
A hemispherical vessel is completely filled with a liquid of refractive index $\mu$. A small coin is kept at…

- $\sqrt{3}$
- $\frac{\sqrt{3}}{2}$
- $\frac{3}{2}$
- $\sqrt{2}$
Solution

For the rays from coin to reach the point $E$, the refracted rays must grazing the surface, i.e. they must be incident at critical angle $\theta_c$ inside the liquid.
$\mu=\frac{1}{\sin \theta_c}$
$\mu$ is minimum when $\theta_c$ is maximum.
Maximum value of $\theta_c=45^{\circ}$
$\Rightarrow \mu$ has a minimum value of $\sqrt{2}$.
Asked in: JEE Main 2025 (28 Jan Shift 1)