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How to prove

$$\int\limits_{-\pi}^{\pi}{\log^2{(\cos{\frac{x}{2})}}dx} = 2\pi\log^2{2} + \frac{\pi^3}{6}$$

I got this result using Fourier representation of $$|\log(\cos(\frac{x}{2}))|$$ and Parseval's identity. But I am wondering if there is a direct way to calculate this integral.

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  • $\begingroup$ Confirmed by Mathematica. $\endgroup$ – David G. Stork Oct 30 at 17:01
  • $\begingroup$ You may find some answers here or here $\endgroup$ – Paul Enta Oct 30 at 17:46
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    $\begingroup$ @PaulEnta I believe those are rather circular because they use Fourier series. $\endgroup$ – Parcly Taxel Oct 30 at 18:13
  • $\begingroup$ These answers 1, 2, 3, 4 don't use Fourier series. $\endgroup$ – Paul Enta Oct 30 at 18:49
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With $t= \frac x2$

\begin{align} I& = \int\limits_{-\pi}^{\pi}{\log^2{(\cos{\frac{x}{2})}}dx}\\ &= 4\int_0^{\frac\pi2}\ln^2 (\cos t) dt= 2\int_0^{\frac\pi2}(\ln^2 (\cos t)+ \ln^2 (\sin t) )dt \\ &=\int_0^{\frac\pi2}\left( \ln^2 (\sin t\cos t) + \ln^2 \frac{\sin t}{\cos t} \right)dt =J+K\tag1 \end{align} where \begin{align} J &= \int_0^{\frac\pi2}\ln^2 (\sin t\cos t) dt \overset{2t\to t}= \frac12 \int_0^{\pi}\ln^2 (\frac12\sin t)dt= \int_0^{\frac\pi2}\ln^2 (\frac12\sin t)dt\\ &= \int_0^{\frac\pi2}\left( \ln^2 2 -2\ln2 \ln\sin t +\ln^2(\sin t ) \right)dt\\ &= \frac\pi2\ln^22 -2\ln 2(-\frac\pi2\ln2) +\int_0^{\frac\pi2}\ln^2(\sin t )dt = \frac{3\pi}2\ln^22 +\frac14I\\ K&=\int_0^{\frac\pi2} \ln^2 (\frac{\sin t}{\cos t}) dt\overset{u=\tan t}= \int^\infty_0 \frac{\ln^2 u} {1+u^2} du=\frac{\pi^3}8 \end{align} Plug $J$ and $K$ into (1) to obtain

$$I = 2\pi\ln^22 +\frac{\pi^3}6$$

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Let us write $$I=\int_{-\pi}^{\pi} \ln^2(\cos(x/2)) dx=4\int_{0}^{\pi/2} \ln^2 \cos y dy$$ Let $\cos y=t$, then $$I=4\int_{0}^{1} \frac{ln^2 t}{\sqrt{1-t^2}} dt =4\int_{0}^{1} \sum_{k=0}^{\infty} \ln^2 t ~ C_k ~(-1)^k~t^{2k} dt, C_k={-1/2,\choose k}$$ Let $t=e^{-u}$, then $$I=4\int_{0}^{1}\sum_{k=0}^{\infty} (-1)^k C_k u^2 e^{-(2k+1)u} =8\sum_{k=0}^{\infty} \frac{(-1)^k ~ C_k}{(2k+1)^3}$$

I may get back.

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In my favorite CAS is has two identic forms integrate in the sense of an unbounded general integral. I can only do screenshots because the MathML is ill-posed. This can be looked up in books with integreal relationsships and representations like Abramovitch, Stegun.

First a longer one:

integral

Now are either integration done automatically or looked up in formula collections.

Evaluating this at the limits of the given integral is:

+∞

doubly singular. The signs do not change for -/+ πœ‹. So the limits have to be taken. These are not too easy and need complex theory and residue methodology.

The problem gets simpler with the substitution t=x/2 and the knowledge that the function is even.

with the substitution t=x/2

For t=0 and t=πœ‹/2 the term is positive ∞.

This is the graph of the function of the question:

graph of the function

With the substitution z=Cos[t] from @z-ahmed we get something even easier:

even easier representation

The process path can be gone in this direction and reverse. Mind the minus sign.

Our limit for z->0 is now 0.

The limit for z->1 is 1/24 πœ‹ (πœ‹^2 + 3 Log5^2)

We remember our factor 4.

So the result is

result.

This can be simplified with 4 Log[2]^2 - Log[4]^2==0.

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