A transparent solid cylindrical rod has a refractive index of 2√3. It is surrounded by air. A light ray is incident at the mid point of one end of the rod as shown in the figure.
The incident angle θ for which the light ray grazes along the wall of the rod is
sin−1(1√3)
Applying snell's law at the first surface
sinθsinr=2√3 ...(1)
at second surface
sin (90 - r) = √32 ...(2)
⇒cosr=√32
⇒sinr=12
⇒2 sin θ = 2√3 from (1)
⇒sinθ = 1√3
⇒θ=sin−1(1√3)