Conducting Sphere Covered By Spherical Dielectric

AI Thread Summary
The discussion centers on calculating the polarization charge density for a metal sphere covered by a dielectric layer. The electric field outside the sphere, without the dielectric, is given by E = kQ/r^2, but the dielectric's effect must be considered. The dielectric behaves like a capacitor, leading to a modified electric field for the region between the sphere and the dielectric. The charge on the inner surface of the dielectric is expressed as q' = σ_inner * 4πa^2, which is crucial for determining the inner and outer surface charge densities. The participant seeks clarification on how to derive the charge densities correctly.
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Homework Statement



An isolated metal sphere of radius a has a free charge Q on its surface. The sphere is covered with a dielectric layer with inner radius a and outer radius b

Calculate the polarization charge density on the inside and outside of the dielectric.

Homework Equations





The Attempt at a Solution


So I know that the electric field outside of the conducting sphere w/o dielectric is:

E = \frac{k Q}{r^2}

This field however, should have the electric field due to the dielectric subtracted from it.

If we can regard the dielectric as a capacitor since it has an equal amount of polarized charge on its inner and outer surfaces, the electric field for a < r < b should be:

E = \frac{k q&#039;}{r^2} where q'=charge on inner surface of dielectric

the charge on the inner surface should just be

q&#039; = \sigma_{inner} 4 \pi a^2


now I know I want \sigma_{inner}, and then it would be simple to find \sigma_{outer}, but I am not really sure how to solve for it
 
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