MCQMediumJEE 2023Refraction & Lenses

JEE Physics 2023 Question with Solution

A ray of light is incident from air on a glass plate having thickness 5cm\sqrt{5} \, cm and refractive index 2\sqrt{2}. The angle of incidence of a ray is equal to the critical angle for glass-air interface. The lateral displacement of the ray when it passes through the plate is <102cm<10^{-2} \, cm: (Given sin15=0.26\sin 15^\circ = 0.26)

  • A

    0.52cm0.52 \, cm

  • B

    0.45cm0.45 \, cm

  • C

    0.48cm0.48 \, cm

  • D

    0.50cm0.50 \, cm

Answer

Correct answer:A

Step-by-step solution

Standard Method

Given: thickness of glass plate t=5cmt = \sqrt{5} \, cm, refractive index μ=2\mu = \sqrt{2}, and angle of incidence is equal to the critical angle.

Find: lateral displacement of the ray through the plate.

For the glass-air interface, the critical angle θc\theta_c is given by

sinθc=1μ\sin \theta_c = \frac{1}{\mu}

So,

sinθc=12    θc=45\sin \theta_c = \frac{1}{\sqrt{2}} \implies \theta_c = 45^\circ

Hence the angle of incidence is i=45i = 45^\circ.

Using Snell's law at the first surface,

sinr=sin452=1/22=12\sin r = \frac{\sin 45^\circ}{\sqrt{2}} = \frac{1/\sqrt{2}}{\sqrt{2}} = \frac{1}{2}

Therefore,

r=30r = 30^\circ

The lateral displacement through a parallel-sided slab is

x=tsin(ir)secrx = t \sin(i-r) \sec r

Substituting the values,

x=5×sin(4530)×sec30x = \sqrt{5} \times \sin(45^\circ - 30^\circ) \times \sec 30^\circ x=5×sin15×sec30x = \sqrt{5} \times \sin 15^\circ \times \sec 30^\circ

Using sin15=0.26\sin 15^\circ = 0.26 and sec30=23\sec 30^\circ = \frac{2}{\sqrt{3}},

x=5×0.26×23x = \sqrt{5} \times 0.26 \times \frac{2}{\sqrt{3}} x=5×0.523=0.52cmx = \frac{\sqrt{5} \times 0.52}{\sqrt{3}} = 0.52 \, cm
Ray diagram of a glass slab showing incident ray, normals at both surfaces, critical angle c, refraction angle theta, refractive index mu equals root 2, and slab thickness marked vertically.

Therefore, the lateral displacement is 0.52cm0.52 \, cm. The correct option is A.

Common mistakes

  • Using the critical angle formula incorrectly as sinθc=μ\sin \theta_c = \mu. This is wrong because for glass to air, sinθc=1μ\sin \theta_c = \frac{1}{\mu}. First find θc\theta_c from the reciprocal of refractive index.

  • Taking the refracted angle inside the slab as 4545^\circ. This is wrong because Snell's law must still be applied at the first surface. Use sinr=siniμ\sin r = \frac{\sin i}{\mu} to get r=30r = 30^\circ.

  • Using an incorrect slab formula for lateral displacement. The displacement is not simply ttan(ir)t \tan(i-r) here. Use the standard relation x=tsin(ir)secrx = t \sin(i-r) \sec r for a parallel glass plate.

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