Let

${\displaystyle A=\sum _{n=1}^{\infty }a_{n}}$ 

be an infinite sum whose value we wish to compute, and let

${\displaystyle B=\sum _{n=1}^{\infty }b_{n}}$ 

be an infinite sum with comparable terms whose value is known. If the limit

${\displaystyle \gamma :=\lim _{n\to \infty }{\frac {a_{n}}{b_{n}}}}$ 

exists, then ${\displaystyle a_{n}-\gamma \,b_{n}}$  is always also a sequence going to zero and the series given by the difference, ${\displaystyle \sum _{n=1}^{\infty }(a_{n}-\gamma \,b_{n})}$ , converges. If ${\displaystyle \gamma \neq 0}$ , this new series differs from the original ${\displaystyle \sum _{n=1}^{\infty }a_{n}}$  and, under broad conditions, converges more rapidly.^[1] We may then compute ${\displaystyle A}$  as

${\displaystyle A=\gamma \,B+\sum _{n=1}^{\infty }(a_{n}-\gamma \,b_{n})}$ ,

where ${\displaystyle \gamma B}$  is a constant. Where ${\displaystyle a_{n}\neq 0}$ , the terms can be written as the product ${\displaystyle (1-\gamma \,b_{n}/a_{n})\,a_{n}}$ . If ${\displaystyle a_{n}\neq 0}$  for all ${\displaystyle n}$ , the sum is over a component-wise product of two sequences going to zero,

${\displaystyle A=\gamma \,B+\sum _{n=1}^{\infty }(1-\gamma \,b_{n}/a_{n})\,a_{n}}$ .

Consider the Leibniz formula for π:

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

We group terms in pairs as

${\displaystyle 1-\left({\frac {1}{3}}-{\frac {1}{5}}\right)-\left({\frac {1}{7}}-{\frac {1}{9}}\right)+\cdots }$ 

${\displaystyle \,=1-2\left({\frac {1}{15}}+{\frac {1}{63}}+\cdots \right)=1-2A}$ 

where we identify

${\displaystyle A=\sum _{n=1}^{\infty }{\frac {1}{16n^{2}-1}}}$ .

We apply Kummer's method to accelerate ${\displaystyle A}$ , which will give an accelerated sum for computing ${\displaystyle \pi =4-8A}$ .

Let

${\displaystyle B=\sum _{n=1}^{\infty }{\frac {1}{4n^{2}-1}}={\frac {1}{3}}+{\frac {1}{15}}+\cdots }$ 

${\displaystyle \,={\frac {1}{2}}-{\frac {1}{6}}+{\frac {1}{6}}-{\frac {1}{10}}+\cdots }$ 

This is a telescoping series with sum value 1⁄2. In this case

${\displaystyle \gamma :=\lim _{n\to \infty }{\frac {\frac {1}{16n^{2}-1}}{\frac {1}{4n^{2}-1}}}=\lim _{n\to \infty }{\frac {4n^{2}-1}{16n^{2}-1}}={\frac {1}{4}}}$ 

and so Kummer's transformation formula above gives

${\displaystyle A={\frac {1}{4}}\cdot {\frac {1}{2}}+\sum _{n=1}^{\infty }\left(1-{\frac {1}{4}}{\frac {\frac {1}{4n^{2}-1}}{\frac {1}{16n^{2}-1}}}\right){\frac {1}{16n^{2}-1}}}$ 

${\displaystyle ={\frac {1}{8}}-{\frac {3}{4}}\sum _{n=1}^{\infty }{\frac {1}{16n^{2}-1}}{\frac {1}{4n^{2}-1}}}$ 

which converges much faster than the original series.

Coming back to Leibniz formula, we obtain a representation of ${\displaystyle \pi }$  that separates ${\displaystyle 3}$  and involves a fastly converging sum over just the squared even numbers ${\displaystyle (2n)^{2}}$ ,

${\displaystyle \pi =4-8A}$ 

${\displaystyle =3+6\cdot \sum _{n=1}^{\infty }{\frac {1}{(4(2n)^{2}-1)((2n)^{2}-1)}}}$ 

${\displaystyle =3+{\frac {2}{15}}+{\frac {2}{315}}+{\frac {6}{5005}}+\cdots }$ 

• Euler transform

• Senatov, V.V. (2001) [1994], "Kummer transformation", Encyclopedia of Mathematics, EMS Press
• Knopp, Konrad (2013). Theory and Application of Infinite Series. Courier Corporation. p. 247. ISBN 9780486318615.
• Conrad, Keith. "Accelerating Convergence of Series" (PDF).
• Kummer, E. (1837). "Eine neue Methode, die numerischen Summen langsam convergirender Reihen zu berech-nen". J. Reine Angew. Math. (16): 206–214.

• Weisstein, Eric W. "Kummer's Series Transformation". MathWorld.