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MHT CET 202625 AprilMorning Shift
Exam
MHT CET
Year
2026
Date
25 April
Shift
Morning Shift
Subject
Physics
Chapter
Wave Optics

MHT CET 2026 · 25 April · Morning Shift · Physics · Wave Optics

In a single-slit Fraunhofer diffraction experiment, the first...

In a single-slit Fraunhofer diffraction experiment, the first secondary minimum is observed at an angle of 30^{}^{\circ} for light of wavelength λ\lambda. If the same slit is now illuminated by light of the same wavelength, the angular position (\theta) of the first secondary maximum is<br>(\sin 30^{}^{\circ} = \dfrac{1}{2}).

Options

  1. Asin⁡−1(1/2)\sin^{-1}(1/2)
  2. Bsin⁡−1(1/4)\sin^{-1}(1/4)
  3. Csin⁡−1(3/4)\sin^{-1}(3/4)
  4. Dsin⁡−1(1/3)\sin^{-1}(1/3)

Correct answer

C. sin⁡−1(3/4)\sin^{-1}(3/4)

Step-by-step solution

For a single-slit Fraunhofer diffraction, the condition for the nn-th secondary minimum is given by:

asin⁡θ=nλa \sin \theta = n\lambda

For the first secondary minimum (n=1n=1) at \theta = 30^{}^{\circ}:

a \sin 30^{}^{\circ} = \lambda

a(12)=λ⇒a=2λa \left(\dfrac{1}{2}\right) = \lambda \Rightarrow a = 2\lambda

The condition for the nn-th secondary maximum is given by:

asin⁡θ′=(n+12)λa \sin \theta' = \left(n + \dfrac{1}{2}\right)\lambda

For the first secondary maximum (n=1n=1):

asin⁡θ′=3λ2a \sin \theta' = \dfrac{3\lambda}{2}

Substituting a=2λa = 2\lambda into the equation:

(2λ)sin⁡θ′=3λ2(2\lambda) \sin \theta' = \dfrac{3\lambda}{2}

sin⁡θ′=34\sin \theta' = \dfrac{3}{4}

θ′=sin⁡−1(34)<br><br>Answer:sin⁡−1(3/4)\theta' = \sin^{-1} \left(\dfrac{3}{4}\right)<br><br>Answer: \sin^{-1}(3/4)
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