The bulk modulus is defined as: \[ B = - \frac{\Delta P}{\frac{\Delta V}{V}} \] Rearranging: \[ \Delta V = \frac{\Delta P}{B} V \] The volume of the cube is: \[ V = (10 \, { cm})^3 = 1000 \, { cm}^3 \] Converting to \( m^3 \): \[ V = 10^{-3} \, { m}^3 \] Substituting values: \[ \Delta V = \frac{(7 \times 10^6)}{1.4 \times 10^{11}} \times 10^{-3} \] \[ \Delta V = 5 \times 10^{-8} \, { m}^3 \] Converting to mm\(^3\): \[ \Delta V = 10.0 \, { mm}^3 \]


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: