Two light waves having the same wavelength $\lambda$ in vacuum are in phase initially. Then the first wave travels a path $L_{1}$ through a medium of refractive index $n_{1}$ while the second wave travels a path of length $L_{2}$ through a medium of refractive index $n_{2}$. After this the phase difference between the two waves is:

  • A
    $\frac{2 \pi}{\lambda}(n_{1}L_{1} - n_{2}L_{2})$
  • B
    $\frac{2 \pi}{\lambda}(\frac{L_{2}}{n_{1}} - \frac{L_{1}}{n_{2}})$
  • C
    $\frac{2 \pi}{\lambda}(\frac{L_{1}}{n_{1}} - \frac{L_{2}}{n_{2}})$
  • D
    $\frac{2 \pi}{\lambda}(n_{2}L_{1} - n_{1}L_{2})$

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