$A$ ray of light is incident on a thick slab of glass of thickness $t$ as shown in the figure. The emergent ray is parallel to the incident ray but displaced sideways by a distance $d$. If the angles are small,then $d$ is

  • A
    $t\left( {1 - \frac{i}{r}} \right)$
  • B
    $rt\left( {1 - \frac{i}{r}} \right)$
  • C
    $it\left( {1 - \frac{r}{i}} \right)$
  • D
    $t\left( {1 - \frac{r}{i}} \right)$

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