Evaluating $\int_0^{\large\frac{\pi}{4}} \log\left( \cos x\right) \, \mathrm{d}x $ It's my first  post here  and I was wondering  if someone  could help me with evaluating the
definite integral 
$$ \int_0^{\Large\frac{\pi}{4}} \log\left( \cos x\right) \, \mathrm{d}x $$
Thanks in advance, any help would be appreciated. 
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\begin{align}&\color{#66f}{\large\int_{0}^{\pi/4}\ln\pars{\cos\pars{x}}\,\dd x}
= \int_{-\pi/2}^{-\pi/4}\ln\pars{-\sin\pars{x}}\,\dd x = \int_{\pi/4}^{\pi/2}\ln\pars{\sin\pars{x}}\,\dd x
\\[5mm]&=\int_{\pi/4}^{\pi/2}\overbrace{\bracks{%
-\ln\pars{2} - \sum_{k\ =\ 1}^{\infty}{\cos\pars{2kx} \over k}}}^{\dsc{\ln\pars{\sin\pars{x}}}}\,\dd x
=-\,{1 \over 4}\,\pi\ln\pars{2}
-\sum_{k\ =\ 1}^{\infty}{1 \over k}\int_{\pi/4}^{\pi/2}\cos\pars{2kx}\,\dd x
\\[5mm]&=-\,{1 \over 4}\,\pi\ln\pars{2}
-\sum_{k\ =\ 1}^{\infty}{1 \over k}{\sin\pars{k\pi} - \sin\pars{k\pi/2} \over 2k}
=-\,{1 \over 4}\,\pi\ln\pars{2}
+\half\sum_{k\ =\ 1}^{\infty}{\sin\pars{k\pi/2} \over k^{2}}
\\[5mm]&=-\,{1 \over 4}\,\pi\ln\pars{2}
+\half\sum_{k\ =\ 0}^{\infty}{\sin\pars{k\pi + \pi/2} \over \pars{2k + 1}^{2}}
=-\,{1 \over 4}\,\pi\ln\pars{2}
+\half\ \underbrace{\sum_{k\ =\ 0}^{\infty}{\pars{-1}^{k} \over \pars{2k + 1}^{2}}}
_{\ds{\mbox{Catalan Constant}\ \dsc{G}}}
\\[5mm]&=\color{#66f}{\large-\,{1 \over 4}\,\pi\ln\pars{2} + \half\,G}
\end{align}
A: Write $$\log(\cos(x))=\log\left(\frac12 e^{ix}(1+e^{-2ix})\right)\\
=-\log 2 + ix +\sum_{k=1}^\infty\frac{(-1)^{k+1}}{k}e^{-2ikx}.$$
Then integrate term by term to obtain
$$\int_0^{\pi/4}\log(\cos(x))dx=-\frac{\pi}{4}\log 2 +i\frac{\pi^2}{32}+\frac{i}{2}\sum_{k=1}^\infty\frac{(-1)^{k+1}}{k^2}\left[e^{-ik\pi/2}-1\right].$$
The odd terms of the series with $e^{-ik\pi/2}$ give rise to the Catalan constant, and the even terms combine with the other infinite series to cancel the $i\pi^2/32$ term.
A: Let
$$
I=\int_0^{\Large\frac\pi4}\ln(\sin x)\ dx\qquad\text{and}\qquad J=\int_0^{\Large\frac\pi4}\ln(\cos x)\ dx
$$
then
\begin{align}
I+J&=\int_0^{\Large\frac\pi4}\ln(\sin x\cos x)\ dx\\
&=\int_0^{\Large\frac\pi4}\ln\left(\frac12\sin 2x\right)\ dx\\
&=\int_0^{\Large\frac\pi4}\ln(\sin 2x)\ dx-\int_0^{\Large\frac\pi4}\ln2\ dx\\
&=\frac12\int_0^{\Large\frac\pi2}\ln(\sin y)\ dy-\frac\pi4\ln2\qquad\color{red}{\Rightarrow}\qquad \text{set}\ y=2x\\
&=-\frac\pi2\ln2
\end{align}
and
\begin{align}
I-J&=\int_0^{\Large\frac\pi4}\ln\left(\frac{\sin x}{\cos x}\right)\ dx\\
&=\int_0^{\Large\frac\pi4}\ln\left(\tan x\right)\ dx\\
&=\int_0^{1}\frac{\ln t}{1+t^2}\ dt\qquad\color{red}{\Rightarrow}\qquad \text{set}\ t=\tan x\\
&=\int_0^{1}\sum_{n=0}^\infty(-1)^n t^{2n}\ln t\ dt\\
&=\sum_{n=0}^\infty(-1)^n\int_0^{1} t^{2n}\ln t\ dt\\
&=-\sum_{n=0}^\infty\frac{(-1)^n}{(2n+1)^2}\\
&=-G,
\end{align}
where $G$ is Catalan's constant. Therefore
$$
I=\int_0^{\Large\frac\pi4}\ln(\sin x)\ dx=-\frac12\left(G+\frac\pi2\ln2\right)
$$
and
$$
J=\int_0^{\Large\frac\pi4}\ln(\cos x)\ dx=\frac12\left(G-\frac\pi2\ln2\right).
$$

References :
$[1]\ \ \displaystyle\int_0^{\Large\frac\pi2}\ln(\sin y)\ dy=\int_0^{\Large\frac\pi2}\ln(\cos y)\ dy=-\frac\pi2\ln2$
$[2]\ \ \displaystyle\int_0^1 x^\alpha \ln^k x\ dx=\frac{(-1)^k k!}{(\alpha+1)^{k+1}}, \qquad\text{for }\  k=0,1,2,\ldots$
A: By the Fourier series of ln(cos x (https://math.stackexchange.com/a/1070809/732917)), we have
$ \begin{aligned}\ln (\cos x) &=-\ln 2+\sum_{n=0}^{\infty} \frac{(-1)^{n+1}}{n} \cos (2 n x) \\\int_{0}^{\frac{\pi}{4}} \ln (\cos x) d x &=-\frac{\pi}{4} \ln 2+\sum_{n=0}^{\infty} \frac{(-1)^{n+1}}{n} \int_{0}^{\frac{\pi}{4}} \cos 2 n x d x \\&=-\frac{\pi}{4} \ln 2+\sum_{n=0}^{\infty} \frac{(-1)^{n+1}}{n}\left[\frac{\sin 2 n x}{2 n}\right]_{0}^{\frac{\pi}{4}} \\&=-\frac{\pi}{4} \ln 2+\sum_{n=0}^{\infty} \frac{(-1)^{n+1}}{2 n^{2}}\left(\sin \frac{n \pi}{2}\right) \\&=-\frac{\pi}{4} \ln 2+\frac{1}{2} \sum_{n=0}^{\infty} \frac{(-1)^{n}}{(2 n+1)^{2}} \\&=-\frac{\pi}{4} \ln 2+\frac{G}{2},\end{aligned} \tag*{} $
$\textrm{where G is the Catalan's constant.}$
A: The integral:
$$S=\int_0^\frac{\pi}{4}\log(\cos(x))dx=\frac{1}{4}(2C-\pi \log 2)$$
where $C$ is the Catalan constant.
A: Since $\cos x =\sqrt{\frac{1+\cos 2x}{2}}$ so the integral is equal to $$\frac{1}{2}\int_0^{\frac{\pi}{4}}\log\left(\frac{1+\cos 2x}{2}\right)dx =-\frac{\pi}{8}\log(2)+\frac{1}{2}\int_0^{\frac{\pi}{4}}\log\left(1+\cos 2x \right) dx$$ substituting $2x=y$ gives us $$\frac{1}{4}\int_0^{\frac{\pi}{2}} \log(1+\cos y) dy$$ which the integral evaluated here and gives us $$-\frac{\pi}{8}\log(2)+\frac{1}{4}\left(2G-\frac{\pi}{2}\log(2)\right)=2G-\frac{\pi}{4}\log(2)$$
The result is straightforward if we use the generalized clausen function (see here)
$$\int_0^{\theta} \log(\cos y)dy =\frac{1}{2}\operatorname{Cl}_2\left(\pi -2\theta\right)-\theta \log(2)$$ or
$$\int_0^{\theta} \log(1+\cos y)dy=2\operatorname{Cl}_2\left(\pi -\theta \right)-\theta \log(2)$$
