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Showing posts from April, 2020

Fermat's treatment of generalized parabolic quadrature

Around 1640 Fermat documented this method in a awkwardly titled paper: De aequationum localium transmutatione et emendatione ad multimodam curvilineorum inter se vel cum rectilineis comparationem (On the transformation and alteration of local equations for the purpose of variously comparing curvilinear figures among themselves or to rectilinear figures, to which is attached the use of geometric proportions in squaring an infinite number of parabolas and hyperbolas). The ideas presented in the paper was dated probably 20 years ago but it was only written in 1658, two years after the publication of John Wallis's Arithmetica Infinitorum (1656). But it was not published or circulated until 1679. , 30 years before Newton and Leibniz officially “invented" calculus, Fermat managed to convinced himself that k0xndx=kn+1n+1=L(n+1) Fermat's trick was to slice the area under the curve of y=xn into infinitely many irregular intervals so that the ...

Infinite products of Bernoulli and Euler

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In 1720, Christian Goldbach's experiments with infinite series was published in the German journal Acta Eruditorum , he titled his paper Specimen methodi ad summas serierum and proceeded to furnish a number of worked examples The following examples are given in Goldbach's 1720 paper: 12+16+112+120+264+11544+261972+475104+12+14+18+116+13+181+119683+143046721+whose general terms are 1x2+x, 3x219x4+36x3+33x26x8, 12x, and 12xxx. of his finite difference technique for relocating the general term of a given sequence. The general principle is that in the general case, the n-th term, an, of any number sequence a1,a2,a3, can be expressed by using an infinite series involving ...

Eulerian integrals and generalized factorials

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Anybody with one-to-two years of basic calculus exposure can easily work out the following definite integral of xn: k0xndx=kn+1n+1=L(n+1) where L(n)=kn/n. This is a mid-17th-century result known to both Newton and Leibniz , but their results were not written in modern notation In his 1669 paper “De Analysi per Aequationes Numero Terminorum Infinitas" (Of analysis by equations of an infinite number of terms), Newton wrote: Let the base AB of any curve AD have BD for its perpendicular ordinate; and call AB=x, BD=y, and let a,b,c, etc be given quantities, and m and n whole numbers, then following rule (Rule I) can be used to compute the quadrature of simple curves. If axm/n=y, thenanm+nxm+nn=areaABDNewton then proceeded to give a number of examples. He wrote: The thing will be evident by an example. If x2=y, th...

R resources

General Mara Averick's blog . R for Data Science by Garrett Grolemund and Hadley Wickham. R for Data Science: Exercise Solutions by Jeffrey B. Arnold. Hands-On Programming with R by Garrett Grolemund. The Tidyverse Cookbook by Garrett Grolemund. Tidy Evaluation by Lionel Henry and Hadley Wickham. Functional Programming by Sara Altman, Bill Behrman, and Hadley Wickham. Advanced R by Hadley Wickham. Advanced R Solutions by Malte Grosser, Henning Bumann and Hadley Wickham. Make your R roar by Purrring by Gavin Fay. Geocomputation with R by Robin Lovelace, Jakub Nowosad, Jannes Muenchow. R Packages by Hadley Wickham and Jenny Bryan. R Cookbook by James Long and Paul Teetor. R语言忍者秘笈 by 谢益辉, 肖楠, 坑主三, and 坑主四. Stat405: Introduction to Data Analysis (Fall 2012, Rice University) by Hadley Wickham. Stat545: Data wrangling, exploration, and analysis with R by Jenny Bryan. Data Visualization ggplot2: Elegant Graphics for Data Analysis by Hadley Wic...

Sins of various degrees

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Euler's formula eiΩ=sin(AΩ)+isinΩ, where A=12π, is an interesting formula because we can use it express various types of sins in our complex world, and it says that sins of various degrees are ultimately imaginary. Here is the proof. First we suppose Ω=12πω, since eiπω/2=e(iπ/2)ω=(eiπ/2)ωwe must have sin(A12πω)+isin12πω=[sin(A12π)+isin12π]ω=iω and if we start with Ω=12πω, the following is true: sin(A+12πω)isin12πω=[sin(A+12π)isin12π]ω=(i)ω Since \(\sin \left(A+ \tfrac{1}{2}\pi \omega \right)=\sin \left(A - \tfrac{1}{2}\pi \omega \righ...