's the easiest way to balance chemical equations? Answers · 1. How many grams of water will be produced from 32 grams of oxygen gas. Answers · 2. RECOMMENDED TUTORS. Brianne Y. 4.6 (27) Kay H.\n\nChemistry: Matter and Change\n\ngive final answer with units and label. 1. Using the Hoffman apparatus for electrolysis, a ... 2 1 2.0 2 2 2 2.0 mol mol H O mol O mol H O ... Microsoft PowerPoint - Stoichiometry Worksheet 2a Author: mjensen Created Date: 4/4/2011 10:56:39 AM ...\n\nVIBRATIONS AND WAVES - Alliance Cindy And Bill Simon ...\n\n1 mol H × 2 2 2 mol H 1 mol O = 2.48 mol O2 CH4 + 2O2 → CO2 + 2H2O 2.48 mol O2 × 2 2 2 mol O 1 mol CO × 2 2 1 mol CO 44.01g CO = 54.6 g CO2 Section 9.3: Team Learning Worksheet We have included choices for many of these questions to test the students’ understanding. We have\n\nChapter 9 Stoichiometry Test Answer Key Modern Chemistry\n\nStoichiometry Practice Worksheet with Answer Keys-- 2 Practice Worksheets (Versions A & B)-- 2 Skill Levels for Each Version (Level 1 - Fill in the Blank; Level 2 - No Blanks)-- 4 Worksheets Total, 15 Exercises Per Worksheet, 60 Exercises Total)-- Answer Keys Provided-- Differentiated Skill Leve...\n\nStoichiometry Review 4-22. Stoichiometry Worksheet Number 1-2 (Stoichimetry Worksheet Number 1-2. To Mole Worksheets - Kiddy Math Stoichiometry Review Assignment Answer Key Stoichiometry Review Assignment Answer Key Example 1: Calculate the mass of a magnesium, Mg, atoms in grams. 0 grams 4) Mn 2Se 7 663.\n\n#### Review Stoichiometry Section 1 And 2 Answers\n\nThe most popular ebook you must read is Review Stoichiometry Section 1 And 2 Answers. I am sure you will love the Review Stoichiometry Section 1 And 2 Answers. You can download it to your laptop through easy steps." ]
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https://www.chemistrylearner.com/gibbs-free-energy.html
[ "# Chemistry Learner\n\nHome / Physical Chemistry / Gibbs Free Energy\n\n# Gibbs Free Energy\n\nThe Gibbs free energy is the energy associated with a chemical process that can be used to do work. It is a state function that is defined in terms of three other state functions – enthalpy, temperature, and entropy. It is denoted by the symbol G. The formula for Gibbs free energy of a system is given by the enthalpy minus the product of the temperature and entropy [1-4].\n\nG = H – TS\n\nWhere,\n\nG: Gibbs free energy\n\nH: Enthalpy\n\nT: Temperature\n\nS: Entropy\n\nUnit: kJ/mol or kilo Joule per mole\n\nAmerican chemist J.W. Gibbs developed the free energy concept in the 1870s.\n\n## How to Calculate Gibbs Free Energy [1-5]\n\n### Change in Gibbs Free Energy\n\nThe change in Gibbs free energy is a useful term to determine the spontaneity of a thermodynamic process. It is defined as the difference between the Gibbs free energies of the final and the initial states of the system .\n\nΔG = Gfinal – Ginitial\n\nConsider a chemical reaction where reactants A and B combine to form products C and D. The equation is given by\n\nA + B ⇌ C + D\n\nReactants ⇌ Products\n\nThen, the change in Gibbs free energy is\n\nΔG = GProducts – GReactants\n\nThis change ΔG depends only on the initial and final values of the free energy and is independent of the path taken. It means that ΔG is independent of the reaction mechanism. From the equation for G, we get\n\nΔG = ΔH – Δ(TS)\n\nThis change is meaningful under two conditions – constant temperature and constant pressure. And, these conditions are typical in a laboratory. Therefore,\n\nΔG = ΔH – TΔS\n\nThus, the change in Gibbs free energy is equal to the change in enthalpy minus the product of temperature and change in entropy.\n\n### Determination of Spontaneity\n\nThe significance of the above equation is to determine the relative importance of the enthalpy and entropy terms as forces that drive a particular chemical reaction. This equation is used to determine the spontaneity of the reaction and predict in which direction it proceeds – forward or backward. Let us look at a few cases where the value of ΔG depends entirely on the values of ΔH and TΔS.\n\n1. If ΔG < 0, the reaction is spontaneous and proceeds in the right or forward direction. It is known as spontaneous reaction or exergonic reaction.\n2. If ΔG > 0, the reaction is nonspontaneous in the forward direction but spontaneous in the reverse direction. Hence, it will proceed toward the left. A nonspontaneous reaction is known as endergonic reaction.\n3. ΔG = 0, the reaction is in equilibrium.\n\n### Standard-State Gibbs Free Energy\n\nAs mentioned before, the equation for ΔG applies to constant temperature and pressure conditions. When the reaction takes place at standard temperature and pressure (STP), the equation is rewritten as,\n\nΔG0 = ΔH0 – TΔS0\n\nG0 is known as the standard-state Gibbs free energy, and ΔG0 is its change. This change can be calculated from the standard-state enthalpy and entropy tables.\n\nNational Institute of Standards and Technology (NIST) in Maryland, USA uses a temperature of 20 °C (293.15 K) and an absolute pressure of 1 atm (101.325 kPa) as the standard temperature and pressure. The difference between the change of standard-state Gibbs free energy ΔG0 and the change of Gibbs free energy ΔG is that the reactants and the products are at STP in the former.\n\nStandard Gibbs Free Energy of Formation\n\nThe standard Gibbs free energy of formation of a substance is defined as the free energy change when 1 mole of the substance is prepared from its elements at standard temperature and pressure. It is denoted by ΔGf0. The following table shows the standard Gibbs free energy of formation of a few substances.\n\n## Gibbs Free Energy at Equilibrium\n\nLet us revisit the following chemical reaction.\n\nA + B ⇌ C + D\n\nAs the reaction progresses, the Gibbs free energy changes with time. The change in Gibbs free energy can be expressed in terms of the change in standard-state Gibbs free energy.\n\nΔG = ΔG0 + RT ln Q\n\nWhere,\n\nΔG: Change in Gibbs free energy\n\nΔG0: Change in standard-state Gibbs free energy\n\nR: Ideal gas constant (= 8.314 J/mol)\n\nT: Temperature (in K)\n\nQ: Reaction quotient (= [C][D]/[A][B])\n\nLet us look at two different situations.\n\nCase 1:\n\nWhen Q = 1, ΔG = ΔG0\n\nThis point describes the standard-state conditions of the reaction, where ΔG is equal to the change in standard-state Gibbs free energy.\n\nCase 2:\n\nWhen ΔG = 0, Q = K\n\nThere is no driving force for the reaction, and the system is at equilibrium. Here, K is known as the equilibrium constant. Therefore,\n\n0 = ΔG0 + RT ln K\n\nOr, ΔG0 = – RT ln K\n\nΔG0 = -2.303 RT log10 K\n\nThis equation gives the relationship between the standard-state Gibbs free energy and the equilibrium constant. It is used to determine the value of K from ΔG0 and vice versa.\n\n## Example of Gibbs Free Energy\n\nFormation of Ammonia (NH3)\n\nLet us take the example of ammonia synthesis to understand Gibbs free energy further .\n\nN2 (g) + 3 H2 (g) ⇌ 2 NH3 (g)\n\nThe standard Gibbs free energy of formation of two moles of ammonia (NH3) from nitrogen (N2) and hydrogen (H2) is ΔGf0 = -32.8 kJ (see table above). This parameter is calculated when the reaction occurs at standard temperature and pressure. It means that the above reaction takes place at 293.15 K and 1 atm pressure.\n\nThe fact that ΔGf0 is negative indicates that the reaction favors the formation of ammonia. In other words, under standard conditions, the reaction proceeds towards the right. The reactants are converted into products before reaching equilibrium. The magnitude of ΔGf0 tells how far the standard-state is from equilibrium. The larger the value, the further the reaction from equilibrium.\n\n## Problems and Solutions\n\nProblem 1. Calculate the ΔG for ice melting at 30 ˚C if the enthalpy and entropy of fusion of water are 6 kJ/mol and 22 J/mol-K.\n\nSolution:\n\nThe reaction is,\n\nH2O (s) ⇌ H2O (l)\n\nGiven,\n\nΔHfus = 6 kJ/mol = 6000 J/mol\n\nΔSfus = 22 J/mol-K\n\nT = 30 ˚C = (273 + 30) K = 303 K\n\nGibbs free energy equation is given by\n\nΔGfus = ΔHfus – T ΔSfus\n\nOr, ΔGfus = 6000 J/mol – 303 K x 22 J/mol-K\n\nOr, ΔGfus = -666 J/mol\n\nThe fact that ΔGfus is negative indicates that the reaction is spontaneous in the forward direction. In other words, ice will melt into the water at 30 ˚C.\n\nProblem 2. ∆G0 for the reaction below is 31.4 kJ/mol at 298.15 K. Use the thermodynamics parameters to decide in which direction the reaction is spontaneous when the concentrations of H2SO4 (aq.), HSO4(aq.), and H3O+ (aq.) are 0.5 M, 0.25 M, and 0.25 M respectively.\n\nH2SO4 (aq.) + H2O (aq.) ⇌ H3O+ (aq.) + HSO4(aq.)\n\nSolution:\n\nThe reaction quotient is given by,\n\nQ = [H3O+ (aq.)][ HSO4(aq.)]/[H2SO4 (aq.)]\n\n= 0.25 M x 0.25 M/0.5 M\n\n= 0.125\n\nGiven\n\nΔG0 = 31.4 kJ/mol = 31400 J/mol\n\nT = 298.15 K\n\nR = 8.314 J/mol-K\n\nThe change in Gibbs free energy is\n\nΔG = ΔG0 + RT ln Q\n\nOr, ΔG = 31400 J/mol + 8.314 J/mol-K x 298.15 K x ln (0.125)\n\nOr, ΔG = 26245 J/mol or 26.2 kJ.mol\n\nSince ΔG > 0, the reaction is spontaneous in the reverse direction.\n\nReferences" ]
[ null ]
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https://www.proprofs.com/quiz-school/story.php?title=amatyc-student-mathematics-league-oct-nov-2008
[ "# Amatyc Student Mathematics League Oct Nov 2008\n\n20 Questions | Total Attempts: 335", null, "", null, "Settings", null, "", null, "LACC Math club\n\nRelated Topics\n• 1.\nLine L has equation y = 2x + 3, and line M has the same y-intercept as L. Which of the points below must M contain to be perpendicular to L?\n• A.\n\n(-4, 5)\n\n• B.\n\n(-2, 5)\n\n• C.\n\n(-1, 5)\n\n• D.\n\n(1, 5)\n\n• E.\n\n(4, 5)\n\n• 2.\nSue just received a 5% raise. Now she earns \\$1200 more than Lisa. Before Sue’s raise, Lisa’s salary was 1% higher than Sue’s. What is Lisa’s salary?\n• A.\n\n\\$28,00\n\n• B.\n\n\\$29,400\n\n• C.\n\n\\$30,000\n\n• D.\n\n\\$30,300\n\n• E.\n\n31,200\n\n• 3.\nIf x = -1 is one solution of ax2 + bx + c = 0, what is the other solution?\n• A.\n\nX = -a/b\n\n• B.\n\nX = -b/a\n\n• C.\n\nX = b/a\n\n• D.\n\nX = -c/a\n\n• E.\n\nX = c/b\n\n• 4.\nRyan told Sam that he had 9 coins worth 45¢. Sam said, \"There is more than one possibility. How many are pennies?\" After Ryan answered truthfully, Sam said, \"Now I know what coins you have.\" How many nickels did Ryan have?\n• A.\n\n0\n\n• B.\n\n3\n\n• C.\n\n4\n\n• D.\n\n5\n\n• E.\n\n9\n\n• 5.\nA point (a, b) is a lattice point if both a and b are integers. It is called visible if the line segment from (0, 0) to it does NOT pass through any other lattice points. Which of the following lattice points is visible?\n• A.\n\n(28, 14)\n\n• B.\n\n(28, 15)\n\n• C.\n\n(28, 16)\n\n• D.\n\n(28, 18)\n\n• E.\n\n(28, 21)\n\n• 6.\nA flea jumps clockwise around a clock starting at 12. The flea first jumps one number to 1, then two numbers to 3, then three to 6, then two to 8, then one to 9, then two, then three, etc. What number does the flea land on at his 2008th jump?\n• A.\n\n4\n\n• B.\n\n5\n\n• C.\n\n6\n\n• D.\n\n7\n\n• E.\n\n8\n\n• 7.\nIn quadrilateral ABCD, E is the midpoint of , F is the midpoint of , G is the midpoint of , and H is the midpoint of Which of the following must be true?\n• A.\n\n∠FEH = ∠FGH\n\n• B.\n\n∠FEH = ∠EHG\n\n• C.\n\n∠FEH + ∠EHG = 180°\n\n• D.\n\nBoth A and C\n\n• E.\n\nBoth B and C\n\n• 8.\nAll nonempty subsets of {2, 4, 5, 7} are selected. How many different sums do the elements of each of these subsets add up to?\n• A.\n\n10\n\n• B.\n\n11\n\n• C.\n\n12\n\n• D.\n\n14\n\n• E.\n\n15\n\n• 9.\nLuis solves the equation ax - b = c, and Anh solves bx - c = a. If they get the same correct answer for x, and a, b, and c are distinct and nonzero, what must be true?\n• A.\n\nA + b + c = 0\n\n• B.\n\nA + b + c = 1\n\n• C.\n\nA + b = c\n\n• D.\n\nB = a + c\n\n• E.\n\nA = b + c\n\n• 10.\nHow many asymptotes does the function f(x) = have?\n• A.\n\n0\n\n• B.\n\n1\n\n• C.\n\n2\n\n• D.\n\n3\n\n• E.\n\n4\n\n• 11.\nReplace each letter of AMATYC with a digit 0 through 9 (equal letters replaced by equal digits, different letters replaced by different digits). If the resulting number is the largest such number divisible by 55, find A + M + A + T + Y + C.\n• A.\n\n36\n\n• B.\n\n38\n\n• C.\n\n40\n\n• D.\n\n42\n\n• E.\n\n44\n\n• 12.\nThe equation a^6 + b^2 + c^2 = 2009 has a solution in positive integers a, b, and c in which exactly two of a, b, and c are powers of 2. Find a + b + c.\n• A.\n\n43\n\n• B.\n\n45\n\n• C.\n\n47\n\n• D.\n\n49\n\n• E.\n\n51\n\n• 13.\nACME Widget employees are paid every other Friday (i. e., on Fridays in alternate weeks). The year 2008 was unusual in that ACME had 3 paydays in February. What is the units digit of the next year in which ACME has 3 February paydays?\n• A.\n\n0\n\n• B.\n\n2\n\n• C.\n\n4\n\n• D.\n\n6\n\n• E.\n\n8\n\n• 14.\nFive murder suspects, including the murderer, are being interrogated by the police. Results of a polygraph indicate two of them are lying and three are telling the truth. If the polygraph results are correct, who is the murder?\n• A.\n\nSuspect A: “D is the murderer”\n\n• B.\n\nSuspect B: “I am innocent”\n\n• C.\n\nSuspect C: “It wasn’t E”\n\n• D.\n\nSuspect D: “A is lying”\n\n• E.\n\nSuspect E: “B is telling the truth”\n\n• 15.\nTwo arithmetic sequences are multiplied together to produce the sequence 468, 462, 384, …. What is the next term of this sequence?\n• A.\n\n234\n\n• B.\n\n286\n\n• C.\n\n300\n\n• D.\n\n324\n\n• E.\n\n336\n\n• 16.\nIn ΔABC, AB = 5, BC = 9, and AC = 7. Find the value of\n• A.\n\n1/8\n\n• B.\n\n7/9\n\n• C.\n\n3/2\n\n• D.\n\n9/7\n\n• E.\n\n8\n\n• 17.\nA pyramid has a square base 6 m on a side and a height of 9 m. Find the volume of the portion of the pyramid which lies above the base and below a plane parallel to the base and 3 m above the base.\n• A.\n\n32 m^3\n\n• B.\n\n36 M^3\n\n• C.\n\n64 M^3\n\n• D.\n\n72 M^3\n\n• E.\n\n76 M^3\n\n• 18.\nIn ΔABC, AB = AC and in ΔDEF, DE = DF. If AB is twice DE and ∠D is twice ∠A, then the ratio of the area of ΔABC to the area of ΔDEF is:\n• A.\n\nTan A\n\n• B.\n\n2 sec A\n\n• C.\n\nCsc 2A\n\n• D.\n\nSec A tan A\n\n• E.\n\nCot 2A\n\n• 19.\nIn hexagon PQRSTU, all interior angles = 120°. If PQ = RS = TU = 50, and QR = ST = UP = 100, find the area of the triangle bounded by QT, RU, and PS to the nearest tenth.\n• A.\n\n1082.5\n\n• B.\n\n1082.9\n\n• C.\n\n1083.3\n\n• D.\n\n1083.5\n\n• E.\n\n1083.9\n\n• 20.\nFor all integers k ≥ 0, P(k) = (2^2+2^1+1)(2^2-2^1+1)(2^4-2^2+1).... ()-1 is always the product of two integers n and n + 1. Find the smallest value of k for which n + (n + 1) ≥ 10^1000.\n• A.\n\n9\n\n• B.\n\n10\n\n• C.\n\n11\n\n• D.\n\n12\n\n• E.\n\n13" ]
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https://zbmath.org/?q=an%3A1252.65112
[ "## The discrete $$(G^{\\prime}/G)$$-expansion method applied to the differential-difference Burgers equation and the relativistic Toda lattice system.(English)Zbl 1252.65112\n\nSummary: We introduce the discrete $$(G^{\\prime}/G)$$-expansion method for solving nonlinear differential-difference equations (NDDEs). As illustrative examples, we consider the differential-difference Burgers equation and the relativistic Toda lattice system. Discrete solitary, periodic, and rational solutions are obtained in a concise manner. The method is also applicable to other types of NDDEs.\n\n### MSC:\n\n 65L03 Numerical methods for functional-differential equations 34K28 Numerical approximation of solutions of functional-differential equations (MSC2010) 34K13 Periodic solutions to functional-differential equations\n\n### Software:\n\nDDESpecialSolutions\nFull Text:\n\n### References:\n\n Fermi, Collected papers of Enrico Fermi II (1965) Tsuchida, Integrable semi-discretization of the coupled modified KdV equations, J Math Phys 39 pp 4785– (1998) · Zbl 0933.35176 Tsuchida, Integrable semi-discretization of the coupled nonlinear Schrödinger equations, J Phys A: Math Gen 32 pp 2239– (1999) · Zbl 0941.35112 Hu, Application of Hirota’s bilinear formalism to the Toeplitz lattice-some special soliton-like solutions, Phys Lett A 293 pp 161– (2002) · Zbl 0985.35072 Baldwin, Symbolic computation of hyperbolic tangent solutions for nonlinear differential-difference equations, Comput Phys Commun 162 pp 203– (2004) · Zbl 1196.68324 Liu, Periodic solutions for a class of nonlinear differential-difference equations, Commun Theor Phys 49 pp 1155– (2008) · Zbl 1392.34085 Dai, Symbolic computation of extended Jacobian elliptic function algorithm for nonlinear differential-different equations, Commun Theor Phys 43 pp 471– (2005) Zhu, Exp-function method for the hybrid-lattice system, Int J Nonlinear Sci 8 pp 461– (2007) · Zbl 06942293 Zhu, The homotopy perturbation method for discontinued problems arising in nanotechnology, Comput Math Appl 58 pp 2398– (2009) · Zbl 1189.65186 Xie, Some solutions of discrete sine-Gordon equation, Chaos Solitons Fract 33 pp 1791– (2007) · Zbl 1129.35456 Zhen, Discrete tanh method for nonlinear difference-differential equations, Comput Phys Commun 180 pp 1104– (2009) · Zbl 1198.65157 Yang, ADM-Padé technique for the nonlinear lattice equations, Appl Math Comput 210 pp 362– (2009) · Zbl 1162.65399 Aslan, A discrete generalization of the extended simplest equation method, Commun Nonlinear Sci Numer Simul 15 pp 1967– (2010) · Zbl 1222.65114 Wang, The (G’/G)-expansion method and traveling wave solutions of nonlinear evolution equations in mathematical physics, Phys Lett A 372 pp 417– (2008) · Zbl 1217.76023 Ganji, Exact traveling solutions of some nonlinear evolution equation by (G’/G)-expansion method, J Math Phys 50 pp 013519– (2009) Wang, Application of the (G’/G)-expansion to travelling wave solutions of the Broer-Kaup and the approximate long water wave equations, Appl Math Comput 206 pp 321– (2008) · Zbl 1157.65459 Ling-Xiao, The (G’/G)-expansion method and travelling wave solutions for a higher-order nonlinear schrödinger equation, Appl Math Comput 208 pp 440– (2009) · Zbl 1170.35536 Zayed, The (G’/G)-expansion method for finding traveling wave solutions of nonlinear partial differential equations in mathematical physics, J Math Phys 50 pp 013502– (2008) Aslan, Analytic study on two nonlinear evolution equations by using the (G’/G)-expansion method, Appl Math Comput 209 pp 425– (2009) · Zbl 1167.35451 Aslan, On the validity and reliability of the (G’/G)-expansion method by using higher-order nonlinear equations, Appl Math Comput 211 pp 531– (2009) · Zbl 1162.65391 Öziş, Symbolic computation and construction of new exact traveling wave solutions to Fitzhugh-Nagumo and Klein-Gordon equations, Z Naturforsch 64a pp 15– (2009) Öziş, Symbolic computations and exact and explicit solutions of some nonlinear evolution equations in mathematical physics, Commun Theor Phys 51 pp 577– (2009) · Zbl 1181.35247 Aslan, Exact and explicit solutions to some nonlinear evolution equations by utilizing the (G’/G)-expansion method, Appl Math Comput 215 pp 857– (2009) · Zbl 1176.35144 Öziş, Application of the (G’/G)-expansion method to Kawahara type equations using symbolic computation, Appl Math Comput Zhang, A generalized (G’/G)-expansion method and its applications, Phys Lett A 372 pp 3653– (2008) · Zbl 1220.37070 Zhang, A generalized (G’/G)-expansion method for the mKdV equation with variable coefficients, Phys Lett A 372 pp 2254– (2008) · Zbl 1220.37072 Zhang, The (G’/G)-expansion method for nonlinear differential-difference equations, Phys Lett A 373 pp 905– (2009) · Zbl 1228.34096 Aslan, Discrete exact solutions to some nonlinear differential-difference equations via the (G’/G)-expansion method, Appl Math Comput 215 pp 3140– (2009) · Zbl 1186.34004 Hirota, The direct method in soliton theory (2004) · Zbl 1099.35111 Ablowitz, Soliton, nonlinear evolution equations and inverse scattering (1991) Toda, Theory of nonlinear lattices (1981) · Zbl 0465.70014 Yaxuan, Rational formal solutions of differential-difference equations, Chaos Solitons Fract 33 pp 1642– (2007) · Zbl 1153.35398\nThis reference list is based on information provided by the publisher or from digital mathematics libraries. Its items are heuristically matched to zbMATH identifiers and may contain data conversion errors. It attempts to reflect the references listed in the original paper as accurately as possible without claiming the completeness or perfect precision of the matching." ]
[ null ]
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https://stackoverflow.com/questions/15125920/how-to-get-distinct-values-from-an-array-of-objects-in-javascript/15125980
[ "# How to get distinct values from an array of objects in JavaScript?\n\nAssuming I have the following:\n\n``````var array =\n[\n{\"name\":\"Joe\", \"age\":17},\n{\"name\":\"Bob\", \"age\":17},\n{\"name\":\"Carl\", \"age\": 35}\n]\n``````\n\nWhat is the best way to be able to get an array of all of the distinct ages such that I get an result array of:\n\n``````[17, 35]\n``````\n\nIs there some way I could alternatively structure the data or better method such that I would not have to iterate through each array checking the value of \"age\" and check against another array for its existence, and add it if not?\n\nIf there was some way I could just pull out the distinct ages without iterating...\n\nCurrent inefficent way I would like to improve... If it means that instead of \"array\" being an array of objects, but a \"map\" of objects with some unique key (i.e. \"1,2,3\") that would be okay too. Im just looking for the most performance efficient way.\n\nThe following is how I currently do it, but for me, iteration appears to just be crummy for efficiency even though it does work...\n\n``````var distinct = []\nfor (var i = 0; i < array.length; i++)\nif (array[i].age not in distinct)\ndistinct.push(array[i].age)\n``````\n• iteration isn't \"crummy for efficiency\" and you can't do anything to every element \"without iterating\". you can use various functional-looking methods, but ultimately, something on some level has to iterate over the items. – Eevee Feb 28 '13 at 1:47\n\nIf this were PHP I'd build an array with the keys and take `array_keys` at the end, but JS has no such luxury. Instead, try this:\n\n``````var flags = [], output = [], l = array.length, i;\nfor( i=0; i<l; i++) {\nif( flags[array[i].age]) continue;\nflags[array[i].age] = true;\noutput.push(array[i].age);\n}\n``````\n• If it were PHP you'd use `array_unique`, wouldn't you? – Barmar Feb 28 '13 at 2:02\n• No, because `array_unique` would compare the entire item, not just the age as is asked here. – Niet the Dark Absol Feb 28 '13 at 2:18\n• I think `flags = {}` is more better than `flags = []` – zhuguowei Jun 12 '17 at 9:35\n• @zhuguowei perhaps, although there's nothing really wrong with sparse arrays - and I also assumed that `age` is a relatively small integer (<120 surely) – Niet the Dark Absol Jun 12 '17 at 14:56\n• how we could also print out the total number of people that have same age? – user1788736 Mar 20 at 1:43\n\nIf you are using ES6/ES2015 or later you can do it this way:\n\n``````const unique = [...new Set(array.map(item => item.age))];\n``````\n\nHere is an example on how to do it.\n\n• I get an error : `TypeError: (intermediate value).slice is not a function` – AngJobs on Github Jul 13 '16 at 10:28\n• @Thomas ... means spread operator. In this case it means create new set and spread it in a list. You can find more about it here: developer.mozilla.org/en-US/docs/Web/JavaScript/Reference/… – Vlad Bezden Jun 16 '17 at 14:09\n• for typescript you have to use new Set wrapped in Array.from()... i will provide that answer below. @AngJobs – Christian Matthew Aug 25 '17 at 16:24\n• is it possible to find out unique objects based on multiple keys in the object? – Jefree Sujit Nov 3 '17 at 12:24\n• This solution was give almost verbatim a few months earlier by @Russell Vea. Did you check for existing answers? But then again, 266+ votes show that nobody else checked either. – Dan Dascalescu Sep 28 '18 at 3:18\n\nusing ES6\n\n``````let array = [\n{ \"name\": \"Joe\", \"age\": 17 },\n{ \"name\": \"Bob\", \"age\": 17 },\n{ \"name\": \"Carl\", \"age\": 35 }\n];\narray.map(item => item.age)\n.filter((value, index, self) => self.indexOf(value) === index)\n\n> [17, 35]\n``````\n• Dang, I love one-liners! – James Harrington Nov 11 '17 at 8:32\n• If I want to get the value with it's index then how can I get Example: I want to get {\"name\": \"Bob\", \"age\":\"17\"},{\"name\": \"Bob\", \"age\":\"17\"} – Abdullah Al Mamun Sep 12 '18 at 3:51\n• That's why you have to keep scrolling – Alejandro Bastidas Sep 12 '18 at 19:42\n• @AbdullahAlMamun you can use map in .filter instead of call .map first, like this: `array.filter((value, index, self) => self.map(x => x.age).indexOf(value.age) == index)` – Leo Sep 14 '18 at 13:42\n• ps: .map inside .filter can be slow, so be careful with large arrays – Leo Sep 14 '18 at 13:53\n\nYou could use a dictionary approach like this one. Basically you assign the value you want to be distinct as the key in a dictionary. If the key did not exist then you add that value as distinct.\n\n``````var unique = {};\nvar distinct = [];\nfor( var i in array ){\nif( typeof(unique[array[i].age]) == \"undefined\"){\ndistinct.push(array[i].age);\n}\nunique[array[i].age] = 0;\n}\n``````\n\nHere is a working demo: http://jsfiddle.net/jbUKP/1\n\nThis will be O(n) where n is the number of objects in array and m is the number of unique values. There is no faster way than O(n) because you must inspect each value at least once.\n\nPerformance\n\nhttp://jsperf.com/filter-versus-dictionary When I ran this dictionary was 30% faster.\n\n• fast, and without any additional plugins required. Really cool – mihai Dec 14 '15 at 21:41\n• how about `if( typeof(unique[array[i].age]) == \"undefined\"){ distinct.push(array[i].age); unique[array[i].age] = 0; }` – Timeless Oct 7 '16 at 4:47\n• Wow the performance has really changed in favour of the map option. Click that jsperf link! – A T Apr 2 '17 at 15:53\n• @98percentmonkey - The object was used to facilitate the \"dictionary approach\". Inside the object, each occurrence being tracked is added as a key (or a bin). This way, when we come across an occurrence, we can check to see if the key (or bin) exists; if it does exist, we know that the occurrence is not unique - if it does not exist, we know that the occurrence is unique and add it in. – Travis J Jul 31 '18 at 20:02\n• @98percentmonkey - The reason for using an object is that the lookup is O(1) since it checks for a property name once, whereas an array is O(n) since it has to look at every value to check for existence. At the end of the process, the set of keys (bins) in the object represents the set of unique occurrences. – Travis J Jul 31 '18 at 20:02\n\nthis is how you would solve this using new Set via ES6 for Typescript as of August 25th, 2017\n\n``````Array.from(new Set(yourArray.map((item: any) => item.id)))\n``````\n• this helped, was getting before thanks. Type 'Set' is not an array type – robert king Apr 5 '18 at 23:38\n\nUsing ES6 features, you could do something like:\n\n``````const uniqueAges = [...new Set( array.map(obj => obj.age)) ];\n``````\n• This approach will only work on primitive types (which is the case here as ages are an array of numbers) yet will fail for objects. – k0pernikus Jun 24 at 13:22\n• any idea how to make it work for objects with two keys? – cegprakash Sep 5 at 12:40\n\nI'd just map and remove dups:\n\n``````var ages = array.map(function(obj) { return obj.age; });\nages = ages.filter(function(v,i) { return ages.indexOf(v) == i; });\n\nconsole.log(ages); //=> [17, 35]\n``````\n\nEdit: Aight! Not the most efficient way in terms of performance, but the simplest most readable IMO. If you really care about micro-optimization or you have huge amounts of data then a regular `for` loop is going to be more \"efficient\".\n\n• note that this is O(n²) – Eevee Feb 28 '13 at 1:46\n• @elclanrs - \"the most performance efficient way\" - This approach is slow. – Travis J Feb 28 '13 at 1:47\n• @Eevee: I see. The underscore version in your answer is not very fast either, I mean, in the end you choose what's more convenient, I doubt 1-30% more or less reflects \"huge improvement\" in generic tests and when OP/s are in the thousands. – elclanrs Feb 28 '13 at 1:58\n• well, sure. with only three elements, the fastest thing is to make three variables and use some `if`s. you'll get some very different results with three million. – Eevee Feb 28 '13 at 2:06\n• not fast but in my case it did the trick as I'm not dealing with a large dataset, thanks. – Felipe Alarcon Feb 4 '18 at 15:26\n``````var unique = array\n.map(p => p.age)\n.filter((age, index, arr) => arr.indexOf(age) == index)\n.sort(); // sorting is optional\n\n// or in ES6\n\nvar unique = [...new Set(array.map(p => p.age))];\n``````\n• While this code may answer the question, providing additional context regarding how and why it solves the problem would improve the answer's long-term value. – Alexander Dec 16 '18 at 16:52\n\nThe `forEach` version of @travis-j's answer (helpful on modern browsers and Node JS world):\n\n``````var unique = {};\nvar distinct = [];\narray.forEach(function (x) {\nif (!unique[x.age]) {\ndistinct.push(x.age);\nunique[x.age] = true;\n}\n});\n``````\n\n34% faster on Chrome v29.0.1547: http://jsperf.com/filter-versus-dictionary/3\n\nAnd a generic solution that takes a mapper function (tad slower than direct map, but that's expected):\n\n``````function uniqueBy(arr, fn) {\nvar unique = {};\nvar distinct = [];\narr.forEach(function (x) {\nvar key = fn(x);\nif (!unique[key]) {\ndistinct.push(key);\nunique[key] = true;\n}\n});\nreturn distinct;\n}\n\n// usage\nuniqueBy(array, function(x){return x.age;}); // outputs [17, 35]\n``````\n• I like the generic solution best since it's unlikely that age is the only distinct value needed in a real world scenario. – Toft Nov 1 '13 at 11:17\n• In the generic, change \"distinct.push(key)\" to \"distinct.push(x)\" to return a list of the actual elements, which I find highly usable! – Silas Hansen Aug 28 '14 at 12:56\n\nThere are many valid answers already, but I wanted to add one that uses only the `reduce()` method because it is clean and simple.\n\n``````function uniqueBy(arr, prop){\nreturn arr.reduce((a, d) => {\nif (!a.includes(d[prop])) { a.push(d[prop]); }\nreturn a;\n}, []);\n}\n``````\n\nUse it like this:\n\n``````var array = [\n{\"name\": \"Joe\", \"age\": 17},\n{\"name\": \"Bob\", \"age\": 17},\n{\"name\": \"Carl\", \"age\": 35}\n];\n\nvar ages = uniqueBy(array, \"age\");\nconsole.log(ages); // [17, 35]\n``````\n\nI've started sticking Underscore in all new projects by default just so I never have to think about these little data-munging problems.\n\n``````var array = [{\"name\":\"Joe\", \"age\":17}, {\"name\":\"Bob\", \"age\":17}, {\"name\":\"Carl\", \"age\": 35}];\nconsole.log(_.chain(array).map(function(item) { return item.age }).uniq().value());\n``````\n\nProduces `[17, 35]`.\n\nusing lodash\n\n``````var array = [\n{ \"name\": \"Joe\", \"age\": 17 },\n{ \"name\": \"Bob\", \"age\": 17 },\n{ \"name\": \"Carl\", \"age\": 35 }\n];\n_.chain(array).pluck('age').unique().value();\n> [17, 35]\n``````\n• Can you explain how to do this with plain javascript as is implied in the question? – Ruskin Jan 21 '15 at 14:06\n• it is an underscore function _.chain – vini May 28 '15 at 19:00\n• lodash has also – Ivan Nosov May 29 '15 at 20:46\n• but pluck() is not in lodash. – Yash Vekaria Nov 29 '16 at 10:57\n• _.chain(array).map('age').unique().value(); worked for me. – Yash Vekaria Nov 29 '16 at 11:07\n\nHere's another way to solve this:\n\n``````var result = {};\nfor(var i in array) {\nresult[array[i].age] = null;\n}\nresult = Object.keys(result);\n``````\n\nI have no idea how fast this solution is compared to the others, but I like the cleaner look. ;-)\n\nEDIT: Okay, the above seems to be the slowest solution of all here.\n\nI've created a performance test case here: http://jsperf.com/distinct-values-from-array\n\nInstead of testing for the ages (Integers), I chose to compare the names (Strings).\n\nMethod 1 (TS's solution) is very fast. Interestingly enough, Method 7 outperforms all other solutions, here I just got rid of .indexOf() and used a \"manual\" implementation of it, avoiding looped function calling:\n\n``````var result = [];\nloop1: for (var i = 0; i < array.length; i++) {\nvar name = array[i].name;\nfor (var i2 = 0; i2 < result.length; i2++) {\nif (result[i2] == name) {\ncontinue loop1;\n}\n}\nresult.push(name);\n}\n``````\n\nThe difference in performance using Safari & Firefox is amazing, and it seems like Chrome does the best job on optimization.\n\nI'm not exactly sure why the above snippets is so fast compared to the others, maybe someone wiser than me has an answer. ;-)\n\nunderscore.js `_.uniq(_.pluck(array,\"age\"))`\n\n• Please add an explanation of how this answers the question. – Robotic Cat May 2 '16 at 17:43\n• _.pluck has been removed in favor of _.map – Ajax3.14 Sep 25 '16 at 9:42\n\nUsing Lodash\n\n``````var array = [\n{ \"name\": \"Joe\", \"age\": 17 },\n{ \"name\": \"Bob\", \"age\": 17 },\n{ \"name\": \"Carl\", \"age\": 35 }\n];\n\n_.chain(array).map('age').unique().value();\n``````\n\nReturns [17,35]\n\n``````function get_unique_values_from_array_object(array,property){\nvar unique = {};\nvar distinct = [];\nfor( var i in array ){\nif( typeof(unique[array[i][property]]) == \"undefined\"){\ndistinct.push(array[i]);\n}\nunique[array[i][property]] = 0;\n}\nreturn distinct;\n}\n``````\n• worked like a charm! – CJLopez Feb 16 '17 at 17:23\n• thats what i really needed. thanks alot – MajiD Dec 11 '18 at 12:21\n\ni think you are looking for groupBy function (using Lodash)\n\n``````_personsList = [{\"name\":\"Joe\", \"age\":17},\n{\"name\":\"Bob\", \"age\":17},\n{\"name\":\"Carl\", \"age\": 35}];\n_uniqAgeList = _.groupBy(_personsList,\"age\");\n_uniqAges = Object.keys(_uniqAgeList);\n``````\n\nproduces result:\n\n``````17,35\n``````\n\njsFiddle demo:http://jsfiddle.net/4J2SX/201/\n\nHere's a versatile solution that uses reduce, allows for mapping, and maintains insertion order.\n\nitems: An array\n\nmapper: A unary function that maps the item to the criteria, or empty to map the item itself.\n\n``````function distinct(items, mapper) {\nif (!mapper) mapper = (item)=>item;\nreturn items.map(mapper).reduce((acc, item) => {\nif (acc.indexOf(item) === -1) acc.push(item);\nreturn acc;\n}, []);\n}\n``````\n\nUsage\n\n``````const distinctLastNames = distinct(items, (item)=>item.lastName);\nconst distinctItems = distinct(items);\n``````\n\nYou can add this to your Array prototype and leave out the items parameter if that's your style...\n\n``````const distinctLastNames = items.distinct( (item)=>item.lastName) ) ;\nconst distinctItems = items.distinct() ;\n``````\n\nYou can also use a Set instead of an Array to speed up the matching.\n\n``````function distinct(items, mapper) {\nif (!mapper) mapper = (item)=>item;\nreturn items.map(mapper).reduce((acc, item) => {\nreturn acc;\n}, new Set());\n}\n``````\n\nJust found this and I thought it's useful\n\n``````_.map(_.indexBy(records, '_id'), function(obj){return obj})\n``````\n\nAgain using underscore, so if you have an object like this\n\n``````var records = [{_id:1,name:'one', _id:2,name:'two', _id:1,name:'one'}]\n``````\n\nit will give you the unique objects only.\n\nWhat happens here is that `indexBy` returns a map like this\n\n``````{ 1:{_id:1,name:'one'}, 2:{_id:2,name:'two'} }\n``````\n\nand just because it's a map, all keys are unique.\n\nThen I'm just mapping this list back to array.\n\nIn case you need only the distinct values\n\n``````_.map(_.indexBy(records, '_id'), function(obj,key){return key})\n``````\n\nKeep in mind that the `key` is returned as a string so, if you need integers instead, you should do\n\n``````_.map(_.indexBy(records, '_id'), function(obj,key){return parseInt(key)})\n``````\n\nIf you have Array.prototype.includes or are willing to polyfill it, this works:\n\n``````var ages = []; array.forEach(function(x) { if (!ages.includes(x.age)) ages.push(x.age); });\n``````\n\nMy below code will show the unique array of ages as well as new array not having duplicate age\n\n``````var data = [\n{\"name\": \"Joe\", \"age\": 17},\n{\"name\": \"Bob\", \"age\": 17},\n{\"name\": \"Carl\", \"age\": 35}\n];\n\nvar unique = [];\nvar tempArr = [];\ndata.forEach((value, index) => {\nif (unique.indexOf(value.age) === -1) {\nunique.push(value.age);\n} else {\ntempArr.push(index);\n}\n});\ntempArr.reverse();\ntempArr.forEach(ele => {\ndata.splice(ele, 1);\n});\nconsole.log('Unique Ages', unique);\nconsole.log('Unique Array', data);```\n``````\n\n``````const x = [\n{\"id\":\"93\",\"name\":\"CVAM_NGP_KW\"},\n{\"id\":\"94\",\"name\":\"CVAM_NGP_PB\"},\n{\"id\":\"93\",\"name\":\"CVAM_NGP_KW\"},\n{\"id\":\"94\",\"name\":\"CVAM_NGP_PB\"}\n].reduce(\n(accumulator, current) => accumulator.some(x => x.id === current.id)? accumulator: [...accumulator, current ], []\n)\n\nconsole.log(x)\n\n/* output\n[\n{ id: '93', name: 'CVAM_NGP_KW' },\n{ id: '94', name: 'CVAM_NGP_PB' }\n]\n*/``````\n\n• this looks like O(n^2) – cegprakash Sep 5 at 12:56\n\nIf like me you prefer a more \"functional\" without compromising speed, this example uses fast dictionary lookup wrapped inside reduce closure.\n\n``````var array =\n[\n{\"name\":\"Joe\", \"age\":17},\n{\"name\":\"Bob\", \"age\":17},\n{\"name\":\"Carl\", \"age\": 35}\n]\nvar uniqueAges = array.reduce((p,c,i,a) => {\nif(!p[c.age]) {\np.push(p[c.age] = c.age);\n}\nif(i<a.length-1) {\nreturn p\n} else {\nreturn p\n}\n}, [{},[]])\n``````\n\nAccording to this test my solution is twice as fast as the proposed answer\n\n``````unique(obj, prop) {\nlet result = [];\nlet seen = new Set();\n\nObject.keys(obj)\n.forEach((key) => {\nlet value = obj[key];\n\nlet test = !prop\n? value\n: value[prop];\n\n!seen.has(test)\n&& result.push(value);\n});\n\nreturn result;\n}\n``````\n\nThere is a library which provides strongly-typed, queryable collections in typescript.\n\nThe collections are:\n\n• List\n• Dictionary\n\nThe library is called ts-generic-collections.\n\nSource code on GitHub:\n\nhttps://github.com/VeritasSoftware/ts-generic-collections\n\nYou can get distinct values like below\n\n`````` it('distinct', () => {\nlet numbers: number[] = [1, 2, 3, 1, 3];\nlet list = new List(numbers);\n\nlet distinct = list.distinct(new EqualityComparer());\n\nexpect(distinct.length == 3);\nexpect(distinct.elementAt(0) == 1);\nexpect(distinct.elementAt(1) == 2);\nexpect(distinct.elementAt(2) == 3);\n});\n\nclass EqualityComparer implements IEqualityComparer<number> {\nequals(x: number, y: number) : boolean {\nreturn x == y;\n}\n}\n``````\n\nUsing new Ecma features are great but not all users have those available yet.\n\nFollowing code will attach a new function named distinct to the Global Array object. If you are trying get distinct values of an array of objects, you can pass the name of the value to get the distinct values of that type.\n\n``````Array.prototype.distinct = function(item){ var results = [];\nfor (var i = 0, l = this.length; i < l; i++)\nif (!item){\nif (results.indexOf(this[i]) === -1)\nresults.push(this[i]);\n} else {\nif (results.indexOf(this[i][item]) === -1)\nresults.push(this[i][item]);\n}\nreturn results;};\n``````\n\nCheck out my post in CodePen for a demo.\n\nJust try\n\n``````var x = [] ;\nfor (var i = 0 ; i < array.length ; i++)\n{\nif(x.indexOf(array[i]['age']) == -1)\n{\nx.push(array[i]['age']);\n}\n}\nconsole.log(x);\n``````\n\nSimple one-liner with great performance. 6% faster than the ES6 solutions in my tests.\n\nvar ages = array.map(function(o){return o.age}).filter(function(v,i,a){return a.indexOf(v)===i});\n\nI know this is an old and relatively well-answered question and the answer I'm giving will get the complete-object back (Which I see suggested in a lot of the comments on this post). It may be \"tacky\" but in terms of readability seems a lot cleaner (although less efficient) than a lot of other solutions.\n\nThis will return a unique array of the complete objects inside the array.\n\n``````let productIds = data.map(d => {\nreturn JSON.stringify({\nid : d.sku.product.productId,\nname : d.sku.product.name,\nprice : `\\${d.sku.product.price.currency} \\${(d.sku.product.price.gross / d.sku.product.price.divisor).toFixed(2)}`\n})\n})\nproductIds = [ ...new Set(productIds)].map(d => JSON.parse(d))```\n``````\n\nI wrote my own in TypeScript, for a generic case, like that in Kotlin's `Array.distinctBy {}`...\n\n``````function distinctBy<T, U extends string | number>(array: T[], mapFn: (el: T) => U) {\nconst uniqueKeys = new Set(array.map(mapFn));\nreturn array.filter((el) => uniqueKeys.has(mapFn(el)));\n}\n``````\n\nWhere `U` is hashable, of course. For Objects, you might need https://www.npmjs.com/package/es6-json-stable-stringify\n\n## protected by adigaJul 14 at 8:53\n\nThank you for your interest in this question. Because it has attracted low-quality or spam answers that had to be removed, posting an answer now requires 10 reputation on this site (the association bonus does not count).\n\nWould you like to answer one of these unanswered questions instead?" ]
[ null ]
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https://www.askiitians.com/forums/Magical-Mathematics%5BInteresting-Approach%5D/29/28441/qadratic-equation.htm
[ "#### Thank you for registering.\n\nOne of our academic counsellors will contact you within 1 working day.\n\nClick to Chat\n\n1800-5470-145\n\n+91 7353221155\n\nCART 0\n\n• 0\nMY CART (5)\n\nUse Coupon: CART20 and get 20% off on all online Study Material\n\nITEM\nDETAILS\nMRP\nDISCOUNT\nFINAL PRICE\nTotal Price: Rs.\n\nThere are no items in this cart.\nContinue Shopping\n\n# An aeroplane lefts 30 minute later than it's shedule time and in order to reach its destination 1500 km away in time. It had to increase its speed by 250 km/hr. from its usual speed. Determine its usual time.\n\n10 years ago\n\nLet the usual speed of the plane be 'x' hours\n\nTime taken to cover 1500km with usual speed = 1500/x hrs\n\ntime taken to cover 1500km with speed of (x+250) = 1500/(x+250) hrs\n\n1500/x = 1500/(x+250) + 1/2\n\n1500/x - 1500/(x+250) = 1/2\n\n1500x + 1500*250 - 1500x / (x*(x+250)) = 1/2\n\n1500*250 / x2+250x = 1/2\n\n750000 = x2 + 250x\n\nx2+250x - 750000 = 0\n\nx2 + 1000x - 750x - 750000 = 0\n\nx ( x+1000) - 750 (x+1000) =0\n\n(x+1000)(x-750) = 0\n\nwhich means x = -1000 , which is not possible , as speed cannot be negative\n\nor x = 750\n\nso the usual speed of the plane is 750 kmph\n\nusual time = distance / speed = 1500 / 750 = 150/75 = 2 hours !" ]
[ null ]
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https://www.cs.sfu.ca/~kabanets/Research/poly.html
[ "## Derandomizing Polynomial Identity Tests means proving circuit lower bounds\n\n### Abstract\n\nWe show that derandomizing the Polynomial Identity Testing is, essentially, equivalent to proving circuit lower bounds for NEXP. More precisely, we prove that if one can test in polynomial time (or, even, nondeterministic subexponential time, infinitely often) whether a given arithmetic circuit over integers computes an identically zero polynomial, then either (i) NEXP ⊄ P/poly or (ii) Permanent is not computable by polynomial-size arithmetic circuits. We also prove a (partial) converse: If Permanent requires superpolynomial-size arithmetic circuits, then one can test in subexponential time whether a given arithmetic formula computes an identically zero polynomial.\n\nSince the Polynomial Identity Testing is a coRP problem, we obtain the following corollary: If RP=P (or, even, coRP ⊆ ∩ε>0 NTIME(2nε), infinitely often), then NEXP is not computable by polynomial-size arithmetic circuits. Thus, establishing that RP=coRP or BPP=P would require proving superpolynomial lower bounds for Boolean or arithmetic circuits. We also show that any derandomization of RNC would yield new circuit lower bounds for a language in NEXP.\n\nOur techniques allow us to prove an unconditional circuit lower bound for a language in NEXPRP: we prove that either (i) Permanent is not computable by polynomial-size arithmetic circuits, or (ii) NEXPRP ⊄ P/poly.\n\nFinally, we prove that NEXP ⊄ P/poly if both BPP=P and the low-degree testing is in P; here, the low-degree testing is the problem of checking whether a given Boolean circuit computes a function that is close to some low-degree polynomial over a finite field.\n\n### Versions\n\n• journal version in Computational Complexity, 13(1-2), pages 1-46, 2004.\n• extended abstract in Proceedings of the Thirty-Fifth Annual ACM Symposium on Theory of Computing (STOC'03), pages 355-364, 2003." ]
[ null ]
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https://www.arxiv-vanity.com/papers/1502.02529/
[ "# Higher order operator splitting Fourier spectral methods for the Allen–Cahn equation\n\nJaemin Shin Hyun Geun Lee June-Yub Lee Institute of Mathematical Sciences, Ewha Womans University, Seoul 120-750, Korea Department of Mathematics, Ewha Womans University, Seoul 120-750, Korea Corresponding author\n31 December 2014\n###### Abstract\n\nThe Allen–Cahn equation is solved numerically by operator splitting Fourier spectral methods. The basic idea of the operator splitting method is to decompose the original problem into sub-equations and compose the approximate solution of the original equation using the solutions of the subproblems. Unlike the first and the second order methods, each of the heat and the free-energy evolution operators has at least one backward evaluation in higher order methods. We investigate the effect of negative time steps on a general form of third order schemes and suggest three third order methods for better stability and accuracy. Two fourth order methods are also presented. The traveling wave solution and a spinodal decomposition problem are used to demonstrate numerical properties and the order of convergence of the proposed methods.\n\n###### keywords:\nOperator splitting method; Allen–Cahn equation; Heat evolution equation; Free-energy evolution equation; Backward time step; Traveling wave solution; Spinodal decomposition;\n\n, , and\n\n## 1 Introduction\n\nThe Allen–Cahn (AC) equation was originally introduced as a phenomenological model for antiphase domain coarsening in a binary alloy :\n\n ∂ϕ(x,t)∂t=−F′(ϕ(x,t))ϵ2+Δϕ(x,t),x∈Ω, 0\n\nwhere is a domain in . The quantity is defined as the difference between the concentrations of two components in a mixture, for example, where and are the masses of phases and . The function is the Helmholtz free-energy density for , which has a double-well form, and is the gradient energy coefficient. The system is completed by taking an initial condition and a homogeneous Neumann boundary condition , where is normal to .\n\nThe AC equation and its various modified forms have been applied in addressing a range of problems, such as phase transitions , image analysis [2, 3], motion by mean curvature [4, 5, 6], two-phase fluid flows , and crystal growth [8, 9, 10]. Therefore, many researchers have studied numerical methods for solving the AC type equation to improve stability and accuracy and to have a better understanding of its dynamics. Stable time step size of explicit schemes is severely restricted due to the nonlinear term and implicit schemes suffer from a solvability problem with large time steps. One of considerable semi-implicit methods is unconditionally gradient stable method proposed by Eyre , which is first order accurate in time, and unconditionally gradient stable means that a discrete energy non-increases from one time level to the next regardless of the time step size. And the authors in [12, 13] proposed first and second order stabilized semi-implicit methods.\n\nAnother numerical method employed for solving the AC equation is the operator splitting method [12, 14, 15]. Operator splitting schemes have been applied for many types of evolution equations [16, 17, 18, 19, 20, 21]. The basic idea of the operator splitting method is to decompose the original problem into subproblems which are simpler than the original problem and then to compose the approximate solution of the original problem by using the exact or approximate solutions of the subproblems in a given sequential order. Operator splitting methods are simple to implement and computationally efficient to achieve higher order accuracy while semi-implicit schemes are hard to improve the order of convergence. The first and the second order operator splitting methods for the AC equation is quite well-known [12, 14, 15], however, the higher order (more than two) operator splitting method for the AC equation is less well-known.\n\nIn this paper, we investigate higher order operator splitting schemes and propose several higher order methods to solve the AC equation with a Fourier spectral method. We decompose the AC equation into heat and free-energy evolution equations, which have closed-form solutions in the Fourier and physical spaces, respectively. Because the first and second operator splitting methods have only forward time steps, the boundedness of the solution is guaranteed regardless of the time step size . However, we could not guarantee the stability with large time step size since each operator has at least one backward time step with third and higher order of accuracy [17, 18]. Because a backward time marching affects numerical stability on both sub-equations, we consider ways of minimizing the effect of negative time steps and introduce a cut-off function to limit the exponential amplification of high-frequency modes in solving the heat evolution equation.\n\nThis paper is organized as follows. In section 2, we briefly review the operator splitting methods which are studied by the authors in . In section 3, we present higher order operator splitting Fourier spectral methods for solving the AC equation. We discuss the stability issues for backward time marching and suggest the three third order operator splitting methods. We present numerical experiments demonstrating numerical properties and the order of convergence of the proposed methods in section 4. Conclusions are drawn in section 5.\n\n## 2 A brief review on the operator splitting method\n\nIn this section, we review some of the basic properties of the operator splitting methods for a time evolution equation with two evolution terms in summarizing the work by D. Goldman and T. Kapper . Let be the solution operator for the time evolution equation , that is , and be the solution operator for . Then the operators and satisfy the semi-group properties. Suppose we want to minimize the number of the operator evaluations of and in order to get a -th order approximation of the following ordinary differential equation consists of two evolution terms,\n\n ∂ϕ∂t=fA(ϕ)+fB(ϕ). (2)\n\nIt is well-known that the simplest form of the first order solution operator for (2) is given as\n\n S(1)=BΔtAΔt, (3)\n\nthat is, is a first order accurate approximation of . Here the choice of and (or and ) is arbitrary, thus without loss of generality, we may assume that the first operator evaluated is always .\n\nWe now consider a solution operator with (or if ) evaluations of the operators and in the following form,\n\n S(p)=BbpΔtAapΔt⋯Bb1ΔtAa1Δt, (4)\n\nwhere all of , are non-zeros. The coefficients and in must satisfy certain conditions to make an -th order approximation operator for (2). It is well-known that there exists at least -th order accurate when . (See and the references therein for the derivation of the following conditions.) For first-order accuracy, , must satisfy\n\n p∑j=1aj=p∑j=1bj=1. (5)\n\nFor second-order accuracy, and must satisfy (5) and the conditions\n\n (6)\n\nFor third-order accuracy, and must satisfy (5), (6), and the conditions\n\n p∑j=2aj(j−1∑k=1bk)2=p∑j=1bj(j∑k=1ak)2=13. (7)\n\nFor a second-order scheme of the form (4) with , , (5) and (6) give\n\n a1+a2=1,b1+b2=1,a2b1=12. (8)\n\nSince there are three equations for the four unknowns, let be a free parameter, then the solution of (8) gives a general form of a second order solution operator with up to 4 operator evaluations,\n\n S(2)ω=B(1−ω)ΔtA12ωΔtBωΔtA(1−12ω)Δt. (9)\n\nNote that\n\nFor a third-order scheme of the form\n\n S(3)=Bb3ΔtAa3ΔtBb2ΔtAa2ΔtBb1ΔtAa1Δt, (10)\n\n(5), (6), and (7) give\n\n a1+a2+a3=1,b1+b2+b3=1,a2b1+a3(b1+b2)=12, (11)\n a2b21+a3(b1+b2)2=13,b1a21+b2(a1+a2)2+b3=13. (12)\n\nChoosing to be a free parameter, we can obtain two branches of the solution for (11) and (12),\n\n b±1=1−ω2∓√D(ω)2(4ω−1),a2=4ω−12(3ω−1),a±3=12−b±1a21−ω,\n a±1=1−a2−a±3,b±2=1−b±1−b3,\n\nwhere\n\n D(ω)=(ω−1)2(4ω−1)2+12(4ω−1)(ω−13)2.\n\nNote that real solutions of (11) and (12) are only possible for and , where is the real root of .", null, "Figure 1: Positive branch solutions, a+1,b+1,a+2,b+2,a+3,b+3 as a function of b+3=ω", null, "Figure 2: Negative branch solutions, a−1,b−1,a−2,b−2,a−3,b−3 as a function of b−3=ω\n\nFigure 1 shows the positive branch solutions, as a function of for the third order operator and Figure 2 shows the negative branch solutions for . In any case, there exists exactly one negative value among and also only one negative value among . There are three special cases when the solutions may blow up. As , with , degenerates into a second order operator,\n\nWe remark that a symmetric with , , and satisfying (5), (6) has only a second-order accuracy, that is, , , and does not satisfy (7). However, a symmetric with , , , and satisfying only (5), (6), and (7),\n\n S(4)U:=Aω2ΔtBωΔtA1−ω2ΔtB(1−2ω)ΔtA1−ω2ΔtBωΔtAω2Δt (13)\n\nhappens to be a fourth-order accuracy with , , and . This is the simplest form of fourth order operator with only 7 operator evaluations and this can be derived as a symmetric combination of a second order operator\n\n S(4)U:=TωΔtT(1−2ω)ΔtTωΔt,ω=ωU.\n\nAnother a well-known fourth order operator splitting method  can be also derived as a symmetric combination of the second order operator ,\n\n S(6)V := TωΔtTωΔtT(1−4ω)ΔtTωΔtTωΔt =\n\nwith . The method is computationally less efficient (11 operator evaluations compared to minimum of 7 evaluations) but has better stability condition (, ) than the method defined in (13).\n\nWe close this section with a remark that not just the third and the fourth order methods mentioned above but any operator splitting methods of third or higher order contains at least one negative time steps for each of the operators, , . (See [17, 18] for the proof of the general theorem.)\n\n## 3 Higher-order operator splitting Fourier spectral methods\n\nWe consider the AC equation (1) in one-dimensional space . Two- and three-dimensional spaces can be analogously defined. For simplicity of notation, we sometimes abuse the notation referring and define the “free-energy evolution operator as follows\n\n FΔt(ϕ(tn)):=ϕ(tn+Δt), (15)\n\nwhere is a solution of the first order differential equation\n\n ∂ϕ∂t=−F′(ϕ)ϵ2\n\nwith an initial condition . For given , we have an analytical formula (See [12, 14, 15]) for the evolution operator in the physical space\n\n FΔt(ϕ)=ϕ√ϕ2+(1−ϕ2)e−2Δtϵ2. (16)\n\nWe also define the “heat evolution operator as follows\n\n HΔt(ϕ(tn)):=ϕ(tn+Δt), (17)\n\nwhere is a solution of the first order differential equation\n\n ∂ϕ∂t=Δϕ\n\nwith an initial condition . In this paper, we employ the discrete cosine transform to solve the AC equation with the zero Neumann boundary condition: for ,\n\n ˆϕk=αkM−1∑l=0ϕlcos[πMk(l+12)],\n\nwhere and , for . Then, we have a semi-analytical formula for the evolution operator in the discrete cosine space\n\n HΔt(ϕ)=C−1[eAkΔtC[ϕ]], (18)\n\nwhere and denotes the discrete cosine transform.\n\nFor the first order operator splitting scheme in (3) and the second order scheme in (9) with , the evaluations are all forward time marching, that is, all of and are positive. We can easily show that both schemes are unconditionally stable, in the sense that if regardless of the time step size. (See for the proof.) However, in the case of third or higher order, each of operators , has at least one backward evaluation as mentioned in section 2. For this reason, we need to investigate the stability of the operators and especially for large .\n\nThe stability issue for backward time heat equation is well-known. Even though (without noise) is always an identity operator regardless of the size of , the numerical composition of the operators (even with small error) is far away from the identity operator when becomes large since is exponentially big for . The stability of the numerical composition of the free energy evolution operators is less well-known and we want to explain why the numerical composition of the operators (even with small error) is far away from the identity operator when becomes large using the following figure.\n\nFigure 3 plots as a function of with various initial values of between to . As you can see, with converges to as , however, the solution with as a result of small perturbation may blow up when . Therefore, composition of two operators followed by even with small evaluation error near 1 is no longer bounded as is getting bigger. And with converges to 0 for thus followed by for may change the sign of result even with small perturbation near 0. This non-linear stability effect is basically a consequence of the fact that the solution of the free-energy evolution operator is exponentially close to 1 or 0 as .", null, "Figure 4: Minimum and maximum of {a+i}3i=1 and {b+j}3j=1 as a function of b+3=ω. The region where values are bounded by [−1,1] is shaded in yellow.", null, "Figure 5: Minimum and maximum of {a−i}3i=1 and {b−j}3j=1 as a function of b−3=ω. The region where values are bounded by [−1,1] is shaded in yellow.\n\nIn order to achieve a better stability condition, we propose third order schemes with bounded values of . Figures 4 and 5 show the minimum and maximum values of and for the positive and negative branches, respectively. It is worth noting that are bounded by when and are bounded by when or . Since there is exactly one negative value among , can be inferred from (5) when . Similarly when . In the shaded regions on the figures where values of are bounded by , there are three local minima of at which values are summarized on the following table.\n\nIt is worth to note that the sets of and are same for . The set for is for and the set for is for . This symmetry gives us a freedom to choose the order of operator evaluations and we define three third order operator splitting methods for the AC equation as follows:\n\n S(3)X,S(3)Y,S(3)Z:=Fb3ΔtHa3ΔtFb2ΔtHa2ΔtFb1ΔtHa1Δt (19)\n\nwhere and are given in Table 1.\n\nAnother issue raised with negative time step is that the heat evolution operator may amplify the high frequency modes exponentially big, . This situation happens when . On the other hand, a physically reasonable bound for in the AC equation is , thus the blow-up may occur only for physically too high frequency modes, . Thus, we introduce a cut-off function to bound of for high frequency modes where . We will numerically demonstrate the effect of introducing the cut-off function in subsection 4.1.\n\n## 4 Numerical experiments\n\nIn this section, we numerically demonstrate the order of convergence of the proposed third order schemes in (19) and the fourth order schemes in (13) and in (2). Two examples are used for the test, one is the traveling wave solution with analytic solution and the other is a three-dimensional spinodal decomposition problem with random initial values.\n\nOne of the well-known traveling wave solutions of the Allen–Cahn equation is\n\n ϕ(x,t)=12(1−tanhx−0.5−st2√2ϵ), (20)\n\nwhere is the speed of the traveling wave. The leftmost plot in Figure 6 shows the initial profile and the analytic solution at with . Using this traveling wave solution, we compare the first, second, third, and fourth order operator splitting Fourier spectral methods described in section 3. The numerical solutions are obtained with various time step sizes but the spatial grid size is fixed to which provides enough spatial accuracy. The traveling wave solution with the same numerical parameters are used in the following two subsections to test the third and the fourth order schemes.", null, "Figure 6: Traveling wave solution ϕ(x,Tf) at Tf=1/s with ϵ=0.03√2. And relative l2 errors of ϕ(x,Tf) by S(1),S(2) with h=2−5 for various time step sizes Δt.\n\nThe rightmost plot in Figure 6 shows the numerical error of the first order scheme in (3) and the second order scheme in (9) compared to the analytic solution at . It is worth to remind that the first and the second order schemes apply only forward time steps of and , thus the stability (or boundedness of the solution) regardless of the size can be easily proven. (See our previous paper  for numerical properties of these first and second order schemes.)\n\n### 4.1 Cut-off function and stability of the third order methods\n\nAs mentioned in section 3, negative time steps of and are unavoidable in the third or higher order operator splitting methods. Especially a negative time step makes the heat evolution operator exponentially big, therefore, we introduce the following cut-off function with a tolerance for the heat evolution operator ,\n\n HajΔt(ϕ)=C−1[min{eAkajΔt,Ktol}C[ϕ]]. (21)\n\nThe choice of depends on the time step size and highest frequency modes which are functions of desired computational accuracy. Following computational examples in this subsection give a basic guideline for the choice of .\n\nAs mentioned in section 2, we have various coefficients and as a function of . To investigate the effect of in the third order method , we consider the traveling wave problem given in (20). We compute relative errors for various values with a fixed time step and Figures 7 (a) and (b) show relative errors of the traveling wave solution by the third order methods for positive and negative branches of various , respectively. Here we set (blue solid line) or (green dashed line).", null, "Figure 7: Relative l2 errors of the traveling wave solution ϕ(x,Tf=1/s) by the third order method S(3)ω for various ω with Δt=2−4/s, ϵ=0.03√2, and h=2−5.\n\nThe first noticeable point in Figure 7 might be that the error is relatively large at or where the third order operator degenerates into a second order operator. Also a region near in the positive branch case, the computation does not provide any accuracy at all. As , contains a big negative time step of the heat evolution operator since . In these cases, the choice of cut-off parameter becomes important, and small is recommended when .\n\nFor in which and are bounded by , especially near at which has a local minimum, the error is smaller than that for other values. The similar phenomenon is observed the computation for the negative branch. We choose three special values , , and for , , and , respectively. For these cases, all are bounded by and the choice of cut-off value does not play an important role in the computation.\n\nWe now investigate the effect of highest frequency to . Plots in Figure 8 show relative errors of the traveling wave solution by the third order method with different spatial grid sizes or . If a cut-off function is not used (labeled as ), the computation provides no accuracy for relatively large time step. The computation may even stop as two biggest cases for and the cases happen more often as becomes large. If is larger than , must be properly chosen in order to valence the accuracy loss while avoiding blow-up. However, the choice of makes no significant difference of the solution when (which is physically valid limit for the AC equation) since the high frequency modes with is negligible for the physically meaningful solution of the AC equation. So the simplest rule of thumb might be setting around the desired accuracy of the computation.", null, "Figure 8: Relative l2 errors of the traveling wave solution ϕ(x,Tf=1/s) by SY with ϵ=0.03√2.\n\n### 4.2 Convergence of the third and the fourth order methods\n\nWe implement the proposed third order schemes in (19) and the fourth order schemes in (13) and in (2). We set the spectral grid size , the cut-off limit and compare the numerical solutions for various time step sizes with the analytic solution (20) with . Figure 9 numerically indicates that the proposed methods have the third and the fourth order accuracy, respectively.", null, "Figure 9: Relative l2 errors of the traveling wave solution ϕ(x,Tf) at Tf=1/s by (a) the third order methods S(3)X, S(3)Y, S(3)Z (b) the fourth order schemes S(4)U, S(6)V\n\n### 4.3 Convergence of the spinodal decomposition problem in 3D\n\nIn this subsection, we compute a spinodal decomposition problem satisfying the AC equation (1) in three-dimensional space with . The intervals and where are called metastable intervals and where is called the spinodal interval . It is known that which lies in the spinodal interval is very unstable and the growth of instabilities results in phase separation, which is called spinodal decomposition. In order to check the numerical convergence, we integrate up to time by the proposed numerical schemes with various time step sizes . The initial condition is given on the computational grid with in the domain as where is a random number between and . Figure 10 shows the initial and the reference solutions at computed by the fourth order numerical scheme with the numerical parameters and .", null, "Figure 10: The reference solutions ϕ(x,y,z,t) by the fourth order method S(6)V with Ktol=109, and Δt=10−3/28.", null, "Figure 11: Relative l2 errors of ϕ(x,y,z,Tf=0.01) by S(1), S(2)ω=1, S(3)X,S(3)Y,S(3)Z, S(4)U, S(6)V with various time step sizes Δt=10−3/2,⋯,10−3/27.\n\nWe also implement the first order scheme in (3), the second order scheme in (9), the proposed third order schemes in (19), and the fourth order schemes in (13) and in (2). The numerical results in Figure 11 show that the cut-off value does not play a role when is smaller than while the computational results have marginal difference when is greater than . The accuracy results numerically demonstrate the proposed schemes provide the expected order of convergence in time.\n\n## 5 Conclusions\n\nWe proposed and studied the higher order operator splitting Fourier spectral methods for solving the AC equation. The methods decompose the AC equation into the subequations with the heat and the free-energy evolution terms. Unlike the first and the second order methods, each of the heat and the free-energy evolution operators has at least one backward evaluation in the higher order methods. For the third order method, we suggested the three values at which have local minimums and we then obtained smaller error than other values. For the fourth order method, we used two symmetric combinations of the second order operators. And a simple cut-off function could limit exponential amplification of the high frequency modes in the heat operator and it worked well with the proposed schemes. We numerically demonstrated, using the traveling wave solution and the spinodal decomposition problem with random initial values, that the proposed methods have the third and the fourth order convergence as expected.\n\n## Acknowledgment\n\nThis research was supported by Basic Science Research Program through the National Research Foundation of Korea(NRF) funded by the Ministry of Education(2009-0093827, 2012-002298)." ]
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https://support.office.com/en-us/article/BITOR-function-f6ead5c8-5b98-4c9e-9053-8ad5234919b2
[ "BITOR function\n\nThis article describes the formula syntax and usage of the BITOR function in Microsoft Excel.\n\nDescription\n\nReturns a bitwise 'OR' of two numbers.\n\nSyntax\n\nBITOR(number1, number2)\n\nThe BITOR function syntax has the following arguments.\n\n• Number1    Required. Must be in decimal form and greater than or equal to 0.\n\n• Number2    Required. Must be in decimal form and greater than or equal to 0.\n\nRemarks\n\n• The result is a bitwise 'OR' of its parameters.\n\n• In the result, each bit position is 1 if any of the parameter's bits at that position are 1.\n\n• The values returned from the bit positions progress from right to left as powers of 2. The rightmost bit returns 1 (2^0), the bit to the left returns 2 (2^1), and so on.\n\n• If either argument is outside their constraints, BITOR returns the #NUM! error value.\n\n• If either argument is greater than (2^48)-1, BITOR returns the #NUM! error value.\n\n• If either argument is a non-numeric value, BITOR returns the #VALUE! error value.\n\nExample\n\nCopy the example data in the following table, and paste it in cell A1 of a new Excel worksheet. For formulas to show results, select them, press F2, and then press Enter. If you need to, you can adjust the column widths to see all the data.\n\nFormula\n\nDescription\n\nResult\n\nHow it works\n\n=BITOR(23,10)\n\nCompares the bit positions for the binary representations of the two numbers, and if either position contains 1, returns 2 raised to a power, depending on bit position. Then, those numbers are summed.\n\n31\n\nThe number 23 is 10111 in binary, and 10 is 1010. The value 1 is found in either position at all 5 positions of either of the two numbers. You can express 1010 as 01010 so that both numbers have the same number of digits. The numbers 2^0, 2^1, 2^2, 2^3, and 2^4 are summed, for a total of 31.\n\n23 = 10111\n\n10 = 01010\n\nTest: Is 1 found at any of the 5 positions?\n\nyyyyy\n\n1+2+4+8+16=31\n\nExpand your Office skills\nExplore training", null, "Get instant Excel help\nConnect to an expert now\nSubject to Got It terms and conditions" ]
[ null, "https://support.office.com/SocImages/got-it-original.png", null ]
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http://gnoobz.com/category/9447ctf2015.html
[ "We were provided with several python files and a pcap dump. Part of the relevant logic is given below.\n\ndef mult(m1, m2, p):\nr = [[0,0], [0,0]]\nfor i in range(2):\nfor j in range(2):\nt = 0\nfor k in range(2):\nt += m1[i][k] * m2[k][j]\nr[i][j] = t % p\nreturn r\n\ndef calcM(p, l, base):\nif l == 0:\nreturn [[base, base], [base, base]]\nx1 = [[base, base], [base, (base + base) % p]]\nx2 = mult(x1, x1, p)\nfor i in bin(l)[3:]:\nif i == '1':\nx1 = mult(x1, x2, p)\nx2 = mult(x2, x2, p)\nelse:\nx2 = mult(x1, x2, p)\nx1 = mult(x1, x1, p)\nreturn x1\n\ndef genKey(p):\nnumBytes = int(math.ceil(math.log(p, 256)))\nexp = int(os.urandom(numBytes).encode('hex'), 16) % p\nr = calcM(p, exp, (0, 1))\nreturn (r, exp)\n\n\nA generated key is given as a pair of a random exponent $$e \\in \\mathbb{Z}_p$$ and a matrix\n\n$$M = \\begin{pmatrix}0&1\\\\1&1\\end{pmatrix}^e \\in \\mathbb{Z}_p^{2 \\times 2}.$$\n\nBased on this a server and client will agree on a shared key using a Diffie Hellman scheme.\n\nFrom the pcap dump we can find the parameters exchanged:\n\ns: 981725946171163877\ns: 58449491987662952,704965025359609904\nc: 453665378628814896,152333692332446539\ns: 59719af4dbb78be07d0398711c0607916dd59bfa57b297cd220b9d2d7d217f278db6adca88c9802098ba704a18cce7dd0124f8ce492b39b64ced0843862ac2a6\n\n\nThere are several ways to solve this problem, we can directly try to break the discrete logarithm in the matrix group, we can diagonalize the matrix and solve in some extension field or we can play smart. First we recognize the exponentiated matrix as generator of Fibonacci numbers in $$\\mathbb{Z}_p$$. By looking at how the matrix behaves when exponentiated we can actually derive a closed formula for the $$n$$-th Fibonacci number \n\n$$F_n = \\frac{1}{\\sqrt{5}}\\left[\\left(\\frac{1 + \\sqrt{5}}{2}\\right)^n - \\left(\\frac{1 - \\sqrt{5}}{2}\\right)^n \\right].$$\n\nThis formula actually works over $$\\mathbb{Z}_p$$ (or if $$\\sqrt{5}$$ does not exist there, over $$\\mathbb{Z}_p\\left(\\sqrt{5}\\right)$$). We may solve above formula for $$n$$, yielding\n\n$$n = \\log_\\varphi \\left( \\frac{F_n \\sqrt{5} + \\sqrt{5F_n^2 \\pm 4}}{2} \\right)$$\n\nwhere $$\\varphi = \\left(1 + \\sqrt{5}\\right)/2$$. Great, we now have reduced the problem to solving a single discrete logarithm over $$\\mathbb{Z}_p$$ (or $$\\mathbb{Z}_p\\left(\\sqrt{5}\\right)$$).\n\nWe can easily do this using SageMath\n\nF = GF(981725946171163877)\n\ndef fib_idx(f):\nx = sqrt(F(5))\nphi = (1 + x)/F(2)\nn = (f*x + sqrt(F(5)*f*f + F(4)))/F(2) # +/- 4\nreturn n.log(phi)\n\nprint \"n =\", fib_idx(152333692332446539)\n#n = 152106608687469950\n\n\nand then decrypt the flag using\n\np = 981725946171163877\nsecret = 152106608687469950\nserver_key = (58449491987662952, 704965025359609904)\nshared = calcM(p, secret, server_key)\nprint decrypt(msg, str(shared))\n# 9447{Pisan0_mU5t_nEv3r_hAve_THougHt_0f_bruTe_f0rce5}\n\n\n## References:\n\n1. Binet's Fibonacci Number Formula http://mathworld.wolfram.com/BinetsFibonacciNumberFormula.html" ]
[ null ]
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https://sourceforge.isae.fr/projects/quantitative-analysis-of-rf-signals/wiki/2_Simulation
[ "### 2. Simulation¶\n\nFirst, we decided to design our signal analyser and to test it with simulated signals such as sine waves.\nTo do so, a VI (Labview program) able to generate a noisy signal has been created. This noisy signal is the addition of three basic signals and a white Gaussian noise. For each basic signal we can set the signal type, the frequency, the amplitude and the offset. For the noise, we can set the noise standard deviation.\nConsequently we can insert the noisy signal into our signal analyser to test it.\n\nFor example if we set 3 sine waves with different frequencies and amplitudes we observe this spectrum :", null, "Figure 13: Power spectrum of three different sine waves\n\nWe can also observe the spectrum of a noisy sine wave :", null, "Figure 14: Power spectrum of a noisy sine wave\n\nIn the two cases, the spectrums match with the expected values (frequencies and amplitudes)" ]
[ null, "https://sourceforge.isae.fr/attachments/download/1480/3sinus.png", null, "https://sourceforge.isae.fr/attachments/download/1481/sinus_and_noise.png", null ]
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https://www.w3resource.com/c-programming-exercises/array/c-array-exercise-18.php
[ " C Program: Read a 2D array of size 3x3 and print the matrix - w3resource\n\n# C Exercises: Read a 2D array of size 3x3 and print the matrix\n\n## C Array: Exercise-18 with Solution\n\nWrite a program in C for a 2D array of size 3x3 and print the matrix.\n\nVisual Presentation:", null, "Sample Solution:\n\nC Code:\n\n``````#include <stdio.h>\n\nvoid main() {\nint arr1, i, j;\n\n// Prompt user for input\nprintf(\"\\n\\nRead a 2D array of size 3x3 and print the matrix :\\n\");\nprintf(\"------------------------------------------------------\\n\");\n\n// Input values for the matrix\nprintf(\"Input elements in the matrix :\\n\");\nfor (i = 0; i < 3; i++) {\nfor (j = 0; j < 3; j++) {\nprintf(\"element - [%d],[%d] : \", i, j);\nscanf(\"%d\", &arr1[i][j]);\n}\n}\n\n// Display the matrix\nprintf(\"\\nThe matrix is : \\n\");\nfor (i = 0; i < 3; i++) {\nprintf(\"\\n\");\nfor (j = 0; j < 3; j++)\nprintf(\"%d\\t\", arr1[i][j]);\n}\nprintf(\"\\n\\n\");\n}\n```\n```\n\nSample Output:\n\n```Read a 2D array of size 3x3 and print the matrix :\n------------------------------------------------------\nInput elements in the matrix :\nelement - , : 1\nelement - , : 2\nelement - , : 3\nelement - , : 4\nelement - , : 5\nelement - , : 6\nelement - , : 7\nelement - , : 8\nelement - , : 9\n\nThe matrix is :\n\n1 2 3\n4 5 6\n7 8 9\n```\n\nFlowchart:", null, "C Programming Code Editor:\n\nWhat is the difficulty level of this exercise?\n\nTest your Programming skills with w3resource's quiz.\n\n" ]
[ null, "https://www.w3resource.com/w3r_images/c-array-image-exercise-18.png", null, "https://www.w3resource.com/w3r_images/c-array-exercise-18.png", null ]
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http://lists.suckless.org/hackers/1611/13718.html
[ "# (wrong string) ée\n\nFrom: <git_AT_suckless.org>\nDate: Wed, 30 Nov 2016 10:16:12 +0100 (CET)\n\ncommit aeb5e44a98cb4158528206c079654357b1c75b16\nAuthor: Mattias Andrée <maandree_AT_kth.se>\nAuthorDate: Wed Nov 30 10:15:59 2016 +0100\nCommit: Mattias Andrée <maandree_AT_kth.se>\nCommitDate: Wed Nov 30 10:15:59 2016 +0100\n\nFix errors in the manual (most of them found by Ivan Zuboff)\n\nSigned-off-by: Mattias Andrée <maandree_AT_kth.se>\n\ndiff --git a/doc/exercises.tex b/doc/exercises.tex\nindex 3a9df19..9a18b99 100644\n--- a/doc/exercises.tex\n+++ b/doc/exercises.tex\n_AT_@ -596,7 +596,7 @@ ptest_llt(z_t n)\n\n$M_n$ is composite if $n$ is composite, therefore,\nif you do not expect prime-only values on $n$, the\n-performance can be improve by using some other\n+performance can be improved by using some other\nprimality test (or this same test if $n$ is a\nMersenne number) to first check that $n$ is prime.\n\ndiff --git a/doc/miscellaneous.tex b/doc/miscellaneous.tex\nindex 8750595..420d6a7 100644\n--- a/doc/miscellaneous.tex\n+++ b/doc/miscellaneous.tex\n_AT_@ -101,7 +101,7 @@ sum of a set of numbers.\nAnother form of assignment available in libzahl is\ncopy-assignment. This done using {\\tt zset}. As\neasily observable, {\\tt zset} is named like\n-{\\tt zseti}, {\\tt zsetu}, and {\\tt zsetu}, but\n+{\\tt zseti}, {\\tt zsetu}, and {\\tt zsets}, but\nwithout the input-type suffix. The lack of a\ninput-type suffix means that the input type is\n{\\tt z\\_t}. {\\tt zset} copies value of second\ndiff --git a/doc/not-implemented.tex b/doc/not-implemented.tex\nindex 59b3efb..9688189 100644\n--- a/doc/not-implemented.tex\n+++ b/doc/not-implemented.tex\n_AT_@ -3,25 +3,25 @@\n\nIn this chapter we maintain a list of\nfeatures we have chosen not to implement,\n-but would fit into libzahl had we not have\n+but would fit into libzahl, had we not have\nour priorities straight. Functions listed\nherein will only be implemented if it is\nshown that it would be overwhelmingly\nadvantageous. For each feature, a sample\nimplementation or a mathematical expression\n-on which you can base your implemention\n-is included. The sample implementations create\n-temporary integer references, this is to\n-simplify the examples. You should try to\n-use dedicated variables; in case of recursion,\n-a robust program should store temporary\n-variables on a stack, so they can be\n-clean up if something happens.\n-\n-Research problems, like prime-factorisation\n-and discrete logarithms do not fit in the\n-scope of bignum libraries. % Unless they are extraordinarily bloated with vague mission-scope, like systemd.\n-And therefore do not fit into libzahl,\n+on which you can base your implementation is\n+included. The sample implementations create\n+temporary integer references to simplify the\n+examples. You should try to use dedicated\n+variables; in case of recursion, a robust\n+program should store temporary variables on\n+a stack, so they can be cleaned up if\n+something happens.\n+\n+Research problems, like prime factorisation\n+and discrete logarithms, do not fit in the\n+scope of bignum libraries % Unless they are extraordinarily bloated with vague mission-scope, like systemd.\n+and therefore do not fit into libzahl,\nand will not be included in this chapter.\nOperators and functions that grow so\nridiculously fast that a tiny lookup table\n_AT_@ -330,7 +330,7 @@ method can be derived from the observation\n\\vspace{1em}\n\n\\noindent\n-The resulting algorithm can be expressed\n+The resulting algorithm can be expressed as\n\n\\begin{alltt}\nvoid\n_AT_@ -690,10 +690,10 @@ in an integer, counting the sign bit:\n\\end{alltt}\n\n\\noindent\n-It requires a compiler extension, if missing,\n-there are other ways to computer the population\n-count for a word: manually bit-by-bit, or with\n-a fully unrolled\n+It requires a compiler extension; if it's not\n+available, there are other ways to computer the\n+population count for a word: manually bit-by-bit,\n+or with a fully unrolled\n\n\\begin{alltt}\nint s;\n_AT_@ -706,7 +706,7 @@ a fully unrolled\n\\label{sec:Hamming distance}\n\nA simple way to compute the Hamming distance,\n-the number of differing bits, between two\n+the number of differing bits between two\nnumbers is with the function\n\n\\begin{alltt}\n_AT_@ -767,13 +767,13 @@ side-effects.\n\\label{sec:Reference duplication}\n\nThis could be useful for creating duplicates\n-with modified sign. But only if neither\n+with modified sign, but only if neither\n{\\tt r} nor {\\tt a} will be modified whilst\nboth are in use. Because it is unsafe,\nfairly simple to create an implementation\nwith acceptable performance — {\\tt *r = *a},\n— and probably seldom useful, this has not\n-be implemented.\n+been implemented.\n\n\\begin{alltt}\nvoid\ndiff --git a/doc/number-theory.tex b/doc/number-theory.tex\nindex 10c485b..b4c2ece 100644\n--- a/doc/number-theory.tex\n+++ b/doc/number-theory.tex\n_AT_@ -145,7 +145,7 @@ definion ensures\n\\noindent\nand analogously for $\\frac{b}{\\gcd(a,\\,b)}$. Note however,\nthe convension $\\gcd(0, 0) = 0$ is adhered. Therefore,\n-before dividing with $\\gcd{a, b}$ you may want to check\n+before dividing with $\\gcd(a, b)$ you may want to check\nwhether $\\gcd(a, b) = 0$. $\\gcd(a, b)$ is calculated\nwith {\\tt zgcd(a, b)}.\n\n_AT_@ -179,7 +179,7 @@ $\\max x : 2^x \\vert z$ is returned by {\\tt zlsb(z)}\n\\section{Primality test}\n\\label{sec:Primality test}\n\n-A primality of an integer can be test with\n+The primality of an integer can be tested with\n\n\\begin{alltt}\nenum zprimality zptest(z_t w, z_t a, int t);\n_AT_@ -235,7 +235,7 @@ test with witness return.\n\n\\hspace{2ex}\n\\begin{minipage}{\\linewidth}\n- \\STATE $k \\xleftarrow{\\$} \\textbf{Z}_{a - 2} \\setminus \\textbf{Z}_{2}$+ \\STATE$k \\xleftarrow{\\$} \\textbf{Z}_{a - 2} \\setminus \\textbf{Z}_{2}$ \\textcolor{c}{\\{Uniformly random assignment.\\}}\n\\STATE $x \\gets k^d \\mod a$\n\\STATE {\\bf continue} {\\bf if} $x = 1$ \\OR $x = a - 1$\n\\STATE {\\bf repeat} $r$ {\\bf times or until} $x = 1$ \\OR $x = a - 1$\ndiff --git a/doc/what-is-libzahl.tex b/doc/what-is-libzahl.tex\nindex b0e80f5..2bf1c52 100644\n--- a/doc/what-is-libzahl.tex\n+++ b/doc/what-is-libzahl.tex\n_AT_@ -141,8 +141,9 @@ Unlike other bignum libraries, errors in libzahl are\ncaught using {\\tt setjmp}. This ensure that it can be\nused in robust applications, catching errors does not\nbecome a mess, and it minimises the overhead of\n-catching errors. Errors are only checked when they can\n-occur, not also after each function return.\n+catching errors. Typically, errors can be checked when\n+they can occur and after each function return; however,\n+here they can be checked only when they can occur.\n\nAdditionally, libzahl tries to keep the functions'\nnames simple and natural rather than technical or\nlibzahl is also only designed for POSIX systems.\nIt will probably run just fine on any modern\nsystem. But it makes some assumption that POSIX\n-stipulates or are unpractical not to implement\n-for machines that should support POSIX (or even\n+stipulates or are unpractical to leave out from\n+machines that should support POSIX (or even\nsupport modern software):\n\n\\begin{itemize}\n_AT_@ -214,12 +215,12 @@ strictly necessary for it to be an CPU-intrinsic,\nbut that would be favourable for performance.)\n\\end{itemize}\n\n-Because of the prevalence of theses properties\n+Because of the prevalence of these properties\nin contemporary machines, and the utilisation of\nthese properties in software, especially software\nfor POSIX and popular platforms with similar\n-properties, any new general-purpose machine most\n-have these properties lest, it but useless with\n+properties, any new general-purpose machine must\n+have these properties, lest it be useless with\ntoday's software. Therefore, libzahl can make\nthe assumption that the machine has these\nproperties. If the machine does not have these\nReceived on Wed Nov 30 2016 - 10:16:12 CET\n\nThis archive was generated by hypermail 2.3.0 : Wed Nov 30 2016 - 10:24:16 CET" ]
[ null ]
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http://www.imooc.com/wiki/clesson/parametertype.html
[ "# C 语言中函数的参数传入类型\n\n1. 使用数组\n2. 使用 & 符号\n\n## 3. 示例\n\n### 3.1 值传入示例\n\n``````#include <stdio.h>\n\n{\nx++;\nprintf(\"sub function\\n x: %d\\n\", x);\nreturn 0;\n}\n\nint main()\n{\nint a = 1;\nprintf(\"mian function\\n a: %d\\n\", a);\nreturn 0;\n}\n``````\n\n``````sub function\nx: 2\nmian function\na: 1\n``````\n\n### 3.2 引用传入示例\n\n#### 使用数组示例\n\n``````#include <stdio.h>\n\n{\nx++;\nprintf(\"sub function\\n x: %d\\n\", x);\nreturn 0;\n}\n\nint main()\n{\nint a[] = {1};\nprintf(\"mian function\\n a: %d\\n\", a);\nreturn 0;\n}\n``````\n\n``````sub function\nx: 2\nmian function\na: 2\n``````\n\n#### 使用指针\n\n``````#include <stdio.h>\n\n{\n(*x)++;\nprintf(\"sub function\\n x: %d\\n\", *x);\nreturn 0;\n}\n\nint main()\n{\nint a = 1;\nprintf(\"mian function\\n a: %d\\n\", a);\nreturn 0;\n}\n``````\n\n``````sub function\nx: 2\nmian function\na: 2\n``````" ]
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https://www.jpost.com/opinion/civil-fights-goldstones-recipe-for-never-ending-conflict
[ "(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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http://club.shopex.cn/b2b2c/dev/400.framework/300.requests.html
[ "# 1. 请求\n\n## 1.1. 基本输入\n\n\\$name = input::get('name');\n\n``````\\$name = input::get('name', 'Sally');\n``````\n\n``````if (input::has('name'))\n{\n//\n}\n``````\n\n``````\\$input = input::all();\n``````\n\n``````\\$input = input::only('username', 'password');\n\n\\$input = input::except('credit_card');\n``````\n\n``````\\$input = input::get('products.0.name');\n``````\n\n## 1.2. 文件上传\n\n``````\\$file = input::file('photo');\n``````\n\n``````if (input::hasFile('photo'))\n{\n//\n}\n``````\n\n`file` 方法返回了一个 `Symfony\\Component\\HttpFoundation\\File\\UploadedFile` 类的实例, 该类继承自PHP的 `SplFileInfo` 类,并提供了大量操作该用户上传的文件的方法。\n\n``````input::file('photo')->move(\\$destinationPath);\n\ninput::file('photo')->move(\\$destinationPath, \\$fileName);\n``````\n\n``````\\$path = input::file('photo')->getRealPath();\n``````\n\n``````\\$size = input::file('photo')->getSize();\n``````\n\n``````\\$mime = input::file('photo')->getMimeType();\n``````\n\n## 1.3. 用户请求的详细信息\n\n`Request` 类提供了许多 方法 用于获取关于请求的详细信息\n\n``````\\$url = kernel::removeIndex(request::url());\n``````\n\n``````kernel::base_url(1);\n``````\n\n``````kernel::base_url();\n``````\n\n``````\\$uri = request::path();\n``````\n\n``````if (request::is('admin/*'))\n{\n//\n}\n``````\n\n``````\\$url = request::url();\n``````\n\n``````\\$value = request::header('Content-Type');\n``````\n\n``````\\$value = request::server('PATH_INFO');\n``````\n\n``````if (request::ajax())\n{\n//\n}\n``````\n\n``````if (request::secure())\n{\n//\n}\n``````\n\n`request::format` 方法基于 HTTP 请求头的 Accept 信息返回客户端希望获取的响应格式:\n\n``````if (request::format() == 'json')\n{\n//\n}\n``````" ]
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https://www.physicsforums.com/threads/absorbtion-coefficent-and-radiation-curve.792263/
[ "# Absorbtion coefficent and radiation curve\n\n## Homework Statement\n\nI have data of an experiment to find absorbtion coefficent of a sample. one curve shows intensity of original beam, the other one is intensity with sample (with wavelenght). Here is the data :", null, "## Homework Equations", null, "Where: I = the intensity of photons transmitted across some distance x\nI0 = the initial intensity of photons\ns = a proportionality constant that reflects the total probability of a photon being scattered or absorbed\nµ = the linear attenuation coefficient\nx = distance traveled\n\n## The Attempt at a Solution\n\nI did similar experiment before (not teoricaly). I set the experiment and took original beam intensity(I) and beam with sample intensity(I0). ln (I/I0) gave absorption coefficent.\nBut now i dont know how to do it with the graph with different wavelengt.\n\n## Answers and Replies\n\nAnd what is the area under the curve. I couldnt estimate that.\nI though the ratio of the areas under curves give the result. Is it correct?\n\nQuantum Defect\nHomework Helper\nGold Member\n\n## Homework Statement\n\nI have data of an experiment to find absorbtion coefficent of a sample. one curve shows intensity of original beam, the other one is intensity with sample (with wavelenght). Here is the data :\nView attachment 77649\n\n## Homework Equations", null, "Where: I = the intensity of photons transmitted across some distance x\nI0 = the initial intensity of photons\ns = a proportionality constant that reflects the total probability of a photon being scattered or absorbed\nµ = the linear attenuation coefficient\nx = distance traveled\n\n## The Attempt at a Solution\n\nI did similar experiment before (not teoricaly). I set the experiment and took original beam intensity(I) and beam with sample intensity(I0). ln (I/I0) gave absorption coefficent.\nBut now i dont know how to do it with the graph with different wavelengt.\nIt looks like you have an Excel spereadsheet with data. You can do the same calculation that you did for a single point with the column vectors in the spreadsheet. Series1 = I0 ; Series 2 = I.\n\nYou can rearrange the equation above to get: ln (I/I0) = -mu x if x = path length, how do you calculate mu at each point?\n\nWith small intensities, you are likely to get nonsense -- values at short wavelength (<300 nm) will likely be nonsense.\n\nTo integrate, you can use Euler's method for numerical integration -- that should be good enough -- but I would limit the integration to where the curve for mu is smooth.\n\nI did -ln(I/I0) and the result is here:", null, "It doesnt seem right to me. Absoprtion coefficent doesnt related with wavelenght acourding to lambert beer law. am i right?\nSo i think it should be like constant not exponential.\n\nQuantum Defect\nHomework Helper\nGold Member\nI did -ln(I/I0) and the result is here:\nView attachment 77656\nIt doesnt seem right to me. Absoprtion coefficent doesnt related with wavelenght acourding to lambert beer law. am i right?\nSo i think it should be like constant not exponential.\nThe absorbance of most things depends upon wavelength. What were you measuring the absorbance of?\n\nIn your spectrum, you see larger absorbance at shorter wavelength, this is quite common, as the electronic transitions of many simple molecules & materials are at higher energy, shorter wavelength.\n\nc.f. http://www.chemistrymag.org/cji/2003/056049pe.htm\n\nhttp://www.chemistrymag.org/cji/2003/images/05604906.gif\n\nLast edited:\nIt s CdSe.\nSo wavelength is another variable for absoption.\nMy main task is to compare this teorotical result with experimental result.\nI did the experiment with many dichoric filters. For example with red filter the absorption was 1,09. when i evaluate teoric curve the red area (615-730) the avarage absorption is0,302.\ngreen filter exp: 1,020, teoric 0,4522\nblue exp:1,02 teoric 0,5949\n\nfirst idea was the ratio between them is about distance that light traveled. But as you see the ratio isnt stable. Then you say wavelength is another variable (and i agree with you). now this is my new problem. Do you have any idea. I am stucked" ]
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https://everything2.com/title/kinetics
[ "Kinetics (as used by chemists) refers to the study of rates of chemical reaction. This is very important as in organic chemistry you can often get several different products from the same mixture of reagents, but by controlling the reaction conditions the rate of formation of each product may be changed. Knowledge of the kinetics of a reaction helps to produce larger quantities of desired products while reducing the presence of unwanted byproducts.\n\nGetting back to the point, rates of reaction are generally determined by two types of variable: temperature, and the concentration of each reagent.\n\nYou can see how this dependence works for a simple reaction if you think about it just a little. A group of molecules can only react if they are all together and if they have energy to form an activated state. Dealing with bulk quantities of materials, you need the probabilities that each type of molecule is in the same place and the probability that enough energy is available. The amount of energy is related to the temperature by a function familiar to anyone who has ever used thermodynamics or statistical mechanics. The probablility of a molecule being in a given place can be measured by the concentration of the molecule.\n\nNeedless to say, if you need N molecules of substance A in the same place, the probability of that happening is proportional to the concentration of A raised to the Nth power. The reaction is said to be Nth order with respect to A.\n\nThis also gives a 1st order differential equation which allows you to predict the rate of reaction for a simple reaction, but often reactions are more complex. Often you have intermediates, which act as products in one step of the reaction and reagents in the next step. This gives you a set of differential equations which must be solved simultaneously. This set of equations can always be reduced to a single differential equation of higher order, but may be nonlinear if the same reagent is involved in multiple steps of the reaction.\n\nTo make things more complicated, you usually don't really know the concentrations of the intermediates, and often don't have any way of measuring them. This is where the steady state approximation is useful.\n\nBasically, for the steady state approximation you pretend the concentrations of the intermediates is constant over the entire duration of the reaction, even if you don't know what it is. Looking at the set of first order equations, you take each equation where a given intermediate is produced or consumed to get an equation describing the concentration of that particular intermediate in terms of concentrations of reagents, products, and other intermediates. Then you go back and substitute that equation for the intermediate concentration in the original equations, and repeat the process with another intermediate, until all you have left are concentrations of product and reagents.\n\nThe rate of a chemical reaction, r, quoted in units of mol dm-3 s-1, is given by the expression\n\nr = k [A]0 [B]1 [C]2\n\nwhere [A], [B] and [C] are the concentrations of the reactants in mol dm-3 and k is the rate constant.\n\nFor example, for the reaction between propanone (acetone) and iodine in the presence of hydrogen ions, the equation is\n\nr = k [CH3COCH3]1 [I2]0 [H+] 1\n\nIf the concentration of a reactant is raised to the power 0 (making it equal to 1), it has no effect on the rate - it is zero order. It does not really have to be included in the equation at all. If it raised to the power 1 (i.e. not changed at all), it affects the rate and is first order. If it raised to the power 2 (i.e. squared), it has an even stronger effect on the rate and is second order.\n\nZero order reactants decrease in concentration at a constant rate throughout a reaction. First order reactants decrease at a rate that continually slows, with a constant half-life. Second order reactants decrease at a rate that continually slows and has an increasing half-life.\n\nThe order of a reactant is related to its role in the actual chemical process. Reactions take place in steps, forming intermediate compounds. The slowest step determines the overall rate of the reaction and is indeed known as the rate determining step. Only those reactants which are involved in or before this step will appear in the rate equation.\n\nReactant-orders cannot be predicted theoretically; we must determine them by experiment.\n\nThe rate constant, k, depends on temperature and on the orientation of the molecules involved and, for many reactions, is approximately given by the Arrhenius equation:\n\nk = A e-EA/RT\n\nwhere A is a pre-exponential factor relating to molecular orientation, EA is the activation energy of the reaction, R is the universal gas constant and T is the temperature. e, of course, is just e. As the temperature increases, EA/RT decreases, so e is being raised to a less negative number. Thus k increases, so the reaction goes faster.\n\nWith thanks to the editors for their patience.\n\n• The study of reaction rates.\n• The study of the relationship between force and mass.\n\n• From the BioTech Dictionary at http://biotech.icmb.utexas.edu/. For further information see the BioTech homenode.\n\nKi*net\"ics (?), n. Physics\n\nSee Dynamics.\n\nLog in or register to write something here or to contact authors." ]
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https://wiki.unifiedmathematics.com/index.php?title=A_subspace_of_a_Hausdorff_space_is_Hausdorff
[ "# A subspace of a Hausdorff space is Hausdorff\n\nThis page is a stub, so it contains little or minimal information and is on a to-do list for being expanded.The message provided is:\nFlesh out and check the proof before removing this\n\n## Statement\n\nSuppose [ilmath](X,\\mathcal{ J })[/ilmath] is a Hausdorff topological space; then for any [ilmath]A\\in\\mathcal{P}(X)[/ilmath] (so [ilmath]A[/ilmath] is an arbitrary subset of [ilmath]X[/ilmath]) considered as a topological subspace, [ilmath](A,\\mathcal{J}_A)[/ilmath], of [ilmath](X,\\mathcal{ J })[/ilmath] is also Hausdorff.\n\n## Proof\n\n• Let [ilmath]a,b\\in A[/ilmath] be given. We wish to show there are neighbourhoods (with respect to the topological space [ilmath](A,\\mathcal{J}_A)[/ilmath]) to [ilmath]a[/ilmath] and [ilmath]b[/ilmath] (which we shall call [ilmath]N_a[/ilmath] and [ilmath]N_b[/ilmath] respectively) such that [ilmath]N_a\\cap N_b=\\emptyset[/ilmath]\n• As [ilmath](X,\\mathcal{ J })[/ilmath] is Hausdorff, there exist neighbourhoods [ilmath]N_a'[/ilmath] and [ilmath]N_b'[/ilmath] neighbourhood to [ilmath]a[/ilmath] and [ilmath]b[/ilmath] respectively (with respect to the topological space [ilmath](X,\\mathcal{ J })[/ilmath] in this case) such that [ilmath]N_a'\\cap N_b'=\\emptyset[/ilmath]\n• Thus [ilmath]\\exists U_a',U_b'\\in\\mathcal{J}[a\\in U_a'\\wedge b\\in U_b'\\wedge U_a'\\cap U_b'=\\emptyset][/ilmath] (by definition of neighbourhood, using [ilmath]U_a'\\subseteq N_a'[/ilmath], [ilmath]U_b'\\subseteq N_b'[/ilmath] and that [ilmath]N_a'\\cap A_b'=\\emptyset[/ilmath])\n• By definition of the subspace topology, we see and define [ilmath]U_a:=U_a'\\cap A\\in\\mathcal{J}_A[/ilmath] and [ilmath]U_b:=U_b'\\cap A\\in\\mathcal{J}_A[/ilmath]\n• Note that [ilmath]a\\in U_a'[/ilmath], [ilmath]b\\in U_b'[/ilmath] and [ilmath]a,b\\in A[/ilmath], so [ilmath]a\\in U_a[/ilmath] and [ilmath]b\\in U_b[/ilmath]\n• Furthermore notice [ilmath]U_a\\cap U_b\\subseteq U_a'\\cap U_b'\\subseteq N_a'\\cap N_b'=\\emptyset[/ilmath]\n• So [ilmath]U_a\\cap U_b=\\emptyset[/ilmath]\n• Since [ilmath]U_a[/ilmath] contains an open set (namely [ilmath]U_a[/ilmath]) containing [ilmath]a[/ilmath] it is a neighbourhood to [ilmath]a[/ilmath]\n• Same for [ilmath]b[/ilmath] and [ilmath]U_b[/ilmath]\n• Thus we have shown there exist disjoint neighbourhoods of [ilmath]a[/ilmath] and [ilmath]b[/ilmath] in the subspace.\n• Since our choice of [ilmath]a[/ilmath] and [ilmath]b[/ilmath] was arbitrary we have shown this for all [ilmath]a,b\\in A[/ilmath]" ]
[ null ]
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http://www.yorku.ca/mack/chi03c.html
[ "Isokoski, P., & MacKenzie, I. S. (2003). Metrics for text entry research: Combined model for text entry rate development. Extended Abstracts of the ACM Conference on Human Factors in Computing Systems - CHI 2003, pp. 752-753. New York: ACM.\n\n# Combined Model for Text Entry Rate Development\n\n### P. Isokoski and I. Scott MacKenzie\n\nUnit for Computer-Human Interaction (TAUCHI)\nDepartment of Computer and Information Sciences\nFIN - 33014 University of Tampere, Finland\n{poika,scott}@cs.uta.fi\nABSTRACT\nWe combine the power law of learning and theoretical upper limit predictions to describe the development of text entry rates from users' first contact to asymptotic expert usage. The combined model makes comparing text entry methods easier. We present the rationale for the model and two candidate implementations. The first is a simple regression model with a reasonable fit to the data. The second fits measured data better, but is more complicated.\n\nKeywords\npower law of learning, text entry, modeling\n\n## INTRODUCTION\n\nThe merits of text entry methods such as handwriting or touch-typing depend on the entry speed achievable. Slower methods are often justified if users lack skill in a faster method. Thus, two critical characteristics of text entry methods are expert performance and the practice required to achieve it.\n\nA model based on the power law of learning is built using text entry rate data measured in a longitudinal experiment. The model is of the form RN = aNx where N is the session number and RN is the text entry rate predicted for session N. a and x are regression constants.\n\nModels for upper limit or expert performance include those for stylus operated soft keyboards , two-thumb text entry on physical keyboards , and unistroke writing time .\n\n## PROBLEMS WITH THE MODELS\n\nThe power law curve usually fits the measured data remarkably well (see Figure 1). However, the predicted text entry rate grows to infinity given enough practice. In reality an upper limit is encountered at some point. This means the power curve is good for describing experimental results (examples in [1, 4]), but has limited reliability as a predictor (as for example in ).\n\nThere are procedures for calculating the upper limit, however they do not predict the time to reach the limit. The purpose herein is to fix this by estimating the whole learning process.\n\nUpper limit models are built using variables for the minimum time for primitive actions. Consequently wrong values produce wrong predictions. The combined model described here is subject to this same limitation, thus care is warranted to ensure that the underlying assumptions are correct and appropriate given the situation that is modeled.", null, "Figure 1. Data for the OPTI soft-keyboard, upper limit, and best fitting power curve by MacKenzie and Zhang .\n\n## THE COMBINED MODEL\n\nCombining the power model and the upper limit model requires a function that initially follows a power curve but is later constrained by the upper limit. A straightforward way to meet these requirements is to first recode the measured text entry rates as Rmax - Re where Rmax is the upper limit prediction and Re the measured entry rate during a session. The result in Figure 2 uses the same data as Figure 1. The \"model 1\" curve shows Rmax minus the value produced by the regression model. Although the model works reasonably well (R2 = 0.92), it underestimates toward the end of the data.\n\nTo improve the fit of the model we propose a second model where the text entry rate for a session is that of the preceding session plus a difference calculated using the power curve and the modeled upper limit. To simplify the following equation we use DN for the difference in consecutive sessions: DN = aNx - a(N - 1)x. With this definition our model is:", null, "The exponent z adjusts the shape of the transfer from the power curve to the upper limit. We use z = Rmax / (Rmax - Rlast) + 1, where Rlast is the highest measured text entry rate. The goal is to keep the predictions close to the observations for the duration of the measured data and then have them approach the upper limit.", null, "Figure 2. Model 1 and the measured data.\n\nWhile the model seems complicated, it is easy to implement in an ordinary spreadsheet. Figure 3 shows the result using the same data. To show long-term behavior the scale extends to 150 sessions. As seen, the best fitting power curve exceeds the theoretical upper limit somewhere around session 50. Models 1 and 2 approach the upper limit at a decreasing rate, as they should. The difference is that model 1 under-estimates the last measured sessions and most likely several sessions after. Model 2 under-estimates too, but not so much.", null, "Figure 3. Long-term behavior of the models.\n\n## DISCUSSION\n\nWe are still examining models that fit the measured data better than model 1 but are simpler than model 2. The assessment of the theoretical foundations of the models is also work in progress. However, even our current imperfect models do a better job at describing the whole learning process than either of the component models.\n\nFurthermore, they provide a clear graphical representation of a text entry method that facilitates comparisons with other methods. The method with the greatest area below the modeled curve during the period of interest is the best. A good method starts high, has a high upper limit, and reaches the upper limit fast. A not-so-good method exhibits a combination of the opposite symptoms. Figure 4 is an example of this kind of comparison. The QWERTY soft keyboard layout is initially faster, but after session 11 the OPTI layout is faster and according to the models it will remain so.", null, "Figure 4. Comparing text entry methods (data from ).\n\nIn the examples above we used data from only one experiment. While other data sets produce similar results, we have not yet tested our models against all available data.\n\n## CONCLUSIONS\n\nWe described models combining the traditional power law regression model and upper limit prediction model of text entry rate. We then proposed two models that satisfy these requirements. The models have both descriptive and predictive uses in comparing text entry methods.\n\n## REFERENCES\n\n1. Card, S. K., Moran, T. P., and Newell, A., The psychology of human-computer interaction, Lawrence Erlbaum, 1983.\n\n2. Isokoski, P., Model for unistroke writing time. Proc. CHI 2001, 357-364.\n\n3. MacKenzie, I. S., and Soukoreff, R. W., A model of two-thumb text entry. Proc. GI 2002, 117-124.\n\n4. MacKenzie, I. S., and Zhang, S. X., The design and evaluation of a high-performance soft keyboard. Proc. CHI '99, 25-31.\n\n5. Soukoreff, R. W., and MacKenzie, I. S. Theoretical upper and lower bounds on typing speed using a stylus and soft keyboard. Behaviour & Information Technology, 14, 370-379, 1995." ]
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http://www.ni.com/documentation/en/labview-comms/2.1/analysis-node-ref/unit-vector/
[ "# Unit Vector (G Dataflow)\n\nFinds the norm of a vector and normalizes the vector with the norm.", null, "", null, "## reset\n\nA Boolean that specifies whether to reset the internal state of the node.\n\n True Resets the internal state of the node. False Does not reset the internal state of the node.\n\nThis input is available only if you wire a double-precision, floating-point number to input vector.\n\nDefault: False", null, "## input vector\n\nInput vector.\n\nThis input can be an array of double-precision, floating-point numbers or an array of complex double-precision, floating-point numbers.\n\nThis input changes to input data point when the data type is a double-precision, floating-point number.\n\nIf input vector is an empty array, unit vector returns an empty array and norm returns NaN.", null, "## input data point\n\nInput data points.\n\nThis input changes to input vector when the data type is a 1D array of double-precision, floating-point numbers or an array of complex double-precision, floating-point numbers.", null, "## norm type\n\nType of norm this node uses to compute the norm.\n\nThis input is available only if you wire an array of double-precision, floating-point numbers or an array of complex double-precision, floating-point numbers to input vector.\n\nLet x represent input vector, y represent user defined norm, and ||x|| represent the norm of the input vector.\n\nName Value Description\n1-norm 1 Calculates norm using the following equation: $‖x‖=|{x}_{0}|+|{x}_{1}|+\\dots +|{x}_{n-1}|$.\n2-norm 2 Calculates norm using the following equation: $‖x‖=\\sqrt{\\left({|{x}_{0}|}^{2}+{|{x}_{1}|}^{2}+\\dots +{|{x}_{n-1}|}^{2}\\right)}$.\nInf-norm 3 Calculates norm using the following equation: $‖x‖={\\mathrm{max}}_{i}\\left(|{x}_{i}|\\right)$.\n-Inf-norm 4 Calculates norm using the following equation: $‖x‖={\\mathrm{min}}_{i}\\left(|{x}_{i}|\\right)$.\nUser Defined 5 Calculates norm using the following equation: $‖x‖={\\left({|{x}_{0}|}^{y}+{|{x}_{1}|}^{y}+\\dots +{|{x}_{n-1}|}^{y}\\right)}^{\\frac{1}{y}}$.\n\nDefault: 2-norm", null, "## sample length\n\nLength of each set of data.\n\nThe node performs computation for each set of data. sample length must be greater than zero.\n\nThis input is available only if you wire a double-precision, floating-point number to input vector.\n\nDefault: 100", null, "## user defined norm\n\nValue that defines the norm type.\n\nThis node uses user defined norm as the norm type only if you set norm type to User Defined. user defined norm must be nonzero.\n\nThis input is available only if you wire an array of double-precision, floating-point numbers or an array of complex double-precision, floating-point numbers to input vector.\n\nDefault: -1", null, "## error in\n\nError conditions that occur before this node runs.\n\nThe node responds to this input according to standard error behavior.\n\nStandard Error Behavior\n\nMany nodes provide an error in input and an error out output so that the node can respond to and communicate errors that occur while code is running. The value of error in specifies whether an error occurred before the node runs. Most nodes respond to values of error in in a standard, predictable way.\n\nerror in does not contain an error error in contains an error", null, "", null, "If no error occurred before the node runs, the node begins execution normally.\n\nIf no error occurs while the node runs, it returns no error. If an error does occur while the node runs, it returns that error information as error out.\n\nIf an error occurred before the node runs, the node does not execute. Instead, it returns the error in value as error out.\n\nDefault: No error", null, "## unit vector\n\nOutput normalized vector.\n\nThis output can return an array of double-precision, floating-point numbers or an array of complex double-precision, floating-point numbers.", null, "## norm\n\nNorm of the input vector.", null, "## error out\n\nError information.\n\nThe node produces this output according to standard error behavior.\n\nStandard Error Behavior\n\nMany nodes provide an error in input and an error out output so that the node can respond to and communicate errors that occur while code is running. The value of error in specifies whether an error occurred before the node runs. Most nodes respond to values of error in in a standard, predictable way.\n\nerror in does not contain an error error in contains an error", null, "", null, "If no error occurred before the node runs, the node begins execution normally.\n\nIf no error occurs while the node runs, it returns no error. If an error does occur while the node runs, it returns that error information as error out.\n\nIf an error occurred before the node runs, the node does not execute. Instead, it returns the error in value as error out.\n\n## Algorithm for Calculating unit vector\n\nThis node calculates unit vector using the following equation:\n\n$U=\\frac{X}{‖X‖}$\n\nwhere U is unit vector.\n\nWhere This Node Can Run:\n\nDesktop OS: Windows\n\nFPGA: Not supported\n\nWeb Server: Not supported in VIs that run in a web application" ]
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https://answers.com.tn/how-do-you-interpret-a-bell-curve-standard-deviation/
[ "Sorry, you do not have a permission to add a post.\n\nPlease briefly explain why you feel this question should be reported.\n\n# How do you interpret a bell curve standard deviation?\n\nHow do you interpret a bell curve standard deviation? Look at the symmetrical shape of a bell curve. The center should be where the largest portion of scores would fall. The smallest areas to the far left and right would be where the very lowest and very highest scores would fall. Read across the curve from left to right.\n\n## What is a normal curve on a graph?\n\nThe normal distribution is a continuous probability distribution that is symmetrical on both sides of the mean, so the right side of the center is a mirror image of the left side. … The normal distribution is often called the bell curve because the graph of its probability density looks like a bell.\n\n## Is bell curve good or bad?\n\nPerformance appraisal using the bell curve will create a sense of uncertainty in the minds of the employees who have been graded badly because they might assume that in a tough job market, they would be the first ones to be fired. This would lead to a loss in morale and even poorer performance at the workplace.\n\n## What does the bell curve tell us?\n\nA bell curve is a graph depicting the normal distribution, which has a shape reminiscent of a bell. The top of the curve shows the mean, mode, and median of the data collected. … Bell curves (normal distributions) are used commonly in statistics, including in analyzing economic and financial data.\n\n## What are examples of normal distribution?\n\nLet’s understand the daily life examples of Normal Distribution.\n\n• Height. Height of the population is the example of normal distribution. …\n• Rolling A Dice. A fair rolling of dice is also a good example of normal distribution. …\n• Tossing A Coin. …\n• IQ. …\n• Technical Stock Market. …\n• Income Distribution In Economy. …\n• Shoe Size. …\n• Birth Weight.\n\n## How do you find the top 5 percent of a normal distribution?\n\nTo find the 5th percentile for Z (or the cutoff point where 5% of the population lies below it), look at the Z-table and find the probability that’s closest to 0.05. You see that the closest probability to 0.05 is either 0.0495 or 0.0505 (use 0.0505 in this case).\n\n## Is a bell curve a function?\n\nA bell-shaped function or simply ‘bell curve’ is a mathematical function having a characteristic « bell »-shaped curve. These functions are typically continuous or smooth, asymptotically approach zero for large negative/positive x, and have a single, unimodal maximum at small x.\n\n## What is the shape of a normal curve?\n\nA bell curve is a common type of distribution for a variable, also known as the normal distribution. The term « bell curve » originates from the fact that the graph used to depict a normal distribution consists of a symmetrical bell-shaped curve.\n\nWhen a teacher grades on a curve, they adjust their class’ scores accordingly so that those who need the grade boost will get it and pass without these changes becoming unfair to those who scored high. Used correctly, curving can benefit students and ensure that all students receive the same standardized scores.\n\n## Why is The Bell Curve important?\n\nIt is important in the field of statistics because they model many real-world data like test results and performance reviews of employees. The bell curve has one mode, and it coincides with the mean and median. … For a bell curve, exactly 95% of the data lies within the two standard deviations of the mean.\n\n## What is the average range on a bell curve?\n\nMost tests have average standard scores of 100. Increments of 15 are used to separate sections of the population into average, below average, and above average sections. For example, if your child gets a standard score between 85 and 115, these scores are considered within the average range.\n\n## How bell curve is used in performance appraisal?\n\nIf you’re unfamiliar with the bell curve rating system in performance appraisals, simply put, it’s a performance evaluation method that force ranks employees into a bell-shaped best to worst scale, which often looks something like this: High Performers (20%) Average Performers (70%)\n\n## How do you tell if a graph is normally distributed?\n\nIn order to be considered a normal distribution, a data set (when graphed) must follow a bell-shaped symmetrical curve centered around the mean. It must also adhere to the empirical rule that indicates the percentage of the data set that falls within (plus or minus) 1, 2 and 3 standard deviations of the mean.\n\n## What is another name of normal distribution?\n\nNormal distribution, also known as the Gaussian distribution, is a probability distribution that is symmetric about the mean, showing that data near the mean are more frequent in occurrence than data far from the mean. In graph form, normal distribution will appear as a bell curve.\n\n## What are the 5 properties of normal distribution?\n\nProperties of a normal distribution\n\nThe mean, mode and median are all equal. The curve is symmetric at the center (i.e. around the mean, μ). Exactly half of the values are to the left of center and exactly half the values are to the right. The total area under the curve is 1.\n\n## What is the z-score 10%?\n\nPercentile z-Score\n10\n-1.282\n11 -1.227\n12 -1.175\n13 -1.126\n\n## How do you find a normal distribution percentage?\n\nConsider the normal distribution N(100, 10). To find the percentage of data below 105.3, that is P(x < 105.3), standartize first: P(x < 105.3) = P ( z < 105.3 − 100 10 ) = P(z < 0.53). Then find the proportion corresponding to 0.53 in Table A: look for the intersection of the row labeled 0.5 and the column labeled .\n\n## What is the z-score for a 95% confidence interval?\n\nThe value of z* for a confidence level of 95% is 1.96. After putting the value of z*, the population standard deviation, and the sample size into the equation, a margin of error of 3.92 is found. The formulas for the confidence interval and margin of error can be combined into one formula.\n\n## How do you calculate bell curve?\n\nAssign the number range for the numerical values, using the lowest observation to the highest observation. Use the bell curve formula to calculate the y axis value for each x axis value. The bell curve formula is y = (e^(?-x?\n\n## What is bell curve grading?\n\nGrading on a curve, more commonly known as bell curving, is a grading practice in which students’ grades are allocated over a normal distribution. … This practice can result in adjusting an entire class average up or down, benefiting those whose grades increase while disadvantaging others whose grades decrease.\n\n## What do you call the center of the normal curve?\n\nAll a z-table does is measure those probabilities (i.e. 50%) and put them in standard deviations from the mean. The mean is in the center of the standard normal distribution, and a probability of 50% equals zero standard deviations.\n\nWhen courses are graded on a curve there is less interaction between students, hence less learning. We have measured that there is also generally overall lower motivation.\n\n## Can grades be curved down?\n\nIn the American education system, a curving method is often employed before assigning grades. … While there exists variation in how this takes place, there is a major downside to curving a given class section’s grades; these grades can be curved down instead of up." ]
[ null ]
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https://answers.everydaycalculation.com/divide-fractions/2-5-divided-by-5-10
[ "Solutions by everydaycalculation.com\n\n## Divide 2/5 with 5/10\n\n2/5 ÷ 5/10 is 4/5.\n\n#### Steps for dividing fractions\n\n1. Find the reciprocal of the divisor\nReciprocal of 5/10: 10/5\n2. Now, multiply it with the dividend\nSo, 2/5 ÷ 5/10 = 2/5 × 10/5\n3. = 2 × 10/5 × 5 = 20/25\n4. After reducing the fraction, the answer is 4/5\n\nMathStep (Works offline)", null, "Download our mobile app and learn to work with fractions in your own time:" ]
[ null, "https://answers.everydaycalculation.com/mathstep-app-icon.png", null ]
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https://www.hexdictionary.com/hex/149
[ "Decimal: 329\nBinary: 101001001\n\nCan also be written as 0x149.\n\nDecimal to hex: 149 = 329. Binary to hex: 149 = 101001001\n\nCosine of 149 (329) is -0.64694230886611, or 0 in hexadecimal\nHyperbolic Cosine of 149 (329) is 3.8181637536449E+142, or 0 in hexadecimal\nBinary of 149 (329) is 101001001,\nHexadecimal of 149 (329) is 149,\nOctal of 149 (329) is 511,\nDegrees to Radian of 149 (329) is 5.7421332390613, or 5 in hexadecimal\nExponent of 149 (329) is 7.6363275072898E+142, or 0 in hexadecimal\nLogarithm of 149 (329) is 5.7960577507654, or 5 in hexadecimal\nRadian to Degrees of 149 (329) is 18850.311459804, or 49A2 in hexadecimal\nSine of 149 (329) is 0.76253894916849, or 0 in hexadecimal\nHyperbolic Sine of 149 (329) is 3.8181637536449E+142, or 0 in hexadecimal\nSquare Root of 149 (329) is 18.138357147217, or 12 in hexadecimal\nTangent of 149 (329) is -1.1786815280407, or FFFFFFFFFFFFFFFF in hexadecimal\nHyperbolic Tangent of 149 (329) is 1, or 1 in hexadecimal" ]
[ null ]
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https://www.fxsolver.com/browse/?like=298&p=164
[ "'\n\n# Search results\n\nFound 1756 matches\nWind turbine angular velocity\n\nThe formula for the calculation of the angular velocity of a wind turbine rotor. The definition is according to the IEC 61400-2. ... more\n\nLinear mass density\n\nLinear density is the measure of a quantity of any characteristic value per unit of length. Linear mass density (titer in textile engineering, the amount ... more\n\nDarcy's Law for membrane performance application\n\nThe selection of synthetic membranes for a targeted separation process is usually based on few requirements. Membranes have to provide enough mass transfer ... more\n\nFront focal length (FFL)\n\nA lens is a transmissive optical device which affects the focusing of a light beam through refraction. A simple lens consists of a single piece of ... more\n\nDoping (semiconductor)\n\nIn semiconductor production, doping intentionally introduces impurities into an extremely pure (also referred to as intrinsic) semiconductor for the ... more\n\nGraham's Law of Effusion\n\nEffusion is the process in which a gas escapes through a small hole. This occurs if the diameter of the hole is considerably smaller than the mean free ... more\n\nSecant of the sum of three angles\n\nTrigonometric identities are equalities that involve trigonometric functions and are true for every single value of the occurring variables. Geometrically, ... more\n\nCosecant of the sum of three angles\n\nTrigonometric identities are equalities that involve trigonometric functions and are true for every single value of the occurring variables. Geometrically, ... more\n\nLength of an Arc of a Circle\n\nCircular arc is a segment of a circle, or of its circumference (boundary) if the circle is considered to be a disc. Central angle is an angle whose apex ... more\n\nMagnetic diffusivity\n\nThe magnetic diffusivity is a parameter in plasma physics which appears in the magnetic Reynolds number.\n\n... more\n\n...can't find what you're looking for?\n\nCreate a new formula\n\n### Search criteria:\n\nSimilar to formula\nCategory" ]
[ null ]
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https://www.numbersaplenty.com/305327476897
[ "Cookie Consent by FreePrivacyPolicy.com\nSearch a number\nBaseRepresentation\nbin1000111000101101110…\n…11111001000010100001\n31002012002210111220011021\n410130112323321002201\n520000302313230042\n6352133203245441\n731026204506062\noct4342673710241\n91065083456137\n10305327476897\n11108541445573\n124b211679881\n1322a3b7889c1\n1410ac68ca569\n157e20250867\nhex4716ef90a1\n\n305327476897 has 2 divisors, whose sum is σ = 305327476898. Its totient is φ = 305327476896.\n\nThe previous prime is 305327476799. The next prime is 305327476901. The reversal of 305327476897 is 798674723503.\n\nIt is a happy number.\n\nIt is a strong prime.\n\nIt can be written as a sum of positive squares in only one way, i.e., 228607340641 + 76720136256 = 478129^2 + 276984^2 .\n\nIt is a cyclic number.\n\nIt is not a de Polignac number, because 305327476897 - 215 = 305327444129 is a prime.\n\nIt is not a weakly prime, because it can be changed into another prime (305327476397) by changing a digit.\n\nIt is a pernicious number, because its binary representation contains a prime number (19) of ones.\n\nIt is a polite number, since it can be written as a sum of consecutive naturals, namely, 152663738448 + 152663738449.\n\nIt is an arithmetic number, because the mean of its divisors is an integer number (152663738449).\n\nAlmost surely, 2305327476897 is an apocalyptic number.\n\nIt is an amenable number.\n\n305327476897 is a deficient number, since it is larger than the sum of its proper divisors (1).\n\n305327476897 is an equidigital number, since it uses as much as digits as its factorization.\n\n305327476897 is an odious number, because the sum of its binary digits is odd.\n\nThe product of its (nonzero) digits is 53343360, while the sum is 61.\n\nThe spelling of 305327476897 in words is \"three hundred five billion, three hundred twenty-seven million, four hundred seventy-six thousand, eight hundred ninety-seven\"." ]
[ null ]
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https://byjus.com/question-answer/according-to-the-second-law-of-motion-force-applied-on-an-object-is-given-by/
[ "", null, "", null, "Question\n\n# According to the second law of motion, force applied on an object is given by:Product of mass and velocity of object.Product of mass and acceleration of object.Sum of mass and acceleration of object.Sum of mass of and velocity of object.\n\nSolution\n\n## The correct option is B Product of mass and acceleration of object.Newton's second law gives the relationship between force and acceleration as force is the product of mass and acceleration.", null, "", null, "Suggest corrections", null, "", null, "", null, "" ]
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https://studylib.net/doc/11665116/course-111--algebra--19th-january-2007-1.-given-u-%3D--u
[ "# Course 111: Algebra, 19th January 2007 1. Given u = (u", null, "```Course 111: Algebra, 19th January 2007\nTo be handed in at tutorials on Jan 22nd and 23rd.\n1. Given u = (u1 , u2 , . . . , un ) and v = (v1 , v2 , . . . , vn ) are two vectors in Rn\nand that w1 , w2 , . . . , wn are positive real numbers (called the weights).\nThe weighted Euclidean inner product is defined\n(u, v) = w1 u1 v1 + w2 u2 v2 + . . . wn un vn .\nShow that this is indeed an inner product.\nSolution: to show this is an inner product we need to show it satisfies\nthe following:\n(i)(u, v) = (v, u)\nWe know that u and v in Rn then\n(u, v) = w1 u1 v1 +w2 u2 v2 +. . .+wn un vn = w1 v1 u1 +w2 v2 u2 +. . .+wn vn un = (v, u)\nsince the ui and vi are real numbers which commute under multiplication.\n(ii) (u, u) ≥ 0 and (u, u) = 0 iff u = 0\n(u, u) = w1 u21 + w2 u22 + . . . + wn u2n ≥ 0\n(1)\nsince the weights wi are all positive and the u2i are also positive.\nNow consider (u, u) = 0. In this case since each of the terms in Eqn is\ngreater than or equal to zero, and the weights are all positive numbers\nthe only way (u, u) = 0 can be zero is for each u2i = 0 and therefore\nui = 0 so u = 0.\n(iii) (αu + βv, y) = α(u, y) + β(v, y) where y is also a vector and α, β\nare scalars.\nAgain, just using the definition of the inner product given\n(αu + βv, y) = w1 (αu1 + βv1 )y1 + w2 (αu2 + βv2 )y2 + . . . + wn (αun + βvn )yn\n= w1 αu1 y1 + w2 αu2 y2 + . . . + wn αun yn\n+w1 βv1 y1 + w2 βv2 y2 + . . . + wn βvn yn\n= α(w1 u1 y1 + w2 u2 y2 + . . . + wn un yn )\n+β(w1 v1 y1 + w2 v2 y2 + . . . + wn vn yn )\n= α(u, y) + β(v, y)\nas required.\n2. Compute (u, v), ||u|| and d(u, v) for the following vectors and inner\nproducts\n• u = (2, −1, 4), v = (3, 2, 0) in R3 with the standard Euclidean\ninner product.\n(u, v) = (2)(3) + (−1)(2) + (4)(0) = 4\n1\n||u|| = (u, u) 2 =\nq\n√\n(2)2 + (−1)2 + (4)2 =\nd(u, v) = ||u−v|| = ||(−1, −3, 4)|| =\nq\n21\n(−1)2 + (−3)2 + (4)2 =\n√\n26\n• u = (2, −1, 4), v = (3, 2, 0) in R3 with the weighted Euclidean\ninner product and w1 = 2, w2 = 6, w3 = 1/5.\n(u, v) = (2)(3)(2) + (−1)(2)(6) + (4)(0)\n1\n2\n||u|| = (u, u) =\ns\n(2)2 (2) + (−1)2 (6) + (4)2\nd(u, v) = ||u−v|| = ||(−1, −3, 4)|| =\n1\n=0\n5\n1\n=\n5\ns\n86 √\n= 17.2\n5\ns\n(−1)2 (2) + (−3)2 (6) + (4)2\n1\n=\n5\ns\n296\n5\n• u = x, v = x2 in C[0, 1] the set of continous real-valued\nfunctions\nR1\non [0, 1] and an inner product, (f (t), g(t)) = 0 f (t)g(t)dt\n(u, v) =\n1\n2\nZ\n||u|| = (u, u) =\n1\n2\nx(x )dx =\n0\ns\nZ\nZ\n1\n0\n1\nx(x)dx =\n0\n2\nd(u, v) = ||u−v|| = ||x−x || =\ns\nZ\n1 4 1 1\nx dx = x =\n4 0 4\n3\ns\nZ\n1\nx2 dx =\n0\ns\n1\n0\n(x −\nx2 )dx\n=\n1\n1 3 1\nx =√\n3 0\n3\ns\n1 5 1 4 1 3 1\n1\nx − x + x =√\n5\n2\n3\n30\n0\n```" ]
[ null, "https://s2.studylib.net/store/data/011665116_1-35991ec7e1c838b6fbae0748a411acd1.png", null ]
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https://math.stackexchange.com/questions/666796/elementary-proof-that-a-n-to-a-implies-a-nr-to-ar-for-r-in-mathbbq/667040
[ "# Elementary proof that $a_n \\to a \\implies a_n^r \\to a^r$ for $r \\in \\mathbb{Q}$\n\nI've been looking for an elementary proof of the fact that rational exponentiation is continuous (for sequences). Let $r = p/q \\in \\mathbb{Q},$ with $p,q \\in \\mathbb{N}.$ Assuming $|a_n - a| \\to 0,$ we have\n\n$$|a_n^r - a^r| = |(a_n^{1/q})^p - (a^{1/q})^p| = \\left|a_n^{1/q} - a^{1/q}\\right|\\left|\\sum_{i=0}^{p-1} a_n^{p-1-i}a^i\\right|.$$\n\nIs there a way to bound this further in terms of $|a_n - a|$ to conclude?\n\nThank you.\n\n• If you're willing to believe that $a^p$ and $a^{\\frac{1}{q}}$ are continuous, then this simply follows from continuity of compositions. Or are you looking for a proof of those as well? – EuYu Feb 7 '14 at 1:18\n• @EuYu I'd like a proof which goes along the lines of what I started, if possible. – user126869 Feb 7 '14 at 1:39\n\nWe need to establish the following inequalities $$rx^{r - 1}(x - y) > x^{r} - y^{r} > ry^{r - 1}(x - y)$$ and $$sx^{s - 1}(x - y) < x^{s} - y^{s} < sy^{s - 1}(x - y)$$ where $x > y > 0$ and $r > 1, 0 < s < 1$ with $r, s \\in \\mathbb{Q}$. Also these inequalities need to be established via algebra. I will establish here the inequalities related to $r > 1$.\nLet $\\alpha > 1$ be a real number and assume $r$ is a positive integer. Then we can easily see that $$r\\alpha^{r} > \\alpha^{r - 1} + \\alpha^{r - 2} + \\cdots + 1$$ so that $$r\\alpha^{r}(\\alpha - 1) > \\alpha^{r} - 1$$ Adding $r(\\alpha^{r} - 1)$ on each side we get $$r(\\alpha^{r + 1} - 1) > (r + 1)(\\alpha^{r} - 1)$$ and finally $$\\frac{\\alpha^{r + 1} - 1}{r + 1} > \\frac{\\alpha^{r} - 1}{r}$$ It thus follows that the expression $\\dfrac{\\alpha^{r} - 1}{r}$ increases with $r$ and therefore if $r, s$ are positive integers with $r > s$ then $$\\frac{\\alpha^{r} - 1}{r} > \\frac{\\alpha^{s} - 1}{s}\\,\\,\\,\\cdots (1)$$ It follows that if $r$ is a positive integer and $r > 1$ then $$\\frac{\\alpha^{r} - 1}{r} > \\frac{\\alpha^{1} - 1}{1}$$ so that $$\\alpha^{r} - 1 > r(\\alpha - 1)\\,\\,\\,\\cdots (2)$$ Similarly we can show that if $0 < \\beta < 1$ then $$\\frac{1 - \\beta^{r}}{r} < \\frac{1 - \\beta^{s}}{s}\\,\\,\\,\\cdots (3)$$ and $$1 - \\beta^{r} < r(1 - \\beta)\\,\\,\\,\\cdots (4)$$ if $r > 1$.\nThe inequalities above have been proved with restriction that $r, s$ be positive integers. This can be easily extended to the case when $r, s$ are rational. Let $r = a/b, s = c/d$ where $a, b, c, d$ are positive integers and then $r > s$ implies that $ad > bc$. Let $\\gamma = \\alpha^{1/bd}$ so that $\\alpha = \\gamma^{bd}$ then $\\gamma > 1$ and hence by $(1)$ we get $$\\frac{\\gamma^{ad} - 1}{ad} > \\frac{\\gamma^{bc} - 1}{bc}$$ or $$\\frac{\\alpha^{r} - 1}{r} > \\frac{\\alpha^{s} - 1}{s}$$ Similarly all the inequalities $(2), (3), (4)$ can be extended to rational values of $r, s$.\nNext if $\\alpha > 1$ then $0 < 1/\\alpha < 1$ and $0 < \\beta < 1$ implies $1/\\beta > 1$. Therefore writing $1/\\beta$ for $\\alpha$ in $(2)$ and $1/\\alpha$ for $\\beta$ in $(4)$ we get $$\\alpha^{r} - 1 < r\\alpha^{r - 1}(\\alpha - 1)\\,\\,\\,\\cdots (5)$$ and $$1 - \\beta^{r} > r\\beta^{r - 1}(1 - \\beta)\\,\\,\\,\\cdots (6)$$ If $x > y > 0$ then we can put $\\alpha = x/y$ and $\\beta = y/x$ in the above inequalities and get $$rx^{r - 1}(x - y) > x^{r} - y^{r} > ry^{r - 1}(x - y)$$\nUsing these inequalities it is possible to bound $|a_{n}^{r} - a^{r}|$ in terms of $|a_{n} - a|$ and you can complete your proof easily.\nUpdate: This is essentially the elementary technique used to prove continuity of $f(x) = x^{r}$ for $x > 0$ and $r \\in \\mathbb{Q}$ and if you notice carefully it can also be used to establish the differentiation formula $(x^{r})' = rx^{r - 1}$." ]
[ null ]
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https://www.ademcetinkaya.com/2023/10/should-you-buy-now-or-wait-lonarb-stock.html
[ "Outlook: ARGO BLOCKCHAIN PLC is assigned short-term B2 & long-term Baa2 estimated rating.\nAUC Score : What is AUC Score?\nShort-Term Revised1 :\nDominant Strategy : Speculative Trend\nTime series to forecast n: for Weeks2\nMethodology : Modular Neural Network (DNN Layer)\nHypothesis Testing : Chi-Square\nSurveillance : Major exchange and OTC\n\n1The accuracy of the model is being monitored on a regular basis.(15-minute period)\n\n2Time series is updated based on short-term trends.\n\nARGO BLOCKCHAIN PLC prediction model is evaluated with Modular Neural Network (DNN Layer) and Chi-Square1,2,3,4 and it is concluded that the LON:ARB stock is predictable in the short/long term. In a modular neural network (MNN), a DNN layer is a type of module that is used to learn complex relationships between input and output data. DNN layers are made up of a series of artificial neurons, which are connected to each other by weighted edges. The weights of the edges are adjusted during training to minimize the error between the network's predictions and the desired output. DNN layers are used in a variety of MNN applications, including natural language processing, speech recognition, and machine translation. In natural language processing, DNN layers are used to extract features from text data, such as the sentiment of a sentence or the topic of a conversation. In speech recognition, DNN layers are used to convert audio data into text data. In machine translation, DNN layers are used to translate text from one language to another.5 According to price forecasts for 1 Year period, the dominant strategy among neural network is: Speculative Trend", null, "## Key Points\n\n1. Technical Analysis with Algorithmic Trading\n2. Investment Risk\n3. Market Signals\n\n## LON:ARB Stock Price Forecast\n\nWe consider ARGO BLOCKCHAIN PLC Decision Process with Modular Neural Network (DNN Layer) where A is the set of discrete actions of LON:ARB stock holders, F is the set of discrete states, P : S × F × S → R is the transition probability distribution, R : S × F → R is the reaction function, and γ ∈ [0, 1] is a move factor for expectation.1,2,3,4\n\nSample Set: Neural Network\nStock/Index: LON:ARB ARGO BLOCKCHAIN PLC\nTime series to forecast: 1 Year\n\nAccording to price forecasts, the dominant strategy among neural network is: Speculative Trend\n\nF(Chi-Square)6,7= $\\begin{array}{cccc}{p}_{a1}& {p}_{a2}& \\dots & {p}_{1n}\\\\ & ⋮\\\\ {p}_{j1}& {p}_{j2}& \\dots & {p}_{jn}\\\\ & ⋮\\\\ {p}_{k1}& {p}_{k2}& \\dots & {p}_{kn}\\\\ & ⋮\\\\ {p}_{n1}& {p}_{n2}& \\dots & {p}_{nn}\\end{array}$ X R(Modular Neural Network (DNN Layer)) X S(n):→ 1 Year $∑ i = 1 n s i$\n\nn:Time series to forecast\n\np:Price signals of LON:ARB stock\n\nj:Nash equilibria (Neural Network)\n\nk:Dominated move of LON:ARB stock holders\n\na:Best response for LON:ARB target price\n\nIn a modular neural network (MNN), a DNN layer is a type of module that is used to learn complex relationships between input and output data. DNN layers are made up of a series of artificial neurons, which are connected to each other by weighted edges. The weights of the edges are adjusted during training to minimize the error between the network's predictions and the desired output. DNN layers are used in a variety of MNN applications, including natural language processing, speech recognition, and machine translation. In natural language processing, DNN layers are used to extract features from text data, such as the sentiment of a sentence or the topic of a conversation. In speech recognition, DNN layers are used to convert audio data into text data. In machine translation, DNN layers are used to translate text from one language to another.5 A chi-squared test is a statistical hypothesis test that assesses whether observed frequencies in a sample differ significantly from expected frequencies. It is one of the most widely used statistical tests in the social sciences and in many areas of observational research. The chi-squared test is a non-parametric test, meaning that it does not assume that the data is normally distributed. This makes it a versatile tool that can be used to analyze a wide variety of data. There are two main types of chi-squared tests: the chi-squared goodness of fit test and the chi-squared test of independence.6,7\n\nFor further technical information as per how our model work we invite you to visit the article below:\n\nHow do AC Investment Research machine learning (predictive) algorithms actually work?\n\n### LON:ARB Stock Forecast (Buy or Sell) Strategic Interaction Table\n\nStrategic Interaction Table Legend:\n\nX axis: *Likelihood% (The higher the percentage value, the more likely the event will occur.)\n\nY axis: *Potential Impact% (The higher the percentage value, the more likely the price will deviate.)\n\nZ axis (Grey to Black): *Technical Analysis%\n\n### Financial Data Adjustments for Modular Neural Network (DNN Layer) based LON:ARB Stock Prediction Model\n\n1. If a put option obligation written by an entity or call option right held by an entity prevents a transferred asset from being derecognised and the entity measures the transferred asset at amortised cost, the associated liability is measured at its cost (ie the consideration received) adjusted for the amortisation of any difference between that cost and the gross carrying amount of the transferred asset at the expiration date of the option. For example, assume that the gross carrying amount of the asset on the date of the transfer is CU98 and that the consideration received is CU95. The gross carrying amount of the asset on the option exercise date will be CU100. The initial carrying amount of the associated liability is CU95 and the difference between CU95 and CU100 is recognised in profit or loss using the effective interest method. If the option is exercised, any difference between the carrying amount of the associated liability and the exercise price is recognised in profit or loss.\n2. Changes in market conditions that give rise to market risk include changes in a benchmark interest rate, the price of another entity's financial instrument, a commodity price, a foreign exchange rate or an index of prices or rates.\n3. An equity method investment cannot be a hedged item in a fair value hedge. This is because the equity method recognises in profit or loss the investor's share of the investee's profit or loss, instead of changes in the investment's fair value. For a similar reason, an investment in a consolidated subsidiary cannot be a hedged item in a fair value hedge. This is because consolidation recognises in profit or loss the subsidiary's profit or loss, instead of changes in the investment's fair value. A hedge of a net investment in a foreign operation is different because it is a hedge of the foreign currency exposure, not a fair value hedge of the change in the value of the investment.\n4. Financial assets that are held within a business model whose objective is to hold assets in order to collect contractual cash flows are managed to realise cash flows by collecting contractual payments over the life of the instrument. That is, the entity manages the assets held within the portfolio to collect those particular contractual cash flows (instead of managing the overall return on the portfolio by both holding and selling assets). In determining whether cash flows are going to be realised by collecting the financial assets' contractual cash flows, it is necessary to consider the frequency, value and timing of sales in prior periods, the reasons for those sales and expectations about future sales activity. However sales in themselves do not determine the business model and therefore cannot be considered in isolation. Instead, information about past sales and expectations about future sales provide evidence related to how the entity's stated objective for managing the financial assets is achieved and, specifically, how cash flows are realised. An entity must consider information about past sales within the context of the reasons for those sales and the conditions that existed at that time as compared to current conditions.\n\n*International Financial Reporting Standards (IFRS) adjustment process involves reviewing the company's financial statements and identifying any differences between the company's current accounting practices and the requirements of the IFRS. If there are any such differences, neural network makes adjustments to financial statements to bring them into compliance with the IFRS.\n\n### LON:ARB ARGO BLOCKCHAIN PLC Financial Analysis*\n\nRating Short-Term Long-Term Senior\nOutlook*B2Baa2\nIncome StatementB1Ba2\nBalance SheetBa2Baa2\nLeverage RatiosBaa2Ba3\nCash FlowCaa2Ba3\nRates of Return and ProfitabilityCBaa2\n\n*Financial analysis is the process of evaluating a company's financial performance and position by neural network. It involves reviewing the company's financial statements, including the balance sheet, income statement, and cash flow statement, as well as other financial reports and documents.\nHow does neural network examine financial reports and understand financial state of the company?\n\n## References\n\n1. Kitagawa T, Tetenov A. 2015. Who should be treated? Empirical welfare maximization methods for treatment choice. Tech. Rep., Cent. Microdata Methods Pract., Inst. Fiscal Stud., London\n2. Jorgenson, D.W., Weitzman, M.L., ZXhang, Y.X., Haxo, Y.M. and Mat, Y.X., 2023. Can Neural Networks Predict Stock Market?. AC Investment Research Journal, 220(44).\n3. Lai TL, Robbins H. 1985. Asymptotically efficient adaptive allocation rules. Adv. Appl. Math. 6:4–22\n4. Gentzkow M, Kelly BT, Taddy M. 2017. Text as data. NBER Work. Pap. 23276\n5. M. J. Hausknecht and P. Stone. Deep recurrent Q-learning for partially observable MDPs. CoRR, abs/1507.06527, 2015\n6. Friedman JH. 2002. Stochastic gradient boosting. Comput. Stat. Data Anal. 38:367–78\n7. V. Borkar. A sensitivity formula for the risk-sensitive cost and the actor-critic algorithm. Systems & Control Letters, 44:339–346, 2001\nFrequently Asked QuestionsQ: What is the prediction methodology for LON:ARB stock?\nA: LON:ARB stock prediction methodology: We evaluate the prediction models Modular Neural Network (DNN Layer) and Chi-Square\nQ: Is LON:ARB stock a buy or sell?\nA: The dominant strategy among neural network is to Speculative Trend LON:ARB Stock.\nQ: Is ARGO BLOCKCHAIN PLC stock a good investment?\nA: The consensus rating for ARGO BLOCKCHAIN PLC is Speculative Trend and is assigned short-term B2 & long-term Baa2 estimated rating.\nQ: What is the consensus rating of LON:ARB stock?\nA: The consensus rating for LON:ARB is Speculative Trend.\nQ: What is the prediction period for LON:ARB stock?\nA: The prediction period for LON:ARB is 1 Year\nWhat did you think about the prediction? (Insufficient-Outstanding)\nTell us how we can improve PredictiveAI" ]
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https://physics.stackexchange.com/questions/602814/a-problem-with-the-bcs-energy-expectation-value-of-an-excited-state
[ "# A problem with the BCS energy expectation value of an excited state\n\nI want to calculate the energy expectation value of the following state. \\begin{align} |\\Psi_{ex}\\rangle = \\hat{c}_{-k'\\downarrow}^\\dagger \\hat{c}_{k''\\uparrow}^\\dagger \\prod_{k \\neq k', k''}(u_{k} + v_{k}\\hat{c}_{k\\uparrow}^\\dagger \\hat{c}_{-k\\downarrow}^\\dagger)|0\\rangle \\end{align} The hamiltonian is the reduced BCS hamiltonian: \\begin{align} \\hat{H} &= \\sum_{k, \\: \\sigma}\\zeta_{k} \\hat{c}_{k\\sigma}^\\dagger\\hat{c}_{k\\sigma} + \\frac{1}{\\Omega}\\sum_{k,k'}V_{k'-k} \\hat{c}_{k'\\uparrow}^\\dagger \\hat{c}_{-k'\\downarrow}^\\dagger \\hat{c}_{-k\\downarrow} \\hat{c}_{k\\uparrow} \\end{align} I tried this before but I got a wrong result (which I know is wrong when I compare it with the original BCS paper): \\begin{align} E_{ex} = \\sum_{k \\neq k', k''}2\\zeta_{k}|v_{k}|^2 + \\frac{1}{\\Omega}\\sum_{k,l \\neq k', k''}V_{l-k}u_{k}^*v_{k}v_{l}^*u_{l} \\end{align}\n\n• How did you get that? What is $\\zeta_k$? As a warm up, do you manage to get the correct BCS ground state energy? – Adam Dec 24 '20 at 15:23\n• It is the kinetic energy minus the chemical potential. And yes I got the correct BCS ground state energy. When I calculate this expectation value I split the sommation up in many case. For example for the kinetic energy term the terms where the operators in the hamiltonian are the same as k', k'' or a k not equal to any of those (and thus inside the product part of the excited state). The same logic I used for the interaction part. Thanks for the comment. – Audrique Dec 24 '20 at 20:29\n• I edited the hamiltonian. I didn't notice there was an epsilon. – Audrique Dec 25 '20 at 11:51\n\n## 1 Answer\n\nIt seems to be almost right, except some missing terms. In the kinetic energy part, you should have the additional $$\\zeta_{-k'}+\\zeta_{k''}.$$ This is because when evaluating $$\\left< \\Psi_{ex}|\\epsilon_k\\hat{c}_{-k'\\downarrow}^\\dagger\\hat{c}_{-k'\\downarrow}|\\Psi_{ex} \\right>$$, you will get a $$1$$ instead of $$v_{-k'}$$ when you move $$\\hat{c}_{-k'\\downarrow}$$ toward $$\\left.|0\\right>$$, which is multiplied to $$1$$ instead of $$v_{k'}^*$$ when you move $$\\hat{c}_{k'\\downarrow}^\\dagger$$ toward $$\\left<0|\\right.$$.\n\nThe interaction term for this particular excitation is actually what you suspected $$0$$. but the actual excitation is really what is described by a combination of $$\\hat{c}$$ on top of the BCS ground state which can be described by the Bogoliubov procedure $$\\hat{b}$$, which turns the $$k$$ related term into $$-v^*_k+u^*_k\\hat{c}_{k\\uparrow}^\\dagger\\hat{c}_{-k\\downarrow}^\\dagger$$.\n\n• Is this not equal to $\\left< 0| \\hat{c}_{k''\\uparrow} \\hat{c}_{-k'\\downarrow} \\hat{c}_{k'\\downarrow}^\\dagger\\hat{c}_{k'\\downarrow} \\hat{c}_{-k'\\downarrow}^\\dagger \\hat{c}_{k''\\uparrow}^\\dagger|0 \\right>$ which gives zero right? – Audrique Dec 25 '20 at 14:27\n• You were right. I meant $\\left<0|\\hat{c}_{k''\\uparrow}\\hat{c}_{-k'\\downarrow}\\hat{c}_{-k'\\downarrow}^\\dagger\\hat{c}_{-k'\\downarrow}\\hat{c}_{-k'\\downarrow}^\\dagger\\hat{c}_{k''\\uparrow}^\\dagger|0\\right>$. – C Tong Dec 25 '20 at 14:56\n• Thanks, now it makes sense to me! – Audrique Dec 25 '20 at 15:28\n• Maybe one last question, in the definition of the excitated state, is the product over k only for the positive k's (because otherwise pairs would be counted double) but in the sommations in the hamiltonian also over the negative k's? – Audrique Dec 25 '20 at 15:34\n• It would actually need something like $(u'+v' \\hat{c}_{-k'\\downarrow}^\\dagger \\hat{c}_{k''\\uparrow}^\\dagger)\\left.|\\Psi_{BCS}\\right>$ to produce the two summation terms. – C Tong Dec 25 '20 at 16:12" ]
[ null ]
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https://www.scipopt.org/doc-3.1.0/examples/VRP/pricer__vrp_8cpp_source.php
[ "", null, "# SCIP\n\nSolving Constraint Integer Programs\n\n Main Page Data Structures Files", null, "pricer_vrp.cpp Go to the documentation of this file. 1 /* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * */ 2 /* */ 3 /* This file is part of the program and library */ 4 /* SCIP --- Solving Constraint Integer Programs */ 5 /* */ 6 /* Copyright (C) 2002-2014 Konrad-Zuse-Zentrum */ 7 /* fuer Informationstechnik Berlin */ 8 /* */ 9 /* SCIP is distributed under the terms of the ZIB Academic License. */ 10 /* */ 11 /* You should have received a copy of the ZIB Academic License. */ 12 /* along with SCIP; see the file COPYING. If not email to [email protected]. */ 13 /* */ 14 /* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * */ 15  16 /**@file pricer_vrp.cpp 17  * @brief VRP pricer plugin 18  * @author Andreas Bley 19  * @author Marc Pfetsch 20  */ 21  22 #include \"pricer_vrp.h\" 23 #include \"pqueue.h\" 24  25 #include 26 #include 27 #include 28  29 #include \"scip/cons_linear.h\" 30  31 using namespace std; 32 using namespace scip; 33  34  35  36  37 /** Constructs the pricer object with the data needed 38  * 39  * An alternative is to have a problem data class which allows to access the data. 40  */ 42  SCIP* scip, /**< SCIP pointer */ 43  const char* p_name, /**< name of pricer */ 44  const int p_num_nodes, /**< number of nodes */ 45  const int p_capacity, /**< vehicle capacity */ 46  const vector< int >& p_demand, /**< demand array */ 47  const vector< vector >& p_distance, /**< matrix of distances */ 48  const vector< vector >& p_arc_var, /**< matrix of arc variables */ 49  const vector< vector >& p_arc_con, /**< matrix of arc constraints */ 50  const vector& p_part_con /**< array of partitioning constraints */ 51  ): 52  ObjPricer(scip, p_name, \"Finds tour with negative reduced cost.\", 0, TRUE), 53  _num_nodes(p_num_nodes), 54  _capacity(p_capacity), 55  _demand(p_demand), 56  _distance(p_distance), 57  _arc_var(p_arc_var), 58  _arc_con(p_arc_con), 59  _part_con(p_part_con) 60 {} 61  62  63 /** Destructs the pricer object. */ 65 {} 66  67  68 /** initialization method of variable pricer (called after problem was transformed) 69  * 70  * Because SCIP transformes the original problem in preprocessing, we need to get the references to 71  * the variables and constraints in the transformed problem from the references in the original 72  * problem. 73  */ 74 SCIP_DECL_PRICERINIT(ObjPricerVRP::scip_init) 75 { 76  for (int i = 0; i < num_nodes(); ++i) 77  { 78  for (int j = 0; j < i; ++j) 79  { 80  SCIP_CALL( SCIPgetTransformedVar(scip, _arc_var[i][j], &_arc_var[i][j]) ); 81  SCIP_CALL( SCIPgetTransformedCons(scip, _arc_con[i][j], &_arc_con[i][j]) ); 82  } 83  } 84  for (int i = 1; i < num_nodes(); ++i) 85  { 86  SCIP_CALL( SCIPgetTransformedCons(scip, _part_con[i], &_part_con[i]) ); 87  } 88  89  return SCIP_OKAY; 90 } 91  92  93 /** perform pricing 94  * 95  * @todo compute shortest length restricted tour w.r.t. duals 96  */ 97 SCIP_RETCODE ObjPricerVRP::pricing( 98  SCIP* scip, /**< SCIP data structure */ 99  bool isfarkas /**< whether we perform Farkas pricing */ 100  ) 101 { 102  /* allocate array for reduced costs */ 103  vector< vector > red_length(num_nodes()); 104  for (int i = 0; i < num_nodes(); ++i) 105  red_length[i].resize(i, 0.0); 106  107  /* compute reduced-cost arc lengths store only lower triangualar matrix, i.e., red_length[i][j] only for i > j */ 108  if ( isfarkas ) 109  { 110  for (int i = 0; i < num_nodes(); ++i) 111  { 112  assert( i == 0 || part_con(i) != 0 ); 113  for (int j = 0; j < i; ++j) 114  { 115  SCIP_Real r = 0.0; 116  assert( arc_con(i,j) != 0 ); 117  118  r -= SCIPgetDualfarkasLinear(scip, arc_con(i,j)); 119  if ( j != 0 ) 120  r -= 0.5 * SCIPgetDualfarkasLinear(scip, part_con(j)); 121  if ( i != 0 ) 122  r -= 0.5 * SCIPgetDualfarkasLinear(scip, part_con(i)); 123  red_length[i][j] = r; 124  } 125  } 126  } 127  else 128  { 129  for (int i = 0; i < num_nodes(); ++i) 130  { 131  assert( i == 0 || part_con(i) != 0 ); 132  for (int j = 0; j < i; ++j) 133  { 134  SCIP_Real r = 0.0; 135  assert( arc_con(i,j) != 0 ); 136  137  r -= SCIPgetDualsolLinear(scip, arc_con(i,j)); 138  if ( j != 0 ) 139  r -= 0.5 * SCIPgetDualsolLinear(scip, part_con(j)); 140  if ( i != 0 ) 141  r -= 0.5 * SCIPgetDualsolLinear(scip, part_con(i)); 142  red_length[i][j] = r; 143  } 144  } 145  } 146  147 #ifdef SCIP_OUTPUT 148  if ( isfarkas ) 149  { 150  SCIPinfoMessage(scip, NULL, \"dual ray solution:\\n\"); 151  for (int i = 0; i < num_nodes(); ++i) 152  { 153  for (int j = 0; j < i; ++j) 154  SCIPinfoMessage(scip, NULL, \"arc_%d_%d: %g\\n\", i, j, SCIPgetDualfarkasLinear(scip, arc_con(i,j))); 155  } 156  157  for (int i = 1; i < num_nodes(); ++i) 158  SCIPinfoMessage(scip, NULL, \"part_%d: %g\\n\", i, SCIPgetDualfarkasLinear(scip, part_con(i))); 159  160  for (int i = 0; i < num_nodes(); ++i) 161  { 162  for (int j = 0; j < i; ++j) 163  SCIPinfoMessage(scip, NULL, \"length_%d_%d: %g\\n\", i, j, red_length[i][j]); 164  } 165  } 166  else 167  { 168  SCIPinfoMessage(scip, NULL, \"dual solution:\\n\"); 169  for (int i = 0; i < num_nodes(); ++i) 170  { 171  for (int j = 0; j < i; ++j) 172  SCIPinfoMessage(scip, NULL, \"arc_%d_%d: %g\\n\", i, j, SCIPgetDualsolLinear(scip, arc_con(i,j))); 173  } 174  175  for (int i = 1; i < num_nodes(); ++i) 176  SCIPinfoMessage(scip, NULL, \"part_%d: %g\\n\", i, SCIPgetDualsolLinear(scip, part_con(i))); 177  178  for (int i = 0; i < num_nodes(); ++i) 179  { 180  for (int j = 0; j < i; ++j) 181  SCIPinfoMessage(scip, NULL, \"length_%d_%d: %g\\n\", i, j, red_length[i][j]); 182  } 183  } 184 #endif 185  186  /* compute shortest length restricted tour w.r.t. reduced-cost arc length */ 187  list tour; 188  SCIP_Real reduced_cost = find_shortest_tour(red_length, tour); 189  190  /* add tour variable */ 191  if ( SCIPisNegative(scip, reduced_cost) ) 192  { 193  return add_tour_variable(scip, tour); 194  } 195  196 #ifdef SCIP_OUTPUT 197  SCIP_CALL( SCIPwriteTransProblem(scip, \"vrp.lp\", \"lp\", FALSE) ); 198 #endif 199  200  return SCIP_OKAY; 201 } 202  203  204  205 /** Pricing of additional variables if LP is feasible. 206  * 207  * - get the values of the dual variables you need 208  * - construct the reduced-cost arc lengths from these values 209  * - find the shortest admissible tour with respect to these lengths 210  * - if this tour has negative reduced cost, add it to the LP 211  * 212  * possible return values for *result: 213  * - SCIP_SUCCESS : at least one improving variable was found, or it is ensured that no such variable exists 214  * - SCIP_DIDNOTRUN : the pricing process was aborted by the pricer, there is no guarantee that the current LP solution is optimal 215  */ 216 SCIP_DECL_PRICERREDCOST(ObjPricerVRP::scip_redcost) 217 { 218  SCIPdebugMessage(\"call scip_redcost ...\\n\"); 219  220  /* set result pointer, see above */ 221  *result = SCIP_SUCCESS; 222  223  /* call pricing routine */ 224  SCIP_CALL( pricing(scip, false) ); 225  226  return SCIP_OKAY; 227 } 228  229  230 /** Pricing of additional variables if LP is infeasible. 231  * 232  * - get the values of the dual Farks multipliers you need 233  * - construct the reduced-cost arc lengths from these values 234  * - find the shortest admissible tour with respect to these lengths 235  * - if this tour has negative reduced cost, add it to the LP 236  */ 237 SCIP_DECL_PRICERFARKAS(ObjPricerVRP::scip_farkas) 238 { 239  SCIPdebugMessage(\"call scip_farkas ...\\n\"); 240  241  /* call pricing routine */ 242  SCIP_CALL( pricing(scip, true) ); 243  244  return SCIP_OKAY; 245 } 246  247  248 /** add tour variable to problem */ 249 SCIP_RETCODE ObjPricerVRP::add_tour_variable( 250  SCIP* scip, /**< SCIP data structure */ 251  const list& tour /**< list of nodes in tour */ 252  ) 253 { 254  /* create meaningful variable name */ 255  char tmp_name; 256  char var_name; 257  SCIPsnprintf(var_name, 255, \"T\"); 258  for (list::const_iterator it = tour.begin(); it != tour.end(); ++it) 259  { 260  strncpy(tmp_name, var_name, 255); 261  SCIPsnprintf(var_name, 255, \"%s_%d\", tmp_name, *it); 262  } 263  SCIPdebugMessage(\"new variable <%s>\\n\", var_name); 264  265  /* create the new variable: Use upper bound of infinity such that we do not have to care about 266  * the reduced costs of the variable in the pricing. The upper bound of 1 is implicitly satisfied 267  * due to the set partitioning constraints. 268  */ 269  SCIP_VAR* var; 270  SCIP_CALL( SCIPcreateVar(scip, &var, var_name, 271  0.0, // lower bound 272  SCIPinfinity(scip), // upper bound 273  0, // objective 274  SCIP_VARTYPE_CONTINUOUS, // variable type 275  false, false, 0, 0, 0, 0, 0) ); 276  277  /* add new variable to the list of variables to price into LP (score: leave 1 here) */ 278  SCIP_CALL( SCIPaddPricedVar(scip, var, 1.0) ); 279  280  /* add coefficient into the set partition constraints */ 281  for (list::const_iterator it = tour.begin(); it != tour.end(); ++it) 282  { 283  assert( 0 <= *it && *it < num_nodes() ); 284  SCIP_CALL( SCIPaddCoefLinear(scip, part_con(*it), var, 1.0) ); 285  } 286  287  /* add coefficient into arc routing constraints */ 288  int last = 0; 289  for (list::const_iterator it = tour.begin(); it != tour.end(); ++it) 290  { 291  assert( 0 <= *it && *it < num_nodes() ); 292  SCIP_CALL( SCIPaddCoefLinear(scip, arc_con(last, *it), var, 1.0) ); 293  last = *it; 294  } 295  SCIP_CALL( SCIPaddCoefLinear(scip, arc_con(last, 0), var, 1.0 ) ); 296  297  /* cleanup */ 298  SCIP_CALL( SCIPreleaseVar(scip, &var) ); 299  300  return SCIP_OKAY; 301 } 302  303  304 /** Computes a shortest admissible tour with respect to the given lengths. The function must return 305  * the computed tour via the parameter tour and the length (w.r.t. given lengths) of this tour as 306  * return parameter. The returned tour must be the ordered list of customer nodes contained in the 307  * tour (i.e., 2-5-7 for the tour 0-2-5-7-0). 308  */ 309 namespace 310 { 311  312 /* types needed for prioity queue -------------------- */ 313 static const SCIP_Real eps = 1e-9; 314  315 struct PQUEUE_KEY 316 { 317  int demand; 318  SCIP_Real length; 319  320  PQUEUE_KEY() : demand(0), length(0.0) {} 321 }; 322  323 bool operator< (const PQUEUE_KEY& l1, const PQUEUE_KEY& l2) 324 { 325  if ( l1.demand < l2.demand ) 326  return true; 327  if ( l1.demand > l2.demand ) 328  return false; 329  if ( l1.length < l2.length-eps ) 330  return true; 331  /* not needed, since we return false anyway: 332  if ( l1.length > l2.length+eps ) 333  return false; 334  */ 335  return false; 336 } 337  338 typedef int PQUEUE_DATA; // node 339 typedef pqueue PQUEUE; 340 typedef PQUEUE::pqueue_item PQUEUE_ITEM; 341  342  343 /* types needed for dyn. programming table */ 344 struct NODE_TABLE_DATA 345 { 346  SCIP_Real length; 347  int predecessor; 348  PQUEUE::pqueue_item queue_item; 349  350  NODE_TABLE_DATA( ) : length(0.0), predecessor(-1), queue_item( NULL ) {} 351 }; 352  353 typedef int NODE_TABLE_KEY; // demand 354 typedef std::map< NODE_TABLE_KEY, NODE_TABLE_DATA > NODE_TABLE; 355 } 356  357  358 /** return negative reduced cost tour (uses restricted shortest path dynamic programming algorithm) 359  * 360  * The algorithm uses the priority queue implementation in pqueue.h. SCIP's implementation of 361  * priority queues cannot be used, since it currently does not support removal of elements that are 362  * not at the top. 363  */ 364 SCIP_Real ObjPricerVRP::find_shortest_tour( 365  const vector< vector >& length, /**< matrix of lengths */ 366  list& tour /**< list of nodes in tour */ 367  ) 368 { 369  tour.clear(); 370  371  SCIPdebugMessage(\"Enter RSP - capacity: %d\\n\", capacity()); 372  373  /* begin algorithm */ 374  PQUEUE PQ; 375  vector< NODE_TABLE > table(num_nodes()); 376  377  /* insert root node (start at node 0) */ 378  PQUEUE_KEY queue_key; 379  PQUEUE_DATA queue_data = 0; 380  PQUEUE_ITEM queue_item = PQ.insert(queue_key, queue_data); 381  382  NODE_TABLE_KEY table_key = 0; 383  NODE_TABLE_DATA table_entry; 384  385  /* run Dijkstra-like updates */ 386  while ( ! PQ.empty() ) 387  { 388  /* get front queue entry */ 389  queue_item = PQ.top(); 390  queue_key = PQ.get_key (queue_item); 391  queue_data = PQ.get_data(queue_item); 392  PQ.pop(); 393  394  /* get corresponding node and node-table key */ 395  const int curr_node = queue_data; 396  const SCIP_Real curr_length = queue_key.length; 397  const int curr_demand = queue_key.demand; 398  399  /* stop as soon as some negative length tour was found */ 400  if ( curr_node == 0 && curr_length < -eps ) 401  break; 402  403  /* stop as soon don't create multi-tours */ 404  if ( curr_node == 0 && curr_demand != 0 ) 405  continue; 406  407  /* update all active neighbors */ 408  for (int next_node = 0; next_node < num_nodes(); ++next_node) 409  { 410  if ( next_node == curr_node ) 411  continue; 412  if ( have_edge( next_node, curr_node ) == false ) 413  continue; 414  415  const int next_demand = curr_demand + demand(next_node); 416  417  if ( next_demand > capacity() ) 418  continue; 419  420  const SCIP_Real next_length = curr_length + ( curr_node > next_node ? 421  length[curr_node][next_node] : 422  length[next_node][curr_node] ); 423  424  NODE_TABLE& next_table = table[next_node]; 425  426  /* check if new table entry would be dominated */ 427  bool skip = false; 428  list dominated; 429  430  for (NODE_TABLE::iterator it = next_table.begin(); it != next_table.end() && ! skip; ++it) 431  { 432  if ( next_demand >= it->first && next_length >= it->second.length - eps ) 433  skip = true; 434  435  if ( next_demand <= it->first && next_length <= it->second.length + eps ) 436  dominated.push_front( it ); 437  } 438  if ( skip ) 439  continue; 440  441  /* remove dominated table and queue entries */ 442  for (list::iterator it = dominated.begin(); it != dominated.end(); ++it) 443  { 444  PQ.remove( (*it)->second.queue_item ); 445  next_table.erase( *it ); 446  } 447  448  /* insert new table and queue entry */ 449  queue_key.demand = next_demand; 450  queue_key.length = next_length; 451  queue_data = next_node; 452  453  queue_item = PQ.insert(queue_key, queue_data); 454  455  table_key = next_demand; 456  table_entry.length = next_length; 457  table_entry.predecessor = curr_node; 458  table_entry.queue_item = queue_item; 459  460  next_table[table_key] = table_entry; 461  462 #ifdef SCIP_OUTPUT 463  printf(\"new entry node = %d demand = %d length = %g pref = %d\\n\", next_node, next_demand, next_length, curr_node); 464 #endif 465  } 466  } 467  468  SCIPdebugMessage(\"Done RSP DP.\\n\"); 469  470  table_entry.predecessor = -1; 471  table_entry.length = 0; 472  int curr_node = 0; 473  474  /* find most negative tour */ 475  for (NODE_TABLE::iterator it = table.begin(); it != table.end(); ++it) 476  { 477  if ( it->second.length < table_entry.length ) 478  { 479  table_key = it->first; 480  table_entry = it->second; 481  } 482  } 483  SCIP_Real tour_length = table_entry.length; 484  485  while ( table_entry.predecessor > 0 ) 486  { 487  table_key -= demand(curr_node); 488  curr_node = table_entry.predecessor; 489  tour.push_front(curr_node); 490  table_entry = table[curr_node][table_key]; 491  } 492  493  SCIPdebugMessage(\"Leave RSP tour length = %g\\n\", tour_length); 494  495  return tour_length; 496 } 497  Generated on Wed Apr 2 2014 for VRP Example (Branch-and-Price) by doxygen (1.8.2) © 2021 by Zuse Institute Berlin (ZIB), Imprint designed with Bootstrap" ]
[ null, "https://scipopt.org/images/newscippy.png", null, "https://www.scipopt.org/doc-3.1.0/examples/VRP/search/mag_sel.png", null ]
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http://www.optimaltjprep.com/tj-prep-problems/2014/2/20/a-geometryalgebra-problem-for-tjsatshsat-prep-medium
[ "# TJ Prep Problems\n\nTJ test prep practice problems  for our students and readers. The problems provide a very small sampling of what Optimal TJ Prep students work with.\n\n# A Geometry/Algebra Problem for TJ/SAT/SHSAT Prep (Medium)\n\nThe figures below (not drawn to scale) show two triangles, ABC and PQT, and their corresponding base and height lengths in terms of X. What is the ratio of the area of the triangle PQT to the area of triangle ABC?" ]
[ null ]
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https://daily-blog.netlify.app/questions/2166605/index.html
[ "# SAS: generate abstractly long and large dataset\n\nAttempting to perform performance testing I cannot evaluate the macro\n\n``````%generate(n_rows,n_cols);\n```\n\n```\n\nwhich will generate a table with n_rows and n_cols filled with random numbers / strings I tried using this link: http://bi-notes.com/2012/08/benchmark-io-performance/\n\nBut I quickly ran into a memory problem\n\nThank!\n\n+3\n\nsource to share\n\nTry it. I added 2 input parameters. So now you have some numbers and some symbols. You can also define the name of the output dataset.\n\n``````%macro generate(n_rows,n_num_cols,n_char_cols,outdata=test,seed=0);\ndata &outdata;\narray nums[&n_num_cols];\narray chars[&n_char_cols] \\$;\ntemp = \"abcdefghijklmnopqrstuvwxyz\";\ndo i=1 to &n_rows;\ndo j=1 to &n_num_cols;\nnums[j] = ranuni(&seed);\nend;\ndo j=1 to &n_char_cols;\nchars[j] = substr(temp,ceil(ranuni(&seed)*18),8);\nend;\noutput;\nend;\ndrop i j temp;\nrun;\n\n%mend;\n\n%generate(10,10,10,outdata=test);\n```\n\n```\n+3\n\nsource\n\nAll Articles" ]
[ null ]
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https://reference.wolfram.com/language/FEMDocumentation/ref/TriangleElement.html
[ "FEMDocumentation`\nFEMDocumentation`\n\n# TriangleElement\n\nTriangleElement[{{i11,i12,i13},,{in1,in2,in3}}]\n\nrepresents n linear triangle elements ek with incidents {ik1,ik2,ik3}.\n\nTriangleElement[{{i11,,i16},,{in1,,in6}}]\n\nrepresents n quadratic triangle elements ek with incidents {ik1,,ik6}.\n\nTriangleElement[{e1,,en},{m1,,mn}]\n\nrepresents n triangle elements ek and n integer markers mk.\n\n# Details\n\n• TriangleElement is used to represent triangle mesh elements in ElementMesh.\n• TriangleElement can be used as an input to ToElementMesh or ToBoundaryMesh.\n• Incidents ik,j are integers that index an array of spatial coordinates. The coordinates referenced by ek={ik1,} are the nodes of the k", null, "triangle.\n• The first three incidents ik1, ik2, and ik3 are always vertices.\n• For quadratic triangle elements, the next three incidents are mid-side nodes of possibly curved edges.\n• Linear elements are order 1 elements and quadratic elements are order 2 elements.\n• In TriangleElement[{e1,,en}], all elements ek need to be of the same order.\n• The triangles in TriangleElement[{e1,,en}] will share common nodes and edges but cannot intersect with each other, or for second order triangles, with themselves.\n• The nodes for a linear and a quadratic triangle are shown:\n•", null, "• The incidents {i1,i2,i3} must be ordered so that going from the coordinates referenced by i1 to i2 to i3 is in the counterclockwise direction.\n• Typically, TriangleElement is used for two-dimensional regions, but may be embedded in three dimensions, for example, as a part of a boundary mesh.\n• The triangle element is known in the finite element method as a Serendipity element.\n\n# Examples\n\nopen allclose all\n\n## Basic Examples(1)\n\nCreate a mesh with one triangle element:\n\n## Scope(1)\n\nA boundary mesh with triangle elements:\n\nVisualize the wireframe:\n\n## Generalizations & Extensions(4)\n\nThe base coordinates of the linear element:\n\nThe base incidents of the linear element:\n\nA mesh with a linear unit element:\n\nVisualization of the linear unit element:\n\nThe base coordinates of the quadratic element:\n\nThe base incidents of the quadratic element:\n\nThe base face incidents of the linear element:\n\nThe base face incidents of the quadratic element:\n\n## Applications(3)\n\nLinear triangle elements in a mesh:\n\nVisualize the mesh with the elements' vertices:\n\nQuadratic triangle elements in a mesh:\n\nVisualize the mesh with the elements' vertices:\n\nA triangle element mesh with markers:\n\nVisualize the mesh with the elements' markers:\n\n## Possible Issues(6)\n\nThe incidents must be of the appropriate length:", null, "The incidents order cannot be mixed:", null, "The incidents must be lists of integers:", null, "The number of markers must match the number of incidents:", null, "Markers must be a vector of integers:", null, "When possible, noninteger markers will be converted to integers:" ]
[ null, "https://reference.wolfram.com/language/FEMDocumentation/ref/Files/TriangleElement.en/1.png", null, "https://reference.wolfram.com/language/FEMDocumentation/ref/Files/TriangleElement.en/Image_2.gif", null, "https://reference.wolfram.com/language/FEMDocumentation/ref/Files/TriangleElement.en/3.gif", null, "https://reference.wolfram.com/language/FEMDocumentation/ref/Files/TriangleElement.en/4.gif", null, "https://reference.wolfram.com/language/FEMDocumentation/ref/Files/TriangleElement.en/5.gif", null, "https://reference.wolfram.com/language/FEMDocumentation/ref/Files/TriangleElement.en/6.gif", null, "https://reference.wolfram.com/language/FEMDocumentation/ref/Files/TriangleElement.en/7.gif", null ]
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http://www.greatestcommonfactor.net/gcf-of-1004/
[ "X\nX\n\n# Calculate the Greatest Common Factor or GCF of 1004\n\nThe instructions to find the GCF of 1004 are the next:\n\n## 1. Decompose all numbers into prime factors\n\n 1004 2 502 2 251 251 1\n\n## 2. Write all numbers as the product of its prime factors\n\n Prime factors of 1004 = 22 . 251\n\n## 3. Choose the common prime factors with the lowest exponent\n\nCommon prime factors: 2 , 251\n\nCommon prime factors with the lowest exponent: 22, 2511\n\n## 4. Calculate the Greatest Common Factor or GCF\n\nRemember, to find the GCF of several numbers you must multiply the common prime factors with the lowest exponent.\n\nGCF = 22. 2511 = 1004\n\nAlso calculates the:" ]
[ null ]
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https://www.physicsforums.com/threads/expanding-functions.83320/
[ "Expanding Functions\n\nAllday\n\nI'm studying for the qualifying exam and I came accross a problem that I'd be able to do in a snap if I had a computer running mathematica in front of me, but regretably Im having trouble with using good old paper and pencil and a reasonable amount of time. I want to look at the low and high temperature behaviour of the function\n\n(deltaE)^2 = C*[sinh(a*B)]^-2\n\nwhere B = 1/T and the rest are constants. I would like to know not just the limit, but the behaviur of the function. ie I could get that in the high T small B limit the function goes like T^2, Im having difficulty with the low T, high B limit. This is connected with the energy fluctiations of a quantum harmonic osccillator if anyone wants a reference point.\n\nAny ideas?\nthanks\n\nRelated Introductory Physics Homework Help News on Phys.org\n\nlurflurf\n\nHomework Helper\nsinh(x)=(exp(x)-exp(-x))/2\nso\nsinh(x) goes like exp(x)/2 for x large\n\nLast edited:\n\nAllday\n\nThats a start. Are you suggesting that I invert that relationship and square it ? I don't know if that will work. The function e^x also can be expanded around the point zero. where its behaviour goes like 1 + x. For the high B regime I think you have to use the definition that B = 1/T and expand around a small number, but I'm not sure how to do that.\n\nlurflurf\n\nHomework Helper\nAllday said:\nThats a start. Are you suggesting that I invert that relationship and square it ? I don't know if that will work. The function e^x also can be expanded around the point zero. where its behaviour goes like 1 + x. For the high B regime I think you have to use the definition that B = 1/T and expand around a small number, but I'm not sure how to do that.\nSo you have\n(deltaE)^2 = C*[sinh(a*B)]^-2\nB large\n(deltaE)^2 = C*[exp(a*B)/2]^-2\n(deltaE)^2 = 4*C*exp(-2*a*B)\nThis goes like 0 (if a is positive).\nIf goes like 0 is not close enough I do not know what you would want as it goes to 0 pretty fast and it is difficult to find other representations.\n\nAllday\n\nIt goes to zero as B becomes large this is true. But does it go to zero like 1/B like 1/B^2 ... thats the thing I'm trying to figure out. Im havent played with it much today, thanks for looking at it. If I can clarify what I mean Ill post it\n\nlurflurf\n\nHomework Helper\nAllday said:\nIt goes to zero as B becomes large this is true. But does it go to zero like 1/B like 1/B^2 ... thats the thing I'm trying to figure out. Im havent played with it much today, thanks for looking at it. If I can clarify what I mean Ill post it\nIt goes to zero exponentially. If you want an expansion in terms of rational functions, none will be useful as it goes to 0 faster than x^y for any negative y. How big is the B you want?\nfor instance\nexp(-20)~2*10^-9\n\nAllday\n\nAhhh, I get it now. I was thinking that even though it goes exponentially that there would be some power that would come out. Now I see thats impossible. The terms in the series just continure to grow so there is no leading term. Thanks for the help.\n\nPhysics Forums Values\n\nWe Value Quality\n• Topics based on mainstream science\n• Proper English grammar and spelling\nWe Value Civility\n• Positive and compassionate attitudes\n• Patience while debating\nWe Value Productivity\n• Disciplined to remain on-topic\n• Recognition of own weaknesses\n• Solo and co-op problem solving" ]
[ null ]
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https://digitalcommons.usu.edu/foundation_wave/4/
[ "## Foundations of Wave Phenomena\n\n#### Title\n\n19 Electromagnetic Energy\n\n#### Description\n\nIn a previous physics course you should have encountered the interesting notion that the electromagnetic field carries energy and momentum. If you have ever been sunburned, you have experimental confirmation of this fact! We are now in a position to explore this idea quantitatively. In physics, the notions of energy and momentum are of interest mainly because they are conserved quantities. We can uncover the energy and momentum quantities associated with the electromagnetic field by searching for conservation laws. As before, such conservation laws will appear embodied in a continuity equation. Thus we begin by investigating a continuity equation for energy and momentum. As was mentioned earlier, there are systematic methods to search for continuity equations associated with a system of differential equations such as the Maxwell equations, but we will not get into that. Instead, we simply write down the continuity equation associated to energy-momentum conservation.\n\n8-2014\n\n#### Keywords\n\nelectromagnetic energy, maxwell equation, energy density, chapter 19\n\n#### Disciplines\n\nPhysical Sciences and Mathematics | Physics\n\nVersion 8.2\n\nChapter 19", null, "COinS" ]
[ null, "https://digitalcommons.usu.edu/foundation_wave/1019/thumbnail.jpg", null ]
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https://mathwords.com/a/area_parallelogram.htm
[ "", null, "index: click on a letter A B C D E F G H I J K L M N O P Q R S T U V W X Y Z A to Z index index: subject areas numbers & symbols sets, logic, proofs geometry algebra trigonometry advanced algebra & pre-calculus calculus advanced topics probability & statistics real world applications multimedia entries", null, "www.mathwords.com about mathwords website feedback\n\n Area of a Parallelogram The formula is given below. Note: This formula works for the area of a rhombus as well, since a rhombus is a special kind of parallelogram.", null, "See also Altitude of a parallelogram, base, sine" ]
[ null, "https://mathwords.com/assets/powered_by_google_135x35.gif", null, "https://mathwords.com/assets/mathwords_logo_small.jpg", null, "https://mathwords.com/a/a_assets/a73.gif", null ]
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https://cse.sc.edu/~mgv/csce582sp09/582Announcement.html
[ "CSCE 582—Bayesian Networks and Decision Graphs [=STAT 582] (3) (Prereq: CSCE 350 and STAT 509) Normative approaches to uncertainty in artificial intelligence. Probabilistic and causal modeling with Bayesian networks and influence diagrams. Applications in decision analysis and support. Algorithms for probability update in graphical models.\n\nCourse Homepage: Spring 2006 (Past Pages: Fall 2003 )\n\nUsually Offered: Once every two years, in the Computer Science Department\n\nPurpose: To appreciate the foundations, power, and limitations of probabilistic and causal modeling with Bayesian networks, solve computer-based decision analysis problems using a Bayesian network and influence diagram tool, and understand and implement structure-based (non-iterative) algorithms for probability update in graphical models.\n\nCurrent Textbook: Bayesian Networks and Decision Graphs, (2nd ed.) Finn V. Jensen and Thomas D. Nielsen, Springer, 2007.\n\n Topics Covered Chapters Time Uncertainty in Artificial Intelligence: symbolic, non-probabilistic, and probabilistic approaches; review of relevant probability theory 1 1 week Causal and Bayesian networks: reasoning under uncertainty, d-separation, factorization of joint probability in graphical models, the chain rule for Bayesian networks, findings and evidence, the variable elimination algorithm for computing posterior marginal probabilities; review of relevant graph theory 2 3 weeks Building models: catching the structure, determining the conditional probabilities; modeling methods, including Kalman filters, hidden Markov models, noisy-Or, divorcing, noisy functional dependencies, interventions 4 3 weeks Learning, adaptation, and tuning parts of 6 and 7 2 weeks Graphical languages for specification of decision problems: decision trees and influence diagrams 9 2 weeks Belief updating in Bayesian networks: triangulated (chordal) graphs, junction trees, Lauritzen-Spiegelhalter, Shenoy-Shafer, and Hugin propagation in junction trees 4 2 weeks" ]
[ null ]
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http://people.sc.fsu.edu/~jburkardt/f_src/asa159/asa159.html
[ "# ASA159 Random generation of a table.\n\nASA159 is a FORTRAN90 library which constructs a table having given row and column sums, by Michael Patefield;\n\nASA159 is Applied Statistics Algorithm 159.\n\nASA159 accepts a table shape (the number of rows and columns), and two vectors, the lists of row and column sums. There may be 0, 1, or many tables with nonnegative, integral entries that have the given shape and sums. The routine will report the case if there are no candidates. If there is at least one candidate, then the routine will choose one, uniformly over the number of distinct candidates.\n\nFor example, suppose M = 2, N = 3, row sum = (/ 6, 5 /) and column sum = (/ 3, 4, 4 /), then here are two tables that satisfy the constraints:\n\n``` 1 2 3\n2 2 1\n```\nand\n``` 3 0 3\n0 4 1\n```\n\n### Languages:\n\nASA159 is available in a C version and a C++ version and a FORTRAN77 version and a FORTRAN90 version and a MATLAB version.\n\n### Related Data and Programs:\n\nASA144, a FORTRAN90 library which randomly generates an RxC contingency table.\n\nASA205, a FORTRAN90 library which generates all the contingency tables corresponding to a given set of row and column sums.\n\nSUBSET, a FORTRAN90 library which includes a routine called I4MAT_01_ROWCOLSUM which generates a (0,1) matrix with given row and column sums.\n\n### Author:\n\nOriginal FORTRAN77 version by Michael Patefield; Matlab version by John Burkardt.\n\n### Reference:\n\n1. Michael Patefield,\nAlgorithm AS 159: An Efficient Method of Generating RXC Tables with Given Row and Column Totals,\nApplied Statistics,\nVolume 30, Number 1, 1981, pages 91-97.\n\n### List of Routines:\n\n• I4VEC_PRINT prints an I4VEC.\n• I4MAT_PRINT prints an I4MAT.\n• I4MAT_PRINT_SOME prints some of an I4MAT.\n• R8_UNIFORM_01 returns a unit pseudorandom R8.\n• RCONT2 constructs a random two-way contingency table with given sums.\n• TIMESTAMP prints the current YMDHMS date as a time stamp.\n\nYou can go up one level to the FORTRAN90 source codes.\n\nLast revised on 10 March 2009." ]
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https://libertyhoffer.com/forum/8oj8xk.php?page=874009-regression-coefficient-excel
[ "regression coefficient excel\n\nDazu müssen mindestens zwei Spalten gefüllt sein. I have selected the LSTAT as the feature to be used. Regression coefficients: The regression coefficients in the last table give us the numbers necessary to write the estimated regression equation: y hat = b 0 + b 1 x 1 + b 2 x 1 2. Subscribe now to receive in-depth stories on AI & Machine Learning. That's not an R problem.\n\n… Step 01: Prepare your data in two adjacent columns. Most or all P-values should be below below 0.05.\n\nFor our data set, where y is the number of umbrellas sold and x is an average monthly rainfall, our linear regression formula goes as follows:. Below you can find our data.\n\nThen, another pop-up is displayed in front of you. Among these packages, you will be able to locate the Analysis ToolPack. Falls das Add-In \"Analyse-Funktionen\" nicht unter \"Aktive Anwendungs-Add-Ins\" aufgelistet wird, klicken Sie unten neben \"Excel-Add-Ins\" auf \"Gehe zu…\".\n\nIn our example this is the case. Regressionsanalyse in Excel erstellen Wechseln Sie zurück in die Tabelle und füllen Sie diese mit Ihren Daten. 1) Select radio button for “Linear”. Now, we need to have a least squared regression line on this graph.\n\nLinear Regression with Excel. Learn more about the analysis toolpak >. That means there is a strong relationship between advertisement expenses (x) and the sales volume (y). Um eine Regressionsanalyse erstellen zu können, müssen Sie zunächst das benötigte Add-In in, Dieser Praxistipp basiert auf Microsoft Office 2010 unter Windows 7.\n\nManual method for simple linear regression analysis. Which provides information, how good our model is fit.\n\nAfter selecting regression you will see that you now have to select the Y and X ranges for the analysis to take place. Here, you will have to select the range of data points in the Y and X axes.\n\nThe regression line is: y = Quantity Sold = 8536.214 -835.722 * Price + 0.592 * Advertising. My goal is to use AI in the field of education to make learning meaningful for everyone. 3) Select the checkbox for “Display R – squared value on chart”. – Roland Nov 11 '14 at 14:49 Learn more about the analysis toolpak > Microsoft Excels functions and tools use the least squares method to calculate regression coefficients. Let us discuss the most important parts of information in the regression analysis output. Excel has three built-in functions that allow for a third method for determining the slope, y-intercept, correlation coefficient, and R-squared values of a set of data. There are times that you only need to find regression coefficients. Excel functions, formula, charts, formatting creating excel dashboard & others. Wie kann man den Zeilenabstand bei Word ändern? This website or its third-party tools use cookies, which are necessary to its functioning and required to achieve the purposes illustrated in the cookie policy. Wouldn’t that make things easy? The dataset chosen for this project is the Boston housing dataset. To do this, first, go to the taskbar and select an option called Data. For example, the first data point equals 8500. Select “Residuals” options from “Residuals” group.\n\nIt is a very powerful add-in in Microsoft Excel. The closer to 1, the better the regression line (read on) fits the data. of Economics, Univ. In other words, for each unit increase in price, Quantity Sold decreases with 835.722 units. Step 1: Input the data. You have to know at least a little bit about the regression formulas to carry out a manual regression analysis. Step 03: Go to → “Insert” Tab → “Charts” group → click “Insert scatter (X,Y ) or Bubble chart” button.Select any of the Scatter Chart type provided in the drop menu. b is intercepting. It enables you to see the equation of least squared regression line on the graph. In other words: can we predict Quantity Sold if we know Price and Advertising? In that case you can simply use Excel worksheet functions or formulas.\nIn this example, Hours studied is a continuous predictor variable that ranges from 0 to 20 hours. This example teaches you how to run a linear regression analysis in Excel and how to interpret the Summary Output. Nachdem Sie auf \"OK\" geklickt haben, wird die Ausgabe dort angezeigt, wo Sie es eingestellt haben. This error term, we don’t need to worry about. This value is considered good if it lies below 0.05 p-value.\n\nStep 03: Calculate the regression coefficients using equations as follows. Equation for slope of the regression line, Equation for intercept of the regression line. Then you should carefully consider whether to include that coefficients in the final regression model or not. These points get selected as a target for training and repeat the same for even the feature column as well.\n\nIf the “significance F” value is lower than the significance level you consider which is 0.05 here, then your regression model is significant. https://andrewpwheeler.com/2016/10/19/testing-the-equality-of-two-regression-coefficients/, Your email address will not be published. Step 02 : Select both columns having X and Y values. Apart from statistical methods like standard deviation, regression, correlation. Regression analysis with Excel formulas or worksheet functions. It will enable you to have a trendline of least square of regression like below. On the Data tab, in the Analysis group, click Data Analysis. This is also called as the coefficient of determination. This is an indication that our results are not random and have a relationship.\n\nObservation: It is pretty easy to test whether a regression coefficient is significantly different from any constant. I have experience in building models in deep learning and reinforcement learning. Wie Sie. 1. Here, select the first package option and select ok. Now you have the package ready to be used. Therefore, we are going to talk about the two methods discussed above only. Sie können auch einen Bereich für die Ausgabe wählen. Regression is used in statistical modeling and it basically tells us the relationship between variables and their movement in the future.\n\nExcel sheets were so far used for storing small to medium-sized datasets either as CSV or in XLS formats and Pandas were used to read them. Note: can't find the Data Analysis button? These were some of the pre-requisites before you actually proceed towards regression analysis in excel. Simple Linear Regression in excel does not need ANOVA and Adjusted R Square to check. All those can be handled by LINEST as well! to test whether the constant for Example 1 is equal to 40, transform the regression equation to the equation (y-40) = b2x + b1z + (b0-40), which takes the form Y = b2x + b1z + B0 and test for B0 = 0. Select the cell range that contains your dependent variable for “input Y range”. Setzen Sie hier den Haken bei \"Analyse-Funktionen\" und bestätigen Sie mit \"OK\". Once you have made this selection just click on okay and almost immediately you will see the result of your analysis on your screen. Equipped with a and b values rounded to three decimal places, it turns into: Y=0.45*x-19.074 Jetzt müssen Sie den Y- und den X-Eingabebereich festlegen. 6. Now, we’ll see how in excel we can fit a regression equation on a scatterplot itself. You should now see that the Excel graphing routine uses linear regression to calculate the slope, y-intercept and correlation coefficient. Step 07 : Click the small black right-arrow head which appears in “Trendline” menu item. R Square equals 0.962, which is a very good fit. Then the “Regression” dialog box appears.\n\nfor the multiple linear equation y = b2x + b1z + b0 to test whether b2 is significantly different from -1, you need to rewrite the regression equation as y+x = (b2+1)x + b1z + b0. From the revised regression analysis, based on the data in range A9:C14, we see that the x coefficient is .069008 with p-value = .85, indicating that coefficient B2 is not significantly different from 0, and so b2 is not significantly different from -1. The next table is the ANOVA which stands for analysis of variance. R-squared value indicates the strength of relationship between independent and dependent variable. Linear relationship means the change in an independent variable(s) causes a change in the dependent variable. Excel will compute Regression analysis for you in a fraction of seconds. With that in mind, Excel offers several different ways to calculate trendlines on a graph, as shown below. of Calif. - Davis; This January 2009 help sheet gives information on; Multiple regression using the Data Analysis Add-in. eine Provision vom Händler, z.B. If it is lesser than 5% (0.05) you can conclude that it provides a better fit. Step 01 : Insert “= RSQ ()” formula within a desired cell.\n\nFinally your table should look like this. Write excel macros using VBA – A simple Guide, View code in excel macro and easily modify as you wish. To test whether b2 is significantly different from b1 in y = b2x + b1z + b0, you need to rewrite the regression equation as y = B2(x+z) + B1(x-z) + b0. Figure 2 – Testing the equivalence of two coefficients.\n\nIt is very close to 1.0. In addition to simple linear regression, Trendline gives you the option to fit your data in to other regression models such as, exponential; logarithmic; polynomial; power and moving average. The packages are available under Analysis ToolPack add-in.\nStep 04 : Click anywhere on the scatter chart. 96% of the variation in Quantity Sold is explained by the independent variables Price and Advertising. In order to build models like linear regression, we need to first locate the packages to do these. The ‘CORREL’ function is an Excel statistical function that calculates the Pearson product-moment correlation coefficient of two sets of variables. There are basically two types of linear relationships as well. Finally, you will see the residual output values below. For each unit increase in Advertising, Quantity Sold increases with 0.592 units. For a continuous predictor variable, the regression coefficient represents the difference in the predicted value of the response variable for each one-unit change in the predictor variable, assuming all other predictor variables are held constant. Go to Next Chapter: Create a Macro, Regression • © 2010-2020 E.g. Click here to load the Analysis ToolPak add-in. Step 01 : Insert “= SLOPE ()” formula within a desired cell.Step 02 : For the first parameter, select the Excel cell range that you have entered the Y-values which is the dependent variable. You have the option to select with or without column headers.\n\nPrepare your independent (X) and dependent (Y) variable values as in previous cases.\n\nPrepare your independent (X) and dependent (Y) variable values as in previous cases. If you find any issues doing regression analysis in those versions, please leave a comment below. (0.000, 0.001 and 0.005).\n\nExcel produces the following Summary Output (rounded to 3 decimal places). One important part of this entire output is R Square/ Adjusted R Square under SUMMARY OUTPUT table.\n\n." ]
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https://tdpelmedia.com/waec-physics-obj-objective-essay-2021-questions-answers?shared=email&msg=fail
[ "# WAEC Physics obj Objective Essay 2021 Questions, Answers\n\nWAEC Physics obj Objective Essay 2021 Questions, Answers\n\n1-10: DACAACBBCC\n\n11-20: BDBABBACAC\n\n21-30: BCBACBBACA\n\n31-40: BDDDDACCCA\n\n41-50: AAAABBCBBC\n\n(1)\nOriginal length Lo= 3m\nExtension e = 310 = 3*3= 9m\n\nF×e\nF=ke where k = 982.3NM-²\nF=982.3*9=8,840.7N\n\nThe five that produce the extension F = 8.840.7N\n\n(2a)\nFlat metal plate are mainly used to collect heat for space heating in solar panels for heat transfer.\n\n(2b)\nThermal insulator is used for reduction of heat transfer between objects in thermal contact\n\n(2c)\ntubes is a device that controls electric current flow in a high vacuum between electrodes to which an electric potential difference has been applied.\n\n(3a)\nhighly purified silica glass.\n\n(3b)\nTo confine the optical signal in the core the refractive index of the core must be greater than that of the cladding.\n\n(5)\nEscape velocity = VE\nRadius of the earth = R\n\nAcceleration due to gravity = 10ms²\nEscape velocity Be=√2R\n\nVE=√2*10R\nVE=√20R\n\n(6)\nAngle at horizontal θ = 30°\nTime of light , T = 25sec\n\nVelocity of projection u = ?\nBut T=2using sinθ/g\n\n25= 2u*sin30/10\n25=0.5u/5\n\n0.5u=125\nU=125/0.5\n\n=250ms-¹\n\n(7)\n(i)Coherence\n\n(ii)Directionality\n(iii)Monochromatic\n\n(8ai)\nA torque is defined as a measure of the force that can cause an object to rotate about an axis\n\nWAEC Physics Questions 2021 and Answers\n(8aii)\n\nFactors that determine torque are;\n– The magnitude of the force\n\n– The angle between the force and the lever arm\n\n(8bi)\nFree fall simply means the act of which are objects fall freely under the influence of gravitational force. An object under free fall does not encounter air resistance\n\n(8bii)\nHeight of tower H = 40.0m\nVelocity v = 10.0m/s, time t= ? , g=10.0m/s\n\nUsing the relation\nS= ut + 1/2gt^2\n\nH= ut + 1/2gt^2\n40= 10t + 1/2*10t^2\n4= t + t^2/2\n\n= t^2 + 2t – 8=0 ( solving quadratically)\n= (t+4)(t-2)=0\n\nt+4=0 or t-2=0\nt= -4 or t=2\n\nTherefore time to fall on the ground t=2s\n\n(8c)\nR.d of oil =R1 = 0.72\n\nR.d of water = R2=1.00\n\nR.d of liquid= R1/R2= 0.72/1 = 0.72\n\nR.d = density of wood(P1)/density of water(P2)\n0.72=P1/1.00\n\nP1= 0.72*1.00=0.72g/cm³\nBut density of wood= mass of wood/volume of wood\n\n0.72= mass of wood/8*8*8\nMass of wood = 0.72*512 = 368.64g" ]
[ null ]
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https://docs.eazybi.com/eazybi/analyze-and-visualize/calculated-measures-and-members/mdx-function-reference/cache
[ "# Cache\n\nCaches the result of the calculation in memory for query in execution. It can be useful when the same calculation is repeated in the report more than once.\n\n## Syntax\n\n` Cache(Expression)`\n\n## Examples\n\nA report has a measure that for calculation uses the result of a previously calculated measure. Using cache would store the first time calculation result in memory and for the next measure would be used to optimize the performance of the report.\n\nOpen issues are calculated much faster using the cache function as the query should go through all time members and repeat the mathematical expression to each of them.\n\n```Cache(\nNonZero(Sum(PreviousPeriods([Time].CurrentHierarchyMember),\nCache([Measures].[Issues created]\n- [Measures].[Issues resolved])\n))\n+ [Measures].[Issues created]\n- [Measures].[Issues resolved]\n)```" ]
[ null ]
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https://rdrr.io/cran/GeomComb/man/comb_EIG1.html
[ "# comb_EIG1: Standard Eigenvector Forecast Combination In GeomComb: (Geometric) Forecast Combination Methods\n\n## Description\n\nComputes forecast combination weights according to the standard eigenvector approach by Hsiao and Wan (2014) and produces forecasts for the test set, if provided.\n\n## Usage\n\n 1 comb_EIG1(x) \n\n## Arguments\n\n x An object of class foreccomb. Contains training set (actual values + matrix of model forecasts) and optionally a test set.\n\n## Details\n\nThe standard eigenvector approach retrieves combination weights from the sample estimated mean squared prediction error matrix as follows: Suppose y_t is the variable of interest, there are N not perfectly collinear predictors, f_t = (f_{1t}, …, f_{Nt})', Σ is the (positive definite) mean squared prediction error matrix of f_t and e is an N * 1 vector of (1, …, 1)'. The N positive eigenvalues are then arranged in increasing order (Φ_1 = Φ_{min}, Φ_2, …, Φ_N), and w^j is defined as the eigenvector corresponding to Φ_j. The combination weights w = (w_1, …, w_N)' are then chosen corresponding to the minimum of (Φ_1/d_1^2, Φ_2/d_2^2, …, Φ_N/d_N^2), denoted as w^l, where d_j = e'w^j, as:\n\nw = 1/d_l w^l\n\nThe combined forecast is then obtained by:\n\n\\hat{y}_t = (f_t)'w\n\nThe difference to extant methods that minimize the population mean squared prediction error (e.g., Newbold and Granger, 1974) is the normalization function. While previous approaches optimize MSPE under the constraint of e'w = 1, Hsiao and Wan (2014) show that this is dominated by using w'w = 1 as constraint in the optimization problem.\n\n## Value\n\nReturns an object of class foreccomb_res with the following components:\n\n Method Returns the used forecast combination method. Models Returns the individual input models that were used for the forecast combinations. Weights Returns the combination weights obtained by applying the combination method to the training set. Fitted Returns the fitted values of the combination method for the training set. Accuracy_Train Returns range of summary measures of the forecast accuracy for the training set. Forecasts_Test Returns forecasts produced by the combination method for the test set. Only returned if input included a forecast matrix for the test set. Accuracy_Test Returns range of summary measures of the forecast accuracy for the test set. Only returned if input included a forecast matrix and a vector of actual values for the test set. Input_Data Returns the data forwarded to the method.\n\n## Author(s)\n\nChristoph E. Weiss and Gernot R. Roetzer\n\n## References\n\nHsiao, C., and Wan, S. K. (2014). Is There An Optimal Forecast Combination? Journal of Econometrics, 178(2), 294–309.\n\nNewbold, P., and Granger, C. W. J. (1974). Experience with Forecasting Univariate Time Series and the Combination of Forecasts. Journal of the Royal Statistical Society, Series A, 137(2), 131–165.\n\nforeccomb, plot.foreccomb_res, summary.foreccomb_res, comb_NG, accuracy\n 1 2 3 4 5 6 7 8 9 obs <- rnorm(100) preds <- matrix(rnorm(1000, 1), 100, 10) train_o<-obs[1:80] train_p<-preds[1:80,] test_o<-obs[81:100] test_p<-preds[81:100,] data<-foreccomb(train_o, train_p, test_o, test_p) comb_EIG1(data)" ]
[ null ]
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https://kr.mathworks.com/matlabcentral/cody/problems/74-balanced-number/solutions/1407301
[ "Cody\n\n# Problem 74. Balanced number\n\nSolution 1407301\n\nSubmitted on 6 Jan 2018 by Miklós Csécsi\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\nn = 13722; assert(isequal(isBalanced(n),true))\n\n[Warning: Integer operands are required for colon operator when used as index] [Warning: Integer operands are required for colon operator when used as index]\n\n2   Pass\nn = 23567414; assert(isequal(isBalanced(n),true))\n\n3   Pass\nn = 20567410; assert(isequal(isBalanced(n),false))\n\n4   Pass\nn = 1; assert(isequal(isBalanced(n),true))\n\n[Warning: Integer operands are required for colon operator when used as index] [Warning: Integer operands are required for colon operator when used as index]\n\n5   Pass\nn = 11111111; assert(isequal(isBalanced(n),true))\n\n6   Pass\nn = 12345678; assert(isequal(isBalanced(n),false))\n\n7   Pass\nn = 12333; assert(isequal(isBalanced(n),false))\n\n[Warning: Integer operands are required for colon operator when used as index] [Warning: Integer operands are required for colon operator when used as index]\n\n8   Pass\nn = 9898; assert(isequal(isBalanced(n),true))\n\n9   Pass\nn = 469200; assert(isequal(isBalanced(n),false))\n\n10   Pass\nn = 57666; assert(isequal(isBalanced(n),true))\n\n[Warning: Integer operands are required for colon operator when used as index] [Warning: Integer operands are required for colon operator when used as index]" ]
[ null ]
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http://www.kkbloves.com/uncategorized/atarax-generic-online-buy-atarax-france/
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[ null, "https://images.unlimrx.com/promo/en/atarax.jpg", null ]
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https://number.academy/36963
[ "# Number 36963\n\nNumber 36,963 spell 🔊, write in words: thirty-six thousand, nine hundred and sixty-three . Ordinal number 36963th is said 🔊 and write: thirty-six thousand, nine hundred and sixty-third. The meaning of number 36963 in Maths: Is Prime? Factorization and prime factors tree. The square root and cube root of 36963. What is 36963 in computer science, numerology, codes and images, writing and naming in other languages. Other interesting facts related to 36963.\n\n## What is 36,963 in other units\n\nThe decimal (Arabic) number 36963 converted to a Roman number is (X)(X)(X)(V)MCMLXIII. Roman and decimal number conversions.\n\n#### Weight conversion\n\n36963 kilograms (kg) = 81488.6 pounds (lbs)\n36963 pounds (lbs) = 16766.3 kilograms (kg)\n\n#### Length conversion\n\n36963 kilometers (km) equals to 22968 miles (mi).\n36963 miles (mi) equals to 59487 kilometers (km).\n36963 meters (m) equals to 121269 feet (ft).\n36963 feet (ft) equals 11267 meters (m).\n36963 centimeters (cm) equals to 14552.4 inches (in).\n36963 inches (in) equals to 93886.0 centimeters (cm).\n\n#### Temperature conversion\n\n36963° Fahrenheit (°F) equals to 20517.2° Celsius (°C)\n36963° Celsius (°C) equals to 66565.4° Fahrenheit (°F)\n\n#### Time conversion\n\n(hours, minutes, seconds, days, weeks)\n36963 seconds equals to 10 hours, 16 minutes, 3 seconds\n36963 minutes equals to 3 weeks, 4 days, 16 hours, 3 minutes\n\n### Zip codes 36963\n\n• Zip code 36963 Colonia Linda Vista, Guanajuato, Cuerámaro, Mexico a map\n• Zip code 36963 Colonia San Miguel, Guanajuato, Cuerámaro, Mexico a map\n• Zip code 36963 Colonia del Carmen, Guanajuato, Cuerámaro, Mexico a map\nZip code areas 36963\n\n### Codes and images of the number 36963\n\nNumber 36963 morse code: ...-- -.... ----. -.... ...--\nSign language for number 36963:", null, "", null, "", null, "", null, "", null, "Number 36963 in braille:", null, "Images of the number\nImage (1) of the numberImage (2) of the number", null, "", null, "More images, other sizes, codes and colors ...\n\n#### Number 36963 infographic", null, "## Share in social networks", null, "## Mathematics of no. 36963\n\n### Multiplications\n\n#### Multiplication table of 36963\n\n36963 multiplied by two equals 73926 (36963 x 2 = 73926).\n36963 multiplied by three equals 110889 (36963 x 3 = 110889).\n36963 multiplied by four equals 147852 (36963 x 4 = 147852).\n36963 multiplied by five equals 184815 (36963 x 5 = 184815).\n36963 multiplied by six equals 221778 (36963 x 6 = 221778).\n36963 multiplied by seven equals 258741 (36963 x 7 = 258741).\n36963 multiplied by eight equals 295704 (36963 x 8 = 295704).\n36963 multiplied by nine equals 332667 (36963 x 9 = 332667).\nshow multiplications by 6, 7, 8, 9 ...\n\n### Fractions: decimal fraction and common fraction\n\n#### Fraction table of 36963\n\nHalf of 36963 is 18481,5 (36963 / 2 = 18481,5 = 18481 1/2).\nOne third of 36963 is 12321 (36963 / 3 = 12321).\nOne quarter of 36963 is 9240,75 (36963 / 4 = 9240,75 = 9240 3/4).\nOne fifth of 36963 is 7392,6 (36963 / 5 = 7392,6 = 7392 3/5).\nOne sixth of 36963 is 6160,5 (36963 / 6 = 6160,5 = 6160 1/2).\nOne seventh of 36963 is 5280,4286 (36963 / 7 = 5280,4286 = 5280 3/7).\nOne eighth of 36963 is 4620,375 (36963 / 8 = 4620,375 = 4620 3/8).\nOne ninth of 36963 is 4107 (36963 / 9 = 4107).\nshow fractions by 6, 7, 8, 9 ...\n\n### Calculator\n\n 36963\n\n#### Is Prime?\n\nThe number 36963 is not a prime number. The closest prime numbers are 36947, 36973.\n\n#### Factorization and factors (dividers)\n\nThe prime factors of 36963 are 3 * 3 * 3 * 37 * 37\nThe factors of 36963 are 1 , 3 , 9 , 27 , 37 , 111 , 333 , 999 , 1369 , 4107 , 12321 , 36963\nTotal factors 12.\nSum of factors 56280 (19317).\n\n#### Powers\n\nThe second power of 369632 is 1.366.263.369.\nThe third power of 369633 is 50.501.192.908.347.\n\n#### Roots\n\nThe square root √36963 is 192,25764.\nThe cube root of 336963 is 33,311107.\n\n#### Logarithms\n\nThe natural logarithm of No. ln 36963 = loge 36963 = 10,517673.\nThe logarithm to base 10 of No. log10 36963 = 4,567767.\nThe Napierian logarithm of No. log1/e 36963 = -10,517673.\n\n### Trigonometric functions\n\nThe cosine of 36963 is 0,557718.\nThe sine of 36963 is -0,83003.\nThe tangent of 36963 is -1,488261.\n\n### Properties of the number 36963\n\nIs a Friedman number: No\nIs a Fibonacci number: No\nIs a Bell number: No\nIs a palindromic number: Yes\nIs a pentagonal number: No\nIs a perfect number: No\n\n## Number 36963 in Computer Science\n\nCode typeCode value\n36963 Number of bytes36.1KB\nUnix timeUnix time 36963 is equal to Thursday Jan. 1, 1970, 10:16:03 a.m. GMT\nIPv4, IPv6Number 36963 internet address in dotted format v4 0.0.144.99, v6 ::9063\n36963 Decimal = 1001000001100011 Binary\n36963 Decimal = 1212201000 Ternary\n36963 Decimal = 110143 Octal\n36963 Decimal = 9063 Hexadecimal (0x9063 hex)\n36963 BASE64MzY5NjM=\n36963 MD5ac957f861e66e00b823bd6d0ffcb603c\n36963 SHA1cab06a4333a41a50778fd4f37f0d12d0517fdd80\n36963 SHA224e4fc4043f68c24f67a7c63f32b2b6cd4fff8c44a36f5cde66be6f2cf\n36963 SHA256247a42542215a3616769d371d691a0434cea23d3e1a849685bc3f7df7856abe1\n36963 SHA3846b76b3a2255750725f3a819d09c9b2895c6632f5baec1d2fca6e26ba749d84696b9a9356daba4d8a6f1139ac228c096e\nMore SHA codes related to the number 36963 ...\n\nIf you know something interesting about the 36963 number that you did not find on this page, do not hesitate to write us here.\n\n## Numerology 36963\n\n### Character frequency in number 36963\n\nCharacter (importance) frequency for numerology.\n Character: Frequency: 3 2 6 2 9 1\n\n### Classical numerology\n\nAccording to classical numerology, to know what each number means, you have to reduce it to a single figure, with the number 36963, the numbers 3+6+9+6+3 = 2+7 = 9 are added and the meaning of the number 9 is sought.\n\n## Interesting facts about the number 36963\n\n### Asteroids\n\n• (36963) 2000 SF285 is asteroid number 36963. It was discovered by LINEAR, Lincoln Near-Earth Asteroid Research from Lincoln Laboratory, Socorro on 9/23/2000.\n\n## Number 36,963 in other languages\n\nHow to say or write the number thirty-six thousand, nine hundred and sixty-three in Spanish, German, French and other languages. The character used as the thousands separator.\n Spanish: 🔊 (número 36.963) treinta y seis mil novecientos sesenta y tres German: 🔊 (Anzahl 36.963) sechsunddreißigtausendneunhundertdreiundsechzig French: 🔊 (nombre 36 963) trente-six mille neuf cent soixante-trois Portuguese: 🔊 (número 36 963) trinta e seis mil, novecentos e sessenta e três Chinese: 🔊 (数 36 963) 三万六千九百六十三 Arabian: 🔊 (عدد 36,963) ستة و ثلاثون ألفاً و تسعمائةثلاثة و ستون Czech: 🔊 (číslo 36 963) třicet šest tisíc devětset šedesát tři Korean: 🔊 (번호 36,963) 삼만 육천구백육십삼 Danish: 🔊 (nummer 36 963) seksogtredivetusinde og nihundrede og treogtreds Dutch: 🔊 (nummer 36 963) zesendertigduizendnegenhonderddrieënzestig Japanese: 🔊 (数 36,963) 三万六千九百六十三 Indonesian: 🔊 (jumlah 36.963) tiga puluh enam ribu sembilan ratus enam puluh tiga Italian: 🔊 (numero 36 963) trentaseimilanovecentosessantatré Norwegian: 🔊 (nummer 36 963) tretti-seks tusen, ni hundre og seksti-tre Polish: 🔊 (liczba 36 963) trzydzieści sześć tysięcy dziewięćset sześćdziesiąt trzy Russian: 🔊 (номер 36 963) тридцать шесть тысяч девятьсот шестьдесят три Turkish: 🔊 (numara 36,963) otuzaltıbindokuzyüzaltmışüç Thai: 🔊 (จำนวน 36 963) สามหมื่นหกพันเก้าร้อยหกสิบสาม Ukrainian: 🔊 (номер 36 963) тридцять шiсть тисяч дев'ятсот шiстдесят три Vietnamese: 🔊 (con số 36.963) ba mươi sáu nghìn chín trăm sáu mươi ba Other languages ...\n\n## News to email\n\nPrivacy Policy.\n\n## Comment\n\nIf you know something interesting about the number 36963 or any natural number (positive integer) please write us here or on facebook." ]
[ null, "https://numero.wiki/s/senas/lenguaje-de-senas-numero-3.png", null, "https://numero.wiki/s/senas/lenguaje-de-senas-numero-6.png", null, "https://numero.wiki/s/senas/lenguaje-de-senas-numero-9.png", null, "https://numero.wiki/s/senas/lenguaje-de-senas-numero-6.png", null, "https://numero.wiki/s/senas/lenguaje-de-senas-numero-3.png", null, "https://number.academy/img/braille-36963.svg", null, "https://numero.wiki/img/a-36963.jpg", null, "https://numero.wiki/img/b-36963.jpg", null, "https://number.academy/i/infographics/3/number-36963-infographic.png", null, "https://numero.wiki/s/share-desktop.png", null ]
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https://mathchat.me/tag/elementary-math/
[ "## Kiss those Math Headaches GOODBYE!", null, "### Recent insight on the GCF (and GPGCF)\n\nA while back I wrote a post about the GCF, and mentioned that there’s a number  related to it — a number that I call the GPGCF. “GPGCF” stands for the “Greatest Possible Greatest Common Factor.”\n\nIn short, the GPGCF is a number that sets an upper limit for the size of the GCF. I’ve seen many students struggle when searching for the GCF, seeking hither and yon for it. I had a sense that students were checking numbers that were too large. That’s what led me to try to figure out what must the the upper limit for the GCF.\n\nIf you check out that post (10/25/10), you’ll see that, for any two numbers, I said that the difference between those numbers has to be the GPGCF.\n\nAnd I was correct, to a degree.\n\nBut I recently realized that my little theory needs modifying.\n\nFor while the difference between any two numbers can be the upper limit for the GCF, that difference is not the only quantity that can set an upper limit for the GCF. There’s another quantity that plays a role.\n\nThat other quantity, I recently realized, is the size of the smaller of the two numbers.\n\nTake the numbers 8 and 24, for example.\n\nThe difference between these two numbers is 16, so I would have said that 16 is the upper limit for the GCF. But there’s actually another quantity that limits the size of the GCF, and that quantity is 8. For since the GCF of 8 and 24 must by definition fit into both 8 and 24, it must fit into 8. And common sense tells us that there’s no number larger than 8 that can fit into 8! So the size of this number — the smaller of the two numbers — also sets an upper limit for the size of the GCF.\n\nSo my revised theory about the GPGCF is this:  when you need to find the GCF for any two numbers, look at two quantities:  1) the smaller of the two numbers, and 2) the difference between the two numbers. Both of these quantities constrains the size of the GPGCF. So therefore, whichever of these is smaller IS the GPGCF. Once you’ve found the GPGCF, that makes it easier to find the actual GCF.\n\nI know this sounds very abstract, so let’s look at a few examples to see what I’m blabbering on about.\n\nExample 1:  What’s the GPGCF for 6 and 16?\n\nSmaller number is 6; difference is 10.\n6 and 10 both limit the size of the GCF, but\n6 is less than 10, so 6 is the GPGCF.\n\nExample 2:  What’s the GPGCF for 8 and 12?\n\nSmaller number is 8; difference is 4.\n4 is less than 8, so 4 is the GPGCF.\n\nExample 3:  What’s the GPGCF for 30 and 75?\n\nSmaller number is 30; difference is 45.\n30 is less than 45, so 30 is the GPGCF.\n\nExample 4:  What’s the GPGCF for 28 and 42?\n\nSmaller number is 28; difference is 14.\n14 is less than 28, so 14 is the GPGCF.\n\nNow, let’s go one step further. From here, how do we figure out the GCF? I’ve done a bit more thinking about this, too, and I’ll share those ideas in my next post.\n\n### Place Value Metaphor\n\nDuring the summer I get to tutor a lot of elementary age students, remediating them on the basics.\n\nAlmost invariably I find that these students are confused about PLACE VALUE, and considering how critical this concept is to all of math, I decided to write this post.\n\nWhenever I have the least suspicion that a student might be confused about place value, I check with a simple test.\n\nI have them write down the number 22, then I ask them if they can tell me the difference between the two 2s. Often they cannot.\n\nTutoring a girl this past week I came up with a way of understanding place value that really resonated with the student. I want to share it because you may be able to use it, or a modification of it, with your students. First it’s important to know that this student’s mom teaches ballet, and the girl dances at her mom’s studio.\n\nI asked the girl if she has ever been to a ballet performance, and of course she said yes.\n\nThen I drew a quick diagram of the stage and first few audience rows. I pointed to two seats, one in the front row, another seat several rows back. I asked her if the two seats would cost the same amount. This girl knew that the close seat costs more money because it is closer to the action on stage.\n\nThen I used that idea to explain place value. I showed this girl that just as seats can be more or less valuable because of where they are, so too digits can be more or less value based on where they are in a number.\n\nShe got this idea very quickly, and now she understands place value.\n\nFor children with different interests, use whatever makes sense. For example if you’re teaching a boy who loves baseball, make the rows of seats those at a baseball game, and so on." ]
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https://essaylux.com/homework/495429/
[ "A student taking Accounting and Finance scores 85 in both of her mid-term exams. The average and standard deviation in the Accounting exam are 70 and 12 points. The average and standard deviation in the Finance exam are 76 and 6 points.\na. Calculate z-score for the student score in the Accounting cl...\n\nSTATUS" ]
[ null ]
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https://answers.everydaycalculation.com/subtract-fractions/5-2-minus-5-4
[ "Solutions by everydaycalculation.com\n\n## Subtract 5/4 from 5/2\n\n1st number: 2 1/2, 2nd number: 1 1/4\n\n5/2 - 5/4 is 5/4.\n\n#### Steps for subtracting fractions\n\n1. Find the least common denominator or LCM of the two denominators:\nLCM of 2 and 4 is 4\n\nNext, find the equivalent fraction of both fractional numbers with denominator 4\n2. For the 1st fraction, since 2 × 2 = 4,\n5/2 = 5 × 2/2 × 2 = 10/4\n3. Likewise, for the 2nd fraction, since 4 × 1 = 4,\n5/4 = 5 × 1/4 × 1 = 5/4\n4. Subtract the two like fractions:\n10/4 - 5/4 = 10 - 5/4 = 5/4\n5. In mixed form: 11/4\n\nMathStep (Works offline)", null, "Download our mobile app and learn to work with fractions in your own time:" ]
[ null, "https://answers.everydaycalculation.com/mathstep-app-icon.png", null ]
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https://www.bartleby.com/solution-answer/chapter-4ct-problem-16ct-elementary-geometry-for-college-students-7e-7th-edition/9781337614085/complete-the-proof-of-the-following-theorem-the-diagonals-of-an-isosceles-trapezoid-are-congruent/0d75a45b-757c-11e9-8385-02ee952b546e
[ "", null, "", null, "", null, "Chapter 4.CT, Problem 16CT", null, "Elementary Geometry For College St...\n\n7th Edition\nAlexander + 2 others\nISBN: 9781337614085\n\nSolutions\n\nChapter\nSection", null, "Elementary Geometry For College St...\n\n7th Edition\nAlexander + 2 others\nISBN: 9781337614085\nTextbook Problem\n\nComplete the proof of the following theorem:“The diagonals of an isosceles trapezoid are congruent.”Given: Trapezoid ABCD; A B ¯ ∥ D C ¯ and A D ¯ ≅ B C ¯ .Prove: A C ¯ ≅ B D ¯", null, "PROOF Statements Reasons 1_________2. ∠ A D C ≅ ∠ B C D 3. D C ¯ ≅ D C ¯   4. Δ A D C ≅ Δ B C D 5.__________ 1.______________2. Base ∠ s of an isosceles trapezoid are _______.3._________4.____________5. CPCTC\n\nTo determine\n\nTo Find:\n\nThe proof of AC¯BD¯.\n\nExplanation\n\nGiven:\n\nTrapezoid ABCD with AB¯DC¯ and AD¯BC¯.\n\nApproach:\n\nConsider the theorem,\n\n“The diagonals of an isosceles trapezoid are congruent.”\n\n PROOF Statements Reasons 1. Trapezoid ABCD withAB¯∥DC¯ and AD¯≅BC¯2. ∠ADC≅∠BCD3. DC¯≅DC¯4. ΔADC≅ΔBCD5. AC¯≅DB¯ 1\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 33-38, rewrite the expression using positive exponents only. 37. 120(s + t)3\n\nApplied Calculus for the Managerial, Life, and Social Sciences: A Brief Approach\n\nEvaluate the limit. limxe2xe2xln(x+1)\n\nSingle Variable Calculus: Early Transcendentals, Volume I\n\nSubtract and check: 98,40572,397\n\nElementary Technical Mathematics\n\nSolve sin2xsinx=0 if 0x2.\n\nTrigonometry (MindTap Course List)\n\nFor y = x3 ln x, y = a) x2(1 + 3 ln x) b) x3 + 3x2 (ln x) c) 3x d) 4x2(ln x)\n\nStudy Guide for Stewart's Single Variable Calculus: Early Transcendentals, 8th\n\nTrue or False: The graph of x = 5 is a cylinder.\n\nStudy Guide for Stewart's Multivariable Calculus, 8th", null, "" ]
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https://metanumbers.com/11319
[ "## 11319\n\n11,319 (eleven thousand three hundred nineteen) is an odd five-digits composite number following 11318 and preceding 11320. In scientific notation, it is written as 1.1319 × 104. The sum of its digits is 15. It has a total of 5 prime factors and 16 positive divisors. There are 5,880 positive integers (up to 11319) that are relatively prime to 11319.\n\n## Basic properties\n\n• Is Prime? No\n• Number parity Odd\n• Number length 5\n• Sum of Digits 15\n• Digital Root 6\n\n## Name\n\nShort name 11 thousand 319 eleven thousand three hundred nineteen\n\n## Notation\n\nScientific notation 1.1319 × 104 11.319 × 103\n\n## Prime Factorization of 11319\n\nPrime Factorization 3 × 73 × 11\n\nComposite number\nDistinct Factors Total Factors Radical ω(n) 3 Total number of distinct prime factors Ω(n) 5 Total number of prime factors rad(n) 231 Product of the distinct prime numbers λ(n) -1 Returns the parity of Ω(n), such that λ(n) = (-1)Ω(n) μ(n) 0 Returns: 1, if n has an even number of prime factors (and is square free) −1, if n has an odd number of prime factors (and is square free) 0, if n has a squared prime factor Λ(n) 0 Returns log(p) if n is a power pk of any prime p (for any k >= 1), else returns 0\n\nThe prime factorization of 11,319 is 3 × 73 × 11. Since it has a total of 5 prime factors, 11,319 is a composite number.\n\n## Divisors of 11319\n\n1, 3, 7, 11, 21, 33, 49, 77, 147, 231, 343, 539, 1029, 1617, 3773, 11319\n\n16 divisors\n\n Even divisors 0 16 8 8\nTotal Divisors Sum of Divisors Aliquot Sum τ(n) 16 Total number of the positive divisors of n σ(n) 19200 Sum of all the positive divisors of n s(n) 7881 Sum of the proper positive divisors of n A(n) 1200 Returns the sum of divisors (σ(n)) divided by the total number of divisors (τ(n)) G(n) 106.391 Returns the nth root of the product of n divisors H(n) 9.4325 Returns the total number of divisors (τ(n)) divided by the sum of the reciprocal of each divisors\n\nThe number 11,319 can be divided by 16 positive divisors (out of which 0 are even, and 16 are odd). The sum of these divisors (counting 11,319) is 19,200, the average is 1,200.\n\n## Other Arithmetic Functions (n = 11319)\n\n1 φ(n) n\nEuler Totient Carmichael Lambda Prime Pi φ(n) 5880 Total number of positive integers not greater than n that are coprime to n λ(n) 1470 Smallest positive number such that aλ(n) ≡ 1 (mod n) for all a coprime to n π(n) ≈ 1371 Total number of primes less than or equal to n r2(n) 0 The number of ways n can be represented as the sum of 2 squares\n\nThere are 5,880 positive integers (less than 11,319) that are coprime with 11,319. And there are approximately 1,371 prime numbers less than or equal to 11,319.\n\n## Divisibility of 11319\n\n m n mod m 2 3 4 5 6 7 8 9 1 0 3 4 3 0 7 6\n\nThe number 11,319 is divisible by 3 and 7.\n\n## Classification of 11319\n\n• Arithmetic\n• Deficient\n\n### Expressible via specific sums\n\n• Polite\n• Non-hypotenuse\n\n• Frugal\n\n## Base conversion (11319)\n\nBase System Value\n2 Binary 10110000110111\n3 Ternary 120112020\n4 Quaternary 2300313\n5 Quinary 330234\n6 Senary 124223\n8 Octal 26067\n10 Decimal 11319\n12 Duodecimal 6673\n20 Vigesimal 185j\n36 Base36 8qf\n\n## Basic calculations (n = 11319)\n\n### Multiplication\n\nn×i\n n×2 22638 33957 45276 56595\n\n### Division\n\nni\n n⁄2 5659.5 3773 2829.75 2263.8\n\n### Exponentiation\n\nni\n n2 128119761 1450187574759 16414673158697121 185797685483292712599\n\n### Nth Root\n\ni√n\n 2√n 106.391 22.4527 10.3146 6.46787\n\n## 11319 as geometric shapes\n\n### Circle\n\n Diameter 22638 71119.4 4.025e+08\n\n### Sphere\n\n Volume 6.07453e+12 1.61e+09 71119.4\n\n### Square\n\nLength = n\n Perimeter 45276 1.2812e+08 16007.5\n\n### Cube\n\nLength = n\n Surface area 7.68719e+08 1.45019e+12 19605.1\n\n### Equilateral Triangle\n\nLength = n\n Perimeter 33957 5.54775e+07 9802.54\n\n### Triangular Pyramid\n\nLength = n\n Surface area 2.2191e+08 1.70906e+11 9241.92\n\n## Cryptographic Hash Functions\n\nmd5 d9aa7942219d9b762ba1b832214e5a7a 4172bc30cd4c11bd58145e2ca4687dab8319bdf7 af3360f632b927e8c60eaa1ea0009f339d35cc6e19c1bed9e3ff472e1862827b 03253a54bfd6bd16e4a4c002f0b6b9bf1607c892fae043682e8c59bee489212b101acbda083036850b430e2cce0e501096a06f30642e6f8b4a86df6ad715d9f2 d5912ec0bbd92658a7929636d02e93794e47b2d2" ]
[ null ]
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https://answers.everydaycalculation.com/simplify-fraction/490-420
[ "Solutions by everydaycalculation.com\n\n## Reduce 490/420 to lowest terms\n\nThe simplest form of 490/420 is 7/6.\n\n#### Steps to simplifying fractions\n\n1. Find the GCD (or HCF) of numerator and denominator\nGCD of 490 and 420 is 70\n2. Divide both the numerator and denominator by the GCD\n490 ÷ 70/420 ÷ 70\n3. Reduced fraction: 7/6\nTherefore, 490/420 simplified to lowest terms is 7/6.\n\nMathStep (Works offline)", null, "Download our mobile app and learn to work with fractions in your own time:\nAndroid and iPhone/ iPad\n\nEquivalent fractions:\n\nMore fractions:" ]
[ null, "https://answers.everydaycalculation.com/mathstep-app-icon.png", null ]
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https://jeeneetqna.in/1326/hydrogen-electron-makes-transition-level-level-frequency
[ "# In a hydrogen atom the electron makes a transition from (n + 1)th level to the nth level. If n >> 1, the frequency\n\nmore_vert\n\nIn a hydrogen atom the electron makes a transition from (n + 1)th level to the nth level. If n >> 1, the frequency of radiation emitted is proportional to :\n\n(1) $1\\over n^4$\n\n(2) $1\\over n$\n\n(3) $1\\over n^3$\n\n(4) $1\\over n^2$" ]
[ null ]
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https://www.rdocumentation.org/packages/spatstat/versions/1.55-1/topics/rpoisppOnLines
[ "# rpoisppOnLines\n\n0th\n\nPercentile\n\n##### Generate Poisson Point Pattern on Line Segments\n\nGiven a line segment pattern, generate a Poisson random point pattern on the line segments.\n\nKeywords\nspatial, datagen\n##### Usage\nrpoisppOnLines(lambda, L, lmax = NULL, ..., nsim=1)\n##### Arguments\nlambda\n\nIntensity of the Poisson process. A single number, a function(x,y), a pixel image (object of class \"im\"), or a vector of numbers, a list of functions, or a list of images.\n\nL\n\nLine segment pattern (object of class \"psp\") on which the points should be generated.\n\nlmax\n\nOptional upper bound (for increased computational efficiency). A known upper bound for the values of lambda, if lambda is a function or a pixel image. That is, lmax should be a number which is known to be greater than or equal to all values of lambda.\n\nAdditional arguments passed to lambda if it is a function.\n\nnsim\n\nNumber of simulated realisations to be generated.\n\n##### Details\n\nThis command generates a Poisson point process on the one-dimensional system of line segments in L. The result is a point pattern consisting of points lying on the line segments in L. The number of random points falling on any given line segment follows a Poisson distribution. The patterns of points on different segments are independent.\n\nThe intensity lambda is the expected number of points per unit length of line segment. It may be constant, or it may depend on spatial location.\n\nIn order to generate an unmarked Poisson process, the argument lambda may be a single number, or a function(x,y), or a pixel image (object of class \"im\").\n\nIn order to generate a marked Poisson process, lambda may be a numeric vector, a list of functions, or a list of images, each entry giving the intensity for a different mark value.\n\nIf lambda is not numeric, then the (Lewis-Shedler) rejection method is used. The rejection method requires knowledge of lmax, the maximum possible value of lambda. This should be either a single number, or a numeric vector of the same length as lambda. If lmax is not given, it will be computed approximately, by sampling many values of lambda.\n\nIf lmax is given, then it must be larger than any possible value of lambda, otherwise the results of the algorithm will be incorrect.\n\n##### Value\n\nIf nsim = 1, a point pattern (object of class \"ppp\") in the same window as L. If nsim > 1, a list of such point patterns.\n\npsp, ppp, runifpointOnLines, rpoispp\n\n##### Aliases\n• rpoisppOnLines\n##### Examples\n# NOT RUN {\nlive <- interactive()\nL <- psp(runif(10), runif(10), runif(10), runif(10), window=owin())\nif(live) plot(L, main=\"\")\n\n# uniform intensity\nY <- rpoisppOnLines(4, L)\n\n# uniform MARKED process with types 'a' and 'b'\nY <- rpoisppOnLines(c(a=4, b=5), L)\nif(live) {\nplot(L, main=\"\")\n}\n\n# intensity is a function\nY <- rpoisppOnLines(function(x,y){ 10 * x^2}, L, 10)\nif(live) {\nplot(L, main=\"\")\n}\n\n# intensity is an image\nZ <- as.im(function(x,y){10 * sqrt(x+y)}, unit.square())\nY <- rpoisppOnLines(Z, L, 15)\nif(live) {\nplot(L, main=\"\")" ]
[ null ]
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https://programming.vip/docs/dynamic-regular-expression-in-matlab.html
[ "# Dynamic regular expression in Matlab\n\ncatalogue\n\nDynamic regular expression\n\nbrief introduction\n\nDynamic matching expression - (?? expr)\n\nModify the command matching the expression - (? @ cmd)\n\nFunctional requirements of (@ cmd)\n\nOverride command in expression - \\${cmd}\n\n## Dynamic regular expression\n\n### brief introduction\n\nIn a dynamic expression, you can require regexp to match. The pattern changes dynamically with the content of the input text. In this way, different input patterns in the parsed text can be more closely matched. Alternatively, you can use dynamic expressions in alternatives for the regexprep function. In this way, there is a way to make the alternative text better adapt to the parsed input.\n\nYou can click match in the following command_ Expr or replace_expr parameter contains any number of dynamic expressions: modify the value in myfunc:\n\n```regexp(text, match_expr)\nregexpi(text, match_expr)\nregexprep(text, match_expr, replace_expr)```\n\nTaking a dynamic expression as an example, the following regexprep command correctly replaces the term internationalization with its abbreviation i18n. However, to use this command with other terms, such as globalization, you must use a different alternative expression:\n\n```match_expr = '(^\\w)(\\w*)(\\w\\$)';\n\nreplace_expr1 = '\\$118\\$3';\nregexprep('internationalization', match_expr, replace_expr1)\nans =\n\n'i18n'\nreplace_expr2 = '\\$111\\$3';\nregexprep('globalization', match_expr, replace_expr2)\nans =\n\n'g11n'```\n\nWith the dynamic expression \\${num2str(length(}))}, you can base an alternative expression on the input text so that you don't have to change the expression every time. This example uses the dynamic substitution syntax \\${cmd}.\n\n```match_expr = '(^\\w)(\\w*)(\\w\\$)';\nreplace_expr = '\\$1\\${num2str(length(\\$2))}\\$3';\n\nregexprep('internationalization', match_expr, replace_expr)\nans =\n\n'i18n'\nregexprep('globalization', match_expr, replace_expr)\nans =\n\n'g11n'```\n\nAfter parsing, the dynamic expression must correspond to a complete valid regular expression. In addition, dynamic matching expressions that use backslashes to escape characters (\\) require two backslashes: one for initial parsing of the expression and one for full matching. Parentheses enclosing dynamic expressions do not create capture groups.\n\nThere are three forms of dynamic expressions that can be used as matching expressions and one form of dynamic expressions that can be used as substitute expressions. These dynamic expressions are introduced below.\n\n### Dynamic matching expression - (?? expr)\n\n(?? expr) operator parses the expression expr and inserts the result back into the matching expression. Then, MATLAB ® The modified matching expression is evaluated.\n\nThe following is an example of an expression type that uses this operator:\n\n```chr = {'5XXXXX', '8XXXXXXXX', '1X'};\nregexp(chr, '^(\\d+)(??X{\\$1})\\$', 'match', 'once');```\n\nThe purpose of this special command is to locate a series of consecutive x characters in each character vector stored in the input cell array. Note, however, that the number of X , varies in each character vector. If the number does not change, you can use the expression {X{n} to indicate n of these characters to match. However, n is a constant value and does not apply to this example.\n\nThe solution used here is to capture the leading count in the markup (e.g. 5 in the first character vector of the cell array), and then use the count in the dynamic expression. The dynamic expression in this example is (? X{ }), where \\$1 is the value captured by the markup \\ d +. The operator {\\$1} creates a qualifier for the token value. The first mock exam is dynamic, so the same pattern applies to all three input vectors in the cell array. For the first input character vector, regexp finds five x characters; For the second input string, the command looks for eight characters, while for the third input string, it looks for only one character:\n\n```regexp(chr, '^(\\d+)(??X{\\$1})\\$', 'match', 'once')\nans =\n\n1×3 cell array\n\n{'5XXXXX'} {'8XXXXXXXX'} {'1X'}```\n\n### Modify the command matching the expression - (? @ cmd)\n\nMatlab uses the (? @ cmd) operator to incorporate the results of MATLAB commands into the matching expression. This command must return items that can be used in matching expressions.\n\nFor example, use the dynamic expression (? @ flilplr( )) to find the palindrome \"Never Odd or Even\" embedded in a larger character vector.\n\nFirst, create the input string. Make sure all letters are lowercase and delete all non word characters.\n\n```chr = lower(...\n'Find the palindrome Never Odd or Even in this string');\n\nchr = regexprep(chr, '\\W*', '')\nchr =\n\n'findthepalindromeneveroddoreveninthisstring'```\n\nFind palindromes in a character vector using the following dynamic expression:\n\n```palindrome = regexp(chr, '(.{3,}).?(??@fliplr(\\$1))', 'match')\npalindrome =\n\n1×1 cell array\n\n{'neveroddoreven'}```\n\nThe dynamic expression reverses the order of the letters that make up the character vector, and then tries to match as many inverse character vectors as possible. This requires a dynamic expression because the value of \\$1} depends on the value of the markup (. {3,}).\n\nDynamic expressions in MATLAB have access to the currently active workspace. This means that you can change any function or variable used in a dynamic expression simply by changing the variables in the workspace. Repeat the last command of the above example, but this time use the function handle stored in the basic workspace to define the function to be invoked in the expression:\n\n```fun = @fliplr;\n\npalindrome = regexp(chr, '(.{3,}).?(??@fun(\\$1))', 'match')\npalindrome =\n\n1×1 cell array\n\n{'neveroddoreven'}```\n\n### Commands that meet functional requirements - (? @ cmd)\n\nThe (? @ cmd) operator is used to specify the matlab command that regexp or regexprep will run when parsing the entire matching expression. Unlike other dynamic expressions in MATLAB, this operator does not change the content of the expression in which it is located. Instead, you can use this feature to let Matlab report only the steps taken when parsing the contents of one of the regular expressions. This feature can be used to diagnose regular expressions.\n\nThe following example parses a word consisting of zero or more characters followed by two identical characters followed by zero or more characters:\n\n```regexp('mississippi', '\\w*(\\w)\\1\\w*', 'match')\nans =\n\n1×1 cell array\n\n{'mississippi'}```\n\nTo track the exact steps that MATLAB takes when determining a match, this example inserts a short script (? @ disp( )) into the expression to display the characters that ultimately make up the match. Since this example uses positive qualifiers, matlab tries to match as many character vectors as possible. In this way, even if matlab finds a match at the beginning of the string, it will continue to find more matches until it reaches the end of the string. From there, it backs up the letters i to p and the next p and stops there because the match finally meets the requirements:\n\n```regexp('mississippi', '\\w*(\\w)(?@disp(\\$1))\\1\\w*', 'match')\ni\np\np\n\nans =\n\n1×1 cell array\n\n{'mississippi'}```\n\nNow try the same example again, this time setting the first qualifier to the de limit qualifier (*?). Similarly, MATLAB generates the same match:\n\n```regexp('mississippi', '\\w*?(\\w)\\1\\w*', 'match')\nans =\n\n1×1 cell array\n\n{'mississippi'}```\n\nHowever, by inserting a dynamic script, you can see the match this time, and MATLAB matches the text in a completely different way. In this example, matlab uses the first match that can be found without even considering the rest of the text:\n\n```regexp('mississippi', '\\w*?(\\w)(?@disp(\\$1))\\1\\w*', 'match')\nm\ni\ns\n\nans =\n\n1×1 cell array\n\n{'mississippi'}```\n\nTo demonstrate the flexibility of this type of dynamic expression, try the following example. When MATLAB parses the input text iteratively, the example will gradually set up a cell array. Found (?!) at the end of the expression The operator is actually an empty forward operator that forces failure at each iteration. This forced failure is necessary if you want to track the steps MATLAB takes when processing expressions.\n\nMATLAB passes through the input text many times, each time trying another letter combination to see if it can find a better match than the previous one. In any pass that does not find a match, the test generates a null character vector. The dynamic script (@ if (~ isempty (\\$&)) is used to omit the empty character vector in the \"matches\" cell array:\n\n```matches = {};\nexpr = ['(Euler\\s)?(Cauchy\\s)?(Boole)?(?@if(~isempty(\\$&)),' ...\n'matches{end+1}=\\$&;end)(?!)'];\n\nregexp('Euler Cauchy Boole', expr);\n\nmatches\nmatches =\n\n1×6 cell array\n\n{'Euler Cauchy Bo...'} {'Euler Cauchy '} {'Euler '} {'Cauchy Boole'} {'Cauchy '} {'Boole'}```\n\nThe operators \\$& (or the equivalent of \\$0), \\$` and \\$'refer to the part of the current match in the input text, all characters before the current match, and all characters after the current match, respectively. These operators are sometimes useful when dealing with dynamic expressions, especially those that use (? @ cmd) operators.\n\nThe following example parses the input text to find the letter G. When scanning the text in each iteration, regexp , compares the current character with , g , and advances to the next character if no match is found. This example tracks the progress of scanning in this text by marking the current position to be parsed with the ^ character.\n\n(\\$` and \\$´ operators capture the text part before and after the current parsing position. When the sequence \\$´ appears in the text, you need to use two single quotation marks (\\$'') to represent it.)\n\n```chr = 'abcdefghij';\nexpr = '(?@disp(sprintf(''starting match: [%s^%s]'',\\$`,\\$'')))g';\n\nregexp(chr, expr, 'once');\nstarting match: [^abcdefghij]\nstarting match: [a^bcdefghij]\nstarting match: [ab^cdefghij]\nstarting match: [abc^defghij]\nstarting match: [abcd^efghij]\nstarting match: [abcde^fghij]\nstarting match: [abcdef^ghij]```\n\n### Override command in expression - \\${cmd}\n\nThe \\${cmd} operator modifies the contents of the regular expression substitution pattern so that it applies to parameters in the input text that may vary depending on usage. Like other dynamic expressions used in MATLAB, any number of these expressions can be included in the whole alternative expression.\n\nIn the 'regexprep' call shown here, the alternative mode is' \\${convertMe({,})} '. In this example, the whole alternative mode is a dynamic expression:\n\n```regexprep('This highway is 125 miles long', ...\n'(\\d+\\.?\\d*)\\W(\\w+)', '\\${convertMe(\\$1,\\$2)}');```\n\nThis dynamic expression instructs MATLAB to execute a function called convertMe using two tags derived from the matched text (\\ d+\\.?\\d *) and (\\ w +) as parameters of the call to convertMe. Because the values of \\$1 , and \\$2 , are generated at run time, alternative patterns require dynamic expressions.\n\nThe following example defines a function called convertMe, which converts measurements from Imperial units to metric units.\n\n```function valout = convertMe(valin, units)\nswitch(units)\ncase 'inches'\nfun = @(in)in .* 2.54;\nuout = 'centimeters';\ncase 'miles'\nfun = @(mi)mi .* 1.6093;\nuout = 'kilometers';\ncase 'pounds'\nfun = @(lb)lb .* 0.4536;\nuout = 'kilograms';\ncase 'pints'\nfun = @(pt)pt .* 0.4731;\nuout = 'litres';\ncase 'ounces'\nfun = @(oz)oz .* 28.35;\nuout = 'grams';\nend\nval = fun(str2num(valin));\nvalout = [num2str(val) ' ' uout];\nend```\n\nOn the command line, call the convertMe function through regexprep, and pass in the quantity value and imperial unit name to be converted:\n\n```regexprep('This highway is 125 miles long', ...\n'(\\d+\\.?\\d*)\\W(\\w+)', '\\${convertMe(\\$1,\\$2)}')\nans =\n\n'This highway is 201.1625 kilometers long'\nregexprep('This pitcher holds 2.5 pints of water', ...\n'(\\d+\\.?\\d*)\\W(\\w+)', '\\${convertMe(\\$1,\\$2)}')\nans =\n\n'This pitcher holds 1.1828 litres of water'\nregexprep('This stone weighs about 10 pounds', ...\n'(\\d+\\.?\\d*)\\W(\\w+)', '\\${convertMe(\\$1,\\$2)}')\nans =\n\n'This stone weighs about 4.536 kilograms'```\n\nLike the (? @) operator discussed in the previous section, the \\${} operator has access to variables in the currently active workspace. The following regexprep command uses array A defined in the underlying workspace:\n\n```A = magic(3)\n\nA =\n\n8 1 6\n3 5 7\n4 9 2\nregexprep('The columns of matrix _nam are _val', ...\n{'_nam', '_val'}, ...\n{'A', '\\${sprintf(''%d%d%d '', A)}'})\nans =\n\n'The columns of matrix A are 834 159 672'```\n\nKeywords: Front-end MATLAB regex\n\nAdded by shan169 on Mon, 14 Feb 2022 03:07:26 +0200" ]
[ null ]
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https://www.stumblingrobot.com/2015/08/10/compute-the-volume-of-the-solid-of-revolution-generated-by-fx-sin-x-cos-x/
[ "Home » Blog » Compute the volume of the solid of revolution generated by f(x) = sin x + cos x\n\n# Compute the volume of the solid of revolution generated by f(x) = sin x + cos x\n\nSketch the graph and compute the volume of the solid of revolution generated by:", null, "The sketch of the ordinate set of", null, "on", null, "is as follows:", null, "We then compute the volume of the solid of revolution. We reference the previous exercises here and here for the integrals of", null, "and", null, ".", null, "1.", null, "2.", null, "It is also possible, and arguably quicker, to use the identity", null, ", followed by the half-angle formula, and using that the integral of", null, "is 0 over any", null, "-length interval." ]
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https://cordis.europa.eu/project/id/235437
[ "", null, "", null, "# Equivariant topology in algebraic geometry\n\n## Objective\n\nIn physical sciences, a very challenging problem is the understanding of sudden changes caused by smooth alterations of parameters. For instance, water suddenly boils, or ice melts. The back of the camel breaks suddenly under a load of just one more straw. These abrupt changes are not only present in dynamical systems, but also in biology (e.g. population models, cell growth), and human society (e.g. stock markets). The proposer studies the mathematical theory of these phenomena, namely uses topological methods to understand how global topology forces singularities. The governing notion of global singularity theory is \"Thom polynomial\". The proposer has a strong research record on computing and applying Thom polynomials in various topological settings, eg. differentiable maps, forms, quivers, discriminants. The objective of the proposal is to support the proposer's career development by extending his expertise from {\\em topology} to modern geometry and related geometric and algebraic combinatorics. Visiting the Renyi Mathematical Institute in Budapest for a year, doing training and research under the supervision of A. Nemethi (scientist in charge) will significantly develop and widen the competences of the researcher. The equivariant techniques Rimanyi used in the theory of singularities is proposed to be applied in geometrically relevant situations. The two concrete proposed projects are the study of matroid versions of linear Gromov-Witten invariants, and the geometry of natural stratifications on punctual Hilbert schemes of high dimension spaces.\n\n### Field of science\n\n• /natural sciences/mathematics/pure mathematics/topology\n• /natural sciences/mathematics/pure mathematics/geometry\n• /natural sciences/physical sciences\n• /natural sciences/mathematics/applied mathematics/dynamical systems\n• /natural sciences/mathematics/pure mathematics/algebra/algebraic geometry\n\n### Call for proposal\n\nFP7-PEOPLE-IEF-2008\nSee other projects for this call\n\n### Funding Scheme\n\nMC-IEF - Intra-European Fellowships (IEF)\n\n### Coordinator\n\nRENYI ALFRED MATEMATIKAI KUTATOINTEZET" ]
[ null, "https://cordis.europa.eu/assets/img/pdf-header.png", null, "https://cordis.europa.eu/assets/img/projects/icons/logo-fp7.jpg", null ]
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