What's the Fourier Series for ln(x)? I'm trying to see what the Fourier Series for ln(x) on $[0,\pi]$.
I plugged all of the formulas in for the coefficients into Wolfram Alpha and got this:
$$\ln(x)=\frac{\pi \ln(\pi)}{\pi}-\frac{2}{\pi}\sum_{n=1}^{\infty}\frac{\sin(nx)(\gamma - \operatorname{Ci(n\pi)}+\ln(n) +\cos(n\pi)\ln(n))}{n}+\frac{2}{\pi}\sum_{n=1}^\infty\frac{\cos(nx)( \ln(n)\sin(n\pi)-\operatorname{Si(n\pi)))}}{n}  $$ 
Is this correct? I find it odd that the Euler-Mascheroni constant appeared which leads me to believe it's incorrect. If it's incorrect, would someone give a hint for a set up that could help? Thanks!
 A: The series is correct. The coefficient of $\cos(nx)$ comes from $\int \cos(nx) \log(x)\,dx$, which, when integrated by parts, becomes 
$$
\int \frac{\sin(nx)}{x}\,dx 
$$
up to a constant. This is where the sine integral $\operatorname{Si}(n\pi)$ comes from in the formula for the cosine coefficient. 
The sine coefficients are a bit more complicated, because $\cos(nx)/x$ is not integrable on $[0, \pi]$. One has to offset the value at $0$ to get a convergent integral:
$$
\int \frac{1-\cos(nx)}{x}\,dx 
$$
But the cosine integral is still defined via $\cos(x)/x$ and not $(1-\cos(x))/x$. Specifically,
$${\displaystyle \operatorname {Ci} (x)=-\int _{x}^{\infty }{\frac {\cos t}{t}}\,dt=\gamma +\ln x+\int _{0}^{x}{\frac {\cos t-1}{t}}\,dt }
$$
Hence the presence of $\gamma$ and $\log$. One may say $\gamma$ is not really present in this Fourier series, it appears only to cancel out the $\gamma$ that's hidden inside of $\operatorname{Ci}(n\pi)$. If we defined the integral cosine by integrating $(1-\cos x)/x$, there would be no $\gamma$ there.
