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Question: If the first minima in Young’s double-slit experiment occur directly in front of the slits (distance...

If the first minima in Young’s double-slit experiment occur directly in front of the slits (distance between slit and screen D=12cmD = 12cm and distance between slits d=5cmd = 5cm, then the wavelength of the radiation used can be
A. 2cm2cm
B. 4cm4cm
C. 23cm\dfrac{2}{3}cm
D. 43cm\dfrac{4}{3}cm

Explanation

Solution

Superposition principle says when two or more waves overlap in space, the resultant disturbance is the sum of the individual disturbances.
In this question, it is given that a first minimum obtained on the screen is directly in front of the slits; hence we have to find the wavelength of the radiation given as x=(2n1)λ2\vartriangle x = \left( {2n - 1} \right)\dfrac{\lambda }{2}. First we need to evaluate the distance travelled by the radiated light in between the two slits one by one and then, equating their difference with the formula x=(2n1)λ2\vartriangle x = \left( {2n - 1} \right)\dfrac{\lambda }{2} to get the result.

Complete step by step solution:
Distance between screen and slit D=12cmD = 12cm
Distance between slits d=5cmd = 5cm
First minima fall directly in front of the slit S1{S_1} at point P


Distance travelled by wave from S1{S_1}to {S_1}P$$$$ = 12cm
The path travelled by light from slit S2{S_2}to {S_2}P$$$$ = \sqrt {{D^2} + {d^2}} = \sqrt {{{12}^2} + {5^2}} = \sqrt {144 + 25} = \sqrt {169} = 13cm
So the path difference between two minima x=S2PS1P=1312=1cm\vartriangle x = {S_2}P - {S_1}P = 13 - 12 = 1cm
Given the point for first minima(n=1)\left( {n = 1} \right), x=(2n1)λ2=(2×x1)λ2=λ2\vartriangle x = \left( {2n - 1} \right)\dfrac{\lambda }{2} = \left( {2 \times x - 1} \right)\dfrac{\lambda }{2} = \dfrac{\lambda }{2}
Hence we can write:

x=λ2 λ2=1 λ=2cm  \vartriangle x = \dfrac{\lambda }{2} \\\ \dfrac{\lambda }{2} = 1 \\\ \lambda = 2cm \\\

Hence the wavelength of the radiation is 2cm Option A.

Note: A point on the screen where the wave crest of one wave falls on the wave crest of other, the resultant amplitude is maxima. A point on the screen where the wave crest of one falls on the wave trough of another, the resulting amplitude is minima.