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Question: Consider a ray of light incident from air onto a slab of glass (refractive index *n*) of width d, at...

Consider a ray of light incident from air onto a slab of glass (refractive index n) of width d, at an angle θ\theta The phase difference between the ray reflected by the top surface of the glass and the bottom surface is

A

4πdλ(11n2sin2θ)1/2+π\frac{4\pi d}{\lambda}\left( 1 - \frac{1}{n^{2}}\sin^{2}\theta \right)^{1/2} + \pi

B

4πdλ(11n2sin2θ)1/2\frac{4\pi d}{\lambda}\left( 1 - \frac{1}{n^{2}}\sin^{2}\theta \right)^{1/2}

C

4πdλ(11n2sin2θ)1/2+π2\frac{4\pi d}{\lambda}\left( 1 - \frac{1}{n^{2}}\sin^{2}\theta \right)^{1/2} + \frac{\pi}{2}

D

4πdλ(11n2sin2θ)1/2+π\frac{4\pi d}{\lambda}\left( 1 - \frac{1}{n^{2}}\sin^{2}\theta \right)^{1/2} + \pi

Answer

4πdλ(11n2sin2θ)1/2+π\frac{4\pi d}{\lambda}\left( 1 - \frac{1}{n^{2}}\sin^{2}\theta \right)^{1/2} + \pi

Explanation

Solution

: 4πdλ(11n2sin2θ)1/2+π\frac{4\pi d}{\lambda}\left( 1 - \frac{1}{n^{2}}\sin^{2}\theta \right)^{1/2} + \pi