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Question: In a YDSE, \(d = 0.1mm\) and distance between slits and screen \(D = 1m\) . At some point P on the s...

In a YDSE, d=0.1mmd = 0.1mm and distance between slits and screen D=1mD = 1m . At some point P on the screen, resulting intensity is equal to the intensity due to either of the individual slits. Then distance of P from the central maxima: (λ=6000A)(\lambda = 6000{\rm A})
A. 1mm
B. 0.5mm0.5mm
C. 0.25mm0.25mm
D. 2mm2mm

Explanation

Solution

Hint We know that the intensity at any point in YDSE is given by I=Imaxcos2ϕ2I = {I_{\max }}{\cos ^2}\dfrac{\phi }{2} where, ϕ\phi is phase difference. Now using phase difference, we can calculate the path difference between the light waves. Once the path difference is known we can equate the equations of path difference to get the desired result.

Complete Step by step solution let the individual intensity of both the slits be Io{I_o}.
Now we know that the resultant intensity at any point in YDSE is given by,
I=Imaxcos2ϕ2......(1)I = {I_{\max }}{\cos ^2}\dfrac{\phi }{2}......(1)
Where, ϕ\phi is phase difference.
If Io{I_o} be the individual intensity of both the slits then,
Imax=(Io+Io)2 Imax=(2Io)2 Imax=4IO......(2)  {I_{\max }} = {(\sqrt {{I_o}} + \sqrt {{I_o}} )^2} \\\ {I_{\max }} = {(2\sqrt {{I_o}} )^2} \\\ {I_{\max }} = 4{I_O}......(2) \\\
Now according to question intensity at point is given by intensity due to single slit i.e. I=IoI = {I_o}
From equation (1) and (2), we get
I0=4Iocos2ϕ2 cos2ϕ2=14 cosϕ2=12   {I_0} = 4{I_o}{\cos ^2}\dfrac{\phi }{2} \\\ {\cos ^2}\dfrac{\phi }{2} = \dfrac{1}{4} \\\ \cos \dfrac{\phi }{2} = \dfrac{1}{2} \\\ \\\
Hence from above we have,
ϕ2=π3 ϕ=2π3......(3)  \dfrac{\phi }{2} = \dfrac{\pi }{3} \\\ \phi = \dfrac{{2\pi }}{3}......(3) \\\
Now, phase difference = 2πλ\dfrac{{2\pi }}{\lambda } path difference
ϕ=2πλΔx\phi = \dfrac{{2\pi }}{\lambda }\Delta x where, Δx\Delta x is path difference.
Using equation (1) we get,
2π3=2πλΔx Δx=λ3......(4)  \dfrac{{2\pi }}{3} = \dfrac{{2\pi }}{\lambda }\Delta x \\\ \therefore \Delta x = \dfrac{\lambda }{3}......\left( 4 \right) \\\
We know that the path difference is given by,
Δx=ydD......(5)\Delta x = \dfrac{{yd}}{D}......(5)
Where,yy is the distance of point P from central maxima.
Hence finally using equation (4) and (5) we get,
λ3=ydD y=λD3d  \dfrac{\lambda }{3} = \dfrac{{yd}}{D} \\\ y = \dfrac{{\lambda D}}{{3d}} \\\
On putting the values, we get
y=6000×1010×13×0.1×103 y=2×103 y=2mm  y = \dfrac{{6000 \times {{10}^{ - 10}} \times 1}}{{3 \times 0.1 \times {{10}^{ - 3}}}} \\\ y = 2 \times {10^{ - 3}} \\\ y = 2mm \\\
Hence distance of point P from central maxima is 2mm2mm.

Option (C) is correct.

Note
Imax{I_{\max }} and Imin{I_{\min }} is calculated by using the formula of resultant intensity at any point that is given by:
I=IA+IB+2IAIBcosδI = {I_A} + {I_B} + 2{I_A}{I_B}\cos \delta
For maximum intensity, δ=1\delta = 1
I=IA+IB+2IAIB I=(IA+IB)2  \therefore I = {I_A} + {I_B} + 2{I_A}{I_B} \\\ I = {(\sqrt {{I_A}} + \sqrt {{I_B}} )^2} \\\

For minimum intensity, δ=1\delta = - 1
I=IA+IB2IAIB I=(IAIB)2  \therefore I = {I_A} + {I_B} - 2{I_A}{I_B} \\\ I = {(\sqrt {{I_A}} - \sqrt {{I_B}} )^2} \\\