Write down the general form of the solution in polar coordinates (r,θ) to Laplace's equation in two dimensions.
Solve Laplace's equation for ϕ(r,θ) in 0<r<1 and in 1<r<∞, subject to the conditions
ϕ→0 as r→0 and r→∞ϕ∣r=1+=ϕ∣r=1− and ∂r∂ϕ∣∣∣∣∣r=1+−∂r∂ϕ∣∣∣∣∣r=1−=cos2θ+cos4θ.