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Aymen Hafeez

Miscellaneous formulae for pi

Various formulae relating to pi that I come across.

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Infinite products

The sinc\text{sinc} function is defined for x≠0x\neq0 as

sinc(x)=sin⁡(x)x\text{sinc}(x)=\frac{\sin(x)}{x}

It can also be expressed as an infinite product:

sin⁡(x)x=∏n=1∞(1−x2π2n2)\frac{\sin(x)}{x}=\prod_{n=1}^{\infty}\left(1-\frac{x^2}{\pi^2n^2}\right)

The normalised sinc\text{sinc} function is

sin⁡(πx)πx=∏n=1∞(1−x2n2)\frac{\sin(\pi x)}{\pi x}=\prod_{n=1}^{\infty}\left(1-\frac{x^2}{n^2}\right)

See this post on the Riemann zeta function at even values for a short overview on expressing functions in this form, or look into the Weierstrass factorisation theorem for a more rigorous explanation. Letting x=12x=\frac{1}{2} gives

2π=∏n=1∞(1−14n2)=∏n=1∞(4n2−14n2)\frac{2}{\pi}=\prod_{n=1}^{\infty}\left(1-\frac{1}{4n^2}\right) = \prod_{n=1}^{\infty}\left(\frac{4n^2-1}{4n^2}\right)

This is Wallis’s formula for π\pi. And taking the reciprocal:

π2=∏n=1∞(4n24n2−1)\frac{\pi}{2}=\prod_{n=1}^{\infty}\left(\frac{4n^2}{4n^2-1}\right)

If instead we let x=14x=\frac{1}{4} we get

22π=∏n=1∞(1−116n2)=∏n=1∞(16n2−116n2)\frac{2\sqrt{2}}{\pi}=\prod_{n=1}^{\infty}\left(1-\frac{1}{16n^2}\right) =\prod_{n=1}^{\infty}\left(\frac{16n^2-1}{16n^2}\right)

Again, taking the reciprocal gives

π22=∏n=1∞(16n216n2−1)\frac{\pi}{2\sqrt{2}}=\prod_{n=1}^{\infty}\left(\frac{16n^2}{16n^2-1}\right) π24=∏n=1∞(16n216n2−1)\frac{\pi\sqrt{2}}{4}=\prod_{n=1}^{\infty}\left(\frac{16n^2}{16n^2-1}\right)

These are both quite nice formulae for π\pi. However, they converge VERY slowly. The first expression approximates π≈3.1415848\pi\approx3.1415848 after ten thousand terms.

Euler

Euler famously proved that ζ(2)=π26\zeta(2) = \frac{\pi^{2}}{6}. He started with the function sin⁡xx\frac{\sin x}{x}, i.e. the sinc\text{sinc} function, which has the Taylor series expansion

sinc x=sin⁡xx=∑n=0∞(−1)n(2n+1)!x2n=1−x23!+x45!−x67!+…\text{sinc }x = \frac{\sin x}{x} = \sum_{n=0}^{\infty} \frac{(-1)^{n}}{(2n+1)!}x^{2n} = 1 - \frac{x^{2}}{3!} + \frac{x^{4}}{5!} - \frac{x^{6}}{7!} + \ldots

The sinc\text{sinc} function can also be expressed as the following infinite product:

sinc x=∏n=1∞(1−x2π2n2)=(1−x2π2)(1−x24π2)(1−x29π2)…\text{sinc }x = \prod_{n=1}^{\infty} \left( 1 - \frac{x^{2}}{\pi^{2}n^{2}} \right) = \left( 1 - \frac{x^{2}}{\pi^{2}} \right) \left( 1 - \frac{x^{2}}{4\pi^{2}} \right) \left( 1 - \frac{x^{2}}{9\pi^{2}} \right) \ldots =1−x2(1π2+14π2+19π2+…)+…= 1 - x^{2} \left( \frac{1}{\pi^{2}} + \frac{1}{4\pi^{2}} + \frac{1}{9\pi^{2}} + \ldots \right) + \ldots

Equating the x2x^{2} coefficients of the above to the Taylor series expansion gives the desired result:

−(1π2+14π2+19π2+…)=−13!-\left( \frac{1}{\pi^{2}} + \frac{1}{4\pi^{2}} + \frac{1}{9\pi^{2}} + \ldots \right) = - \frac{1}{3!} ζ(2)=∑_n=1∞1n2=π26\zeta(2) = \sum\_{n=1}^{\infty} \frac{1}{n^{2}} = \frac{\pi^{2}}{6}

A similar result can be derived for the odd squares. Instead of sinc x\text{sinc } x we start with cos⁡x\cos x. The series expansion for cos⁡x\cos x is

cos⁡x=∑n=0∞(−1)n(2n)!x2n=1−x22!+x44!−x66!+…\cos x = \sum_{n=0}^{\infty} \frac{(-1)^{n}}{(2n)!}x^{2n} = 1 - \frac{x^{2}}{2!} + \frac{x^{4}}{4!} - \frac{x^{6}}{6!} + \ldots

cos⁡x\cos x can also be expressed as an infinite product:

cos⁡x=∏n=1∞(1−4x2π2(2n−1)2)=1−x2(4π2+49π2+425π2+…)+…\cos x = \prod_{n=1}^{\infty} \left( 1 - \frac{4x^{2}}{\pi^{2}(2n - 1)^{2}} \right) = 1 - x^{2}\left( \frac{4}{\pi^{2}} + \frac{4}{9\pi^{2}} + \frac{4}{25\pi^{2}} + \ldots \right) + \ldots

And again, equating the x2x^{2} coefficients:

−4π2(1+19+125+…)=−12!-\frac{4}{\pi^{2}}\left( 1 + \frac{1}{9} + \frac{1}{25} + \ldots \right) = - \frac{1}{2!} ∑n=1∞1(2n−1)2=π28\sum_{n=1}^{\infty} \frac{1}{(2n - 1)^{2}} = \frac{\pi^{2}}{8}

Going back to the infinite product form of sin⁡xx\frac{\sin x}{x},

sinc x=∏n=1∞(1−x2π2n2)=(1−x2π2)(1−x24π2)(1−x29π2)…,\text{sinc }x = \prod_{n=1}^{\infty} \left( 1 - \frac{x^{2}}{\pi^{2}n^{2}} \right) = \left( 1 - \frac{x^{2}}{\pi^{2}} \right) \left( 1 - \frac{x^{2}}{4\pi^{2}} \right) \left( 1 - \frac{x^{2}}{9\pi^{2}} \right) \ldots,

and noting that each term is the difference of two squares, we can separate them out:

sin⁡x=x(1−xπ)(1+xπ)(1−x2π)(1+x2π)(1−x3π)(1+x3π)…\sin x = x\left( 1 - \frac{x}{\pi} \right)\left( 1 + \frac{x}{\pi} \right) \left( 1 - \frac{x}{2\pi} \right)\left( 1 + \frac{x}{2\pi} \right) \left( 1 - \frac{x}{3\pi} \right)\left( 1 + \frac{x}{3\pi} \right) \ldots

Taking the log⁡\log of both sides:

log⁡sin⁡x=log⁡x+log⁡(1−xπ)+log⁡(1+xπ)+log⁡(1−x2π)+…,\log \sin x = \log x + \log \left( 1 - \frac{x}{\pi} \right) + \log \left( 1 + \frac{x}{\pi} \right) + \log \left( 1 - \frac{x}{2\pi} \right) + \ldots,

and then taking the derivative:

cos⁡xsin⁡x=1x−1π−x+1π+x−12π−x+…\frac{\cos x}{\sin x} = \frac{1}{x} - \frac{1}{\pi - x} + \frac{1}{\pi + x} - \frac{1}{2\pi - x} + \ldots

Letting x=π4x = \frac{\pi}{4} gives Leibniz’s formula for π\pi:

π4=1−13+15−17+19−….\frac{\pi}{4} = 1 - \frac{1}{3} + \frac{1}{5} - \frac{1}{7} + \frac{1}{9} - \ldots .