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A spherical conductor having charge q an...

A spherical conductor having charge q and radius r is placed at the centre of a spherical shell of radius R and having charge Q (R `gt` r). The potential difference between the two is

A

proportional to Q

B

Proportional to q

C

Dependent on both Q and q

D

independent of both Q and q

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The correct Answer is:
To find the potential difference between a spherical conductor of charge \( q \) and radius \( r \) placed at the center of a spherical shell of radius \( R \) and charge \( Q \) (where \( R > r \)), we can follow these steps: ### Step-by-Step Solution: 1. **Understanding the System**: - We have a spherical conductor (let's call it SC) with charge \( q \) and radius \( r \). - This conductor is placed at the center of a spherical shell (let's call it SS) with charge \( Q \) and radius \( R \). 2. **Potential Inside the Spherical Conductor**: - The potential \( V_{SC} \) at the surface of the spherical conductor is given by the formula: \[ V_{SC} = \frac{kq}{r} \] - Here, \( k \) is the electrostatic constant. 3. **Potential Outside the Spherical Shell**: - For the spherical shell, since it is a conductor, the potential outside the shell (at a distance greater than \( R \)) is given by: \[ V_{SS} = \frac{kQ}{R} \] 4. **Potential Inside the Spherical Shell**: - Inside the shell (between the inner conductor and the shell), the potential is constant and equal to the potential at the surface of the shell: \[ V_{inside} = \frac{kQ}{R} \] 5. **Calculating the Potential Difference**: - The potential difference \( \Delta V \) between the spherical conductor and the spherical shell is given by: \[ \Delta V = V_{SC} - V_{SS} \] - Substituting the values we found: \[ \Delta V = \frac{kq}{r} - \frac{kQ}{R} \] 6. **Final Expression**: - Therefore, the potential difference between the two is: \[ \Delta V = \frac{kq}{r} - \frac{kQ}{R} \] ### Final Answer: The potential difference between the spherical conductor and the spherical shell is: \[ \Delta V = \frac{kq}{r} - \frac{kQ}{R} \]
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