Electrostatic energy of spherical shell.

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Homework Help Overview

The problem involves determining the electrostatic energy of a spherical shell with a uniform charge distribution. Participants are discussing two methods for calculating the energy, one involving potential and the other involving electric field calculations.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore two methods for calculating electrostatic energy: using potential and using electric field. There are attempts to clarify the integration limits and the constants involved in the calculations. Some participants question the consistency of results between the two methods.

Discussion Status

The discussion is active, with participants providing insights and questioning each other's calculations. There is a focus on clarifying the integration limits and the interpretation of constants in the equations. Some guidance has been offered regarding the integration process.

Contextual Notes

There are mentions of potential typos and assumptions regarding the electric field inside the shell being zero. The integration limits are under scrutiny, with suggestions that they should extend from R to infinity rather than from 0 to R.

Fabio010
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Homework Statement



Determine the electrostatic energy, W, of a spherical shell of radius R with total charge q, uniformly distributed. Compute it with the following methods:

a) Calculate the potential V in spherical shell and calculate the energy with the equation:

W = (1/2) * ∫σVda

b) Calculate the electric field inside and outside, and calculate the energy with the equation:

W = (1/2) *εo ∫ E^2 dV




The Attempt at a Solution



a)
Electric filed inside = 0


Electric field outside = (1/4piεo) * Q/r^2


The Potential is v(r)-v(infinity) = - ∫(infinity to R) (Electric field outside) dr

= (1/4piεo) * Q/R

W = (1/2) * ∫σVda


because dq = σda

W = (1/2) * ∫(1/4piεo) * q/R * dq = (1/8piεo) * Q^2/R


b) The electric field is already calculated...


W = (1/2) *εo ∫ E^2 dV

= (1/2) *εo ∫ (1/16pi^2εo^2) * q^2/r^4 dV

(1/2) *εo ∫(0 to 2pi) ∫(0 to pi) ∫ (0 to R ) [(1/16pi^2εo^2) * q^2/r^4 ] * r^2 sinθ dr dθ dβ


= -(1/8piεo) * Q^2/R




The problem is, the difference in the signal...isn't it supposed to be equal??
 
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Fabio010 said:
W = (1/2) * ∫σVda

because dq = σda

W = (1/2) * ∫(1/4piεo) * q/R * dq = (1/8piεo) * Q^2/R

You undid the simplification that was made for you :)
W = 1/2 ∫ V dq = 1/2 ∫ σV da

The q inside your integral is the constant Q, not little q that varies, but I think you made a typo since the constants are still right.
b) The electric field is already calculated...W = (1/2) *εo ∫ E^2 dV

= (1/2) *εo ∫ (1/16pi^2εo^2) * q^2/r^4 dV

(1/2) *εo ∫(0 to 2pi) ∫(0 to pi) ∫ (0 to R ) [(1/16pi^2εo^2) * q^2/r^4 ] * r^2 sinθ dr dθ dβ

Didn't you say in part a that the E field inside the sphere was everywhere 0?
 
aralbrec said:
You undid the simplification that was made for you :)
W = 1/2 ∫ V dq = 1/2 ∫ σV da

The q inside your integral is the constant Q, not little q that varies, but I think you made a typo since the constants are still right.




Didn't you say in part a that the E field inside the sphere was everywhere 0?


So the energy is zero?
 
the integration must be from R to infinity,not from 0 to R.
 
andrien said:
the integration must be from R to infinity,not from 0 to R.

yeh, it makes sense. And the result is positive.

Thanks for the help.
 

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