Variable dielectric permitivity

lanwatch
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Homework Statement



The dielectric permitivity need not be a constant. Typically one can find problems where the permitivity varies, but always does so in the direction of the field. I came up with a problem that may (or may not) be solvable without the use of numerical methods.

Consider a spherical capacitor formed by two concentric spheres of radii 'a' and 'b'. The dielectric filling the volume between both spheres has permitivity given by

\varepsilon = \varepsilon_0 (2+\cos(\theta))

Find the capacity of the setup.

The Attempt at a Solution



Still at it, I am trying to decompose the dielectric in sections between two discrete θs and apply the constitutive equations, and then trying to reduce it to a PDE.
 
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welcome to pf!

hi lanwatch! welcome to pf! :smile:

(have an epsilon: ε and a theta: θ :wink:)

can't you treat it as lots of very thin capacitors in parallel, and integrate to find the total capacitance?
 
That was my first thought, but you need to prove before that the field is radial. To me that is not obvious...
 
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hi lanwatch! :smile:

(i'm very sorry i didn't reply earlier … somehow i lost this thread :redface:)
lanwatch said:
That was my first thought, but you need to prove before that the field is radial. To me that is not obvious...

but the electric displacement field (D) is unaffected by the dielectric, so that will be radial, and we are given that the permittivity is scalar, so the E electric field will always be parallel to the D field :wink:
 
To solve this, I first used the units to work out that a= m* a/m, i.e. t=z/λ. This would allow you to determine the time duration within an interval section by section and then add this to the previous ones to obtain the age of the respective layer. However, this would require a constant thickness per year for each interval. However, since this is most likely not the case, my next consideration was that the age must be the integral of a 1/λ(z) function, which I cannot model.
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