The light travels along the surface of the cylindrical rod. For this to happen, the angle of incidence \( \theta \) must be such that the light is refracted along the surface. Using Snell's law at the interface between the rod and air: \[ n_{\text{air}} \sin \theta = n_{\text{rod}} \sin 90^\circ \] Given \( n_{\text{air}} = 1 \) and \( n_{\text{rod}} = \frac{2}{\sqrt{3}} \), we have: \[ \sin \theta = \frac{n_{\text{rod}}}{n_{\text{air}}} = \frac{2}{\sqrt{3}} \] Thus: \[ \theta = \sin^{-1} \left( \frac{2}{\sqrt{3}} \right) \] Therefore, the angle \( \theta \) is \( \sin^{-1} \left( \frac{2}{\sqrt{3}} \right) \).
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
On $1^{\text {st }}$ April, 2024, Diya was admitted in the firm for $\frac{1}{7}$ share in the profits on the following terms:
Prepare Revaluation Account and Partners' Capital Accounts.
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.