Finding potential of conducting sphere

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Homework Help Overview

The problem involves finding the electric potential at the center and a point P of a hollow uncharged conducting spherical shell when a charge q is placed at a distance of 2r from the center of the shell. The subject area pertains to electrostatics and the behavior of conductors in electric fields.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the method of images and its application to the problem, questioning the assumptions about the charge on the shell and the implications of grounding. There are attempts to clarify the potential at various points and the nature of induced charges.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the problem, particularly regarding the charge of the shell and the use of image charges. Some guidance has been provided about the potential being constant inside the shell, but no consensus has been reached on the correct approach or interpretation of the problem.

Contextual Notes

There is uncertainty about whether the spherical shell is grounded or uncharged, which affects the interpretation of the problem. Participants also note the lack of explicit information about the charge on the shell and its implications for the potential calculations.

Titan97
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Homework Statement


Find the potential at the centre and at P of a hollow uncharged conducting spherical shell if a charge q is placed at a distance of 2r from centre of shell.
(r is the radius)
IMG_20151126_190834_538.JPG


Homework Equations


All the charge induced on the sphere has to reside on the sphere's outer surface.

Mirror charge is given by ##\frac{-qR}{a}##
At a distance ##\frac{R^2}{a}## from centre.
(R is radius and 'a' is distance of charge from centre)

The Attempt at a Solution


Using method of images, mirror charge is -q/2 and its distance from C is r/2
Potential at centre is then $$\frac{-k\frac{q}{2}}{2.(r/2)}+\frac{kq}{2r}=0$$
Answer given is ##\frac{kq}{r}##

Similarly at Point P, I got ##0## as the potential. But answer given is ##\frac{-kq}{6r}## at P.
 
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Note that the problem does not state that the spherical conductor is grounded.

Is point P on the surface of the conductor?

The given answers do not appear to be correct to me.

Putting an image charge inside the sphere is useful for finding the potential outside the sphere. What can you say about the potential everywhere inside the sphere?
 
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P is a point on the surface of the sphere.
Actually, the problem specifies "charged conducting spherical shell". But charge of the shell is not given. So I thought it was a printing mistake. Is there any difference?

Potential at every point inside the shell is constant.

I would like to add this point. Let's say the induced charge density on the outer surface of the shell is σ (a function in terms of the point on the sphere).

Then, potential is centre $$V_C=\frac{kq}{r}+\frac{k\int\sigma da}{r}$$
Since total charge on sphere is zero,
$$V_C=\frac{kq}{r}$$
 
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Would you please state the problem word for word as it was given to you.

I agree that the potential is constant throughout the hollow region inside the shell. So, I don't see how the potential at C can be different than at P.
 
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Titan97 said:
P is a point on the surface of the sphere.
Actually, the problem specifies "charged conducting spherical shell". But charge of the shell is not given. So I thought it was a printing mistake. Is there any difference?

Potential at every point inside the shell is constant.
The solution to this problem can be done with superposition together with the method of images.

The image charge together with the charge, q, produce an equipotential surface with potential of zero co-incident with the surface of the sphere.

However, that's the solution if the sphere has a charge of -qr/(2r) = -q/2 .

Superimpose upon this, the solution for an isolated conducting sphere with the opposite charge (+q/2). That is, replace the sphere with a charge of q/2 at the sphere's center.

I.e., combine the image charge and this charge at the center.
 
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received_762439810566180.jpeg
 
I'm not sure of the interpretation of the problem.You might be right that the problem meant to state that the sphere is uncharged rather than charged.

Also, it could be that the problem wants you to find the contribution to the potential at P due to just the induced charges on the sphere. When I work the problem with this interpretation, I get kq/(6r) which differs in sign from the given answer. So, I'm not sure what's going on.

I don't see where the problem asks for the potential at the center.
 
I added that part. The minus was a typo. Did you solve using method of images?
 
Titan97 said:
I added that part. The minus was a typo. Did you solve using method of images?
The potential at the center is the same at the potential at P, as is the potential anywhere on the surface or in the interior.

The answer key is almost correct.
 
  • #10
Titan97 said:
I added that part. The minus was a typo. Did you solve using method of images?
Yes, I used the method of images. (See SammyS post #5 for more details.)
 
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  • #11
SammyS said:
However, that's the solution if the sphere has a charge of -qr/(2r) = -q/2 .

Why?
 
  • #12
Titan97 said:
Why?
As I understand the problem, the net charge on the sphere is zero.
 
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  • #13
In which case does the sphere get -q/2 charge? Is it when the sphere is grounded? But in that case as well, initial charge on he sphere is zero.
 
  • #14
Titan97 said:
In which case does the sphere get -q/2 charge? Is it when the sphere is grounded? But in that case as well, initial charge on he sphere is zero.
For there to be an equipotential surface at the location of the surface of the sphere, you replace the sphere with the image charge ( -q/2 ). That as it turns out gives a potential of zero for the sphere. However, Mr. Gauss tells us that this solution is equivalent to the sphere having a net charge of -q/2 .

So we need another charge. One with charge of +q/2. Where can we place it?
 
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  • #15
I am totally confused.

http://www.physicspages.com/2011/12/12/method-of-images-point-charge-and-sphere/

The above link does not specify any extra q/2. How does gauss law state that?
 
  • #16
Titan97 said:
I am totally confused.

http://www.physicspages.com/2011/12/12/method-of-images-point-charge-and-sphere/

The above link does not specify any extra q/2. How does gauss law state that?
If the sphere is neutral, how much flux passes through a Gaussian surface just outside the sphere?
 
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  • #17
It will only be due to the charge inside the sphere.
 
  • #18
Titan97 said:
It will only be due to the charge inside the sphere.
The sphere is neutral. There is no charge inside the sphere. Therefore the flux is ____ .
 
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  • #19
Zero.
 
  • #20
Titan97 said:
Zero.
Right.

Replacing the sphere with individual charges must give the same result (at locations external to the sphere) as the sphere gives.
 
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  • #21
OK. So a mirror charge -q/2 is equivalent to the sphere have a total charge of -q/2.
Since the question needs an uncharged sphere, u need to place +q/2. But nothing like this was discussed in the link I gave.
 
  • #22
Titan97 said:
OK. So a mirror charge -q/2 is equivalent to the sphere have a total charge of -q/2.
Since the question needs an uncharged sphere, u you need to place +q/2. But nothing like this was discussed in the link I gave.
The example in that link has a grounded sphere. The problem in this thread has a neutral sphere. That grounded sphere does have a non-zero net charge.
 
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  • #23
SammyS said:
So we need another charge. One with charge of +q/2. Where can we place it?

Can I place it at the centre of the shell? But If I do that, how will I calculate potential at centre of the shell? (Due to the new central charge, potential at centre will be ##\frac{kq}{2\cdot 0}## which is undefined)
 
  • #24
Titan97 said:
Can I place it at the centre of the shell? But If I do that, how will I calculate potential at centre of the shell? (Due to the new central charge, potential at centre will be ##\frac{kq}{2\cdot 0}## which is undefined)
The image charges along with the external charge give you the potential everywhere external to the sphere, and on its surface. The potential inside the sphere is constant and is equal to the potential at the surface. Do not use the image charges to calculate the potential inside the sphere.
 
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