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

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SUMMARY

The discussion focuses on the distribution of electric charge between two concentric metal spheres when connected by a wire. The smaller sphere has a charge of 3.7 μC and a radius of 3.1 cm, while the larger sphere has a charge of 13 μC and a radius of 5.6 cm. Upon connection, all charge redistributes to the larger sphere due to the principle that the electric field inside a conductor is zero, resulting in a total charge of 16.7 μC on the larger sphere and 0 μC on the smaller sphere. The potential difference between the spheres can be calculated using Gauss' law and the formula for electric potential.

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  • Understanding of Gauss' law
  • Knowledge of electric potential and electric fields
  • Familiarity with the properties of conductors in electrostatics
  • Basic calculus for integration of electric fields
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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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