alternating series

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

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

$$1-\backslash frac\{1\}\{3\}+\backslash frac\{1\}\{5\}-\backslash ldots=\backslash sum\_\{n=0\}^\backslash infty\backslash frac\{(-1)^n\}\{2n+1\}$$

converges to $\backslash frac\{\backslash pi\}\{4\}$, but is not absolutely convergent.

The Mercator series provides an analytic power series expression of the natural logarithm, given by

$$\backslash sum\_\{n=1\}^\backslash infty\; \backslash frac\{(-1)^\{n+1\}\}\{n\}\; x^n\; =\; \backslash ln\; (1+x),\backslash ;\backslash ;\backslash ;|x|\backslash le1,$$

x\ne-1.

The functions sine and cosine used in trigonometry and introduced in elementary algebra as the ratio of sides of a right triangle can also be defined as alternating series in calculus.

$$\backslash sin\; x\; =\; \backslash sum\_\{n=0\}^\backslash infty\; (-1)^n\; \backslash frac\{x^\{2n+1\}\}\{(2n+1)!\}$$ and

$$\backslash cos\; x\; =\; \backslash sum\_\{n=0\}^\backslash infty\; (-1)^n\; \backslash frac\{x^\{2n\}\}\{(2n)!\}\; .$$

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

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

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

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

$$\backslash eta(s)\; =\; \backslash sum\_\{n=1\}^\{\backslash infty\}\{(-1)^\{n-1\}\; \backslash over\; n^s\}\; =\; \backslash frac\{1\}\{1^s\}\; -\; \backslash frac\{1\}\{2^s\}\; +\; \backslash frac\{1\}\{3^s\}\; -\; \backslash frac\{1\}\{4^s\}\; +\; \backslash cdots$$

that is used in analytic number theory.

{{main|Alternating series test}}

The theorem known as the "Leibniz Test" or the alternating series test states that an alternating series will converge if the terms {{math|a_n}} converge to 0 monotonically.

Proof: Suppose the sequence $a\_n$ converges to zero and is monotone decreasing. If $m$ is odd and

$$\backslash begin\{align\}$$

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\\

& = a_{m+1}-(a_{m+2}-a_{m+3}) - (a_{m+4}-a_{m+5}) - \cdots - a_n \le a_{m+1} \le a_{m}.

\end{align}

Since $a\_n$ is monotonically decreasing, the terms $-(a\_m\; -\; a\_\{m+1\})$ are negative. Thus, we have the final inequality: $S\_n\; -\; S\_m\; \backslash le\; a\_m$. Similarly, it can be shown that $-a\_m\; \backslash le\; S\_n\; -\; S\_m$. Since $a\_m$ converges to $0$, the partial sums $S\_m$ form a Cauchy sequence (i.e., the series satisfies the Cauchy criterion) and therefore they converge. The argument for $m$ even is similar.

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:

$$\backslash left|\backslash sum\_\{k=0\}^\backslash infty(-1)^k\backslash ,a\_k\backslash ,-\backslash ,\backslash sum\_\{k=0\}^m\backslash ,(-1)^k\backslash ,a\_k\backslash right|\backslash le\; |a\_\{m+1\}|.$$That does not mean that this estimate always finds the very first element after which error is less than the modulus of the next term in the series. Indeed if you take $1-1/2+1/3-1/4+...\; =\; \backslash ln\; 2$ and try to find the term after which error is at most 0.00005, the inequality above shows that the partial sum up through $a\_\{20000\}$ is enough, but in fact this is twice as many terms as needed. Indeed, the error after summing first 9999 elements is 0.0000500025, and so taking the partial sum up through $a\_\{10000\}$ is sufficient. This series happens to have the property that constructing a new series with $a\_n\; -a\_\{n+1\}$ also gives an alternating series where the Leibniz test applies and thus makes this simple error bound not optimal. This was improved by the Calabrese bound,{{Cite journal |last=Calabrese |first=Philip |date=March 1962 |title=A Note on Alternating Series |url=https://www.jstor.org/stable/2311056 |journal=The American Mathematical Monthly |volume=69 |issue=3 |pages=215–217 |doi=10.2307/2311056|jstor=2311056 }} discovered in 1962, that says that this property allows for a result 2 times less than with the Leibniz error bound. In fact this is also not optimal for series where this property applies 2 or more times, which is described by Johnsonbaugh error bound.{{Cite journal |last=Johnsonbaugh |first=Richard |date=October 1979 |title=Summing an Alternating Series |url=https://www.jstor.org/stable/2321292 |journal=The American Mathematical Monthly |volume=86 |issue=8 |pages=637–648 |doi=10.2307/2321292|jstor=2321292 }} If one can apply the property an infinite number of times, Euler's transform applies.{{cite arXiv |last=Villarino |first=Mark B. |date=2015-11-27 |title=The error in an alternating series |class=math.CA |eprint=1511.08568 }}

A series $\backslash sum\; a\_n$ converges absolutely if the series $\backslash sum\; |a\_n|$ converges.

Theorem: Absolutely convergent series are convergent.

Proof: Suppose $\backslash sum\; a\_n$ is absolutely convergent. Then, $\backslash sum\; |a\_n|$ is convergent and it follows that $\backslash sum\; 2|a\_n|$ converges as well. Since $0\; \backslash leq\; a\_n\; +\; |a\_n|\; \backslash leq\; 2|a\_n|$, the series $\backslash sum\; (a\_n\; +\; |a\_n|)$ converges by the comparison test. Therefore, the series $\backslash sum\; a\_n$ converges as the difference of two convergent series $\backslash sum\; a\_n\; =\; \backslash sum\; (a\_n\; +\; |a\_n|)\; -\; \backslash sum\; |a\_n|$.

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

For example, the harmonic series

$$\backslash sum\_\{n=1\}^\backslash infty\; \backslash frac\{1\}\{n\}$$

diverges, while the alternating version

$$\backslash sum\_\{n=1\}^\backslash infty\; \backslash frac\{(-1)^\{n+1\}\}\{n\}$$

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.{{cite journal |last1=Mallik |first1=AK |year=2007 |title=Curious Consequences of Simple Sequences |journal=Resonance |volume=12 |issue=1 |pages=23–37 |doi=10.1007/s12045-007-0004-7|s2cid=122327461 }} Agnew's theorem describes rearrangements that preserve convergence for all convergent series. 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, by Mercator series

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

But, since the series does not converge absolutely, we can rearrange the terms to obtain a series for $\backslash tfrac\; 1\; 2\; \backslash ln(2)$:

$$\backslash begin\{align\}$$

& {} \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{align}

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.

• Grandi's series
• Nörlund–Rice integral

{{reflist}}

• Earl D. Rainville (1967) Infinite Series, pp 73–6, Macmillan Publishers.
• {{MathWorld|title=Alternating Series|urlname=AlternatingSeries}}

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