Question on Electric Potential Energy

AI Thread Summary
The discussion centers on deriving the total electric potential energy of a uniformly charged solid sphere with radius R and charge density ρ. Participants suggest using concentric shells of charge to approach the problem, emphasizing the need to calculate the work done in bringing each shell from infinity to its position. Key equations involve the charge of the shell dq and the potential energy formula U = (kQq)/r, where integration is necessary to find the total energy. There is confusion regarding the integration process, particularly in substituting the volume and charge density into the equations. The conversation highlights the complexity of the problem and the need for careful consideration of the relationships between charge, volume, and energy.
Lewis
I can't get this question, can someone give me a hand? I will reprint the question below as it appears in the text:


A Solid sphere of radius R has a uniform charge density p(roh) and a total charge Q. Derive an expression for the total electric potential energy.(Suggestion: imagine that the sphere is constructed by adding successive layers of concentric shells of charge dq=[4(pi)r^2 dr)p and use dU=V dq)


I tried it a few times but I couldn't come up with a reasonable answer. Any help would be greatly appreciated. Thanks.
 
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Start with an initial point charge. The work required to bring that charge to that region of space is zero. Now bring in a new charged "shell" of thickness dr. How much work is required to put this shell of radius "r" and thickness "dr" outside the charge that is already there?

try changing the "dq" statement you're given into a "dr" statement: what's the volume of that shell?
 
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Ohhhh, that makes a lot of sense and I wasn't looking at it that way. I will go try that and report back with the result. Thank you kindly.
 
O.K. I tried that for a white, but I am still getting nowhere . Do I have to integrate dV first then integrate it again to get U?

For the dr statement you were talking about, I get either dr=dq/((4 PI r^2)p), or I can get dr=(r^2)/3 if I play around with dq=p dV. Can you offer me any more help? Thanks a lot!
 
Sorry, I was out.

Let's go straight to the source for EPE:

U=(kQq)/r [Q= one charge, q = other charge, k = 1/4pi epsilon]

You are integrating U from 0 to R.
For each successive shell of thickness dr, you are bringing in charge q "from infinity" to the previous volume of point charge Q.

the shell with thickness dr will have charge "dq" =(4 PI r^2)p dr [this is essentiall what you had.

dU will then be [(kQ)/r]dq
Q will be the volume of the sphere (that's already there when dq arrives) times charge density. Radius of the sphere and the shell are essentially "r"

you're going to get an integral that ends in "r^4 dr"
 
Aha! Now I see! Thank you very, very much. What a tricky question.

:)
 
lol Could you explain this one more time , sub in the volumex charge density for Q , then sub in the dq definition , which gives me a (4*p^2 *pi/3Eo) int r^4 dr , i know I am messing up somewhere , i just can't wrap my head around where.

thx for any help :)
 
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