Proof Of Wallis Product
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mathematics Mathematics is an area of knowledge that includes the topics of numbers, formulas and related structures, shapes and the spaces in which they are contained, and quantities and their changes. These topics are represented in modern mathematics ...
, the Wallis product for , published in 1656 by
John Wallis John Wallis (; la, Wallisius; ) was an English clergyman and mathematician who is given partial credit for the development of infinitesimal calculus. Between 1643 and 1689 he served as chief cryptographer for Parliament and, later, the royal ...
, states that :\begin \frac & = \prod_^ \frac = \prod_^ \left(\frac \cdot \frac\right) \\ pt& = \Big(\frac \cdot \frac\Big) \cdot \Big(\frac \cdot \frac\Big) \cdot \Big(\frac \cdot \frac\Big) \cdot \Big(\frac \cdot \frac\Big) \cdot \; \cdots \\ \end


Proof using integration

Wallis derived this infinite product as it is done in calculus books today, by examining \int_0^\pi \sin^n x\,dx for even and odd values of n, and noting that for large n, increasing n by 1 results in a change that becomes ever smaller as n increases. Let :I(n) = \int_0^\pi \sin^n x\,dx. (This is a form of Wallis' integrals.)
Integrate by parts In calculus, and more generally in mathematical analysis, integration by parts or partial integration is a process that finds the integral of a product of functions in terms of the integral of the product of their derivative and antiderivative. ...
: :\begin u &= \sin^x \\ \Rightarrow du &= (n-1) \sin^x \cos x\,dx \\ dv &= \sin x\,dx \\ \Rightarrow v &= -\cos x \end :\begin \Rightarrow I(n) &= \int_0^\pi \sin^n x\,dx \\ pt &= -\sin^x\cos x \Biggl, _0^\pi - \int_0^\pi (-\cos x)(n-1) \sin^x \cos x\,dx \\ pt &= 0 + (n-1) \int_0^\pi \cos^2x \sin^x\,dx, \qquad n > 1 \\ pt &= (n - 1) \int_0^\pi (1-\sin^2 x) \sin^x\,dx \\ pt &= (n - 1) \int_0^\pi \sin^x\,dx - (n - 1) \int_0^\pi \sin^x\,dx \\ pt &= (n - 1) I(n-2)-(n-1) I(n) \\ pt &= \frac I(n-2) \\ pt \Rightarrow \frac &= \frac \\ pt\end Now, we make two variable substitutions for convenience to obtain: :I(2n) = \fracI(2n-2) :I(2n+1) = \fracI(2n-1) We obtain values for I(0) and I(1) for later use. :\begin I(0) &= \int_0^\pi dx = x\Biggl, _0^\pi = \pi \\ pt I(1) &= \int_0^\pi \sin x\,dx = -\cos x \Biggl, _0^\pi = (-\cos \pi)-(-\cos 0) = -(-1)-(-1) = 2 \\ pt\end Now, we calculate for even values I(2n) by repeatedly applying the recurrence relation result from the integration by parts. Eventually, we end get down to I(0), which we have calculated. :I(2n)=\int_0^\pi \sin^x\,dx = \fracI(2n-2) = \frac \cdot \fracI(2n-4) :=\frac \cdot \frac \cdot \frac \cdot \cdots \cdot \frac \cdot \frac \cdot \frac I(0)=\pi \prod_^n \frac Repeating the process for odd values I(2n+1), :I(2n+1)=\int_0^\pi \sin^x\,dx=\fracI(2n-1)=\frac \cdot \fracI(2n-3) :=\frac \cdot \frac \cdot \frac \cdot \cdots \cdot \frac \cdot \frac \cdot \frac I(1)=2 \prod_^n \frac We make the following observation, based on the fact that \sin \leq 1 :\sin^x \le \sin^x \le \sin^x, 0 \le x \le \pi :\Rightarrow I(2n+1) \le I(2n) \le I(2n-1) Dividing by I(2n+1): :\Rightarrow 1 \le \frac \le \frac=\frac, where the equality comes from our recurrence relation. By the squeeze theorem, :\Rightarrow \lim_ \frac=1 :\lim_ \frac=\frac \lim_ \prod_^n \left(\frac \cdot \frac\right)=1 :\Rightarrow \frac=\prod_^\infty \left(\frac \cdot \frac\right)=\frac \cdot \frac \cdot \frac \cdot \frac \cdot \frac \cdot \frac \cdot \cdots


Proof using

Laplace's method In mathematics, Laplace's method, named after Pierre-Simon Laplace, is a technique used to approximate integrals of the form :\int_a^b e^ \, dx, where f(x) is a twice-differentiable function, ''M'' is a large number, and the endpoints ''a'' an ...

See the main page on Gaussian integral.


Proof using Euler's infinite product for the sine function

While the proof above is typically featured in modern calculus textbooks, the Wallis product is, in retrospect, an easy corollary of the later Euler infinite product for the
sine function In mathematics, sine and cosine are trigonometric functions of an angle. The sine and cosine of an acute angle are defined in the context of a right triangle: for the specified angle, its sine is the ratio of the length of the side that is opp ...
. :\frac = \prod_^\infty\left(1 - \frac\right) Let x = \frac: :\begin \Rightarrow\frac &= \prod_^\infty \left(1 - \frac\right) \\ pt \Rightarrow\frac &= \prod_^\infty \left(\frac\right) \\ pt &= \prod_^\infty \left(\frac\cdot\frac\right) = \frac \cdot \frac \cdot \frac \cdot \frac \cdot \frac \cdot \frac \cdots \end    


Relation to Stirling's approximation

Stirling's approximation for the factorial function n! asserts that :n! = \sqrt ^n \left + O\left(\frac\right) \right Consider now the finite approximations to the Wallis product, obtained by taking the first k terms in the product :p_k = \prod_^ \frac\frac, where p_k can be written as :\begin p_k &= \prod_^ \frac \\ pt &= \cdot . \end Substituting Stirling's approximation in this expression (both for k! and (2k)!) one can deduce (after a short calculation) that p_k converges to \frac as k \rightarrow \infty.


Derivative of the Riemann zeta function at zero

The
Riemann zeta function The Riemann zeta function or Euler–Riemann zeta function, denoted by the Greek letter (zeta), is a mathematical function of a complex variable defined as \zeta(s) = \sum_^\infty \frac = \frac + \frac + \frac + \cdots for \operatorname(s) > ...
and the Dirichlet eta function can be defined: :\begin \zeta(s) &= \sum_^\infty \frac, \Re(s)>1 \\ pt \eta(s) &= (1-2^)\zeta(s) \\ pt &= \sum_^\infty \frac, \Re(s)>0 \end Applying an Euler transform to the latter series, the following is obtained: :\begin \eta(s) &= \frac+\frac \sum_^\infty (-1)^\left frac-\frac\right \Re(s)>-1 \\ pt \Rightarrow \eta'(s) &= (1-2^)\zeta'(s)+2^ (\ln 2) \zeta(s) \\ pt &= -\frac \sum_^\infty (-1)^\left frac-\frac\right \Re(s)>-1 \end :\begin \Rightarrow \eta'(0) &= -\zeta'(0) - \ln 2 = -\frac \sum_^\infty (-1)^\left ln n-\ln (n+1)\right\\ pt &= -\frac \sum_^\infty (-1)^\ln \frac \\ pt &= -\frac \left(\ln \frac - \ln \frac + \ln \frac - \ln \frac + \ln \frac - \cdots\right) \\ pt &= \frac \left(\ln \frac + \ln \frac + \ln \frac + \ln \frac + \ln \frac + \cdots\right) \\ pt &= \frac \ln\left(\frac\cdot\frac\cdot\frac\cdot\frac\cdot\cdots\right) = \frac \ln\frac \\ \Rightarrow \zeta'(0) &= -\frac \ln\left(2 \pi\right) \end


See also

*
John Wallis John Wallis (; la, Wallisius; ) was an English clergyman and mathematician who is given partial credit for the development of infinitesimal calculus. Between 1643 and 1689 he served as chief cryptographer for Parliament and, later, the royal ...
, English mathematician who is given partial credit for the development of
infinitesimal calculus Calculus, originally called infinitesimal calculus or "the calculus of infinitesimals", is the mathematical study of continuous change, in the same way that geometry is the study of shape, and algebra is the study of generalizations of arithm ...
and pi. * Viète's formula, a different infinite product formula for \pi. * Leibniz formula for , an infinite sum that can be converted into an infinite Euler product for \pi. *
Wallis sieve Wallis (derived from ''Wallace'') may refer to: People * Wallis (given name) **Wallis, Duchess of Windsor * Wallis (surname) Places * Wallis (Ambleston), a hamlet within the parish of Ambleston in Pembrokeshire, West Wales, United Kingdom * ...


Notes


External links

* * {{cbignore Articles containing proofs Pi algorithms Infinite products