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CBSE Class 12 Physics 2019 Outside Delhi Set 1 Paper

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Question : 26 of 27
Marks: +1, -0
Explain, with the help of a diagram, how plane polarized light can be produced by scattering of light from the Sun.
Two polaroids P1P_1 and P2P_2 are placed with their pass axes perpendicular to each other. Unpolarised light of intensity II is incident on P1P_1. A third polaroid P3P_3 is kept between P1P_1 and P2P_2 such that its pass axis makes an angle of 4545^{\circ} with that of P1P_1. Calculate the intensity of light transmitted through P1,P2P_1, P_2 and P3P_3.
OR
(a) Why cannot the phenomenon of interference be observed by illuminating two pin holes with two sodium lamps?
(b) Two monochromatic waves having displacements y1=acosωty_1 = a \cos \omega t and y2=acosy_2 = a \cos (ωt+f)(\omega t + f) from two coherent sources interfere to produce an interference pattern. Derive the expression for the resultant intensity and obtain the conditions for constructive and destructive interference.
(c) Two wavelengths of sodium light of 590 nm590 \text{ nm} and 596 nm596 \text{ nm} are used in turn to study the diffraction taking place at a single slit of aperture 2×106 m2 \times 10^{-6} \text{ m}. If the distance between the slit and the screen is 1.5 m1.5 \text{ m}. Calculate the separation between the positions of the second maxima of diffraction pattern obtained in the two cases.
Solution:  
ns. Diagram production of polarized light by scattering of sun light
● Explanation
● Calculation of intensity of light transmitted through P1,P2P_1, P_2 and P3P_3
Diagram :
Explanation: Charges accelerating parallel to the double arrows do not radiate energy towards the observer. The radiation scattered by the molecules therefore is polarised perpendicular to the plane of the figure.
Alternatively: If the student writes " scattered light when viewed in a perpendicular direction is found to be polarised
(Award one mark) Intensity of light transmitted by 1  st  1^{\;\text{st}\;} Polaroid is,
I1=I2I_1 = \frac{I}{2}
Intensity of light transmitted by 2  nd  2^{\;\text{nd}\;} Polaroid is,
I2=I1cos245I_2 = I_1 \cos^2 45^{\circ} =I2(12)2=I4= \frac{I}{2} \left( \frac{1}{\sqrt{2}} \right)^2 = \frac{I}{4}
Intensity of light transmitted by 3  rd  3^{\;\text{rd}\;} Polaroid is,
I3=I1cos245I_3 = I_1 \cos^2 45^{\circ} =I2(12)2=I8= \frac{I}{2} \left( \frac{1}{\sqrt{2}} \right)^2 = \frac{I}{8}
OR
● Reason
● Deriving the expression for resultant intensity and condition for constructive and destructive interference
● Calculating the separation
(a) Because two independent sources cannot be coherent OR they are not coherent
(b) y1=acosωty_1 = a \cos \omega t
y2=acos(ωt+ϕ)y_2 = a \cos (\omega t + \phi)
So resultant displacement is give by
y=y1+y2y = y_1 + y_2
y=acosωt+acos(ωt+ϕ)y = a \cos \omega t + a \cos (\omega t + \phi)
y=2acos(ϕ2)cos(ωt+ϕ2)y = 2a \cos \left( \frac{\phi}{2} \right) \cos \left( \omega t + \frac{\phi}{2} \right)
The amplitude of the resultant displacement is 2πcos(ϕ2)2\pi \cos \left( \frac{\phi}{2} \right) and therefore intensity at that point will be I=4I0cos2(ϕ2)I = 4 I_0 \cos^2 \left( \frac{\phi}{2} \right)
For constructive interference:
ϕ=0,±2π,±4π,\phi = 0, \pm 2\pi, \pm 4\pi, \dots
For destructive interference:
ϕ=0,±π,±3π,±5π,\phi = 0, \pm \pi, \pm 3\pi, \pm 5\pi, \dots
(c) Position of second maxima,
y2=5λ2λDay_2 = \frac{5\lambda}{2} \frac{\lambda D}{a}
Separation between the positions of the second maxima with λ1\lambda_1 and λ2\lambda_2 is:
Δy=5D(λ2λ1)2a\Delta y = \frac{5 D (\lambda_2 - \lambda_1)}{2a}
=5×1.5×(596590)×1092×2×106= \frac{5 \times 1.5 \times (596-590) \times 10^{-9}}{2 \times 2 \times 10^{-6}}
=11.25×103 m= 11.25 \times 10^{-3} \text{ m}
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