MCQEasyJEE 2025Refraction & Lenses

JEE Physics 2025 Question with Solution

What is the lateral shift of a ray refracted through a parallel-sided glass slab of thickness hh in terms of the angle of incidence ii and angle of refraction rr, if the glass slab is placed in air medium?

  • A

    htan(ir)tanr\frac{h \, \tan(i - r)}{\tan r}

  • B

    hcos(ir)sinr\frac{h \, \cos(i - r)}{\sin r}

  • C

    hh

  • D

    hsin(ir)cosr\frac{h \, \sin(i - r)}{\cos r}

Answer

Correct answer:D

Step-by-step solution

Standard Method

Given: A parallel-sided glass slab of thickness hh is placed in air. A ray is incident at angle ii and refracts inside the slab at angle rr.

Find: The lateral shift of the emergent ray.

Concept: In a parallel-sided slab, the ray emerges parallel to the incident ray but gets displaced sideways. This sideways displacement is called the lateral shift.

From the geometry of refraction in the slab, the lateral shift is

S=hsin(ir)cosrS = \frac{h \sin(i-r)}{\cos r}

where hh is the slab thickness, ii is the angle of incidence, and rr is the angle of refraction.

Therefore, the correct formula for the lateral shift is

hsin(ir)cosr\frac{h \sin(i-r)}{\cos r}

So, the correct option is D.

Geometrical Derivation

Given: Thickness of slab hh, angle of incidence ii, and angle of refraction rr.

Find: Lateral shift dd.

Inside the slab, the ray travels along a slanted path. If the refracted path length inside the slab is LL, then from geometry

L=hsecrL = h \sec r

The lateral shift is the component of this path associated with the angle difference iri-r. Hence,

d=Lsin(ir)d = L \sin(i-r)

Substituting L=hsecrL = h \sec r,

d=hsecrsin(ir)d = h \sec r \cdot \sin(i-r)

Using secr=1cosr\sec r = \frac{1}{\cos r},

d=hsin(ir)cosrd = \frac{h \sin(i-r)}{\cos r}

Thus, the lateral shift is hsin(ir)cosr\frac{h \sin(i-r)}{\cos r}, so the correct option is D.

Common mistakes

  • Using the slab thickness hh itself as the lateral shift is incorrect because the shift depends on both ii and rr. Always use the geometrical relation involving the angles of incidence and refraction.

  • Confusing the trigonometric factor in the denominator is a common error. The correct expression contains cosr\cos r in the denominator, not sinr\sin r or tanr\tan r, because the internal path length is related through secr\sec r.

  • Assuming the emergent ray is not parallel to the incident ray leads to a wrong setup. In a parallel-sided slab, the emergent ray is parallel to the incident ray, and only a lateral displacement occurs.

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