uruz said:
Is this because there should not be any extra charge at where the real charge stands.
Well, why is the method of images ever applicable in the first place? It has to do with a certain uniqueness theorem right? Are all the conditions of that theorem satsfied if there are image charges in the region of interest?
Another issue that i can not handle is
How many image charges do i need to have?
You tell me. Like any physics problem, the best way to approach things is with a step by step process. Start by trying to find the image charge configuration needed to determine the potential outside the shell:
(1)Where are you allowed to place image charges?
(2)Where are the boundaries of the region you are interested in? What value do you want the potential to have on those boundaries?
(3)If there were no conducting shell (and no image charges yet), what would the potential be on those boundaries?
(4)Where could you place an image charge (and what magnitude would it need to be) so that the potential due to just Q1 and that image charge on those boundaries was zero?
(5)Where could you place an image charge (and what magnitude would it need to be) so that the potential on those boundaries do to just Q2 and that image charge was zero?
https://www.physicsforums.com/showthread.php?t=260107"
Here you say, the boundary conditions which are zero potential for both inner and outer surface can not be satisfied with only one charge.
That was a very different problem; he needed to find the potential in the region N<r<M. Unlike your problem, that region was not filled with a conducting material and so the potential wasn't zero there. He had to place image charges in the regions r<N and r>M in such a way that would make V(N)=V(M)=0, and it turns out that the only way to do that requires an
infinite number of charges...your problem is much simpler!