To solve the problem, we need to determine the area \( A \) of a surface on which electromagnetic radiation is incident. The given values are:
We know that intensity \( I \) is related to force \( F \) and area \( A \) by the following relation for a non-reflecting surface:
F = \dfrac{I \cdot A}{c}
Where:
First, convert the intensity from \(\text{W/cm}^2\) to \(\text{W/m}^2\):
360 \, \text{W/cm}^2 = 360 \times 10^4 \, \text{W/m}^2 = 3.6 \times 10^6 \, \text{W/m}^2
Substitute the values in the formula:
2.4 \times 10^{-4} = \dfrac{3.6 \times 10^6 \cdot A}{3 \times 10^8}
Simplify to find A:
2.4 \times 10^{-4} = \dfrac{3.6 \cdot A}{300}
2.4 \times 10^{-4} \times 300 = 3.6 \cdot A
72 \times 10^{-4} = 3.6 \cdot A
A = \dfrac{72 \times 10^{-4}}{3.6} = 20 \times 10^{-4} = 0.02 \, \text{m}^2
Therefore, the area \( A \) is 0.02 \, \text{m}^2.
Hence, the correct answer is 0.02 m2.

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: