
Using Snell’s law for the critical angle \( \theta_c \): \[ n_A \sin \theta_c = n_B \sin 90^\circ = 1 \] Hence, \[ \sin \theta_c = \frac{v_A}{v_B} = \frac{2 \times 10^8}{2.5 \times 10^8} = \frac{4}{5} \] Thus, the critical angle is: \[ \theta_c = \sin^{-1} \left(\frac{4}{5} \right) \] Thus, the correct answer is: \[ \text{(B) } \sin^{-1} \left(\frac{4}{5} \right) \]

A transparent block A having refractive index $ \mu_2 = 1.25 $ is surrounded by another medium of refractive index $ \mu_1 = 1.0 $ as shown in figure. A light ray is incident on the flat face of the block with incident angle $ \theta $ as shown in figure. What is the maximum value of $ \theta $ for which light suffers total internal reflection at the top surface of the block ?