Download JEE MCQs for JEE Physics: Wave Optics
Explore reliable objective questions for Wave Optics tailored for JEE learners. Utilizing these Physics multiple-choice formats ensures thorough preparation and strengthens problem-solving speed for upcoming school assessments.
Chapter-wise Objective Questions: Wave Optics
Navigate directly to the 50 objective questions for Wave Optics using the digital viewer below. Each practice set includes verified answer keys, allowing students to instantly cross-check their work and identify areas requiring further revision.
Multiple Choice Questions
(a) 3 : 2
(b) 2 : 1
(c) \( \sqrt2:1 \)
(d) 4 : 1
Show Answer & Explanation
Answer: (b) 2 : 1
Explanation:
1. At P the phase difference is 0: \( I_P=4I_0 \).
2. At Q the phase difference is \( \pi/2 \): \( I_Q=4I_0\cos^2\frac\pi4=2I_0 \).
3. Ratio \( 2:1 \).
Teacher's Note:
1. Intensity at a point is Imax cos squared of half the phase difference.
(a) \( \frac{Da}{\lambda} \)
(b) \( \frac{2Da}{\lambda} \)
(c) \( \frac{2D\lambda}{a} \)
(d) \( \frac{D\lambda}{a} \)
Show Answer & Explanation
Answer: (c) \( \frac{2D\lambda}{a} \)
Explanation:
1. First minima at \( y=\pm\frac{D\lambda}{a} \).
2. Width of the central maximum \( =\frac{2D\lambda}a \).
Teacher's Note:
1. The central maximum extends between the first minima on either side.
(a) 0.5 mm
(b) 0.02 mm
(c) 0.2 mm
(d) 0.1 mm
Show Answer & Explanation
Answer: (c) 0.2 mm
Explanation:
1. Central single-slit width \( =\frac{2\lambda D}{a} \); fringe width \( \beta=\frac{\lambda D}{d} \).
2. Ten fringes inside: \( \frac{2\lambda D}a=10\frac{\lambda D}d\Rightarrow a=\frac d5=0.2\ \text{mm} \)
Teacher's Note:
1. Equate the central diffraction width to ten interference fringe widths.
Assertion (A): A thin air film is formed by putting the convex surface of a plano-convex lens over a plane glass plate. With monochromatic light, this film gives an interference pattern due to light reflected from the top (convex) surface and the bottom (glass plate) surface of the film. When light reflects at the air-glass plate interface, the reflected wave suffers a phase change of pi.
Reason (R): The centre of the interference pattern is dark.
(a) Both A and R are true, and R is the correct explanation of A.
(b) Both A and R are true, but R is not the correct explanation of A.
(c) A is true, but R is false.
(d) A is false, but R is true.
Show Answer & Explanation
Answer: (a) Both A and R are true, and R is the correct explanation of A.
Explanation:
1. Reflection from the glass plate (air to glass) gives a phase change of pi, while reflection at the lens-air boundary gives none, so A is true.
2. At the centre the film thickness is zero, so the net path difference is lambda/2: destructive interference, a dark centre. R follows from A.
Teacher's Note:
1. The extra half-wavelength shift at one reflection makes the zero-thickness point dark.
(a) \( 2\pi \)
(b) \( 3\pi \)
(c) \( 4\pi \)
(d) \( \pi\lambda \)
Show Answer & Explanation
Answer: (c) \( 4\pi \)
Explanation:
1. Second minimum: path difference \( a\sin\theta=2\lambda \).
2. Phase difference \( =\frac{2\pi}\lambda\times2\lambda=4\pi \)
Teacher's Note:
1. The nth minimum has a path difference of n wavelengths between the slit edges.
(a) \( \frac1{\sqrt2} \)
(b) \( \frac{\sqrt3}{2} \)
(c) \( \frac12 \)
(d) \( \frac34 \)
Show Answer & Explanation
Answer: (d) \( \frac34 \)
Explanation:
1. Phase difference \( \phi=\frac{2\pi}\lambda\cdot\frac\lambda6=\frac\pi3 \).
2. \( \frac I{I_0}=\cos^2\frac\phi2=\cos^230^\circ=\frac34 \)
Teacher's Note:
1. I over Imax equals cos squared of half the phase difference.
(a) \( 2I_0 \)
(b) \( 4I_0 \)
(c) \( I_0 \)
(d) \( I_0/2 \)
Show Answer & Explanation
Answer: (b) \( 4I_0 \)
Explanation:
1. The amplitude at the central maximum is proportional to the slit width, since all the wavelets add in phase.
2. Doubling the width doubles the amplitude, so the intensity becomes \( 4I_0 \).
Teacher's Note:
1. Central intensity varies as the square of the slit width, for the same light intensity per unit width.
(a) Points
(b) Straight line
(c) Semi-circle
(d) Concentric circles
Show Answer & Explanation
Answer: (d) Concentric circles
Explanation:
1. The path difference at a screen point depends only on the angle from the axis (S1S2 line), \( \Delta=d\cos\theta \).
2. Points with the same path difference lie on a circle about the axis, so fringes are concentric circles.
Teacher's Note:
1. Rotational symmetry about the line joining the sources gives circular fringes.
(a) \( \sin^{-1}(n) \)
(b) \( \sin^{-1}\left(\frac1n\right) \)
(c) \( \tan^{-1}\left(\frac1n\right) \)
(d) \( \tan^{-1}(n) \)
Show Answer & Explanation
Answer: (d) \( \tan^{-1}(n) \)
Explanation:
1. Brewster's law: \( \tan i_B=n \).
Teacher's Note:
1. At the polarizing angle the reflected and refracted rays are at right angles.
(a) 0.30 mm
(b) 0.40 mm
(c) 0.53 mm
(d) 450 microns
Show Answer & Explanation
Answer: (a) 0.30 mm
Explanation:
1. \( \beta'=\frac\beta\mu=\frac{0.4}{4/3}=0.30\ \text{mm} \)
Teacher's Note:
1. Wavelength shrinks by mu in the medium, so the fringe width does too.
(a) 16 : 25
(b) 9 : 1
(c) 4 : 5
(d) 5 : 4
Show Answer & Explanation
Answer: (d) 5 : 4
Explanation:
1. Resolving power is proportional to \( 1/\lambda \).
2. \( \frac{R_1}{R_2}=\frac{\lambda_2}{\lambda_1}=\frac54 \)
Teacher's Note:
1. Shorter wavelengths resolve better.
(a) \( a=\frac{\lambda^2}L \) and \( b_{min}=\left(\frac{2\lambda^2}L\right) \)
(b) \( a=\sqrt{\lambda L} \) and \( b_{min}=\left(\frac{2\lambda^2}L\right) \)
(c) \( a=\sqrt{\lambda L} \) and \( b_{min}=\sqrt{4\lambda L} \)
(d) \( a=\frac{\lambda^2}L \) and \( b_{min}=\sqrt{4\lambda L} \)
Show Answer & Explanation
Answer: (c) \( a=\sqrt{\lambda L} \) and \( b_{min}=\sqrt{4\lambda L} \)
Explanation:
1. Spot size \( b=a+\frac{\lambda L}a \).
2. Minimum when \( a=\frac{\lambda L}a\Rightarrow a=\sqrt{\lambda L} \), giving \( b_{min}=2\sqrt{\lambda L}=\sqrt{4\lambda L} \)
Teacher's Note:
1. Minimise the sum of geometrical and diffraction spreads.
(a) \( 10^8 \) km
(b) \( 10^{10} \) km
(c) \( 10^{11} \) km
(d) \( 10^6 \) km
Show Answer & Explanation
Answer: (a) \( 10^8 \) km
Explanation:
1. \( \theta=\frac{1.22\lambda}D=\frac{1.22\times6\times10^{-7}}{0.3}=2.44\times10^{-6}\ \text{rad} \)
2. \( s=\theta\times10\times9.46\times10^{15}\approx2.3\times10^{11}\ \text{m}\approx2.3\times10^8\ \text{km} \)
Teacher's Note:
1. Minimum resolvable separation is the angular limit times the distance.
(a) \( 100\ \mu m \)
(b) \( 300\ \mu m \)
(c) \( 1\ \mu m \)
(d) \( 30\ \mu m \)
Show Answer & Explanation
Answer: (d) \( 30\ \mu m \)
Explanation:
1. \( \theta=\frac{1.22\lambda}D=\frac{1.22\times5\times10^{-7}}{5\times10^{-3}}=1.22\times10^{-4}\ \text{rad} \)
2. \( s=\theta\times25\ \text{cm}\approx3\times10^{-5}\ \text{m}=30\ \mu m \)
Teacher's Note:
1. Use the pupil diameter (twice the radius) in Rayleigh's criterion.
(a) \( \frac\beta2 \)
(b) \( \frac\beta4 \)
(c) \( \frac\beta3 \)
(d) \( \frac\beta6 \)
Show Answer & Explanation
Answer: (b) \( \frac\beta4 \)
Explanation:
1. \( I=I_0\cos^2\frac\phi2=\frac{I_0}2\Rightarrow\phi=\frac\pi2 \), a path difference of \( \lambda/4 \).
2. \( y=\frac{D}{d}\cdot\frac\lambda4=\frac\beta4 \)
Teacher's Note:
1. Half intensity corresponds to a path difference of a quarter wavelength.
(a) 4
(b) 9
(c) 16
(d) 25
Show Answer & Explanation
Answer: (c) 16
Explanation:
1. \( \frac{I_{max}}{I_{min}}=\frac{(5+3)^2}{(5-3)^2}=\frac{64}{4}=16 \)
Teacher's Note:
1. Amplitudes add for maximum and subtract for minimum.
(a) 0.75
(b) 1.0
(c) 1.34
(d) 2.0
Show Answer & Explanation
Answer: (b) 1.0
Explanation:
1. \( \lambda'=\frac{700}{4/3}=525\ \text{nm} \).
2. \( \beta=\frac{\lambda'D}{d}=\frac{525\times10^{-9}\times0.48}{0.25\times10^{-3}}\approx1.0\times10^{-3}\ \text{m}=1.0\ \text{mm} \)
Teacher's Note:
1. Use the wavelength in water in the fringe width formula.
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FAQs
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