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MHT CET 202623 AprilEvening Shift
Exam
MHT CET
Year
2026
Date
23 April
Shift
Evening Shift
Subject
Physics
Chapter
Wave Optics

MHT CET 2026 · 23 April · Evening Shift · Physics · Wave Optics

In a diffraction pattern due to a single slit of width a, the first...

In a diffraction pattern due to a single slit of width a, the first minimum is observed at an angle 30∘30^\circ when light of wavelength 50005000 Å is incident on the slit. The first secondary maximum is observed at an angle of
{sin⁡(30)∘=cos⁡(60)∘=12}\{\sin(30)^\circ = \cos(60)^\circ = \dfrac{1}{2}\}

Options

  1. Asin⁡−1(23)\sin^{-1}\left(\dfrac{2}{3}\right)
  2. Bsin⁡−1(12)\sin^{-1}\left(\dfrac{1}{2}\right)
  3. Csin⁡−1(34)\sin^{-1}\left(\dfrac{3}{4}\right)
  4. Dsin⁡−1(14)\sin^{-1}\left(\dfrac{1}{4}\right)

Correct answer

C. sin⁡−1(34)\sin^{-1}\left(\dfrac{3}{4}\right)

Step-by-step solution

The condition for the first minimum in a single slit diffraction pattern is given by asin⁡θ=λa \sin \theta = \lambda.

Substituting θ=30∘\theta = 30^\circ, we get asin⁡30∘=λa \sin 30^\circ = \lambda.

Since sin⁡30∘=12\sin 30^\circ = \dfrac{1}{2}, we have a(12)=λa \left(\dfrac{1}{2}\right) = \lambda, which gives a=2λa = 2\lambda.

The condition for the first secondary maximum is given by asin⁡θ′=3λ2a \sin \theta' = \dfrac{3\lambda}{2}.

Substituting a=2λa = 2\lambda, we get 2λsin⁡θ′=3λ22\lambda \sin \theta' = \dfrac{3\lambda}{2}.

Solving for sin⁡θ′\sin \theta', we get sin⁡θ′=34\sin \theta' = \dfrac{3}{4}.

Therefore, θ′=sin⁡−1(34)\theta' = \sin^{-1}\left(\dfrac{3}{4}\right).

Answer: $\sin^{-1}\left(\dfrac{3}{4}\right)
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