$A$ narrow parallel beam of light falls on a glass sphere of radius $R$ and refractive index $\mu$ at normal incidence. The distance of the image from the outer edge is given by

  • A
    $\frac{R(2-\mu)}{2(\mu-1)}$
  • B
    $\frac{R(2+\mu)}{2(\mu-1)}$
  • C
    $\frac{R(2-\mu)}{2(\mu+1)}$
  • D
    $\frac{R(2+\mu)}{2(\mu+1)}$

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In the figure shown,$O$ is the centre of the glass sphere. When the spot $P$ on the sphere is viewed almost normally,it appears:

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