$A$ paraxial beam of light is converging towards a point $P$ on the screen. $A$ plane parallel sheet of glass of thickness $t$ and refractive index $\mu$ is introduced in the path of the beam. The convergence point is shifted by:

  • A
    $t (1 - 1/\mu)$ away
  • B
    $t (1 + 1/\mu)$ away
  • C
    $t (1 - 1/\mu)$ nearer
  • D
    $t (1 + 1/\mu)$ nearer

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In determining the refractive index of a glass slab using a travelling microscope,the following readings are tabulated:
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