Spherical Shell-Potential Energy, Energy density

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Homework Help Overview

The discussion revolves around the potential energy and energy density of a spherical shell, particularly focusing on the electric field both inside and outside a metallic sphere. Participants are exploring the implications of charge distribution and the integration limits for calculating potential energy.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the charge distribution on a metallic sphere and its implications for the electric field inside and outside the sphere. Questions are raised about the correct limits for integration when calculating potential energy and energy density. There is also exploration of the signs in the equations and the meaning behind them.

Discussion Status

The conversation is ongoing, with participants providing insights and questioning each other's reasoning. Some guidance has been offered regarding the integration limits and the interpretation of energy density, but no consensus has been reached on the final calculations or interpretations.

Contextual Notes

Participants are grappling with the implications of integrating from different limits, particularly from infinity to the radius of the sphere, and the associated signs in their calculations. There is a noted absence of volume charge density within the sphere, which influences the discussion on energy density.

Arman777
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Homework Statement


Shell.png


Homework Equations

The Attempt at a Solution


I fount these

Part(a)its ##E=\frac {ρa^3} {3ε_0}## and
##υ=\frac 1 2ε_0E^2##
Part (b)
##dU=4πr^2drυ##
Part (c)
##U=\int_0^a 4πr^2udr## but it gives me ##U=\frac {-Q^2} {8πε_0a}##

This"-" bothers me.
 
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Arman777 said:
Part(a)its ##E=\frac {ρa^3} {3ε_0}##
How is the charge Q distributed for a metallic sphere?
What is ##E## for points inside the sphere?
What is ##E## for points outside the sphere?

[EDIT: Note that your expression for ##E## does not have the correct dimensions for an electric field.]
##U=\int_0^a 4πr^2udr## but it gives me ##U=\frac {-Q^2} {8πε_0a}##

This"-" bothers me.
The "-" sign should bother you. Your integrand is positive (including the dr). So, the integral must be positive. But are you sure you want to integrate from 0 to ##a##? If you can answer my questions above, it should help you see what you should use for the range of integration.
 
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Likes   Reactions: Monci
Someone was faster :P
 
TSny said:
How is the charge Q distributed for a metallic sphere?
Just in surface
TSny said:
What is EEE for points inside the sphere?
E=0
TSny said:
What is EEE for points outside the sphere?
##E=\frac {ρa^3} {3ε_0r^2}## where ##r≥a## I know in the upside I forget ##r^2##
TSny said:
But are you sure you want to integrate from 0 to aaa?
What else it could be.. ?
Monci said:
The idea of the problem is that you bring the charge from infinity, since at infinity there is potential energy zero, while using a spherical distribution of charge. With this in mind, what should be the integration limits?
I thought about that but it still give me nothing...
I am thinking there should be minus cause I am thinking like bringing charges from ##r=0## to ##r=a## but I should bring charges ##r=∞## to ##r=a## but still there appears "-" sign also in ##r=∞## case what should I use the volume...? Or is it make sense ?
The result of integral will be ##U=Constant\int_∞^a\frac {1} {r^2}dr=constant\frac {-1} {r}## I can't get rid of "-".I think its cause of potential energy case.
 
Is it ##U=Constant\int_a^r\frac {1} {r^2}dr## where r goes to ∞ ?
 
Arman777 said:
Just in surface
So, all the charge Q is on the surface. So, there is no volume charge density ##\rho##.

E=0
Yes, ##E = 0## inside the sphere. So, what is the energy density inside the sphere? What would you get if you integrated the energy density over the volume of the inside of the sphere (##0<r<a##)?

##E=\frac {ρa^3} {3ε_0r^2}##
There is no volume charge density. For points outside the sphere, try to express E in term of Q and r.

I thought about that but it still give me nothing...
I am thinking there should be minus cause I am thinking like bringing charges from ##r=0## to ##r=a## but I should bring charges ##r=∞## to ##r=a## but still there appears "-" sign also in ##r=∞## case what should I use the volume...? Or is it make sense ?
The result of integral will be ##U=Constant\int_∞^a\frac {1} {r^2}dr=constant\frac {-1} {r}## I can't get rid of "-".I think its cause of potential energy case.
I'm not sure what you are doing here. Follow the outline given in the problem. How would you express the energy contained in a spherical shell of radius r and thickness dr?
 
TSny said:
Yes, E=0E=0E = 0 inside the sphere. So, what is the energy density inside the sphere? What would you get if you integrated the energy density over the volume of the inside of the sphere (0<r<a0<r<a0
Zero ?
##E=\frac {Q} {4πε_0r^2}##
##dU=4πr^2drυ##
 
Arman777 said:
Zero ?
##E=\frac {Q} {4πε_0r^2}##
##dU=4πr^2drυ##
Yes Yes Yes
 
TSny said:
Yes Yes Yes
soo?
 
  • #10
Arman777 said:
soo?
What is preventing you from finishing the problem?
 
  • #11
TSny said:
What is preventing you from finishing the problem?
Limits of integral
 
  • #12
Arman777 said:
Limits of integral
You need to add up the energy in every spherical shell for which ##E \neq 0##.
 
  • #13
from a to ∞ ?
 
  • #14
TSny said:
You need to add up the energy in every spherical shell for which ##E \neq 0##.
a to ∞ ?
 
  • #15
Arman777 said:
a to ∞ ?
Yes
 
  • #16
TSny said:
Yes
İnteresting... ok thanks a lot
 
  • #17
Arman777 said:
İnteresting... ok thanks a lot
Yes, it is very interesting. The potential energy stored in the system can be thought of as stored in the field that extends from the surface of the sphere all the way out to infinity!
 
  • #18
TSny said:
Yes, it is very interesting. The potential energy stored in the system can be thought of as stored in the field that extends from the surface of the sphere all the way out to infinity!
Thats just amazing...
 
  • #19
I used gaussian law and surface charge density etc to find E
 
  • #20
Arman777 said:
I used gaussian law and surface charge density etc to find E
OK
 

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