Average field inside spherical shell of charge

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SUMMARY

The average electric field inside a spherical shell of non-uniform charge density can be analyzed using the dipole moment of the charge distribution. If the non-uniform density maintains spherical symmetry, the average field can be computed by considering the contributions of elemental charges on the sphere's surface. The discussion highlights the application of the dipole momentum approach for a shell with a radius slightly larger than the shell itself, specifically when dealing with a double polarity charge density represented as ## \sigma = A \cos{\theta} ##.

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chimay
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TL;DR
Calculation of the electric field inside a spherical shell of charge with non-uniform density
A known result is that the average field inside a sphere due to all the charges inside the sphere itself is proportional to the dipole momentum of the charge distribution (see, for example, here).

I wonder whether the same result can be applied in the case of a spherical shell of non-uniform charge density. Is there any result about the average electric field inside the shell?
 
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chimay said:
I wonder whether the same result can be applied in the case of a spherical shell of non-uniform charge density. Is there any result about the average electric field inside the shell?
It depends on whether the non-uniform density is still spherically symmetrical.
 
Can't you answer the question with two point charges at different locations plus superposition?
 
Thank you both of you for your replies. I understand it is a matter to average the contribution of each elemental charge on the sphere surface and then sum all of them, but I am not able to go through all the calculations. For that reason, I was thinking to apply the result that I mentioned in my first post to a sphere with radius slightly larger than that of the spherical shell, let's say $$ R_{sphere} = R_{shell} + \Delta R $$ with ##\Delta R \rightarrow 0##. In this case I would get, again, that I can compute the average field inside the shell by computing the dipole momentum of the shell. Am I correct?

From a practical standpoint, I am working with a double polarity charge density. Let's say something like ## \sigma = A \cos{\theta} ##, to fix the ideas.PS: It seems I am not able to render the latex code in my reply. Can you render it correctly or did I make anything wrong?
 

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