For the given case, using Snell’s law: \[ n_A \sin \theta_A = n_B \sin \theta_B \] Here, since the refracted ray is parallel to the interface, \( \theta_B = 90^\circ \), and hence: \[ n_A \sin 30^\circ = n_B \sin 90^\circ \] \[ n_A \times \frac{1}{2} = n_B \times 1 \] Thus, the refractive index of medium B is: \[ n_B = \frac{n_A}{2} \] Since the refractive index of the denser medium (A) is \( \sqrt{\frac{4}{3}} \), we have: \[ n_B = \frac{\sqrt{\frac{4}{3}}}{2} = \frac{2}{\sqrt{3}} \] Thus, the correct answer is: \[ \text{(D) } \frac{2}{\sqrt{3}} \]
Bittu and Chintu were partners in a firm sharing profit and losses in the ratio of 4 : 3. Their Balance Sheet as at 31st March, 2024 was as follows:
On 1st April, 2024, Diya was admitted in the firm for \( \frac{1}{7} \)th share in the profits on the following terms:
Prepare Revaluation Account and Partners' Capital Accounts.