Paper 1, Section II, D

Methods
Part IB, 2014

(a) Legendre's differential equation may be written

(1x2)d2ydx22xdydx+n(n+1)y=0,y(1)=1\left(1-x^{2}\right) \frac{d^{2} y}{d x^{2}}-2 x \frac{d y}{d x}+n(n+1) y=0, \quad y(1)=1

Show that for non-negative integer nn, this equation has a solution Pn(x)P_{n}(x) that is a polynomial of degree nn. Find P0,P1P_{0}, P_{1} and P2P_{2} explicitly.

(b) Laplace's equation in spherical coordinates for an axisymmetric function U(r,θ)U(r, \theta) (i.e. no ϕ\phi dependence) is given by

1r2r(r2Ur)+1r2sinθθ(sinθUθ)=0\frac{1}{r^{2}} \frac{\partial}{\partial r}\left(r^{2} \frac{\partial U}{\partial r}\right)+\frac{1}{r^{2} \sin \theta} \frac{\partial}{\partial \theta}\left(\sin \theta \frac{\partial U}{\partial \theta}\right)=0

Use separation of variables to find the general solution for U(r,θ)U(r, \theta).

Find the solution U(r,θ)U(r, \theta) that satisfies the boundary conditions

U(r,θ)v0rcosθ as rUr=0 at r=r0\begin{aligned} &U(r, \theta) \rightarrow v_{0} r \cos \theta \quad \text { as } r \rightarrow \infty \\ &\frac{\partial U}{\partial r}=0 \quad \text { at } r=r_{0} \end{aligned}

where v0v_{0} and r0r_{0} are constants.