Am I correct in thinking that the steady state solution for U(r,theta)
can be computed as the sum of the N Green's functions corresponding to
the sources (with the b.c. U(a,theta) = 0) and the Poisson's integral
formula corresponding to the boundary function f?
Thanks.
Delta u(i) = f(i) on D , u=0 on \partial D i=1,..,N
f(i) representing the source terms
Delta u(N+1) = 0 on D , u=f on \partial D
let
v= sum_{i=1,...,N+1} u(i)
=>
Delta v = sum_{i=1,..,N} f(i) on D, v=f on \partial D
hth
peter
Thanks Peter, I was fairly sure, just wanted confirmation.