Show that the Fourier series expansion for $f(x)$ is $$\frac2{\sqrt3}\left(\cos x-\frac{\cos5x}5+\frac{\cos7x}7-\frac{\cos11x}{11}+\cdots\right)$$ where $$f(x)=\begin{cases}\dfrac\pi3&\text{for }x\in\left[0,\dfrac\pi3\right)\\[1ex]0&\text{for }x\in\left[\dfrac\pi3,\dfrac{2\pi}3\right)\\[1ex]-\dfrac\pi3&\text{for }x\in\left[\dfrac{2\pi}3,\pi\right)\end{cases}$$ and $f(x)=f(x+\pi)$ for all $x\in\mathbb R$.
Attempt:
$$f(x)=\frac{a_0}2+\sum_{n\ge1}(a_n\cos2nx+b_n\sin2nx)$$
where
$$a_0=\frac2\pi\int_0^\pi f(x)\,\mathrm dx$$ $$a_n=\frac2\pi\int_0^\pi f(x)\cos2nx\,\mathrm dx$$ $$b_n=\frac2\pi\int_0^\pi f(x)\sin2nx\,\mathrm dx$$
I know that $f(x)$ is odd, so $a_0=0$ and $a_n=0$ for all $n\in\mathbb N$. For the sine series, I end up with, among several equivalent expressions,
$$b_n=\frac1{3n}\left(2-\cos\frac{2n\pi}3-\cos\frac{4n\pi}3\right)$$ $$b_n=\frac2{3n}\left(\sin^2\frac{2n\pi}3+\sin^2\frac{4n\pi}3\right)$$
which gives me (using $g$ to distinguish my result from the expected $f$)
$$g(x)=\sum_{n\ge1}\frac{c_n\sin2nx}n=\sin2x+\frac{\sin4x}2+\frac{\sin8x}4+\frac{\sin10x}5+\frac{\sin14x}7+\cdots$$
where $c_n=1$ if $n$ is not a multiple of $3$, and $0$ otherwise. Plotting the first few partial sums suggests that this answer is just as valid as the suggested one.
Is there some manipulation I can do to my result in order to get the solution to match? Or is there another way of finding the series expansion to arrive at the cosine series directly?
There is also a second part to the problem, which is to
Show that $$\frac\pi{2\sqrt3}=1-\frac15+\frac17-\frac1{11}+\cdots$$
which I can easily get from evaluating $f(x)$ and the given expansion at $x=0$:
$$\frac\pi3=\frac2{\sqrt3}\left(1-\frac15+\frac17-\frac1{11}+\frac1{13}-\frac1{17}+\frac1{19}-\frac1{23}+\cdots\right)$$
but I don't immediately see a way to use $g(x)$. At first glance, choosing $x=\dfrac\pi4$ seems to be the right thing to do, but this yields
$$\frac\pi3=1+\frac15-\frac17-\frac1{11}+\frac1{13}+\frac1{17}-\frac1{19}-\frac1{23}+\cdots$$


You need to make an even $2\pi$-periodic extension of the function $f$, that is, define $\tilde{f}$ such that
$$ \tilde{f}(-x) = \tilde{f}(x) $$
and
$$ \tilde{f}(x) = f(x) ~~~\mbox{for}~~ 0 < x < \pi $$
Since $\tilde{f}$ is periodic, the only Fourier coefficients that are not trivially zero are
$$ a_n = \frac{1}{2\pi}\int_{-\pi}^{\pi}{\rm d}x~\tilde{f}(x)\cos n x $$
After evaluating the integral you get $a_0 = 0$ and
$$ a_{n} = \frac{2}{3n}\left[\sin \frac{n\pi}{3} + \sin\frac{2n\pi}{3} -\sin n\pi \right] ~~~ n \ge 1 $$
Here's a reconstruction of the function with the 60 lowest modes $n \le 60$
$$ \tilde{f}(x) = \sum_{n\ge 1} a_n \cos nx $$
With this you can solve the second problem
$$ f(0) = \frac{\pi}{3} = \sum_{n\ge 1} a_n = \frac{2}{\sqrt{3}}\left[ 1 - \frac{1}{5} + \frac{1}{7} \cdots \right] $$
or equivalently
$$ \frac{\pi}{2\sqrt{3}} = 1 -\frac{1}{5} + \frac{1}{7} \cdots $$