To solve this problem, let's explore the potential distribution in a conductor when it is charged.
According to electrostatic principles, when a conductor is charged, all the excess charge resides on the surface of the conductor. This occurs due to the repulsive forces between like charges, which push them to the furthest possible distance from each other, which is on the surface.
Now, considering the potential, which is a measure of the work done in bringing a unit positive charge from infinity to a point in the electric field, follows a fascinating rule for conductors. The key point to understand here is:
Thus, for a charged conductor, the potential at every point inside it, including the surface, is the same. Therefore, irrespective of the shape of the conductor, the potential remains uniform throughout, including the surface and the interior.
Now, let's eliminate the incorrect options:
The correct explanation, as understood from electrostatic principles, is:
Therefore, the correct answer is that the potential remains the same throughout the conductor.
Two charges, \( q_1 = +3 \, \mu C \) and \( q_2 = -4 \, \mu C \), are placed 20 cm apart. Calculate the force between the charges.