Variable dielectric permitivity

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Homework Help Overview

The discussion revolves around a problem involving a spherical capacitor with a variable dielectric permittivity described by the equation ε = ε₀(2 + cos(θ)). Participants are exploring the implications of this variable permittivity on the capacitance of the setup.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • The original poster attempts to decompose the dielectric into sections and apply constitutive equations, aiming to reduce the problem to a partial differential equation. Some participants question the assumption that the electric field is radial, noting that this is not immediately obvious.

Discussion Status

Participants are actively engaging with the problem, with some suggesting methods to approach the calculation of capacitance by treating the setup as multiple thin capacitors in parallel. There is a recognition of the need to establish the nature of the electric field before proceeding with certain assumptions.

Contextual Notes

There is an emphasis on the need to prove the radial nature of the electric field, which is seen as a critical step in the problem-solving process. The discussion reflects uncertainty regarding the implications of the variable dielectric on the electric field and displacement field.

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

[itex]\varepsilon = \varepsilon_0 (2+\cos(\theta))[/itex]

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.
 
Last edited:
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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...
 
Last edited:
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:
 

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