MCQEasyJEE 2023Diffraction & Polarisation

JEE Physics 2023 Question with Solution

Two polaroide A and B are placed in such a way that the pass-axis of polaroids are perpendicular to each other. Now, another polaroid C is placed between A and B bisecting the angle between them. If intensity of unpolarised light is I0I_0, then intensity of transmitted light after passing through polaroid B will be:

  • A

    I04\frac{I_0}{4}

  • B

    I02\frac{I_0}{2}

  • C

    I08\frac{I_0}{8}

  • D

    Zero

Answer

Correct answer:A

Step-by-step solution

Standard Method

Given: The pass-axes of polaroids A and B are perpendicular. Polaroid C is placed between them so that it bisects the angle, hence the angle between A and C is 4545^\circ and the angle between C and B is also 4545^\circ. The incident light is unpolarised with intensity I0I_0.

Find: The intensity after passing through polaroid B.

For unpolarised light passing through the first polaroid,

IA=I02I_A = \frac{I_0}{2}

Using Malus' law for polaroid C,

IC=IAcos245=I02×12=I04I_C = I_A \cos^2 45^\circ = \frac{I_0}{2} \times \frac{1}{2} = \frac{I_0}{4}

Again applying Malus' law for polaroid B,

IB=ICcos245=I04×12=I08I_B = I_C \cos^2 45^\circ = \frac{I_0}{4} \times \frac{1}{2} = \frac{I_0}{8}

Therefore, the transmitted intensity is I08\frac{I_0}{8}. The solution states the correct option is A, but this value corresponds to option C in the given options. Hence the defensible correct option is C.

Step-by-step Intensity Reduction

Given: Three polaroids are arranged in sequence. A and B are crossed, and C is inserted midway between their axes.

Find: Final transmitted intensity.

  1. After the first polaroid A, unpolarised light becomes plane polarised and its intensity becomes
I02\frac{I_0}{2}
  1. Since C bisects the angle between A and B, the angle between A and C is 4545^\circ.
  2. By Malus' law,
IC=I02cos245I_C = \frac{I_0}{2} \cos^2 45^\circ

Since

cos245=(12)2=12\cos^2 45^\circ = \left(\frac{1}{\sqrt{2}}\right)^2 = \frac{1}{2}

we get

IC=I02×12=I04I_C = \frac{I_0}{2} \times \frac{1}{2} = \frac{I_0}{4}
  1. The angle between C and B is also 4545^\circ, so
IB=ICcos245=I04×12=I08I_B = I_C \cos^2 45^\circ = \frac{I_0}{4} \times \frac{1}{2} = \frac{I_0}{8}

Therefore, the final transmitted light intensity is I08\frac{I_0}{8}.

Common mistakes

  • Applying crossed-polaroid logic directly to A and B and concluding the final intensity is zero. This is wrong because insertion of polaroid C changes the polarization direction in two stages. Use Malus' law successively for A \to C and C \to B.

  • Forgetting that unpolarised light loses half its intensity at the first polaroid. This is wrong because the first transmission gives IA=I02I_A = \frac{I_0}{2}, not I0I_0. Start from I02\frac{I_0}{2} before applying any cos2θ\cos^2 \theta factor.

  • Using cos45\cos 45^\circ instead of cos245\cos^2 45^\circ in Malus' law. This is wrong because transmitted intensity varies as the square of the cosine of the angle. Always use I=Iincos2θI = I_{\text{in}} \cos^2 \theta.

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