How to Calculate the Work to Charge a Spherical Shell?

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Homework Help Overview

The problem involves calculating the work required to charge a spherical shell of radius R to a total charge Q. The context is within electrostatics, specifically focusing on the concepts of electric potential energy and work done in the presence of electric fields.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss various approaches to the problem, including the use of energy density of electric fields and the concept of integrating over space. There is also mention of using discrete point charges to derive expressions for continuous charge distributions. Some participants express uncertainty about the applicability of certain equations, particularly regarding the movement of test charges in electric fields.

Discussion Status

The discussion is active, with participants providing hints and alternative methods for approaching the problem. Some guidance has been offered regarding the integration of electric fields and potential energy, though there is no explicit consensus on a single method to solve the problem.

Contextual Notes

Participants note a lack of specific information in the textbook regarding energy density, which may affect their ability to apply certain concepts. There is also a reference to a previous thread on the same topic that did not yield a solution.

thirteen
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Homework Statement


Calculate the work that must be done to charge a spherical shell of radius [tex]R[/tex] to a total charge [tex]Q[/tex].
No diagram was provided.
(Another user posted the same question at https://www.physicsforums.com/showthread.php?t=109489, but there was no solution and the thread is ancient.)

Homework Equations


I'm not sure what equations are needed, so I'm just guessing here.
[tex]U = k_e\frac{q_1q_2}{r_{12}}[/tex]

[tex]W = -\Delta U[/tex]

[tex]V = k_e\frac{q}{r}[/tex] for a sphere

The Attempt at a Solution


I know the answer is [tex]\frac{k_eQ^2}{2R}[/tex] from the back of the book, but I don't know how to get it. I've reread the chapter and all the examples, but I can't find anything talking about energy with just one object. Everything deals with pairs or movement in a field. I thought about making up an identical sphere with charge [tex]-Q[/tex] next to the existing one and finding the change in potential energy. This gets me the right answer, but I doubt that this is a correct process.

Any help would be appreciated.
 
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You correctly said [tex]W = - \Delta U[/tex]. Also, keep in mind [tex]\Delta U = -q \int^{A}_{B} E dr[/tex]. Now you can find out what E equals and integrate
 
Hi thirteen,

There are several ways to approach this problem. Does your textbook have an expression for the energy density of an electric field? If so, you can integrate that expression over all space to find the energy.

Another approach is to think of the stored energy in a set of discrete point charges, and follow that idea to write out the correct expression for a continuous charge distribution.
 
cryptoguy said:
You correctly said [tex]W = - \Delta U[/tex]. Also, keep in mind [tex]\Delta U = -q \int^{A}_{B} E dr[/tex]. Now you can find out what E equals and integrate
Thanks, but I thought that equation was for the movement of a test charge q in a different field. I don't see how it can be used.

alphysicist said:
Hi thirteen,

There are several ways to approach this problem. Does your textbook have an expression for the energy density of an electric field? If so, you can integrate that expression over all space to find the energy.

Another approach is to think of the stored energy in a set of discrete point charges, and follow that idea to write out the correct expression for a continuous charge distribution.
Thanks, I'll look into the latter, since I don't have anything on energy density.
 
thirteen said:
Thanks, but I thought that equation was for the movement of a test charge q in a different field. I don't see how it can be used.

It can be used because that is essentially what you are doing: moving a charge from infinity to R against an electric field supplied by the charges you already moved. Another hint:
[tex]E = \frac{kq}{r^2}[/tex] so [tex]\Delta U = -q \int^{A}_{B} \frac{kq}{r^2} dr[/tex]. Integrate that from infinity to R.
 

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