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QJEEAdv23Ph0ee4: JEE Advanced 2023 Physics - Class 12 JEEAdv23Ph0ee4 Solution: A monochromatic light wave is incident normally on a glass slab …

A monochromatic light wave is incident normally on a glass slab of thickness dd , as shown in the figure. The refractive index of the slab increases linearly from n1n_1 to n2n_2 over the height hh . Which of the following statement(s) is(are) true about the light wave emerging out of the slab?

JEE Advanced 2023 Paper 2 Online Physics - Geometrical Optics Question 6 English

Multiple Choice Options

  • A It will deflect up by an angle tan⁡−1[(n22−n12)d2h]\tan ^{-1}\left[\frac{\left(n_2^2-n_1^2\right) d}{2 h}\right] .
  • B It will deflect up by an angle tan⁡−1[(n2−n1)dh]\tan ^{-1}\left[\frac{\left(n_2-n_1\right) d}{h}\right] .
  • C It will not deflect.
  • D The deflection angle depends only on (n2−n1)\left(n_2-n_1\right) and not on the individual values of n1n_1 and n2n_2 .

Step-by-Step Verified Solution

JEE Advanced 2023 Paper 2 Online Physics - Geometrical Optics Question 6 English Explanation

At point A on one end of the slab, the wavefront takes a time tt to reach the other end. The time tt can be expressed as the ratio of the distance traveled, dd , to the speed of the wave in the medium, which is cn1\frac{c}{n_1} (where cc is the speed of light in vacuum and n1n_1 is the refractive index of the medium at A). Therefore, the time taken tt is given by t=dcn1=n1dct = \frac{d}{\frac{c}{n_1}} = \frac{n_1 d}{c} .

Simultaneously, consider the wavefront at point B, located in a different medium with a refractive index n2n_2 . In the same time tt , the wavefront at B travels a distance s1s_1 . The distance s1s_1 can be calculated as the product of the speed of light in the medium at B, cn2\frac{c}{n_2} , and the time tt , yielding s1=cn2×n1dc=dn1n2s_1 = \frac{c}{n_2} \times \frac{n_1 d}{c} = \frac{d n_1}{n_2} .

Once the wavefront at B reaches the end of the slab, an additional time t1t_1 elapses. The time t1t_1 can be determined by considering the remaining distance the wavefront must travel in the slab, which is d−s1d - s_1 , and dividing it by the speed of light in the medium at B. This gives us t1=(d−s1c)n2=(d−dn1n2)n2c=d(n2−n1)ct_1 = \left(\frac{d - s_1}{c}\right) n_2 = \left(d - \frac{d n_1}{n_2}\right) \frac{n_2}{c} = \frac{d(n_2 - n_1)}{c} .

During this time t1t_1 , the wavefront at A will travel a distance s2s_2 . The distance s2s_2 is simply the speed of light in vacuum multiplied by the time t1t_1 , leading to s2=ct1=d(n2−n1)s_2 = c t_1 = d(n_2 - n_1) .

Finally, the angle θ\theta can be determined using the tangent function, where tan⁡θ\tan \theta is the ratio of the difference in distances traveled by the wavefronts in the two media to the height hh of the slab.

Therefore, tan⁡θ=(n2−n1)dh\tan \theta = \frac{(n_2 - n_1) d}{h} .

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