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A solid sphere of radius R has charge q ...

A solid sphere of radius R has charge q uniformly distributed over its volume. The distance from it surfce at which the electrostatic potential is equal to half of the potential at the centre is

A

R

B

R/2

C

R/3

D

2R

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The correct Answer is:
To solve the problem, we need to find the distance from the surface of a solid sphere of radius \( R \) with charge \( q \) uniformly distributed over its volume, at which the electrostatic potential is equal to half of the potential at the center of the sphere. ### Step-by-Step Solution: 1. **Calculate the Potential at the Center of the Sphere**: The potential \( V \) at a point inside a uniformly charged solid sphere is given by the formula: \[ V(r) = \frac{kq}{2R} \left( 3R^2 - r^2 \right) \] where \( k \) is Coulomb's constant, \( q \) is the total charge, and \( R \) is the radius of the sphere. For the center of the sphere, \( r = 0 \): \[ V_{\text{center}} = \frac{kq}{2R} \left( 3R^2 - 0 \right) = \frac{3kq}{2R} \] 2. **Determine Half of the Potential at the Center**: We need to find a point \( P \) where the potential is half of the potential at the center: \[ V_P = \frac{1}{2} V_{\text{center}} = \frac{1}{2} \left( \frac{3kq}{2R} \right) = \frac{3kq}{4R} \] 3. **Set Up the Equation for Potential at Point \( P \)**: The potential at a distance \( r \) from the center of the sphere (where \( r > R \)) is given by: \[ V(r) = \frac{kq}{r} \] We set this equal to \( \frac{3kq}{4R} \): \[ \frac{kq}{r} = \frac{3kq}{4R} \] 4. **Solve for \( r \)**: Cancel \( kq \) from both sides (assuming \( kq \neq 0 \)): \[ \frac{1}{r} = \frac{3}{4R} \] Thus, \[ r = \frac{4R}{3} \] 5. **Calculate the Distance from the Surface**: The distance from the surface of the sphere to point \( P \) is given by: \[ \text{Distance from surface} = r - R = \frac{4R}{3} - R = \frac{4R}{3} - \frac{3R}{3} = \frac{R}{3} \] ### Final Answer: The distance from the surface at which the electrostatic potential is equal to half of the potential at the center is: \[ \frac{R}{3} \]
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