How Do Charges Distribute Between Concentric Spheres When Connected by a Wire?

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Homework Help Overview

The problem involves two concentric metal spheres with given charges and radii, focusing on the potential difference between them and the distribution of charge when connected by a wire. The subject area pertains to electrostatics and the behavior of conductors in electrostatic equilibrium.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss using Gauss' law to find the electric field and potential difference, with one participant questioning the implications of charge distribution upon connecting the spheres. Others raise points about the nature of charge repulsion and the behavior of charges on conductors.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of charge behavior and potential differences. Some guidance has been offered regarding the properties of charged conducting spheres, but there is no explicit consensus on the implications of the results derived from Gauss' law.

Contextual Notes

Participants are navigating assumptions about charge distribution and the effects of connecting the spheres, with some uncertainty about the implications of their findings. There is a mention of constraints related to electric fields and charge conservation.

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Homework Statement


A metal sphere with charge q=3.7 μC and radius r=3.1 cm is concentric with a larger metal sphere with charge Q=13 μC and radius R=5.6 cm. (a) What is the magnitude of the potential difference between the spheres? If we connect the spheres with a wire, what then is the charge on (b) the smaller sphere and (c) the larger sphere?

Homework Equations


[/B]

The Attempt at a Solution


I don't know what the answer is, but if I find an expression for the electric field outside the larger conductor using Gauss' law and then integrate that from infinity to 0.056, then find the potential at the surface of the second conductor by simply using q/4*pi*epsilonnaught*r I should have the correct potentials at both surfaces, and for the second part the constraints are that the electric field between the two conductors is zero and q+Q= 16.7e-6 C?

edit: I just realized that according to Gauss' law, all the charge must move on to the larger sphere once they two are connected (since E_inside = 0). Not sure if I can make sense of this result, could someone please explain?
 
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The potential at the surface of a charged conducting sphere is the same as if all the charge were confined at the center.
When the spheres are connected, remember that like charges repel... so they will try to get as far apart as possible.
 
Simon Bridge said:
The potential at the surface of a charged conducting sphere is the same as if all the charge were confined at the center.
When the spheres are connected, remember that like charges repel... so they will try to get as far apart as possible.
Not sure where you're going with the second point.
 
The second point is in response to this:
I just realized that according to Gauss' law, all the charge must move on to the larger sphere once they two are connected (since E_inside = 0). Not sure if I can make sense of this result, could someone please explain?
 

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