(d) From Snell’s law
$\mu = \frac{1}{\sin i_{C}}$
Since, $i_{B}\ > i_{A}$
$\sin{i_{:B} > \sin i_{A}}$
$\Rightarrow \mu_{B} < \mu_{A}$
When angle of incidence in the denser medium is increased even very slightly beyond the critical angle, then the ray of light is reflected back completely in the denser medium and total internal reflection takes place. Let $\theta$ be critical angle from medium $A\ to\ B,\ $then
$\ _{B}\mu_{A} = \frac{1}{\sin\theta}$
$\Rightarrow \sin\theta = \frac{1}{\ _{B}\mu_{A}}\frac{\mu_{B}}{\mu_{A}}$
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ = \frac{1}{\sin i_{B}} \times \frac{\sin i_{A}}{1}$
$\Rightarrow \ \theta = \sin^{- 1}\left\lbrack \frac{\sin i_{A}}{\sin i_{B}} \right\rbrack$