Question:

Interference pattern is observed at 'P' due to superposition of two rays coming out from a source 'S' as shown in the figure. The value of 'l' for which maxima is obtained at 'P' is: (R is perfect reflecting surface)

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Find the reflected path length from the geometry, add the extra half-wavelength phase shift on reflection from the mirror, and set the effective path difference equal to an integral multiple of the wavelength.
Updated On: Nov 11, 2026
  • \(l=\dfrac{2n\lambda}{\sqrt3-1}\)
  • \(l=\dfrac{(2n-1)\lambda}{2(\sqrt3-1)}\)
  • \(l=\dfrac{(2n-1)\lambda\sqrt3}{4(2-\sqrt3)}\)
  • \(l=\dfrac{(2n-1)\lambda}{\sqrt3-1}\)
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The Correct Option is C

Solution and Explanation

The direct ray travels SP = 2l. The reflected ray goes from S to the mirror at O and then to P. Taking the 30° angle as the angle made by the rays with the mirror (and with SP, which is parallel to the mirror), triangle SOP is isosceles with base angles 30° and half-base l.
SO = OP = l/cos 30° = 2l/\(\sqrt3\).
Reflected path = 4l/\(\sqrt3\).
Geometrical path difference = \(\frac{4l}{\sqrt3}-2l=\frac{2l(2-\sqrt3)}{\sqrt3}\).
Reflection from the perfectly reflecting surface adds a phase change of \(\pi\), i.e. an extra \(\lambda/2\).
For maxima: \(\frac{2l(2-\sqrt3)}{\sqrt3}+\frac{\lambda}{2}=n\lambda\), so \(\frac{2l(2-\sqrt3)}{\sqrt3}=\frac{(2n-1)\lambda}{2}\).
Hence \(l=\frac{(2n-1)\lambda\sqrt3}{4(2-\sqrt3)}\).
Answer: (3) \(l=\dfrac{(2n-1)\lambda\sqrt3}{4(2-\sqrt3)}\)
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