$A$ ray of light is incident on a parallel slab of thickness $t$ and refractive index $n$. If the angle of incidence $\theta$ is small,then the lateral displacement between the incident and emergent ray will be

  • A
    $\frac{t\theta (n - 1)}{n}$
  • B
    $\frac{t\theta}{n}$
  • C
    $\frac{t\theta n}{n - 1}$
  • D
    $\frac{t\theta (n + 1)}{n}$

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