$A$ ray of light is incident on a medium of refractive index $\mu$ at an angle of incidence $i$. On refraction in the medium,$\delta$ is the angle of deviation. Then:

  • A
    $\frac{1}{\mu} = \cos \delta - \frac{\sin \delta}{\tan i}$
  • B
    $\frac{1}{\mu} = \sin \delta - \frac{\cos \delta}{\tan i}$
  • C
    $\frac{1}{\mu} = \cos \delta - \sin \delta \cdot \tan i$
  • D
    $\frac{1}{\mu} = \sin \delta - \cos \delta \cdot \tan i$

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