How Is Charge Distributed on a Conducting Shell with a Central Charge?

In summary, the conversation discusses the problem of finding the excess charge on a solid spherical conducting shell with a point charge at its center, in order to make the charge density on the inner and outer surfaces of the shell equal. The solution involves adding a charge of -5Q to the shell, with the inner wall having a charge of -Q and the outer wall having a charge of -4Q. The reasoning and solution are both supported by the answer key, but there is some disagreement with a physics teacher. The conversation also includes a helpful explanation of the solution.
  • #1
thechunk
11
0
I need a little help with this problem. Its from the 2004 physics bowl.

50. A solid spherical conducting shell has inner radius a and outer radius 2a. At the center of the shell is located a point charge +Q. What must the excess charge on the shell be in order for the charge density on the inner and outer surfaces of the shell to be exactly equal?

I reasoned that the charge on the inner surfaces of the shell is -Q because the electrons are attracted towards the point charge. Thus the charge on the outer shell is +Q. The surface area of the outer shell is [tex]16\pi a^2 [/itex] and the surface are of the inner shell is [tex] 4\pi a^2 [/itex]. So the charge density on the outer is shell is [tex]\frac{Q}{16\pi a^2} [/itex] and the charge denisty on the inner shell is [tex]\frac{-Q}{4\pi a^2} [/itex]. So in order to make the charge density equal you need to add -5Q to the shell so that that charge accumulates outside and yields a charge density on the outer surface of [tex]\frac{-Q}{4\pi a^2} [/itex]. So the answer is -5Q which is also the answer according to the answer key, however my physics teacher does not agree. Is my reasoning correct cause I have to agrue this with him tommorow. Thanks
 
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  • #2
Any help people, I am not very familiar with E&M
 
  • #3
thechunk said:
Any help people, I am not very familiar with E&M

Your solution looks right to me. The electric field inside the conductor must be zero, so the inner wall of the shell must have a total charge of -Q to balance the point charge. This of course gives a density of

[tex]\kappa=-\frac{Q}{4\pi a^2}[/tex]

When charge is added to the conductor, the inner wall must retain the same charge density if the field is remain zero inside, so all added charge goes to the outer surface. The outer surface has a larger radius, so it'll need a larger charge to get the same density:

[tex]\kappa=\frac{Q_{outer}}{16\pi a^2}=-\frac{Q}{4\pi a^2}[/tex]

The solution to this equation is, of course,

[tex]Q_{outer}=-4Q[/tex]

Giving a total charge on the conductor of

[tex]Q_{tot}=Q_{outer}+Q_{inner}=-4Q+(-Q)=-5Q[/tex]
 
  • #4
Thanks, your explanation is clearer
 

FAQ: How Is Charge Distributed on a Conducting Shell with a Central Charge?

What is the concept of charges?

The concept of charges refers to the fundamental property of matter that produces an electric field. It can either be positive or negative, and particles with the same charge repel each other while particles with opposite charges attract each other.

What are conducting shells?

Conducting shells are thin, hollow, metallic objects that can conduct electricity. They are often used as protective shields or enclosures for electrical components and systems.

How do charges interact with conducting shells?

Charges interact with conducting shells by inducing an equal but opposite charge on the surface of the shell. This results in the charge being distributed evenly on the outer surface of the shell, and the electric field inside the shell becomes zero.

What is the significance of conducting shells in electrostatics?

Conducting shells play an important role in electrostatics because they help to shield the interior of a system from external electric fields. They also help to protect sensitive electrical components from potentially damaging charges.

Can conducting shells be used to manipulate electric fields?

Yes, conducting shells can be used to manipulate electric fields by changing the shape or configuration of the shell. This can alter the distribution of charges and the resulting electric field inside and outside the shell.

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