Electric Potential with Non-conducting sphere and conducting shell

In summary, a spherical nonconductor of radius a carries charge +Q uniformly spread through its volume. Two hemispherical conducting shells of inner radius b and outer radius c are placed concentrically with the nonconducting sphere to form a single conducting sphere. The potential at r=b just outside the conducting shell is determined for three scenarios: a) before the conducting shell is introduced, b) after the conducting shell is introduced but before it is grounded, and c) after the conducting shell is grounded. The potential at b is ##{\frac{Q}{4πε_0b}} ## for scenario a), while it is ##{\frac{Q}{4πε_0c}} ## for scenario b). In scenario c
  • #1
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Homework Statement


A spherical nonconductor of radius a carries charge +Q uniformly spread through its volume. 2 hemispherical conducting shells of inner radius b and outer radius c are placed concentrically with the nonconducting sphere to form a single conducting sphere.

The conducting shell is momentarily connected by a wire to 0 potential (grounded) and then the wire is removed.
Determine the electric potential at r=b just outside the conducting shell
a) Before the conducting shell is introduced
b) After the conductor is introduced but before it is grounded
c) After the conductor is grounded.[/B]

Homework Equations


Potential difference =
V= ##{\frac{Q}{4πε_0r}} ##. [/B]

The Attempt at a Solution


For a) The nonconducting sphere can be modeled as a point charge, so the potential at b is simply ##{\frac{Q}{4πε_0b}} ##.

For b) The electric field is the same at all points except that when b<r<c, where the electric field is 0. So the potential at b should be the same as the potential at c, so V = ##{\frac{Q}{4πε_0c}} ##.

For c) While the conducting shell is grounded it will gain negative charge -Q due to the positive charge on the nonconducting sphere. Once the wire is removed the net charge of both the nonconducting sphere and shell will be 0, and so the electric field for r>c will be 0. The electric field inside of the conducting will also be 0. Since the field is zero from infinitely far away to b, the electric potential is 0. I'm not at all confident about this answer, though.

Any assistance would be greatly appreciated.
[/B]
 
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  • #2
(b) check your reasoning ... the conducting sphere is electrically neutral, so what happens to the charges when it is brought close to the charged sphere?
(c) think of it as charge conducted away.
 

Related to Electric Potential with Non-conducting sphere and conducting shell

1. What is the difference between a non-conducting sphere and a conducting shell?

A non-conducting sphere is a material that does not allow electricity to flow through it easily, while a conducting shell is a material that allows electricity to flow through it easily.

2. How does the electric potential of a non-conducting sphere and conducting shell differ?

The electric potential of a non-conducting sphere is constant throughout its surface, while the electric potential of a conducting shell is strongest at its surface and decreases as you move towards the center.

3. Why does a conducting shell have a stronger electric potential at its surface?

This is because the electric charges on the surface of the conducting shell repel each other, causing them to spread out evenly and creating a stronger electric field at the surface.

4. How does the electric potential of a non-conducting sphere and conducting shell affect the movement of charges?

In a non-conducting sphere, the electric potential does not affect the movement of charges as it is constant. However, in a conducting shell, the electric potential can cause charges to move towards the surface of the shell.

5. What is the significance of electric potential in the context of a non-conducting sphere and conducting shell?

The electric potential is a measure of the amount of work required to move a unit charge from one point to another. In the context of a non-conducting sphere and conducting shell, it helps to explain how electric charges behave and how they are distributed on the surface of these objects.

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