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Geometrical Optics question

2023 · Shift 2 · Q39
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Geometrical Optics question

2023 · Shift 2 · Q39

JEE AdvancedPhysicsGeometrical OpticsMultiple correct+4 / −2
A monochromatic light wave is incident normally on a glass slab of thickness ddd, as shown in the figure. The refractive index of the slab increases linearly from n1n_1n1​ to n2n_2n2​ over the height hhh. 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 8 English
  1. 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]tan−1[2h(n22​−n12​)d​].
  2. 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]tan−1[h(n2​−n1​)d​].
  3. C
    It will not deflect.
  4. D
    The deflection angle depends only on (n2−n1)\left(n_2-n_1\right)(n2​−n1​) and not on the individual values of n1n_1n1​ and n2n_2n2​.
View written solutionFree

Correct answer: B, D

  1. Given refractive index variation

The refractive index varies linearly with height yyy:

n(y)=n1+n2−n1hyn(y)=n_1+\frac{n_2-n_1}{h}yn(y)=n1​+hn2​−n1​​y

So,

dndy=n2−n1h=constant\frac{dn}{dy}=\frac{n_2-n_1}{h}=\text{constant}dydn​=hn2​−n1​​=constant

The light is incident normally on the slab, so initially its direction is along the horizontal xxx-axis.


  1. Ray equation in a medium with transverse refractive index gradient

For a stratified medium where nnn varies with yyy, the ray bends continuously. Using the standard ray equation for small bending,

dds(ndr⃗ds)=∇n\frac{d}{ds}\left(n\frac{d\vec r}{ds}\right)=\nabla ndsd​(ndsdr​)=∇n

Since the ray mainly moves along xxx, we take ds≈dxds\approx dxds≈dx, and the transverse component gives

ddx(ndydx)=dndy\frac{d}{dx}\left(n\frac{dy}{dx}\right)=\frac{dn}{dy}dxd​(ndxdy​)=dydn​

Initially, the ray enters normally, so

dydx∣x=0=0\left.\frac{dy}{dx}\right|_{x=0}=0dxdy​​x=0​=0

Over slab thickness ddd, integrating,

ndydx=dndyxn\frac{dy}{dx}=\frac{dn}{dy}xndxdy​=dydn​x

At exit x=dx=dx=d, for small angle θ\thetaθ,

tan⁡θ≈dydx∣x=d\tan\theta \approx \frac{dy}{dx}\Big|_{x=d}tanθ≈dxdy​​x=d​

A simpler and exact optical-path argument for this linear gradient gives the transverse change in direction as

tan⁡θ=d dndy\tan\theta = d\,\frac{dn}{dy}tanθ=ddydn​

Thus,

tan⁡θ=d⋅n2−n1h\tan\theta=d\cdot \frac{n_2-n_1}{h}tanθ=d⋅hn2​−n1​​

Hence,

θ=tan⁡−1((n2−n1)dh)\theta=\tan^{-1}\left(\frac{(n_2-n_1)d}{h}\right)θ=tan−1(h(n2​−n1​)d​)

Since refractive index increases upward, the ray bends toward higher refractive index, i.e. upward.

So Option B is correct.


  1. Check Option A

Option A says

θ=tan⁡−1[(n22−n12)d2h]\theta=\tan^{-1}\left[\frac{(n_2^2-n_1^2)d}{2h}\right]θ=tan−1[2h(n22​−n12​)d​]

This would involve the average of nnn in a way not supported by the ray equation. The correct result depends on the gradient

dndy=n2−n1h\frac{dn}{dy}=\frac{n_2-n_1}{h}dydn​=hn2​−n1​​

not on n22−n122h\frac{n_2^2-n_1^2}{2h}2hn22​−n12​​.

So Option A is false.


  1. Check Option C

Because the refractive index varies with height, different parts of the wavefront move with different speeds. This causes the wavefront to tilt and the ray to bend toward larger nnn.

Therefore, the emergent ray does deflect.

So Option C is false.


  1. Check Option D

From the derived result,

θ=tan⁡−1((n2−n1)dh)\theta=\tan^{-1}\left(\frac{(n_2-n_1)d}{h}\right)θ=tan−1(h(n2​−n1​)d​)

Thus the deflection depends on n2−n1n_2-n_1n2​−n1​ only, not on the individual values of n1n_1n1​ and n2n_2n2​ separately.

So Option D is correct.


  1. Final answer

Correct statements are:

B, D\boxed{\text{B, D}}B, D​


  1. Comparison with stored correct answer

Stored correct answer: B, D

My derived answer: B, D

They match.

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