Electric Potential of a Spherical Shell of Charge

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Homework Help Overview

The discussion revolves around the electric potential of a spherical shell of charge, particularly focusing on the effects of thickness in the shell and how it influences the electric potential both inside and outside the shell.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the implications of having a thick spherical shell versus a thin one, questioning how to treat the shell as a point charge at various distances from the shell. There is also discussion on the relationship between charge density and total charge in the context of calculating electric potential.

Discussion Status

Some participants have provided clarifications regarding the treatment of the shell as a point charge at distances greater than the outer radius and the constancy of potential inside the inner radius. Others have suggested the need for integration to find the electric field and potential in the region between the inner and outer radii, indicating a productive exploration of the topic.

Contextual Notes

Participants are considering the implications of charge density and total charge in their calculations, as well as the specific conditions under which the electric potential behaves differently based on the shell's thickness.

Polarbear
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Ok if you have a spherical shell of radius R with an even distribution of charge then outside the shell at a distance r where r>R I get that the shell can be treated as a point charge and inside the sphere (r<R) the electric potential will be constant.
All my notes cover when the shell has no thickness and I was thinking what happen if the spherical shell did have thickness (say inner radius a and outer radius b)? When r is greater then b can the shell still be treated as a point charge? How about when a<r<b?
 
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If the charge is uniformly distributed throughout the (nonconducting) shell:

(r > b) Treat as a point charge

(r < a) potential will be constant

(a < r < b) the field (and potential) will vary throughout this range; you'll need to integrate. (The field at a radius r depends only on the charge within that radius; the field is that of a point charge, but only the charge within r contributes to the field.)
 
Thanks for just clearing that up for me. I've managed to find a question on this (I'm getting practise in before mid-year exams) however it deals in terms of charge density. Is it just as simple as finding Q in terms of the sphere (volume of shell at such and such density).
 
Right. You should be able to work with either total charge Q or with the charge density. As an exercise, you might want to find the field as a function of radius for a uniform ball of charge density [itex]\rho[/itex].
 

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