At steady state, the inductor behaves as a short circuit, meaning it has zero resistance. The circuit becomes a simple resistor connected to the voltage source.
Using Ohm’s law, the steady-state current (\( I \)) through the resistor is given by:
\[ I = \frac{V}{R}. \]
Substitute \( V = 10 \, \text{V} \) and \( R = 4 \, \Omega \):
\[ I = \frac{10}{4} = \frac{5}{2} = 2.5 \, \text{A}. \]
The energy (\( E \)) stored in the magnetic field of the inductor is given by:
\[ E = \frac{1}{2} L I^2. \]
Substitute \( L = 2 \, \text{H} \) and \( I = 2.5 \, \text{A} \):
\[ E = \frac{1}{2} \cdot 2 \cdot \left(2.5\right)^2. \]
Calculate \( (2.5)^2 \):
\[ (2.5)^2 = 6.25. \]
Substitute back into the equation:
\[ E = \frac{1}{2} \cdot 2 \cdot 6.25 = 6.25 \, \text{J}. \]
Convert to scientific notation:
\[ E = 625 \times 10^{-2} \, \text{J}. \]
The energy stored in the magnetic field is \( 625 \times 10^{-2} \, \text{J} \).

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: