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Question: In modified YDSE setup $SS_1 - SS_2 = \frac{\lambda}{4}$ where $\lambda$ is wavelength of light used...

In modified YDSE setup SS1SS2=λ4SS_1 - SS_2 = \frac{\lambda}{4} where λ\lambda is wavelength of light used. S1S_1 & S2S_2 are two slits separated by distance dd. A screen is placed at distance D(D>>d>>λ)D (D>> d>> \lambda). Source is also placed at distance DD from slits asymmetrically such that source SS is below the central line CCCC'. (CS1=S2CCS_1 = S_2C). If point PP is corresponding to central maxima then angle θ\theta is

Answer

θ=sin1(λ4d)\theta = \sin^{-1}\left(\frac{\lambda}{4d}\right)

Explanation

Solution

  1. The source introduces an initial path difference so that
SS1SS2=λ4ϕ0=2πλλ4=π2.SS_1 - SS_2 = \frac{\lambda}{4} \quad \Longrightarrow \quad \phi_0 = \frac{2\pi}{\lambda}\cdot\frac{\lambda}{4} = \frac{\pi}{2}.
  1. On the screen at an angle θ\theta, the extra path difference from the slits is
δ=dsinθϕ=2πλdsinθ.\delta = d\sin \theta \quad\Longrightarrow\quad \phi = \frac{2\pi}{\lambda}\,d\sin\theta.
  1. For the resultant phase difference to yield a central maximum (bright fringe), the total phase difference must be zero modulo 2π2\pi. That is, for the principal maximum,
2πλdsinθπ2=0.\frac{2\pi}{\lambda}\,d\sin \theta - \frac{\pi}{2} = 0.
  1. Solving for θ\theta:
2πλdsinθ=π2dsinθ=λ4θ=sin1(λ4d).\frac{2\pi}{\lambda}\,d\sin \theta = \frac{\pi}{2} \quad \Longrightarrow \quad d\sin\theta = \frac{\lambda}{4} \quad \Longrightarrow \quad \theta = \sin^{-1}\left(\frac{\lambda}{4d}\right).

Minimal Explanation

The initial phase difference from the source is π/2\pi/2. For maximum, the additional phase difference from the path difference dsinθd\sin\theta must cancel this, leading to dsinθ=λ/4d\sin\theta=\lambda/4 and hence θ=sin1(λ/(4d))\theta=\sin^{-1}(\lambda/(4d)).