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In mathematics, an alternating series is an infinite series of the form

\( {\displaystyle \sum _{n=0}^{\infty }(-1)^{n}a_{n}} \) or \( {\displaystyle \sum _{n=0}^{\infty }(-1)^{n+1}a_{n}} \)

with an > 0 for all n. The signs of the general terms alternate between positive and negative. Like any series, an alternating series converges if and only if the associated sequence of partial sums converges.


The geometric series 1/2 − 1/4 + 1/8 − 1/16 + ⋯ sums to 1/3.

The alternating harmonic series has a finite sum but the harmonic series does not.

The Mercator series provides an analytic expression of the natural logarithm:

\( \sum _{{n=1}}^{\infty }{\frac {(-1)^{{n+1}}}{n}}x^{n}\;=\;\ln(1+x). \)

The functions sine and cosine used in trigonometry can be defined as alternating series in calculus even though they are introduced in elementary algebra as the ratio of sides of a right triangle. In fact,

\( \sin x=\sum _{{n=0}}^{\infty }(-1)^{n}{\frac {x^{{2n+1}}}{(2n+1)!}}, \) and
\( \cos x=\sum _{{n=0}}^{\infty }(-1)^{n}{\frac {x^{{2n}}}{(2n)!}}. \)

When the alternating factor (–1)n is removed from these series one obtains the hyperbolic functions sinh and cosh used in calculus.

For integer or positive index α the Bessel function of the first kind may be defined with the alternating series

\( J_{\alpha }(x)=\sum _{m=0}^{\infty }{\frac {(-1)^{m}}{m!\,\Gamma (m+\alpha +1)}}{\left({\frac {x}{2}}\right)}^{2m+\alpha } \) where Γ(z) is the gamma function.

If s is a complex number, the Dirichlet eta function is formed as an alternating series

\( \eta(s) = \sum_{n=1}^{\infty}{(-1)^{n-1} \over n^s} = \frac{1}{1^s} - \frac{1}{2^s} + \frac{1}{3^s} - \frac{1}{4^s} + \cdots \)

that is used in analytic number theory.
Alternating series test
Main article: Alternating series test

The theorem known as "Leibniz Test" or the alternating series test tells us that an alternating series will converge if the terms an converge to 0 monotonically.

Proof: Suppose the sequence a n {\displaystyle a_{n}} a_{n} converges to zero and is monotone decreasing. If m is odd and m<n, we obtain the estimate \( {\displaystyle S_{n}-S_{m}\leq a_{m}} \) via the following calculation:

\( {\displaystyle {\begin{aligned}S_{n}-S_{m}&=\sum _{k=0}^{n}(-1)^{k}\,a_{k}\,-\,\sum _{k=0}^{m}\,(-1)^{k}\,a_{k}\ =\sum _{k=m+1}^{n}\,(-1)^{k}\,a_{k}\\&=a_{m+1}-a_{m+2}+a_{m+3}-a_{m+4}+\cdots +a_{n}\\&=\displaystyle a_{m+1}-(a_{m+2}-a_{m+3})-(a_{m+4}-a_{m+5})-\cdots -a_{n}\leq a_{m+1}\leq a_{m}.\end{aligned}}} \)

Since \( a_{n} \) is monotonically decreasing, the terms \( -(a_{m}-a_{{m+1}}) \) are negative. Thus, we have the final inequality: \( {\displaystyle S_{n}-S_{m}\leq a_{m}} \). Similarly, it can be shown that \( {\displaystyle -a_{m}\leq S_{n}-S_{m}} \). Since \( a_{{m}} \) converges to \( {\displaystyle 0} \), our partial sums \( S_m \) form a Cauchy sequence (i.e. the series satisfies the Cauchy criterion) and therefore converge. The argument for m even is similar.
Approximating sums

The estimate above does not depend on n. So, if \( a_{n} \) is approaching 0 monotonically, the estimate provides an error bound for approximating infinite sums by partial sums:

\( \left|\sum _{{k=0}}^{\infty }(-1)^{k}\,a_{k}\,-\,\sum _{{k=0}}^{m}\,(-1)^{k}\,a_{k}\right|\leq |a_{{m+1}}|. \)

Absolute convergence

A series \( \sum a_{n} \) converges absolutely if the series ∑ | a n | {\displaystyle \sum |a_{n}|} \sum |a_n| converges.

Theorem: Absolutely convergent series are convergent.

Proof: Suppose \( \sum a_{n} \) is absolutely convergent. Then, \( \sum |a_n| \) is convergent and it follows that \( \sum 2|a_{n}| \) converges as well. Since \( 0\leq a_{n}+|a_{n}|\leq 2|a_{n}|, the series ∑ ( a n + | a n | ) {\displaystyle \sum (a_{n}+|a_{n}|)} \sum (a_{n}+|a_{n}|) \)converges by the comparison test. Therefore, the series \( \sum a_{n} \) converges as the difference of two convergent series \( \sum a_{n}=\sum (a_{n}+|a_{n}|)-\sum |a_{n}|. \)

Conditional convergence

A series is conditionally convergent if it converges but does not converge absolutely.

For example, the harmonic series

\( \sum _{{n=1}}^{\infty }{\frac {1}{n}},\!

diverges, while the alternating version

\( \sum _{{n=1}}^{\infty }{\frac {(-1)^{{n+1}}}{n}},\!

converges by the alternating series test.

For any series, we can create a new series by rearranging the order of summation. A series is unconditionally convergent if any rearrangement creates a series with the same convergence as the original series. Absolutely convergent series are unconditionally convergent. But the Riemann series theorem states that conditionally convergent series can be rearranged to create arbitrary convergence.[1] The general principle is that addition of infinite sums is only commutative for absolutely convergent series.

For example, one false proof that 1=0 exploits the failure of associativity for infinite sums.

As another example, we know that

\( \ln(2)=\sum _{{n=1}}^{\infty }{\frac {(-1)^{{n+1}}}{n}}=1-{\frac {1}{2}}+{\frac {1}{3}}-{\frac {1}{4}}+\cdots . \)

But, since the series does not converge absolutely, we can rearrange the terms to obtain a series for \( {\frac {1}{2}}\ln(2): \)

\( {\begin{aligned}&{}\quad \left(1-{\frac {1}{2}}\right)-{\frac {1}{4}}+\left({\frac {1}{3}}-{\frac {1}{6}}\right)-{\frac {1}{8}}+\left({\frac {1}{5}}-{\frac {1}{10}}\right)-{\frac {1}{12}}+\cdots \\[8pt]&={\frac {1}{2}}-{\frac {1}{4}}+{\frac {1}{6}}-{\frac {1}{8}}+{\frac {1}{10}}-{\frac {1}{12}}+\cdots \\[8pt]&={\frac {1}{2}}\left(1-{\frac {1}{2}}+{\frac {1}{3}}-{\frac {1}{4}}+{\frac {1}{5}}-{\frac {1}{6}}+\cdots \right)={\frac {1}{2}}\ln(2).\end{aligned}} \)

Series acceleration

In practice, the numerical summation of an alternating series may be sped up using any one of a variety of series acceleration techniques. One of the oldest techniques is that of Euler summation, and there are many modern techniques that can offer even more rapid convergence.
See also

Grandi's series
Nörlund–Rice integral


Mallik, AK (2007). "Curious Consequences of Simple Sequences". Resonance. 12 (1): 23–37. doi:10.1007/s12045-007-0004-7.


Earl D. Rainville (1967) Infinite Series, pp 73–6, Macmillan Publishers.
Weisstein, Eric W. "Alternating Series". MathWorld.


Sequences and series

Arithmetic progression Geometric progression Harmonic progression Square number Cubic number Factorial Powers of two Powers of three Powers of 10

Advanced (list)

Complete sequence Fibonacci numbers Figurate number Heptagonal number Hexagonal number Lucas number Pell number Pentagonal number Polygonal number Triangular number

Fibonacci spiral with square sizes up to 34.
Properties of sequences

Cauchy sequence Monotone sequence Periodic sequence

Properties of series

Convergent series Divergent series Conditional convergence Absolute convergence Uniform convergence Alternating series Telescoping series

Explicit series

1/2 − 1/4 + 1/8 − 1/16 + ⋯ 1/2 + 1/4 + 1/8 + 1/16 + ⋯ 1/4 + 1/16 + 1/64 + 1/256 + ⋯ 1 + 1/2s+ 1/3s + ... (Riemann zeta function)


1 + 1 + 1 + 1 + ⋯ 1 + 2 + 3 + 4 + ⋯ 1 + 2 + 4 + 8 + ⋯ 1 − 1 + 1 − 1 + ⋯ (Grandi's series) Infinite arithmetic series 1 − 2 + 3 − 4 + ⋯ 1 − 2 + 4 − 8 + ⋯ 1 + 1/2 + 1/3 + 1/4 + ⋯ (harmonic series) 1 − 1 + 2 − 6 + 24 − 120 + ⋯ (alternating factorials) 1/2 + 1/3 + 1/5 + 1/7 + 1/11 + ⋯ (inverses of primes)

Kinds of series

Taylor series Power series Formal power series Laurent series Puiseux series Dirichlet series Trigonometric series Fourier series Generating series


Generalized hypergeometric series Hypergeometric function of a matrix argument Lauricella hypergeometric series Modular hypergeometric series Riemann's differential equation Theta hypergeometric series

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