Monochromatic light is incident on a glass prism of angle A. If the refractive index of the material of the prism is \[\mu \], a ray incident at an angle \[\theta \], on the face AB would get transmitted through the face AC of the prism provided

A) \[\theta > si{n^{ - 1}}\left( {\mu sin\left( {A - si{n^{ - 1}}\left( {\dfrac{1}{\mu }} \right)} \right)} \right)\]
B) \[\theta < si{n^{ - 1}}\left( {\mu sin\left( {A - si{n^{ - 1}}\left( {\dfrac{1}{\mu }} \right)} \right)} \right)\]
C) \[\theta > {\cos ^{ - 1}}\left( {\mu sin\left( {A - si{n^{ - 1}}\left( {\dfrac{1}{\mu }} \right)} \right)} \right)\]
D) \[\theta < {\cos ^{ - 1}}\left( {\mu sin\left( {A - si{n^{ - 1}}\left( {\dfrac{1}{\mu }} \right)} \right)} \right)\]

Hint: In this solution, we will use Schell’s law of refraction to determine the angle of refraction when the ray of light passes from the surface AB. This angle of refraction from the first surface should be such that the angle of incidence on the surface AC will be such that the ray will be internally reflected.
Formula used: In this solution, we will use the following formula:
Snell's law: ${\mu _1}\sin {\theta _1} = {\mu _2}\sin {\theta _2}$ where ${\mu _1}$ and ${\mu _2}$ are the refractive index of two different mediums and ${\theta _1}$ and ${\theta _2}$ are the angles made by the ray of light with the normal to the surface of refraction.

Complete step by step answer:
Let the angle of incidence on the surface AB be $\theta $. Then using Snell’s law on the first surface, the incident medium will be air so its refractive index will be 1.
$1\sin \theta = \mu \sin r$
Now the angle of incidence on the other surface will be $r'$. The relation between $r$ and $r'$ will be determined from the triangle APQ as the sum of all the angles in the triangle will be $180^\circ $.
$A + (90^\circ - r) + (90^\circ - r') = 180$
Which gives us
$r' = A - r$
Now for the surface, AC, the angle of incidence on the surface $r'$ will be such that the angle of reflection will be $90^\circ $ or greater which implies
$\mu \sin r' < 1\sin 90^\circ $
So, dividing both sides by $\mu $ and taking the sine inverse on both sides, we get
$r' < {\sin ^{ - 1}}\dfrac{1}{\mu }$
Since $r' = A - r$, we can write
$A - r < {\sin ^{ - 1}}\dfrac{1}{\mu }$
$r > A - {\sin ^{ - 1}}\dfrac{1}{\mu }$
Again as $1\sin \theta = \mu \sin r$, we can write
\[\theta > si{n^{ - 1}}\left( {\mu sin\left( {A - si{n^{ - 1}}\left( {\dfrac{1}{\mu }} \right)} \right)} \right)\] which corresponds to option (A).

Note: To solve such questions, we must be aware of the phenomenon of internal reflection and how it behaves in a prism. Unless mentioned otherwise, we must assume the medium outside the prism to be air and have a refractive index of 1.