
In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by:
The potential energy of a system of point charges is calculated as:
U = ∑i<j \( \frac{K q_i q_j}{r_{ij}} \),
where \( r_{ij} \) is the separation between charges \( i \) and \( j \).
Configuration (1): Charges are positioned at the vertices of a square. The distance between adjacent charges is \( a \), and the distance between diagonally opposite charges is \( \sqrt{2}a \).
Configuration (2): Charges are positioned at the midpoints of the sides of the square. Consequently, the distance between adjacent charges is \( \frac{a}{\sqrt{2}} \), and the distance between diagonally opposite charges is \( a \).
The potential energy for configuration (1) is:
\( U_1 = 4 \times \frac{K q_0^2}{a} + 2 \times \frac{K q_0^2}{\sqrt{2}a} \).
The potential energy for configuration (2) is:
\( U_2 = 4 \times \frac{K q_0^2}{\frac{a}{\sqrt{2}}} + 2 \times \frac{K q_0^2}{a} \).
The difference in potential energy, calculated as \( U_2 - U_1 \), yields the required result:
\( \Delta U = U_2 - U_1 = \frac{K q_0^2}{a} (4\sqrt{2} - 2) \).
Final Answer: \( \frac{K q_0^2}{a} (4\sqrt{2} - 2) \).

In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: