The Legendre Polynomials can be defined in many different ways and have several properties. Many of these can be found in books or in the net, but I couldn't find this one anywhere:
Prove that:
$$\frac{1}{2\pi} \int_0^{2\pi} \sum_{n = 0}^{+\infty} P_n(cos\phi)d\phi = \sum_{n = 0}^{+\infty} \lvert P_n(0) \rvert ^2.$$
Where $P_n(x)$ is the $n$-th Legendre Polynomial.
I put th "power series" as a tag because of the definition of the Legendre Polynomials: by definition this is their generating function: $ f(x) = \frac{1}{\sqrt{1 + a^2 - 2ax}}$
From looking at the first few $n$, it seems that in fact you don't need the sum:
$$ \dfrac{1}{2\pi} \int_0^{2\pi} P_n(\cos \phi)\; d\phi = P_n(0)^2 $$
where in fact for odd $n$, both sides are $0$.
The right sides are easy to find using Bonnet's recursion formula
$$ (n+1) P_{n+1}(x) = (2n+1) x P_n(x) - n P_{n-1}(x) $$
I'm not sure how best to get the left sides. In Maple you can use the generating function as follows:
$${\frac {4}{a+1}{\rm EllipticK} \left( 2\,{\frac {\sqrt {a}}{a+1}} \right) } $$
$$\sum _{k=0}^{\infty }2\,{\frac {\pi \, \left( \left( 2\,k \right) ! \right) ^{2}{16}^{-k}{a}^{2\,k}}{ \left( k! \right) ^{4}}} $$