Potential Difference between concentric shells

In summary, the potential of the concentric spherical shell with radii a and b when outer shell is earthed is V = q(b-a)/4πεοab.
  • #1
zorro
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Homework Statement


The figure shows two concentric shells of radii R and 2R. A charge q is initially imparted to the inner shell. After the keys k1 and k2 are alternately closed n times, find the potential difference between the shells.

The Attempt at a Solution



Initially, the charge q is induced on the outer shell so that it has -q charge on its inner surface.
When the key k1 is pressed, the outer shell gets earthed.
So the potential which V1 between them is Kq/2R
Now when k2 is closed (after opening k1) the charge q on inner shell disappears so that it gains 0 potential. The charge -q which was induced on the outer surface remains as it is.
Now the potential is given by V2 = -Kq/2R

When k1 is closed again, outer shell gains 0 potential, But the inner shell has an induced charge of +Q. So potential is Kq/2R
In this way, the potential alternates with + and - sign. At the end of 'n', the potential is -Kq/2R

But the answer is Kq/2n+1R
Any hint appreciated.
 

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  • #2
Potential of the concentric spherical shell with radii a and b when outer shell is earthed is

V = q(b-a)/4πεοab.

When the inner shell is earthed

V = q(b-a)/4πεοb^2.
 
  • #3
How did you get this expression-

"When the inner shell is earthed

V = q(b-a)/4πεοb^2. "

What is wrong with my approach? I would like to tackle the problem conceptually rather than using just formulae.
 
  • #4
When you open k1, net charge on A is -q and on B is Q.
when you ground B, net potential of B is zero. It is due to potential of B, potential due to inner surface of A and potential due to outer surface of A.
Let -q' be the charge in the inner surface of A, x be the charge on the outer surface of A and +q' on B. So the potential on B is ( assuming the thickness of the shell is small compared to 2R.)
Kq'/R -Kq'/2R + Kx/2R = 0
From the charge conservation of the outer shell, -q = x -q' or x = q' - q.
So Kq'/R -Kq'/2R + K(q'-q)/2R = 0 or q' = q/2.

So V2 = Kq/2*2R
 
Last edited:
  • #5
Thank you very much Sir!...you cleared my misconception. I thought that if potential on a surface is 0, q must be 0...which is not so.
Thanks once again!
 

1. What is the potential difference between concentric shells?

The potential difference between concentric shells refers to the difference in electric potential between two concentric conducting spheres or cylinders. It is typically measured in volts (V) and is a key factor in determining the strength of an electric field.

2. How is the potential difference between concentric shells calculated?

The potential difference between concentric shells can be calculated using the formula V = k*(Q1-Q2)/r, where V is the potential difference, k is the Coulomb's constant, Q1 and Q2 are the charges on the shells, and r is the distance between them. This formula is based on the equation for electric potential energy.

3. What factors affect the potential difference between concentric shells?

The potential difference between concentric shells is affected by several factors, including the charges on the shells, the distance between them, and the medium between them. The type of materials used for the shells can also have an impact on the potential difference.

4. How does potential difference between concentric shells relate to electric fields?

The potential difference between concentric shells is directly related to the strength of the electric field between them. A larger potential difference indicates a stronger electric field, while a smaller potential difference indicates a weaker electric field. The electric field is also the gradient of the potential difference, meaning it is the change in potential per unit distance.

5. Why is potential difference between concentric shells important in electrical systems?

Potential difference between concentric shells is an important concept in electrical systems because it determines the flow of electric charge between the shells. This is crucial in understanding and designing electrical circuits and devices. It also plays a role in the behavior of electrical conductors and insulators.

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