Electrostatic energy of spherical shell.

In summary, the conversation discussed the determination of electrostatic energy for a spherical shell with uniformly distributed charge. Two methods were proposed: calculating potential and using the equation W = (1/2) * ∫σVda, and calculating electric field and using the equation W = (1/2) *εo ∫ E^2 dV. The final solution involved correcting a typo and adjusting the limits of integration.
  • #1
Fabio010
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0

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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  • #2
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?
 
  • #3
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?
 
  • #4
the integration must be from R to infinity,not from 0 to R.
 
  • #5
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.
 

1. What is the definition of electrostatic energy of a spherical shell?

The electrostatic energy of a spherical shell is the amount of potential energy stored in the electric field created by the distribution of charges on the surface of the shell.

2. How is the electrostatic energy of a spherical shell calculated?

The electrostatic energy of a spherical shell can be calculated using the equation U = Q^2/(4πεr), where U is the energy in joules, Q is the total charge on the shell in coulombs, ε is the permittivity of the surrounding medium, and r is the radius of the shell.

3. What is the relationship between the electrostatic energy and the charge on the spherical shell?

The electrostatic energy of a spherical shell is directly proportional to the square of the total charge on the shell. This means that as the charge on the shell increases, the electrostatic energy also increases.

4. How does the distance between the charges on a spherical shell affect the electrostatic energy?

The electrostatic energy of a spherical shell is inversely proportional to the distance between the charges on the shell. This means that as the distance between the charges increases, the electrostatic energy decreases.

5. What is the significance of the electrostatic energy of a spherical shell in physics?

The electrostatic energy of a spherical shell is important in understanding the behavior of electric charges and their interactions. It is also used in various applications, such as in the design of capacitors and in studying the stability of atomic nuclei.

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