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A parallel-plate capacitor is made using two circular plates of radius a, with the bottom plate on the xy plane, centered at the origin. The top plate is located at z = d, with its center on the z axis. Potential is on the top plate; the bottom plate is grounded. Dielectric having radially dependent permittivity fills the region between plates. The permittivity is given by Find (a)V(z); (b) E; (c) Q; (d)C.
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We have learned in the Problem 6.36. that even if the permittivity varies in space, the Poisson equation is still valid if permittivity varies in a direction perpendicular to the electric field. That is the case here, so we can start with the Laplace equation (since ):
The solution that satifies the boundary conditions is a simple linear function:
The electric field is the negative gradient of the potential:
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