NVAMediumJEE 2023Diffraction & Polarisation

JEE Physics 2023 Question with Solution

Unpolarised light of intensity 32Wm232 \, \text{Wm}^{-2} passes through the combination of three polaroids such that the pass axis of the last polaroid is perpendicular to that of the pass axis of the first polaroid. If the intensity of the emerging light is 3Wm23 \, \text{Wm}^{-2}, then the angle between the pass axis of the first two polaroids is:

Answer

Correct answer:30

Step-by-step solution

Using Malus law

Given: Unpolarised light of intensity I0=32Wm2I_0 = 32 \, \text{Wm}^{-2} passes through three polaroids. The pass axis of the third polaroid is perpendicular to that of the first. The emerging intensity is Inet=3Wm2I_{\text{net}} = 3 \, \text{Wm}^{-2}.

Find: The angle θ\theta between the pass axes of the first two polaroids.

After the first polaroid, the intensity becomes

I1=I02I_1 = \frac{I_0}{2}

If the angle between the first and second polaroids is θ\theta, then after the second polaroid,

I2=I02cos2θI_2 = \frac{I_0}{2}\cos^2\theta

Since the third polaroid is perpendicular to the first, the angle between the second and third polaroids is 90θ90^\circ - \theta. Therefore, after the third polaroid,

Inet=I2cos2(90θ)I_{\text{net}} = I_2 \cos^2(90^\circ - \theta)

Using cos(90θ)=sinθ\cos(90^\circ - \theta) = \sin\theta,

Inet=I02cos2θsin2θI_{\text{net}} = \frac{I_0}{2}\cos^2\theta \sin^2\theta

Using sin2(2θ)=4cos2θsin2θ\sin^2(2\theta) = 4\cos^2\theta\sin^2\theta,

Inet=I08sin2(2θ)I_{\text{net}} = \frac{I_0}{8}\sin^2(2\theta)

Substitute Inet=3I_{\text{net}} = 3 and I0=32I_0 = 32:

3=328sin2(2θ)3 = \frac{32}{8}\sin^2(2\theta) 3=4sin2(2θ)3 = 4\sin^2(2\theta) sin2(2θ)=34\sin^2(2\theta) = \frac{3}{4} sin(2θ)=32\sin(2\theta) = \frac{\sqrt{3}}{2}

Hence,

2θ=60 or 1202\theta = 60^\circ \text{ or } 120^\circ θ=30 or 60\theta = 30^\circ \text{ or } 60^\circ

Therefore, the angle between the pass axes of the first two polaroids is 3030^\circ or 6060^\circ.

Ray diagram of three polaroid arrangement showing incident unpolarised intensity, intermediate axes, angle theta, and intensity changes labeled I0 by 2 and I0 by 8.

Stepwise intensity tracking

Given: Initial unpolarised intensity 32Wm232 \, \text{Wm}^{-2} and final intensity 3Wm23 \, \text{Wm}^{-2}.

Find: Possible values of θ\theta.

  1. Unpolarised light passing through the first polaroid gives
I1=322=16Wm2I_1 = \frac{32}{2} = 16 \, \text{Wm}^{-2}
  1. After the second polaroid at angle θ\theta,
I2=16cos2θI_2 = 16\cos^2\theta
  1. The third polaroid is perpendicular to the first, so its angle with the second is 90θ90^\circ - \theta. Thus,
Inet=16cos2θcos2(90θ)I_{\text{net}} = 16\cos^2\theta \cos^2(90^\circ - \theta) Inet=16cos2θsin2θI_{\text{net}} = 16\cos^2\theta \sin^2\theta
  1. Since the final intensity is 3Wm23 \, \text{Wm}^{-2},
3=16cos2θsin2θ3 = 16\cos^2\theta \sin^2\theta
  1. Rewrite using
4cos2θsin2θ=sin2(2θ)4\cos^2\theta \sin^2\theta = \sin^2(2\theta)

So,

3=4sin2(2θ)3 = 4\sin^2(2\theta) sin2(2θ)=34\sin^2(2\theta) = \frac{3}{4}
  1. Therefore,
sin(2θ)=32\sin(2\theta) = \frac{\sqrt{3}}{2}

which gives

2θ=60,1202\theta = 60^\circ, 120^\circ

Hence,

θ=30,60\theta = 30^\circ, 60^\circ

So the required numerical values are 3030 and 6060.

Common mistakes

  • Taking the intensity after the first polaroid as unchanged. This is wrong because unpolarised light loses half its intensity after passing through the first polaroid. Use I1=I0/2I_1 = I_0/2 first.

  • Using angle θ\theta again for the third polaroid. This is wrong because the third polaroid is perpendicular to the first, so the angle between the second and third axes is 90θ90^\circ - \theta. Apply Malus law with that angle.

  • Forgetting the identity connecting cos2θsin2θ\cos^2\theta\sin^2\theta with sin2(2θ)\sin^2(2\theta). This can lead to incorrect algebra. Use sin2(2θ)=4cos2θsin2θ\sin^2(2\theta)=4\cos^2\theta\sin^2\theta to simplify.

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