Electrostatic Energy of a solid sphere with a cavity

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Homework Help Overview

The discussion revolves around calculating the electrostatic energy of a solid sphere with a cavity, focusing on the electric field and energy expressions derived from it. The subject area includes electrostatics and energy calculations in physics.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the use of the energy formula involving the electric field, questioning the applicability of derived expressions for different regions of space. There is a focus on boundary conditions and the correct formulation of the electric field in specified regions.

Discussion Status

The discussion is active, with participants sharing their findings and questioning the validity of their approaches. Some guidance has been offered regarding the regions of space to consider for the electric field, and there is an ongoing exploration of the correct expressions for the electric field in different regions.

Contextual Notes

Participants are considering three distinct regions for the electric field and are facing challenges with boundary conditions and the integration limits for calculating energy. There is an emphasis on ensuring the correct formulation of the electric field in the context of the problem.

Arman777
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Homework Statement
Determine the electrostatic energy U stored in the sphere
Relevant Equations
##W = ε_0/2 \int E^2d\tau## for all space
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I tried to use ##W = ε_0/2 \int E^2d\tau## for all space. So I find that ##E = \frac{(R^3 - b^3)\rho}{3ε_0r^2}## where ##\rho## is the charge denisty. So from here when I plug the equation I get something like

$$W = \frac{(R^3 - b^3)^2\rho^2 4 \ pi}{18ε_0} \int_{?}^{\inf}1/r^2dr$$

Is this approach correct ?

At this point I get stuck for the boundary conditions. If I put R I get something meaningless
 
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Arman777 said:
I tried to use ##W = ε_0/2 \int E^2d\tau## for all space.
OK
So I find that ##E = \frac{(R^3 - b^3)\rho}{3ε_0r^2}## where ##\rho## is the charge denisty.
For what region of space is this expression for E applicable? You have three distinct regions to consider.
 
TSny said:
OK
For what region of space is this expression for E applicable? You have three distinct regions to consider.
This is for ##r>R## so I have to also find ##E(r<b)##, ##E(b<r<R)## ?

Then The U will be,

$$U = \frac{(R^3 - b^3)^2\rho^2 4 \ pi}{18ε_0} \int_{R}^{\inf}1/r^2dr + \frac{e_0}{2} \int_{b}^{R}\frac{\rho (r - b^3)}{3ε_0}dr$$

Where ##E = \frac{\rho (r - b^3)}{3ε_0}, (b<r<R)##
 
I think the correct expression for the E-field for ##b<r<R## is $$E=\frac{\rho(r^3-b^3)}{3\epsilon_0r^2}$$.
 

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