Electric Potential of two conductors

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Homework Help Overview

The problem involves a hollow spherical conducting shell surrounding a solid conducting sphere, with specific charges assigned to each. The goal is to find the potential difference from infinity to the surface of the sphere.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of Gauss's law and the potential difference between various regions, including the inside and outside of the shell. There are attempts to express the electric field and potential using relevant equations.

Discussion Status

Some participants have suggested using Gauss's law to determine the electric field outside the shell and compute the potential difference. Others have noted the lack of potential difference between the inside and outside of the shell, indicating a productive exploration of the problem.

Contextual Notes

There is mention of uncertainty regarding the need for calculus in the solution process, as well as the implications of the charges on the surfaces of the conductors. Participants are also considering the effects of the inner sphere on the overall electric field.

jesuslovesu
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Homework Statement


A hollow spherical conducting shell of inner radius b and outer radius c surrounds its concentric with a solid conducting sphere of radius a. The sphere carries a net charge -Q. The shell carries net +3Q. Find an expression for the potential difference from infinity to the surface of the sphere.
http://img185.imageshack.us/img185/3596/rabbitatesthekv2.th.jpg
Sorry it's a little cut off, but you get the idea.

Homework Equations


V = kq/r

The Attempt at a Solution


Well, I'm not quite sure if I need to use calculus or Gauss's law or what. The best so far that I've been able to come up with is V1 = k(-Q)/a, V2 = k(3Q)/(c-b)

I know that if the inner sphere were not there, then the electric field would be zero inside the shell.
If I recall correctly from the last chapter I had, the outside surface of the shell will be charged at +2q and the inner surface of the shell will be at q
 
Last edited by a moderator:
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jesuslovesu said:

Homework Statement


A hollow spherical conducting shell of inner radius b and outer radius c surrounds its concentric with a solid conducting sphere of radius a. The sphere carries a net charge -Q. The shell carries net +3Q. Find an expression for the potential difference from infinity to the surface of the sphere.
http://img185.imageshack.us/img185/3596/rabbitatesthekv2.th.jpg
Sorry it's a little cut off, but you get the idea.

Homework Equations


V = kq/r


The Attempt at a Solution


Well, I'm not quite sure if I need to use calculus or Gauss's law or what. The best so far that I've been able to come up with is V1 = k(-Q)/a, V2 = k(3Q)/(c-b)

I know that if the inner sphere were not there, then the electric field would be zero inside the shell.
If I recall correctly from the last chapter I had, the outside surface of the shell will be charged at +2q and the inner surface of the shell will be at q

Use Gauss' Law. That will give you the field outside the outer sphere, which is a function of the net enclosed charge.

AM
 
Last edited by a moderator:
To extend Andrew's suggestion, there is no potential difference between the outside of the shell and the inside of the shell. So just pick up the same game inside the shell. Compute the potential difference between the surface of the sphere and the inside of the shell and add it to the outside.
 
Will it be something like this:

Using Gauss's Law,

E=k2q/r^r for r>c. E=-dv/dr, integrating this from inf to r, and that's your potential?
 
chaoseverlasting said:
Will it be something like this:

Using Gauss's Law,

E=k2q/r^r for r>c. E=-dv/dr, integrating this from inf to r, and that's your potential?
Yes. Gauss' law will give you the enclosed charge:

[tex]\phi = \oint E\cdot dA = \frac{q_{encl}}{\epsilon_0}[/tex]

By symmetry, E is uniform over a gaussian sphere of radius r > c

[tex]\oint E\cdot dA = E4\pi r^2 = \frac{q_{encl}}{\epsilon_0}[/tex]

[tex]E = \frac{q_{encl}}{4\pi\epsilon_0 r^2}[/tex]

The potential (work per unit charge) is:

[tex]\int_\infty^c E\cdot dr[/tex]

Work out that integral to get the potential on the surface c

AM
 
Last edited:

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