Leibniz formula for π

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See Leibniz (disambiguation) for other formulas known under the same name.

In mathematics, the Leibniz formula for π, named after Gottfried Leibniz, states that

1 \,-\, \frac{1}{3} \,+\, \frac{1}{5} \,-\, \frac{1}{7} \,+\, \frac{1}{9} \,-\, \cdots \;=\; \frac{\pi}{4}.\!

Using summation notation:

\sum_{n=0}^\infty \, \frac{(-1)^n}{2n+1} \;=\; \frac{\pi}{4}.\!

Names[edit]

The infinite series above is called the Leibniz series. It is also called the Gregory–Leibniz series, recognizing the work of James Gregory. The formula was first discovered by Madhava of Sangamagrama[1] in the 14th century, but was not widely known in the West. Since Leibniz, however, was the first person to rediscover the series in continental Europe, it is named after him. In retrospect, the naming is sometimes modified to Madhava–Leibniz series in order to recognize Madhava's contribution.[2]

It also is the Dirichlet L-series of the non-principal Dirichlet character of modulus 4 evaluated at s=1, and therefore the value β(1) of the Dirichlet beta function.

Proof[edit]


{\begin{align}
\frac{\pi}{4} & = \arctan(1)\;=\;\int_0^1 \frac 1{1+x^2} \, dx \\[8pt]
& = \int_0^1\left(\sum_{k=0}^n (-1)^k x^{2k}+\frac{(-1)^{n+1}\,x^{2n+2} }{1+x^2}\right) \, dx \\[8pt]
& = \sum_{k=0}^n \frac{(-1)^k}{2k+1}
+(-1)^{n+1}\int_0^1\frac{x^{2n+2}}{1+x^2} \, dx.
\end{align}}

Considering only the integral in the last line, we have:

0 < \int_0^1 \frac{x^{2n+2}}{1+x^2}\,dx \;<\; \int_0^1 x^{2n+2}\,dx \;=\; \frac{1}{2n+3} \;\rightarrow\; 0 \text{ as } n \rightarrow \infty.\!

Therefore, as n → ∞ we are left with the Leibniz series:

\frac{\pi}4\;=\;\sum_{k=0}^\infty\frac{(-1)^k}{2k+1}.

for a more detailed proof, together with the original geometric proof by Leibniz himself, see.[3]

Inefficiency[edit]

Leibniz's formula converges extremely slowly: it exhibits sublinear convergence. Calculating π to 10 correct decimal places using direct summation of the series requires about 5,000,000,000 terms because \scriptstyle \frac 1{2k+1}<10^{-10} for \scriptstyle k>\frac{10^{10}-1}2.

However, the Leibniz formula can be used to calculate π to high precision (hundreds of digits or more) using various convergence acceleration techniques. For example, the Shanks transformation, Euler transform or Van Wijngaarden transformation, which are general methods for alternating series, can be applied effectively to the partial sums of the Leibniz series. Further, combining terms pairwise gives the non-alternating series

\frac{\pi}{4} = \sum_{n=0}^{\infty} \bigg(\frac{1}{4n+1}-\frac{1}{4n+3}\bigg) = \sum_{n=0}^{\infty} \frac{2}{(4n+1)(4n+3)}

which can be evaluated to high precision from a small number of terms using Richardson extrapolation or the Euler–Maclaurin formula. This series can also be transformed into an integral by means of the Abel–Plana formula and evaluated using techniques for numerical integration.

Unusual behavior[edit]

If the series is truncated at the right time, the decimal expansion of the approximation will agree with that of π for many more digits, except for isolated digits or digit groups. For example, taking 5,000,000 terms yields

3.1415924535897932384646433832795027841971693993873058...

where the underlined digits are wrong. The errors can in fact be predicted; they are generated by the Euler numbers En according to the asymptotic formula

\frac{\pi}{2} - 2 \sum_{k=1}^{N/2} \frac{(-1)^{k-1}}{2k-1} \sim \sum_{m=0}^{\infty} \frac{E_{2m}}{N^{2m+1}}\!

where N is an integer divisible by 4. If N is chosen to be a power of ten, each term in the right sum becomes a finite decimal fraction. The formula is a special case of the Boole summation formula for alternating series, providing yet another example of a convergence acceleration technique that can be applied to the Leibniz series. In 1992, Jonathan Borwein and Mark Limber used the first thousand Euler numbers to calculate π to 5,263 decimal places with Leibniz' formula.

Euler product[edit]

The Leibniz formula can be interpreted as a Dirichlet series using the (unique) Dirichlet character modulo 4. As with other Dirichlet series, this allows the infinite sum to be converted to an infinite product with one term for each prime number. Such a product is called an Euler product. It is:

\pi/4=\left(\prod_{p\equiv 1\pmod 4}\frac{p}{p-1}\right)\cdot\left( \prod_{p\equiv 3\pmod 4}\frac{p}{p+1}\right)=\frac{3}{4} \cdot \frac{5}{4} \cdot \frac{7}{8} \cdot \frac{11}{12} \cdot \frac{13}{12}\cdot\frac{17}{16} \cdots

In this product, each term is a superparticular ratio, each numerator is a odd prime number, and each denominator is the nearest multiple of four to the numerator.[4]

See also[edit]

Notes[edit]

  1. ^ George E. Andrews, Richard Askey, Ranjan Roy (1999), Special Functions, Cambridge University Press, p. 58, ISBN 0-521-78988-5 
  2. ^ Gupta, R. C. (1992), "On the remainder term in the Madhava–Leibniz's series", Ganita Bharati 14 (1-4): 68–71 
  3. ^ Leibniz's formula for Pi, proofwiki.org 
  4. ^ Debnath, Lokenath (2010), The Legacy of Leonhard Euler: A Tricentennial Tribute, World Scientific, p. 214, ISBN 9781848165267 .

References[edit]

  • Jonathan Borwein, David Bailey & Roland Girgensohn, Experimentation in Mathematics - Computational Paths to Discovery, A K Peters 2003, ISBN 1-56881-136-5, pages 28–30.

External links[edit]