The Legendre polynomials are the solutions of an important differential equation in Science, namely \begin{equation*} C(1-x^2)P-m_l^2P+(1-x^2)\frac{d}{dx}\left((1-x^2)\frac{dP}{dx}\right)=0. \end{equation*} Here C is a constant. For m_l=0 we obtain the Legendre polynomials as solutions, whereas m_l \ne 0 yields the so-called associated Legendre polynomials. This differential equation arises in for example the solution of the angular dependence of Schroedinger's equation with spherically symmetric potentials such as the Coulomb potential.