Consider the Fourier series of $\cos{\alpha x}$, considered as a function on $[-\pi,\pi]$ (yes, this is perverse): it satisfies the Dirichlet conditions, so on the interior, we have
$$ \cos{\alpha x} = \frac{1}{2}a_0+\sum_{k=1}^{\infty} a_k \cos{kx}, $$
where we find $a_k$ with the usual formula,
$$ a_k = \frac{1}{\pi}\int_{-\pi}^{\pi} \cos{\alpha x} \cos{kx} \, dx = \frac{(-1)^k 2\alpha\sin{\pi\alpha}}{\pi(\alpha^2-k^2)}, $$
by an easy calculation. Oh dear, now it's fairly obvious what's about to happen:
$$ \cos{\alpha x} = \frac{\sin{\pi\alpha}}{\pi \alpha}+\sum_{k=1}^{\infty} \frac{(-1)^k 2\alpha\sin{\pi\alpha}}{\pi(\alpha^2-k^2)} \cos{kx}. $$
Now set $x=0$ and multiply everything by $\pi/\sin{\pi \alpha}$. You can do the same thing for the cotangent by setting $x=\pi$.
To get from the cotangent to the cosecant, we go hunting for a trigonometric identity. Let's think about where the poles of each are: $\csc{\pi z}$ has poles at integers, as does $\cot{\pi z}$, but the residues alternate for the $\csc{\pi z}$. Therefore, can we make a linear combination of cotangents that has these poles? If you think for a few minutes, you come up with
$$ \cot{\tfrac{1}{2}\pi z}-\cot{\pi z}, $$
which it is easy to verify works:
$$ \frac{\cos{x}}{\sin{x}}-\frac{\cos{2x}}{\sin{2x}} = \frac{\cos{x}}{\sin{x}}-\frac{2\cos^2{x}-1}{2\sin{x}\cos{x}} = \frac{1}{2\sin{x}\cos{x}} = \csc{2x} $$
Now we just have to fiddle with the series expansions.
$$ \pi\cot{\tfrac{1}{2}\pi z}-\pi\cot{\pi z} = \frac{2}{z} + \sum_{n=1}^{\infty} \frac{z}{z^2/4-n^2}-\frac{1}{z} - \sum_{n=1}^{\infty} \frac{2z}{z^2-n^2} \\
=\frac{1}{z} + 2\sum_{n=1}^{\infty} \frac{2z}{z^2-(2n)^2} - \sum_{n=1}^{\infty} \frac{2z}{z^2-n^2}. $$
Ah, but hang on: the term with $n=2m$, even, in the second sum are half of the $m$th term of the first sum, whereas the odd terms have no corresponding terms. Hence the sums collapse into
$$ \pi\csc{\pi z} = \frac{1}{z}+2z\sum_{n=1}^{\infty} \frac{(-1)^n}{z^2-n^2}. $$