The configuration of Problem 3.12 is modified by placing a conducting plane held at zero potential parallel to and a distance L away from the plane with the disc insert in it. For definiteness put the grounded plane at z=0 and the other plane with the center of the disc on the z axis at z=L.
(a) Show that the potential between the planes can be written in cylindrical coordinates (z,ρ,ϕ) as
Φ(z,ρ)=V∫0∞dλJ1(λ)J0(λρ/a)sinh(λL/a)sinh(λz/a)
(b) Show that in the limit a→∞ with z, ρ, L fixed the solution of part a reduces to the expected result. Viewing your result as the lowest order answer in an expansion in powers of a−1, consider the question of corrections to the lowest order expression if a is large compared to ρ and L, but not infinite. Are there difficulties? Can you obtain an explicit estimate of the corrections?
(c) Consider the limit of L→∞ with (L−z), a and ρ fixed and show that the results of Problem 3.12 are recovered. What about corrections for L≫a, but not L→∞?