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Question

A parallel beam of visible light consisting of wavelengths λ1 & λ2 is incident on a standard YDSE apparatus with d=1 mm,D=1 m. P is a point on the screen at a distance y from center of screen O. y=y1 is the nearest point above O where the two maxima coincide and y=y2 is the nearest point above O where the two minima coincide. β1 & β2 are fringe width corresponding to wave length λ1 & λ2.

Column_IColumn-II(A) β1=0.3 mm,β2=0.5 mm(P) The 2nd nearest point above O where two maxima coincide is y=2y1(B) β1=0.3 mm,β2=0.4 mm(Q)y2 has no finite value(C) β1=0.2 mm,β2=0.4 mm(R) The 2nd nearest point above O where the two minima coincide is y=3y2(D) β1=0.2 mm,β2=0.6 mm(S) y1=LCM of β1 and β2(T) The 2nd nearest point above O where two minima coincide is y=2y2
Which of the following option has the correct combination considering column-I and column-II ?

A
CR,T
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B
AQ,S
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C
DP,R,S
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D
BQ,T,S
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Solution

The correct option is C DP,R,S
For maxima the distance of nth bright fringe from center O is
yn=nDλd=nβ
Given that y=y1 is the nearest point above O, where nth1 maxima of wavelength λ1 coincides with nth2 maxima of wavelength λ2
y1=n1β1=n2β2= LCM of β1 and β2
For y=2y1=2n1β1=2n2β2
Hence at this point both maxima again coincide.
Similary for minima, distance of nth dark fringe from center O is
yn=(2n±1)Dλ2d=(2n±1)β2

Given that y=y2 is the nearest point above O, where nth1 minima of wavelength λ1 coincides with nth2 minima of wavelength λ2
y2=(n112)β1=(n212)β2
β1β2=n212n112
β1β2=2n212n11
Which will have a solution only if β1β2 expressed as a proper fraction of form oddodd.
Option B & C :β1β2 is not of form oddodd. hence not real value of y2 exists.
Hence at some finite y2 the two minima will coincide.
At y=2y2 the two maxima (and not minima) will coincide.
y=3y2 is the next nearest point where minima coincide.


AP,R,S;:BP,Q,R,S:CP,Q,R,S:DP,R,S

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