How can the following integral be evaluated for x^2<1?

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Discussion Overview

The discussion centers around evaluating the integral \(\int_0^{2\pi}\ln(1 + x^2 - 2x\cos\theta)d\theta\) for the condition \(x^2 < 1\). Participants explore various methods and substitutions to understand why the integral evaluates to zero under this condition.

Discussion Character

  • Exploratory
  • Mathematical reasoning
  • Technical explanation

Main Points Raised

  • One participant suggests that the integral evaluates to zero for \(x^2 < 1\) but is unsure of the reasoning behind it.
  • Another participant proposes a change of variable to \(u = x^2 - 2x\cos\theta\) to facilitate the evaluation.
  • A participant expresses difficulty in making the substitution bijective and considers using symmetry to simplify the integral.
  • One participant mentions that Mathematica failed to evaluate the integral analytically but suggests that plotting the function supports the claim that the integral is zero for \(x^2 < 1\).
  • Another participant notes that Mathematica provided an answer of zero when given specific assumptions about \(x\) and discusses a vector interpretation related to the law of cosines.
  • A later reply presents a series expansion approach using \(\ln(1 - t)\) and shows a detailed calculation leading to the conclusion that the integral evaluates to zero.
  • One participant expresses appreciation for the series method and acknowledges its effectiveness.

Areas of Agreement / Disagreement

Participants generally agree that the integral evaluates to zero for \(x^2 < 1\), but the reasoning and methods to arrive at this conclusion are debated and explored without a definitive consensus on a single approach.

Contextual Notes

Some participants note challenges in making substitutions bijective and the complexity of the integral, indicating that the discussion involves unresolved mathematical steps and assumptions.

meichenl
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The following integral came up in a paper I was reading recently.

\int_0^{2\pi}\ln(1 + x^2 - 2x\cos\theta)d\theta

The answer, for x^2<1, is zero. I'm not sure why. I tried writing it as a power series and showing that the integral for any given power of x vanishes, but it got too messy to work through. Anyone have a trick?
 
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hint change variable to
u=x^2-2x cos(theta)
 
lurflurf, thank you for your reply, but I am still stuck. To make the substitution you suggest, I need to be able to completely eliminate theta, so:

<br /> u = x^2 - 2x\cos\theta \vspace{10mm}

<br /> du = 2x\sin\theta d\theta

<br /> d\theta = \frac{du}{2x\sin\theta}

<br /> \frac{u - x^2}{-2x} = \cos\theta

<br /> \frac{u^2 - 2ux^2 + x^4}{4x^2} = 1-\sin^2\theta

<br /> \sin\theta = \sqrt{1-\frac{u^2 - 2ux^2 + x^4}{4x^2}}

<br /> d\theta = \frac{du}{2x \sqrt{1-\frac{u^2 - 2ux^2 + x^4}{4x^2}}}<br />

I can't quite put this in the original problem yet, because the substitution is not bijective. There are multiple theta values over the range of the original integral that correspond to the same u value. I could split the integral into different pieces, or use the symmetry of the cosine function to play with the limits of integration before making any substitution, as I do below.

<br /> \int_0^{2\pi} \ln(1+x^2 - 2x\cos\theta)d\theta = 2\int_0^\pi \ln(1+x^2 - 2x\cos\theta)d\theta<br /> =2\int_{x^2 - 2x}^{x^2+2x} \ln(1+u) \frac{du}{2x \sqrt{1-\frac{u^2 - 2ux^2 + x^4}{4x^2}}}<br />

Perhaps I'm missing something or made a mistake, but it doesn't look inviting from there.
 
I had Mathematica attempt to evaluate the integral analytically, but it failed. Plotting the function, it certainly looked plausible that for x^2<1 the integral evaluates to zero, and it's not really crucial for my research that I understand exactly why this works, but I am interested in how to do it, if anyone has a good method handy. The integral does appear in tables, but I didn't find an explanation of where the answer comes from.
 
Mathematica seemed to be happy with Integrate[Log[1 + x^2 - 2 x Cos[theta]], {theta, 0, 2 Pi}, Assumptions -> x > 0 && x < 1]: it gave an answer of zero. I'm thinking about how one could actually perform the integral; note that 1 + x^2 - 2x cos \theta = \lvert 1 - xe^{i\theta} \rvert^2.
 
Last edited:
adrian,

you're right - thank you. mathematica just took a minute or so to do it, and i wasn't very patient.

you're also right about the vector interpretation. the argument of the natural log is essentially coming from the law of cosines.
 
Well, I think I found something that works, based on the series
\ln(1 - t) = - \sum_{n = 1}^{\infty} \frac{t^n}{n}, \lvert t \rvert &lt; 1.

Here goes:
<br /> \begin{split}<br /> \int_{0}^{2\pi} \ln(1 + x^2 - 2x \cos \theta) \,d\theta<br /> &amp;= \int_{0}^{2\pi} \ln \lvert 1 - xe^{i\theta} \rvert^2 \,d\theta \\<br /> &amp;= \int_{0}^{2\pi} \ln \left[(1 - xe^{i\theta})(1 - xe^{-i\theta})\right] \,d\theta \\<br /> &amp;= \int_{0}^{2\pi} \ln (1 - xe^{i\theta}) + \ln (1 - xe^{-i\theta}) \,d\theta \\<br /> &amp;= - \int_{0}^{2\pi} \sum_{n = 1}^{\infty} \frac{(xe^{i\theta})^n}{n} + \sum_{n = 1}^{\infty} \frac{(xe^{-i\theta})^n}{n} \,d\theta \text{\quad if $\lvert x \rvert &lt; 1$} \\<br /> &amp;= - \sum_{n = 1}^{\infty} \frac{x^n}{n} \int_{0}^{2\pi} e^{in\theta} + e^{-in\theta} \,d\theta \\<br /> &amp;= 0.<br /> \end{split}<br />
 
Last edited:
adrian - that's pretty cool. thanks!
 

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