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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 Young's double-slit experiment, the intensity at a point is...

In Young's double-slit experiment, the intensity at a point is (14)\left(\dfrac{1}{4}\right) of the maximum intensity. The angular position of this point is
\{\lambda =\text{ wavelength }\text{ of }\text{ light }\text{ used }, d =\text{ separation }\text{ between }\text{ the }\text{ two }\text{ slits }, \cos(60)^{}^{\circ} = \dfrac{1}{2}\}

Options

  1. Asin⁡−1(λd)\sin^{-1} \left(\dfrac{\lambda}{d}\right)
  2. Bsin⁡−1(λ2d)\sin^{-1} \left(\dfrac{\lambda}{2d}\right)
  3. Csin⁡−1(λ3d)\sin^{-1} \left(\dfrac{\lambda}{3d}\right)
  4. Dsin⁡−1(λ4d)\sin^{-1} \left(\dfrac{\lambda}{4d}\right)

Correct answer

C. sin⁡−1(λ3d)\sin^{-1} \left(\dfrac{\lambda}{3d}\right)

Step-by-step solution

The intensity at a point in Young's double-slit experiment is given by I=I0cos⁡2(ϕ2),whereI = I_0 \cos^2 \left(\dfrac{\phi}{2}\right), whereI_0 is the maximum intensity and ϕ\phi is the phase difference.

Given I=I =\dfrac{I_0}{4}

\dfrac{I_0}{4} =I0cos⁡2(ϕ2)I_0 \cos^2 \left(\dfrac{\phi}{2}\right)

cos⁡(ϕ2)=12\cos\left(\dfrac{\phi}{2}\right) = \dfrac{1}{2}

ϕ2=π3⇒ϕ=2π3\dfrac{\phi}{2} = \dfrac{\pi}{3} \Rightarrow \phi = \dfrac{2\pi}{3}

The phase difference ϕ\phi is related to the path difference Δx\Delta x by ϕ=2πλΔx\phi = \dfrac{2\pi}{\lambda} \Delta x

2π3=2πλΔx⇒Δx=λ3\dfrac{2\pi}{3} = \dfrac{2\pi}{\lambda} \Delta x \Rightarrow \Delta x = \dfrac{\lambda}{3}

The path difference is also given by Δx=dsin⁡θ\Delta x = d \sin \theta

dsin⁡θ=λ3d \sin \theta = \dfrac{\lambda}{3}

sin⁡θ=λ3d\sin \theta = \dfrac{\lambda}{3d}

θ=sin⁡−1(λ3d)<br><br>Answer:\theta = \sin^{-1} \left(\dfrac{\lambda}{3d}\right)<br><br>Answer:\sin^{-1} \left(\dfrac{\lambda}{3d}\right)
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