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Wave Optics question

2019 · 12 Apr · Shift 1 · Q59
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Wave Optics question

2019 · 12 Apr · Shift 1 · Q59

JEE MainPhysicsWave OpticsMCQ+4 / −1
In a double slit experiment, when a thin film of thickness t having refractive index μ\muμ. is introduced in front of one of the slits, the maximum at the centre of the fringe pattern shifts by one fringe width. The value of t is (λ\lambdaλ is the wavelength of the light used) :
  1. A
    λ2(μ−1){\lambda \over {2\left( {\mu - 1} \right)}}2(μ−1)λ​
  2. B
    λ(2μ−1){\lambda \over {\left( {2\mu - 1} \right)}}(2μ−1)λ​
  3. C
    2λ(μ−1){{2\lambda } \over {\left( {\mu - 1} \right)}}(μ−1)2λ​
  4. D
    λ(μ−1){\lambda \over {\left( {\mu - 1} \right)}}(μ−1)λ​
View written solutionFree

Correct answer: D

  1. Effect of introducing a thin film in one path

When a thin film of thickness ttt and refractive index μ\muμ is placed in front of one slit, the optical path in that arm increases by

Δ=(μ−1)t\Delta = (\mu - 1)tΔ=(μ−1)t

This is the extra optical path difference introduced between the two waves.

  1. Relation between fringe shift and path difference

In Young’s double slit experiment, if an extra path difference Δ\DeltaΔ is introduced, the fringe pattern shifts by

n=Δλn = \frac{\Delta}{\lambda}n=λΔ​

fringe widths.

Given that the central maximum shifts by one fringe width, we have

Δλ=1\frac{\Delta}{\lambda} = 1λΔ​=1

So,

Δ=λ\Delta = \lambdaΔ=λ

  1. Substitute the expression for Δ\DeltaΔ

(μ−1)t=λ(\mu - 1)t = \lambda(μ−1)t=λ

Therefore,

t=λμ−1t = \frac{\lambda}{\mu - 1}t=μ−1λ​

  1. Match with the options

This corresponds to:

λμ−1\boxed{\frac{\lambda}{\mu - 1}}μ−1λ​​

So the correct option is D.

  1. Comparison with stored correct answer

Stored correct answer: D

Derived answer: D

Hence, the derived answer agrees with the stored correct answer.

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