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Wave Motion

Questions
614
MHT CET
351
JEE Main
169
NEET
94
Years
1988–2026
0 of 614 attemptedPick an answer to see the solution

Q1MHT CET 2026 · 20 MAY · SHIFT 1Easy

Wave Basics & Properties of Sound · Wave relation v = nλ

A body sends waves 150150 mm long through medium P and 0.300.30 m long in medium Q. If the velocity of wave in medium P is 8080 cm/s, the velocity of wave in medium Q in m/s is

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Answer: (a)

  1. Frequency is set by the source and stays the same in both media: n=vλn = \frac{v}{\lambda}.
  2. n=vPλP=0.800.150=163n = \frac{v_P}{\lambda_P} = \frac{0.80}{0.150} = \frac{16}{3} Hz
  3. vQ=nλQ=163×0.30=1.6v_Q = n\lambda_Q = \frac{16}{3} \times 0.30 = 1.6 m/s
  4. So the answer is (a) 1.61.6 m/s.
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Q2MHT CET 2026 · 19 APR · SHIFT 2Easy

Wave Basics & Properties of Sound · Wave relation v = nλ

A body sends a wave 150150 mm long through medium P and 0.300.30 m long in medium Q. If velocity of the wave in medium P is 8080 cm s−1-1, the velocity of wave in medium Q is

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Answer: (d)

  1. Frequency is the same in both media, so vQvP=λQλP\frac{v_Q}{v_P} = \frac{\lambda_Q}{\lambda_P}.
  2. vQ=0.80×0.300.150=1.6v_Q = 0.80 \times \frac{0.30}{0.150} = 1.6 m/s
  3. So the answer is (d) 1.61.6 m s−1^{-1}.
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Q3MHT CET 2026 · 18 APR · SHIFT 1Easy

Wave Basics & Properties of Sound · Wave relation v = nλ

The number of waves counted by an observer on the sea-coast in one minute is 54. If the wavelength of the waves is 55 m then the velocity of the waves in m/s will be

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Answer: (a)

  1. Frequency n=5460=0.9n = \frac{54}{60} = 0.9 Hz
  2. v=nλ=0.9×5=4.5v = n\lambda = 0.9 \times 5 = 4.5 m/s
  3. So the answer is (a) 4.54.5 m/s.
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Q4MHT CET 2026 · 13 APR · SHIFT 2Easy

Wave Basics & Properties of Sound · Wave relation v = nλ

Sound waves travel at 350350 m/s through a warm air and at 35003500 m/s through brass. Which of the following is correct about the wavelength of a 700700 Hz accoustic wave as it enters brass from warm air?

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Answer: (c)

  1. Frequency does not change on entering a new medium, so λ=vn∝v\lambda = \frac{v}{n} \propto v.
  2. λbrassλair=3500350=10\frac{\lambda_{brass}}{\lambda_{air}} = \frac{3500}{350} = 10
  3. So the answer is (c) it increases by a factor 1010.
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Q5MHT CET 2026 · 13 APR · SHIFT 1Easy

Wave Basics & Properties of Sound · Wave relation v = nλ

Waves having a velocity 10m/s, strike a stationary boat near the sea shore. The distance between two consecutive crests of the waves is 40m. After how many second, the consecutive waves strike the boat?

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Answer: (c)

  1. Distance between consecutive crests is the wavelength: λ=40\lambda = 40 m.
  2. Time between consecutive waves is the period: T=λv=4010=4T = \frac{\lambda}{v} = \frac{40}{10} = 4 s
  3. So the answer is (c) 44 s.
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Q6MHT CET 2026 · 20 APR · SHIFT 1Easy

Wave Basics & Properties of Sound · Pitch, loudness and musical instruments

The 'Loudness' and 'Pitch' of sound respectively are the human perception to

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Answer: (a)

  1. Loudness is the ear's response to intensity (energy per unit area per second).
  2. Pitch is the ear's response to frequency.
  3. So the answer is (a) intensity of sound and frequency of sound.
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Q7MHT CET 2026 · 19 APR · SHIFT 1Easy

Wave Basics & Properties of Sound · Pitch, loudness and musical instruments

Which one of the following statements regarding pitch of sound is 'WRONG'?

(A) Pitch refers to sharpness of sound.

(B) Tone refers to the single frequency of that wave.

(C) High pitch sound need not be louder.

(D) In general male sound is sharper than that of a female.

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Answer: (a)

  1. (A) True: pitch is the shrillness or sharpness of sound.
  2. (B) True: a tone is a sound of a single frequency.
  3. (C) True: pitch depends on frequency, loudness on intensity, so a high pitch sound can be soft.
  4. (D) Wrong: a female voice usually has higher frequency, so it is sharper than a male voice.
  5. So the answer is (a) D.
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Q8MHT CET 2026 · 17 APR · SHIFT 1Easy

Wave Basics & Properties of Sound · Pitch, loudness and musical instruments

Out of the following musical instruments which is ' NOT ' a percussion instrument?

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Answer: (b)

  1. Percussion instruments produce sound when struck: drum, daphali, xylophone.
  2. The saxophone is a wind instrument (vibrating air column).
  3. So the answer is (b) Saxophone.
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Q9MHT CET 2026 · 19 MAY · SHIFT 1Easy

Wave Basics & Properties of Sound · Intensity and sound level

The amplitude of a sound wave at a distance rr from a point source is AA. The amplitude at a distance 2r2r from the point source is

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Answer: (b)

  1. For a point source, I=P4πr2∝1r2I = \frac{P}{4\pi r^2} \propto \frac{1}{r^2}.
  2. Also I∝A2I \propto A^2, so A∝1rA \propto \frac{1}{r}.
  3. At 2r2r: A′=A2A' = \frac{A}{2}
  4. So the answer is (b) A2\frac{A}{2}.
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Q10JEE Main 2026 · 24 JAN · SHIFT 2Easy

Wave Basics & Properties of Sound · Intensity and sound level

A point source is kept at the center of a spherically enclosed detector. If the volume of the detector increased by 8 times, the intensity will

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Answer: (b)

  1. V=43πr3V = \frac{4}{3}\pi r^3, so V→8VV \to 8V means r→2rr \to 2r.
  2. I=P4πr2∝1r2I = \frac{P}{4\pi r^2} \propto \frac{1}{r^2}, so I→I4I \to \frac{I}{4}
  3. So the answer is (b) decrease by 4 times.
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Q11MHT CET 2026 · 13 APR · SHIFT 1Medium

Wave Basics & Properties of Sound · Intensity and sound level

A musical instrument P produces sound waves of frequency 'n' and amplitude 'A'. Another musical instrument Q produces sound waves of frequency n/4. The waves produced by P and Q have equal energies. The amplitude of waves produced by Q will be

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Answer: (c)

  1. Wave energy E∝A2n2E \propto A^2 n^2.
  2. Equal energies: AQnQ=An⇒AQ=Ann/4A_Q n_Q = A n \Rightarrow A_Q = A \frac{n}{n/4}
  3. AQ=4AA_Q = 4A
  4. So the answer is (c) 4A4A.
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Q12MHT CET 2025 · 21 APR · SHIFT 1Easy

Wave Basics & Properties of Sound · Wave relation v = nλ

An observer on sea-coast counts 45 waves in one minute. If the wavelength of the waves is 7 m, then the velocity of the waves will be

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Answer: (b)

  1. Frequency n=4560=0.75n = \frac{45}{60} = 0.75 Hz
  2. v=nλ=0.75×7=5.25v = n\lambda = 0.75 \times 7 = 5.25 m/s
  3. So the answer is (b) 5.255.25 m/s.
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Q13MHT CET 2025 · 26 APR · SHIFT 2Medium

Wave Basics & Properties of Sound · Intensity and sound level

A musical instrument ' P ' produce sound waves of frequency ' nn ' and amplitude ' AA '. Another musical instrument ' QQ ' produces sound waves of frequency ' n4\frac{n}{4} ' The waves produced by ' P ' and ' QQ ' have equal energies. If the amplitude of waves produced by ' P ' is ' ApA_p ', the amplitude of waves produced by ' QQ ' will be

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Answer: (b)

  1. Wave energy E∝A2n2E \propto A^2 n^2, so equal energies give An=A n = constant.
  2. AQ=Apnn/4=4ApA_Q = A_p \frac{n}{n/4} = 4A_p
  3. So the answer is (b) 4Ap4A_p.
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Q14MHT CET 2024 · 11 MAY · SHIFT 2Easy

Wave Basics & Properties of Sound · Nature and types of waves

Which of the following statements is NOT true?

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Answer: (c)

  1. Sound is a mechanical wave: it needs a material medium (solid, liquid or gas) to travel.
  2. In vacuum there are no particles to vibrate, so sound cannot travel there.
  3. Statements (a), (b), (d) are true.
  4. So the answer is (c) Sound can travel through vacuum.
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Q15MHT CET 2024 · 10 MAY · SHIFT 2Easy

Wave Basics & Properties of Sound · Wave relation v = nλ

Prong of a vibrating tuning fork is in contact with water surface. It produces concentric circular waves on the surface of water. The distance between five consecutive crests is 0.8 m and the velocity of wave on the water surface is 56 m/s56\text{ m/s}. The frequency of tuning fork is

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Answer: (b)

  1. Five consecutive crests have four gaps: 4λ=0.84\lambda = 0.8 m, so λ=0.2\lambda = 0.2 m.
  2. n=vλ=560.2=280n = \frac{v}{\lambda} = \frac{56}{0.2} = 280 Hz
  3. So the answer is (b) 280 Hz.
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Q16MHT CET 2024 · 9 MAY · SHIFT 1Easy

Wave Basics & Properties of Sound · Pitch, loudness and musical instruments

Out of the following musical instruments, which is 'NOT' a percussion instrument?

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Answer: (d)

  1. Daphali, sambal and cymbals are struck, so they are percussion instruments.
  2. The clarinet is a wind instrument (vibrating air column).
  3. So the answer is (d) Clarinet.
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Q17MHT CET 2024 · 16 MAY · SHIFT 1Easy

Wave Basics & Properties of Sound · Intensity and sound level

How many times more intense is a 60 dB sound than a 30 dB sound?

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Answer: (c)

  1. L2−L1=10log⁡10I2I1L_2 - L_1 = 10\log_{10}\frac{I_2}{I_1}
  2. 60−30=30=10log⁡10I2I1⇒I2I1=10360 - 30 = 30 = 10\log_{10}\frac{I_2}{I_1} \Rightarrow \frac{I_2}{I_1} = 10^{3}
  3. So the answer is (c) 1000.
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Q18JEE Main 2024 · 30 JAN · SHIFT 2Easy

Wave Basics & Properties of Sound · Intensity and sound level

A point source is emitting sound waves of intensity 16×10−8 Wm−216 \times 10^{-8}\text{ Wm}^{-2} at the origin. The difference in intensity (magnitude only) at two points located at distances of 2 m2\text{ m} and 4 m4\text{ m} from the origin respectively will be _________ ×10−8 Wm−2\times 10^{-8}\text{ Wm}^{-2}.

Numerical answer type. Work it out, then open the answer.

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Answer: 3

  1. Take the given 16×10−816 \times 10^{-8} W m−2^{-2} as the intensity at 11 m from the source; I∝1r2I \propto \frac{1}{r^2}.
  2. I2=1622×10−8=4×10−8I_2 = \frac{16}{2^2} \times 10^{-8} = 4 \times 10^{-8} W m−2^{-2}
  3. I4=1642×10−8=1×10−8I_4 = \frac{16}{4^2} \times 10^{-8} = 1 \times 10^{-8} W m−2^{-2}
  4. Difference =3×10−8= 3 \times 10^{-8} W m−2^{-2}, so the answer is 33.
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Q19MHT CET 2024 · 10 MAY · SHIFT 1Medium

Wave Basics & Properties of Sound · Intensity and sound level

A musical instrument X produces sound waves of frequency n and amplitude A. Another musical instrument YY produces sound waves of frequency n3\frac{n}{3}. The waves produced by XX and YY have equal energies. The amplitude of waves produced by Y will be

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Answer: (a)

  1. Wave energy E∝A2n2E \propto A^2 n^2, so equal energies give An=A n = constant.
  2. AY=Ann/3=3AA_Y = A \frac{n}{n/3} = 3A
  3. So the answer is (a) 3A.
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Q20MHT CET 2024 · 9 MAY · SHIFT 2Medium

Wave Basics & Properties of Sound · Intensity and sound level

A musical instrument ' PP ' produces sound waves of frequency ' nn ' and amplitude ' AA '. Another musical instrument ' QQ ' produces sound waves of frequency n4\frac{n}{4}. The waves produced by ' PP ' and ' QQ ' have equal energies. If the amplitude of waves produced by ' PP ' is ' APA_P ', the amplitude of waves produced by ' QQ ' will be

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Answer: (b)

  1. Wave energy E∝A2n2E \propto A^2 n^2, so equal energies give An=A n = constant.
  2. AQ=APnn/4=4APA_Q = A_P \frac{n}{n/4} = 4A_P
  3. So the answer is (b) 4AP4A_P.
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Q21MHT CET 2023 · 11 MAY · SHIFT 2Easy

Wave Basics & Properties of Sound · Wave relation v = nλ

A sound of frequency 480 Hz480\text{ Hz} is emitted from the stringed instrument. The velocity of sound in air is 320 m/s320\text{ m/s}. After completing 180 vibrations, the distance covered by a wave is

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Answer: (c)

  1. In each vibration the wave advances one wavelength, so distance =Nλ=Nvn= N\lambda = N\frac{v}{n}.
  2. λ=320480=23\lambda = \frac{320}{480} = \frac{2}{3} m
  3. Distance =180×23=120= 180 \times \frac{2}{3} = 120 m
  4. So the answer is (c) 120 m.
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Q22MHT CET 2023 · 11 MAY · SHIFT 2Easy

Wave Basics & Properties of Sound · Related oscillation questions

A rectangular block of mass 'mm' and crosssectional area A, floats on a liquid of density 'ρ\rho'. It is given a small vertical displacement from equilibrium, it starts oscillating with frequency 'nn' equal to ( g=g = acceleration due to gravity)

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Answer: (a)

  1. Pushing the block down by xx displaces extra liquid volume AxAx, giving extra upthrust F=−Aρg xF = -A\rho g\,x.
  2. This is SHM with force constant k=Aρgk = A\rho g.
  3. n=12πkm=12πAρgmn = \frac{1}{2\pi}\sqrt{\frac{k}{m}} = \frac{1}{2\pi}\sqrt{\frac{A\rho g}{m}}
  4. So the answer is (a).
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Q23JEE Main 2022 · 27 JUN · SHIFT 2Easy

Wave Basics & Properties of Sound · Wave relation v = nλ

If a wave gets refracted into a denser medium, then which of the following is true?

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Answer: (c)

  1. Frequency is fixed by the source, so it does not change on refraction.
  2. In a denser medium the wave speed decreases, and λ=vn\lambda = \frac{v}{n} decreases with it.
  3. So the answer is (c) wavelength and speed decrease, frequency remains constant.
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Q24MHT CET 2021 · 20 SEP · SHIFT 2Easy

Wave Basics & Properties of Sound · Nature and types of waves

Which one of the following statements is true?

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Answer: (a)

  1. Sound in air travels as compressions and rarefactions, so particles vibrate along the direction of travel: longitudinal.
  2. Light is an electromagnetic wave with E⃗\vec E and B⃗\vec B perpendicular to the direction of travel: transverse.
  3. So the answer is (a).
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Q25MHT CET 2021 · 24 SEP · SHIFT 1Easy

Wave Basics & Properties of Sound · Wave relation v = nλ

Two tuning forks of frequencies 320 Hz320\text{ Hz} and 480 Hz480\text{ Hz} are sounded together to produce sound waves. The velocity of sound in air is 320 ms−1320\text{ ms}^{-1}. The difference between wavelengths of these waves is nearly

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Answer: (c)

  1. λ=vn\lambda = \frac{v}{n} for each fork.
  2. λ1=320320=1\lambda_1 = \frac{320}{320} = 1 m, λ2=320480=0.667\lambda_2 = \frac{320}{480} = 0.667 m
  3. Δλ=1−0.667=0.333\Delta\lambda = 1 - 0.667 = 0.333 m ≈33\approx 33 cm
  4. So the answer is (c) 33 cm.
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Q26MHT CET 2021 · 23 SEP · SHIFT 2Easy

Wave Basics & Properties of Sound · Wave relation v = nλ

The frequency of a tuning fork is 220 Hz220\text{ Hz} and the velocity of sound in air is 330 m/s330\text{ m/s}. When the tuning fork completes 80 vibrations, the distance travelled by the sound wave is

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Answer: (a)

  1. Distance =Nλ=Nvn= N\lambda = N\frac{v}{n}.
  2. λ=330220=1.5\lambda = \frac{330}{220} = 1.5 m
  3. Distance =80×1.5=120= 80 \times 1.5 = 120 m
  4. So the answer is (a) 120 m.
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Q27MHT CET 2021 · 20 SEP · SHIFT 1Easy

Wave Basics & Properties of Sound · Wave relation v = nλ

The frequency of a tuning fork is 'n' Hz and velocity of sound in air is 'V' m/s. When the tuning fork completes 'x' vibrations, the distance travelled by the wave is

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Answer: (c)

  1. One vibration moves the wave forward by one wavelength λ=Vn\lambda = \frac{V}{n}.
  2. After xx vibrations: distance =xλ=xVn= x\lambda = \frac{xV}{n}
  3. So the answer is (c) xVn\frac{xV}{n}.
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Q28JEE Main 2020 · 4 SEP · SHIFT 1Medium

Wave Basics & Properties of Sound · Wave relation v = nλ

For a transverse wave travelling along a straight line, the distance between two peaks (crests) is 5 m, while the distance between one crest and one trough is 1.5 m. The possible wavelengths (in m) of the wave are:

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Answer: (b)

  1. Two crests are a whole number of wavelengths apart: 5=nλ5 = n\lambda.
  2. A crest and a trough are an odd number of half wavelengths apart: 1.5=(2m+1)λ21.5 = (2m+1)\frac{\lambda}{2}, so λ=32m+1\lambda = \frac{3}{2m+1}.
  3. Both hold for λ=1,13,15,…\lambda = 1, \frac{1}{3}, \frac{1}{5}, \dots e.g. λ=1\lambda = 1: 5=5λ5 = 5\lambda, 1.5=3⋅λ21.5 = 3 \cdot \frac{\lambda}{2}.
  4. So the answer is (b) 11,13,15,…\frac{1}{1}, \frac{1}{3}, \frac{1}{5}, \dots
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Q29JEE Main 2020 · 5 SEP · SHIFT 1Medium

Wave Basics & Properties of Sound · Intensity and sound level

Assume that the displacement(s) of air is proportional to the pressure difference (Δ\Deltap) created by a sound wave. Displacement (s) further depends on the speed of sound (v), density of air (ρ\rho) and the frequency (f). If Δ\Deltap ~ 10 Pa, v ~ 300 m/s, ρ\rho ~ 1 kg/m3 and f ~ 1000 Hz, then s will be of the order of (take the multiplicative constant to be 1):

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Answer: (b)

  1. Write s=Δp vaρbfcs = \Delta p\, v^a \rho^b f^c; [s]=[s] = L and [Δp]=[\Delta p] = M L−1^{-1} T−2^{-2}.
  2. Matching M, L, T gives b=−1b = -1, a=−1a = -1, c=−1c = -1: s=Δpρvfs = \frac{\Delta p}{\rho v f}.
  3. s=101×300×1000=3.3×10−5s = \frac{10}{1 \times 300 \times 1000} = 3.3 \times 10^{-5} m ≈3100\approx \frac{3}{100} mm
  4. So the answer is (b) 3100\frac{3}{100} mm.
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Q30JEE Main 2019 · 12 APR · SHIFT 2Medium

Wave Basics & Properties of Sound · Intensity and sound level

A small speaker delivers 2 W of audio output. At what distance from the speaker will one detect 120 dB intensity sound? [Given reference intensity of sound as 10–12 W/m2 ]

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Answer: (c)

  1. Sound level L=10log⁡10(I/I0)L = 10\log_{10}(I/I_0), so 120=10log⁡10(I/10−12)120 = 10\log_{10}(I/10^{-12}) gives I=1 W/m2I = 1\ \text{W/m}^2.
  2. Point source: I=P4πr2⇒r=P4πI=24π×1I = \dfrac{P}{4\pi r^2} \Rightarrow r = \sqrt{\dfrac{P}{4\pi I}} = \sqrt{\dfrac{2}{4\pi \times 1}}
  3. r=0.159≈0.40 mr = \sqrt{0.159} \approx 0.40\ \text{m}
  4. So the answer is (c) 40 cm40\ \text{cm}.
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Q31JEE Main 2017 · 9 APR · SHIFT 1Medium

Wave Basics & Properties of Sound · Related oscillation questions

In an experiment to determine the period of a simple pendulum of length 1 m, it is attached to different spherical bobs of radii r1 and r2. The two spherical bobs have uniform mass distribution. If the relative difference in the periods, is found to be 5×10−4 s, the difference in radii, ∣\vert r1 −- r2 ∣\vert is best given by:

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Answer: (b)

  1. Effective length ≈L+r\approx L + r, so T=2π(L+r)/gT = 2\pi\sqrt{(L+r)/g} and ΔTT=12ΔrL\dfrac{\Delta T}{T} = \dfrac{1}{2}\dfrac{\Delta r}{L}.
  2. Δr=2LΔTT=2×1×5×10−4=10−3 m\Delta r = 2L\dfrac{\Delta T}{T} = 2 \times 1 \times 5\times10^{-4} = 10^{-3}\ \text{m}
  3. So the answer is (b) 0.1 cm0.1\ \text{cm}.
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Q32JEE Main 2013 · 25 APR · SHIFT 1Easy

Wave Basics & Properties of Sound · Wave relation v = nλ

In a transverse wave the distance between a crest and neighbouring trough at the same instant is 4.0 cm and the distance between a crest and trough at the same place is 1.0 cm. The next crest appears at the same place after a time interval of 0.4 s. The maximum speed of the vibrating particles in the medium is:

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Answer: (b)

λ/2 = 4 cm2A = 1 cmcresttrough
  1. Crest to neighbouring trough at one instant is λ2=4\frac{\lambda}{2} = 4 cm, so λ=8\lambda = 8 cm.
  2. Crest to trough at the same place (vertical) is 2A=12A = 1 cm, so A=0.5A = 0.5 cm.
  3. Next crest at the same place after one period: T=0.4T = 0.4 s, so ω=2πT=5π\omega = \frac{2\pi}{T} = 5\pi rad/s.
  4. vmax=Aω=0.5×5π=5π2v_{max} = A\omega = 0.5 \times 5\pi = \frac{5\pi}{2} cm/s
  5. So the answer is (b) 5π2\frac{5\pi}{2} cm/s.
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Q33NEET 2011 · AIPMT · PRELIMSEasy

Wave Basics & Properties of Sound · Wave relation v = nλ

Sound waves travel at 350 m/s through a warm air and at 3500 m/s through brass. The wavelength of a 700 Hz acoustic wave as it enters brass from warm air

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Answer: (c)

  1. Frequency stays 700700 Hz in both media, so λ∝v\lambda \propto v.
  2. λbrassλair=3500350=10\frac{\lambda_{brass}}{\lambda_{air}} = \frac{3500}{350} = 10
  3. So the answer is (c) increases by a factor 10.
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Q34NEET 2008 · AIPMTEasy

Wave Basics & Properties of Sound · Related oscillation questions

A point performs simple harmonic oscillation of period T and the equation of motion is given by x = a sin(ω\omegat + π\pi/6). After the elapse of what fraction of the time period the velocity of the point will be equal to half of its maximum velocity?

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Answer: (b)

  1. v=aωcos⁡(ωt+π6)v = a\omega\cos(\omega t + \frac{\pi}{6}), vmax=aωv_{max} = a\omega.
  2. v=vmax2⇒cos⁡(ωt+π6)=12⇒ωt+π6=π3v = \frac{v_{max}}{2} \Rightarrow \cos(\omega t + \frac{\pi}{6}) = \frac{1}{2} \Rightarrow \omega t + \frac{\pi}{6} = \frac{\pi}{3}
  3. ωt=π6⇒2πTt=π6⇒t=T12\omega t = \frac{\pi}{6} \Rightarrow \frac{2\pi}{T}t = \frac{\pi}{6} \Rightarrow t = \frac{T}{12}
  4. So the answer is (b) T/12T/12.
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Q35JEE Main 2007 · AIEEEMedium

Wave Basics & Properties of Sound · Intensity and sound level

A sound absorber attenuates the sound level by 20 dB20\text{ dB}. The intensity decreases by a factor of

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Answer: (a)

  1. ΔL=10log⁡10(I1/I2)\Delta L = 10\log_{10}(I_1/I_2)
  2. 20=10log⁡10(I1/I2)⇒I1/I2=10220 = 10\log_{10}(I_1/I_2) \Rightarrow I_1/I_2 = 10^2
  3. So the answer is (a) 100100.
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Q36NEET 2006 · AIPMTEasy

Wave Basics & Properties of Sound · Nature and types of waves

Which one of the following statements is true?

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Answer: (c)

  1. Light (electromagnetic) travels in vacuum; sound (mechanical) does not, so (a) is false.
  2. Sound in air is longitudinal; light is transverse.
  3. So the answer is (c).
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Q37NEET 2006 · AIPMTEasy

Wave Basics & Properties of Sound · Intensity and sound level

The time of reverberation of a room A is one second. What will be the time (in seconds of reverberation of a room, having all the dimensions double of those of room A?

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Answer: (b)

  1. Sabine's formula: T=0.161 VaST = \frac{0.161\,V}{aS}, so T∝VST \propto \frac{V}{S}.
  2. Doubling every dimension: V→8VV \to 8V, S→4SS \to 4S.
  3. T′=84×1=2T' = \frac{8}{4} \times 1 = 2 s
  4. So the answer is (b) 2.
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Q38NEET 2005 · AIPMTEasy

Wave Basics & Properties of Sound · Intensity and sound level

A point source emits sound equally in all directions in a non-absorbing medium. Two points P and Q are at distances of 2 m and 3 m respectively from the source. The ratio of the intensities of the waves at P and Q is

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Answer: (c)

  1. For a point source, I∝1r2I \propto \frac{1}{r^2}.
  2. IPIQ=rQ2rP2=94\frac{I_P}{I_Q} = \frac{r_Q^2}{r_P^2} = \frac{9}{4}
  3. So the answer is (c) 9 : 4.
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Q39NEET 2000 · AIPMTEasy

Wave Basics & Properties of Sound · Related oscillation questions

The equations of two waves acting in perpendicular directions are given as

x = aacos(ω\omegat +δ\delta) and y = aacos(ω\omegat + α\alpha), where δ=α+π2\delta = \alpha + \frac{\pi}{2}, the resultant wave represents

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Answer: (b)

  1. With δ=α+π2\delta = \alpha + \frac{\pi}{2}: x=acos⁡(ωt+α+π2)=−asin⁡(ωt+α)x = a\cos(\omega t + \alpha + \frac{\pi}{2}) = -a\sin(\omega t + \alpha).
  2. y=acos⁡(ωt+α)y = a\cos(\omega t + \alpha)
  3. x2+y2=a2x^2 + y^2 = a^2: equal amplitudes with π2\frac{\pi}{2} phase difference.
  4. So the answer is (b) a circle.
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Q40NEET 1998 · AIPMTEasy

Wave Basics & Properties of Sound · Wave relation v = nλ

In a sinusoidal wave, the time required for a particular point, to move from maximum displacement to zero displacement is 0.170 s0.170\text{ s}. The frequency of the wave is

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Answer: (a)

  1. Going from maximum displacement to zero (mean position) takes a quarter period: T4=0.170\frac{T}{4} = 0.170 s.
  2. T=0.680T = 0.680 s
  3. n=1T=10.680≈1.47n = \frac{1}{T} = \frac{1}{0.680} \approx 1.47 Hz
  4. So the answer is (a) 1.471.47 Hz.
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Q41NEET 1995 · AIPMTEasy

Wave Basics & Properties of Sound · Wave relation v = nλ

A hospital uses an ultrasonic scanner to locate tumours in a tissue. The operating frequency of the scanner is 4.2 MHz4.2\text{ MHz}. The speed of sound in a tissue is 1.7 km/s1.7\text{ km/s}. The wavelength of sound in the tissue is close to

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Answer: (c)

  1. λ=vn\lambda = \frac{v}{n}
  2. λ=1.7×1034.2×106≈4.0×10−4\lambda = \frac{1.7 \times 10^{3}}{4.2 \times 10^{6}} \approx 4.0 \times 10^{-4} m
  3. So the answer is (c) 4×10−44 \times 10^{-4} m.
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Q42NEET 1992 · AIPMTEasy

Wave Basics & Properties of Sound · Nature and types of waves

With the propogation of a longitudinal wave through a material medium, the quantities transmitted in the propogation direction are

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Answer: (b)

  1. In a wave, the particles of the medium only oscillate about their mean positions; they do not move along with the wave.
  2. So no mass is carried forward; the disturbance carries energy.
  3. So the answer is (b) energy.
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Q43NEET 1989 · AIPMTMedium

Wave Basics & Properties of Sound · Intensity and sound level

If the amplitude of sound is doubled and the frequency reduced to one fourth, the intensity of sound at the same point will be

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Answer: (c)

  1. Intensity I∝A2n2I \propto A^2 n^2.
  2. I′I=(2)2×(14)2=4×116=14\frac{I'}{I} = (2)^2 \times \left(\frac{1}{4}\right)^2 = 4 \times \frac{1}{16} = \frac{1}{4}
  3. So the answer is (c) decreasing by a factor of 4.
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Q44MHT CET 2026 · 15 MAY · SHIFT 1Easy

Speed of Waves · Speed on a stretched string

The speed of a wave on a string is 150150 m/s when the tension is 120120 N. The percentage increase in the tension to raise the wave speed by 20%20\% is

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Answer: (a)

  1. v=T/μ⇒T∝v2v = \sqrt{T/\mu} \Rightarrow T \propto v^2
  2. T′/T=(1.2)2=1.44T'/T = (1.2)^2 = 1.44
  3. So the answer is (a) 44%44\%.
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Q45MHT CET 2026 · 15 APR · SHIFT 1Easy

Speed of Waves · Speed on a stretched string

A wire is under tension of 22 kg wt and a wave is travelling through it with some speed. Tension in the wire is so increased that the wave travels through it with thrice the original speed. The increase in tension is (in kg wt)

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Answer: (c)

  1. T∝v2T \propto v^2, so tripling the speed makes T′=9T=9×2=18T' = 9T = 9 \times 2 = 18 kg wt.
  2. Increase =18−2=16= 18 - 2 = 16 kg wt.
  3. So the answer is (c) 1616.
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Q46MHT CET 2026 · 11 APR · SHIFT 1Easy

Speed of Waves · Effect of temperature, pressure and humidity

What is the effect of humidity on sound waves when humidity increases?

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Answer: (a)

  1. Water vapour (M=18M = 18) is lighter than dry air (M≈29M \approx 29), so moist air has lower density.
  2. v=γP/ρv = \sqrt{\gamma P/\rho} increases as ρ\rho decreases.
  3. So the answer is (a) Speed of sound waves is more.
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Q47JEE Main 2026 · 23 JAN · SHIFT 2Easy

Speed of Waves · Effect of temperature, pressure and humidity

The velocity of sound in air is doubled when the temperature is raised from 0∘C0^\circ\text{C} to α∘C\alpha^\circ\text{C}. The value of α\alpha is ______.

Numerical answer type. Work it out, then open the answer.

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Answer: 819

  1. v∝Tv \propto \sqrt{T}, so doubling vv needs T′=4×273=1092T' = 4 \times 273 = 1092 K.
  2. α=1092−273=819\alpha = 1092 - 273 = 819
  3. Answer: 819∘819^\circC.
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Q48MHT CET 2026 · 11 APR · SHIFT 1Medium

Speed of Waves · Speed on a stretched string

A string of length 0.50.5 m and mass 10−310^{-3} kg is tightly clamped at its ends. The tension in the string is 0.80.8 N. Identical wave pulses are produced at one end at equal intervals of time Δt\Delta t. What is the minimum value of Δt\Delta t which allows constructive interference between successive pulses?

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Answer: (d)

  1. μ=10−3/0.5=2×10−3\mu = 10^{-3}/0.5 = 2\times10^{-3} kg/m, v=0.8/(2×10−3)=20v = \sqrt{0.8/(2\times10^{-3})} = 20 m/s.
  2. A pulse reflects at both fixed ends (two inversions), returning upright after a round trip 2L2L.
  3. Minimum Δt=2Lv=2×0.520=0.05 s\Delta t = \dfrac{2L}{v} = \dfrac{2\times0.5}{20} = 0.05\ \text{s}
  4. So the answer is (d) 0.050.05 s.
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Q49MHT CET 2026 · 20 APR · SHIFT 2Medium

Speed of Waves · Speed of sound in solids, liquids and gases

Two monoatomic ideal gases '1' and '2' of molecular masses m1m_1 and m2m_2 respectively are enclosed in separate containers kept at the same temperature. The ratio of the speed of sound in gas '1' to that in gas '2' is

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Answer: (b)

  1. v=γRTMv = \sqrt{\dfrac{\gamma RT}{M}}; both monoatomic (same γ\gamma) at the same TT, so v∝1/Mv \propto 1/\sqrt{M}.
  2. v1v2=m2m1\dfrac{v_1}{v_2} = \sqrt{\dfrac{m_2}{m_1}}
  3. So the answer is (b).
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Q50MHT CET 2026 · 20 APR · SHIFT 1Medium

Speed of Waves · Speed of sound in solids, liquids and gases

The ratio of the speed of sound in helium gas to that in nitrogen gas at 295295 K is ( Ratio of specific heats γ\gamma for helium is 53\frac{5}{3} and that for nitrogen is 75\frac{7}{5}. Molecular weight for helium and nitrogen are 44 and 2828 respectively.)

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Answer: (d)

  1. vHevN2=γHeγN2⋅MN2MHe\dfrac{v_{He}}{v_{N_2}} = \sqrt{\dfrac{\gamma_{He}}{\gamma_{N_2}}\cdot\dfrac{M_{N_2}}{M_{He}}}
  2. =5/37/5×284=2521×7=253= \sqrt{\dfrac{5/3}{7/5}\times\dfrac{28}{4}} = \sqrt{\dfrac{25}{21}\times 7} = \sqrt{\dfrac{25}{3}}
  3. So the answer is (d) 53\dfrac{5}{\sqrt{3}}.
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Q51MHT CET 2026 · 17 APR · SHIFT 1Medium

Speed of Waves · Effect of temperature, pressure and humidity

The enclosed air inside a closed box of rigid walls has pressure P1P_1. The density of air inside this box is constant. On heating the gas, the pressure of the enclosed air is increased from P1P_1 to P2P_2. Now it is observed that the sound travels 1.41.4 times faster than at pressure P1P_1. The ratio P2P_2 by P1P_1 is

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Answer: (b)

  1. v=γP/ρv = \sqrt{\gamma P/\rho} with ρ\rho constant, so v∝Pv \propto \sqrt{P}.
  2. P2P1=(1.4)2=1.96\dfrac{P_2}{P_1} = (1.4)^2 = 1.96
  3. So the answer is (b) 1.961.96.
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Q52JEE Main 2026 · 21 JAN · SHIFT 1Difficult

Speed of Waves · Speed on a stretched string

Two strings (A,B)(A, B) having linear densities μA=2×10−4 kg/m\mu_A = 2 \times 10^{-4}\text{ kg/m} and, μB=4×10−4 kg/m\mu_B = 4 \times 10^{-4}\text{ kg/m} and lengths LA=2.5 mL_A = 2.5\text{ m} and LB=1.5 mL_B = 1.5\text{ m} respectively are joined. Free ends of AA and BB are tied to two rigid supports CC and DD, respectively creating a tension of 500 N in the wire. Two identical pulses, sent from CC and DD ends, take time t1t_1 and t2t_2, respectively, to reach the joint. The ratio t1/t2t_1/t_2 is:

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Answer: (b)

  1. t=L/v=Lμ/Tt = L/v = L\sqrt{\mu/T}, same TT for both.
  2. t1t2=LALBμAμB=2.51.512=1.667×0.707\dfrac{t_1}{t_2} = \dfrac{L_A}{L_B}\sqrt{\dfrac{\mu_A}{\mu_B}} = \dfrac{2.5}{1.5}\sqrt{\dfrac{1}{2}} = 1.667 \times 0.707
  3. t1/t2≈1.18t_1/t_2 \approx 1.18
  4. So the answer is (b) 1.18.
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Q53MHT CET 2026 · 14 MAY · SHIFT 2Difficult

Speed of Waves · Hanging rope and rope with a block

A uniform rope of mass 0.10.1 kg and length 2.52.5 m hangs from ceiling. The speed of transverse wave in the rope at upper end and at a point 0.50.5 m distance from lower end will be (g=10g = 10 m/s22)

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Answer: (a)

  1. For a hanging rope, at height yy above the lower end v=gyv = \sqrt{gy}.
  2. Upper end: y=2.5y = 2.5 m, v=25=5v = \sqrt{25} = 5 m/s.
  3. At y=0.5y = 0.5 m: v=5v = \sqrt{5} m/s.
  4. So the answer is (a) 55 m/s, 5\sqrt{5} m/s.
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Q54JEE Main 2025 · 8 APR · SHIFT 2Easy

Speed of Waves · Speed on a stretched string

Two strings with circular cross section and made of same material, are stretched to have same amount of tension. A transverse wave is then made to pass through both the strings. The velocity of the wave in the first string having the radius of cross section R is v1v_1, and that in the other string having radius of cross section R/2 is v2v_2. Then v2v1\frac{v_2}{v_1} =

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Answer: (c)

  1. μ=ρπR2\mu = \rho \pi R^2, so with equal TT: v=T/μ∝1Rv = \sqrt{T/\mu} \propto \dfrac{1}{R}.
  2. v2v1=RR/2=2\dfrac{v_2}{v_1} = \dfrac{R}{R/2} = 2
  3. So the answer is (c) 22.
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Q55JEE Main 2025 · 28 JAN · SHIFT 1Easy

Speed of Waves · Speed of sound in solids, liquids and gases

Given below are two statements: one is labelled as Assertion A and the other is labelled as Reason R\mathbf{R}

Assertion A: A sound wave has higher speed in solids than gases.

Reason R: Gases have higher value of Bulk modulus than solids.

In the light of the above statements, choose the correct answer from the options given below

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Answer: (c)

  1. A: true, v=E/ρv = \sqrt{E/\rho} and solids have far larger elastic moduli, so sound is faster in solids.
  2. R: false, gases are highly compressible, so their bulk modulus is much smaller than that of solids.
  3. So the answer is (c) A is true but R is false.
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Q56MHT CET 2024 · 9 MAY · SHIFT 2Easy

Speed of Waves · Speed on a stretched string

A string of mass 0.2 Kg is under a tension of 2.5 N. The length of the string is 2 m. A transverse wave starts from one end of the string. The time taken by the wave to reach the other end is

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Answer: (b)

  1. μ=0.2/2=0.1 kg/m\mu = 0.2/2 = 0.1\ \text{kg/m}
  2. v=T/μ=2.5/0.1=5 m/sv = \sqrt{T/\mu} = \sqrt{2.5/0.1} = 5\ \text{m/s}
  3. t=L/v=2/5=0.4 st = L/v = 2/5 = 0.4\ \text{s}
  4. So the answer is (b) 0.40.4 s.
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Q57JEE Main 2024 · 31 JAN · SHIFT 2Easy

Speed of Waves · Speed of sound in solids, liquids and gases

The speed of sound in oxygen at S.T.P. will be approximately: (given, R=8.3 JK−1, γ=1.4R = 8.3\text{ JK}^{-1},\ \gamma = 1.4)

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Answer: (d)

  1. v=γRTMv = \sqrt{\dfrac{\gamma RT}{M}} with M=0.032M = 0.032 kg/mol, T=273T = 273 K.
  2. v=1.4×8.3×2730.032=9.91×104v = \sqrt{\dfrac{1.4 \times 8.3 \times 273}{0.032}} = \sqrt{9.91\times10^4}
  3. v≈315 m/sv \approx 315\ \text{m/s}
  4. So the answer is (d) 315 m/s.
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Q58JEE Main 2023 · 1 FEB · SHIFT 1Easy

Speed of Waves · Speed on a stretched string

A steel wire with mass per unit length 7.0×10−3 kg m−17.0 \times 10^{-3}\text{ kg m}^{-1} is under tension of 70 N70\text{ N}. The speed of transverse waves in the wire will be:

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Answer: (c)

  1. v=T/μ=707×10−3=104v = \sqrt{T/\mu} = \sqrt{\dfrac{70}{7\times10^{-3}}} = \sqrt{10^4}
  2. So the answer is (c) 100100 m/s.
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Q59JEE Main 2023 · 6 APR · SHIFT 2Easy

Speed of Waves · Speed of sound in solids, liquids and gases

The ratio of speed of sound in hydrogen gas to the speed of sound in oxygen gas at the same temperature is:

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Answer: (d)

  1. Both diatomic (same γ\gamma), same TT: v∝1Mv \propto \dfrac{1}{\sqrt{M}}.
  2. vH2vO2=322=4\dfrac{v_{H_2}}{v_{O_2}} = \sqrt{\dfrac{32}{2}} = 4
  3. So the answer is (d) 4:14:1.
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Q60MHT CET 2023 · 13 MAY · SHIFT 1Medium

Speed of Waves · Hanging rope and rope with a block

A uniform wire 20 m20\text{ m} long and weighing 50 N50\text{ N} hangs vertically. The speed of the wave at mid point of the wire is (acceleration due to gravity =g=10 ms−2= g = 10\text{ ms}^{-2})

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Answer: (c)

  1. At height yy above the lower end, tension =μgy= \mu g y, so v=gyv = \sqrt{gy}.
  2. Midpoint: y=10y = 10 m, v=10×10=10v = \sqrt{10 \times 10} = 10 m/s.
  3. So the answer is (c) 10 ms−110\ \text{ms}^{-1}.
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Q61MHT CET 2023 · 12 MAY · SHIFT 2Medium

Speed of Waves · Effect of temperature, pressure and humidity

A tuning fork of frequency 220 Hz220\text{ Hz} produces sound waves of wavelength 1.5 m1.5\text{ m} in air at N.T.P. The increase in wavelength when the temperature of air is 27∘C27^\circ\text{C} is nearly (300273=1.05)\left(\sqrt{\frac{300}{273}} = 1.05\right)

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Answer: (d)

  1. Frequency fixed, so λ∝v∝T\lambda \propto v \propto \sqrt{T}.
  2. λ′=1.5×300/273=1.5×1.05≈1.575\lambda' = 1.5 \times \sqrt{300/273} = 1.5 \times 1.05 \approx 1.575 m (exact root 1.048 gives 1.572 m).
  3. Increase ≈0.07\approx 0.07 m.
  4. So the answer is (d) 0.07 m.
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Q62MHT CET 2023 · 14 MAY · SHIFT 2Difficult

Speed of Waves · Speed on a stretched string

A wire PQPQ has length 4.8 m4.8\text{ m} and mass 0.06 kg0.06\text{ kg}. Another wire QR has length 2.56 m2.56\text{ m} and mass 0.2 kg0.2\text{ kg}. Both wires have same radii and are joined as a single wire. This wire is under tension of 80 N80\text{ N}. A wave pulse of amplitude 3.5 cm3.5\text{ cm} is sent along the wire PQPQ from end PP. the time taken by the wave pulse to travel along the wire from point P to R is?

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Answer: (c)

  1. PQ: μ1=0.06/4.8=0.0125\mu_1 = 0.06/4.8 = 0.0125 kg/m, v1=80/0.0125=80v_1 = \sqrt{80/0.0125} = 80 m/s, t1=4.8/80=0.06t_1 = 4.8/80 = 0.06 s.
  2. QR: μ2=0.2/2.56=0.078\mu_2 = 0.2/2.56 = 0.078 kg/m, v2=80/0.078125=32v_2 = \sqrt{80/0.078125} = 32 m/s, t2=2.56/32=0.08t_2 = 2.56/32 = 0.08 s.
  3. t=0.06+0.08=0.14t = 0.06 + 0.08 = 0.14 s
  4. So the answer is (c) 0.14 s.
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Q63MHT CET 2023 · 10 MAY · SHIFT 2Difficult

Speed of Waves · Hanging rope and rope with a block

A uniform rope of length 'LL' and mass 'm1m_1 ' hangs vertically from a rigid support. A block of mass 'm2m_2' is attached to the free end of the rope. A transverse wave of wavelength 'λ1\lambda_1' is produced at the lower end of the rope. The wavelength of the wave when it reaches the top of the rope is 'λ2\lambda_2'. The ratio λ1λ2\frac{\lambda_1}{\lambda_2} is

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Answer: (a)

  1. Frequency unchanged, so λ∝T\lambda \propto \sqrt{T}.
  2. Bottom tension m2gm_2 g, top tension (m1+m2)g(m_1+m_2)g.
  3. λ1λ2=[m2m1+m2]1/2\dfrac{\lambda_1}{\lambda_2} = \left[\dfrac{m_2}{m_1+m_2}\right]^{1/2}
  4. So the answer is (a).
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Q64NEET 2022 · PHASE 1Easy

Speed of Waves · Speed on a stretched string

If the initial tension on a stretched string is doubled, then the ratio of the initial and final speeds of a transverse wave along the string is

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Answer: (c)

  1. v∝Tv \propto \sqrt{T}
  2. vivf=T2T=12\dfrac{v_i}{v_f} = \sqrt{\dfrac{T}{2T}} = \dfrac{1}{\sqrt{2}}
  3. So the answer is (c) 1:21:\sqrt{2}.
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Q65NEET 2022 · PHASE 2Medium

Speed of Waves · Effect of temperature, pressure and humidity

An organ pipe filled with a gas at 27∘^\circC resonates at 400 Hz in its fundamental mode. If it is filled with the same gas at 90∘^\circC, the resonance frequency at the same mode will be

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Answer: (c)

  1. Pipe length fixed, so f∝v∝Tf \propto v \propto \sqrt{T}.
  2. f′=400363300=400×1.1=440f' = 400\sqrt{\dfrac{363}{300}} = 400 \times 1.1 = 440 Hz
  3. So the answer is (c) 440 Hz.
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Q66JEE Main 2021 · 25 FEB · SHIFT 2Easy

Speed of Waves · Speed on a stretched string

The percentage increase in the speed of transverse waves produced in a stretched string if the tension is increased by 4%, will be __________%.

Numerical answer type. Work it out, then open the answer.

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Answer: 2

  1. v∝T1/2⇒Δvv=12ΔTTv \propto T^{1/2} \Rightarrow \dfrac{\Delta v}{v} = \dfrac{1}{2}\dfrac{\Delta T}{T}
  2. Δvv=12×4%=2%\dfrac{\Delta v}{v} = \dfrac{1}{2}\times 4\% = 2\%
  3. Answer: 2%2\%.
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Q67MHT CET 2021 · 24 SEP · SHIFT 1Easy

Speed of Waves · Speed of sound in solids, liquids and gases

The wavelength of sound in any gas depends upon

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Answer: (c)

  1. λ=v/f\lambda = v/f and v=E/ρv = \sqrt{E/\rho} depends on the elasticity and density of the gas.
  2. So for a given source, the wavelength in the gas depends on its density and elasticity.
  3. So the answer is (c) density and elasticity of the gas.
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Q68MHT CET 2021 · 23 SEP · SHIFT 2Easy

Speed of Waves · Effect of temperature, pressure and humidity

What is the effect of pressure on the speed of sound in a medium, if pressure is doubled at constant temperature?

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Answer: (a)

  1. v=γP/ρv = \sqrt{\gamma P/\rho}; at constant TT, P∝ρP \propto \rho (Boyle's law), so P/ρP/\rho stays constant.
  2. Equivalently v=γRT/Mv = \sqrt{\gamma RT/M} does not depend on PP.
  3. So the answer is (a) Remains same.
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Q69MHT CET 2021 · 23 SEP · SHIFT 2Difficult

Speed of Waves · Hanging rope and rope with a block

A uniform rope of length 12 m12\text{ m} and mass 6 kg6\text{ kg} hangs vertically from the rigid support. A block of mass 2 kg2\text{ kg} is attached to the free end of the rope. A transverse pulse of wavelength 0.06 m0.06\text{ m} is produced at the lower end of the rope. The wavelength of the pulse when it reaches the top of the rope is

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Answer: (c)

  1. Frequency stays the same along the rope, so λ∝v∝T\lambda \propto v \propto \sqrt{T}.
  2. Tension at the bottom: T1=2gT_1 = 2g; at the top: T2=(6+2)g=8gT_2 = (6+2)g = 8g.
  3. λ2λ1=8g2g=2⇒λ2=2×0.06=0.12 m\dfrac{\lambda_2}{\lambda_1} = \sqrt{\dfrac{8g}{2g}} = 2 \Rightarrow \lambda_2 = 2 \times 0.06 = 0.12\text{ m}
  4. So the answer is (c) 0.12 m0.12\text{ m}.
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Q70MHT CET 2020 · 19 OCT · SHIFT 2Easy

Speed of Waves · Speed on a stretched string

A uniform metal wire has length LL, mass MM and density ρ\rho. It is under tension TT and vv is the speed of transverse wave along the wire. The area of cross-section of the wire is

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Answer: (a)

  1. Mass per unit length μ=ρA\mu = \rho A, so v=TρAv = \sqrt{\dfrac{T}{\rho A}}.
  2. v2=TρA⇒A=Tv2ρv^2 = \dfrac{T}{\rho A} \Rightarrow A = \dfrac{T}{v^2\rho}
  3. So the answer is (a) Tv2ρ\dfrac{T}{v^2\rho}.
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Q71JEE Main 2020 · 8 JAN · SHIFT 2Easy

Speed of Waves · Speed on a stretched string

A transverse wave travels on a taut steel wire with a velocity of v when tension in it is 2.06 × 104 N. When the tension is changed to T, the velocity changed to v/2. The value of T is close to:

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Answer: (d)

  1. T∝v2T \propto v^2, so halving vv makes T′=T/4T' = T/4.
  2. T′=2.06×1044=5.15×103 NT' = \dfrac{2.06\times10^4}{4} = 5.15\times10^3\ \text{N}
  3. So the answer is (d) 5.15×1035.15\times10^3 N.
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Q72MHT CET 2020 · 16 OCT · SHIFT 1Medium

Speed of Waves · Speed on a stretched string

The extension in a wire obeying Hooke's law is xx. The speed of sound in the stretched wire is vv. If the extension in the wire is increased to 4x4x, then the speed of sound in a wire is

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Answer: (b)

  1. Hooke's law: T∝xT \propto x, and v=T/μ∝xv = \sqrt{T/\mu} \propto \sqrt{x}.
  2. v′=v4x/x=2vv' = v\sqrt{4x/x} = 2v
  3. So the answer is (b) 2v2v.
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Q73JEE Main 2020 · 3 SEP · SHIFT 1Medium

Speed of Waves · Hanging rope and rope with a block

A uniform thin rope of length 12 m and mass 6 kg hangs vertically from a rigid support and a block of mass 2 kg is attached to its free end. A transverse short wavetrain of wavelength 6 cm is produced at the lower end of the rope. What is the wavelength of the wavetrain (in cm) when it reaches the top of the rope?

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Answer: (a)

  1. λ∝T\lambda \propto \sqrt{T} (frequency unchanged).
  2. Bottom T=2gT = 2g, top T=(6+2)g=8gT = (6+2)g = 8g, so λtop=68/2=12\lambda_{top} = 6\sqrt{8/2} = 12 cm.
  3. So the answer is (a) 12.
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Q74JEE Main 2020 · 7 JAN · SHIFT 1Difficult

Speed of Waves · Speed on a stretched string

Speed of a transverse wave on a straight wire (mass 6.0 g, length 60 cm and area of cross-section 1.0 mm2) is 90 ms-1. If the Young's modulus of wire is 16 ×\times 1011 Nm-2, the extension of wire over its natural length is:

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Answer: (a)

  1. μ=6×10−3/0.6=0.01\mu = 6\times10^{-3}/0.6 = 0.01 kg/m, so T=μv2=0.01×902=81T = \mu v^2 = 0.01 \times 90^2 = 81 N.
  2. Δl=TLAY=81×0.610−6×16×1011=3.0×10−5\Delta l = \dfrac{TL}{AY} = \dfrac{81 \times 0.6}{10^{-6} \times 16\times10^{11}} = 3.0\times10^{-5} m
  3. So the answer is (a) 0.03 mm.
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Q75JEE Main 2019 · 9 JAN · SHIFT 1Difficult

Speed of Waves · Speed on a stretched string

A heavy ball of mass M is suspendeed from the ceiling of a car by a light string of mass m (m < < M). When the car is at rest, the speed of transverse waves in the string is 60 ms−1{}^{-1}. When the car has acceleration a, the wave-speed increases to 60.5 ms−1{}^{-1}. The value of a, in terms of gravitational acceleration g, is closest to:

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Answer: (b)

  1. Tension ∝geff\propto g_{eff}; at rest geff=gg_{eff} = g, with acceleration geff=g2+a2g_{eff} = \sqrt{g^2 + a^2}.
  2. v∝Tv \propto \sqrt{T}: g2+a2g=(60.560)2≈1.0168\dfrac{\sqrt{g^2+a^2}}{g} = \left(\dfrac{60.5}{60}\right)^2 \approx 1.0168
  3. a2=(1.01682−1)g2≈0.034 g2⇒a≈0.18ga^2 = (1.0168^2 - 1)g^2 \approx 0.034\,g^2 \Rightarrow a \approx 0.18g
  4. So the answer is (b) g5\dfrac{g}{5}.
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Q76JEE Main 2019 · 9 APR · SHIFT 1Difficult

Speed of Waves · Effect of temperature, pressure and humidity

The pressure wave, P = 0.01 sin [1000t – 3x] Nm–2, corresponds to the sound produced by a vibrating blade on a day when atmospheric temperature is 0°C. On some other day, when temperature is T, the speed of sound produced by the same blade and at the same frequency is found to be 336 ms–1. Approximate value of T is

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Answer: (c)

  1. At 0∘C0^\circ\text{C}: v0=ωk=10003=333.3 m/sv_0 = \dfrac{\omega}{k} = \dfrac{1000}{3} = 333.3\text{ m/s}.
  2. v∝Tv \propto \sqrt{T}, so T=273(336333.3)2≈273×1.016≈277.4 KT = 273\left(\dfrac{336}{333.3}\right)^2 \approx 273 \times 1.016 \approx 277.4\text{ K}
  3. T≈4.4∘CT \approx 4.4^\circ\text{C}
  4. So the answer is (c) 4∘C4^\circ\text{C}.
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Q77JEE Main 2018Difficult

Speed of Waves · Speed of sound in solids, liquids and gases

A granite rod of 60 cm length is clamped at its middle point and is set into longitudinal vibrations. The density of granite is 2.7 ×\times 103 kg/m3 and its Young’s modulus is 9.27 ×\times 1010 Pa. What will be the fundamental frequency of the longitudinal vibrations?

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Answer: (b)

  1. Clamped at the middle, both ends free: fundamental has L=λ2L = \dfrac{\lambda}{2}, so λ=2×0.6=1.2 m\lambda = 2 \times 0.6 = 1.2\text{ m}.
  2. v=Yρ=9.27×10102.7×103≈5.86×103 m/sv = \sqrt{\dfrac{Y}{\rho}} = \sqrt{\dfrac{9.27 \times 10^{10}}{2.7 \times 10^{3}}} \approx 5.86 \times 10^{3}\text{ m/s}
  3. f=vλ=58601.2≈4.9×103 Hzf = \dfrac{v}{\lambda} = \dfrac{5860}{1.2} \approx 4.9 \times 10^{3}\text{ Hz}
  4. So the answer is (b) 5 kHz5\text{ kHz}.
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Q78NEET 2016 · PHASE 1Medium

Speed of Waves · Hanging rope and rope with a block

A uniform rope of length L and mass m1 hangs vertically from a rigid support. A block of mass m2 is attached to the free end of the rope. A transverse pulse of wavelength λ\lambda1 is produced at the lower end of the rope. The wavelength of the pulse when it reaches the top of the rope is λ\lambda2. The ratio λ\lambda 2/λ\lambda1 is

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Answer: (d)

  1. Frequency stays the same, so λ∝v∝T\lambda \propto v \propto \sqrt{T}.
  2. Bottom: T1=m2gT_1 = m_2 g; top: T2=(m1+m2)gT_2 = (m_1+m_2)g.
  3. λ2λ1=m1+m2m2\dfrac{\lambda_2}{\lambda_1} = \sqrt{\dfrac{m_1+m_2}{m_2}}
  4. So the answer is (d).
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Q79JEE Main 2016Medium

Speed of Waves · Hanging rope and rope with a block

A uniform string of length 20 m20\text{ m} is suspended from a rigid support. A short wave pulse is introduced at its lowest end. It starts moving up the string. The time taken to reach the supports is: (take g=10 ms−2g = 10\text{ ms}^{-2})

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Answer: (a)

  1. At distance yy from the lower end, v=gyv = \sqrt{gy}, so dt=dygydt = \dfrac{dy}{\sqrt{gy}}.
  2. t=∫0Ldygy=2Lg=22010t = \displaystyle\int_0^L \dfrac{dy}{\sqrt{gy}} = 2\sqrt{\dfrac{L}{g}} = 2\sqrt{\dfrac{20}{10}}
  3. So the answer is (a) 222\sqrt{2} s.
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Q80NEET 2015 · AIPMTMedium

Speed of Waves · Speed of sound in solids, liquids and gases

4.0 g of a gas occupies 22.4 litres at NTP. The specific heat capacity of the gas at constant volume is 5.0 J K−1{}^{-1} mol−1{}^{-1}. If the speed of sound in this gas at NTP is 952 m s−1{}^{-1}, then the heat capacity at constant pressure is

(Take gas constant R == 8.3 J K−1{}^{-1} mol−1{}^{-1})

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Answer: (c)

  1. 22.4 L at NTP is 1 mol, so M=4M = 4 g/mol =4×10−3= 4\times10^{-3} kg/mol.
  2. γ=v2MRT=9522×4×10−38.3×273≈1.6\gamma = \dfrac{v^2 M}{RT} = \dfrac{952^2 \times 4\times10^{-3}}{8.3 \times 273} \approx 1.6
  3. Cp=γCv=1.6×5.0=8.0 J K−1mol−1C_p = \gamma C_v = 1.6 \times 5.0 = 8.0\ \text{J K}^{-1}\text{mol}^{-1}
  4. So the answer is (c).
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Q81NEET 1993 · AIPMTEasy

Speed of Waves · Effect of temperature, pressure and humidity

The temperature at which the speed of sound becomes double as was at 27∘C27^\circ\text{C} is

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Answer: (c)

  1. v∝Tv \propto \sqrt{T} (kelvin), so doubling vv needs T′=4TT' = 4T.
  2. T′=4×300=1200 K=927∘CT' = 4 \times 300 = 1200\ \text{K} = 927^\circ\text{C}
  3. So the answer is (c) 927∘927^\circC.
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Q82NEET 1989 · AIPMTEasy

Speed of Waves · Speed on a stretched string

A 5.55.5 metre length of string has a mass of 0.035 kg0.035\text{ kg}. If the tension in the string in 77 N77\text{ N}, the speed of a wave on the string is

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Answer: (a)

  1. μ=0.035/5.5=6.36×10−3 kg/m\mu = 0.035/5.5 = 6.36\times10^{-3}\ \text{kg/m}
  2. v=T/μ=77×5.50.035=12100v = \sqrt{T/\mu} = \sqrt{\dfrac{77 \times 5.5}{0.035}} = \sqrt{12100}
  3. So the answer is (a) 110 m s−1110\ \text{m s}^{-1}.
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Q83NEET 1988 · AIPMTEasy

Speed of Waves · Speed of sound in solids, liquids and gases

The velocity of sound in any gas depends upon

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Answer: (b)

  1. v=γP/ρv = \sqrt{\gamma P/\rho} (bulk modulus over density); it does not depend on wavelength, intensity, amplitude or frequency.
  2. So the answer is (b) density and elasticity of gas.
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Q84MHT CET 2026 · 15 MAY · SHIFT 1Easy

Progressive Wave Equation · Reading the wave equation

The equation of a wave is y=0.07sin⁡(12πx−3000πt)y = 0.07\sin(12\pi x - 3000\pi t) where xx is in metre and tt is in second then 11 m m

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Answer: (a)

  1. Compare with y=Asin⁡(kx−ωt)y = A\sin(kx - \omega t): A=0.07 mA = 0.07\text{ m}, k=12πk = 12\pi, ω=3000π\omega = 3000\pi.
  2. λ=2πk=2π12π=16 m\lambda = \dfrac{2\pi}{k} = \dfrac{2\pi}{12\pi} = \dfrac{1}{6}\text{ m}, n=ω2π=1500 Hzn = \dfrac{\omega}{2\pi} = 1500\text{ Hz}
  3. v=ωk=3000π12π=250 m/sv = \dfrac{\omega}{k} = \dfrac{3000\pi}{12\pi} = 250\text{ m/s}
  4. So the answer is (a) λ=16 m\lambda = \dfrac{1}{6}\text{ m}, v=250 m/sv = 250\text{ m/s}.
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Q85MHT CET 2026 · 14 MAY · SHIFT 2Easy

Progressive Wave Equation · Reading the wave equation

The equation of a plane progressive wave is Y=0.025sin⁡(100t+0.25x)Y = 0.025\sin(100t + 0.25x). The frequency of this wave would be

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Answer: (a)

  1. Compare with Y=Asin⁡(ωt+kx)Y = A\sin(\omega t + kx): ω=100 rad/s\omega = 100\text{ rad/s}.
  2. f=ω2π=1002π=50π Hzf = \dfrac{\omega}{2\pi} = \dfrac{100}{2\pi} = \dfrac{50}{\pi}\text{ Hz}
  3. So the answer is (a) 50π Hz\dfrac{50}{\pi}\text{ Hz}.
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Q86MHT CET 2026 · 16 APR · SHIFT 1Easy

Progressive Wave Equation · Reading the wave equation

The equation of wave motion is Y=6sin⁡(12πt−0.02πx+π3)Y = 6\sin\left(12\pi t - 0.02\pi x + \frac{\pi}{3}\right) where x is in metre and time in second. The velocity of the wave is

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Answer: (d)

  1. ω=12π\omega = 12\pi, k=0.02πk = 0.02\pi
  2. v=ωk=12π0.02π=600 m/sv = \dfrac{\omega}{k} = \dfrac{12\pi}{0.02\pi} = 600\text{ m/s}
  3. So the answer is (d) 600 m/s600\text{ m/s}.
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Q87MHT CET 2026 · 13 APR · SHIFT 2Easy

Progressive Wave Equation · Reading the wave equation

A traveling wave is described by the equation y(x,t)=[0.05sin⁡(8x−4t)]y(x, t) = [0.05\sin(8x - 4t)] m

The velocity of the wave is [All the quantities are in SI unit]

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Answer: (c)

  1. k=8 m−1k = 8\text{ m}^{-1}, ω=4 rad/s\omega = 4\text{ rad/s}
  2. v=ωk=48=0.5 m/sv = \dfrac{\omega}{k} = \dfrac{4}{8} = 0.5\text{ m/s}
  3. So the answer is (c) 0.5 m s−10.5\text{ m s}^{-1}.
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Q88MHT CET 2026 · 11 APR · SHIFT 2Easy

Progressive Wave Equation · Reading the wave equation

The equation of a progressive wave is Y=3sin⁡[π(t3−x5)+π4]Y = 3\sin\left[\pi\left(\frac{t}{3} - \frac{x}{5}\right) + \frac{\pi}{4}\right] where X and Y are in metre and time in second. Which of the following is correct?

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Answer: (c)

  1. Y=3sin⁡(π3t−π5x+π4)Y = 3\sin\left(\dfrac{\pi}{3}t - \dfrac{\pi}{5}x + \dfrac{\pi}{4}\right): A=3 mA = 3\text{ m}, ω=π3\omega = \dfrac{\pi}{3}, k=π5k = \dfrac{\pi}{5}.
  2. λ=2πk=10 m\lambda = \dfrac{2\pi}{k} = 10\text{ m}; f=ω2π=16 Hzf = \dfrac{\omega}{2\pi} = \dfrac{1}{6}\text{ Hz}; v=ωk=53 m/sv = \dfrac{\omega}{k} = \dfrac{5}{3}\text{ m/s}
  3. Only the wavelength matches.
  4. So the answer is (c) wavelength =10 m= 10\text{ m}.
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Q89JEE Main 2026 · 2 APR · SHIFT 1Easy

Progressive Wave Equation · Reading the wave equation

The equation of a plane progressive wave is given by y=5cos⁡π(200t−x150)y = 5\cos\pi\left(200t - \frac{x}{150}\right) where xx and yy are in cm and tt is in second. The velocity of the wave is ________ m/s.

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Answer: (d)

  1. y=5cos⁡(200πt−π150x)y = 5\cos\left(200\pi t - \dfrac{\pi}{150}x\right): ω=200π s−1\omega = 200\pi\text{ s}^{-1}, k=π150 cm−1k = \dfrac{\pi}{150}\text{ cm}^{-1}.
  2. v=ωk=200×150=30000 cm/s=300 m/sv = \dfrac{\omega}{k} = 200 \times 150 = 30000\text{ cm/s} = 300\text{ m/s}
  3. So the answer is (d) 300 m/s300\text{ m/s}.
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Q90JEE Main 2026 · 5 APR · SHIFT 1Easy

Progressive Wave Equation · Reading the wave equation

A transverse wave on a string is described by y=3sin⁡(36t+0.018x+π/4)y = 3\sin(36t + 0.018x + \pi/4), where x,yx, y are in cm and tt in seconds. The least distance between the two successive crests in the wave is ______ cm. (Nearest integer)

(π=3.14)(\pi = 3.14)

Numerical answer type. Work it out, then open the answer.

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Answer: 349

  1. Distance between successive crests is the wavelength λ=2πk\lambda = \dfrac{2\pi}{k}.
  2. k=0.018 cm−1k = 0.018\text{ cm}^{-1}
  3. λ=2×3.140.018=348.9 cm\lambda = \dfrac{2 \times 3.14}{0.018} = 348.9\text{ cm}
  4. So the answer is 349 cm349\text{ cm}.
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Q91MHT CET 2026 · 14 MAY · SHIFT 1Easy

Progressive Wave Equation · Writing the wave equation and its direction

A wave travelling in the positive xx-direction having displacement along yy-direction as 11 m, wavelength 2π2\pi m and frequency Hz is represented by

1π\frac{1}{\pi}

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Answer: (a)

  1. k=2πλ=2π2π=1 m−1k = \dfrac{2\pi}{\lambda} = \dfrac{2\pi}{2\pi} = 1\text{ m}^{-1}
  2. ω=2πf=2π×1π=2 rad/s\omega = 2\pi f = 2\pi \times \dfrac{1}{\pi} = 2\text{ rad/s}
  3. Wave along +x+x with A=1 mA = 1\text{ m}: y=sin⁡(kx−ωt)=sin⁡(x−2t)y = \sin(kx - \omega t) = \sin(x - 2t)
  4. So the answer is (a) y=sin⁡(x−2t)y = \sin(x - 2t).
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Q92MHT CET 2026 · 19 APR · SHIFT 2Easy

Progressive Wave Equation · Particle velocity and wave velocity

The equation of a progressive wave is given by y=6cos⁡(100t−4x)y = 6\cos(100t - 4x) where yy is in μ\mum, xx in metre and tt in second. The ratio of the maximum particle velocity to the velocity of wave is

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Answer: (c)

  1. For y=Acos⁡(ωt−kx)y = A\cos(\omega t - kx): vmax=Aωv_{max} = A\omega and v=ωkv = \frac{\omega}{k}, so vmaxv=Ak\frac{v_{max}}{v} = Ak.
  2. A=6 μm=6×10−6A = 6\ \mu\text{m} = 6 \times 10^{-6} m, k=4 m−1k = 4\ \text{m}^{-1}
  3. vmaxv=6×10−6×4=2.4×10−5\frac{v_{max}}{v} = 6 \times 10^{-6} \times 4 = 2.4 \times 10^{-5}
  4. So the answer is (c) 2.4×10−52.4 \times 10^{-5}.
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Q93MHT CET 2026 · 15 MAY · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

In a sine wave, minimum distance between 22 particles always having same speed is

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Answer: (a)

  1. Particle speed =Aω∣cos⁡ϕ∣= A\omega|\cos\phi|, so two particles always have the same speed if their phases differ by π\pi.
  2. Phase difference π\pi corresponds to path difference λ2π×π=λ2\frac{\lambda}{2\pi} \times \pi = \frac{\lambda}{2}.
  3. So the answer is (a) λ2\frac{\lambda}{2}.
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Q94MHT CET 2026 · 15 MAY · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

Two points separated by 66 cm on a string has phase difference of 60∘60^\circ. If frequency of oscillation is 500500 Hz, the velocity of the wave in ms\frac{m}{s} is

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Answer: (b)

  1. Δϕ=2πλΔx\Delta\phi = \frac{2\pi}{\lambda}\Delta x; 60∘=π360^\circ = \frac{\pi}{3} means Δx=λ6\Delta x = \frac{\lambda}{6}.
  2. λ=6×6=36\lambda = 6 \times 6 = 36 cm =0.36= 0.36 m
  3. v=fλ=500×0.36=180v = f\lambda = 500 \times 0.36 = 180 m/s
  4. So the answer is (b) 180180.
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Q95MHT CET 2026 · 13 MAY · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

The path difference between two waves Y1=a1sin⁡(ωt−2πxλ)Y_1 = a_1\sin\left(\omega t - \frac{2\pi x}{\lambda}\right) and Y2=a2cos⁡(ωt−2πxλ+Φ)Y_2 = a_2\cos\left(\omega t - \frac{2\pi x}{\lambda} + \Phi\right) is

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Answer: (b)

  1. Write Y2Y_2 as a sine: cos⁡θ=sin⁡(θ+π2)\cos\theta = \sin\left(\theta + \frac{\pi}{2}\right), so Y2=a2sin⁡(ωt−2πxλ+Φ+π2)Y_2 = a_2\sin\left(\omega t - \frac{2\pi x}{\lambda} + \Phi + \frac{\pi}{2}\right).
  2. Phase difference Δϕ=Φ+π2\Delta\phi = \Phi + \frac{\pi}{2}
  3. Path difference =λ2πΔϕ=λ2π(Φ+π2)= \frac{\lambda}{2\pi}\Delta\phi = \frac{\lambda}{2\pi}\left(\Phi + \frac{\pi}{2}\right)
  4. So the answer is (b).
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Q96MHT CET 2026 · 13 MAY · SHIFT 1Easy

Progressive Wave Equation · Phase difference and path difference

Two points on a travelling wave having frequency 500500 Hz and velocity 300300 m/s are 60∘60^\circ out of phase, then the minimum distance between the two points is

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Answer: (b)

  1. λ=vf=300500=0.6\lambda = \frac{v}{f} = \frac{300}{500} = 0.6 m
  2. 60∘=π360^\circ = \frac{\pi}{3}, so Δx=λ2π×π3=λ6\Delta x = \frac{\lambda}{2\pi} \times \frac{\pi}{3} = \frac{\lambda}{6}
  3. Δx=0.66=0.1\Delta x = \frac{0.6}{6} = 0.1 m
  4. So the answer is (b) 0.10.1 m.
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Q97MHT CET 2026 · 12 MAY · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

The equation of a wave travelling on a string is Y=sin⁡(20πx+10πt)Y = \sin(20\pi x + 10\pi t), where xx and tt are distance and time in SI units. The minimum distance between two points having the same oscillating speed is

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Answer: (b)

  1. k=20π m−1k = 20\pi\ \text{m}^{-1}, so λ=2πk=0.1\lambda = \frac{2\pi}{k} = 0.1 m =10= 10 cm.
  2. Points always having the same speed are at least λ2\frac{\lambda}{2} apart (phase difference π\pi).
  3. λ2=5\frac{\lambda}{2} = 5 cm
  4. So the answer is (b) 55 cm.
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Q98MHT CET 2026 · 12 MAY · SHIFT 1Easy

Progressive Wave Equation · Phase difference and path difference

Two simple harmonic progressive waves have displacements y1=5sin⁡(2πxλ−ωt)y_1 = 5\sin\left(\frac{2\pi x}{\lambda} - \omega t\right) and y2=5cos⁡(2πxλ−ωt+π6)y_2 = 5\cos\left(\frac{2\pi x}{\lambda} - \omega t + \frac{\pi}{6}\right). The phase difference between the two waves is

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Answer: (c)

  1. Let θ=2πxλ−ωt\theta = \frac{2\pi x}{\lambda} - \omega t. Then y1=5sin⁡θy_1 = 5\sin\theta.
  2. y2=5cos⁡(θ+π6)=5sin⁡(θ+π6+π2)=5sin⁡(θ+2π3)y_2 = 5\cos\left(\theta + \frac{\pi}{6}\right) = 5\sin\left(\theta + \frac{\pi}{6} + \frac{\pi}{2}\right) = 5\sin\left(\theta + \frac{2\pi}{3}\right)
  3. Phase difference =2π3= \frac{2\pi}{3}
  4. So the answer is (c) 2π3\frac{2\pi}{3}.
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Q99MHT CET 2026 · 20 APR · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

Two waves are represented as

Figureand

The path difference between two waves is

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Answer: (c)

  1. From the figure: y1=a1sin⁡(ωt−2πxλ)y_1 = a_1\sin\left(\omega t - \frac{2\pi x}{\lambda}\right), y2=a2cos⁡(ωt−2πxλ+π6)y_2 = a_2\cos\left(\omega t - \frac{2\pi x}{\lambda} + \frac{\pi}{6}\right).
  2. y2=a2sin⁡(ωt−2πxλ+π6+π2)y_2 = a_2\sin\left(\omega t - \frac{2\pi x}{\lambda} + \frac{\pi}{6} + \frac{\pi}{2}\right), so Δϕ=2π3\Delta\phi = \frac{2\pi}{3}.
  3. Path difference =λ2π×2π3=λ3= \frac{\lambda}{2\pi} \times \frac{2\pi}{3} = \frac{\lambda}{3}
  4. So the answer is (c) λ3\frac{\lambda}{3}.
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Q100MHT CET 2026 · 16 APR · SHIFT 1Easy

Progressive Wave Equation · Phase difference and path difference

A progressive wave of frequency 50 Hz is travelling with velocity 350 m/s through a medium. The change in phase at given time interval of 0.01s is

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Answer: (c)

  1. At a fixed point, phase changes with time as Δϕ=ω Δt=2πf Δt\Delta\phi = \omega\,\Delta t = 2\pi f\,\Delta t.
  2. Δϕ=2π×50×0.01=π\Delta\phi = 2\pi \times 50 \times 0.01 = \pi rad
  3. So the answer is (c) π\pi rad.
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Q101MHT CET 2026 · 15 APR · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

A simple harmonic progressive wave is represented by y=Asin⁡(120πt+3x)y = A\sin(120\pi t + 3x). The distance between two points on the wave at a phase difference of π3\frac{\pi}{3} radian is

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Answer: (b)

  1. From y=Asin⁡(120πt+3x)y = A\sin(120\pi t + 3x): k=3 m−1k = 3\ \text{m}^{-1}.
  2. Δx=Δϕk=π/33=π9\Delta x = \frac{\Delta\phi}{k} = \frac{\pi/3}{3} = \frac{\pi}{9} m
  3. So the answer is (b) π9\frac{\pi}{9} m.
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Q102MHT CET 2026 · 13 APR · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

Two waves are represented by the equations, y1=asin⁡(ωt+kx+0.57)y_1 = a\sin(\omega t + kx + 0.57) m and y2=acos⁡(ωt+kx)y_2 = a\cos(\omega t + kx) m, where xx is in metre and tt is in second. What is the phase difference between them? (π=3.14\pi = 3.14)

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Answer: (d)

  1. y2=acos⁡(ωt+kx)=asin⁡(ωt+kx+π2)=asin⁡(ωt+kx+1.57)y_2 = a\cos(\omega t + kx) = a\sin\left(\omega t + kx + \frac{\pi}{2}\right) = a\sin(\omega t + kx + 1.57)
  2. y1y_1 has phase constant 0.570.57, y2y_2 has 1.571.57.
  3. Δϕ=1.57−0.57=1.0\Delta\phi = 1.57 - 0.57 = 1.0 rad
  4. So the answer is (d) 1.01.0 radian.
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Q103MHT CET 2026 · 13 APR · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

The distance between two consecutive points with phase difference of 60∘60^\circ in a wave of frequency nn is xx meter. The velocity with which wave is traveling is

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Answer: (d)

  1. 60∘=π360^\circ = \frac{\pi}{3} corresponds to Δx=λ6\Delta x = \frac{\lambda}{6}, so x=λ6x = \frac{\lambda}{6} and λ=6x\lambda = 6x.
  2. v=nλ=6nxv = n\lambda = 6nx
  3. So the answer is (d) 6nx6nx.
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Q104NEET 2026Easy

Progressive Wave Equation · Phase difference and path difference

For a travelling harmonic wave

y(x,t)=2.0cos⁡2π(10t−0.0080x+0.35)y(x, t) = 2.0\cos 2\pi(10t - 0.0080x + 0.35), where xx and yy are in cm and tt in s\text{s}. The phase difference between oscillatory motion of two points separated by a distance of 0.5 m is:

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Answer: (b)

  1. k=2π×0.0080 cm−1k = 2\pi \times 0.0080\ \text{cm}^{-1} (xx in cm).
  2. Δx=0.5\Delta x = 0.5 m =50= 50 cm
  3. Δϕ=k Δx=2π×0.0080×50=0.8π\Delta\phi = k\,\Delta x = 2\pi \times 0.0080 \times 50 = 0.8\pi rad
  4. So the answer is (b) 0.8π0.8\pi rad.
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Q105MHT CET 2026 · 12 MAY · SHIFT 1Medium

Progressive Wave Equation · Particle velocity and wave velocity

A simple harmonic progressive wave is given by the equation y=asin⁡2π(nt−xλ)y = a\sin 2\pi\left(nt - \frac{x}{\lambda}\right). If the wave velocity is equal to 16×\frac{1}{6} \times (maximum particle velocity), then the wavelength λ\lambda is {a=\{a = amplitude, n=n = frequency, t=t = time, y=y = displacement, x=x = distance}\}

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Answer: (b)

  1. Wave velocity v=nλv = n\lambda; maximum particle velocity =aω=2πna= a\omega = 2\pi n a
  2. nλ=16(2πna)⇒λ=πa3n\lambda = \frac{1}{6}(2\pi n a) \Rightarrow \lambda = \frac{\pi a}{3}
  3. So the answer is (b) πa3\frac{\pi a}{3}.
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Q106MHT CET 2026 · 15 MAY · SHIFT 1Medium

Progressive Wave Equation · Tension from the wave equation

A transverse wave is propagating on the string. The linear density of vibrating string is 10−310^{-3} kg/m. The equation of the wave is Y=0.05sin⁡(x+15t)Y = 0.05\sin(x + 15t) where xx and YY are in metre and time in second. The tension in the string is

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Answer: (c)

  1. Wave speed v=ωk=151=15 m/sv = \frac{\omega}{k} = \frac{15}{1} = 15\text{ m/s}
  2. v=T/μ⇒T=μv2=10−3×225v = \sqrt{T/\mu} \Rightarrow T = \mu v^2 = 10^{-3} \times 225
  3. T=0.225 NT = 0.225\text{ N}
  4. So the answer is (c) 0.225 N.
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Q107MHT CET 2026 · 20 APR · SHIFT 2Medium

Progressive Wave Equation · Tension from the wave equation

The equation of a wave on a string of linear mass density 0.020.02 kg m−1^{-1} is

Y=0.01sin⁡[2π(t0.02−x0.50)]Y = 0.01\sin\left[2\pi\left(\frac{t}{0.02} - \frac{x}{0.50}\right)\right] m. The tension in the string is

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Answer: (a)

  1. From the equation: Tperiod=0.02 sT_{period} = 0.02\text{ s} (f=50 Hzf = 50\text{ Hz}), λ=0.50 m\lambda = 0.50\text{ m}
  2. v=fλ=50×0.5=25 m/sv = f\lambda = 50 \times 0.5 = 25\text{ m/s}
  3. Tension =μv2=0.02×625=12.5 N= \mu v^2 = 0.02 \times 625 = 12.5\text{ N}
  4. So the answer is (a) 12.50 N.
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Q108MHT CET 2025 · 21 APR · SHIFT 2Easy

Progressive Wave Equation · Reading the wave equation

The equation of a progressive wave is Y=3sin⁡[π(t3−x5)+π4]Y = 3\sin\left[\pi\left(\frac{t}{3} - \frac{x}{5}\right) + \frac{\pi}{4}\right] where x and y are in meter and time in second. Which of the following is correct?

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Answer: (a)

  1. ω=π3\omega = \dfrac{\pi}{3}, k=π5k = \dfrac{\pi}{5}, A=3 mA = 3\text{ m}.
  2. λ=2ππ/5=10 m\lambda = \dfrac{2\pi}{\pi/5} = 10\text{ m}; v=53 m/sv = \dfrac{5}{3}\text{ m/s}; f=16 Hzf = \dfrac{1}{6}\text{ Hz}
  3. So the answer is (a) wavelength =10 m= 10\text{ m}.
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Q109JEE Main 2025 · 4 APR · SHIFT 2Easy

Progressive Wave Equation · Reading the wave equation

Displacement of a wave is expressed as x(t)=5cos⁡(628t+π2)mx(t) = 5\cos\left(628t + \frac{\pi}{2}\right)\text{m}. The wavelength of the wave when its velocity is 300 m/s300\text{ m/s} is:

(π=3.14)(\pi = 3.14)

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Answer: (c)

  1. ω=628 rad/s\omega = 628\text{ rad/s}, so f=6282×3.14=100 Hzf = \dfrac{628}{2 \times 3.14} = 100\text{ Hz}.
  2. λ=vf=300100=3 m\lambda = \dfrac{v}{f} = \dfrac{300}{100} = 3\text{ m}
  3. So the answer is (c) 3 m3\text{ m}.
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Q110JEE Main 2025 · 23 JAN · SHIFT 2Easy

Progressive Wave Equation · Reading the wave equation

The equation of a transverse wave travelling along a string is

y(x,t)=4.0sin⁡[20×10−3x+600t]mmy(x, t) = 4.0\sin\left[20 \times 10^{-3}x + 600t\right]\text{mm}, where xx is in mm and tt is in second. The velocity of the wave is:

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Answer: (d)

  1. k=20×10−3 mm−1k = 20 \times 10^{-3}\text{ mm}^{-1}, ω=600 s−1\omega = 600\text{ s}^{-1}
  2. v=ωk=6000.02=3×104 mm/s=30 m/sv = \dfrac{\omega}{k} = \dfrac{600}{0.02} = 3 \times 10^{4}\text{ mm/s} = 30\text{ m/s}
  3. kxkx and ωt\omega t have the same sign, so the wave moves along −x-x.
  4. So the answer is (d) −30 m/s-30\text{ m/s}.
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Q111MHT CET 2025 · 23 APR · SHIFT 1Easy

Progressive Wave Equation · Particle velocity and wave velocity

A particle performs S.H.M. of amplitude 'A' and wavelength ' λ\lambda ', Then the velocity of the wave (V) and the maximum particle velocity (v) are related as

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Answer: (c)

  1. Maximum particle velocity v=Aωv = A\omega; wave velocity V=ωk=ωλ2πV = \frac{\omega}{k} = \frac{\omega\lambda}{2\pi}.
  2. vV=Aωωλ/2π=2πAλ\frac{v}{V} = \frac{A\omega}{\omega\lambda/2\pi} = \frac{2\pi A}{\lambda}
  3. So the answer is (c) v=2πAλVv = \frac{2\pi A}{\lambda}V.
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Q112MHT CET 2025 · 22 APR · SHIFT 1Easy

Progressive Wave Equation · Particle velocity and wave velocity

The equation of wave is y=60sin⁡(1200t−6x)y = 60\sin(1200t - 6x), where ' yy ' is in micron, ' tt ' is in second and ' xx ' is in metre. The ratio of maximum particle velocity to the wave velocity of wave propagation is

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Answer: (c)

  1. vmaxv=Aωω/k=Ak\frac{v_{max}}{v} = \frac{A\omega}{\omega/k} = Ak
  2. A=60 μm=6×10−5A = 60\ \mu\text{m} = 6 \times 10^{-5} m, k=6 m−1k = 6\ \text{m}^{-1}
  3. Ak=6×10−5×6=3.6×10−4Ak = 6 \times 10^{-5} \times 6 = 3.6 \times 10^{-4}
  4. So the answer is (c) 3.6×10−43.6 \times 10^{-4}.
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Q113MHT CET 2025 · 5 MAY · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

The distance between two consecutive points with phase difference of 45∘45^\circ in a wave of frequency 300 Hz is 4.0 m. The velocity of the travelling wave is (in km/s\text{km/s})

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Answer: (d)

  1. 45∘=π445^\circ = \frac{\pi}{4} corresponds to Δx=λ8\Delta x = \frac{\lambda}{8}, so λ=8×4=32\lambda = 8 \times 4 = 32 m.
  2. v=fλ=300×32=9600v = f\lambda = 300 \times 32 = 9600 m/s
  3. So the answer is (d) 9.69.6 km/s.
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Q114MHT CET 2025 · 19 APR · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

A progressive wave of frequency 400 Hz is travelling with velocity 336 m/s336\text{ m/s}. How far apart are the two points on a wave which are 60∘60^\circ out of phase?

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Answer: (b)

  1. λ=vf=336400=0.84\lambda = \frac{v}{f} = \frac{336}{400} = 0.84 m
  2. 60∘60^\circ out of phase means Δx=λ6=0.846=0.14\Delta x = \frac{\lambda}{6} = \frac{0.84}{6} = 0.14 m
  3. So the answer is (b) 0.140.14 m.
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Q115JEE Main 2025 · 7 APR · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

The equation of a wave travelling on a string is y = sin[20πx + 10πt], where x and t are distance and time in SI units. The minimum distance between two points having the same oscillating speed is:

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Answer: (d)

  1. k=20π m−1⇒λ=2πk=0.1 m=10 cmk = 20\pi\text{ m}^{-1} \Rightarrow \lambda = \frac{2\pi}{k} = 0.1\text{ m} = 10\text{ cm}
  2. Particle speed ∝∣cos⁡(20πx+10πt)∣\propto |\cos(20\pi x + 10\pi t)|, which repeats when the phase changes by π\pi.
  3. Phase difference π\pi corresponds to Δx=λ2=5 cm\Delta x = \frac{\lambda}{2} = 5\text{ cm}
  4. So the answer is (d) 5.0 cm.
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Q116JEE Main 2025 · 2 APR · SHIFT 2Medium

Progressive Wave Equation · Writing the wave equation and its direction

A sinusoidal wave of wavelength 7.5 cm travels a distance of 1.2 cm along the xx-direction in 0.3 sec. The crest P is at x=0x = 0 at t=0 sect = 0\text{ sec} and maximum displacement of the wave is 2 cm. Which equation correctly represents this wave?

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Answer: (a)

  1. v=1.20.3=4 cm/sv = \frac{1.2}{0.3} = 4\text{ cm/s}, k=2π7.5=0.83 cm−1k = \frac{2\pi}{7.5} = 0.83\text{ cm}^{-1}
  2. ω=kv=0.838×4≈3.35 rad/s\omega = kv = 0.838 \times 4 \approx 3.35\text{ rad/s}
  3. Crest at x=0x = 0, t=0t = 0 means y=Ay = A there, so use cosine; travelling along +x+x gives (kx−ωt)(kx - \omega t).
  4. So the answer is (a) y=2cos⁡(0.83x−3.35t) cmy = 2\cos(0.83x - 3.35t)\text{ cm}.
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Q117MHT CET 2025 · 21 APR · SHIFT 2Medium

Progressive Wave Equation · Tension from the wave equation

A transverse displacement of vibrating string is y=0.06sin⁡(2π3x)cos⁡(120πt)y = 0.06\sin\left(\frac{2\pi}{3}x\right)\cos(120\pi t).

If the mass per unit length of a string is 4×10−2 kg/m4 \times 10^{-2}\text{ kg/m}, then the tension in the string will be

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Answer: (a)

  1. Stationary wave: k=2π3 m−1k = \frac{2\pi}{3}\text{ m}^{-1}, ω=120π rad/s\omega = 120\pi\text{ rad/s}
  2. Speed of component waves v=ωk=120π×32π=180 m/sv = \frac{\omega}{k} = \frac{120\pi \times 3}{2\pi} = 180\text{ m/s}
  3. T=μv2=4×10−2×32400=1296 NT = \mu v^2 = 4\times10^{-2} \times 32400 = 1296\text{ N}
  4. So the answer is (a) 1296 N.
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Q118MHT CET 2024 · 15 MAY · SHIFT 2Easy

Progressive Wave Equation · Reading the wave equation

A wave is given by Y=3sin⁡2π(t0.04−x0.01)Y = 3\sin 2\pi\left(\frac{t}{0.04} - \frac{x}{0.01}\right) where Y is in cm. Frequency of the wave and maximum acceleration will be (π2=10)(\pi^2 = 10)

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Answer: (d)

  1. Compare with Y=Asin⁡2π(tT−xλ)Y = A\sin 2\pi\left(\dfrac{t}{T} - \dfrac{x}{\lambda}\right): T=0.04 sT = 0.04\text{ s}, f=25 Hzf = 25\text{ Hz}, A=3 cmA = 3\text{ cm}.
  2. ω=2πf=50π rad/s\omega = 2\pi f = 50\pi\text{ rad/s}
  3. amax=ω2A=2500π2×3=2500×10×3=7.5×104 cm/s2a_{max} = \omega^2 A = 2500\pi^2 \times 3 = 2500 \times 10 \times 3 = 7.5 \times 10^{4}\text{ cm/s}^2
  4. So the answer is (d) 25 Hz25\text{ Hz}, 7.5×104 cm/s27.5 \times 10^{4}\text{ cm/s}^2.
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Q119NEET 2024Easy

Progressive Wave Equation · Reading the wave equation

The displacement of a travelling wave y=Csin⁡2πλ(at−x)y = C\sin\frac{2\pi}{\lambda}(at - x) where tt is time, xx is distance and λ\lambda is the wavelength, all in S.I. units. Then the frequency of the wave is

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Answer: (d)

  1. y=Csin⁡(2πaλt−2πλx)y = C\sin\left(\dfrac{2\pi a}{\lambda}t - \dfrac{2\pi}{\lambda}x\right), so ω=2πaλ\omega = \dfrac{2\pi a}{\lambda}.
  2. f=ω2π=aλf = \dfrac{\omega}{2\pi} = \dfrac{a}{\lambda}
  3. So the answer is (d) aλ\dfrac{a}{\lambda}.
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Q120JEE Main 2024 · 8 APR · SHIFT 2Easy

Progressive Wave Equation · Reading the wave equation

A plane progressive wave is given by y=2cos⁡2π(330t−x)my = 2\cos 2\pi(330t - x)\text{m}. The frequency of the wave is:

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Answer: (c)

  1. y=2cos⁡(2π⋅330 t−2πx)y = 2\cos(2\pi \cdot 330\, t - 2\pi x), so ω=2π×330\omega = 2\pi \times 330.
  2. f=ω2π=330 Hzf = \dfrac{\omega}{2\pi} = 330\text{ Hz}
  3. So the answer is (c) 330 Hz330\text{ Hz}.
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Q121MHT CET 2024 · 3 MAY · SHIFT 1Easy

Progressive Wave Equation · Writing the wave equation and its direction

The displacement of a wave is given by y=0.002sin⁡(100t+x)y = 0.002\sin(100t + x) where ' xx 'and ' yy ' are in metre and ' tt ' is in second. This represents a wave

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Answer: (b)

  1. ω=100 rad/s\omega = 100\text{ rad/s}, k=1 m−1k = 1\text{ m}^{-1}
  2. λ=2π m\lambda = 2\pi\text{ m} (not 1 m); f=1002π=50π Hzf = \dfrac{100}{2\pi} = \dfrac{50}{\pi}\text{ Hz} (not 100π\dfrac{100}{\pi})
  3. v=ωk=100 m/sv = \dfrac{\omega}{k} = 100\text{ m/s}, and (ωt+kx)(\omega t + kx) means motion along −x-x.
  4. So the answer is (b) 100 m/s100\text{ m/s} in the negative xx-direction.
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Q122MHT CET 2024 · 15 MAY · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

Velocity of sound waves in air is 330 m/s330\text{ m/s}. For a particular sound wave in air, path difference of 40 cm is equivalent to phase difference of 1.6π1.6\pi. frequency of this wave is

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Answer: (c)

  1. Δϕ=2πλΔx⇒1.6π=2π×0.4λ\Delta\phi = \frac{2\pi}{\lambda}\Delta x \Rightarrow 1.6\pi = \frac{2\pi \times 0.4}{\lambda}
  2. λ=0.81.6=0.5\lambda = \frac{0.8}{1.6} = 0.5 m
  3. f=vλ=3300.5=660f = \frac{v}{\lambda} = \frac{330}{0.5} = 660 Hz
  4. So the answer is (c) 660 Hz.
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Q123MHT CET 2024 · 9 MAY · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

The diagram shows the propagation of a progressive wave. A, B, C, D, E are five points on this wave

Figure

Which of the following points are in the same state of vibration?

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Answer: (d)

  1. Points in the same state of vibration have the same displacement and the same direction of motion (phase difference 2πn2\pi n).
  2. B and E both have the same positive displacement and both lie on the falling side of a crest.
  3. B and E are two full wavelengths apart, so they are in phase.
  4. So the answer is (d) E, B.
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Q124MHT CET 2024 · 4 MAY · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

A transverse wave travelling along a stretched string has a speed of 30 m/s30\text{ m/s} and a frequency of 250 Hz. The phase difference between two points on the string 10 cm apart at the same instant is

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Answer: (c)

  1. λ=vf=30250=0.12\lambda = \frac{v}{f} = \frac{30}{250} = 0.12 m
  2. Δϕ=2πλΔx=2π×0.100.12=5π3\Delta\phi = \frac{2\pi}{\lambda}\Delta x = \frac{2\pi \times 0.10}{0.12} = \frac{5\pi}{3} rad
  3. So the answer is (c) (5π3)c\left(\frac{5\pi}{3}\right)^c.
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Q125MHT CET 2024 · 4 MAY · SHIFT 1Easy

Progressive Wave Equation · Phase difference and path difference

The distance between two consecutive points with phase difference of 60∘60^\circ in wave of frequency 500 Hz is 0.6 m. The velocity with which wave is travelling is

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Answer: (a)

  1. 60∘60^\circ phase difference means Δx=λ6\Delta x = \frac{\lambda}{6}, so λ=6×0.6=3.6\lambda = 6 \times 0.6 = 3.6 m.
  2. v=fλ=500×3.6=1800v = f\lambda = 500 \times 3.6 = 1800 m/s
  3. So the answer is (a) 1.81.8 km/s.
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Q126MHT CET 2024 · 4 MAY · SHIFT 1Easy

Progressive Wave Equation · Phase difference and path difference

A progressive wave of frequency 400 Hz is travelling with a velocity 336 m/s336\text{ m/s}. How far apart are the two points which are 60∘60^\circ out of phase?

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Answer: (a)

  1. λ=vf=336400=0.84\lambda = \frac{v}{f} = \frac{336}{400} = 0.84 m
  2. Δx=λ6=0.14\Delta x = \frac{\lambda}{6} = 0.14 m for 60∘60^\circ
  3. So the answer is (a) 0.14 m.
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Q127MHT CET 2024 · 3 MAY · SHIFT 1Easy

Progressive Wave Equation · Phase difference and path difference

The path difference between two waves Y1=a1sin⁡(ωt−2πxλ)Y_1 = a_1\sin\left(\omega t - \frac{2\pi x}{\lambda}\right) and Y2=a2cos⁡(ωt−2πxλ+ϕ)Y_2 = a_2\cos\left(\omega t - \frac{2\pi x}{\lambda} + \phi\right) is

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Answer: (b)

  1. Y2=a2cos⁡(θ+ϕ)=a2sin⁡(θ+ϕ+π2)Y_2 = a_2\cos(\theta + \phi) = a_2\sin\left(\theta + \phi + \frac{\pi}{2}\right) with θ=ωt−2πxλ\theta = \omega t - \frac{2\pi x}{\lambda}.
  2. Phase difference =ϕ+π2= \phi + \frac{\pi}{2}
  3. Path difference =λ2π(ϕ+π2)= \frac{\lambda}{2\pi}\left(\phi + \frac{\pi}{2}\right)
  4. So the answer is (b).
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Q128MHT CET 2024 · 2 MAY · SHIFT 1Easy

Progressive Wave Equation · Phase difference and path difference

Two simple harmonic progressive waves have displacements y1=a1sin⁡(2πxλ−ωt)y_1 = a_1\sin\left(\frac{2\pi x}{\lambda} - \omega t\right) and y2=a2cos⁡(2πxλ−ωt+ϕ)y_2 = a_2\cos\left(\frac{2\pi x}{\lambda} - \omega t + \phi\right) What is the phase difference between two waves?

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Answer: (a)

  1. Let θ=2πxλ−ωt\theta = \frac{2\pi x}{\lambda} - \omega t; then y1=a1sin⁡θy_1 = a_1\sin\theta.
  2. y2=a2cos⁡(θ+ϕ)=a2sin⁡(θ+ϕ+π2)y_2 = a_2\cos(\theta + \phi) = a_2\sin\left(\theta + \phi + \frac{\pi}{2}\right)
  3. Phase difference =ϕ+π2= \phi + \frac{\pi}{2}
  4. So the answer is (a).
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Q129MHT CET 2024 · 2 MAY · SHIFT 1Easy

Progressive Wave Equation · Phase difference and path difference

Velocity of sound waves in air is 330 m/s330\text{ m/s}. For a particular sound wave in air, path difference of 40 cm is equivalent to phase difference of 1.6π1.6\pi. The frequency of this wave is

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Answer: (c)

  1. Δϕ=2πλΔx⇒1.6π=2π×0.4λ\Delta\phi = \frac{2\pi}{\lambda}\Delta x \Rightarrow 1.6\pi = \frac{2\pi \times 0.4}{\lambda}, so λ=0.5\lambda = 0.5 m.
  2. f=vλ=3300.5=660f = \frac{v}{\lambda} = \frac{330}{0.5} = 660 Hz
  3. So the answer is (c) 660 Hz.
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Q130MHT CET 2024 · 15 MAY · SHIFT 2Medium

Progressive Wave Equation · Tension from the wave equation

A string has mass per unit length of 10−6 kg/cm10^{-6}\text{ kg/cm} The equation of simple harmonic wave produced in it is Y=0.2sin⁡(2x+80t) mY = 0.2\sin(2x + 80t)\text{ m}. The tension in the string is

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Answer: (a)

  1. μ=10−6 kg/cm=10−4 kg/m\mu = 10^{-6}\text{ kg/cm} = 10^{-4}\text{ kg/m}
  2. v=ωk=802=40 m/sv = \frac{\omega}{k} = \frac{80}{2} = 40\text{ m/s}
  3. T=μv2=10−4×1600=0.16 NT = \mu v^2 = 10^{-4} \times 1600 = 0.16\text{ N}
  4. So the answer is (a) 0.16 N.
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Q131MHT CET 2023 · 12 MAY · SHIFT 2Easy

Progressive Wave Equation · Reading the wave equation

The equation of wave motion is Y=5sin⁡(10πt−0.02πx+π/3)Y = 5\sin(10\pi t - 0.02\pi x + \pi/3) where xx is in metre and tt in second. The velocity of the wave is

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Answer: (c)

  1. ω=10π\omega = 10\pi, k=0.02πk = 0.02\pi
  2. v=ωk=10π0.02π=500 m/sv = \dfrac{\omega}{k} = \dfrac{10\pi}{0.02\pi} = 500\text{ m/s}
  3. So the answer is (c) 500 m/s500\text{ m/s}.
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Q132MHT CET 2023 · 10 MAY · SHIFT 2Easy

Progressive Wave Equation · Reading the wave equation

The equation of wave is Y=6sin⁡(12πt−0.02πx+π3)Y = 6\sin\left(12\pi t - 0.02\pi x + \frac{\pi}{3}\right) where 'xx' is in m\text{m} and 'tt' in s\text{s}. The velocity of the wave is

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Answer: (d)

  1. ω=12π\omega = 12\pi, k=0.02πk = 0.02\pi
  2. v=ωk=12π0.02π=600 m/sv = \dfrac{\omega}{k} = \dfrac{12\pi}{0.02\pi} = 600\text{ m/s}
  3. So the answer is (d) 600 m/s600\text{ m/s}.
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Q133JEE Main 2023 · 24 JAN · SHIFT 1Easy

Progressive Wave Equation · Reading the wave equation

A travelling wave is described by the equation

y(x,t)=[0.05sin⁡(8x−4t)]y(x, t) = [0.05\sin(8x - 4t)] m

The velocity of the wave is: [all the quantities are in SI unit]

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Answer: (d)

  1. k=8 m−1k = 8\text{ m}^{-1}, ω=4 rad/s\omega = 4\text{ rad/s}
  2. v=ωk=48=0.5 m/sv = \dfrac{\omega}{k} = \dfrac{4}{8} = 0.5\text{ m/s}
  3. So the answer is (d) 0.5 m s−10.5\text{ m s}^{-1}.
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Q134JEE Main 2023 · 11 APR · SHIFT 1Easy

Progressive Wave Equation · Reading the wave equation

The equation of wave is given by

Y=10−2sin⁡2π(160t−0.5x+π/4)Y = 10^{-2}\sin 2\pi(160t - 0.5x + \pi/4)

where xx and YY are in m\text{m} and tt in s\text{s}. The speed of the wave is ________ km h−1\text{km h}^{-1}.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 1152

  1. Y=10−2sin⁡(2π⋅160 t−2π⋅0.5 x+… )Y = 10^{-2}\sin(2\pi \cdot 160\, t - 2\pi \cdot 0.5\, x + \dots): ω=320π\omega = 320\pi, k=πk = \pi.
  2. v=ωk=320 m/sv = \dfrac{\omega}{k} = 320\text{ m/s}
  3. 320×185=1152 km/h320 \times \dfrac{18}{5} = 1152\text{ km/h}
  4. So the answer is 1152 km h−11152\text{ km h}^{-1}.
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Q135JEE Main 2023 · 10 APR · SHIFT 1Easy

Progressive Wave Equation · Reading the wave equation

A transverse harmonic wave on a string is given by

y(x,t)=5sin⁡(6t+0.003x)y(x, t) = 5\sin(6t + 0.003x)

where x and y are in cm and t in sec. The wave velocity is _______________ ms−1-1.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 20

  1. ω=6 rad/s\omega = 6\text{ rad/s}, k=0.003 cm−1k = 0.003\text{ cm}^{-1}
  2. v=ωk=60.003=2000 cm/sv = \dfrac{\omega}{k} = \dfrac{6}{0.003} = 2000\text{ cm/s}
  3. So the answer is 20 m s−120\text{ m s}^{-1}.
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Q136MHT CET 2023 · 13 MAY · SHIFT 2Easy

Progressive Wave Equation · Particle velocity and wave velocity

The equation of a progressive wave is Y=asin⁡2π(nt−x5)Y = a\sin 2\pi\left(nt - \frac{x}{5}\right). The ratio of maximum particle velocity to wave velocity is

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Answer: (b)

  1. Y=asin⁡(2πnt−2π5x)Y = a\sin\left(2\pi n t - \frac{2\pi}{5}x\right), so k=2π5k = \frac{2\pi}{5}.
  2. vmaxv=aωω/k=ak=2πa5\frac{v_{max}}{v} = \frac{a\omega}{\omega/k} = ak = \frac{2\pi a}{5}
  3. So the answer is (b) 2πa5\frac{2\pi a}{5}.
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Q137MHT CET 2023 · 14 MAY · SHIFT 1Easy

Progressive Wave Equation · Phase difference and path difference

A progressive wave is given by, Y=12sin⁡(5t−4x)Y = 12\sin(5t - 4x). On this wave, how far away are the two points having a phase difference of 90∘90^\circ?

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Answer: (b)

  1. From Y=12sin⁡(5t−4x)Y = 12\sin(5t - 4x): k=4k = 4.
  2. 90∘=π290^\circ = \frac{\pi}{2}, so Δx=Δϕk=π/24=π8\Delta x = \frac{\Delta\phi}{k} = \frac{\pi/2}{4} = \frac{\pi}{8}
  3. So the answer is (b) π8\frac{\pi}{8}.
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Q138MHT CET 2023 · 12 MAY · SHIFT 1Easy

Progressive Wave Equation · Phase difference and path difference

The displacement of two sinusoidal waves is given by the equation

y1=8sin⁡(20x−30t)y2=8sin⁡(25x−40t)\begin{matrix} y_1 = 8\sin(20x - 30t) \\ y_2 = 8\sin(25x - 40t) \end{matrix}

then the phase difference between the waves after time t=2 st = 2\text{ s} and distance x=5 cmx = 5\text{ cm} will be

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Answer: (d)

  1. Phases: ϕ1=20x−30t\phi_1 = 20x - 30t, ϕ2=25x−40t\phi_2 = 25x - 40t.
  2. Δϕ=ϕ2−ϕ1=5x−10t\Delta\phi = \phi_2 - \phi_1 = 5x - 10t (magnitude taken).
  3. With x=5x = 5 and t=2t = 2: Δϕ=25−20=5\Delta\phi = 25 - 20 = 5 rad
  4. So the answer is (d) 5 radian.
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Q139MHT CET 2023 · 11 MAY · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

The path difference between two waves, represented by y1=a1sin⁡(ωt−2πxλ)y_1 = a_1\sin\left(\omega t - \frac{2\pi x}{\lambda}\right) and y2=a2cos⁡(ωt−2πxλ+ϕ)y_2 = a_2\cos\left(\omega t - \frac{2\pi x}{\lambda} + \phi\right) is

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Answer: (b)

  1. y2=a2cos⁡(θ+ϕ)=a2sin⁡(θ+ϕ+π2)y_2 = a_2\cos(\theta + \phi) = a_2\sin\left(\theta + \phi + \frac{\pi}{2}\right) with θ=ωt−2πxλ\theta = \omega t - \frac{2\pi x}{\lambda}.
  2. Phase difference =ϕ+π2= \phi + \frac{\pi}{2}
  3. Path difference =λ2π(ϕ+π2)= \frac{\lambda}{2\pi}\left(\phi + \frac{\pi}{2}\right)
  4. So the answer is (b).
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Q140JEE Main 2023 · 25 JAN · SHIFT 1Easy

Progressive Wave Equation · Phase difference and path difference

The distance between two consecutive points with phase difference of 60∘^\circ in a wave of frequency 500 Hz is 6.0 m. The velocity with which wave is travelling is __________ km/s

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 18

  1. Δx=λ2πΔϕ\Delta x = \frac{\lambda}{2\pi}\Delta\phi with Δϕ=π3\Delta\phi = \frac{\pi}{3} gives Δx=λ6\Delta x = \frac{\lambda}{6}
  2. λ6=6.0 m⇒λ=36 m\frac{\lambda}{6} = 6.0\text{ m} \Rightarrow \lambda = 36\text{ m}
  3. v=fλ=500×36=18000 m/sv = f\lambda = 500 \times 36 = 18000\text{ m/s}
  4. So v=18 km/sv = 18\text{ km/s}.
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Q141MHT CET 2023 · 11 MAY · SHIFT 1Medium

Progressive Wave Equation · Reading the wave equation

A transverse wave Y=2sin⁡(0.01x+30t)Y = 2\sin(0.01x + 30t) moves on a stretched string from one end to another end in 0.5 second. If xx and yy are in cm\text{cm} and tt in second, then the length of the string is

Show answer and solution

Answer: (c)

  1. Wave speed v=ωk=300.01=3000 cm/s=30 m/sv = \frac{\omega}{k} = \frac{30}{0.01} = 3000\text{ cm/s} = 30\text{ m/s}
  2. Length L=vt=30×0.5=15 mL = v t = 30 \times 0.5 = 15\text{ m}
  3. So the answer is (c) 15 m.
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Q142MHT CET 2023 · 11 MAY · SHIFT 2Medium

Progressive Wave Equation · Particle velocity and wave velocity

A transverse wave in a medium is given by y=Asin⁡2(ωt−kx)y = A\sin 2(\omega t - kx). It is found that the magnitude of the maximum velocity of particles in the medium is equal to that of the wave velocity. What is the value of AA?

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Answer: (d)

  1. y=Asin⁡(2ωt−2kx)y = A\sin(2\omega t - 2kx): maximum particle velocity =2ωA= 2\omega A
  2. Wave velocity =2ω2k=ωk= \frac{2\omega}{2k} = \frac{\omega}{k}
  3. 2ωA=ωk⇒A=12k2\omega A = \frac{\omega}{k} \Rightarrow A = \frac{1}{2k}; with k=2πλk = \frac{2\pi}{\lambda}, A=λ4πA = \frac{\lambda}{4\pi}
  4. So the answer is (d) λ4π\frac{\lambda}{4\pi}.
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Q143MHT CET 2023 · 9 MAY · SHIFT 2Medium

Progressive Wave Equation · Particle velocity and wave velocity

The equation of simple harmonic progressive wave is given by y=asin⁡2π(bt−cx)y = a\sin 2\pi(bt - cx). The maximum particle velocity will be half the wave velocity, if c=c =

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Answer: (b)

  1. y=asin⁡(2πbt−2πcx)y = a\sin(2\pi b t - 2\pi c x): vp,max⁡=2πbav_{p,\max} = 2\pi b a, wave velocity v=2πb2πc=bcv = \frac{2\pi b}{2\pi c} = \frac{b}{c}
  2. 2πba=12⋅bc⇒c=14πa2\pi b a = \frac{1}{2}\cdot\frac{b}{c} \Rightarrow c = \frac{1}{4\pi a}
  3. So the answer is (b) 14πa\frac{1}{4\pi a}.
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Q144MHT CET 2023 · 14 MAY · SHIFT 1Medium

Progressive Wave Equation · Phase difference and path difference

The equation of the wave is Y=10sin⁡(2πt30+α)Y = 10\sin\left(\frac{2\pi t}{30} + \alpha\right) If the displacement is 5 cm5\text{ cm} at t=0t = 0 then the total phase at t=7.5 st = 7.5\text{ s} will be (sin⁡30∘=0.5)(\sin 30^\circ = 0.5)

Show answer and solution

Answer: (d)

  1. At t=0t = 0: 10sin⁡α=5⇒α=π610\sin\alpha = 5 \Rightarrow \alpha = \frac{\pi}{6}
  2. Phase at t=7.5 st = 7.5\text{ s}: 2π(7.5)30+π6=π2+π6\frac{2\pi(7.5)}{30} + \frac{\pi}{6} = \frac{\pi}{2} + \frac{\pi}{6}
  3. =2π3 rad= \frac{2\pi}{3}\text{ rad}
  4. So the answer is (d) 2π3 rad\frac{2\pi}{3}\text{ rad}.
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Q145JEE Main 2022 · 28 JUL · SHIFT 1Easy

Progressive Wave Equation · Reading the wave equation

In the wave equation

y=0.5sin⁡2πλ(400t−x) my = 0.5\sin\frac{2\pi}{\lambda}(400t - x)\text{ m}

the velocity of the wave will be:

Show answer and solution

Answer: (c)

  1. Compare with y=Asin⁡2πλ(vt−x)y = A\sin\dfrac{2\pi}{\lambda}(vt - x).
  2. So v=400 m/sv = 400\text{ m/s}.
  3. So the answer is (c) 400 m/s400\text{ m/s}.
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Q146JEE Main 2022 · 30 JUN · SHIFT 1Easy

Progressive Wave Equation · Writing the wave equation and its direction

Which of the following equations correctly represents a travelling wave having wavelength λ\lambda = 4.0 cm, frequency ν\nu = 100 Hz and travelling in positive x-axis direction?

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Answer: (d)

  1. k=2πλ=2π4=0.5π cm−1k = \dfrac{2\pi}{\lambda} = \dfrac{2\pi}{4} = 0.5\pi\text{ cm}^{-1}
  2. ω=2πν=200π s−1\omega = 2\pi\nu = 200\pi\text{ s}^{-1}
  3. y=Asin⁡(0.5πx−200πt)=Asin⁡π[(0.5)x−(200)t]y = A\sin(0.5\pi x - 200\pi t) = A\sin\pi[(0.5)x - (200)t]
  4. So the answer is (d).
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Q147JEE Main 2022 · 26 JUL · SHIFT 2Medium

Progressive Wave Equation · Particle velocity and wave velocity

A transverse wave is represented by y=2sin⁡(ωt−kx) cmy = 2\sin(\omega t - kx)\text{ cm}. The value of wavelength (in cm\text{cm}) for which the wave velocity becomes equal to the maximum particle velocity, will be:

Show answer and solution

Answer: (a)

  1. Wave velocity ωk=ωλ2π\frac{\omega}{k} = \frac{\omega\lambda}{2\pi}; maximum particle velocity =Aω= A\omega
  2. Equal when λ=2πA=2π(2)=4π cm\lambda = 2\pi A = 2\pi(2) = 4\pi\text{ cm}
  3. So the answer is (a) 4π4\pi.
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Q148JEE Main 2022 · 29 JUN · SHIFT 1Medium

Progressive Wave Equation · Particle velocity and wave velocity

A longitudinal wave is represented by x=10sin⁡2π(nt−xλ)x = 10\sin 2\pi\left(nt - \frac{x}{\lambda}\right) cm. The maximum particle velocity will be four times the wave velocity if the determined value of wavelength is equal to:

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Answer: (b)

  1. Wave velocity v=nλv = n\lambda; maximum particle velocity =2πn(10) cm/s= 2\pi n (10)\text{ cm/s}
  2. 20πn=4nλ⇒λ=5π cm20\pi n = 4 n\lambda \Rightarrow \lambda = 5\pi\text{ cm}
  3. So the answer is (b) 5π5\pi.
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Q149MHT CET 2021 · 21 SEP · SHIFT 2Easy

Progressive Wave Equation · Reading the wave equation

Equation of two simple harmonic waves are given by Y1=2sin⁡8π(t0.2−x2)mY_1 = 2\sin 8\pi\left(\frac{t}{0.2} - \frac{x}{2}\right)\text{m} and Y2=4sin⁡8π(t0.16−x1.6)mY_2 = 4\sin 8\pi\left(\frac{t}{0.16} - \frac{x}{1.6}\right)\text{m} then both waves have

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Answer: (d)

  1. Y1Y_1: ω1=8π0.2=40π\omega_1 = \dfrac{8\pi}{0.2} = 40\pi, k1=8π2=4πk_1 = \dfrac{8\pi}{2} = 4\pi, so v1=10 m/sv_1 = 10\text{ m/s}.
  2. Y2Y_2: ω2=8π0.16=50π\omega_2 = \dfrac{8\pi}{0.16} = 50\pi, k2=8π1.6=5πk_2 = \dfrac{8\pi}{1.6} = 5\pi, so v2=10 m/sv_2 = 10\text{ m/s}.
  3. Periods, frequencies and wavelengths differ; speeds are equal.
  4. So the answer is (d) same velocity.
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Q150JEE Main 2021 · 24 FEB · SHIFT 2Easy

Progressive Wave Equation · Writing the wave equation and its direction

Which of the following equations represents a travelling wave?

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Answer: (c)

  1. A travelling wave has the form f(kx±ωt)f(kx \pm \omega t), a single function of a combination of xx and tt.
  2. Asin⁡(15x−2t)A\sin(15x - 2t) has this form, moving along +x+x with v=215v = \dfrac{2}{15}.
  3. Asin⁡xcos⁡ωtA\sin x\cos\omega t is a stationary wave; the others do not depend on xx and tt only through (x±vt)(x \pm vt).
  4. So the answer is (c) y=Asin⁡(15x−2t)y = A\sin(15x - 2t).
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Q151MHT CET 2021 · 24 SEP · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

Velocity of sound waves in air is 'VV' m/s\text{m/s}. For a particular sound wave in air, path difference of 'x' cm\text{cm} is equivalent to phase difference nπn\pi. The frequency of this wave is

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Answer: (c)

  1. Δϕ=2πλΔx⇒nπ=2πxλ\Delta\phi = \frac{2\pi}{\lambda}\Delta x \Rightarrow n\pi = \frac{2\pi x}{\lambda}
  2. λ=2xn\lambda = \frac{2x}{n}
  3. f=Vλ=Vn2xf = \frac{V}{\lambda} = \frac{Vn}{2x}
  4. So the answer is (c) Vn2x\frac{Vn}{2x}.
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Q152MHT CET 2021 · 23 SEP · SHIFT 1Easy

Progressive Wave Equation · Phase difference and path difference

Two waves are represented by the equation, y1=Asin⁡(ωt+kx+0.57)my_1 = A\sin(\omega t + kx + 0.57)\text{m} and y2=Acos⁡(ωt+kx)my_2 = A\cos(\omega t + kx)\text{m}, where xx is in metre and tt is in second. What is the phase difference between them?

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Answer: (b)

  1. y2=Acos⁡(ωt+kx)=Asin⁡(ωt+kx+1.57)y_2 = A\cos(\omega t + kx) = A\sin(\omega t + kx + 1.57) since π2≈1.57\frac{\pi}{2} \approx 1.57.
  2. Δϕ=1.57−0.57=1.0\Delta\phi = 1.57 - 0.57 = 1.0 rad
  3. So the answer is (b) 1.0 radian.
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Q153MHT CET 2021 · 22 SEP · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

A sound wave of frequency 160 Hz160\text{ Hz} has a velocity of 320 m/s320\text{ m/s}. When it travels through air, the particles having a phase difference of 90∘90^\circ, are separated by a distance of

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Answer: (a)

  1. λ=vf=320160=2\lambda = \frac{v}{f} = \frac{320}{160} = 2 m
  2. 90∘90^\circ phase difference means Δx=λ4=0.5\Delta x = \frac{\lambda}{4} = 0.5 m
  3. So the answer is (a) 50 cm.
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Q154MHT CET 2021 · 22 SEP · SHIFT 1Easy

Progressive Wave Equation · Phase difference and path difference

A sound wave is travelling with a frequency of 50 Hz50\text{ Hz}. The phase difference between the two points in the path of a wave is π3\frac{\pi}{3}. The distance between those two points is (Velocity of sound in air =330 m/s= 330\text{ m/s})

Show answer and solution

Answer: (a)

  1. λ=vf=33050=6.6\lambda = \frac{v}{f} = \frac{330}{50} = 6.6 m
  2. Δϕ=π3\Delta\phi = \frac{\pi}{3} means Δx=λ6=6.66=1.1\Delta x = \frac{\lambda}{6} = \frac{6.6}{6} = 1.1 m
  3. So the answer is (a) 1.1 m.
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Q155MHT CET 2021 · 21 SEP · SHIFT 1Easy

Progressive Wave Equation · Phase difference and path difference

A progressive wave of frequency 50 Hz is travelling with velocity 350 m/s through a medium. The change in phase at a given time interval of 0.01 second is

Figure

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Answer: (c)

  1. At a fixed point, phase changes with time as Δϕ=2πf Δt\Delta\phi = 2\pi f\,\Delta t.
  2. Δϕ=2π×50×0.01=π\Delta\phi = 2\pi \times 50 \times 0.01 = \pi rad
  3. So the answer is (c) π\pi rad.
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Q156MHT CET 2021 · 22 SEP · SHIFT 1Medium

Progressive Wave Equation · Reading the wave equation

A transverse wave given by y=2sin⁡(0.01x+30t)y = 2\sin(0.01x + 30t) moves on a stretched string from one end to another end in 0.5 second. If 'xx' and 'yy' are in cm\text{cm} and 'tt' is in second, then the length of the string is

Show answer and solution

Answer: (d)

  1. Wave speed v=ωk=300.01=3000 cm/s=30 m/sv = \frac{\omega}{k} = \frac{30}{0.01} = 3000\text{ cm/s} = 30\text{ m/s}
  2. Length L=vt=30×0.5=15 mL = v t = 30 \times 0.5 = 15\text{ m}
  3. So the answer is (d) 15 m.
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Q157JEE Main 2021 · 17 MAR · SHIFT 2Medium

Progressive Wave Equation · Writing the wave equation and its direction

A sound wave of frequency 245 Hz travels with the speed of 300 ms−1{}^{-1} along the positive x-axis. Each point of the wave moves to and fro through a total distance of 6 cm. What will be the mathematical expression of this travelling wave?

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Answer: (b)

  1. Total to-and-fro distance =2A=6 cm⇒A=0.03 m= 2A = 6\text{ cm} \Rightarrow A = 0.03\text{ m}
  2. ω=2πf=2π(245)≈1.5×103 rad/s\omega = 2\pi f = 2\pi(245) \approx 1.5 \times 10^3\text{ rad/s}
  3. k=ωv=1539300≈5.1 m−1k = \frac{\omega}{v} = \frac{1539}{300} \approx 5.1\text{ m}^{-1}
  4. So the answer is (b) Y=0.03sin⁡[5.1x−(1.5×103)t]Y = 0.03\sin[5.1x - (1.5\times10^3)t].
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Q158MHT CET 2021 · 21 SEP · SHIFT 1Medium

Progressive Wave Equation · Particle velocity and wave velocity

A simple harmonic progressive wave is given by Y=Y0sin⁡2π(nt−xλ)Y = Y_0\sin 2\pi\left(nt - \frac{x}{\lambda}\right). If the wave velocity is (18)\left(\frac{1}{8}\right)th the maximum particle velocity then the wavelength is

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Answer: (b)

  1. Wave velocity v=nλv = n\lambda; maximum particle velocity =2πnY0= 2\pi n Y_0
  2. nλ=18(2πnY0)⇒λ=πY04n\lambda = \frac{1}{8}(2\pi n Y_0) \Rightarrow \lambda = \frac{\pi Y_0}{4}
  3. So the answer is (b) πY04\frac{\pi Y_0}{4}.
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Q159MHT CET 2021 · 20 SEP · SHIFT 1Medium

Progressive Wave Equation · Phase difference and path difference

The equation of wave is given by y=10sin⁡(2πt30+α)y = 10\sin\left(\frac{2\pi t}{30} + \alpha\right). If the displacement is 5 cm5\text{ cm} at t=0t = 0, then the total phase at t=7.5 st = 7.5\text{ s} will be

[sin⁡30∘=cos⁡60∘=12,cos⁡30∘=sin⁡60∘=32]\left[\sin 30^\circ = \cos 60^\circ = \frac{1}{2}, \cos 30^\circ = \sin 60^\circ = \frac{\sqrt{3}}{2}\right]

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Answer: (d)

  1. At t=0t = 0: 10sin⁡α=5⇒sin⁡α=12, α=π610\sin\alpha = 5 \Rightarrow \sin\alpha = \frac{1}{2},\ \alpha = \frac{\pi}{6}
  2. Phase at t=7.5 st = 7.5\text{ s}: 2π(7.5)30+π6=π2+π6\frac{2\pi(7.5)}{30} + \frac{\pi}{6} = \frac{\pi}{2} + \frac{\pi}{6}
  3. =2π3 rad= \frac{2\pi}{3}\text{ rad}
  4. So the answer is (d) 2π3 rad\frac{2\pi}{3}\text{ rad}.
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Q160MHT CET 2021 · 21 SEP · SHIFT 2Medium

Progressive Wave Equation · Tension from the wave equation

The equation of simple harmonic wave produced in the string under tension 0.4 N0.4\text{ N} is given by y=4sin⁡(3x+60t) my = 4\sin(3x + 60t)\text{ m}. The mass per unit length of the string is

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Answer: (a)

  1. v=ωk=603=20 m/sv = \frac{\omega}{k} = \frac{60}{3} = 20\text{ m/s}
  2. μ=Tv2=0.4400=10−3 kg m−1\mu = \frac{T}{v^2} = \frac{0.4}{400} = 10^{-3}\text{ kg m}^{-1}
  3. So the answer is (a) 10−3 kg m−110^{-3}\text{ kg m}^{-1}.
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Q161JEE Main 2021 · 26 FEB · SHIFT 1Medium

Progressive Wave Equation · Tension from the wave equation

The mass per unit length of a uniform wire is 0.135 g/cm. A transverse wave of the form y = −- 0.21 sin (x + 30t) is produced in it, where x is in meter and t is in second. Then, the expected value of tension in the wire is x ×\times 10−-2 N. Value of x is _________. (Round off to the nearest integer)

Numerical answer type. Work it out, then open the answer.

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Answer: 1215

  1. μ=0.135 g/cm=0.0135 kg/m\mu = 0.135\text{ g/cm} = 0.0135\text{ kg/m}
  2. v=ωk=301=30 m/sv = \frac{\omega}{k} = \frac{30}{1} = 30\text{ m/s}
  3. T=μv2=0.0135×900=12.15 N=1215×10−2 NT = \mu v^2 = 0.0135 \times 900 = 12.15\text{ N} = 1215 \times 10^{-2}\text{ N}
  4. So x=1215x = 1215.
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Q162JEE Main 2021 · 20 JUL · SHIFT 1Difficult

Progressive Wave Equation · Writing the wave equation and its direction

The amplitude of wave disturbance propagating in the positive x-direction is given by y=11+x2y = \frac{1}{1 + x^2} at time t = 0 and y=11+(x−2)2y = \frac{1}{1 + (x - 2)^2} at t = 1 s, where x and y are in metres. The shape of wave does not change during the propagation. The velocity of the wave will be ___________ m/s.

Numerical answer type. Work it out, then open the answer.

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Answer: 2

  1. The peak (y=1y = 1) is at x=0x = 0 at t=0t = 0 and at x=2 mx = 2\text{ m} at t=1 st = 1\text{ s}.
  2. Shape is unchanged, so the pulse moves 2 m2\text{ m} in 1 s1\text{ s}.
  3. v=2 m/sv = 2\text{ m/s}
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Q163JEE Main 2019 · 12 JAN · SHIFT 1Easy

Progressive Wave Equation · Reading the wave equation

A travelling harmonic wave is represented by the equation y(x,t) = 10–3sin (50t + 2x), where, x and y are in metre and t is in seconds. Which of the following is a correct statement about the wave?

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Answer: (c)

  1. ω=50 rad/s\omega = 50\text{ rad/s}, k=2 m−1k = 2\text{ m}^{-1}, so v=ωk=25 m/sv = \dfrac{\omega}{k} = 25\text{ m/s}.
  2. Form (ωt+kx)(\omega t + kx) means the wave travels along −x-x.
  3. So the answer is (c) negative xx-axis with speed 25 m s−125\text{ m s}^{-1}.
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Q164MHT CET 2019 · 2 MAY · SHIFT 2Easy

Progressive Wave Equation · Phase difference and path difference

A simple harmonic progressive wave is represented as y=0.03sin⁡π(2t−0.01x)my = 0.03\sin\pi(2t - 0.01x)\text{m}. At a given instant of time, the phase difference between two particles 25 m apart is

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Answer: (c)

  1. y=0.03sin⁡(2πt−0.01πx)y = 0.03\sin(2\pi t - 0.01\pi x), so k=0.01π m−1k = 0.01\pi\ \text{m}^{-1}.
  2. Δϕ=k Δx=0.01π×25=π4\Delta\phi = k\,\Delta x = 0.01\pi \times 25 = \frac{\pi}{4} rad
  3. So the answer is (c) π4\frac{\pi}{4} rad.
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Q165MHT CET 2019 · 2 MAY · SHIFT 1Medium

Progressive Wave Equation · Particle velocity and wave velocity

The equation of simple harmonic progressive wave is given by Y=asin⁡2π(bt−cx)Y = a\sin 2\pi(bt - cx). The maximum particle velocity will be twice the wave velocity if

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Answer: (c)

  1. vp,max⁡=2πbav_{p,\max} = 2\pi b a, wave velocity v=bcv = \frac{b}{c}
  2. 2πba=2⋅bc⇒c=1πa2\pi b a = 2\cdot\frac{b}{c} \Rightarrow c = \frac{1}{\pi a}
  3. So the answer is (c) c=1πac = \frac{1}{\pi a}.
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Q166MHT CET 2019 · 2 MAY · SHIFT 1Medium

Progressive Wave Equation · Tension from the wave equation

A transverse wave is propagating on the string. The linear density of a vibrating string is 10−3 kg/m10^{-3}\text{ kg/m}. The equation of the wave is Y=0.05sin⁡(x+15t)Y = 0.05\sin(x + 15t) where xx and YY are measured in metre and time in second. The tension force in the string is

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Answer: (c)

  1. Wave speed v=ωk=151=15 m/sv = \frac{\omega}{k} = \frac{15}{1} = 15\text{ m/s}
  2. T=μv2=10−3×225=0.225 NT = \mu v^2 = 10^{-3} \times 225 = 0.225\text{ N}
  3. So the answer is (c) 0.225 N.
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Q167JEE Main 2019 · 11 JAN · SHIFT 1Medium

Progressive Wave Equation · Tension from the wave equation

Equation of travelling wave on a stretched string of linear density 5 g/m is y = 0.03 sin(450 t – 9x) where distance and time are measured in SI units. The tension in the string is:

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Answer: (d)

  1. v=ωk=4509=50 m/sv = \frac{\omega}{k} = \frac{450}{9} = 50\text{ m/s}
  2. μ=5 g/m=5×10−3 kg/m\mu = 5\text{ g/m} = 5\times10^{-3}\text{ kg/m}
  3. T=μv2=5×10−3×2500=12.5 NT = \mu v^2 = 5\times10^{-3} \times 2500 = 12.5\text{ N}
  4. So the answer is (d) 12.5 N.
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Q168JEE Main 2019 · 12 APR · SHIFT 1Difficult

Progressive Wave Equation · Writing the wave equation and its direction

A progressive wave travelling along the positive x-direction is represented by y(x,t) = Asin(kx – ω\omegat + ϕ\phi). Its snapshot at t = 0 is given in the figure.

Figure

For this wave, the phase ϕ\phi is:

Show answer and solution

Answer: (b)

  1. At t=0t = 0: y=Asin⁡(kx+ϕ)y = A\sin(kx + \phi).
  2. From the graph, y=0y = 0 at x=0x = 0 and yy becomes negative for small x>0x > 0, so y=−Asin⁡kxy = -A\sin kx.
  3. −Asin⁡kx=Asin⁡(kx+π)⇒ϕ=π-A\sin kx = A\sin(kx + \pi) \Rightarrow \phi = \pi
  4. So the answer is (b) π\pi.
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Q169JEE Main 2014 · 9 APR · SHIFT 1Medium

Progressive Wave Equation · Particle velocity and wave velocity

A transverse wave is represented by:

y = 10π\frac{10}{\pi} sin (2πTt−2πλx)\left(\frac{2\pi}{T}t - \frac{2\pi}{\lambda}x\right)

For what value of the wavelength the wave velocity is twice the maximum particle velocity?

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Answer: (a)

  1. Wave velocity v=λTv = \frac{\lambda}{T}; maximum particle velocity =10π⋅2πT=20T= \frac{10}{\pi}\cdot\frac{2\pi}{T} = \frac{20}{T}
  2. λT=2⋅20T⇒λ=40\frac{\lambda}{T} = 2\cdot\frac{20}{T} \Rightarrow \lambda = 40 (cm)
  3. So the answer is (a) 40 cm.
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Q170NEET 2013Easy

Progressive Wave Equation · Writing the wave equation and its direction

A wave travelling in the + ve x-direction having displacement along y-direction as 1 m, wavelength 2π\pi m and frequency of 1π\frac{1}{\pi} Hz is represented by

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Answer: (c)

  1. k=2π2π=1 m−1k = \dfrac{2\pi}{2\pi} = 1\text{ m}^{-1}, ω=2π×1π=2 rad/s\omega = 2\pi \times \dfrac{1}{\pi} = 2\text{ rad/s}
  2. Wave along +x+x, A=1 mA = 1\text{ m}: y=sin⁡(x−2t)y = \sin(x - 2t)
  3. So the answer is (c) y=sin⁡(x−2t)y = \sin(x - 2t).
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Q171NEET 2012 · AIPMT · MAINSEasy

Progressive Wave Equation · Particle velocity and wave velocity

The equation of a simple harmonic wave is given by

y = 3 sinπ2\frac{\pi}{2} (50t −- x),

where x and y are in metres and t is in seconds. The ratio of maximum particle velocity to the wave velocity is

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Answer: (b)

  1. y=3sin⁡(25πt−π2x)y = 3\sin\left(25\pi t - \frac{\pi}{2}x\right), so A=3A = 3 m, k=π2 m−1k = \frac{\pi}{2}\ \text{m}^{-1}.
  2. vmaxv=Ak=3×π2=3π2\frac{v_{max}}{v} = Ak = 3 \times \frac{\pi}{2} = \frac{3\pi}{2}
  3. So the answer is (b) 3π2\frac{3\pi}{2}.
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Q172JEE Main 2011 · AIEEEEasy

Progressive Wave Equation · Writing the wave equation and its direction

The transverse displacement y(x,t)y(x, t) of a wave on a string is given by y(x,t)=e−(ax2+bt2+2ab xt).y(x, t) = e^{-\left(ax^2 + bt^2 + 2\sqrt{ab}\,xt\right)}. This represents a:

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Answer: (a)

  1. The exponent is a perfect square: ax2+bt2+2ab xt=(a x+b t)2ax^2 + bt^2 + 2\sqrt{ab}\,xt = (\sqrt{a}\,x + \sqrt{b}\,t)^2.
  2. So y=f(a x+b t)=f(x+ba t)y = f(\sqrt{a}\,x + \sqrt{b}\,t) = f\left(x + \sqrt{\frac{b}{a}}\,t\right), a function of (x+vt)(x + vt).
  3. A function of (x+vt)(x + vt) is a wave moving in the −x-x direction with speed v=bav = \sqrt{\frac{b}{a}}.
  4. So the answer is (a).
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Q173NEET 2011 · AIPMT · PRELIMSEasy

Progressive Wave Equation · Phase difference and path difference

Two waves are represented by the equations

y1 = aasin(ω\omegat + kx + 0.57) m and

y2 = acos(ω\omegat + kx) m, where x is in meter and t in\text{in} sec. The phase difference between them is

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Answer: (a)

  1. y2=acos⁡(ωt+kx)=asin⁡(ωt+kx+1.57)y_2 = a\cos(\omega t + kx) = a\sin(\omega t + kx + 1.57)
  2. Δϕ=1.57−0.57=1.0\Delta\phi = 1.57 - 0.57 = 1.0 rad
  3. So the answer is (a) 1.0 radian.
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Q174NEET 2010 · AIPMT · PRELIMSMedium

Progressive Wave Equation · Particle velocity and wave velocity

A transverse wave is represented by

y = Asin(ω\omegat −- kx). For what value of the wavelength is the wave velocity equal to the maximum particle velocity?

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Answer: (c)

  1. Wave velocity v=ωk=ωλ2πv = \frac{\omega}{k} = \frac{\omega\lambda}{2\pi}; maximum particle velocity =Aω= A\omega
  2. ωλ2π=Aω⇒λ=2πA\frac{\omega\lambda}{2\pi} = A\omega \Rightarrow \lambda = 2\pi A
  3. So the answer is (c) 2πA2\pi A.
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Q175JEE Main 2010 · AIEEEMedium

Progressive Wave Equation · Tension from the wave equation

The equation of a wave on a string of linear mass density 0.04 kg m−10.04\text{ kg m}^{-1} is given by y=0.02 (m)sin⁡[2π(t0.04 (s)−x0.50 (m))].y = 0.02\,(\text{m})\sin\left[2\pi\left(\frac{t}{0.04\,(\text{s})} - \frac{x}{0.50\,(\text{m})}\right)\right].

The tension in the string is

Show answer and solution

Answer: (d)

  1. From the equation: period 0.04 s0.04\text{ s} (f=25 Hzf = 25\text{ Hz}), λ=0.50 m\lambda = 0.50\text{ m}
  2. v=fλ=25×0.5=12.5 m/sv = f\lambda = 25 \times 0.5 = 12.5\text{ m/s}
  3. Tension =μv2=0.04×156.25=6.25 N= \mu v^2 = 0.04 \times 156.25 = 6.25\text{ N}
  4. So the answer is (d) 6.25 N.
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Q176NEET 2009 · AIPMTMedium

Progressive Wave Equation · Writing the wave equation and its direction

A wave in a string has an amplitude of 2 cm. The wave travels in the +ve direction of x axis with a speed of 128 m/s. and it is noted that 5 complete waves fit in 4m length of the string. The equation describing the wave is

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Answer: (c)

  1. 5 waves in 4 m: λ=0.8 m\lambda = 0.8\text{ m}, so k=2π0.8=7.85 m−1k = \frac{2\pi}{0.8} = 7.85\text{ m}^{-1}
  2. ω=kv=7.85×128≈1005 rad/s\omega = kv = 7.85 \times 128 \approx 1005\text{ rad/s}
  3. Wave along +x+x has the form sin⁡(kx−ωt)\sin(kx - \omega t); A=2 cm=0.02 mA = 2\text{ cm} = 0.02\text{ m}
  4. So the answer is (c) y=0.02sin⁡(7.85x−1005t)y = 0.02\sin(7.85x - 1005t).
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Q177JEE Main 2008 · AIEEEEasy

Progressive Wave Equation · Reading the wave equation

A wave travelling along the xx-axis is described by the equation y(x,t)=0.005cos⁡(αx−βt).y(x, t) = 0.005\cos(\alpha x - \beta t). If the wavelength and the time period of the wave are 0.08 m0.08\text{ m} and 2.0 s2.0\text{ s}, respectively, then α\alpha and β\beta in appropriate units are

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Answer: (a)

  1. α=k=2πλ=2π0.08=25π m−1\alpha = k = \dfrac{2\pi}{\lambda} = \dfrac{2\pi}{0.08} = 25\pi\text{ m}^{-1}
  2. β=ω=2πT=2π2.0=π rad/s\beta = \omega = \dfrac{2\pi}{T} = \dfrac{2\pi}{2.0} = \pi\text{ rad/s}
  3. So the answer is (a) α=25.00π\alpha = 25.00\pi, β=π\beta = \pi.
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Q178NEET 2008 · AIPMTEasy

Progressive Wave Equation · Writing the wave equation and its direction

The wave described by y = 0.25 sin(10π\pix −- 2π\pit), where x and y are in metres and t in seconds, is a wave travelling along the

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Answer: (a)

  1. k=10πk = 10\pi, so λ=2π10π=0.2 m\lambda = \dfrac{2\pi}{10\pi} = 0.2\text{ m}.
  2. ω=2π\omega = 2\pi, so f=1 Hzf = 1\text{ Hz}.
  3. Form (kx−ωt)(kx - \omega t) means the wave travels along +x+x.
  4. So the answer is (a) +x+x direction, f=1 Hzf = 1\text{ Hz}, λ=0.2 m\lambda = 0.2\text{ m}.
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Q179NEET 2008 · AIPMTEasy

Progressive Wave Equation · Phase difference and path difference

Two points are located at a distance of 10 m and 15 m from the source of oscillation. The period of oscillation is 0.05 sec and the velocity of the wave is 300 m/s. What is the phase difference between the oscillations of two points?

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Answer: (d)

  1. λ=vT=300×0.05=15\lambda = vT = 300 \times 0.05 = 15 m
  2. Path difference Δx=15−10=5\Delta x = 15 - 10 = 5 m
  3. Δϕ=2πλΔx=2π×515=2π3\Delta\phi = \frac{2\pi}{\lambda}\Delta x = \frac{2\pi \times 5}{15} = \frac{2\pi}{3}
  4. So the answer is (d) 2π/32\pi/3.
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Q180NEET 2006 · AIPMTEasy

Progressive Wave Equation · Reading the wave equation

A transverse wave propagating along x-axis is represented by y(x, t) = 8.0 sin (0.5 π\pix −- 4π\pit −π-\pi/4) where x is in metres and t is in seconds. The speed of the wave is

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Answer: (a)

  1. k=0.5π m−1k = 0.5\pi\text{ m}^{-1}, ω=4π rad/s\omega = 4\pi\text{ rad/s}
  2. v=ωk=4π0.5π=8 m/sv = \dfrac{\omega}{k} = \dfrac{4\pi}{0.5\pi} = 8\text{ m/s}
  3. So the answer is (a) 8 m/s8\text{ m/s}.
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Q181JEE Main 2004 · AIEEEEasy

Progressive Wave Equation · Reading the wave equation

The displacement yy of a particle in a medium can be expressed as, y=10−6sin⁡(100t+20x+π4) my = 10^{-6}\sin\left(100t + 20x + \frac{\pi}{4}\right)\text{ m} where tt is in second and xx in meter. The speed of the wave is

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Answer: (b)

  1. ω=100 rad/s\omega = 100\text{ rad/s}, k=20 m−1k = 20\text{ m}^{-1}
  2. v=ωk=10020=5 m/sv = \dfrac{\omega}{k} = \dfrac{100}{20} = 5\text{ m/s}
  3. So the answer is (b) 5 m/s5\text{ m/s}.
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Q182NEET 2004 · AIPMTEasy

Progressive Wave Equation · Phase difference and path difference

The phase difference between two waves. represented by

y1 = 10−-6 sin[100t + (x/50) + 0.5] m

y2 = 10−-6 cos[100t + (x/50)] m,

where x is expressed in metres and t is exressed in secondss, is approximately.

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Answer: (a)

  1. y2=10−6cos⁡(100t+x50)=10−6sin⁡(100t+x50+1.57)y_2 = 10^{-6}\cos\left(100t + \frac{x}{50}\right) = 10^{-6}\sin\left(100t + \frac{x}{50} + 1.57\right)
  2. y1y_1 has phase constant 0.50.5, y2y_2 has 1.571.57.
  3. Δϕ=1.57−0.5=1.07\Delta\phi = 1.57 - 0.5 = 1.07 rad
  4. So the answer is (a) 1.07 radians.
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Q183JEE Main 2003 · AIEEEEasy

Progressive Wave Equation · Reading the wave equation

The displacement yy of a wave travelling in the xx-direction is given by

y=10−4sin⁡(600t−2x+π3) metresy = 10^{-4}\sin\left(600t - 2x + \frac{\pi}{3}\right)\text{ metres}

where xx is expressed in metres and tt in seconds. The speed of the wave - motion, in ms−1\text{ms}^{-1}, is

Show answer and solution

Answer: (a)

  1. ω=600 rad/s\omega = 600\text{ rad/s}, k=2 m−1k = 2\text{ m}^{-1}
  2. v=ωk=6002=300 m/sv = \dfrac{\omega}{k} = \dfrac{600}{2} = 300\text{ m/s}
  3. So the answer is (a) 300300.
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Q184NEET 2002 · AIPMTEasy

Progressive Wave Equation · Writing the wave equation and its direction

A wave travelling in positive X-direction with a == 0.2 m, velocity = 360 ms−1{}^{-1} and λ=\lambda = 60 m, then correct expression for the wave is

Show answer and solution

Answer: (c)

  1. f=vλ=36060=6 Hzf = \dfrac{v}{\lambda} = \dfrac{360}{60} = 6\text{ Hz}
  2. Wave along +x+x: y=asin⁡2π(ft−xλ)y = a\sin 2\pi\left(ft - \dfrac{x}{\lambda}\right)
  3. y=0.2sin⁡[2π(6t−x60)]y = 0.2\sin\left[2\pi\left(6t - \dfrac{x}{60}\right)\right]
  4. So the answer is (c).
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Q185NEET 2001 · AIPMTEasy

Progressive Wave Equation · Reading the wave equation

The equation of a wave is represented by

y == 10−-4 sin(100t −x10-\frac{x}{10}) m. then the velocity of wave will be

Show answer and solution

Answer: (c)

  1. y=10−4sin⁡(100t−x10)y = 10^{-4}\sin\left(100t - \dfrac{x}{10}\right): ω=100\omega = 100, k=110k = \dfrac{1}{10}.
  2. v=ωk=1000.1=1000 m/sv = \dfrac{\omega}{k} = \dfrac{100}{0.1} = 1000\text{ m/s}
  3. So the answer is (c) 1000 m/s1000\text{ m/s}.
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Q186NEET 1998 · AIPMTMedium

Progressive Wave Equation · Particle velocity and wave velocity

A transverse wave is represented by the equation

y=y0sin⁡2πλ(vt−x)y = y_0\sin\frac{2\pi}{\lambda}(vt - x)

For what value of λ\lambda is the maximum particle velocity equal to two times the wave velocity?

Show answer and solution

Answer: (d)

  1. y=y0sin⁡(2πvλt−2πλx)y = y_0\sin\left(\frac{2\pi v}{\lambda}t - \frac{2\pi}{\lambda}x\right): vp,max⁡=2πvy0λv_{p,\max} = \frac{2\pi v y_0}{\lambda}
  2. 2πvy0λ=2v⇒λ=πy0\frac{2\pi v y_0}{\lambda} = 2v \Rightarrow \lambda = \pi y_0
  3. So the answer is (d) λ=πy0\lambda = \pi y_0.
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Q187NEET 1996 · AIPMTEasy

Progressive Wave Equation · Reading the wave equation

The equation of a sound wave is y=0.0015sin⁡(62.4x+316t)y = 0.0015\sin(62.4x + 316t). The wavelength of this wave is

Show answer and solution

Answer: (c)

  1. k=62.4k = 62.4
  2. λ=2πk=6.2862.4≈0.1\lambda = \dfrac{2\pi}{k} = \dfrac{6.28}{62.4} \approx 0.1 unit
  3. So the answer is (c) 0.10.1 unit.
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Q188NEET 1996 · AIPMTEasy

Progressive Wave Equation · Phase difference and path difference

Two sound waves having a phase difference of 60∘60^\circ have path difference of

Show answer and solution

Answer: (a)

  1. Path difference Δx=λ2π Δϕ\Delta x = \frac{\lambda}{2\pi}\,\Delta\phi.
  2. Δϕ=60∘=π3\Delta\phi = 60^\circ = \frac{\pi}{3}, so Δx=λ2π⋅π3=λ6\Delta x = \frac{\lambda}{2\pi}\cdot\frac{\pi}{3} = \frac{\lambda}{6}
  3. So the answer is (a) λ6\frac{\lambda}{6}.
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Q189NEET 1994 · AIPMTEasy

Progressive Wave Equation · Writing the wave equation and its direction

Which one of the following represents a wave?

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Answer: (a)

  1. A travelling wave must be a function of (ωt±kx)(\omega t \pm kx), depending on both xx and tt.
  2. y=Asin⁡(ωt−kx)y = A\sin(\omega t - kx) is the standard progressive wave.
  3. Asin⁡kxA\sin kx has no time dependence and Asin⁡ωtA\sin\omega t has no space dependence, so they are not waves.
  4. So the answer is (a) y=Asin⁡(ωt−kx)y = A\sin(\omega t - kx).
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Q190NEET 1992 · AIPMTEasy

Progressive Wave Equation · Reading the wave equation

The frequency of sinusodial wave y=0.40cos⁡[2000t+0.80]y = 0.40\cos[2000t + 0.80] would be

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Answer: (d)

  1. ω=2000 rad/s\omega = 2000\text{ rad/s}
  2. f=ω2π=20002π=1000π Hzf = \dfrac{\omega}{2\pi} = \dfrac{2000}{2\pi} = \dfrac{1000}{\pi}\text{ Hz}
  3. So the answer is (d) 1000π Hz\dfrac{1000}{\pi}\text{ Hz}.
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Q191NEET 1990 · AIPMTEasy

Progressive Wave Equation · Phase difference and path difference

Velocity of sound waves in air is 330 m/s330\text{ m/s}. For a particular sound wave in air, a path difference of 40 cm40\text{ cm} is equivalent to phase difference of 1.6π1.6\pi. The frequency of this wave is

Show answer and solution

Answer: (c)

  1. Δϕ=2πλΔx⇒1.6π=2π(0.4)λ\Delta\phi = \frac{2\pi}{\lambda}\Delta x \Rightarrow 1.6\pi = \frac{2\pi(0.4)}{\lambda}
  2. λ=0.81.6=0.5 m\lambda = \frac{0.8}{1.6} = 0.5\text{ m}
  3. f=vλ=3300.5=660 Hzf = \frac{v}{\lambda} = \frac{330}{0.5} = 660\text{ Hz}
  4. So the answer is (c) 660 Hz660\text{ Hz}.
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Q192NEET 1988 · AIPMTEasy

Progressive Wave Equation · Reading the wave equation

Equation of progressive wave is given by y=4sin⁡[π(t5−x9)+π6]y = 4\sin\left[\pi\left(\frac{t}{5} - \frac{x}{9}\right) + \frac{\pi}{6}\right] where y,xy, x are in cm and tt is in seconds. Then which of the following is correct?

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Answer: (b)

  1. y=4sin⁡(π5t−π9x+π6)y = 4\sin\left(\dfrac{\pi}{5}t - \dfrac{\pi}{9}x + \dfrac{\pi}{6}\right): A=4 cmA = 4\text{ cm}, ω=π5\omega = \dfrac{\pi}{5}, k=π9k = \dfrac{\pi}{9}.
  2. λ=2ππ/9=18 cm\lambda = \dfrac{2\pi}{\pi/9} = 18\text{ cm}; v=95=1.8 cm/sv = \dfrac{9}{5} = 1.8\text{ cm/s}; f=0.1 Hzf = 0.1\text{ Hz}
  3. So the answer is (b) λ=18 cm\lambda = 18\text{ cm}.
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Q193MHT CET 2026 · 19 MAY · SHIFT 2Easy

Reflection, Superposition & Interference · Reflection of waves and echo

A man standing between two parallel cliffs fires a gun. He hear two echos one after 33 second and the other after 55 second. The separation between the two cliffs is 13601360 m, the speed of sound is

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Answer: (c)

  1. Echo time t=2dvt = \frac{2d}{v}, so distances to the cliffs are d1=3v2d_1 = \frac{3v}{2} and d2=5v2d_2 = \frac{5v}{2}
  2. d1+d2=4v=1360⇒v=340 m/sd_1 + d_2 = 4v = 1360 \Rightarrow v = 340\text{ m/s}
  3. So the answer is (c) 340 m/s.
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Q194MHT CET 2026 · 18 APR · SHIFT 2Easy

Reflection, Superposition & Interference · Reflection of waves and echo

A person standing between two parallel cliffs fires a gun and hears two echoes, first echo after 1 second and second echo after 3 second. The distance between the two cliffs is (The velocity of sound =330= 330 m/s)

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Answer: (b)

  1. d1=vt12=330×12=165 md_1 = \frac{v t_1}{2} = \frac{330 \times 1}{2} = 165\text{ m}, d2=330×32=495 md_2 = \frac{330 \times 3}{2} = 495\text{ m}
  2. Separation =165+495=660 m= 165 + 495 = 660\text{ m}
  3. So the answer is (b) 660 m.
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Q195MHT CET 2026 · 20 APR · SHIFT 2Medium

Reflection, Superposition & Interference · Superposition: resultant amplitude

Two sound waves each of wavelength λ\lambda and same amplitude AA interfere at point QQ. If the path difference is λ4\frac{\lambda}{4}, the amplitude of the resultant wave at point QQ is [sin⁡π2=1,cos⁡π2=0]\left[\sin\frac{\pi}{2} = 1, \cos\frac{\pi}{2} = 0\right]

Show answer and solution

Answer: (b)

  1. Phase difference ϕ=2πλ×λ4=π2\phi = \frac{2\pi}{\lambda} \times \frac{\lambda}{4} = \frac{\pi}{2}.
  2. AR=A2+A2+2A2cos⁡π2=2AA_R = \sqrt{A^2 + A^2 + 2A^2\cos\frac{\pi}{2}} = \sqrt{2}A.
  3. So the answer is (b) 2A\sqrt{2}A.
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Q196JEE Main 2026 · 22 JAN · SHIFT 1Difficult

Reflection, Superposition & Interference · Interference: maximum and minimum intensity

Two loudspeakers (L1(L_1 and L2)L_2) are placed with a separation of 10 m, as shown in figure. Both speakers are fed with an audio input signal of same frequency with constant volume. A voice recorder, initially at point AA, at equidistant to both loudspeakers, is moved by 25 m along the line ABAB while monitoring the audio signal. The measured signal was found to undergo 10 cycles of minima and maxima during the movement. The frequency of the input signal is ______ Hz (Speed of sound in air is 324 m/s324\text{ m/s} and 5=2.23\sqrt{5} = 2.23)

Figure

Numerical answer type. Work it out, then open the answer.

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Answer: 600

  1. At AA the path difference is 00. At BB (25 m up): L1B=402+202=205=44.6 mL_1B = \sqrt{40^2 + 20^2} = 20\sqrt{5} = 44.6\text{ m}, L2B=402+302=50 mL_2B = \sqrt{40^2 + 30^2} = 50\text{ m}.
  2. Path difference at BB =50−44.6=5.4 m= 50 - 44.6 = 5.4\text{ m}.
  3. 10 cycles of maxima and minima means the path difference changed by 10λ10\lambda: λ=0.54 m\lambda = 0.54\text{ m}.
  4. f=vλ=3240.54=600 Hzf = \frac{v}{\lambda} = \frac{324}{0.54} = 600\text{ Hz}.
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Q197MHT CET 2025 · 22 APR · SHIFT 1Easy

Reflection, Superposition & Interference · Reflection of waves and echo

A person standing between two parallel cliffs fires a gun and hears two echoes, first echo after 1 second and the second echo after 3 second. The distance between the two cliffs is (Velocity of sound =340 m/s= 340\text{ m/s})

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Answer: (b)

  1. d1=vt12=340×12=170 md_1 = \frac{v t_1}{2} = \frac{340 \times 1}{2} = 170\text{ m}, d2=340×32=510 md_2 = \frac{340 \times 3}{2} = 510\text{ m}
  2. Separation =170+510=680 m= 170 + 510 = 680\text{ m}
  3. So the answer is (b) 680 m.
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Q198JEE Main 2025 · 8 APR · SHIFT 2Difficult

Reflection, Superposition & Interference · Superposition: resultant amplitude

The amplitude and phase of a wave that is formed by the superposition of two harmonic travelling waves, y1(x,t)=4sin⁡(kx−ωt)y_1(x, t) = 4\sin(kx - \omega t) and y2(x,t)=2sin⁡(kx−ωt+2π3)y_2(x, t) = 2\sin\left(kx - \omega t + \frac{2\pi}{3}\right), are:

(Take the angular frequency of initial waves same as ω\omega)

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Answer: (b)

  1. A2=42+22+2(4)(2)cos⁡2π3=16+4−8=12⇒A=23A^2 = 4^2 + 2^2 + 2(4)(2)\cos\frac{2\pi}{3} = 16 + 4 - 8 = 12 \Rightarrow A = 2\sqrt{3}.
  2. tan⁡δ=2sin⁡120∘4+2cos⁡120∘=33=13⇒δ=π6\tan\delta = \frac{2\sin 120^\circ}{4 + 2\cos 120^\circ} = \frac{\sqrt{3}}{3} = \frac{1}{\sqrt{3}} \Rightarrow \delta = \frac{\pi}{6}.
  3. So the answer is (b) [23,π6]\left[2\sqrt{3}, \frac{\pi}{6}\right].
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Q199MHT CET 2024 · 9 MAY · SHIFT 2Easy

Reflection, Superposition & Interference · Superposition: resultant amplitude

The equations of two waves are given as

y1=asin⁡(ωt+ϕ1)y2=asin⁡(ωt+ϕ2)\begin{matrix} y_1 = a\sin(\omega t + \phi_1) \\ y_2 = a\sin(\omega t + \phi_2) \end{matrix}

If amplitude and time period of resultant wave is same as the individual waves, then (ϕ1−ϕ2)(\phi_1 - \phi_2) is

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Answer: (a)

  1. Resultant amplitude: AR2=a2+a2+2a2cos⁡ϕA_R^2 = a^2 + a^2 + 2a^2\cos\phi, with ϕ=ϕ1−ϕ2\phi = \phi_1 - \phi_2
  2. AR=a⇒a2=2a2(1+cos⁡ϕ)⇒cos⁡ϕ=−12A_R = a \Rightarrow a^2 = 2a^2(1 + \cos\phi) \Rightarrow \cos\phi = -\frac{1}{2}
  3. So the answer is (a) cos⁡−1(−12)\cos^{-1}\left(-\frac{1}{2}\right).
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Q200MHT CET 2024 · 9 MAY · SHIFT 1Easy

Reflection, Superposition & Interference · Superposition: resultant amplitude

Two sound waves having same amplitude ' AA ' and angular frequency ' ω\omega ' but having a phase difference of (π2)c\left(\frac{\pi}{2}\right)^{c} are superimposed then the maximum amplitude of the resultant wave is

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Answer: (c)

  1. AR=A2+A2+2A2cos⁡ϕA_R = \sqrt{A^2 + A^2 + 2A^2\cos\phi}
  2. ϕ=π2⇒cos⁡ϕ=0\phi = \frac{\pi}{2} \Rightarrow \cos\phi = 0, so AR=2AA_R = \sqrt{2}A
  3. So the answer is (c) 2A\sqrt{2}A.
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Q201MHT CET 2023 · 13 MAY · SHIFT 2Easy

Reflection, Superposition & Interference · Reflection of waves and echo

A transverse wave strike against a wall,

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Answer: (a)

  1. A wall is a rigid (denser) boundary, so the reflected wave is inverted: phase change of 180∘180^\circ.
  2. The reflected wave travels back in the same medium, so its speed is unchanged.
  3. So the answer is (a).
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Q202MHT CET 2023 · 9 MAY · SHIFT 1Easy

Reflection, Superposition & Interference · Superposition: resultant amplitude

Equation of simple harmonic progressive wave is given by y=1asin⁡ωt±1bcos⁡ωty = \frac{1}{\sqrt{a}}\sin\omega t \pm \frac{1}{\sqrt{b}}\cos\omega t then the resultant amplitude of the wave is (cos⁡90∘=0)(\cos 90^\circ = 0)

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Answer: (d)

  1. sin⁡ωt\sin\omega t and cos⁡ωt\cos\omega t differ in phase by 90∘90^\circ, so AR=A12+A22A_R = \sqrt{A_1^2 + A_2^2}
  2. AR=1a+1b=a+babA_R = \sqrt{\frac{1}{a} + \frac{1}{b}} = \sqrt{\frac{a + b}{ab}}
  3. So the answer is (d) a+bab\sqrt{\frac{a+b}{ab}}.
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Q203JEE Main 2023 · 31 JAN · SHIFT 2Easy

Reflection, Superposition & Interference · Superposition: resultant amplitude

The displacement equations of two interfering waves are given by

y1=10sin⁡(ωt+π3) cm,y2=5[sin⁡ωt+3cos⁡ωt] cmy_1 = 10\sin\left(\omega t + \frac{\pi}{3}\right)\text{ cm}, y_2 = 5[\sin\omega t + \sqrt{3}\cos\omega t]\text{ cm} respectively.

The amplitude of the resultant wave is _______ cm\text{cm}.

Numerical answer type. Work it out, then open the answer.

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Answer: 20

  1. y2=5sin⁡ωt+53cos⁡ωt=10sin⁡(ωt+π3)y_2 = 5\sin\omega t + 5\sqrt{3}\cos\omega t = 10\sin\left(\omega t + \frac{\pi}{3}\right) since 52+(53)2=10\sqrt{5^2 + (5\sqrt{3})^2} = 10 and tan⁡ϕ=3\tan\phi = \sqrt{3}.
  2. So y1y_1 and y2y_2 are in phase, each of amplitude 10 cm10\text{ cm}.
  3. Resultant amplitude =10+10=20 cm= 10 + 10 = 20\text{ cm}.
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Q204JEE Main 2023 · 29 JAN · SHIFT 1Easy

Reflection, Superposition & Interference · Superposition: resultant amplitude

Two simple harmonic waves having equal amplitudes of 8 cm and equal frequency of 10 Hz are moving along the same direction. The resultant amplitude is also 8 cm. The phase difference between the individual waves is _________ degree.

Numerical answer type. Work it out, then open the answer.

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Answer: 120

  1. AR=A2+2cos⁡ϕA_R = A\sqrt{2 + 2\cos\phi} with AR=A=8 cmA_R = A = 8\text{ cm}.
  2. 2+2cos⁡ϕ=1⇒cos⁡ϕ=−122 + 2\cos\phi = 1 \Rightarrow \cos\phi = -\frac{1}{2}.
  3. So ϕ=120∘\phi = 120^\circ.
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Q205JEE Main 2022 · 25 JUL · SHIFT 2EasyOld syllabus

Reflection, Superposition & Interference · Superposition: resultant amplitude

Two waves executing simple harmonic motions travelling in the same direction with same amplitude and frequency are superimposed. The resultant amplitude is equal to the 3\sqrt{3} times of amplitude of individual motions. The phase difference between the two motions is ___________ (degree).

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 60

  1. Resultant amplitude AR=A2+A2+2A2cos⁡ϕ=A2+2cos⁡ϕA_R = \sqrt{A^2 + A^2 + 2A^2\cos\phi} = A\sqrt{2 + 2\cos\phi}.
  2. 2+2cos⁡ϕ=3⇒2+2cos⁡ϕ=3⇒cos⁡ϕ=12\sqrt{2 + 2\cos\phi} = \sqrt{3} \Rightarrow 2 + 2\cos\phi = 3 \Rightarrow \cos\phi = \frac{1}{2}.
  3. So ϕ=60∘\phi = 60^\circ.
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Q206MHT CET 2022 · 11 AUG · SHIFT 2Easy

Reflection, Superposition & Interference · Interference: maximum and minimum intensity

Two waves are superimposed whose ratio of intensities is 9:19 : 1. The ratio of maximum and minimum intensity is

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Answer: (b)

  1. I∝a2I \propto a^2, so a1a2=91=3\frac{a_1}{a_2} = \sqrt{\frac{9}{1}} = 3.
  2. ImaxImin=(a1+a2a1−a2)2=(3+13−1)2=4\frac{I_{max}}{I_{min}} = \left(\frac{a_1 + a_2}{a_1 - a_2}\right)^2 = \left(\frac{3 + 1}{3 - 1}\right)^2 = 4.
  3. So the answer is (b) 4:14 : 1.
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Q207JEE Main 2022 · 24 JUN · SHIFT 1Medium

Reflection, Superposition & Interference · Superposition: resultant amplitude

The equations of two waves are given by:

y1 = 5 sin 2π\pi(x - vt) cm

y2 = 3 sin 2π\pi(x −- vt + 1.5) cm

These waves are simultaneously passing through a string. The amplitude of the resulting wave is:

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Answer: (a)

  1. Phase difference ϕ=2π×1.5=3π\phi = 2\pi \times 1.5 = 3\pi, i.e. the waves are in opposite phase.
  2. AR=5−3=2 cmA_R = 5 - 3 = 2\text{ cm}.
  3. So the answer is (a) 2 cm2\text{ cm}.
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Q208JEE Main 2021 · 26 AUG · SHIFT 2Medium

Reflection, Superposition & Interference · Superposition: resultant amplitude

Two waves are simultaneously passing through a string and their equations are: y1 = A1 sin k(x −- vt), y2 = A2 sin k(x −- vt + x0). Given amplitudes A1 = 12 mm and A2 = 5 mm, x0 = 3.5 cm and wave number k = 6.28 cm−1{}^{-1}. The amplitude of resulting wave will be ................ mm.

Numerical answer type. Work it out, then open the answer.

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Answer: 7

  1. Phase difference ϕ=kx0=6.28×3.5=2π×3.5=7π\phi = kx_0 = 6.28 \times 3.5 = 2\pi \times 3.5 = 7\pi, i.e. opposite phase.
  2. AR=A1−A2=12−5=7 mmA_R = A_1 - A_2 = 12 - 5 = 7\text{ mm}.
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Q209JEE Main 2020 · 9 JAN · SHIFT 1Difficult

Reflection, Superposition & Interference · Superposition: resultant amplitude

Three harmonic waves having equal frequency ν\nu and same intensity I0I_0, have phase angles 0, π4\frac{\pi}{4} and −π4-\frac{\pi}{4} respectively. When they are superimposed the intensity of the resultant wave is close to:

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Answer: (a)

  1. Equal intensities, so equal amplitudes aa with I0∝a2I_0 \propto a^2.
  2. The ±π4\pm\frac{\pi}{4} waves add to 2acos⁡π4=2a2a\cos\frac{\pi}{4} = \sqrt{2}a along the phase-0 wave.
  3. AR=a+2a=2.414aA_R = a + \sqrt{2}a = 2.414a, so I=(2.414)2I0≈5.8I0I = (2.414)^2 I_0 \approx 5.8I_0.
  4. So the answer is (a) 5.8I05.8I_0.
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Q210JEE Main 2020 · 5 SEP · SHIFT 2Difficult

Reflection, Superposition & Interference · Interference: maximum and minimum intensity

Two coherent sources of sound, S1 and S2, produce sound waves of the same wavelength, λ\lambda = 1 m, in phase. S1 and S2 are placed 1.5 m apart (see fig). A listener, located at L, directly in front of S2 finds that the intensity is at a minimum

when he is 2 m away from S2. The listener moves away from S1, keeping his distance from S2 fixed. The adjacent maximum of intensity is observed when the listener is at a distance d from S1. Then, d is:

Figure

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Answer: (c)

  1. At LL: S1L=1.52+22=2.5 mS_1L = \sqrt{1.5^2 + 2^2} = 2.5\text{ m}, path difference =2.5−2=0.5 m=λ2= 2.5 - 2 = 0.5\text{ m} = \frac{\lambda}{2} (minimum).
  2. Moving away from S1S_1 increases the path difference; the next maximum needs path difference =λ=1 m= \lambda = 1\text{ m}.
  3. d−2=1⇒d=3 md - 2 = 1 \Rightarrow d = 3\text{ m}.
  4. So the answer is (c) 3 m3\text{ m}.
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Q211JEE Main 2013 · 9 APR · SHIFT 1Medium

Reflection, Superposition & Interference · Reflection of waves and echo

An engine approaches a hill with a constant speed. When it is at a distance of 0.9 km, it blows a whistle whose echo is heard by the driver after 5 seconds. If the speed of sound in air is 330 m/s, then the speed of the engine is:

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Answer: (d)

  1. In 5 s5\text{ s} the engine moves 5v5v, so it is at 900−5v900 - 5v from the hill when it hears the echo.
  2. Sound path: 900+(900−5v)=330×5=1650900 + (900 - 5v) = 330 \times 5 = 1650.
  3. 1800−5v=1650⇒v=30 m/s1800 - 5v = 1650 \Rightarrow v = 30\text{ m/s}.
  4. So the answer is (d) 30 m/s30\text{ m/s}.
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Q212NEET 2008 · AIPMTEasy

Reflection, Superposition & Interference · Interference: maximum and minimum intensity

Two periodic waves of intensities II1 and II2 pass through a region at the same time in the same direction. The sum of the maximum and minimum intensities is

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Answer: (b)

  1. Imax=(I1+I2)2I_{max} = \left(\sqrt{I_1} + \sqrt{I_2}\right)^2, Imin=(I1−I2)2I_{min} = \left(\sqrt{I_1} - \sqrt{I_2}\right)^2.
  2. Adding, the cross terms ±2I1I2\pm 2\sqrt{I_1 I_2} cancel: Imax+Imin=2(I1+I2)I_{max} + I_{min} = 2(I_1 + I_2).
  3. So the answer is (b) 2(I1+I2)2(I_1 + I_2).
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Q213NEET 2001 · AIPMTEasy

Reflection, Superposition & Interference · Superposition: resultant amplitude

Two waves having equation x1 = aasin(ω\omegat −- kx + ϕ\phi1), x2 = asin(ω\omegat −-kx + ϕ\phi2). If in the resultant wave the frequency and amplitude remain equal to amplitude of superimposing waves, the phase difference between them is

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Answer: (b)

  1. AR2=2a2(1+cos⁡ϕ)A_R^2 = 2a^2(1 + \cos\phi) where ϕ=ϕ1−ϕ2\phi = \phi_1 - \phi_2
  2. AR=a⇒1+cos⁡ϕ=12⇒cos⁡ϕ=−12A_R = a \Rightarrow 1 + \cos\phi = \frac{1}{2} \Rightarrow \cos\phi = -\frac{1}{2}
  3. ϕ=2π3\phi = \frac{2\pi}{3}
  4. So the answer is (b) 2π3\frac{2\pi}{3}.
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Q214NEET 1993 · AIPMTEasy

Reflection, Superposition & Interference · Superposition: resultant amplitude

Wave has simple harmonic motion whose period is 4 seconds while another wave which also possesses simple harmonic motion has its period 3 second. If both are combined, then the resultant wave will have the period equal to

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Answer: (c)

  1. The combined motion repeats only when both waves complete whole numbers of cycles together.
  2. Resultant period == LCM of 4 s4\text{ s} and 3 s3\text{ s} =12 s= 12\text{ s}.
  3. So the answer is (c) 12 s12\text{ s}.
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Q215MHT CET 2026 · 19 MAY · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Stationary wave equation

For a stationary wave, y=10cos⁡(πx/15)sin⁡(48πt)y = 10\cos(\pi x/15)\sin(48\pi t) cm, the distance between a node and the successive antinode is

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Answer: (d)

  1. k=π15=2πλ⇒λ=30 cmk = \frac{\pi}{15} = \frac{2\pi}{\lambda} \Rightarrow \lambda = 30\text{ cm}.
  2. Node to next antinode =λ4=7.5 cm= \frac{\lambda}{4} = 7.5\text{ cm}.
  3. So the answer is (d) 7.57.5 cm.
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Q216MHT CET 2026 · 14 MAY · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Stationary wave equation

The equation of a stationary wave along a stretched string is y=5sin⁡πx3cos⁡40πty = 5\sin\frac{\pi x}{3}\cos 40\pi t where xx and yy are in cm and tt in second. The separation between two adjacent nodes is

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Answer: (c)

  1. k=π3=2πλ⇒λ=6 cmk = \frac{\pi}{3} = \frac{2\pi}{\lambda} \Rightarrow \lambda = 6\text{ cm}.
  2. Adjacent nodes are λ2=3 cm\frac{\lambda}{2} = 3\text{ cm} apart.
  3. So the answer is (c) 33 cm.
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Q217MHT CET 2026 · 19 APR · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Stationary wave equation

For stationary wave, y=12cos⁡(πx10)sin⁡(36πt)y = 12\cos\left(\frac{\pi x}{10}\right)\sin(36\pi t) cm, the distance between a node and the successive antinode is

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Answer: (d)

  1. k=π10=2πλ⇒λ=20 cmk = \frac{\pi}{10} = \frac{2\pi}{\lambda} \Rightarrow \lambda = 20\text{ cm}.
  2. Node to next antinode =λ4=5 cm= \frac{\lambda}{4} = 5\text{ cm}.
  3. So the answer is (d) 55 cm.
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Q218MHT CET 2026 · 19 APR · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Nodes, antinodes and properties

Two waves of same frequency (nn) approaching each other with same velocity of 1818 m/s interfere. The distance between two consecutive antinodes is

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Answer: (c)

  1. λ=vn=18n\lambda = \frac{v}{n} = \frac{18}{n}.
  2. Consecutive antinodes are λ2=9n\frac{\lambda}{2} = \frac{9}{n} apart.
  3. So the answer is (c) 9n\frac{9}{n}.
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Q219MHT CET 2026 · 17 APR · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Nodes, antinodes and properties

In case of stationary wave pattern, which of the following statement is CORRECT?

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Answer: (d)

  1. (a) Consecutive antinodes are λ2\frac{\lambda}{2} apart, not λ\lambda: false.
  2. (b) An open pipe gives all harmonics: false.
  3. (c) A closed pipe gives only odd harmonics: false.
  4. (d) For a string the first overtone is the second harmonic 2n2n: true.
  5. So the answer is (d).
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Q220MHT CET 2026 · 13 APR · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Nodes, antinodes and properties

In a stationary wave, all the particles

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Answer: (a)

  1. In a stationary wave all particles (except nodes, which stay at rest) oscillate with the same period.
  2. Amplitude 2Asin⁡kx2A\sin kx varies with position: zero at nodes, maximum at antinodes.
  3. So the answer is (a).
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Q221MHT CET 2026 · 19 MAY · SHIFT 1Easy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A stretched string of length 'LL' is fixed at both the ends, has 'nn' nodes (n>2n > 2). The length of the string in terms of nn and wavelength λ\lambda is

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Answer: (d)

  1. nn nodes (including both ends) divide the string into n−1n - 1 loops.
  2. Each loop is λ2\frac{\lambda}{2}, so L=(n−1)λ2L = (n - 1)\frac{\lambda}{2}.
  3. So the answer is (d).
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Q222MHT CET 2026 · 18 APR · SHIFT 2Easy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

The fundamental frequency 'nn' of the tuning fork is 288 Hz, it will not resonate with the frequency

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Answer: (c)

  1. Resonance occurs at the fundamental or its whole-number multiples: 288,576,864,…288, 576, 864, \dots Hz.
  2. 844288=2.93\frac{844}{288} = 2.93 is not a whole number.
  3. So the answer is (c) 844844 Hz.
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Q223MHT CET 2026 · 16 APR · SHIFT 1Easy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

When a sonometer wire vibrates in the third overtone, the number of antinodes and nodes formed on the wire are respectively

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Answer: (a)

  1. Third overtone == fourth harmonic, so the wire forms 4 loops.
  2. 4 loops give 4 antinodes and 4+1=54 + 1 = 5 nodes.
  3. So the answer is (a) 4,54, 5.
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Q224MHT CET 2026 · 13 APR · SHIFT 1Easy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A sonometer wire is vibrating in third overtone. There are

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Answer: (a)

  1. Third overtone == fourth harmonic, so the wire forms 4 loops.
  2. 4 loops give 5 nodes and 4 antinodes.
  3. So the answer is (a).
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Q225MHT CET 2026 · 15 MAY · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Laws of a vibrating string

A uniform wire of length LL, diameter DD and density ρ\rho is stretched under tension TT. The relation between its fundamental frequency ff, length LL and diameter DD is

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Answer: (a)

  1. f=12LTμf = \dfrac{1}{2L}\sqrt{\dfrac{T}{\mu}} with μ=ρ⋅πD24\mu = \rho \cdot \dfrac{\pi D^2}{4}.
  2. f=12L4TπρD2=1LDTπρf = \dfrac{1}{2L}\sqrt{\dfrac{4T}{\pi \rho D^2}} = \dfrac{1}{LD}\sqrt{\dfrac{T}{\pi\rho}}.
  3. For fixed TT and ρ\rho: f∝1LDf \propto \dfrac{1}{LD}.
  4. So the answer is (a) f∝1LDf \propto \frac{1}{LD}.
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Q226MHT CET 2026 · 15 APR · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Laws of a vibrating string

To increase the frequency of transverse oscillations of a stretched string by 40%, the tension must be increased by

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Answer: (c)

  1. f∝T⇒T2T1=(f2f1)2f \propto \sqrt{T} \Rightarrow \dfrac{T_2}{T_1} = \left(\dfrac{f_2}{f_1}\right)^2.
  2. T2T1=(1.4)2=1.96\dfrac{T_2}{T_1} = (1.4)^2 = 1.96.
  3. Increase =96%= 96\%.
  4. So the answer is (c) 96%96\%.
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Q227MHT CET 2026 · 13 MAY · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Bridges, segments and composite wires

A stretched wire of length 110110 cm is divided in to 3 segments whose frequencies are in the ratio 1:2:31:2:3. Their respective lengths must be

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Answer: (b)

  1. Same wire and tension: f∝1lf \propto \dfrac{1}{l}, so l1:l2:l3=1:12:13=6:3:2l_1 : l_2 : l_3 = 1 : \dfrac{1}{2} : \dfrac{1}{3} = 6 : 3 : 2.
  2. Total parts =11= 11, each part =11011=10 cm= \dfrac{110}{11} = 10\text{ cm}.
  3. Lengths: 60,30,20 cm60, 30, 20\text{ cm}.
  4. So the answer is (b) 6060 cm, 3030 cm, 2020 cm.
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Q228MHT CET 2026 · 13 MAY · SHIFT 2Medium

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A spring of mass 0.20.2 kg/m has length l=0.6l = 0.6 m. It is fixed at both ends and stretched such that is has a tension 8080 N. The string vibrates in three segments with amplitude 0.50.5 cm. The amplitude of transverse (particle) velocity is

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Answer: (c)

  1. v=Tμ=800.2=20 m/sv = \sqrt{\dfrac{T}{\mu}} = \sqrt{\dfrac{80}{0.2}} = 20\text{ m/s}.
  2. 3 segments: L=3λ2⇒λ=0.4 mL = \dfrac{3\lambda}{2} \Rightarrow \lambda = 0.4\text{ m}, so f=200.4=50 Hzf = \dfrac{20}{0.4} = 50\text{ Hz} and ω=100π rad/s\omega = 100\pi\text{ rad/s}.
  3. Maximum particle velocity (at an antinode) =Aω=0.005×100π=0.5π≈1.57 m/s= A\omega = 0.005 \times 100\pi = 0.5\pi \approx 1.57\text{ m/s}.
  4. So the answer is (c) 1.57 m/s1.57\text{ m/s}.
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Q229MHT CET 2026 · 12 MAY · SHIFT 2Medium

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

In sonometer experiment, the string of length ′L′'L' under tension vibrates in second overtone between the two bridges. The amplitude of vibration is maximum at length

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Answer: (b)

L/6L/25L/60L
  1. Second overtone = 3rd harmonic: 3 loops, each of length L/3L/3.
  2. Antinodes lie at the middle of each loop: L6,L2,5L6\dfrac{L}{6}, \dfrac{L}{2}, \dfrac{5L}{6}.
  3. So the answer is (b) L6,L2,5L6\frac{L}{6}, \frac{L}{2}, \frac{5L}{6}.
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Q230MHT CET 2026 · 18 APR · SHIFT 2Medium

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A wire of length 'L' and linear density 'm' is stretched between two rigid supports with tension 'T'. It is observed that wire resonates in the PthP^{th} harmonic at a frequency of 320 Hz and resonates again at next higher frequency of 400 Hz in two successive modes. The value of 'P' is

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Answer: (b)

  1. For a string fixed at both ends, np=p n1n_p = p\,n_1, so two successive harmonics differ by n1n_1.
  2. n1=400−320=80 Hzn_1 = 400 - 320 = 80\text{ Hz}
  3. p=32080=4p = \dfrac{320}{80} = 4
  4. So the answer is (b) 44.
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Q231MHT CET 2026 · 20 MAY · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

Two vibrating metal wires of the same material of length 'L' and '3L' and have radii '2r' and 'r' respectively. They are stretched under same tension. Both the wires vibrate in their fundamental modes. The ratio n1n2\frac{n_1}{n_2} is [n1n_1 and n2n_2 are the frequencies of first and second wire respectively]

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Answer: (b)

  1. n=12LTπr2ρ⇒n∝1Lrn = \dfrac{1}{2L}\sqrt{\dfrac{T}{\pi r^2\rho}} \Rightarrow n \propto \dfrac{1}{Lr} for same TT and material.
  2. n1n2=L2r2L1r1=3L⋅rL⋅2r=32\dfrac{n_1}{n_2} = \dfrac{L_2 r_2}{L_1 r_1} = \dfrac{3L \cdot r}{L \cdot 2r} = \dfrac{3}{2}
  3. So the answer is (b) 1.5:11.5:1.
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Q232MHT CET 2026 · 14 MAY · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

Two uniform strings A and B made of steel are vibrating under the same tension. If the first overtone of A is equal to the second overtone of B and if the radius of A is twice that of B, the ratio of the lengths of the strings is

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Answer: (d)

  1. First overtone =2n= 2n, second overtone =3n= 3n, and n∝1Lrn \propto \dfrac{1}{Lr} (same TT, same material).
  2. 2LArA=3LBrB\dfrac{2}{L_A r_A} = \dfrac{3}{L_B r_B}
  3. LALB=2rB3rA=23×2=13\dfrac{L_A}{L_B} = \dfrac{2 r_B}{3 r_A} = \dfrac{2}{3\times2} = \dfrac{1}{3}
  4. So the answer is (d) 1:31:3.
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Q233MHT CET 2026 · 20 APR · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

A wire of length 'LL', diameter 'dd', density of material 'ρ\rho' is under tension 'TT' has fundamental frequency of vibration 'nAn_A'. Another wire of length '2L2L', diameter '3d3d', density of material '2ρ2\rho' is vibrated under tension '2T2T', the fundamental frequency of vibration becomes 'nBn_B'. The ratio nB:nAn_B : n_A is

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Answer: (c)

  1. n=1LdTπρ⇒n∝1LdTρn = \dfrac{1}{Ld}\sqrt{\dfrac{T}{\pi\rho}} \Rightarrow n \propto \dfrac{1}{Ld}\sqrt{\dfrac{T}{\rho}}
  2. nBnA=L⋅d2L⋅3d2T/2ρT/ρ=16\dfrac{n_B}{n_A} = \dfrac{L \cdot d}{2L \cdot 3d}\sqrt{\dfrac{2T/2\rho}{T/\rho}} = \dfrac{1}{6}
  3. So the answer is (c) 1:61:6.
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Q234MHT CET 2026 · 15 APR · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

The fundamental frequency of sonometer wire is 5050 Hz for some length and tension. If the length is increased by 25%25\% by keeping the tension same, then the frequency change of second harmonic is

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Answer: (b)

  1. For fixed tension, every harmonic ∝1L\propto \dfrac{1}{L}.
  2. L′=1.25L⇒n′=n1.25=0.8nL' = 1.25L \Rightarrow n' = \dfrac{n}{1.25} = 0.8n
  3. Second harmonic goes from 100 Hz100\text{ Hz} to 80 Hz80\text{ Hz}: a 20%20\% decrease.
  4. So the answer is (b) decrease by 20%20\%.
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Q235MHT CET 2026 · 11 APR · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

Two uniform wires of same material are vibrating under the same tension. If the first overtone of the first wire is equal to the second overtone of the second wire and radius of first wire is twice the radius of second wire then the ratio of length of first to second wire is

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Answer: (b)

  1. n∝1Lrn \propto \dfrac{1}{Lr} (same TT, same material); first overtone =2n1= 2n_1, second overtone =3n2= 3n_2.
  2. 2L1r1=3L2r2\dfrac{2}{L_1 r_1} = \dfrac{3}{L_2 r_2}
  3. L1L2=2r23r1=23×2=13\dfrac{L_1}{L_2} = \dfrac{2 r_2}{3 r_1} = \dfrac{2}{3\times2} = \dfrac{1}{3}
  4. So the answer is (b) 13\dfrac{1}{3}.
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Q236MHT CET 2026 · 19 MAY · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

A sonometer wire resonates with a given tuning fork, forming standing waves with five antinodes between the two bridges, when a mass of 99 kg is suspended from the wire. When this mass is replaced by mass MM, the wire resonates with the same tuning fork, forming three antinodes for the same positions of the bridges. The value of MM (in kg) is

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Answer: (d)

  1. With pp loops: n=p2LMgμn = \dfrac{p}{2L}\sqrt{\dfrac{Mg}{\mu}}. Same nn, LL, μ\mu gives p2M=constantp^2 M = \text{constant}.
  2. 5 antinodes means p=5p = 5; 3 antinodes means p=3p = 3.
  3. 25×9=9×M⇒M=25 kg25 \times 9 = 9 \times M \Rightarrow M = 25\text{ kg}
  4. So the answer is (d) 2525.
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Q237MHT CET 2026 · 12 MAY · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

A sonometer wire resonates with a given tuning fork forming standing wave with 55 antinodes between two bridges when mass of 99 kg is suspended from the wire. When mass MM is suspended from the wire with same fork and same length between two bridges, 33 antinodes are formed. Mass MM is

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Answer: (d)

  1. Same fork and length: n=p2LMgμ⇒p2M=constantn = \dfrac{p}{2L}\sqrt{\dfrac{Mg}{\mu}} \Rightarrow p^2 M = \text{constant}.
  2. 52×9=32×M⇒M=25 kg5^2 \times 9 = 3^2 \times M \Rightarrow M = 25\text{ kg}
  3. So the answer is (d) 2525 kg.
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Q238MHT CET 2026 · 17 APR · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

In a sonometer experiment, the fundamental frequency of vibration of wire is 'n1n_1' when wire is stretched by hanging a metal bob. If the bob is completely immersed in water, the frequency of vibration of wire becomes 'n2n_2'. The relative density of the metal of the bob is

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Answer: (c)

  1. n∝Tn \propto \sqrt{T}. In air T1=VρgT_1 = V\rho g; in water T2=V(ρ−ρw)gT_2 = V(\rho - \rho_w)g.
  2. n22n12=ρ−ρwρ=d−1d\dfrac{n_2^2}{n_1^2} = \dfrac{\rho - \rho_w}{\rho} = \dfrac{d-1}{d}, where dd is the relative density.
  3. d=n12n12−n22d = \dfrac{n_1^2}{n_1^2 - n_2^2}
  4. So the answer is (c).
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Q239MHT CET 2026 · 15 APR · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

A sonometer wire resonates with 44 antinodes between the two bridges for a given tuning fork when 11 kg mass is suspended from the wire. Using same fork, when mass M is suspended, the wire resonates producing 22 antinodes between the two bridges. (Distance between the bridges as before) The value of M is

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Answer: (c)

  1. Same fork and length: n=p2LMgμ⇒p2M=constantn = \dfrac{p}{2L}\sqrt{\dfrac{Mg}{\mu}} \Rightarrow p^2 M = \text{constant}.
  2. 42×1=22×M⇒M=4 kg4^2 \times 1 = 2^2 \times M \Rightarrow M = 4\text{ kg}
  3. So the answer is (c) 44 kg.
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Q240MHT CET 2025 · 22 APR · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Nodes, antinodes and properties

Two waves of same frequency ( n) are approaching each other with same velocity 12 m/s12\text{ m/s} along the same linear path and interfere. The distance between two consecutive nodes is

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Answer: (d)

  1. λ=vn=12n\lambda = \frac{v}{n} = \frac{12}{n}.
  2. Consecutive nodes are λ2=6n\frac{\lambda}{2} = \frac{6}{n} apart.
  3. So the answer is (d) 6n\frac{6}{n}.
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Q241MHT CET 2025 · 26 APR · SHIFT 1Easy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

In Sonometer experiment, the frequency of a tuning fork used is 288 Hz. Harmonics will 'NOT' be produced at the frequency

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Answer: (c)

  1. A sonometer wire resonates only at integer multiples of the fork frequency: fp=p×288 Hzf_p = p \times 288\text{ Hz}.
  2. p=1,2,3⇒288,576,864 Hzp = 1, 2, 3 \Rightarrow 288, 576, 864\text{ Hz}.
  3. 844/288≈2.93844/288 \approx 2.93 is not an integer.
  4. So the answer is (c) 844 Hz844\text{ Hz}.
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Q242MHT CET 2025 · 19 APR · SHIFT 2Easy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

The frequency of a tuning fork is 256 Hz. It will not resonate with the tuning fork of frequency

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Answer: (c)

  1. Resonance (harmonics) occurs only at integer multiples of 256 Hz256\text{ Hz}.
  2. 256×1=256256 \times 1 = 256, 256×2=512256 \times 2 = 512, 256×3=768 Hz256 \times 3 = 768\text{ Hz}.
  3. 754/256754/256 is not an integer.
  4. So the answer is (c) 754 Hz754\text{ Hz}.
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Q243MHT CET 2025 · 26 APR · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Laws of a vibrating string

Fundamental frequency of sonometer wire is ' nn '. If the tension and length are increased 3 times and diameter is increased twice, the new frequency will be

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Answer: (c)

  1. n=1LDTπρ⇒n∝TLDn = \dfrac{1}{LD}\sqrt{\dfrac{T}{\pi\rho}} \Rightarrow n \propto \dfrac{\sqrt{T}}{LD}.
  2. n′n=33×2=123\dfrac{n'}{n} = \dfrac{\sqrt{3}}{3 \times 2} = \dfrac{1}{2\sqrt{3}}.
  3. So the answer is (c) n23\frac{n}{2\sqrt{3}}.
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Q244MHT CET 2025 · 23 APR · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Laws of a vibrating string

The fundamental frequency of sonometer wire is ' nn '. If the tension and length are increased 3 times and diameter is increased twice, the new frequency will be

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Answer: (c)

  1. n=1LDTπρ⇒n∝TLDn = \dfrac{1}{LD}\sqrt{\dfrac{T}{\pi\rho}} \Rightarrow n \propto \dfrac{\sqrt{T}}{LD}.
  2. n′n=33×2=123\dfrac{n'}{n} = \dfrac{\sqrt{3}}{3 \times 2} = \dfrac{1}{2\sqrt{3}}.
  3. So the answer is (c) n23\frac{n}{2\sqrt{3}}.
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Q245MHT CET 2025 · 19 APR · SHIFT 1Medium

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A string of mass per unit length 0.1 kg m−10.1\text{ kg m}^{-1} has length 0.9 m. It is fixed at both ends and stretched such that it has a tension of 40 N. The string vibrates in three segments with amplitude 0.3 cm. The amplitude (maximum) of the particle velocity is (in m/s\text{m/s})

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Answer: (c)

  1. Wave speed v=T/μ=40/0.1=20 m/sv = \sqrt{T/\mu} = \sqrt{40/0.1} = 20\text{ m/s}.
  2. Three segments: 3λ2=0.9⇒λ=0.6 m3\dfrac{\lambda}{2} = 0.9 \Rightarrow \lambda = 0.6\text{ m}, so n=vλ=1003 Hzn = \dfrac{v}{\lambda} = \dfrac{100}{3}\text{ Hz}.
  3. ω=2πn=200π3 rad/s\omega = 2\pi n = \dfrac{200\pi}{3}\text{ rad/s}
  4. vmax=Aω=0.003×200π3=0.2π=π5 m/sv_{max} = A\omega = 0.003 \times \dfrac{200\pi}{3} = 0.2\pi = \dfrac{\pi}{5}\text{ m/s}
  5. So the answer is (c) π5\dfrac{\pi}{5}.
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Q246MHT CET 2025 · 22 APR · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

The fundamental frequency of a sonometer wire is 50 Hz for some length and tension. If the length is increased by 25%25\% by keeping tension same then frequency change of second harmonic is

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Answer: (b)

  1. At constant tension, all harmonics ∝1L\propto \dfrac{1}{L}.
  2. L′=1.25L⇒n′=0.8nL' = 1.25L \Rightarrow n' = 0.8n: second harmonic 100 Hz→80 Hz100\text{ Hz} \to 80\text{ Hz}.
  3. So the answer is (b) decreased by 20%20\%.
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Q247MHT CET 2025 · 21 APR · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

Two uniform wires of same material are vibrating under the same tension. If the 11st overtone of 11st wire is equal to the 22nd overtone of 22nd wire and radius of 11st wire is twice the radius of 22nd wire, the ratio of length of 11st wire to that 22nd wire is

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Answer: (a)

  1. n∝1Lrn \propto \dfrac{1}{Lr}; first overtone =2n1= 2n_1, second overtone =3n2= 3n_2.
  2. 2L1r1=3L2r2⇒L1L2=2r23r1=26\dfrac{2}{L_1 r_1} = \dfrac{3}{L_2 r_2} \Rightarrow \dfrac{L_1}{L_2} = \dfrac{2r_2}{3r_1} = \dfrac{2}{6}
  3. So the answer is (a) 1:31:3.
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Q248MHT CET 2025 · 20 APR · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

A wire of length L, diameter ' d ' density of material ' e ' is under tension ' T ', having fundamental frequency of vibration nAn_A. Another wire of length 2 L, tension 2 T, density 2 e and diameter 3 d has fundamental frequency of vibration nBn_B. The ratio nB:nAn_B : n_A is

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Answer: (c)

  1. n=1LdTπe⇒n∝1LdTen = \dfrac{1}{Ld}\sqrt{\dfrac{T}{\pi e}} \Rightarrow n \propto \dfrac{1}{Ld}\sqrt{\dfrac{T}{e}}
  2. nBnA=12×322=16\dfrac{n_B}{n_A} = \dfrac{1}{2\times3}\sqrt{\dfrac{2}{2}} = \dfrac{1}{6}
  3. So the answer is (c) 1:61:6.
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Q249MHT CET 2025 · 25 APR · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

At poles, a stretched wire of a given length vibrates in unison with a tuning fork. At the equator, for same setting, to produce resonance with same fork, the vibrating length of wire

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Answer: (a)

  1. gg is smaller at the equator, so the tension T=MgT = Mg and the wave speed v=T/μv = \sqrt{T/\mu} decrease.
  2. For the same frequency n=v2Ln = \dfrac{v}{2L}, LL must decrease along with vv.
  3. So the answer is (a) should be decreased.
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Q250MHT CET 2024 · 4 MAY · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Stationary wave equation

A stationery wave is represented by y=12cos⁡(π6x)sin⁡(8πt)y = 12\cos\left(\frac{\pi}{6}x\right)\sin(8\pi t), where x & yx \,\&\, y are in cm and tt in second. The distance between two successive antinodes is

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Answer: (c)

  1. k=π6=2πλ⇒λ=12 cmk = \frac{\pi}{6} = \frac{2\pi}{\lambda} \Rightarrow \lambda = 12\text{ cm}.
  2. Successive antinodes are λ2=6 cm\frac{\lambda}{2} = 6\text{ cm} apart.
  3. So the answer is (c) 6 cm.
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Q251MHT CET 2024 · 10 MAY · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Nodes, antinodes and properties

When the string is stretched between two rigid supports, under certain tension and vibrated

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Answer: (b)

  1. Rigid supports cannot move, so both ends are nodes.
  2. Even the fundamental mode has one antinode in the middle.
  3. So the answer is (b).
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Q252MHT CET 2024 · 2 MAY · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Nodes, antinodes and properties

In a vibrating string with fixed ends the waves are of type

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Answer: (b)

  1. Particles of the string vibrate perpendicular to its length: transverse.
  2. Waves reflected from the fixed ends superpose to form a stationary pattern.
  3. So the answer is (b) stationary transverse.
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Q253MHT CET 2024 · 15 MAY · SHIFT 1Easy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

When a sonometer wire vibrates in third overtone there are

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Answer: (c)

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  1. Third overtone = 4th harmonic, so the wire forms p=4p = 4 loops.
  2. For a wire fixed at both ends: nodes =p+1= p + 1, antinodes =p= p.
  3. Nodes =5= 5, antinodes =4= 4.
  4. So the answer is (c) 5 nodes and 4 antinodes.
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Q254MHT CET 2024 · 10 MAY · SHIFT 2Easy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

Stationary wave is produced along the stretched string of length 80 cm. The resonant frequencies of string are 90 Hz,150 Hz90\text{ Hz}, 150\text{ Hz} and 210 Hz. The speed of transverse wave in the string is

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Answer: (c)

  1. The given frequencies 90,150,210 Hz90, 150, 210\text{ Hz} are all multiples of 30 Hz30\text{ Hz} (their HCF), so take the fundamental f0=30 Hzf_0 = 30\text{ Hz}.
  2. For a string fixed at both ends, f0=v2Lf_0 = \dfrac{v}{2L}, so v=2Lf0v = 2Lf_0.
  3. v=2×0.80×30=48 m/sv = 2 \times 0.80 \times 30 = 48\text{ m/s}.
  4. So the answer is (c) 48 m/s48\text{ m/s}.
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Q255MHT CET 2024 · 9 MAY · SHIFT 2Easy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A stationary wave is formed having 3 nodes along the length of the string 90 cm. The wavelength of the wave is

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Answer: (c)

  1. 3 nodes on a string means 2 loops; each loop is λ/2\lambda/2.
  2. L=2×λ2=λL = 2 \times \dfrac{\lambda}{2} = \lambda.
  3. λ=90 cm\lambda = 90\text{ cm}.
  4. So the answer is (c) 90 cm90\text{ cm}.
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Q256MHT CET 2024 · 2 MAY · SHIFT 2Easy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A stretched string is fixed at both ends. It is made to vibrate so that the total number of nodes formed in it is ' xx '. The length of the string in terms of the wavelength of waves formed in it is ( λ=\lambda = wavelength ))

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Answer: (d)

  1. With both ends fixed, xx nodes give (x−1)(x - 1) loops.
  2. Each loop has length λ/2\lambda/2.
  3. L=(x−1)λ2L = (x - 1)\dfrac{\lambda}{2}.
  4. So the answer is (d) (X−1)λ2(X - 1)\frac{\lambda}{2}.
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Q257MHT CET 2024 · 9 MAY · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Laws of a vibrating string

When the tension in string is increased by 3 kg wt3\text{ kg wt}, the frequency of the fundamental mode increases in the ratio 2:32:3. The initial tension in the string is

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Answer: (c)

  1. f∝Tf \propto \sqrt{T}: TT+3=23\sqrt{\dfrac{T}{T + 3}} = \dfrac{2}{3}.
  2. TT+3=49⇒9T=4T+12\dfrac{T}{T + 3} = \dfrac{4}{9} \Rightarrow 9T = 4T + 12.
  3. T=2.4 kg wtT = 2.4\text{ kg wt}.
  4. So the answer is (c) 2.4 kg wt2.4\text{ kg wt}.
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Q258MHT CET 2024 · 3 MAY · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Laws of a vibrating string

A violin emits sound waves of frequency ' n1n_1 ' under tension T. When tension is increased by 44%44\%, keeping the length and mass per unit length constant, frequency of sound waves becomes ' n2n_2 '. The ratio of frequency ' n2n_2 ' to frequency ' n1n_1 ' is

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Answer: (c)

  1. With LL and μ\mu fixed, n∝Tn \propto \sqrt{T}.
  2. n2n1=1.44=1.2=65\dfrac{n_2}{n_1} = \sqrt{1.44} = 1.2 = \dfrac{6}{5}.
  3. So the answer is (c) 6:56:5.
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Q259JEE Main 2024 · 5 APR · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Laws of a vibrating string

A sonometer wire of resonating length 90 cm90\text{ cm} has a fundamental frequency of 400 Hz400\text{ Hz} when kept under some tension. The resonating length of the wire with fundamental frequency of 600 Hz600\text{ Hz} under same tension _______ cm\text{cm}.

Numerical answer type. Work it out, then open the answer.

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Answer: 60

  1. Same tension and wire: f∝1Lf \propto \dfrac{1}{L}.
  2. L2=90×400600=60 cmL_2 = 90 \times \dfrac{400}{600} = 60\text{ cm}.
  3. So the resonating length is 60 cm60\text{ cm}.
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Q260MHT CET 2024 · 10 MAY · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Bridges, segments and composite wires

The length of a sonometer wire 'AB' is 110 cm. Where should the two bridges be placed from end ' AA ' to divide the wire in three segments whose fundamental frequencies are in the ratio 1:2:31:2:3?

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Answer: (a)

  1. f∝1lf \propto \dfrac{1}{l}: l1:l2:l3=1:12:13=6:3:2l_1 : l_2 : l_3 = 1 : \dfrac{1}{2} : \dfrac{1}{3} = 6 : 3 : 2.
  2. Each part =11011=10 cm⇒60,30,20 cm= \dfrac{110}{11} = 10\text{ cm} \Rightarrow 60, 30, 20\text{ cm}.
  3. Bridges from A at 60 cm60\text{ cm} and 60+30=90 cm60 + 30 = 90\text{ cm}.
  4. So the answer is (a) 60 cm and 90 cm.
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Q261MHT CET 2024 · 15 MAY · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Stationary wave equation

Two progressive waves Y1=sin⁡2π(t0.4−x4)Y_1 = \sin 2\pi\left(\frac{t}{0.4} - \frac{x}{4}\right) and Y2=sin⁡2π(t0.4+x4)Y_2 = \sin 2\pi\left(\frac{t}{0.4} + \frac{x}{4}\right) superpose to form a standing wave. ' xx ' and ' yy ' are in SI system. Amplitude of the particle at x=0.5 mx = 0.5\text{ m} is [sin⁡45∘=cos⁡45∘=12]\left[\sin 45^\circ = \cos 45^\circ = \frac{1}{\sqrt{2}}\right]

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Answer: (c)

  1. sin⁡(A−B)+sin⁡(A+B)=2sin⁡Acos⁡B\sin(A - B) + \sin(A + B) = 2\sin A\cos B, so Y=2cos⁡(2πx4)sin⁡(2πt0.4)Y = 2\cos\left(\dfrac{2\pi x}{4}\right)\sin\left(\dfrac{2\pi t}{0.4}\right).
  2. Amplitude at xx: A(x)=2cos⁡(πx2)A(x) = 2\cos\left(\dfrac{\pi x}{2}\right).
  3. At x=0.5 mx = 0.5\text{ m}: A=2cos⁡45∘=2×12=2 mA = 2\cos 45^\circ = 2 \times \dfrac{1}{\sqrt{2}} = \sqrt{2}\text{ m}.
  4. So the answer is (c) 2 m\sqrt{2}\text{ m}.
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Q262MHT CET 2024 · 16 MAY · SHIFT 1Medium

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A string is under tension of 180 N and mass per unit length 2×10−3 kg/m2 \times 10^{-3}\text{ kg/m}. It produces two consecutive resonant frequencies with a tuning fork, which are 375 Hz and 450 Hz. The mass of the string is

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Answer: (d)

  1. Consecutive resonant frequencies differ by the fundamental: n1=450−375=75 Hzn_1 = 450 - 375 = 75\text{ Hz}.
  2. v=T/μ=1802×10−3=300 m/sv = \sqrt{T/\mu} = \sqrt{\dfrac{180}{2\times10^{-3}}} = 300\text{ m/s}
  3. L=v2n1=300150=2 mL = \dfrac{v}{2n_1} = \dfrac{300}{150} = 2\text{ m}
  4. Mass =μL=2×10−3×2=4×10−3 kg=4 g= \mu L = 2\times10^{-3}\times 2 = 4\times10^{-3}\text{ kg} = 4\text{ g}
  5. So the answer is (d) 4 gram.
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Q263MHT CET 2024 · 11 MAY · SHIFT 2Medium

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A wire of length ' LL ' and linear density ' mm ' is stretched between two rigid supports with tension ' TT '. It is observed that wire resonates in the PPth harmonic at a frequency of 320 Hz and resonates again at next higher frequency of 400 Hz. The value of ' pp ' is

Show answer and solution

Answer: (b)

  1. Successive harmonics of a string differ by the fundamental: n1=400−320=80 Hzn_1 = 400 - 320 = 80\text{ Hz}.
  2. p=32080=4p = \dfrac{320}{80} = 4
  3. So the answer is (b) 4.
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Q264MHT CET 2024 · 16 MAY · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

Two uniform strings A and B made of steel are made to vibrate under the same tension. If first overtone of A is equal to the second overtone of BB and if the radius of AA is twice that of BB, the ratio of the length of string BB to that of AA is

Show answer and solution

Answer: (d)

  1. n∝1Lrn \propto \dfrac{1}{Lr}; first overtone of A =2nA= 2n_A, second overtone of B =3nB= 3n_B.
  2. 2LArA=3LBrB⇒LBLA=3rA2rB=3×22=3\dfrac{2}{L_A r_A} = \dfrac{3}{L_B r_B} \Rightarrow \dfrac{L_B}{L_A} = \dfrac{3 r_A}{2 r_B} = \dfrac{3\times2}{2} = 3
  3. So the answer is (d) 3:13:1.
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Q265MHT CET 2024 · 4 MAY · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

A string A has twice the length, twice the diameter, twice the tension and twice the density of another string B. The overtone of A which will have the same fundamental frequency as that of BB is

Show answer and solution

Answer: (c)

  1. n∝1LDTρn \propto \dfrac{1}{LD}\sqrt{\dfrac{T}{\rho}}
  2. nAnB=12×222=14⇒nB=4nA\dfrac{n_A}{n_B} = \dfrac{1}{2\times2}\sqrt{\dfrac{2}{2}} = \dfrac{1}{4} \Rightarrow n_B = 4n_A
  3. The 4th harmonic of A equals nBn_B; the 4th harmonic is the third overtone.
  4. So the answer is (c) third.
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Q266MHT CET 2024 · 11 MAY · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

At the poles of earth, a stretched wire of a given length vibrates in unison with a tuning fork. At the equator of earth, for same setting, to produce resonance with same fork, the vibrating length of wire

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Answer: (a)

  1. gequator<gpoleg_{equator} < g_{pole}, so T=MgT = Mg and v=T/μv = \sqrt{T/\mu} are smaller at the equator.
  2. To keep n=v2Ln = \dfrac{v}{2L} unchanged, LL must be reduced.
  3. So the answer is (a) should be decreased.
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Q267MHT CET 2024 · 9 MAY · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

A sonometer wire is in unison with a tuning fork of frequency ' nn ' when it is stretched by a weight of specific gravity ' dd '. When the weight is completely immersed in water, ' xx ' beats are produced per second, then

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Answer: (b)

  1. In water the tension falls to Td−1dT\dfrac{d-1}{d}, so the frequency drops to n−xn - x (that gives xx beats with the fork).
  2. n∝T⇒n−xn=d−1dn \propto \sqrt{T} \Rightarrow \dfrac{n-x}{n} = \sqrt{\dfrac{d-1}{d}}
  3. nn−x=dd−1\dfrac{n}{n-x} = \sqrt{\dfrac{d}{d-1}}
  4. So the answer is (b).
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Q268MHT CET 2024 · 9 MAY · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

A sonometer wire is stretched by hanging a metal bob, the fundamental frequency of the wire is ' n1n_1 '. When the bob is completely immersed in water, the frequency of vibration of wire becomes ' n2n_2 '. The relative density of the metal of the bob is

Show answer and solution

Answer: (c)

  1. n∝Tn \propto \sqrt{T}; T1=VρgT_1 = V\rho g in air, T2=V(ρ−ρw)gT_2 = V(\rho - \rho_w)g in water.
  2. n22n12=d−1d⇒d=n12n12−n22\dfrac{n_2^2}{n_1^2} = \dfrac{d-1}{d} \Rightarrow d = \dfrac{n_1^2}{n_1^2 - n_2^2}
  3. So the answer is (c).
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Q269MHT CET 2024 · 2 MAY · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

A sonometer wire is stretched by hanging a metal bob. The fundamental frequency of vibration of wire is ' n1n_1 '. When the bob is completely immersed in water, the frequency of vibration of wire becomes ' n2n_2 '. The relative density of the metal of the bob is

Show answer and solution

Answer: (c)

  1. n∝Tn \propto \sqrt{T}; the buoyant force reduces tension from VρgV\rho g to V(ρ−ρw)gV(\rho - \rho_w)g.
  2. n22n12=d−1d⇒d=n12n12−n22\dfrac{n_2^2}{n_1^2} = \dfrac{d-1}{d} \Rightarrow d = \dfrac{n_1^2}{n_1^2 - n_2^2}
  3. So the answer is (c).
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Q270MHT CET 2023 · 11 MAY · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Nodes, antinodes and properties

Two progressive waves are travelling towards each other with velocity 50 m/s50\text{ m/s} and frequency 200 Hz200\text{ Hz}. The distance between the two consecutive antinodes is

Show answer and solution

Answer: (a)

  1. λ=vn=50200=0.25 m\lambda = \frac{v}{n} = \frac{50}{200} = 0.25\text{ m}.
  2. Consecutive antinodes are λ2=0.125 m\frac{\lambda}{2} = 0.125\text{ m} apart.
  3. So the answer is (a) 0.125 m0.125\text{ m}.
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Q271MHT CET 2023 · 11 MAY · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Nodes, antinodes and properties

A string fixed at both the ends forms standing wave with node separation of 5 cm5\text{ cm}. If the velocity of the wave on the string is 2 m/s2\text{ m/s}, then the frequency of vibration of the string is

Show answer and solution

Answer: (c)

  1. Node separation λ2=5 cm⇒λ=0.1 m\frac{\lambda}{2} = 5\text{ cm} \Rightarrow \lambda = 0.1\text{ m}.
  2. n=vλ=20.1=20 Hzn = \frac{v}{\lambda} = \frac{2}{0.1} = 20\text{ Hz}.
  3. So the answer is (c) 20 Hz.
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Q272MHT CET 2023 · 10 MAY · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Nodes, antinodes and properties

In case of a stationary wave pattern which of the following statements is CORRECT?

Show answer and solution

Answer: (d)

  1. (a) Consecutive nodes are λ2\frac{\lambda}{2} apart: false.
  2. (b) A pipe open at both ends gives all harmonics: false.
  3. (c) A closed pipe gives only odd harmonics: false.
  4. (d) For a string the first overtone is the second harmonic: true.
  5. So the answer is (d).
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Q273MHT CET 2023 · 9 MAY · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Nodes, antinodes and properties

Stationary waves can be produced in

Show answer and solution

Answer: (d)

  1. Stationary waves form wherever two identical waves travel in opposite directions, transverse or longitudinal.
  2. Examples: strings and rods (solid), water surface (liquid), air columns (gas).
  3. So the answer is (d).
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Q274JEE Main 2023 · 8 APR · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Laws of a vibrating string

A guitar string of length 90 cm vibrates with a fundamental frequency of 120 Hz. The length of the string producing a fundamental frequency of 180 Hz will be _________ cm.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 60

  1. Same string and tension: f∝1Lf \propto \dfrac{1}{L}.
  2. L2=90×120180=60 cmL_2 = 90 \times \dfrac{120}{180} = 60\text{ cm}.
  3. So the length is 60 cm60\text{ cm}.
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Q275MHT CET 2023 · 9 MAY · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Bridges, segments and composite wires

When a string of length 'll' is divided into three segments of length l1,l2l_1, l_2 and l3l_3. The fundamental frequencies of three segments are n1,n2n_1, n_2 and n3n_3 respectively. The original fundamental frequency 'nn' of the string is

Show answer and solution

Answer: (c)

  1. Same tension and μ\mu: n=kln = \dfrac{k}{l}, so l=knl = \dfrac{k}{n}.
  2. l=l1+l2+l3⇒kn=kn1+kn2+kn3l = l_1 + l_2 + l_3 \Rightarrow \dfrac{k}{n} = \dfrac{k}{n_1} + \dfrac{k}{n_2} + \dfrac{k}{n_3}.
  3. 1n=1n1+1n2+1n3\dfrac{1}{n} = \dfrac{1}{n_1} + \dfrac{1}{n_2} + \dfrac{1}{n_3}.
  4. So the answer is (c).
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Q276MHT CET 2023 · 14 MAY · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Nodes, antinodes and properties

Sound waves of frequency 600 Hz600\text{ Hz} fall normally on a perfectly reflecting wall. The shortest distance from the wall at which all particles will have maximum amplitude of vibration is (speed of sound =300 m s−1= 300\text{ m s}^{-1})

Show answer and solution

Answer: (b)

  1. λ=vf=300600=0.5 m\lambda = \dfrac{v}{f} = \dfrac{300}{600} = 0.5\text{ m}.
  2. A rigid wall is a displacement node; the nearest displacement antinode (maximum amplitude) is λ/4\lambda/4 away.
  3. d=0.54=18 md = \dfrac{0.5}{4} = \dfrac{1}{8}\text{ m}.
  4. So the answer is (b) 18 m\frac{1}{8}\text{ m}.
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Q277MHT CET 2023 · 14 MAY · SHIFT 1Medium

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A string is stretched between two rigid supports separated by 75 cm75\text{ cm}. There are no resonant frequencies between 420 Hz420\text{ Hz} and 315 Hz315\text{ Hz}. The lowest resonant frequency for the string is

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Answer: (c)

  1. No resonance between them, so 315 Hz and 420 Hz are consecutive harmonics.
  2. Difference of consecutive harmonics = fundamental: n1=420−315=105 Hzn_1 = 420 - 315 = 105\text{ Hz}.
  3. So the answer is (c) 105 Hz105\text{ Hz}.
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Q278JEE Main 2023 · 15 APR · SHIFT 1Medium

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

The fundamental frequency of vibration of a string stretched between two rigid supports is 50 Hz50\text{ Hz}. The mass of the string is 18 g18\text{ g} and its linear mass density is 20 g/m20\text{ g/m}. The speed of the transverse waves so produced in the string is ___________ m s−1\text{m s}^{-1}

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 90

  1. Length L=mμ=1820=0.9 mL = \dfrac{m}{\mu} = \dfrac{18}{20} = 0.9\text{ m}.
  2. Fundamental: n=v2L⇒v=2Ln=2×0.9×50n = \dfrac{v}{2L} \Rightarrow v = 2Ln = 2\times0.9\times50
  3. v=90 m/sv = 90\text{ m/s}
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Q279MHT CET 2023 · 12 MAY · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

A uniform string is vibrating with a fundamental frequency 'nn'. If radius and length of string both are doubled keeping tension constant then the new frequency of vibration is

Show answer and solution

Answer: (c)

  1. n=12LrTπρ⇒n∝1Lrn = \dfrac{1}{2Lr}\sqrt{\dfrac{T}{\pi\rho}} \Rightarrow n \propto \dfrac{1}{Lr} at constant TT.
  2. n′=n2×2=n4n' = \dfrac{n}{2\times2} = \dfrac{n}{4}
  3. So the answer is (c) n4\dfrac{n}{4}.
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Q280MHT CET 2023 · 11 MAY · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

A sonometer wire 'AA' of diameter 'dd' under tension 'TT' having density 'ρ1\rho_1' vibrates with fundamental frequency 'nn'. If we use another wire 'BB' which vibrates with same frequency under tension '2T2T' and diameter '2d2d' then density 'ρ2\rho_2 ' of wire 'BB' will be

Show answer and solution

Answer: (c)

  1. Same length: n∝1dTρn \propto \dfrac{1}{d}\sqrt{\dfrac{T}{\rho}}.
  2. 1dTρ1=12d2Tρ2⇒1ρ1=24ρ2\dfrac{1}{d}\sqrt{\dfrac{T}{\rho_1}} = \dfrac{1}{2d}\sqrt{\dfrac{2T}{\rho_2}} \Rightarrow \dfrac{1}{\rho_1} = \dfrac{2}{4\rho_2}
  3. ρ2=ρ12\rho_2 = \dfrac{\rho_1}{2}
  4. So the answer is (c) ρ2=ρ12\rho_2 = \dfrac{\rho_1}{2}.
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Q281MHT CET 2023 · 10 MAY · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

Two uniform wires of same material are vibrating under the same tension. If the first overtone of first wire is equal to the 22nd overtone of 22nd wire and radius of the first wire is twice the radius of the 22nd wire then the ratio of length of first wire to 22nd wire is

Show answer and solution

Answer: (a)

  1. n∝1Lrn \propto \dfrac{1}{Lr}; first overtone =2n1= 2n_1, second overtone =3n2= 3n_2.
  2. 2L1r1=3L2r2⇒L1L2=2r23r1=13\dfrac{2}{L_1 r_1} = \dfrac{3}{L_2 r_2} \Rightarrow \dfrac{L_1}{L_2} = \dfrac{2r_2}{3r_1} = \dfrac{1}{3}
  3. So the answer is (a) 1:31:3.
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Q282MHT CET 2023 · 10 MAY · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

If the length of stretched string is reduced by 40%40\% and tension is increased by 44%44\% then the ratio of final to initial frequencies of stretched string is

Show answer and solution

Answer: (a)

  1. n∝TLn \propto \dfrac{\sqrt{T}}{L}
  2. L′=0.6LL' = 0.6L, T′=1.44TT' = 1.44T: n′n=1.440.6=1.20.6=2\dfrac{n'}{n} = \dfrac{\sqrt{1.44}}{0.6} = \dfrac{1.2}{0.6} = 2
  3. So the answer is (a) 2:12:1.
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Q283JEE Main 2023 · 11 APR · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

A wire of density 8×103 kg/m38 \times 10^{3}\text{ kg/m}^3 is stretched between two clamps 0.5 m0.5\text{ m} apart. The extension developed in the wire is 3.2×10−4 m3.2 \times 10^{-4}\text{ m}. If Y=8×1010 N/m2Y = 8 \times 10^{10}\text{ N/m}^2, the fundamental frequency of vibration in the wire will be ___________ Hz\text{Hz}.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 80

  1. Stress TA=Y×strain=8×1010×3.2×10−40.5=5.12×107 N/m2\dfrac{T}{A} = Y \times \text{strain} = 8\times10^{10} \times \dfrac{3.2\times10^{-4}}{0.5} = 5.12\times10^{7}\text{ N/m}^2
  2. v=Tμ=T/Aρ=5.12×1078×103=80 m/sv = \sqrt{\dfrac{T}{\mu}} = \sqrt{\dfrac{T/A}{\rho}} = \sqrt{\dfrac{5.12\times10^7}{8\times10^3}} = 80\text{ m/s}
  3. n=v2L=802×0.5=80 Hzn = \dfrac{v}{2L} = \dfrac{80}{2\times0.5} = 80\text{ Hz}
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Q284JEE Main 2023 · 13 APR · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

In an experiment with sonometer when a mass of 180 g180\text{ g} is attached to the string, it vibrates with fundamental frequency of 30 Hz30\text{ Hz}. When a mass m\text{m} is attached, the string vibrates with fundamental frequency of 50 Hz50\text{ Hz}. The value of m\text{m} is ___________ g.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 500

  1. n∝T∝mn \propto \sqrt{T} \propto \sqrt{m} for the same string.
  2. m=180(5030)2=180×259m=180\left(\frac{50}{30}\right)^2=180\times\frac{25}{9}
  3. m=500 gm=500\text{ g}
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Q285MHT CET 2022 · 11 AUG · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Stationary wave equation

A stationary wave is represented by y=10sin⁡(πx4)cos⁡(20πt)y = 10\sin\left(\frac{\pi x}{4}\right)\cos(20\pi t) where xx and yy are in cm\text{cm} and tt in second. The distance between two consecutive nodes is

Show answer and solution

Answer: (c)

  1. k=π4=2πλ⇒λ=8 cmk = \frac{\pi}{4} = \frac{2\pi}{\lambda} \Rightarrow \lambda = 8\text{ cm}.
  2. Consecutive nodes are λ2=4 cm\frac{\lambda}{2} = 4\text{ cm} apart.
  3. So the answer is (c) 4 cm.
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Q286JEE Main 2022 · 24 JUN · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Stationary wave equation

Two travelling waves of equal amplitudes and equal frequencies move in opposite directions along a string. They interfere to produce a stationary wave whose equation is given by y=(10cos⁡πxsin⁡2πtT)y = \left(10\cos\pi x\sin\frac{2\pi t}{T}\right) cm

The amplitude of the particle at x=43x = \frac{4}{3} cm will be ___________ cm.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 5

  1. Amplitude at xx: ∣10cos⁡πx∣|10\cos\pi x|.
  2. At x=43x = \frac{4}{3}: 10∣cos⁡4π3∣=10×12=5 cm10\left|\cos\frac{4\pi}{3}\right| = 10 \times \frac{1}{2} = 5\text{ cm}.
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Q287MHT CET 2022 · 11 AUG · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Nodes, antinodes and properties

Consider the following statements about stationary waves.

A. The distance between two adjacent nodes or antinodes is equal to λ2(λ=\frac{\lambda}{2}(\lambda = wavelength of the wave)

B. A node is always formed at the open end of the open organ pipe.

Choose the correct option from the following.

Show answer and solution

Answer: (c)

  1. A: Adjacent nodes (or antinodes) are λ2\frac{\lambda}{2} apart: true.
  2. B: The open end of a pipe is always an antinode, not a node: false.
  3. So the answer is (c) only A is true.
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Q288JEE Main 2022 · 27 JUL · SHIFT 2Medium

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A wire of length 30 cm, stretched between rigid supports, has it's nth and (n + 1)th harmonics at 400 Hz and 450 Hz, respectively. If tension in the string is 2700 N, it's linear mass density is ____________ kg/m.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 3

  1. Fundamental n1=450−400=50 Hzn_1 = 450 - 400 = 50\text{ Hz}.
  2. v=2Ln1=2×0.3×50=30 m/sv = 2Ln_1 = 2\times0.3\times50 = 30\text{ m/s}
  3. μ=Tv2=2700900=3 kg/m\mu = \dfrac{T}{v^2} = \dfrac{2700}{900} = 3\text{ kg/m}
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Q289JEE Main 2021 · 26 AUG · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Stationary wave equation

Two travelling waves produce a standing wave represented by equation,

y = 1.0 mm cos(1.57 cm−1{}^{-1}) x sin(78.5 s−1{}^{-1})t.

The node closest to the origin in the region x > 0 will be at x = .............. cm.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 1

  1. Nodes where cos⁡(1.57x)=0\cos(1.57x) = 0, i.e. 1.57x=π21.57x = \frac{\pi}{2} for the first node.
  2. x=1.571.57=1 cmx = \frac{1.57}{1.57} = 1\text{ cm}.
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Q290JEE Main 2021 · 31 AUG · SHIFT 1Easy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A wire having a linear mass density 9.0 ×\times 10−-4 kg/m is stretched between two rigid supports with a tension of 900 N. The wire resonates at a frequency of 500 Hz. The next higher frequency at which the same wire resonates is 550 Hz. The length of the wire is ____________ m.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 10

  1. Wave speed v=Tμ=9009.0×10−4=106=1000 m/sv = \sqrt{\dfrac{T}{\mu}} = \sqrt{\dfrac{900}{9.0 \times 10^{-4}}} = \sqrt{10^6} = 1000\text{ m/s}.
  2. Consecutive resonances differ by f0=v2Lf_0 = \dfrac{v}{2L}: f0=550−500=50 Hzf_0 = 550 - 500 = 50\text{ Hz}.
  3. L=v2f0=10002×50=10 mL = \dfrac{v}{2f_0} = \dfrac{1000}{2 \times 50} = 10\text{ m}.
  4. So the length is 10 m10\text{ m}.
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Q291MHT CET 2021 · 24 SEP · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

The length and diameter of a metal wire used in sonometer is doubled. The fundamental frequency will change from 'n' to

Show answer and solution

Answer: (a)

  1. n=1LDTπρ⇒n∝1LDn = \dfrac{1}{LD}\sqrt{\dfrac{T}{\pi\rho}} \Rightarrow n \propto \dfrac{1}{LD}
  2. Doubling both: n′=n2×2=n4n' = \dfrac{n}{2\times2} = \dfrac{n}{4}
  3. So the answer is (a) n4\dfrac{n}{4}.
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Q292MHT CET 2021 · 22 SEP · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

A sonometer wire resonates with a given tuning fork forming standing waves with five antinodes between the two bridges when a mass of 9 kg9\text{ kg} is suspended from the wire. When this mass is replaced by a mass MM, the wire resonates with the same tuning fork forming three antinodes for the same positions of the bridges. The value of 'MM' is

Show answer and solution

Answer: (d)

  1. Same fork and same bridge length: n=p2LTμn=\frac{p}{2L}\sqrt{\frac{T}{\mu}}, so pT=p\sqrt{T}= constant (pp = number of loops = antinodes).
  2. 59g=3Mg⇒M=55\sqrt{9g}=3\sqrt{Mg} \Rightarrow \sqrt{M}=5
  3. So the answer is (d) 25 kg25\text{ kg}.
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Q293MHT CET 2021 · 20 SEP · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

A sonometer wire resonates with 4 antinodes between two bridges for a given tuning fork, when 1 kg mass is suspended from the wire. Using same fork, when mass M is suspended, the wire resonates producing 2 antinodes between the two bridges (distance between two bridges is as before). The value of M is

Show answer and solution

Answer: (c)

  1. Same nn and LL: pT=p\sqrt{T}= constant.
  2. 41=2M⇒M=24\sqrt{1}=2\sqrt{M} \Rightarrow \sqrt{M}=2
  3. So the answer is (c) 4 kg4\text{ kg}.
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Q294MHT CET 2021 · 20 SEP · SHIFT 1Difficult

Stationary Waves & Vibrating Strings · Bridges, segments and composite wires

Two wires of same material of radius 'r' and '2r' respectively are welded together end to end. The combination is then used as a sonometer wire under tension 'T'. The joint is kept midway between the two bridges. The ratio of the number of loops formed in the wires such that the joint is a node is

Show answer and solution

Answer: (b)

  1. μ=πr2d⇒μ2=4μ1\mu=\pi r^2 d \Rightarrow \mu_2=4\mu_1, so v=T/μv=\sqrt{T/\mu} gives v1=2v2v_1=2v_2.
  2. Same frequency and same length ll for both parts: n=pv2l⇒p∝1vn=\frac{p v}{2l} \Rightarrow p \propto \frac{1}{v}.
  3. p1:p2=1:2p_1:p_2=1:2, so the answer is (b) 1:21:2.
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Q295NEET 2020 · PHASE 2Easy

Stationary Waves & Vibrating Strings · Laws of a vibrating string

The length of the string of a musical instrument is 90 cm and has a fundamental frequency of 120 Hz. Where should it be pressed to produce fundamental frequency of 180 Hz?

Show answer and solution

Answer: (c)

  1. Same tension and string, so f∝1Lf \propto \dfrac{1}{L}.
  2. L2=L1f1f2=90×120180=60 cmL_2 = L_1\dfrac{f_1}{f_2} = 90 \times \dfrac{120}{180} = 60\text{ cm}.
  3. So the answer is (c) 60 cm60\text{ cm}.
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Q296JEE Main 2020 · 2 SEP · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Laws of a vibrating string

Two identical strings X and Z made of same material have tension TX and TZ in them. If their fundamental frequencies are 450 Hz and 300 Hz, respectively, then the ratio TX/TZ is

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Answer: (a)

  1. Identical strings (same LL, μ\mu): f∝T⇒T∝f2f \propto \sqrt{T} \Rightarrow T \propto f^2.
  2. TXTZ=(450300)2=(1.5)2=2.25\dfrac{T_X}{T_Z} = \left(\dfrac{450}{300}\right)^2 = (1.5)^2 = 2.25.
  3. So the answer is (a) 2.252.25.
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Q297JEE Main 2020 · 9 JAN · SHIFT 2Medium

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A wire of length L and mass per unit length 6.0 × 10–3 kgm–1 is put under tension of 540 N. Two consecutive frequencies that it resonates at are: 420 Hz and 490 Hz. Then L in meters is:

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Answer: (b)

  1. Fundamental n1=490−420=70 Hzn_1 = 490 - 420 = 70\text{ Hz}.
  2. v=T/μ=5406×10−3=300 m/sv = \sqrt{T/\mu} = \sqrt{\dfrac{540}{6\times10^{-3}}} = 300\text{ m/s}
  3. L=v2n1=300140≈2.14 mL = \dfrac{v}{2n_1} = \dfrac{300}{140} \approx 2.14\text{ m}
  4. So the answer is (b) 2.1 m.
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Q298MHT CET 2020 · 16 OCT · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

Two identical strings of length ll and 2l2l vibrate with fundamental frequencies N HzN\text{ Hz} and 1.5N1.5N Hz, respectively. The ratio of tensions for smaller length to large length is

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Answer: (b)

  1. Identical strings (same μ\mu): n=12LTμ⇒T∝(nL)2n = \dfrac{1}{2L}\sqrt{\dfrac{T}{\mu}} \Rightarrow T \propto (nL)^2.
  2. T1T2=(N⋅l1.5N⋅2l)2=(13)2=19\dfrac{T_1}{T_2} = \left(\dfrac{N \cdot l}{1.5N \cdot 2l}\right)^2 = \left(\dfrac{1}{3}\right)^2 = \dfrac{1}{9}
  3. So the answer is (b) 1:91:9.
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Q299JEE Main 2020 · 2 SEP · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

A wire of density 9 ×\times 10–3 kg cm–3 is stretched between two clamps 1 m apart. The resulting strain in the wire is 4.9 ×\times 10–4. The lowest frequency of the transverse vibrations in the wire is: (Young’s modulus of wire Y = 9 ×\times 1010 Nm–2), (to the nearest integer), _________

Numerical answer type. Work it out, then open the answer.

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Answer: 35

  1. ρ=9×10−3 kg/cm3=9×103 kg/m3\rho = 9\times10^{-3}\text{ kg/cm}^3 = 9\times10^{3}\text{ kg/m}^3
  2. Stress =Y×strain=9×1010×4.9×10−4=4.41×107 N/m2= Y \times \text{strain} = 9\times10^{10}\times4.9\times10^{-4} = 4.41\times10^{7}\text{ N/m}^2
  3. v=stressρ=4.41×1079×103=70 m/sv = \sqrt{\dfrac{\text{stress}}{\rho}} = \sqrt{\dfrac{4.41\times10^7}{9\times10^3}} = 70\text{ m/s}
  4. n=v2L=702=35 Hzn = \dfrac{v}{2L} = \dfrac{70}{2} = 35\text{ Hz}
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Q300MHT CET 2020 · 19 OCT · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

At the poles, a stretched wire of a given length vibrates in unison with a tuning fork. At the equator, for same setting to produce resonance with same fork, the vibrating length of wire

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Answer: (c)

  1. n=12lMgμn=\frac{1}{2l}\sqrt{\frac{Mg}{\mu}}, so for fixed nn: l∝gl \propto \sqrt{g}.
  2. gg is smaller at the equator than at the poles, so tension and wave speed fall.
  3. So the length must be decreased: answer (c).
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Q301MHT CET 2020 · 16 OCT · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

A sonometer wire under suitable tension having specific gravity ρ\rho, vibrates with frequency nn in air. If the load is completely immersed in water the frequency of vibration of wire will become

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Answer: (b)

  1. Immersed load loses weight equal to buoyancy: T′=Mg(1−1ρ)=T ρ−1ρT'=Mg\left(1-\frac{1}{\rho}\right)=T\,\frac{\rho-1}{\rho}.
  2. n∝T⇒n′=n[ρ−1ρ]1/2n \propto \sqrt{T} \Rightarrow n'=n\left[\frac{\rho-1}{\rho}\right]^{1/2}
  3. So the answer is (b).
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Q302MHT CET 2020 · 16 OCT · SHIFT 2Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

When tension TT is applied to a sonometer wire of length ll, it vibrates with the fundamental frequency nn. Keeping the experimental setup same, when the tension is increased by 8 N, the fundamental frequency becomes three times the earlier fundamental frequency nn. The initial tension applied to the wire (in newton) was

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Answer: (d)

  1. n∝Tn \propto \sqrt{T} for the same wire and length.
  2. T+8T=3⇒T+8=9T\sqrt{\frac{T+8}{T}}=3 \Rightarrow T+8=9T
  3. T=1 NT=1\text{ N}, so the answer is (d) 1.0.
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Q303MHT CET 2019 · 2 MAY · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Stationary wave equation

Find the wrong statement from the following about the equation of stationary wave given by Y=0.04cos⁡(πx)sin⁡(50πt) mY = 0.04\cos(\pi x)\sin(50\pi t)\text{ m} where tt is in second. Then for the stationary wave.

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Answer: (a)

  1. ω=50π⇒T=2π50π=0.04 s\omega = 50\pi \Rightarrow T = \frac{2\pi}{50\pi} = 0.04\text{ s}, so (a) is wrong.
  2. k=π⇒λ=2 mk = \pi \Rightarrow \lambda = 2\text{ m}; v=ωk=50 m/sv = \frac{\omega}{k} = 50\text{ m/s}: (b), (c) true.
  3. Each component wave has amplitude 0.042=0.02 m\frac{0.04}{2} = 0.02\text{ m}: (d) true.
  4. So the wrong statement is (a).
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Q304MHT CET 2019 · 2 MAY · SHIFT 2Easy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A stretched string fixed at both ends has ' mm ' nodes, then the length of the string will be

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Answer: (a)

  1. mm nodes on a string fixed at both ends give (m−1)(m - 1) loops.
  2. Each loop is λ/2\lambda/2 long, so L=(m−1)λ2L = (m - 1)\dfrac{\lambda}{2}.
  3. So the answer is (a) (m−1)λ2(m - 1)\frac{\lambda}{2}.
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Q305JEE Main 2019 · 9 APR · SHIFT 2Easy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A string 2.0 m long and fixed at its ends is driven by a 240 Hz vibrator. The string vibrates in its third harmonic mode. The speed of the wave and its fundamental frequency is :-

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Answer: (d)

  1. Third harmonic: L=3λ2⇒λ=2×2.03=43 mL = \dfrac{3\lambda}{2} \Rightarrow \lambda = \dfrac{2 \times 2.0}{3} = \dfrac{4}{3}\text{ m}.
  2. v=fλ=240×43=320 m/sv = f\lambda = 240 \times \dfrac{4}{3} = 320\text{ m/s}.
  3. Fundamental f0=2403=80 Hzf_0 = \dfrac{240}{3} = 80\text{ Hz}.
  4. So the answer is (d) 320 m/s,80 Hz320\text{ m/s}, 80\text{ Hz}.
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Q306MHT CET 2019 · 2 MAY · SHIFT 2Easy

Stationary Waves & Vibrating Strings · Bridges, segments and composite wires

A stretched wire of length 260 cm is set into vibrations. It is divided into three segments whose frequencies are in the ratio 2:3:42:3:4. Their lengths must be

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Answer: (b)

  1. f∝1lf \propto \dfrac{1}{l}: l1:l2:l3=12:13:14=6:4:3l_1 : l_2 : l_3 = \dfrac{1}{2} : \dfrac{1}{3} : \dfrac{1}{4} = 6 : 4 : 3.
  2. Total parts =13= 13, each part =26013=20 cm= \dfrac{260}{13} = 20\text{ cm}.
  3. Lengths: 120,80,60 cm120, 80, 60\text{ cm}.
  4. So the answer is (b) 120 cm,80 cm,60 cm120\text{ cm}, 80\text{ cm}, 60\text{ cm}.
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Q307JEE Main 2019 · 9 APR · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Stationary wave equation

A string is clamped at both the ends and it is vibrating in its 4th harmonic. The equation of the stationary wave is Y = 0.3 sin(0.157x) cos(200π\pit). The length of the string is: (All quantities are in SI units.)

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Answer: (c)

  1. k=0.157=π20 m−1k = 0.157 = \dfrac{\pi}{20}\text{ m}^{-1}, so λ=2πk=40 m\lambda = \dfrac{2\pi}{k} = 40\text{ m}.
  2. 4th harmonic: L=4×λ2=2λL = 4 \times \dfrac{\lambda}{2} = 2\lambda.
  3. L=2×40=80 mL = 2 \times 40 = 80\text{ m}.
  4. So the answer is (c) 80 m80\text{ m}.
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Q308JEE Main 2019 · 10 JAN · SHIFT 1Medium

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A string of length 1 m and mass 5 g is fixed at both ends. The tension in the string is 8.0 N. The string is set into vibration using an external vibrator of frequency 100 Hz. The separation between successive nodes on the string is close to -

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Answer: (c)

  1. μ=5×10−31=5×10−3 kg/m\mu = \dfrac{5\times10^{-3}}{1} = 5\times10^{-3}\text{ kg/m}, v=85×10−3=40 m/sv = \sqrt{\dfrac{8}{5\times10^{-3}}} = 40\text{ m/s}.
  2. The string vibrates at the driver frequency: λ=vn=40100=0.4 m\lambda = \dfrac{v}{n} = \dfrac{40}{100} = 0.4\text{ m}.
  3. Successive nodes are λ2=0.2 m=20 cm\dfrac{\lambda}{2} = 0.2\text{ m} = 20\text{ cm} apart.
  4. So the answer is (c) 20.0 cm.
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Q309MHT CET 2019 · 3 MAY · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

The fundamental frequency of sonometer wire increases by 9 Hz, if its tension is increased by 69%69\%, keeping the length constant. The frequency of the wire is

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Answer: (c)

  1. n∝Tn \propto \sqrt{T} at fixed length.
  2. T′=1.69T⇒n′=1.3nT' = 1.69T \Rightarrow n' = 1.3n, so the increase is 0.3n0.3n.
  3. 0.3n=9⇒n=30 Hz0.3n = 9 \Rightarrow n = 30\text{ Hz}
  4. So the answer is (c) 30 Hz.
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Q310MHT CET 2019 · 3 MAY · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Sonometer: load and immersed bob

A sonometer wire is in unison with a tuning fork, when it is stretched by weight ww and the corresponding resonating length is L1L_1. If the weight is reduced to (w4)\left(\frac{w}{4}\right), the corresponding resonating length becomes L2L_2. The ratio (L1L2)\left(\frac{L_1}{L_2}\right) is

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Answer: (d)

  1. Unison with same fork: n=12Lwμn=\frac{1}{2L}\sqrt{\frac{w}{\mu}}, so L∝wL \propto \sqrt{w}.
  2. L1L2=ww/4=2\frac{L_1}{L_2}=\sqrt{\frac{w}{w/4}}=2
  3. So the answer is (d) 2:12:1.
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Q311JEE Main 2019 · 8 APR · SHIFT 1Difficult

Stationary Waves & Vibrating Strings · Bridges, segments and composite wires

Figure

A wire of length 2L, is made by joining two wires A and B of same length but different radii r and 2r and made of the same material. It is vibrating at a frequency such that the joint of the two wires forms a node. If the number of antinodes in wire A is p and that in B is q then the ratio p: q is:

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Answer: (c)

  1. Radii rr and 2r2r: μB=4μA\mu_B=4\mu_A, so vA=2vBv_A=2v_B.
  2. Same ff, same length LL, joint a node: f=pvA2L=qvB2Lf=\frac{p v_A}{2L}=\frac{q v_B}{2L}.
  3. pq=vBvA=12\frac{p}{q}=\frac{v_B}{v_A}=\frac{1}{2}, so the answer is (c) 1:21:2.
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Q312JEE Main 2017 · 9 APR · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Stationary wave equation

A standing wave is formed by the superposition of two waves travelling in opposite directions. The transverse displacement is given by

y(x, t) = 0.5 sin (5π4x)\left(\frac{5\pi}{4}x\right) cos(200 π\pit).

What is the speed of the travelling wave moving in the positive x direction?

(x and t are in meter and second, respectively.)

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Answer: (a)

  1. Speed of each travelling wave v=ωkv = \frac{\omega}{k}.
  2. v=200π5π/4=160 m/sv = \frac{200\pi}{5\pi/4} = 160\text{ m/s}.
  3. So the answer is (a) 160 m/s.
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Q313JEE Main 2017 · 8 APR · SHIFT 1Difficult

Stationary Waves & Vibrating Strings · Bridges, segments and composite wires

Two wires W1 and W2 have the same radius r and respective densities ρ\rho1 and ρ\rho2 such that ρ2 = 4ρ\rho1. They are joined together at the point O, as shown in the figure. The combination is used as a sonometer wire and kept under tension T. The point O is midway between the two bridges. When a stationary wave is set up in the composite wire, the joint is found to be a node. The ratio of the number of antinodes formed in W1 to W2 is:

Figure

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Answer: (b)

  1. Same radius: μ∝ρ\mu \propto \rho, so μ2=4μ1\mu_2=4\mu_1 and v1=2v2v_1=2v_2.
  2. Equal lengths, same frequency, joint a node: p∝1vp \propto \frac{1}{v}.
  3. p1:p2=1:2p_1:p_2=1:2, so the answer is (b).
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Q314NEET 2015 · AIPMTEasy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A string is stretched between fixed points separated by 75.0 cm. It is observed to have resonant frequencies of 420 Hz and 315 Hz. There are no other resonant frequencies between these two. The lowest resonant frequency for this string is

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Answer: (b)

  1. Consecutive resonant frequencies of a string differ by the fundamental: f0=fp+1−fpf_0 = f_{p+1} - f_p.
  2. f0=420−315=105 Hzf_0 = 420 - 315 = 105\text{ Hz} (check: 315=3×105315 = 3 \times 105, 420=4×105420 = 4 \times 105).
  3. So the answer is (b) 105 Hz105\text{ Hz}.
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Q315NEET 2014 · AIPMTEasy

Stationary Waves & Vibrating Strings · Bridges, segments and composite wires

If n1, n2 and n3 are the fundamental frequencies of three segments into which a string is divided, then the original fundamental frequency n of the string is given by

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Answer: (a)

  1. Same tension and μ\mu: n∝1ln \propto \dfrac{1}{l}, so l=knl = \dfrac{k}{n}.
  2. l=l1+l2+l3⇒1n=1n1+1n2+1n3l = l_1 + l_2 + l_3 \Rightarrow \dfrac{1}{n} = \dfrac{1}{n_1} + \dfrac{1}{n_2} + \dfrac{1}{n_3}.
  3. So the answer is (a).
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Q316JEE Main 2014 · 19 APR · SHIFT 1Medium

Stationary Waves & Vibrating Strings · Bridges, segments and composite wires

The total length of a sonometer wire between fixed ends is 110 cm. Two bridges are placed to divide the length of wire in ratio 6: 3: 2. The tension in the wire is 400 N and the mass per unit length is 0.01 kg/m. What is the minimum common frequency with which three parts can vibrate?

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Answer: (b)

  1. Lengths: 60,30,20 cm60, 30, 20\text{ cm}. Wave speed v=T/μ=400/0.01=200 m/sv=\sqrt{T/\mu}=\sqrt{400/0.01}=200\text{ m/s}.
  2. Fundamentals f=v2lf=\frac{v}{2l}: 2001.2=166.7\frac{200}{1.2}=166.7, 2000.6=333.3\frac{200}{0.6}=333.3, 2000.4=500 Hz\frac{200}{0.4}=500\text{ Hz}.
  3. Common frequency must be a whole multiple of each: LCM of 5003,10003,500\frac{500}{3}, \frac{1000}{3}, 500 is 1000 Hz1000\text{ Hz}.
  4. So the answer is (b) 1000 Hz.
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Q317NEET 2013Easy

Stationary Waves & Vibrating Strings · Bridges, segments and composite wires

The length of the wire between two ends of a sonometer is 100 cm. What should be the positions of two bridges below the wire so that the three segments of the wire have their fundamental frequencies in the ratio 1: 3: 5.

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Answer: (d)

  1. f∝1lf \propto \dfrac{1}{l}: l1:l2:l3=1:13:15=15:5:3l_1 : l_2 : l_3 = 1 : \dfrac{1}{3} : \dfrac{1}{5} = 15 : 5 : 3.
  2. Total parts =23= 23: l1=150023l_1 = \dfrac{1500}{23}, l2=50023l_2 = \dfrac{500}{23}, l3=30023 cml_3 = \dfrac{300}{23}\text{ cm}.
  3. Bridges at 150023 cm\dfrac{1500}{23}\text{ cm} and 1500+50023=200023 cm\dfrac{1500 + 500}{23} = \dfrac{2000}{23}\text{ cm} from one end.
  4. So the answer is (d) 150023 cm,200023 cm\frac{1500}{23}\text{ cm}, \frac{2000}{23}\text{ cm}.
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Q318JEE Main 2013 · 23 APR · SHIFT 1Easy

Stationary Waves & Vibrating Strings · Bridges, segments and composite wires

A sonometer wire of length 114 cm is fixed at both the ends. Where should the two bridges be placed so as to divide the wire into three segments whose fundamental frequencies are in the ratio 1: 3: 4?

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Answer: (d)

  1. f∝1lf \propto \dfrac{1}{l}: l1:l2:l3=1:13:14=12:4:3l_1 : l_2 : l_3 = 1 : \dfrac{1}{3} : \dfrac{1}{4} = 12 : 4 : 3.
  2. Total parts =19= 19, each part =11419=6 cm⇒72,24,18 cm= \dfrac{114}{19} = 6\text{ cm} \Rightarrow 72, 24, 18\text{ cm}.
  3. Bridges at 72 cm72\text{ cm} and 72+24=96 cm72 + 24 = 96\text{ cm} from one end.
  4. So the answer is (d) at 72 cm and 96 cm from one end.
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Q319JEE Main 2013Difficult

Stationary Waves & Vibrating Strings · Laws of a vibrating string

A sonometer wire of length 1.5 m1.5\text{ m} is made of steel. The tension in it produces an elastic strain of 1%1\%. What is the fundamental frequency of steel if density and elasticity of steel are 7.7×103 kg/m37.7 \times 10^{3}\text{ kg/m}^{3} and 2.2×1011 N/m22.2 \times 10^{11}\text{ N/m}^{2} respectively?

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Answer: (b)

  1. Stress TA=Y×strain=2.2×1011×0.01=2.2×109 N/m2\frac{T}{A}=Y\times\text{strain}=2.2\times10^{11}\times0.01=2.2\times10^{9}\text{ N/m}^2.
  2. v=TAρ=2.2×1097.7×103=2.857×105≈534.5 m/sv=\sqrt{\frac{T}{A\rho}}=\sqrt{\frac{2.2\times10^9}{7.7\times10^3}}=\sqrt{2.857\times10^5}\approx534.5\text{ m/s}
  3. n=v2L=534.53≈178.2 Hzn=\frac{v}{2L}=\frac{534.5}{3}\approx178.2\text{ Hz}
  4. So the answer is (b).
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Q320NEET 2012 · AIPMT · PRELIMSEasy

Stationary Waves & Vibrating Strings · Bridges, segments and composite wires

When a string is divided into three segments of length ll1, ll2 and ll3 the fundamental frequencies of these three segments are v1,v2v_1, v_2 and v3v_3 respectively. The original fundamental frequency (vv) of the string is

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Answer: (c)

  1. Same tension and μ\mu: v∝1lv \propto \dfrac{1}{l}, so l=kvl = \dfrac{k}{v}.
  2. l=l1+l2+l3⇒1v=1v1+1v2+1v3l = l_1 + l_2 + l_3 \Rightarrow \dfrac{1}{v} = \dfrac{1}{v_1} + \dfrac{1}{v_2} + \dfrac{1}{v_3}.
  3. So the answer is (c).
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Q321JEE Main 2006 · AIEEEEasy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A string is stretched between fixed points separated by 75.0 cm.75.0\text{ cm.} It is observed to have resonant frequencies of 420 Hz420\text{ Hz} and 315 Hz315\text{ Hz}. There are no other resonant frequencies between these two. Then, the lowest resonant frequency for this string is

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Answer: (a)

  1. Consecutive resonant frequencies differ by the fundamental.
  2. f0=420−315=105 Hzf_0 = 420 - 315 = 105\text{ Hz} (315=3f0315 = 3f_0, 420=4f0420 = 4f_0).
  3. So the answer is (a) 105 Hz105\text{ Hz}.
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Q322JEE Main 2003 · AIEEEMedium

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

A metal wire of linear mass density of 9.8 g/m9.8\text{ g/m} is stretched with a tension of 10 kg-wt10\text{ kg-wt} between two rigid supports 11 metre apart. The wire passes at its middle point between the poles of a permanent magnet, and it vibrates in resonance when carrying an alternating current of frequency n.n. The frequency nn of the alternating source is

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Answer: (a)

  1. Force on the wire at its middle excites the fundamental (antinode at the centre).
  2. T=10×9.8=98 NT = 10 \times 9.8 = 98\text{ N}, μ=9.8×10−3 kg/m\mu = 9.8\times10^{-3}\text{ kg/m}, so v=989.8×10−3=100 m/sv = \sqrt{\dfrac{98}{9.8\times10^{-3}}} = 100\text{ m/s}.
  3. n=v2L=1002×1=50 Hzn = \dfrac{v}{2L} = \dfrac{100}{2\times1} = 50\text{ Hz}
  4. So the answer is (a) 50 Hz50\text{ Hz}.
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Q323JEE Main 2002 · AIEEEEasy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

length of a string tied to two rigid supports is 40 cm40\text{ cm}. Maximum length (wavelength in cm\text{cm}) of a stationary wave produced on it is

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Answer: (b)

  1. The longest wavelength is in the fundamental mode, one loop: L=λ2L = \dfrac{\lambda}{2}.
  2. λmax=2L=2×40=80 cm\lambda_{max} = 2L = 2 \times 40 = 80\text{ cm}.
  3. So the answer is (b) 8080.
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Q324JEE Main 2002 · AIEEEMedium

Stationary Waves & Vibrating Strings · Stationary wave equation

A wave y=asin⁡(ωt−kx)y = a\sin(\omega t - kx) on a string meets with another wave producing a node at x=0.x = 0. Then the equation of the unknown wave is

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Answer: (b)

  1. A standing wave needs a wave of the same aa, ω\omega, kk moving in the opposite direction: y2=±asin⁡(ωt+kx)y_2 = \pm a\sin(\omega t + kx).
  2. Node at x=0x = 0: y1+y2=0y_1 + y_2 = 0 for all tt, i.e. asin⁡ωt+y2(0,t)=0a\sin\omega t + y_2(0, t) = 0.
  3. This needs y2=−asin⁡(ωt+kx)y_2 = -a\sin(\omega t + kx); then y=−2acos⁡ωtsin⁡kxy = -2a\cos\omega t\sin kx, which is zero at x=0x = 0.
  4. So the answer is (b) y=−asin⁡(ωt+kx)y = -a\sin(\omega t + kx).
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Q325NEET 2001 · AIPMTMedium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

If the tension and diameter of a sonometer wire of fundamental frequency n is doubled and density is halved then its fundamental frequency will become

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Answer: (c)

  1. n∝1DTρn \propto \dfrac{1}{D}\sqrt{\dfrac{T}{\rho}} at fixed length.
  2. n′n=1221/2=12×2=1\dfrac{n'}{n} = \dfrac{1}{2}\sqrt{\dfrac{2}{1/2}} = \dfrac{1}{2}\times 2 = 1
  3. So the answer is (c) n.
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Q326NEET 2000 · AIPMTEasy

Stationary Waves & Vibrating Strings · Bridges, segments and composite wires

A string is cut into three parts, having fundamental frequencies n1, n2, n3 respectively. Then original fundamental frequency n related by the expression as

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Answer: (a)

  1. For the same string material and tension, n∝1ln \propto \dfrac{1}{l}, so l=knl = \dfrac{k}{n}.
  2. l=l1+l2+l3⇒1n=1n1+1n2+1n3l = l_1 + l_2 + l_3 \Rightarrow \dfrac{1}{n} = \dfrac{1}{n_1} + \dfrac{1}{n_2} + \dfrac{1}{n_3}.
  3. So the answer is (a).
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Q327NEET 1998 · AIPMTEasy

Stationary Waves & Vibrating Strings · Nodes, antinodes and properties

A standing wave having 3 nodes and 2 antinodes is formed between two atoms having a distance 1.211.21 Å between them. The wavelength of the standing wave is

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Answer: (a)

  1. 3 nodes and 2 antinodes means 2 loops, with nodes at both atoms.
  2. Each loop is λ2\frac{\lambda}{2}, so 2×λ2=λ=1.212 \times \frac{\lambda}{2} = \lambda = 1.21 Å.
  3. So the answer is (a) 1.211.21 Å.
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Q328NEET 1997 · AIPMTEasy

Stationary Waves & Vibrating Strings · String modes: harmonics and overtones

Standing waves are produced in 10 m10\text{ m} long stretched string. If the string vibrates in 5 segments and wave velocity is 20 m/s20\text{ m/s}, the frequency is

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Answer: (a)

  1. 5 segments (loops): L=5λ2L = 5\dfrac{\lambda}{2}.
  2. λ=2×105=4 m\lambda = \dfrac{2 \times 10}{5} = 4\text{ m}.
  3. f=vλ=204=5 Hzf = \dfrac{v}{\lambda} = \dfrac{20}{4} = 5\text{ Hz}.
  4. So the answer is (a) 5 Hz5\text{ Hz}.
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Q329NEET 1995 · AIPMTEasy

Stationary Waves & Vibrating Strings · Bridges, segments and composite wires

The length of a sonometer wire ABAB is 110 cm110\text{ cm}. Where should the two bridges be placed from AA to divide the wire in 3 segments whose fundamental frequencies are in the ratio of 1:2:31:2:3?

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Answer: (a)

  1. f∝1lf \propto \dfrac{1}{l}: l1:l2:l3=1:12:13=6:3:2l_1 : l_2 : l_3 = 1 : \dfrac{1}{2} : \dfrac{1}{3} = 6 : 3 : 2.
  2. Each part =11011=10 cm⇒60,30,20 cm= \dfrac{110}{11} = 10\text{ cm} \Rightarrow 60, 30, 20\text{ cm}.
  3. Bridges from A at 60 cm60\text{ cm} and 90 cm90\text{ cm}.
  4. So the answer is (a) 60 cm60\text{ cm} and 90 cm90\text{ cm}.
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Q330NEET 1994 · AIPMTEasy

Stationary Waves & Vibrating Strings · Nodes, antinodes and properties

A wave of frequency 100 Hz100\text{ Hz} travels along a string towards its fixed end. When this wave travels back, after reflection, a node is formed at a distance of 10 cm10\text{ cm} from the fixed end. The speed of the wave (incident and reflected) is

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Answer: (a)

  1. The fixed end is a node; the next node is λ2\frac{\lambda}{2} away.
  2. λ2=10 cm⇒λ=0.2 m\frac{\lambda}{2} = 10\text{ cm} \Rightarrow \lambda = 0.2\text{ m}.
  3. v=nλ=100×0.2=20 m/sv = n\lambda = 100 \times 0.2 = 20\text{ m/s}.
  4. So the answer is (a) 20 m/s20\text{ m/s}.
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Q331NEET 1994 · AIPMTMedium

Stationary Waves & Vibrating Strings · Stationary wave equation

A stationary wave is represented by y=Asin⁡(100t)cos⁡(0.01x)y = A\sin(100t)\cos(0.01x), where yy and AA are in millimetres, tt is in seconds and xx is in metres. The velocity of the wave is

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Answer: (a)

  1. Compare with y=Asin⁡(ωt)cos⁡(kx)y = A\sin(\omega t)\cos(kx): ω=100 rad/s\omega = 100\text{ rad/s}, k=0.01 m−1k = 0.01\text{ m}^{-1}.
  2. Speed of the component waves v=ωk=1000.01=104 m/sv = \dfrac{\omega}{k} = \dfrac{100}{0.01} = 10^4\text{ m/s}.
  3. So the answer is (a) 104 m/s10^4\text{ m/s}.
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Q332NEET 1993 · AIPMTMedium

Stationary Waves & Vibrating Strings · Laws of a vibrating string

A stretched string resonates with tuning fork frequency 512 Hz512\text{ Hz} when length of the string is 0.5 m0.5\text{ m}. The length of the string required to vibrate resonantly with a tuning fork of frequency 256 Hz256\text{ Hz} would be

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Answer: (c)

  1. Same string and tension: n∝1Ln \propto \dfrac{1}{L}, so nLnL is constant.
  2. 512×0.5=256×L⇒L=1 m512 \times 0.5 = 256 \times L \Rightarrow L = 1\text{ m}
  3. So the answer is (c) 1 m1\text{ m}.
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Q333MHT CET 2026 · 17 APR · SHIFT 2Easy

Organ Pipes & Resonance Tube · Closed organ pipe

In a pipe closed at one end, air column is vibrating in the fourth overtone so the vibrating air column has 'xx' nodes and 'yy' antinodes. The values of xx and yy are respectively

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Answer: (d)

  1. Fourth overtone of a closed pipe is the 9th harmonic: L=9λ4L=\frac{9\lambda}{4}.
  2. The kk-th overtone of a closed pipe has k+1k+1 nodes and k+1k+1 antinodes.
  3. So x=5x=5, y=5y=5: answer (d).
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Q334MHT CET 2026 · 16 APR · SHIFT 2Easy

Organ Pipes & Resonance Tube · Closed organ pipe

An air column in a pipe which is closed at one end will be in resonance with a vibrating tuning fork of frequency 415 Hz for various vibrating air columns. Which one of the following lengths is not in resonance? (velocity of sound in air = 332 m/s) (Neglect end correction)

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Answer: (b)

  1. λ=vf=332415=0.8 m\lambda=\frac{v}{f}=\frac{332}{415}=0.8\text{ m}, so λ4=20 cm\frac{\lambda}{4}=20\text{ cm}.
  2. Closed pipe resonates at odd multiples of λ4\frac{\lambda}{4}: 20,60,100,140 cm…20, 60, 100, 140\text{ cm} \ldots
  3. 40 cm40\text{ cm} is an even multiple, so the answer is (b).
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Q335JEE Main 2026 · 24 JAN · SHIFT 2Easy

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The fifth harmonic of a closed organ pipe is found to be in unison with the first harmonic of an open pipe. The ratio of lengths of closed pipe to that of the open pipe is 5/x5/x. The value of xx is ______

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Answer: (b)

  1. Fifth harmonic of closed pipe: 5v4Lc\frac{5v}{4L_c}. First harmonic of open pipe: v2Lo\frac{v}{2L_o}.
  2. 5v4Lc=v2Lo⇒LcLo=52\frac{5v}{4L_c}=\frac{v}{2L_o} \Rightarrow \frac{L_c}{L_o}=\frac{5}{2}
  3. So x=2x=2: answer (b).
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Q336MHT CET 2026 · 19 MAY · SHIFT 2Easy

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

A pipe open at both ends has a frequency ff in air. The pipe is dipped vertically in water, so that its (1/3)(1/3) part of its length is in water. The fundamental frequency of the air column is now xfxf, the value of xx is

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Answer: (b)

  1. In air (open pipe): f=v2Lf=\frac{v}{2L}.
  2. With 13\frac{1}{3} in water it becomes a closed pipe of length 2L3\frac{2L}{3}: f′=v4⋅2L3=3v8Lf'=\frac{v}{4\cdot\frac{2L}{3}}=\frac{3v}{8L}.
  3. f′=34ff'=\frac{3}{4}f, so x=34x=\frac{3}{4}: answer (b).
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Q337MHT CET 2026 · 15 MAY · SHIFT 2Easy

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

In an experiment with a closed organ pipe, it is filled with water by (15)th\left(\frac{1}{5}\right)^{th} of its volume. The frequency of the fundamental note will change by

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Answer: (a)

  1. Closed pipe: f=v4Lf=\frac{v}{4L}. Water fills 15\frac{1}{5}, so the air column is L′=4L5L'=\frac{4L}{5}.
  2. f′=54ff'=\frac{5}{4}f
  3. Change =+25%=+25\%, so the answer is (a).
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Q338MHT CET 2026 · 18 APR · SHIFT 2Easy

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

In an organ pipe closed at one end produces a fundamental note of frequency 'ν\nu'. The pipe is cut into two pipes of equal length. The fundamental frequencies produced in the two pipes are

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Answer: (c)

  1. Original closed pipe: ν=v4L\nu=\frac{v}{4L}.
  2. Piece with the closed end: closed pipe of length L2\frac{L}{2}: v4(L/2)=2ν\frac{v}{4(L/2)}=2\nu.
  3. Other piece is open at both ends, length L2\frac{L}{2}: v2(L/2)=vL=4ν\frac{v}{2(L/2)}=\frac{v}{L}=4\nu.
  4. So the answer is (c) 2ν,4ν2\nu, 4\nu.
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Q339MHT CET 2026 · 15 APR · SHIFT 2Easy

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

A pipe open at both ends has a fundamental frequency 'f' in air. The pipe is dipped in water, so that 23rd{\frac{2}{3}}^{rd} length of pipe is in water, Now the fundamental frequency of the air column is

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Answer: (b)

  1. Open pipe of length LL: f=v2Lf = \frac{v}{2L}.
  2. Dipping in water closes the lower end; air column left =L−23L=L3= L - \frac{2}{3}L = \frac{L}{3} (closed pipe).
  3. f′=v4(L/3)=3v4L=32⋅v2Lf' = \frac{v}{4(L/3)} = \frac{3v}{4L} = \frac{3}{2}\cdot\frac{v}{2L}
  4. So the answer is (b) 32f\frac{3}{2}f.
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Q340MHT CET 2026 · 13 MAY · SHIFT 2Medium

Organ Pipes & Resonance Tube · Closed organ pipe

An organ pipe closed at one end has fundamental frequency of 15001500 Hz. The maximum number of overtones generated by this pipe a normal person can hear is (neglect end connection)

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Answer: (c)

  1. Closed pipe gives only odd harmonics: (2n+1)f0(2n+1)f_0, where nn = overtone number.
  2. Audible limit ≈20 kHz\approx 20\text{ kHz}: (2n+1)(1500)≤20000⇒2n+1≤13.3(2n+1)(1500) \le 20000 \Rightarrow 2n+1 \le 13.3
  3. Highest odd harmonic =13= 13, so 2n+1=13⇒n=62n+1 = 13 \Rightarrow n = 6.
  4. So the answer is (c) 66.
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Q341MHT CET 2026 · 13 APR · SHIFT 1Medium

Organ Pipes & Resonance Tube · Closed organ pipe

In fundamental mode, the time required for the sound wave to reach upto the closed end of a pipe filled with air is tt second. The frequency of vibration of air column is

(λ\lambda = wavelength of the wave)

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Answer: (b)

  1. Fundamental of closed pipe: L=λ4L = \frac{\lambda}{4} and f=v4Lf = \frac{v}{4L}.
  2. Time to travel the pipe length: t=Lvt = \frac{L}{v}.
  3. f=14⋅vL=14t=0.25tf = \frac{1}{4}\cdot\frac{v}{L} = \frac{1}{4t} = \frac{0.25}{t}
  4. So the answer is (b) 0.25t\frac{0.25}{t}.
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Q342MHT CET 2026 · 20 MAY · SHIFT 1Medium

Organ Pipes & Resonance Tube · Open organ pipe

A pipe open at both ends has length 11 m. The air column in a pipe cannot resonate for a frequency (Neglect end correction, speed of sound in air =340= 340 m/s)

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Answer: (d)

  1. Open pipe: fn=nv2Lf_n = \frac{nv}{2L}, fundamental =3402×1=170 Hz= \frac{340}{2 \times 1} = 170\text{ Hz}.
  2. Allowed: 170,340,510,…170, 340, 510, \dots (integer multiples of 170 Hz).
  3. 85 Hz=12×17085\text{ Hz} = \frac{1}{2}\times 170 is not a multiple, so it cannot resonate.
  4. So the answer is (d) 8585 Hz.
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Q343JEE Main 2026 · 22 JAN · SHIFT 2Medium

Organ Pipes & Resonance Tube · Open organ pipe

In an open organ pipe ν3\nu_3 and ν6\nu_6 are 33rd and 66th harmonic frequencies, respectively. If ν6−ν3=2200 Hz\nu_6 - \nu_3 = 2200\text{ Hz} then length of the pipe is ______ mm.

(Take velocity of sound in air is 330 m/s330\text{ m/s}.)

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Answer: (b)

  1. Open pipe: νn=nv2L\nu_n = \frac{nv}{2L}.
  2. ν6−ν3=3v2L=2200\nu_6 - \nu_3 = \frac{3v}{2L} = 2200
  3. L=3×3302×2200=0.225 m=225 mmL = \frac{3 \times 330}{2 \times 2200} = 0.225\text{ m} = 225\text{ mm}
  4. So the answer is (b) 225.
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Q344MHT CET 2026 · 15 MAY · SHIFT 2Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

An organ pipe P1P_1 closed at one end and vibrating in its first overtone and other pipe P2P_2 open at both ends vibrating in its third overtone are in resonance with a given tuning fork. The ratio of length of P1P_1 and P2P_2 will be

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Answer: (a)

  1. Closed pipe, first overtone (3rd harmonic): f=3v4L1f = \frac{3v}{4L_1}.
  2. Open pipe, third overtone (4th harmonic): f=4v2L2=2vL2f = \frac{4v}{2L_2} = \frac{2v}{L_2}.
  3. 3v4L1=2vL2⇒L1L2=38\frac{3v}{4L_1} = \frac{2v}{L_2} \Rightarrow \frac{L_1}{L_2} = \frac{3}{8}
  4. So the answer is (a) 3:83 : 8.
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Q345MHT CET 2026 · 12 MAY · SHIFT 2Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The third overtone of a closed organ pipe is in unison with 3rd3^{rd} overtone of an open pipe. The ratio of length of closed to open pipe is

Show answer and solution

Answer: (d)

  1. Closed pipe, third overtone (7th harmonic): 7v4Lc\frac{7v}{4L_c}.
  2. Open pipe, third overtone (4th harmonic): 4v2Lo=2vLo\frac{4v}{2L_o} = \frac{2v}{L_o}.
  3. 74Lc=2Lo⇒LcLo=78\frac{7}{4L_c} = \frac{2}{L_o} \Rightarrow \frac{L_c}{L_o} = \frac{7}{8}
  4. So the answer is (d) 78\frac{7}{8}.
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Q346MHT CET 2026 · 12 MAY · SHIFT 1Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

A pipe closed at one end vibrating in the sixth overtone is in unison with the open pipe vibrating in its sixth overtone. The ratio lc:lol_c : l_o is {lc=\{l_c = vibrating length of pipe closed at one end, lo=l_o = vibrating length of pipe open at both ends}\}

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Answer: (a)

  1. Closed pipe, sixth overtone (13th harmonic): 13v4lc\frac{13v}{4l_c}.
  2. Open pipe, sixth overtone (7th harmonic): 7v2lo\frac{7v}{2l_o}.
  3. 134lc=72lo⇒lclo=2628=1314\frac{13}{4l_c} = \frac{7}{2l_o} \Rightarrow \frac{l_c}{l_o} = \frac{26}{28} = \frac{13}{14}
  4. So the answer is (a) 13:1413 : 14.
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Q347MHT CET 2026 · 19 APR · SHIFT 1Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The third overtone of a closed pipe of length 'LcL_c' has the same frequency as the third overtone of the open pipe of length 'L0L_0'. Both the pipes have same diameters. The ratio Lc:L0L_c : L_0 is equal to

Show answer and solution

Answer: (b)

  1. Closed pipe, third overtone (7th harmonic): 7v4Lc\frac{7v}{4L_c}.
  2. Open pipe, third overtone (4th harmonic): 4v2L0=2vL0\frac{4v}{2L_0} = \frac{2v}{L_0}.
  3. 74Lc=2L0⇒Lc:L0=7:8\frac{7}{4L_c} = \frac{2}{L_0} \Rightarrow L_c : L_0 = 7 : 8
  4. So the answer is (b) 7:87 : 8.
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Q348MHT CET 2026 · 18 APR · SHIFT 1Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

Fifth overtone of an open pipe of length L0L_0 is in unison with the fifth overtone of the pipe closed at one end of length LcL_c.

The ratio L0L_0 to LcL_c is

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Answer: (d)

  1. Open pipe, fifth overtone (6th harmonic): 6v2L0=3vL0\frac{6v}{2L_0} = \frac{3v}{L_0}.
  2. Closed pipe, fifth overtone (11th harmonic): 11v4Lc\frac{11v}{4L_c}.
  3. 3L0=114Lc⇒L0Lc=1211\frac{3}{L_0} = \frac{11}{4L_c} \Rightarrow \frac{L_0}{L_c} = \frac{12}{11}
  4. So the answer is (d) 12:1112 : 11.
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Q349MHT CET 2026 · 16 APR · SHIFT 2Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

When open pipe is closed from one end then third overtone of closed pipe is higher in frequency by 150Hz than second overtone of open pipe. The fundamental frequency of open end pipe will be (Neglect end correction)

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Answer: (d)

  1. Open pipe fundamental f=v2Lf = \frac{v}{2L}; closing one end gives fundamental v4L=f2\frac{v}{4L} = \frac{f}{2}.
  2. Closed third overtone (7th harmonic) =7f2= \frac{7f}{2}; open second overtone (3rd harmonic) =3f= 3f.
  3. 7f2−3f=f2=150⇒f=300 Hz\frac{7f}{2} - 3f = \frac{f}{2} = 150 \Rightarrow f = 300\text{ Hz}
  4. So the answer is (d) 300300 Hz.
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Q350MHT CET 2026 · 15 APR · SHIFT 2Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

When open pipe is closed from one end then second overtone of closed pipe is higher in frequency by 100 Hz than first overtone of open pipe. The fundamental frequency of open end pipe will be (Neglect end correction)

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Answer: (a)

  1. Open pipe fundamental f=v2Lf = \frac{v}{2L}; closing one end gives fundamental f2\frac{f}{2}.
  2. Closed second overtone (5th harmonic) =5f2= \frac{5f}{2}; open first overtone (2nd harmonic) =2f= 2f.
  3. 5f2−2f=f2=100⇒f=200 Hz\frac{5f}{2} - 2f = \frac{f}{2} = 100 \Rightarrow f = 200\text{ Hz}
  4. So the answer is (a) 200200 Hz.
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Q351NEET 2026 · RE-NEETMedium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

For sound waves, if the number of nodes for the 55th harmonic of an open-ended pipe is nn and that for the 99th harmonic of the same pipe with one of its ends closed is mm, the ratio nm\frac{n}{m} is

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Answer: (d)

  1. Open pipe, kkth harmonic: L=kλ2L = k\frac{\lambda}{2} with antinodes at both ends, so it has kk displacement nodes. 5th harmonic: n=5n = 5.
  2. Closed pipe, (2k−1)(2k-1)th harmonic: L=(2k−1)λ4L = (2k-1)\frac{\lambda}{4} has kk nodes (one at the closed end). 9th harmonic: 2k−1=9⇒m=52k-1 = 9 \Rightarrow m = 5.
  3. nm=55=1\frac{n}{m} = \frac{5}{5} = 1
  4. So the answer is (d) 1.
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Q352MHT CET 2026 · 13 MAY · SHIFT 1Medium

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

The fundamental frequency of a closed pipe is 400400 Hz. If 13rd{\frac{1}{3}}^{rd} pipe is filled with water then the frequency of 3rd3^{rd} harmonic of the pipe will be (Neglect end correction)

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Answer: (b)

  1. Closed pipe: n0=v4L=400n_0 = \frac{v}{4L} = 400 Hz.
  2. With 13\frac{1}{3} filled, air column =2L3= \frac{2L}{3}, so new fundamental =400×32=600= 400 \times \frac{3}{2} = 600 Hz.
  3. 3rd harmonic =3×600=1800= 3 \times 600 = 1800 Hz
  4. So the answer is (b) 1800 Hz.
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Q353MHT CET 2026 · 14 MAY · SHIFT 2Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

Two closed organ pipes A and B have the same length and A is wider than B. They resonate in the fundamental mode at frequencies nAn_A and nBn_B respectively, then

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Answer: (c)

  1. End correction e=0.3de = 0.3d, so the effective length is L+0.3dL + 0.3d.
  2. Fundamental n=v4(L+0.3d)n = \frac{v}{4(L + 0.3d)}: the wider pipe A has the larger effective length.
  3. So nA<nBn_A < n_B, the answer is (c).
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Q354MHT CET 2026 · 20 APR · SHIFT 1Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

A tuning fork of frequency 'nn' is held near the open end of a tube which is dipped in water and length of the tube is adjusted until resonance occurs. If the two shortest lengths that produce resonance are l1l_1 and l2l_2, the speed of sound in air is (neglect end correction)

Show answer and solution

Answer: (a)

  1. Successive resonating lengths of a closed tube differ by half a wavelength: l2−l1=λ2l_2 - l_1 = \frac{\lambda}{2}.
  2. λ=2(l2−l1)\lambda = 2(l_2 - l_1), so v=nλ=2n(l2−l1)v = n\lambda = 2n(l_2 - l_1)
  3. So the answer is (a) 2n(l2−l1)2n(l_2 - l_1).
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Q355MHT CET 2026 · 19 APR · SHIFT 2Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

In a resonance tube open at one end, the end correction is 1.11.1 cm. If the shortest length of resonating air column with a tuning fork is 1818 cm, the next resonating length will be

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Answer: (d)

1st2nde = 1.1 cm (above top)l1 + e = λ/4 = 19.1 cml2 + e = 3λ/4 = 57.3 cm
  1. First resonance: l1+e=λ4⇒λ4=18+1.1=19.1l_1 + e = \frac{\lambda}{4} \Rightarrow \frac{\lambda}{4} = 18 + 1.1 = 19.1 cm.
  2. Second resonance: l2+e=3λ4=3×19.1=57.3l_2 + e = \frac{3\lambda}{4} = 3 \times 19.1 = 57.3 cm.
  3. l2=57.3−1.1=56.2l_2 = 57.3 - 1.1 = 56.2 cm
  4. So the answer is (d) 56.2 cm.
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Q356MHT CET 2026 · 14 MAY · SHIFT 1Medium

Organ Pipes & Resonance Tube · Joined pipes, gases and string-pipe resonance

n1n_1 is the fundamental frequency of the pipe closed at one end and n2n_2 is the fundamental frequency of the pipe open at both ends. If both are joined end to end, the fundamental frequency of closed pipe so formed is

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Answer: (a)

  1. Closed pipe: L1=v4n1L_1 = \frac{v}{4n_1}; open pipe: L2=v2n2L_2 = \frac{v}{2n_2}.
  2. Joined: closed pipe of length L1+L2L_1 + L_2, fundamental n=v4(L1+L2)n = \frac{v}{4(L_1 + L_2)}.
  3. n=vvn1+2vn2=n1n2n2+2n1n = \frac{v}{\frac{v}{n_1} + \frac{2v}{n_2}} = \frac{n_1 n_2}{n_2 + 2n_1}
  4. So the answer is (a) n1n2n2+2n1\frac{n_1 n_2}{n_2 + 2n_1}.
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Q357MHT CET 2026 · 15 APR · SHIFT 1Difficult

Organ Pipes & Resonance Tube · Joined pipes, gases and string-pipe resonance

A Pipe open at one end has length 0.80.8 m. At the open end of the tube a string 0.50.5 m long is vibrating in its first overtone and resonates with fundamental frequency of pipe. If tension in the string is 5050 N, the mass of string is (Neglect end correction) (Speed of sound =320= 320 m/s)

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Answer: (c)

  1. Pipe (closed at one end) fundamental: f=v4L=3204×0.8=100 Hzf = \frac{v}{4L} = \frac{320}{4 \times 0.8} = 100\text{ Hz}
  2. String first overtone (2nd harmonic): f=22lTμ=10.550μf = \frac{2}{2l}\sqrt{\frac{T}{\mu}} = \frac{1}{0.5}\sqrt{\frac{50}{\mu}}
  3. 250μ=100⇒μ=502500=0.02 kg/m2\sqrt{\frac{50}{\mu}} = 100 \Rightarrow \mu = \frac{50}{2500} = 0.02\text{ kg/m}
  4. Mass =μl=0.02×0.5=0.01 kg=10 g= \mu l = 0.02 \times 0.5 = 0.01\text{ kg} = 10\text{ g}
  5. So the answer is (c) 10 gram.
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Q358MHT CET 2025 · 22 APR · SHIFT 2Easy

Organ Pipes & Resonance Tube · Closed organ pipe

In a pipe closed at one end, air column is vibrating in its second overtone. The column has

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Answer: (a)

NNNAAAClosed pipe, second overtone: L = 5λ/4
  1. Second overtone of a closed pipe: L=5λ4L=\frac{5\lambda}{4} (5th harmonic).
  2. Pattern from closed end: N A N A N A, i.e. 3 nodes and 3 antinodes.
  3. So the answer is (a).
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Q359MHT CET 2025 · 25 APR · SHIFT 2Easy

Organ Pipes & Resonance Tube · Open organ pipe

In an open end organ pipe of length ' LL ', if the velocity of sound is ' V ', then the fundamental frequency will be (Neglect end correction)

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Answer: (a)

  1. Open pipe: antinodes at both ends, L=λ2L=\frac{\lambda}{2}, so n=V2Ln=\frac{V}{2L}.
  2. Allowed modes L=pλ2L=\frac{p\lambda}{2}, p=1,2,3…p=1,2,3\ldots, so all harmonics are present.
  3. So the answer is (a).
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Q360MHT CET 2025 · 26 APR · SHIFT 2Easy

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The fundamental frequency of an air column in a pipe closed at one end is 150 Hz. If the same pipe is open at both the end, the frequencies produced in Hz are

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Answer: (d)

  1. Closed: v4L=150 Hz\frac{v}{4L}=150\text{ Hz}, so open: v2L=300 Hz\frac{v}{2L}=300\text{ Hz}.
  2. Open pipe gives all harmonics: 300,600,900,1200…300, 600, 900, 1200 \ldots
  3. So the answer is (d).
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Q361MHT CET 2025 · 25 APR · SHIFT 2Easy

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The fundamental frequencies of vibrations of air column in pipe open at both ends and in pipe closed at one end are ' n1n_1 ' and ' n2n_2 ' respectively, then

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Answer: (b)

  1. For the same length: n1=v2Ln_1=\frac{v}{2L}, n2=v4Ln_2=\frac{v}{4L}.
  2. n1=2n2n_1=2n_2, so the answer is (b).
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Q362MHT CET 2025 · 22 APR · SHIFT 1Easy

Organ Pipes & Resonance Tube · Comparing closed and open pipes

An organ pipe has fundamental frequency 80 Hz. If its one end is closed, the frequencies produced will be (in Hz) (Neglect end correction)

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Answer: (c)

  1. Open: v2L=80 Hz\frac{v}{2L}=80\text{ Hz}. Closing one end: v4L=40 Hz\frac{v}{4L}=40\text{ Hz}.
  2. Closed pipe gives only odd harmonics: 40,120,200,28040, 120, 200, 280.
  3. So the answer is (c).
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Q363MHT CET 2025 · 23 APR · SHIFT 1Easy

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

A pipe open at both ends produces a fundamental frequency n1n_1. When the pipe is kept with 34th{\frac{3}{4}}^{\text{th}} of its length in water, it produces a note of fundamental frequency n2n_2. The ratio of n1n2\frac{n_1}{n_2} is

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Answer: (d)

  1. Open pipe: n1=v2Ln_1 = \frac{v}{2L}.
  2. With 34\frac{3}{4} in water it becomes a closed pipe of length L4\frac{L}{4}: n2=v4(L/4)=vLn_2 = \frac{v}{4(L/4)} = \frac{v}{L}.
  3. n1n2=v/2Lv/L=12\frac{n_1}{n_2} = \frac{v/2L}{v/L} = \frac{1}{2}
  4. So the answer is (d) 12\frac{1}{2}.
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Q364NEET 2025Easy

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

A pipe open at both ends has a fundamental frequency ff in air. The pipe is now dipped vertically in a water drum to half of its length. The fundamental frequency of the air column is now equal to:

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Answer: (d)

  1. Open pipe: f=v2Lf = \frac{v}{2L}.
  2. Half in water leaves a closed pipe of length L2\frac{L}{2}: f′=v4(L/2)=v2Lf' = \frac{v}{4(L/2)} = \frac{v}{2L}.
  3. So the answer is (d) ff.
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Q365JEE Main 2025 · 4 APR · SHIFT 1Easy

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

In an experiment with a closed organ pipe, it is filled with water by (15)\left(\frac{1}{5}\right) th of its volume. The frequency of the fundamental note will change by

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Answer: (b)

  1. Closed pipe: f=v4Lf = \frac{v}{4L}, so f∝1Lf \propto \frac{1}{L}.
  2. Water fills 15\frac{1}{5} of the volume, so air column L′=45LL' = \frac{4}{5}L.
  3. f′=54ff' = \frac{5}{4}f, change =f′−ff×100=+25%= \frac{f'-f}{f}\times 100 = +25\%
  4. So the answer is (b) 25%25\%.
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Q366MHT CET 2025 · 5 MAY · SHIFT 2Medium

Organ Pipes & Resonance Tube · Closed organ pipe

An organ pipe closed at one end has fundamental frequency of 1500 Hz. The maximum number of overtones generated by this pipe which a normal person can hear is (Normal man can hear the frequency up to 19.5 kHz, Neglect end correction)

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Answer: (a)

  1. Closed pipe gives only odd harmonics: (2n+1)f0(2n+1)f_0, where nn = overtone number.
  2. (2n+1)(1500)≤19500⇒2n+1≤13(2n+1)(1500) \le 19500 \Rightarrow 2n+1 \le 13
  3. 2n+1=13⇒n=62n+1 = 13 \Rightarrow n = 6 overtones.
  4. So the answer is (a) 6.
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Q367MHT CET 2025 · 20 APR · SHIFT 1Medium

Organ Pipes & Resonance Tube · Closed organ pipe

In fundamental mode, the time required for the sound wave to reach up to closed end of a pipe filled with air is ' tt ' second. The frequency of vibration of air column is (Neglect end correction)

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Answer: (a)

  1. Fundamental of closed pipe: f=v4Lf = \frac{v}{4L}.
  2. Time to travel the pipe length: t=Lvt = \frac{L}{v}.
  3. f=14t=(4t)−1f = \frac{1}{4t} = (4t)^{-1}
  4. So the answer is (a) (4t)−1(4t)^{-1}.
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Q368MHT CET 2025 · 19 APR · SHIFT 2Medium

Organ Pipes & Resonance Tube · Closed organ pipe

In an organ pipe closed at one end; the sum of the frequencies of first three overtones is 3930 Hz. The frequency of the fundamental mode of organ pipe is

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Answer: (b)

  1. Closed pipe overtones are odd harmonics: first three overtones =3f,5f,7f= 3f, 5f, 7f.
  2. 3f+5f+7f=15f=39303f + 5f + 7f = 15f = 3930
  3. f=393015=262 Hzf = \frac{3930}{15} = 262\text{ Hz}
  4. So the answer is (b) 262 Hz.
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Q369MHT CET 2025 · 26 APR · SHIFT 1Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

An air column is of length 17 cm. The ratio of frequencies of 55th overtone if the air column is closed at one end to that open at both ends is (velocity of sound in air =340 ms−1= 340\text{ ms}^{-1})

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Answer: (c)

  1. Closed pipe, 5th overtone (11th harmonic): 11v4L\frac{11v}{4L}.
  2. Open pipe, 5th overtone (6th harmonic): 6v2L=12v4L\frac{6v}{2L} = \frac{12v}{4L}.
  3. Ratio =1112= \frac{11}{12} (independent of LL and vv).
  4. So the answer is (c) 1112\frac{11}{12}.
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Q370MHT CET 2025 · 23 APR · SHIFT 2Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

An open organ pipe is closed such that the third overtone of the closed pipe is found to be higher in frequency by 200 Hz than the second overtone of the original pipe. The fundamental frequency of the open pipe is (Neglect end correction)

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Answer: (c)

  1. Open pipe fundamental f=v2Lf = \frac{v}{2L}; closing one end gives fundamental f2\frac{f}{2}.
  2. Closed third overtone (7th harmonic) =7f2= \frac{7f}{2}; open second overtone (3rd harmonic) =3f= 3f.
  3. 7f2−3f=f2=200⇒f=400 Hz\frac{7f}{2} - 3f = \frac{f}{2} = 200 \Rightarrow f = 400\text{ Hz}
  4. So the answer is (c) 400 Hz.
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Q371MHT CET 2025 · 20 APR · SHIFT 2Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The length of closed and open pipe is same. The ratio of frequency of nnth overtone for closed pipe to that of open pipe is (Neglect end correction)

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Answer: (a)

  1. Closed pipe, nnth overtone =(2n+1)= (2n+1)th harmonic: (2n+1)v4L\frac{(2n+1)v}{4L}.
  2. Open pipe, nnth overtone =(n+1)= (n+1)th harmonic: (n+1)v2L\frac{(n+1)v}{2L}.
  3. Ratio =(2n+1)2(n+1)= \frac{(2n+1)}{2(n+1)}
  4. So the answer is (a) (2n+1)2(n+1)\frac{(2n+1)}{2(n+1)}.
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Q372MHT CET 2025 · 19 APR · SHIFT 1Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The frequency of fourth overtone of a closed pipe is in unison with the fifth overtone of an open pipe. The ratio of length of closed pipe to that of open pipe is

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Answer: (b)

  1. Closed pipe, fourth overtone (9th harmonic): 9v4Lc\frac{9v}{4L_c}.
  2. Open pipe, fifth overtone (6th harmonic): 6v2Lo=3vLo\frac{6v}{2L_o} = \frac{3v}{L_o}.
  3. 94Lc=3Lo⇒LcLo=912=34\frac{9}{4L_c} = \frac{3}{L_o} \Rightarrow \frac{L_c}{L_o} = \frac{9}{12} = \frac{3}{4}
  4. So the answer is (b) 3:43 : 4.
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Q373MHT CET 2025 · 19 APR · SHIFT 1Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The fundamental frequency of a closed pipe of length LL is equal to the second overtone of a pipe open at both the ends of length (XL). The value of X is (Neglect end correction)

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Answer: (c)

  1. Closed pipe fundamental: nc=v4Ln_c = \frac{v}{4L}.
  2. Open pipe second overtone (3rd harmonic): no=3v2(XL)n_o = \frac{3v}{2(XL)}.
  3. v4L=3v2XL⇒2XL=12L⇒X=6\frac{v}{4L} = \frac{3v}{2XL} \Rightarrow 2XL = 12L \Rightarrow X = 6
  4. So the answer is (c) 6.
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Q374MHT CET 2025 · 25 APR · SHIFT 1Medium

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

The fundamental frequency of a closed pipe is 400 Hz. If (13)\left(\frac{1}{3}\right)rd length of the pipe is filled with water, the frequency of the 22nd harmonic of the pipe will be (Neglect end correction)

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Answer: (d)

  1. Closed pipe: n0=v4L=400n_0 = \frac{v}{4L} = 400 Hz.
  2. With 13\frac{1}{3} filled, air column =2L3= \frac{2L}{3}, new fundamental =400×32=600= 400 \times \frac{3}{2} = 600 Hz.
  3. A closed pipe gives only odd harmonics, so the next (second) note is the 3rd harmonic: 3×600=18003 \times 600 = 1800 Hz.
  4. So the answer is (d) 1800 Hz.
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Q375MHT CET 2025 · 20 APR · SHIFT 2Medium

Organ Pipes & Resonance Tube · Joined pipes, gases and string-pipe resonance

The frequency of a stretched uniform wire of length LL under tension is in resonance with the fundamental frequency of a closed pipe of same length. If the tension in the wire is increased by 8 N, it is in resonance with the first overtone of the same closed pipe. The initial tension in the wire is

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Answer: (d)

  1. String frequency f∝Tf \propto \sqrt{T}; closed pipe first overtone =3×= 3 \times fundamental.
  2. T+8T=3⇒T+8=9T\sqrt{\frac{T + 8}{T}} = 3 \Rightarrow T + 8 = 9T
  3. T=1T = 1 N
  4. So the answer is (d) 1 N.
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Q376MHT CET 2025 · 20 APR · SHIFT 1Medium

Organ Pipes & Resonance Tube · Joined pipes, gases and string-pipe resonance

Two pipes of lengths L1L_1 and L2L_2, open at both ends are joined in series. If ' f1f_1 ' and ' f2f_2 ' are the fundamental frequencies of two pipes, then the fundamental frequency of series combination will be (neglect end correction)

Show answer and solution

Answer: (c)

  1. Open pipes: L1=v2f1L_1 = \frac{v}{2f_1}, L2=v2f2L_2 = \frac{v}{2f_2}.
  2. Combined open pipe: f=v2(L1+L2)=11f1+1f2f = \frac{v}{2(L_1 + L_2)} = \frac{1}{\frac{1}{f_1} + \frac{1}{f_2}}
  3. f=f1f2f1+f2f = \frac{f_1 f_2}{f_1 + f_2}, so the answer is (c).
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Q377MHT CET 2025 · 21 APR · SHIFT 1Difficult

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

A pipe open at both ends of length 1.5 m is dipped in water at one end such that 22nd overtone of vibrating air column is resonating with a tuning fork of frequency 330 Hz. The length of the pipe immersed in water is (Speed of sound in air =330 m/s= 330\text{ m/s}) (Neglect end correction)

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Answer: (d)

  1. Dipped in water, the pipe acts as a closed pipe of air length ll
  2. 2nd overtone of closed pipe = 5th harmonic: f=5v4lf = \frac{5v}{4l}
  3. 330=5×3304l⇒l=1.25 m330 = \frac{5 \times 330}{4l} \Rightarrow l = 1.25\text{ m}
  4. Immersed length =1.5−1.25=0.25 m= 1.5 - 1.25 = 0.25\text{ m}
  5. So the answer is (d) 0.25 m.
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Q378JEE Main 2025 · 22 JAN · SHIFT 1Difficult

Organ Pipes & Resonance Tube · Joined pipes, gases and string-pipe resonance

A closed organ and an open organ tube are filled by two different gases having same bulk modulus but different densities ρ1\rho_1 and ρ2\rho_2, respectively. The frequency of 99th harmonic of closed tube is identical with 44th harmonic of open tube. If the length of the closed tube is 10 cm and the density ratio of the gases is ρ1:ρ2=1:16\rho_1 : \rho_2 = 1 : 16, then the length of the open tube is:

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Answer: (b)

  1. Closed tube 9th harmonic: 9v14Lc\frac{9v_1}{4L_c}; open tube 4th harmonic: 4v22Lo=2v2Lo\frac{4v_2}{2L_o} = \frac{2v_2}{L_o}
  2. Equate: Lo=8Lc9v2v1L_o = \frac{8L_c}{9}\frac{v_2}{v_1}
  3. Same BB: v2v1=ρ1ρ2=116=14\frac{v_2}{v_1} = \sqrt{\frac{\rho_1}{\rho_2}} = \sqrt{\frac{1}{16}} = \frac{1}{4}
  4. Lo=8×109×4=209 cmL_o = \frac{8 \times 10}{9 \times 4} = \frac{20}{9}\text{ cm}
  5. So the answer is (b) 209 cm\frac{20}{9}\text{ cm}.
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Q379MHT CET 2024 · 2 MAY · SHIFT 1Easy

Organ Pipes & Resonance Tube · Closed organ pipe

An air column in a closed organ pipe vibrating in unison with a fork, produces second overtone. The vibrating air column has

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Answer: (b)

  1. Second overtone of a closed pipe: L=5λ4L=\frac{5\lambda}{4}.
  2. From the closed end: N A N A N A, giving 3 nodes and 3 antinodes.
  3. So the answer is (b).
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Q380MHT CET 2024 · 16 MAY · SHIFT 2Easy

Organ Pipes & Resonance Tube · Open organ pipe

A pipe 60 cm long and open at both the ends produces harmonics. Which harmonic mode of pipe resonates a 2.2 KHz source? (Speed of sound in air =330 m/s)(= 330\text{ m/s})( Neglect end correction)

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Answer: (b)

  1. Fundamental n=v2L=3302×0.6=275 Hzn=\frac{v}{2L}=\frac{330}{2\times0.6}=275\text{ Hz}.
  2. 2200275=8\frac{2200}{275}=8
  3. So it is the eighth harmonic: answer (b).
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Q381MHT CET 2024 · 10 MAY · SHIFT 1Easy

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The pipe open at both ends and pipe closed at one end have same length and both are vibrating in fundamental mode. Air column vibrating in open pipe has resonance frequency n1n_1 and air column vibrating in closed pipe has resonance frequency n2n_2, then

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Answer: (a)

  1. n1=v2Ln_1=\frac{v}{2L}, n2=v4Ln_2=\frac{v}{4L} for the same length.
  2. n1=2n2n_1=2n_2, so the answer is (a).
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Q382JEE Main 2024 · 31 JAN · SHIFT 1Easy

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The fundamental frequency of a closed organ pipe is equal to the first overtone frequency of an open organ pipe. If length of the open pipe is 60 cm60\text{ cm}, the length of the closed pipe will be:

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Answer: (a)

  1. First overtone of open pipe: 2v2Lo=vLo\frac{2v}{2L_o}=\frac{v}{L_o}. Closed fundamental: v4Lc\frac{v}{4L_c}.
  2. v4Lc=vLo⇒Lc=Lo4=604\frac{v}{4L_c}=\frac{v}{L_o} \Rightarrow L_c=\frac{L_o}{4}=\frac{60}{4}
  3. Lc=15 cmL_c=15\text{ cm}, so the answer is (a).
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Q383JEE Main 2024 · 8 APR · SHIFT 1Easy

Organ Pipes & Resonance Tube · Comparing closed and open pipes

A closed and an open organ pipe have same lengths. If the ratio of frequencies of their seventh overtones is (a−1a)\left(\frac{a-1}{a}\right) then the value of aa is _________.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 16

  1. Seventh overtone of closed pipe = 15th harmonic: 15v4L\frac{15v}{4L}.
  2. Seventh overtone of open pipe = 8th harmonic: 8v2L=16v4L\frac{8v}{2L}=\frac{16v}{4L}.
  3. Ratio =1516=a−1a⇒a=16=\frac{15}{16}=\frac{a-1}{a} \Rightarrow a=16
  4. a=16a=16
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Q384MHT CET 2024 · 3 MAY · SHIFT 1Easy

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

The fundamental frequency of an air column in a pipe open at both ends is ' f1f_1 '. Now 80%80\% of its length is immersed in water, the fundamental frequency of the air column becomes f2f_2. The ratio of f1:f2f_1 : f_2 is

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Answer: (d)

  1. Open pipe: f1=v2Lf_1 = \frac{v}{2L}.
  2. 80%80\% in water leaves a closed pipe of length 0.2L0.2L: f2=v4(0.2L)=v0.8Lf_2 = \frac{v}{4(0.2L)} = \frac{v}{0.8L}.
  3. f1f2=0.8L2L=25\frac{f_1}{f_2} = \frac{0.8L}{2L} = \frac{2}{5}
  4. So the answer is (d) 2:52 : 5.
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Q385MHT CET 2024 · 3 MAY · SHIFT 2Easy

Organ Pipes & Resonance Tube · Resonance tube and end correction

If ' ll ' is the length of pipe, ' rr ' is the internal radius of the pipe and ' vv ' is the velocity of sound in air then fundamental frequency of open pipe is

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Answer: (a)

  1. End correction at each open end e=0.6re = 0.6r; an open pipe has two ends, so effective length =l+1.2r= l + 1.2r.
  2. Fundamental of open pipe: f=V2(l+1.2r)f = \frac{V}{2(l + 1.2r)}
  3. So the answer is (a) V2(l+1.2r)\frac{V}{2(l+1.2r)}.
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Q386JEE Main 2024 · 6 APR · SHIFT 2Medium

Organ Pipes & Resonance Tube · Open organ pipe

Two open organ pipes of lengths 60 cm60\text{ cm} and 90 cm90\text{ cm} resonate at 66th and 55th harmonics respectively. The difference of frequencies for the given modes is _________ Hz\text{Hz}. (Velocity of sound in air =333 m/s= 333\text{ m/s})

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 740

  1. Open pipe: fn=nv2Lf_n = \frac{nv}{2L}.
  2. f6=6×3332×0.6=1665 Hzf_6 = \frac{6 \times 333}{2 \times 0.6} = 1665\text{ Hz}
  3. f5=5×3332×0.9=925 Hzf_5 = \frac{5 \times 333}{2 \times 0.9} = 925\text{ Hz}
  4. Difference =1665−925=740 Hz= 1665 - 925 = 740\text{ Hz}
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Q387MHT CET 2024 · 11 MAY · SHIFT 2Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The frequency of the third overtone of a pipe of length ' LcL_c ', closed at one end is same as the frequency of the sixth overtone of a pipe of length ' L0L_0 ', open at both ends. Then the ratio Lc:L0L_c : L_0 is

Show answer and solution

Answer: (b)

  1. Closed pipe third overtone = 7th harmonic: 7v4Lc\frac{7v}{4L_c}.
  2. Open pipe sixth overtone = 7th harmonic: 7v2L0\frac{7v}{2L_0}.
  3. 7v4Lc=7v2L0⇒4Lc=2L0⇒Lc:L0=1:2\frac{7v}{4L_c} = \frac{7v}{2L_0} \Rightarrow 4L_c = 2L_0 \Rightarrow L_c : L_0 = 1 : 2
  4. So the answer is (b) 1:21:2.
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Q388MHT CET 2024 · 15 MAY · SHIFT 2Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

The end correction for the vibrations of air column in a tube of circular cross-section will be more if the tube is

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Answer: (d)

  1. End correction e=0.3de = 0.3d (open end, circular tube), so it depends only on the diameter, not the length.
  2. Widening the tube increases dd, so ee increases.
  3. So the answer is (d) widened.
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Q389MHT CET 2024 · 11 MAY · SHIFT 1Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

A resonance tube closed at one end is of height 1.5 m. A tuning fork of frequency 340 Hz is vibrating above the tube. Water is poured in the tube gradually. The minimum height of water column for which resonance is obtained is (Neglect end correction, speed of sound in air =340 m/s= 340\text{ m/s})

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Answer: (d)

  1. λ=vn=340340=1\lambda = \frac{v}{n} = \frac{340}{340} = 1 m.
  2. Resonating air-column lengths: λ4,3λ4,5λ4=25,75,125\frac{\lambda}{4}, \frac{3\lambda}{4}, \frac{5\lambda}{4} = 25, 75, 125 cm (all within 150 cm).
  3. Minimum water height uses the longest air column: 150−125=25150 - 125 = 25 cm
  4. So the answer is (d) 25 cm.
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Q390MHT CET 2024 · 10 MAY · SHIFT 2Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

The end correction for the vibrations of air column in a tube of circular cross-section will be more if the tube is

Show answer and solution

Answer: (d)

  1. End correction e=0.3de = 0.3d (open end, circular tube), so it depends only on the diameter, not the length.
  2. Widening the tube increases dd, so ee increases.
  3. So the answer is (d) widened.
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Q391MHT CET 2024 · 9 MAY · SHIFT 1Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

A tuning fork of frequency 340 Hz is vibrated just above a tube of 120 cm height. Water is slowly poured in the tube. What is the minimum height of water necessary for resonance?

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Answer: (a)

  1. Taking v=340v = 340 m/s: λ=340340=1\lambda = \frac{340}{340} = 1 m.
  2. Resonating lengths: 25,75,12525, 75, 125 cm; within 120 cm the longest is 75 cm.
  3. Minimum water height =120−75=45= 120 - 75 = 45 cm
  4. So the answer is (a) 45 cm.
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Q392MHT CET 2024 · 3 MAY · SHIFT 2Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

The end correction of resonance tube is 1 cm. If the shortest length resonating with a tuning fork is 15 cm, the next resonating length will be

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Answer: (c)

  1. l1+e=λ4⇒λ4=15+1=16l_1 + e = \frac{\lambda}{4} \Rightarrow \frac{\lambda}{4} = 15 + 1 = 16 cm.
  2. l2+e=3λ4=48l_2 + e = \frac{3\lambda}{4} = 48 cm ⇒l2=48−1=47\Rightarrow l_2 = 48 - 1 = 47 cm
  3. So the answer is (c) 47 cm.
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Q393JEE Main 2024 · 30 JAN · SHIFT 1Difficult

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

In a closed organ pipe, the frequency of fundamental note is 30 Hz30\text{ Hz}. A certain amount of water is now poured in the organ pipe so that the fundamental frequency is increased to 110 Hz110\text{ Hz}. If the organ pipe has a cross-sectional area of 2 cm22\text{ cm}^{2}, the amount of water poured in the organ tube is __________ g. (Take speed of sound in air is 330 m/s330\text{ m/s})

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 400

  1. Closed pipe fundamental: f=v4L⇒L=v4ff = \frac{v}{4L} \Rightarrow L = \frac{v}{4f}
  2. Before: L1=3304×30=2.75 mL_1 = \frac{330}{4 \times 30} = 2.75\text{ m}; after: L2=3304×110=0.75 mL_2 = \frac{330}{4 \times 110} = 0.75\text{ m}
  3. Water column height =2 m=200 cm= 2\text{ m} = 200\text{ cm}
  4. Volume =200×2=400 cm3= 200 \times 2 = 400\text{ cm}^3, mass =400 g= 400\text{ g} (density 1 g/cm31\text{ g/cm}^3)
  5. Answer: 400 g400\text{ g}
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Q394MHT CET 2023 · 9 MAY · SHIFT 2Easy

Organ Pipes & Resonance Tube · Open organ pipe

If the length of an open organ pipe is 33.3 cm33.3\text{ cm}, then the frequency of fifth overtone is [Neglect end correction, velocity of sound =333 m/s= 333\text{ m/s} ]

Show answer and solution

Answer: (b)

  1. Fundamental n=v2L=3332×0.333=500 Hzn=\frac{v}{2L}=\frac{333}{2\times0.333}=500\text{ Hz}.
  2. Fifth overtone of an open pipe is the 6th harmonic: 6×5006\times500.
  3. 3000 Hz3000\text{ Hz}, so the answer is (b).
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Q395JEE Main 2023 · 8 APR · SHIFT 1Easy

Organ Pipes & Resonance Tube · Open organ pipe

An organ pipe 40 cm40\text{ cm} long is open at both ends. The speed of sound in air is 360 ms−1360\text{ ms}^{-1}. The frequency of the second harmonic is ___________ Hz\text{Hz}.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 900

  1. Open pipe: np=pv2Ln_p=\frac{p v}{2L}.
  2. n2=2×3602×0.40n_2=\frac{2\times360}{2\times0.40}
  3. n2=900 Hzn_2=900\text{ Hz}
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Q396NEET 2023Easy

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The ratio of frequencies of fundamental harmonic produced by an open pipe to that of closed pipe having the same length is

Show answer and solution

Answer: (a)

  1. nopennclosed=v/2Lv/4L=2\frac{n_{open}}{n_{closed}}=\frac{v/2L}{v/4L}=2
  2. So the answer is (a) 2:12:1.
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Q397MHT CET 2023 · 14 MAY · SHIFT 1Easy

Organ Pipes & Resonance Tube · Resonance tube and end correction

If 'll' is the length of the open pipe, 'rr' is the internal radius of the pipe and 'VV ' is the velocity of sound in air then fundamental frequency of open pipe is

Show answer and solution

Answer: (d)

  1. End correction at each open end e=0.6re = 0.6r; an open pipe has two ends, so effective length =l+1.2r= l + 1.2r.
  2. Fundamental of open pipe: f=V2(l+1.2r)f = \frac{V}{2(l + 1.2r)}
  3. So the answer is (d) V2(l+1.2r)\frac{V}{2(l+1.2r)}.
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Q398MHT CET 2023 · 9 MAY · SHIFT 2Easy

Organ Pipes & Resonance Tube · Resonance tube and end correction

If the end correction of an open pipe is 0.8 cm0.8\text{ cm}, then the inner radius of that pipe is

Show answer and solution

Answer: (b)

  1. An open pipe has two open ends, so its total end correction is 2(0.6r)=1.2r2(0.6r) = 1.2r.
  2. 1.2r=0.8⇒r=0.81.2=23 cm1.2r = 0.8 \Rightarrow r = \frac{0.8}{1.2} = \frac{2}{3}\text{ cm}
  3. So the answer is (b) 23 cm\frac{2}{3}\text{ cm}.
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Q399JEE Main 2023 · 12 APR · SHIFT 1Medium

Organ Pipes & Resonance Tube · Closed organ pipe

For a certain organ pipe, the first three resonance frequencies are in the ratio of 1:3:51 : 3 : 5 respectively. If the frequency of fifth harmonic is 405 Hz405\text{ Hz} and the speed of sound in air is 324 ms−1324\text{ ms}^{-1} the length of the organ pipe is _________ m\text{m}.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 1

  1. Ratio 1:3:51 : 3 : 5 means odd harmonics only, so it is a closed pipe: fn=nv4Lf_n = \frac{nv}{4L}.
  2. Fifth harmonic: 5v4L=405⇒f0=81 Hz\frac{5v}{4L} = 405 \Rightarrow f_0 = 81\text{ Hz}
  3. L=v4f0=3244×81=1 mL = \frac{v}{4f_0} = \frac{324}{4 \times 81} = 1\text{ m}
  4. So the length is 1 m1\text{ m}.
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Q400MHT CET 2023 · 13 MAY · SHIFT 2Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

A closed pipe and an open pipe have their first overtone equal in frequency. Then, the lengths of these pipe are in the ratio

Show answer and solution

Answer: (c)

  1. Closed pipe first overtone: 3v4Lc\frac{3v}{4L_c}; open pipe first overtone: 2v2Lo=vLo\frac{2v}{2L_o} = \frac{v}{L_o}.
  2. 3v4Lc=vLo⇒Lc:Lo=3:4\frac{3v}{4L_c} = \frac{v}{L_o} \Rightarrow L_c : L_o = 3 : 4
  3. So the answer is (c) 3:43:4.
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Q401MHT CET 2023 · 11 MAY · SHIFT 1Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The second overtone of an open pipe has the same frequency as the first overtone of a closed pipe of length 'LL'. The length of the open pipe will be

Show answer and solution

Answer: (c)

  1. Open pipe second overtone: 3v2Lo\frac{3v}{2L_o}; closed pipe first overtone: 3v4L\frac{3v}{4L}.
  2. 3v2Lo=3v4L⇒Lo=2L\frac{3v}{2L_o} = \frac{3v}{4L} \Rightarrow L_o = 2L
  3. So the answer is (c) 2L2L.
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Q402MHT CET 2023 · 10 MAY · SHIFT 2Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The fundamental frequency of air column in pipe 'A' closed at one end is in unison with second overtone of an air column in pipe 'B' open at both ends. The ratio of length of air column in pipe 'AA' to that of air column in pipe 'BB' is

Show answer and solution

Answer: (a)

  1. Pipe A (closed) fundamental: v4LA\frac{v}{4L_A}; pipe B (open) second overtone: 3v2LB\frac{3v}{2L_B}.
  2. v4LA=3v2LB⇒12LA=2LB⇒LA:LB=1:6\frac{v}{4L_A} = \frac{3v}{2L_B} \Rightarrow 12L_A = 2L_B \Rightarrow L_A : L_B = 1 : 6
  3. So the answer is (a) 1:61:6.
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Q403NEET 2023Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The 44th overtone of a closed organ pipe is same as that of 33rd overtone of an open pipe. The ratio of the length of the closed pipe to the length of the open pipe is:

Show answer and solution

Answer: (c)

  1. Closed pipe 4th overtone = 9th harmonic: 9v4Lc\frac{9v}{4L_c}.
  2. Open pipe 3rd overtone = 4th harmonic: 4v2Lo=2vLo\frac{4v}{2L_o} = \frac{2v}{L_o}.
  3. 9v4Lc=2vLo⇒Lc:Lo=9:8\frac{9v}{4L_c} = \frac{2v}{L_o} \Rightarrow L_c : L_o = 9 : 8
  4. So the answer is (c) 9:89:8.
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Q404MHT CET 2023 · 13 MAY · SHIFT 1Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

In resonance tube, first and second resonance are obtained at depths 22.7 cm22.7\text{ cm} and 70.2 cm70.2\text{ cm} respectively. The third resonance will be obtained at a depth

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Answer: (a)

  1. Successive resonances differ by λ2\frac{\lambda}{2}: λ2=70.2−22.7=47.5\frac{\lambda}{2} = 70.2 - 22.7 = 47.5 cm.
  2. Third resonance: l3=l2+λ2=70.2+47.5=117.7l_3 = l_2 + \frac{\lambda}{2} = 70.2 + 47.5 = 117.7 cm
  3. So the answer is (a) 117.7 cm.
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Q405MHT CET 2023 · 12 MAY · SHIFT 2Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

End correction at open end for air column in a pipe of length 'll' is 'ee'. For its second overtone of an open pipe, the wavelength of the wave is

Show answer and solution

Answer: (b)

  1. An open pipe has end correction at both ends: effective length =l+2e= l + 2e.
  2. Second overtone = 3rd harmonic: l+2e=3λ2l + 2e = \frac{3\lambda}{2}.
  3. λ=2(l+2e)3\lambda = \frac{2(l + 2e)}{3}
  4. So the answer is (b) 2(l+2e)3\frac{2(l+2e)}{3}.
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Q406MHT CET 2023 · 10 MAY · SHIFT 1Medium

Organ Pipes & Resonance Tube · Joined pipes, gases and string-pipe resonance

An open organ pipe having fundamental frequency (n) is in unison with a vibrating string. If the tube is dipped in water so that 75%75\% of the length of the tube is inside the water then the ratio of fundamental frequency of the air column of dipped tube with that of string will be (Neglect end corrections)

Show answer and solution

Answer: (b)

  1. Open pipe: n=v2Ln = \frac{v}{2L} = string frequency.
  2. Dipped 75%: closed pipe of length L4\frac{L}{4}, fundamental =v4⋅L/4=vL=2n= \frac{v}{4 \cdot L/4} = \frac{v}{L} = 2n.
  3. Ratio 2n:n=2:12n : n = 2 : 1
  4. So the answer is (b) 2:12:1.
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Q407MHT CET 2023 · 9 MAY · SHIFT 1Difficult

Organ Pipes & Resonance Tube · Joined pipes, gases and string-pipe resonance

A closed organ pipe of length 'L1L_1' and an open organ pipe contain diatomic gases of densities 'ρ1\rho_1 ' and 'ρ2\rho_2' respectively. The compressibilities of the gases are same in both pipes, which are vibrating in their first overtone with same frequency. The length of the open organ pipe is (Neglect end correction)

Show answer and solution

Answer: (b)

  1. Speed v=Bρv = \sqrt{\frac{B}{\rho}}; same BB, so v2v1=ρ1ρ2\frac{v_2}{v_1} = \sqrt{\frac{\rho_1}{\rho_2}}
  2. Closed pipe first overtone: 3v14L1\frac{3v_1}{4L_1}; open pipe first overtone: v2Lo\frac{v_2}{L_o}
  3. Equate: Lo=4L13v2v1=4L13ρ1ρ2L_o = \frac{4L_1}{3}\frac{v_2}{v_1} = \frac{4L_1}{3}\sqrt{\frac{\rho_1}{\rho_2}}
  4. So the answer is (b).
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Q408JEE Main 2022 · 25 JUN · SHIFT 1Easy

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The first overtone frequency of an open organ pipe is equal to the fundamental frequency of a closed organ pipe. If the length of the closed organ pipe is 20 cm, the length of the open organ pipe is _____________ cm.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 80

  1. First overtone of open pipe: vLo\frac{v}{L_o}. Closed fundamental: v4Lc\frac{v}{4L_c}.
  2. vLo=v4Lc⇒Lo=4Lc=4×20\frac{v}{L_o}=\frac{v}{4L_c} \Rightarrow L_o=4L_c=4\times20
  3. Lo=80 cmL_o=80\text{ cm}
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Q409JEE Main 2022 · 29 JUN · SHIFT 2Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

In an experiment to determine the velocity of sound in air at room temperature using a resonance tube, the first resonance is observed when the air column has a length of 20.0 cm for a tuning fork of frequency 400 Hz is used. The velocity of the sound at room temperature is 336 ms−1{}^{-1}. The third resonance is observed when the air column has a length of _____________ cm.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 104

  1. λ=336400=0.84\lambda = \frac{336}{400} = 0.84 m =84= 84 cm, so λ4=21\frac{\lambda}{4} = 21 cm.
  2. First resonance: 20+e=21⇒e=120 + e = 21 \Rightarrow e = 1 cm.
  3. Third resonance: l3=5λ4−e=105−1=104l_3 = \frac{5\lambda}{4} - e = 105 - 1 = 104 cm
  4. So the answer is 104 cm.
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Q410JEE Main 2022 · 28 JUN · SHIFT 2Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

A tuning fork of frequency 340 Hz resonates in the fundamental mode with an air column of length 125 cm in a cylindrical tube closed at one end. When water is slowly poured in it, the minimum height of water required for observing resonance once again is ___________ cm.

(Velocity of sound in air is 340 ms−1{}^{-1})

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 50

  1. λ=340340=1\lambda = \frac{340}{340} = 1 m, so resonating lengths are 25,75,12525, 75, 125 cm.
  2. The 125 cm column is the 5λ4\frac{5\lambda}{4} resonance; as water is poured the column shortens to the next resonance at 75 cm.
  3. Water height needed =125−75=50= 125 - 75 = 50 cm
  4. So the answer is 50 cm.
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Q411MHT CET 2022 · 11 AUG · SHIFT 2Difficult

Organ Pipes & Resonance Tube · Joined pipes, gases and string-pipe resonance

A hollow pipe of length 0.8 m0.8\text{ m} is closed at one end. At its open end, a 0.5 m0.5\text{ m} long uniform string is vibrating in its second harmonic and it resonates with the fundamental frequency of pipe. If the tension in the string is 50 N50\text{ N} and speed of sound in air is 320 m/s320\text{ m/s}, the mass of the string is

Show answer and solution

Answer: (a)

  1. Pipe fundamental: f=v4L=3204×0.8=100 Hzf = \frac{v}{4L} = \frac{320}{4 \times 0.8} = 100\text{ Hz}
  2. String 2nd harmonic: f=22lTμ=10.550μf = \frac{2}{2l}\sqrt{\frac{T}{\mu}} = \frac{1}{0.5}\sqrt{\frac{50}{\mu}}
  3. 250μ=100⇒μ=0.02 kg/m2\sqrt{\frac{50}{\mu}} = 100 \Rightarrow \mu = 0.02\text{ kg/m}
  4. Mass =μl=0.02×0.5=0.01 kg=10 g= \mu l = 0.02 \times 0.5 = 0.01\text{ kg} = 10\text{ g}
  5. So the answer is (b) 10 g.
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Q412MHT CET 2021 · 20 SEP · SHIFT 2Easy

Organ Pipes & Resonance Tube · Closed organ pipe

An air column in a pipe, which is closed at one end will be in resonance with a vibrating tuning fork of frequency 264 Hz for various lengths. Which one of the following lengths is not possible? (V = 330 m/s)

Show answer and solution

Answer: (a)

  1. λ=330264=1.25 m\lambda=\frac{330}{264}=1.25\text{ m}, so λ4=31.25 cm\frac{\lambda}{4}=31.25\text{ cm}.
  2. Possible lengths are odd multiples: 31.25,93.75,156.25 cm…31.25, 93.75, 156.25\text{ cm} \ldots
  3. 62.50 cm=2×λ462.50\text{ cm}=2\times\frac{\lambda}{4} is not possible, so the answer is (a).
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Q413JEE Main 2021 · 27 AUG · SHIFT 2Easy

Organ Pipes & Resonance Tube · Closed organ pipe

A tuning fork is vibrating at 250 Hz. The length of the shortest closed organ pipe that will resonate with the tuning fork will be __________ cm. (Take speed of sound in air as 340 ms−1{}^{-1})

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 34

  1. Shortest closed pipe: L=λ4=v4fL=\frac{\lambda}{4}=\frac{v}{4f}.
  2. L=3404×250=0.34 mL=\frac{340}{4\times250}=0.34\text{ m}
  3. L=34 cmL=34\text{ cm}
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Q414MHT CET 2021 · 24 SEP · SHIFT 1Easy

Organ Pipes & Resonance Tube · Open organ pipe

When an air column in a pipe open at both ends vibrates such that four antinodes and three nodes are formed, then the corresponding mode of vibration is

Show answer and solution

Answer: (b)

  1. An open pipe in the pp-th harmonic has pp nodes and p+1p+1 antinodes.
  2. 3 nodes, 4 antinodes ⇒p=3\Rightarrow p=3, the third harmonic.
  3. Third harmonic = second overtone, so the answer is (b).
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Q415MHT CET 2021 · 24 SEP · SHIFT 2Easy

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

A cylindrical tube open at both ends has fundamental frequency 'n' in air. The tube is dipped vertically in water so that one-fourth of it is in water. The fundamental frequency of the air column becomes

Show answer and solution

Answer: (d)

  1. Open pipe: n=v2Ln = \frac{v}{2L}.
  2. One-fourth in water leaves a closed pipe of length 3L4\frac{3L}{4}: n′=v4(3L/4)=v3Ln' = \frac{v}{4(3L/4)} = \frac{v}{3L}.
  3. n′=23⋅v2L=2n3n' = \frac{2}{3}\cdot\frac{v}{2L} = \frac{2n}{3}
  4. So the answer is (d) 2n3\frac{2n}{3}.
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Q416MHT CET 2021 · 21 SEP · SHIFT 1Medium

Organ Pipes & Resonance Tube · Closed organ pipe

In fundamental mode, the time required for the sound wave to reach upto the closed end of pipe filled with air is tt second. The frequency of vibration of air column is

Show answer and solution

Answer: (d)

  1. Fundamental of closed pipe: f=v4Lf = \frac{v}{4L}.
  2. Time to travel the pipe length: t=Lvt = \frac{L}{v}.
  3. f=14t=0.25tf = \frac{1}{4t} = \frac{0.25}{t}
  4. So the answer is (d) 0.25t\frac{0.25}{t}.
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Q417MHT CET 2021 · 20 SEP · SHIFT 2Medium

Organ Pipes & Resonance Tube · Closed organ pipe

Two consecutive harmonics of an air column in a pipe closed at one end are of frequencies 150 Hz and 250 Hz. The fundamental frequency of an air column is

Show answer and solution

Answer: (d)

  1. A closed pipe has only odd harmonics, so consecutive harmonics differ by 2f02f_0.
  2. 2f0=250−150=100⇒f0=50 Hz2f_0 = 250 - 150 = 100 \Rightarrow f_0 = 50\text{ Hz}
  3. Check: 150=3f0150 = 3f_0, 250=5f0250 = 5f_0.
  4. So the answer is (d) 50 Hz.
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Q418MHT CET 2021 · 23 SEP · SHIFT 1Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The fundamental frequency of an air column in pipe 'A' closed at one end coincides with second overtone of pipe 'B' open at both ends. The ratio of length of pipe 'A' to that of pipe 'B' is

Show answer and solution

Answer: (c)

  1. Pipe A (closed) fundamental: v4LA\frac{v}{4L_A}; pipe B (open) second overtone: 3v2LB\frac{3v}{2L_B}.
  2. v4LA=3v2LB⇒LA:LB=2:12=1:6\frac{v}{4L_A} = \frac{3v}{2L_B} \Rightarrow L_A : L_B = 2 : 12 = 1 : 6
  3. So the answer is (c) 1:61:6.
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Q419MHT CET 2021 · 22 SEP · SHIFT 2Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

A tuning fork of frequency 'nn' is held near the open end of tube which is closed at the other end and the lengths are adjusted until resonance occurs. The first resonance occurs at length L1L_1 and immediate next resonance occurs at length L2L_2. The speed of sound in air is

Show answer and solution

Answer: (c)

  1. First two resonances: L1+e=λ4L_1 + e = \frac{\lambda}{4}, L2+e=3λ4L_2 + e = \frac{3\lambda}{4}.
  2. Subtract: L2−L1=λ2⇒λ=2(L2−L1)L_2 - L_1 = \frac{\lambda}{2} \Rightarrow \lambda = 2(L_2 - L_1).
  3. v=nλ=2n(L2−L1)v = n\lambda = 2n(L_2 - L_1)
  4. So the answer is (c) 2n(L2−L1)2n(L_2 - L_1).
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Q420MHT CET 2021 · 22 SEP · SHIFT 2Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

A glass tube of 1 m1\text{ m} length is filled with water. The water can be drained out slowly from the bottom of the tube. If vibrating tuning fork of frequency 500 Hz500\text{ Hz} is brought at the upper end of the tube then total number of resonances obtained are [Velocity of sound in air is 320 ms−1320\text{ ms}^{-1} ]

Show answer and solution

Answer: (a)

  1. λ=320500=0.64\lambda = \frac{320}{500} = 0.64 m, so λ4=0.16\frac{\lambda}{4} = 0.16 m.
  2. Resonating lengths: (2k−1)λ4=0.16,0.48,0.80,1.12\frac{(2k-1)\lambda}{4} = 0.16, 0.48, 0.80, 1.12 m...
  3. Only lengths up to 1 m are possible: 0.16, 0.48, 0.80 m, i.e. 3 resonances.
  4. So the answer is (a) 3.
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Q421JEE Main 2021 · 25 FEB · SHIFT 1Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

A student is performing the experiment of resonance column. The diameter of the column tube is 6 cm. The frequency of the tuning fork is 504 Hz. Speed of the sound at the given temperature is 336 m/s. The zero of the metre scale coincides with the top end of the resonance column tube. The reading of the water level in the column when the first resonance occurs is:

Show answer and solution

Answer: (d)

  1. λ=336504=0.667\lambda = \frac{336}{504} = 0.667 m, so λ4=16.67\frac{\lambda}{4} = 16.67 cm.
  2. End correction e=0.3d=0.3×6=1.8e = 0.3d = 0.3 \times 6 = 1.8 cm.
  3. First resonance: l1=λ4−e=16.67−1.8≈14.8l_1 = \frac{\lambda}{4} - e = 16.67 - 1.8 \approx 14.8 cm
  4. So the answer is (d) 14.8 cm.
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Q422JEE Main 2021 · 16 MAR · SHIFT 2Medium

Organ Pipes & Resonance Tube · Joined pipes, gases and string-pipe resonance

A closed organ pipe of length L and an open organ pipe contain gases of densities ρ\rho1 and ρ\rho2 respectively. The compressibility of gases are equal in both the pipes. Both the pipes are vibrating in their first overtone with same frequency. The length of the open pipe is x3Lρ1ρ2\frac{x}{3} L \sqrt{\frac{\rho_1}{\rho_2}} where x is ___________. (Round off to the Nearest Integer)

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 4

  1. Speed v=Bρv = \sqrt{\frac{B}{\rho}}; same BB, so v2v1=ρ1ρ2\frac{v_2}{v_1} = \sqrt{\frac{\rho_1}{\rho_2}}
  2. Closed pipe first overtone: 3v14L\frac{3v_1}{4L}; open pipe first overtone: 2v22Lo=v2Lo\frac{2v_2}{2L_o} = \frac{v_2}{L_o}
  3. Equate: Lo=4L3v2v1=43Lρ1ρ2L_o = \frac{4L}{3}\frac{v_2}{v_1} = \frac{4}{3}L\sqrt{\frac{\rho_1}{\rho_2}}
  4. So x=4x = 4.
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Q423MHT CET 2021 · 22 SEP · SHIFT 1Difficult

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

A pipe open at both ends of length 1.5 m is dipped in water such that the second overtone of vibrating air column is resonating with a tuning fork of frequency 330 Hz. If speed of sound in air is 330 m/s then the length of the pipe immersed in water is (Neglect and correction)

Show answer and solution

Answer: (b)

  1. Dipped in water, the pipe acts as a closed pipe of air length ll
  2. 2nd overtone of closed pipe = 5th harmonic: f=5v4lf = \frac{5v}{4l}
  3. 330=5×3304l⇒l=1.25 m330 = \frac{5 \times 330}{4l} \Rightarrow l = 1.25\text{ m}
  4. Immersed length =1.5−1.25=0.25 m= 1.5 - 1.25 = 0.25\text{ m}
  5. So the answer is (b) 0.25 m.
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Q424MHT CET 2021 · 21 SEP · SHIFT 2Difficult

Organ Pipes & Resonance Tube · Joined pipes, gases and string-pipe resonance

A pipe closed at one end has length 0.8 m0.8\text{ m}. At its open end 0.5 m0.5\text{ m} long uniform string is vibrating in its 22nd harmonic and it resonates with the fundamental frequency of the pipe. If the tension in the wire is 50 N50\text{ N} and the speed of sound is 320 m/s320\text{ m/s}, the mass of the string is

Show answer and solution

Answer: (b)

  1. Pipe fundamental: f=v4L=3204×0.8=100 Hzf = \frac{v}{4L} = \frac{320}{4 \times 0.8} = 100\text{ Hz}
  2. String 2nd harmonic: f=22lTμ=10.550μf = \frac{2}{2l}\sqrt{\frac{T}{\mu}} = \frac{1}{0.5}\sqrt{\frac{50}{\mu}}
  3. 250μ=100⇒μ=0.02 kg/m2\sqrt{\frac{50}{\mu}} = 100 \Rightarrow \mu = 0.02\text{ kg/m}
  4. Mass =μl=0.02×0.5=0.01 kg=10 g= \mu l = 0.02 \times 0.5 = 0.01\text{ kg} = 10\text{ g}
  5. So the answer is (b) 10 gram.
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Q425MHT CET 2021 · 21 SEP · SHIFT 1Difficult

Organ Pipes & Resonance Tube · Joined pipes, gases and string-pipe resonance

A closed organ pipe of length 'LcL_c' and an open organ pipe of length 'LoL_o' contain different gases of densities 'ρ1\rho_1' and 'ρ2\rho_2' respectively. The compressibility of the gases is the same in both the pipes. The gases are vibrating in their first overtone with the same frequency. What is the length of open organ pipe?

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Answer: (a)

  1. Speed v=Bρv = \sqrt{\frac{B}{\rho}}; same BB, so v2v1=ρ1ρ2\frac{v_2}{v_1} = \sqrt{\frac{\rho_1}{\rho_2}}
  2. Closed pipe first overtone: 3v14Lc\frac{3v_1}{4L_c}; open pipe first overtone: v2Lo\frac{v_2}{L_o}
  3. Equate: Lo=4Lc3ρ1ρ2L_o = \frac{4L_c}{3}\sqrt{\frac{\rho_1}{\rho_2}}
  4. So the answer is (a).
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Q426JEE Main 2020 · 5 SEP · SHIFT 1Easy

Organ Pipes & Resonance Tube · Resonance tube and end correction

In a resonance tube experiment when the tube is filled with water up to a height of 17.0 cm from bottom, it resonates with a given tuning fork. When the water level is raised the next resonance with the same tuning fork occurs at a height of 24.5 cm. If the velocity of sound in air is 330 m/s, the tuning fork frequency is:

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Answer: (a)

  1. Two successive resonances differ in air-column length by λ2\frac{\lambda}{2}.
  2. λ2=24.5−17.0=7.5 cm⇒λ=15 cm=0.15 m\frac{\lambda}{2} = 24.5 - 17.0 = 7.5\text{ cm} \Rightarrow \lambda = 15\text{ cm} = 0.15\text{ m}
  3. f=vλ=3300.15=2200 Hzf = \frac{v}{\lambda} = \frac{330}{0.15} = 2200\text{ Hz}
  4. So the answer is (a) 2200 Hz.
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Q427JEE Main 2020 · 8 JAN · SHIFT 1Medium

Organ Pipes & Resonance Tube · Open organ pipe

A one metre long (both ends open) organ pipe is kept in a gas that has double the density of air at STP. Assuming the speed of sound in air at STP is 300 m/s, the frequency difference between the fundamental and second harmonic of this pipe is ________ Hz.

Numerical answer type. Work it out, then open the answer.

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Answer: 105.75

  1. v=γPρ∝1ρv = \sqrt{\frac{\gamma P}{\rho}} \propto \frac{1}{\sqrt{\rho}}, so in the gas v′=3002≈212.1 m/sv' = \frac{300}{\sqrt{2}} \approx 212.1\text{ m/s}.
  2. Open pipe: fn=nv′2Lf_n = \frac{nv'}{2L}, so f2−f1=v′2Lf_2 - f_1 = \frac{v'}{2L}.
  3. f2−f1=212.12×1≈106 Hzf_2 - f_1 = \frac{212.1}{2 \times 1} \approx 106\text{ Hz}
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Q428MHT CET 2020 · 16 OCT · SHIFT 2Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

An open organ pipe and a closed organ pipe have the frequency of their first overtone identical. The ratio of length of open pipe to that of closed pipe is

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Answer: (c)

  1. Open pipe first overtone: 2v2Lo=vLo\frac{2v}{2L_o} = \frac{v}{L_o}; closed pipe first overtone: 3v4Lc\frac{3v}{4L_c}.
  2. vLo=3v4Lc⇒Lo:Lc=4:3\frac{v}{L_o} = \frac{3v}{4L_c} \Rightarrow L_o : L_c = 4 : 3
  3. So the answer is (c) 4:34:3.
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Q429MHT CET 2020 · 16 OCT · SHIFT 1Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

When open pipe is closed from one end third overtone of closed pipe is higher in frequency by 150 Hz150\text{ Hz}, then second overtone of open pipe. The fundamental frequency of open end pipe will be

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Answer: (d)

  1. Open pipe of length LL: fundamental n=v2Ln = \frac{v}{2L}, second overtone =3n= 3n.
  2. Closed from one end (same LL): fundamental v4L=n2\frac{v}{4L} = \frac{n}{2}, third overtone =7×n2=3.5n= 7 \times \frac{n}{2} = 3.5n.
  3. 3.5n−3n=150⇒0.5n=150⇒n=3003.5n - 3n = 150 \Rightarrow 0.5n = 150 \Rightarrow n = 300 Hz
  4. So the answer is (d) 300 Hz.
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Q430MHT CET 2020 · 19 OCT · SHIFT 2Medium

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

The fundamental frequency of a closed pipe is 400 Hz. If 13\frac{1}{3} rd pipe is filled with water, then the frequency of 2nd harmonic of the pipe will be (neglect and correction)

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Answer: (b)

  1. Closed pipe: n0=v4L=400n_0 = \frac{v}{4L} = 400 Hz.
  2. With 13\frac{1}{3} filled, air column =2L3= \frac{2L}{3}, new fundamental =400×32=600= 400 \times \frac{3}{2} = 600 Hz.
  3. A closed pipe gives only odd harmonics, so the next (second) note is the 3rd harmonic: 3×600=18003 \times 600 = 1800 Hz.
  4. So the answer is (b) 1800 Hz.
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Q431JEE Main 2019 · 10 JAN · SHIFT 2EasyOld syllabus

Organ Pipes & Resonance Tube · Closed organ pipe

A closed organ pipe has a fundamental frequency of 1.5 kHz. The number of overtones that can be distinctly heard by a person with this organ pipe will be (Assume that the highest frequency a person can hear is 20,000 Hz)

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Answer: (b)

  1. Closed pipe frequencies: (2n+1)×1.5 kHz(2n+1)\times1.5\text{ kHz}.
  2. (2n+1)×1.5≤20⇒2n+1≤13.3(2n+1)\times1.5 \le 20 \Rightarrow 2n+1 \le 13.3, so the highest audible is the 13th harmonic (19.5 kHz19.5\text{ kHz}).
  3. Audible tones: harmonics 1, 3, 5, 7, 9, 11, 13, i.e. 7 tones, of which 6 are overtones.
  4. The key counts all 7 audible frequencies: answer (b) 7.
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Q432MHT CET 2019 · 2 MAY · SHIFT 1Medium

Organ Pipes & Resonance Tube · Closed organ pipe

In a fundamental mode,the time required for the sound wave to reach upto the closed end of a pipe filled with air is ' tt ' second. The frequency of vibration of air column is

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Answer: (d)

  1. Fundamental of closed pipe: f=v4Lf = \frac{v}{4L}.
  2. Time to travel the pipe length: t=Lvt = \frac{L}{v}.
  3. f=14t=(4t)−1f = \frac{1}{4t} = (4t)^{-1}
  4. So the answer is (d) (4t)−1(4t)^{-1}.
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Q433MHT CET 2019 · 3 MAY · SHIFT 1Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

A pipe open at both ends and a pipe closed at one end have same length. The ratio of frequencies of their ppth overtone is

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Answer: (c)

  1. Open pipe ppth overtone = (p+1)(p+1)th harmonic: (p+1)v2L\frac{(p+1)v}{2L}.
  2. Closed pipe ppth overtone = (2p+1)(2p+1)th harmonic: (2p+1)v4L\frac{(2p+1)v}{4L}.
  3. Ratio =(p+1)/2(2p+1)/4=2(p+1)2p+1= \frac{(p+1)/2}{(2p+1)/4} = \frac{2(p+1)}{2p+1}
  4. So the answer is (c) 2(p+1)2p+1\frac{2(p+1)}{2p+1}.
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Q434NEET 2019Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

A tuning fork with frequency 800 Hz produces resonance in a resonance column tube with upper end open and lower end closed by water surface. Successive resonance are observed at lengths 9.75 cm, 31.25 cm and 52.75 cm. The speed of sound in air is,

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Answer: (d)

  1. Successive resonances differ by λ2\frac{\lambda}{2}: 31.25−9.75=21.531.25 - 9.75 = 21.5 cm.
  2. λ=43\lambda = 43 cm =0.43= 0.43 m
  3. v=nλ=800×0.43=344v = n\lambda = 800 \times 0.43 = 344 m/s
  4. So the answer is (d) 344 m/s.
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Q435JEE Main 2019 · 12 APR · SHIFT 2Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

A tuning fork of frequency 480 Hz is used in an experiment for measuring speed of sound (v) in air by resonance tube method. Resonance is observed to occur at two successive lengths of the air column, l1 = 30 cm and l2 = 70 cm. Then, v is equal to -

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Answer: (b)

  1. Successive resonances differ by λ2\frac{\lambda}{2}: 70−30=4070 - 30 = 40 cm, so λ=0.8\lambda = 0.8 m.
  2. v=nλ=480×0.8=384v = n\lambda = 480 \times 0.8 = 384 m s−1^{-1}
  3. So the answer is (b) 384 m s−1^{-1}.
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Q436MHT CET 2019 · 2 MAY · SHIFT 1Medium

Organ Pipes & Resonance Tube · Joined pipes, gases and string-pipe resonance

Two open pipes of different lengths and same diameter in which the air column vibrates with fundamental frequencies ' n1n_1 ', and ' n2n_2 ' respectively. When both pipes are joined to form a single pipe, its fundamental frequency will be

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Answer: (d)

  1. Open pipe fundamental: n=v2L⇒L=v2nn = \frac{v}{2L} \Rightarrow L = \frac{v}{2n}
  2. L1=v2n1L_1 = \frac{v}{2n_1}, L2=v2n2L_2 = \frac{v}{2n_2}; joined pipe has L=L1+L2=v2(1n1+1n2)L = L_1 + L_2 = \frac{v}{2}\left(\frac{1}{n_1} + \frac{1}{n_2}\right)
  3. n=v2L=11n1+1n2=n1n2n1+n2n = \frac{v}{2L} = \frac{1}{\frac{1}{n_1} + \frac{1}{n_2}} = \frac{n_1 n_2}{n_1 + n_2}
  4. So the answer is (d) n1n2n1+n2\frac{n_1 n_2}{n_1 + n_2}.
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Q437JEE Main 2019 · 12 JAN · SHIFT 2Difficult

Organ Pipes & Resonance Tube · Resonance tube and end correction

A resonance tube is old and has jagged end. It is still used in the laboratory to determine velocity of sound in air. A tuning fork of frequency 512 Hz produces first resonance when the tube is filled with water to a mark 11 cm below a reference mark, near the open end of the tube. The experiment is repeated with another fork of frequency 256 Hz which produces first resonance when water reaches a mark 27 cm below the reference mark. The velocity of sound in air, obtained in the experiment, is close to:

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Answer: (b)

  1. First resonance: l+e=λ4=v4fl + e = \frac{\lambda}{4} = \frac{v}{4f}; the unknown end/reference offset ee is the same in both runs
  2. Subtract: l2−l1=v4(1256−1512)=v2048l_2 - l_1 = \frac{v}{4}\left(\frac{1}{256} - \frac{1}{512}\right) = \frac{v}{2048}
  3. 0.27−0.11=0.16=v2048⇒v=327.7 m/s0.27 - 0.11 = 0.16 = \frac{v}{2048} \Rightarrow v = 327.7\text{ m/s}
  4. So the answer is (b) 328 m s−1328\text{ m s}^{-1}.
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Q438JEE Main 2018 · 16 APR · SHIFT 1Easy

Organ Pipes & Resonance Tube · Resonance tube and end correction

The end correction of a resonance column is 1 cm. If the shortest length resonating with the tuning fork is 10 cm, the next resonating length should be:

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Answer: (b)

  1. First resonance: l1+e=λ4⇒10+1=11 cml_1 + e = \frac{\lambda}{4} \Rightarrow 10 + 1 = 11\text{ cm}, so λ=44 cm\lambda = 44\text{ cm}.
  2. Second resonance: l2+e=3λ4=33 cml_2 + e = \frac{3\lambda}{4} = 33\text{ cm}
  3. l2=33−1=32 cml_2 = 33 - 1 = 32\text{ cm}
  4. So the answer is (b) 32 cm.
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Q439NEET 2018Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The fundamental frequency in an open organ pipe is equal to the third harmonic of a closed organ pipe. If the length of the closed organ pipe is 20 cm, the length of the open organ pipe is

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Answer: (a)

  1. Open pipe fundamental v2Lo\frac{v}{2L_o} = closed pipe third harmonic 3v4Lc\frac{3v}{4L_c}.
  2. Lo=4Lc6=23×20=13.3L_o = \frac{4L_c}{6} = \frac{2}{3} \times 20 = 13.3 cm
  3. So the answer is (a) 13.2 cm (nearest option).
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Q440NEET 2018Medium

Organ Pipes & Resonance Tube · Resonance tube and end correction

A tuning fork is used to produce resonance in a glass tube. The length of the air column in this tube can be adjusted by a variable piston. At room temperature of 27°C two successive resonances are produced at 20 cm and 73 cm of column length. If the frequency of the tuning fork is 320 Hz, the velocity of sound in air at 27°C is

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Answer: (b)

  1. Successive resonances differ by λ2\frac{\lambda}{2}: 73−20=5373 - 20 = 53 cm, so λ=1.06\lambda = 1.06 m.
  2. v=nλ=320×1.06=339.2v = n\lambda = 320 \times 1.06 = 339.2 m/s
  3. So the answer is (b) 339 m s−1^{-1}.
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Q441NEET 2017Easy

Organ Pipes & Resonance Tube · Closed organ pipe

The two nearest harmonics of a tube closed at one end and open at other end are 220 Hz and 260 Hz. What is the fundamental frequency of the system?

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Answer: (a)

  1. Closed pipe has only odd harmonics, so neighbouring ones differ by 2f02f_0.
  2. 2f0=260−220=40⇒f0=20 Hz2f_0=260-220=40 \Rightarrow f_0=20\text{ Hz} (check: 220=11f0220=11f_0, 260=13f0260=13f_0).
  3. So the answer is (a) 20 Hz.
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Q442JEE Main 2016Easy

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

A pipe open at both ends has a fundamental frequency ff in air. The pipe is dipped vertically in water so that half of it is in water. The fundamental frequency of the air column is now:

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Answer: (b)

  1. Open pipe: f=v2Lf = \frac{v}{2L}.
  2. Half in water leaves a closed pipe of length L2\frac{L}{2}: f′=v4(L/2)=v2Lf' = \frac{v}{4(L/2)} = \frac{v}{2L}.
  3. So the answer is (b) ff.
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Q443NEET 2016 · PHASE 1Easy

Organ Pipes & Resonance Tube · Resonance tube and end correction

An air column, closed at one end open at the other, resonates with a tuning fork when the smallest length of the column is 50 cm. The next larger length of the column resonating with the same tuning fork is

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Answer: (a)

  1. Closed pipe resonates at l1=λ4l_1 = \frac{\lambda}{4}, l2=3λ4l_2 = \frac{3\lambda}{4}, so l2=3l1l_2 = 3l_1.
  2. l2=3×50=150 cml_2 = 3 \times 50 = 150\text{ cm}
  3. So the answer is (a) 150 cm.
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Q444NEET 2016 · PHASE 2Medium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The second overtone of an open organ pipe has the same frequency as the first overtone of a closed pipe L metre long. The length of the open pipe will be

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Answer: (b)

  1. Open pipe second overtone: 3v2Lo\frac{3v}{2L_o}; closed pipe first overtone: 3v4L\frac{3v}{4L}.
  2. 3v2Lo=3v4L⇒Lo=2L\frac{3v}{2L_o} = \frac{3v}{4L} \Rightarrow L_o = 2L
  3. So the answer is (b) 2L2L.
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Q445NEET 2015 · AIPMT · CANCELLED PAPERMedium

Organ Pipes & Resonance Tube · Comparing closed and open pipes

The fundamental frequency of a closed organ pipe of length 20 cm is equal to the second overtone of an organ pipe open at both the ends. The length of organ pipe open at both the ends is

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Answer: (a)

  1. Closed pipe fundamental: v4×20\frac{v}{4 \times 20}; open pipe second overtone: 3v2Lo\frac{3v}{2L_o}.
  2. v80=3v2Lo⇒2Lo=240⇒Lo=120\frac{v}{80} = \frac{3v}{2L_o} \Rightarrow 2L_o = 240 \Rightarrow L_o = 120 cm
  3. So the answer is (a) 120 cm.
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Q446NEET 2014 · AIPMTMedium

Organ Pipes & Resonance Tube · Closed organ pipe

The number of possible natural oscillations of air column in a pipe closed at one end length 85 cm whose frequencies lie below 1250 Hz are (Velocity of sound = 340 m s−1{}^{-1})

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Answer: (d)

  1. Fundamental: f0=v4L=3404×0.85=100 Hzf_0 = \frac{v}{4L} = \frac{340}{4 \times 0.85} = 100\text{ Hz}.
  2. Allowed frequencies (odd harmonics): 100,300,500,700,900,1100,1300,…100, 300, 500, 700, 900, 1100, 1300, \dots
  3. Below 1250 Hz1250\text{ Hz}: 100100 to 11001100, i.e. 6 modes.
  4. So the answer is (d) 6.
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Q447JEE Main 2014Difficult

Organ Pipes & Resonance Tube · Closed organ pipe

A pipe of length 85 cm85\text{ cm} is closed from one end. Find the number of possible natural oscillations of air column in the pipe whose frequencies lie below 1250 Hz1250\text{ Hz}. The velocity of sound in air is 340 m/s340\text{ m/s}.

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Answer: (c)

  1. Closed pipe: f=(2n−1)v4Lf = (2n-1)\frac{v}{4L} (odd harmonics only)
  2. v4L=3404×0.85=100 Hz\frac{v}{4L} = \frac{340}{4 \times 0.85} = 100\text{ Hz}
  3. Allowed: 100,300,500,700,900,1100 Hz100, 300, 500, 700, 900, 1100\text{ Hz} (next is 1300>12501300 > 1250)
  4. So the answer is (c) 66.
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Q448NEET 2013Easy

Organ Pipes & Resonance Tube · Open organ pipe

If we study the vibration of a pipe open at both ends. then the following statement is not true.

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Answer: (b)

  1. (a) True: an open pipe gives all harmonics. (d) True: odd harmonics are among them.
  2. (c) True: open ends are displacement antinodes.
  3. (b) False: at open ends pressure stays atmospheric, so pressure change is zero (pressure node).
  4. So the answer is (b).
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Q449JEE Main 2012 · AIEEEEasy

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

A cylindrical tube, open at both ends, has a fundamental frequency, f,f, in air. The tube is dipped vertically in water so that half of it is in water. The fundamental frequency of the air-column is now:

Show answer and solution

Answer: (a)

  1. Open pipe: f=v2Lf = \frac{v}{2L}.
  2. Half in water leaves a closed pipe of length L2\frac{L}{2}: f′=v4(L/2)=v2Lf' = \frac{v}{4(L/2)} = \frac{v}{2L}.
  3. So the answer is (a) ff.
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Q450JEE Main 2008 · AIEEEMedium

Organ Pipes & Resonance Tube · Resonance tube and end correction

While measuring the speed of sound by performing a resonance column experiment, a student gets the first resonance condition at a column length of 18 cm18\text{ cm} during winter. Repeating the same experiment during summer, she measures the column length to be x cmx\text{ cm} for the second resonance. Then

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Answer: (b)

  1. Winter: 18+e=λ418 + e = \frac{\lambda}{4}, so the second resonance would be at 3λ4−e=54+2e>54\frac{3\lambda}{4} - e = 54 + 2e > 54 cm.
  2. In summer the temperature is higher, so vv and λ=vn\lambda = \frac{v}{n} increase.
  3. So the second resonance length is even larger: x>54x > 54 cm.
  4. So the answer is (b) x>54x > 54.
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Q451JEE Main 2002 · AIEEEEasy

Organ Pipes & Resonance Tube · Comparing closed and open pipes

Tube AA has both ends open while tube BB has one end closed, otherwise they are identical. The ratio of fundamental frequency of tube AA and BB is

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Answer: (c)

  1. fAfB=v/2Lv/4L=2\frac{f_A}{f_B}=\frac{v/2L}{v/4L}=2
  2. So the answer is (c) 2:12:1.
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Q452NEET 1997 · AIPMTEasy

Organ Pipes & Resonance Tube · Pipe dipped in water, cut or filled

A cylindrical tube, open at both ends has fundamental frequency ff in air. The tube is dipped vertically in water, so that half of it is in water. The fundamental frequency of air column is now

Show answer and solution

Answer: (d)

  1. Open pipe: f=v2Lf = \frac{v}{2L}.
  2. Half in water leaves a closed pipe of length L2\frac{L}{2}: f′=v4(L/2)=v2Lf' = \frac{v}{4(L/2)} = \frac{v}{2L}.
  3. So the answer is (d) ff.
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Q453NEET 1991 · AIPMTEasy

Organ Pipes & Resonance Tube · Closed organ pipe

A closed organ pipe (closed at one end) is excited to support the third overtone. It is found that air in the pipe has

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Answer: (d)

  1. Third overtone of a closed pipe: L=7λ4L=\frac{7\lambda}{4} (7th harmonic).
  2. From the closed end: N A N A N A N A, i.e. 4 nodes and 4 antinodes.
  3. So the answer is (d).
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Q454MHT CET 2026 · 19 MAY · SHIFT 1Easy

Beats · Beat frequency from two waves

Two simple harmonic sound waves travelling in the same direction are given by y1(x,t)=Asin⁡(0.5πx−100πt)y_1(x,t) = A\sin(0.5\pi x - 100\pi t) and y2(x,t)=Asin⁡(0.46πx−92πt)y_2(x,t) = A\sin(0.46\pi x - 92\pi t)

The number of times, a stationary listener can hear sound of maximum intensity in one second is

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Answer: (b)

  1. Frequency f=ω2πf = \frac{\omega}{2\pi}: f1=100π2π=50 Hzf_1 = \frac{100\pi}{2\pi} = 50\text{ Hz}, f2=92π2π=46 Hzf_2 = \frac{92\pi}{2\pi} = 46\text{ Hz}
  2. Beat frequency =f1−f2=4 Hz= f_1 - f_2 = 4\text{ Hz}, i.e. 4 maxima per second
  3. So the answer is (b) 44.
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Q455MHT CET 2026 · 18 APR · SHIFT 1Easy

Beats · Beat frequency from two waves

Two sources of sound are emitting progressive waves y1=4sin⁡708πty_1 = 4\sin 708\pi t and y2=3sin⁡700πty_2 = 3\sin 700\pi t. The sources are placed close to each other. The number of beats heard per second and intensity ratio between waxing and wanning are respectively

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Answer: (d)

  1. f1=708π2π=354 Hzf_1 = \frac{708\pi}{2\pi} = 354\text{ Hz}, f2=700π2π=350 Hzf_2 = \frac{700\pi}{2\pi} = 350\text{ Hz}, so 4 beats/s
  2. ImaxImin=(A1+A2)2(A1−A2)2=7212=49:1\frac{I_{max}}{I_{min}} = \frac{(A_1 + A_2)^2}{(A_1 - A_2)^2} = \frac{7^2}{1^2} = 49 : 1
  3. So the answer is (d) 4, 49:14,\ 49 : 1.
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Q456MHT CET 2026 · 17 APR · SHIFT 2Easy

Beats · Beat frequency from two waves

The beats are produced when there is a superposition of two sound waves which will have

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Answer: (c)

  1. Beats need a small frequency difference; equal frequencies give no beats
  2. Equal amplitudes make the minima zero, so the beats are clearest
  3. So the answer is (c) same amplitude but slightly different frequencies.
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Q457MHT CET 2026 · 16 APR · SHIFT 2Easy

Beats · Beat frequency from two waves

Two waves Y1=0.25sin⁡316tY_1 = 0.25\sin 316t and Y2=0.25sin⁡310tY_2 = 0.25\sin 310t are propagating along the same direction. The number of beats produced per second are

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Answer: (a)

  1. f=ω2πf = \frac{\omega}{2\pi}, so beat frequency =ω1−ω22π= \frac{\omega_1 - \omega_2}{2\pi}
  2. =316−3102π=62π=3π= \frac{316 - 310}{2\pi} = \frac{6}{2\pi} = \frac{3}{\pi} per second
  3. So the answer is (a) 3π\frac{3}{\pi}.
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Q458MHT CET 2026 · 19 MAY · SHIFT 2Easy

Beats · Series of tuning forks

A set of 88 tuning forks is arranged in ascending order of frequencies. Each fork produces 44 beats with the next one and frequency of last fork is octave of first. The frequency of 55th fork is

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Answer: (c)

  1. Fork frequencies: f,f+4,…f, f+4, \dots; last (8th) =f+7×4=f+28= f + 7 \times 4 = f + 28
  2. Octave: f+28=2f⇒f=28 Hzf + 28 = 2f \Rightarrow f = 28\text{ Hz}
  3. 5th fork =28+4×4=44 Hz= 28 + 4 \times 4 = 44\text{ Hz}
  4. So the answer is (c) 4444 Hz.
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Q459MHT CET 2026 · 19 APR · SHIFT 1Easy

Beats · Series of tuning forks

A set of 1414 tuning forks is arranged in a series of increasing frequencies. Each fork produces 'xx' beats per second with the preceding fork and the last fork is an octave of the first fork. If the seventh fork has the frequency of 114114 Hz, the value of xx is

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Answer: (c)

  1. Last (14th) fork =f+13x=2f⇒f=13x= f + 13x = 2f \Rightarrow f = 13x
  2. 7th fork =f+6x=19x=114⇒x=6= f + 6x = 19x = 114 \Rightarrow x = 6
  3. So the answer is (c) 66.
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Q460JEE Main 2026 · 28 JAN · SHIFT 2Easy

Beats · Loading, filing and unknown frequency

Two tuning forks A and B are sounded together giving rise to 8 beats in 2 s. When fork A is loaded with wax, the beat frequency is reduced to 4 beats in 2 s. If the original frequency of tuning fork B is 380 Hz then original frequency of tuning fork A is _________ Hz.

Numerical answer type. Work it out, then open the answer.

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Answer: 384

  1. Beat frequency: 8/2=4 Hz8/2 = 4\text{ Hz}, then 4/2=2 Hz4/2 = 2\text{ Hz}.
  2. nA=380±4=384n_A = 380 \pm 4 = 384 or 376 Hz376\text{ Hz}.
  3. Wax lowers nAn_A and the beats fall, so nA>380n_A > 380: 384→382 Hz384 \to 382\text{ Hz}.
  4. So nA=384 Hzn_A = 384\text{ Hz}.
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Q461MHT CET 2026 · 17 APR · SHIFT 2Medium

Beats · Beat frequency from two waves

Two sounding waves send waves at certain temperature in air of wavelength 50 cm and 50.5 cm repectively. The frequency of sources differ by 6 Hz. The velocity of sound in air at same temperature is

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Answer: (c)

  1. n1−n2=vλ1−vλ2=6n_1 - n_2 = \dfrac{v}{\lambda_1} - \dfrac{v}{\lambda_2} = 6 with λ1=0.50 m\lambda_1 = 0.50\text{ m}, λ2=0.505 m\lambda_2 = 0.505\text{ m}.
  2. v⋅0.505−0.500.50×0.505=6⇒v⋅0.0050.2525=6v \cdot \dfrac{0.505 - 0.50}{0.50 \times 0.505} = 6 \Rightarrow v \cdot \dfrac{0.005}{0.2525} = 6
  3. v=6×0.25250.005=303 m/sv = \dfrac{6 \times 0.2525}{0.005} = 303\text{ m/s}
  4. So the answer is (c) 303 m/s.
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Q462MHT CET 2026 · 20 MAY · SHIFT 1Medium

Beats · Beats with strings and sonometer wires

There are two wires vibrating with same frequency of 500500 Hz. Tension in one wire is increased by 'x' % so that 55 beats per second are heard. The value of 'x' in % is

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Answer: (d)

  1. f∝T⇒Δff=12ΔTTf \propto \sqrt{T} \Rightarrow \dfrac{\Delta f}{f} = \dfrac{1}{2}\dfrac{\Delta T}{T}
  2. Δff=5500=0.01\dfrac{\Delta f}{f} = \dfrac{5}{500} = 0.01
  3. ΔTT=0.02=2%\dfrac{\Delta T}{T} = 0.02 = 2\%
  4. So the answer is (d) 2.
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Q463MHT CET 2026 · 19 APR · SHIFT 1Medium

Beats · Beats with strings and sonometer wires

A tuning fork gives 55 beats per second with a 3333 cm length of sonometer wire. If the length of the wire is shortened by 11 cm, the number of beats is still the same. The frequency of the fork is

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Answer: (b)

  1. f∝1Lf \propto \dfrac{1}{L}, so the 33 cm wire is below the fork and the 32 cm wire above it.
  2. (n−5)×33=(n+5)×32(n - 5) \times 33 = (n + 5) \times 32
  3. 33n−165=32n+160⇒n=325 Hz33n - 165 = 32n + 160 \Rightarrow n = 325\text{ Hz}
  4. So the answer is (b) 325 Hz.
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Q464MHT CET 2026 · 17 APR · SHIFT 1Medium

Beats · Beats with strings and sonometer wires

A and B are two wires whose fundamental frequencies are 256 Hz and 382 Hz respectively. When third harmonic of A and the second harmonic of B are sounded together, the number of beats heard in two second will be

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Answer: (a)

  1. Third harmonic of A: 3×256=768 Hz3 \times 256 = 768\text{ Hz}.
  2. Second harmonic of B: 2×382=764 Hz2 \times 382 = 764\text{ Hz}.
  3. Beats per second =4= 4, so in 2 s: 88.
  4. So the answer is (a) 8.
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Q465MHT CET 2026 · 11 APR · SHIFT 1Medium

Beats · Beats with strings and sonometer wires

A tuning fork of frequency nn produces xx beats per second when sounded with a vibrating sonometer string. What must have been the frequency of the string, when a slight increase in tension produces lesser beats per second than before?

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Answer: (b)

  1. String frequency =n±x= n \pm x.
  2. Increasing tension raises the string frequency; beats decrease, so the string was moving toward nn from below.
  3. So the answer is (b) n−xn - x.
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Q466MHT CET 2026 · 18 APR · SHIFT 1Medium

Beats · Beats with organ pipes

The lengths of the two pipes open at both ends are L and (L+L1)(L + L_1). If they are sounded together, the beat frequency will be

(vv = velocity of sound in air)

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Answer: (d)

  1. Open pipe fundamental: f=v2Lf = \frac{v}{2L}.
  2. f1=v2Lf_1 = \frac{v}{2L}, f2=v2(L+L1)f_2 = \frac{v}{2(L+L_1)}
  3. Beat frequency =f1−f2=v2[1L−1L+L1]=vL12L(L+L1)= f_1 - f_2 = \frac{v}{2}\left[\frac{1}{L} - \frac{1}{L+L_1}\right] = \frac{vL_1}{2L(L+L_1)}
  4. So the answer is (d) vL12L(L+L1)\frac{vL_1}{2L(L+L_1)}.
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Q467MHT CET 2026 · 11 APR · SHIFT 2Difficult

Beats · Beats with organ pipes

The closed and open organ pipe have same length and when they are vibrating simultaneously in first overtone produce 33 beats. The length of open pipe is made (13)rd\left(\frac{1}{3}\right)^{rd} and closed pipe is made 33 times the original, the number of beats produced will be {neglect end correction}

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Answer: (c)

  1. First overtone: closed fc=3v4Lf_c = \frac{3v}{4L}, open fo=2v2L=vLf_o = \frac{2v}{2L} = \frac{v}{L}.
  2. Beats: vL−3v4L=v4L=3⇒vL=12\frac{v}{L} - \frac{3v}{4L} = \frac{v}{4L} = 3 \Rightarrow \frac{v}{L} = 12
  3. New lengths, fundamental modes: open (L3\frac{L}{3}): 3v2L=18\frac{3v}{2L} = 18 Hz; closed (3L3L): v12L=1\frac{v}{12L} = 1 Hz
  4. Beats =18−1=17= 18 - 1 = 17. So the answer is (c) 17.
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Q468MHT CET 2025 · 25 APR · SHIFT 1Easy

Beats · Beat frequency from two waves

Two tuning forks of frequencies 256 Hz and 258 Hz are sounded together. The time interval between two consecutive maxima is

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Answer: (d)

  1. Beat frequency =258−256=2 Hz= 258 - 256 = 2\text{ Hz}
  2. Time between consecutive maxima =12 s=0.5 s= \frac{1}{2}\text{ s} = 0.5\text{ s}
  3. So the answer is (d) 0.5 s.
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Q469MHT CET 2025 · 23 APR · SHIFT 2Easy

Beats · Beat frequency from two waves

Two sound waves travelling in the same direction have displacement y1=asin⁡(0.2πx−50πt)y_1 = a\sin(0.2\pi x - 50\pi t) and y2=asin⁡(0.15πx−46πt)y_2 = a\sin(0.15\pi x - 46\pi t).

How many times, a listener can hear sound of maximum intensity in one second?

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Answer: (b)

  1. f1=50π2π=25 Hzf_1 = \frac{50\pi}{2\pi} = 25\text{ Hz}, f2=46π2π=23 Hzf_2 = \frac{46\pi}{2\pi} = 23\text{ Hz}
  2. Beat frequency =2 Hz= 2\text{ Hz}, so 2 maxima per second
  3. So the answer is (b) 2.
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Q470MHT CET 2025 · 21 APR · SHIFT 1Easy

Beats · Beat frequency from two waves

Two sources of sound are emitting progressive waves y1=4sin⁡710πty_1 = 4\sin 710\pi t and y2=3sin⁡702πty_2 = 3\sin 702\pi t. The sources are placed close to each other. The number of beats heard per second and intensity ratio between waxing and waning are respectively

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Answer: (c)

  1. f1=710π2π=355 Hzf_1 = \frac{710\pi}{2\pi} = 355\text{ Hz}, f2=702π2π=351 Hzf_2 = \frac{702\pi}{2\pi} = 351\text{ Hz}, so 4 beats/s
  2. ImaxImin=(4+3)2(4−3)2=49:1\frac{I_{max}}{I_{min}} = \frac{(4+3)^2}{(4-3)^2} = 49 : 1
  3. So the answer is (c) 4, 49:14,\ 49 : 1.
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Q471JEE Main 2025 · 7 APR · SHIFT 1Medium

Beats · Beat frequency from two waves

Two harmonic waves moving in the same direction superimpose to form a wave x=acos⁡(1.5t)cos⁡(50.5t)x = a\cos(1.5t)\cos(50.5t) where t is in seconds. Find the period with which they beat. (close to nearest integer)

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Answer: (c)

  1. acos⁡(1.5t)cos⁡(50.5t)=a2[cos⁡52t+cos⁡49t]a\cos(1.5t)\cos(50.5t) = \dfrac{a}{2}[\cos 52t + \cos 49t], so ω1=52\omega_1 = 52, ω2=49 rad/s\omega_2 = 49\text{ rad/s}.
  2. Beat frequency fb=ω1−ω22π=32π Hzf_b = \dfrac{\omega_1 - \omega_2}{2\pi} = \dfrac{3}{2\pi}\text{ Hz}.
  3. Beat period Tb=2π3≈2.09 s≈2 sT_b = \dfrac{2\pi}{3} \approx 2.09\text{ s} \approx 2\text{ s}
  4. So the answer is (c) 2 s.
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Q472MHT CET 2025 · 25 APR · SHIFT 2Medium

Beats · Beats with strings and sonometer wires

A tuning fork gives 5 beats per second with 40 cm length of sonometer wire. If the length of the wire is shortened by 1 cm, the number of beats is still the same. The frequency of the fork is

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Answer: (b)

  1. f∝1Lf \propto \dfrac{1}{L}: 40 cm wire gives n−5n - 5, 39 cm wire gives n+5n + 5.
  2. (n−5)×40=(n+5)×39(n - 5) \times 40 = (n + 5) \times 39
  3. 40n−200=39n+195⇒n=395 Hz40n - 200 = 39n + 195 \Rightarrow n = 395\text{ Hz}
  4. So the answer is (b) 395 Hz.
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Q473MHT CET 2025 · 23 APR · SHIFT 1Medium

Beats · Beats with strings and sonometer wires

Two identical straight wires are stretched so as to produce 6 beats per second when vibrating simultaneously with tensions ' T1T_1 ' and ' T2T_2 ' respectively. On changing the tension slightly in one of them, the beat frequency remains unchanged. This will happen when (Given →T1>T2\rightarrow T_1 > T_2)

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Answer: (d)

  1. T1>T2⇒f1=f2+6T_1 > T_2 \Rightarrow f_1 = f_2 + 6 (since f∝Tf \propto \sqrt{T}).
  2. Beats stay 6 only if the two frequencies swap order: f1f_1 drops to f2−6f_2 - 6, or f2f_2 rises to f1+6f_1 + 6.
  3. That needs T1T_1 decreased or T2T_2 increased. Increasing T1T_1 or decreasing T2T_2 would only raise the beats.
  4. So the answer is (d).
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Q474MHT CET 2025 · 23 APR · SHIFT 1Medium

Beats · Beats with strings and sonometer wires

Two tuning forks when sounded together produce 4 beats per second. One of the forks is in unison with 23 cm length of sonometer wire and other with 24 cm length of the same wire. The frequencies of the two tuning forks are

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Answer: (a)

  1. f∝1Lf \propto \dfrac{1}{L}: f1×23=f2×24f_1 \times 23 = f_2 \times 24, with f1−f2=4f_1 - f_2 = 4.
  2. f2(2423−1)=4⇒f2=92 Hzf_2\left(\dfrac{24}{23} - 1\right) = 4 \Rightarrow f_2 = 92\text{ Hz}
  3. f1=96 Hzf_1 = 96\text{ Hz}
  4. So the answer is (a) 96 Hz, 92 Hz.
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Q475MHT CET 2025 · 21 APR · SHIFT 2Medium

Beats · Beats with strings and sonometer wires

Two strings ' X ' and ' Y ' of a guitar produces a beat frequency of 6 Hz. When the tension of the string ' Y ' is increased, the beat frequency is found to be 4 Hz. If the frequency of string ' X ' is 300 Hz, then the original frequency of string ' Y ' is

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Answer: (b)

  1. fY=300±6=306f_Y = 300 \pm 6 = 306 or 294 Hz294\text{ Hz}.
  2. Increasing tension raises fYf_Y, and the beats fall to 4, so fY<300f_Y < 300.
  3. 294→296 Hz294 \to 296\text{ Hz} gives 4 beats.
  4. So the answer is (b) 294 Hz.
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Q476MHT CET 2025 · 19 APR · SHIFT 2Medium

Beats · Beats with strings and sonometer wires

When two tuning forks are sounded together, 6 beats per second are heard. One of the fork is in unison with 0.70 m length of sonometer wire and another fork is in unison with 0.69 m length of the same sonometer wire. The frequencies of the two tuning forks are

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Answer: (b)

  1. f∝1Lf \propto \dfrac{1}{L}: f1×0.69=f2×0.70f_1 \times 0.69 = f_2 \times 0.70, with f1−f2=6f_1 - f_2 = 6.
  2. f2(0.700.69−1)=6⇒f2=6×0.690.01=414 Hzf_2\left(\dfrac{0.70}{0.69} - 1\right) = 6 \Rightarrow f_2 = \dfrac{6 \times 0.69}{0.01} = 414\text{ Hz}
  3. f1=420 Hzf_1 = 420\text{ Hz}
  4. So the answer is (b) 414 Hz, 420 Hz.
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Q477MHT CET 2025 · 5 MAY · SHIFT 2Medium

Beats · Beats with organ pipes

An open organ pipe and closed organ pipe of same length produce 2 beats per second, when they are set into vibrations together, in fundamental mode. The length of open pipe is made half and that of closed pipe is doubled.

The number of beats produced per second will be (neglect end correction)

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Answer: (c)

  1. Open pipe: fo=v2Lf_o = \frac{v}{2L}; closed pipe: fc=v4Lf_c = \frac{v}{4L}.
  2. Beats: fo−fc=v4L=2⇒vL=8f_o - f_c = \frac{v}{4L} = 2 \Rightarrow \frac{v}{L} = 8
  3. Open pipe of length L2\frac{L}{2}: fo′=vL=8f_o' = \frac{v}{L} = 8 Hz; closed pipe of length 2L2L: fc′=v8L=1f_c' = \frac{v}{8L} = 1 Hz
  4. Beats =8−1=7= 8 - 1 = 7. So the answer is (c) 7.
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Q478MHT CET 2025 · 22 APR · SHIFT 2Medium

Beats · Beats with organ pipes

The lengths of the two organ pipes open at both ends are ' L ' and (L+L1)(L + L_1). If they are sounded together, the beat frequency will be ( v=v = velocity of sound in air)

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Answer: (d)

  1. Open pipe fundamental: f=v2Lf = \frac{v}{2L}.
  2. Beat frequency =v2L−v2(L+L1)=v2⋅L1L(L+L1)= \frac{v}{2L} - \frac{v}{2(L+L_1)} = \frac{v}{2}\cdot\frac{L_1}{L(L+L_1)}
  3. So the answer is (d) vL12L(L+L1)\frac{vL_1}{2L(L+L_1)}.
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Q479JEE Main 2025 · 3 APR · SHIFT 2Medium

Beats · Beats with organ pipes

In the resonance experiment, two air columns (closed at one end) of 100 cm and 120 cm long, give 15 beats per second when each one is sounding in the respective fundamental modes. The velocity of sound in the air column is:

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Answer: (d)

  1. Closed pipe fundamental: f=v4Lf = \frac{v}{4L}.
  2. v4(1.00)−v4(1.20)=15\frac{v}{4(1.00)} - \frac{v}{4(1.20)} = 15
  3. v4(1−56)=v24=15⇒v=360\frac{v}{4}\left(1 - \frac{5}{6}\right) = \frac{v}{24} = 15 \Rightarrow v = 360 m/s
  4. So the answer is (d) 360360 m/s.
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Q480MHT CET 2025 · 26 APR · SHIFT 2Difficult

Beats · Beats with organ pipes

The closed and open organ pipes have same length. When they are vibrating simultaneously in first overtone, they produce four beats. The length of open pipe is made half and that of the closed pipe is made two times the original. Now the number of beats produced if the two pipes are vibrating in their fundamental modes simultaneously is

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Answer: (c)

  1. First overtone: closed 3v4L\frac{3v}{4L}, open vL\frac{v}{L}; beats v4L=4⇒vL=16\frac{v}{4L} = 4 \Rightarrow \frac{v}{L} = 16.
  2. Open pipe L2\frac{L}{2}, fundamental: vL=16\frac{v}{L} = 16 Hz
  3. Closed pipe 2L2L, fundamental: v8L=2\frac{v}{8L} = 2 Hz
  4. Beats =16−2=14= 16 - 2 = 14. So the answer is (c) 14.
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Q481MHT CET 2025 · 20 APR · SHIFT 2Difficult

Beats · Beats with organ pipes

The closed and open organ pipe have same length and when they are vibrating simultaneously in first overtone produce 3 beats. The length of open pipe is made (13)rd\left(\frac{1}{3}\right)^{\text{rd}} and that of closed pipe is made 3 times the original, the number of beats produced will be (Neglect end correction)

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Answer: (b)

  1. First overtone: closed 3v4L\frac{3v}{4L}, open vL\frac{v}{L}; beats v4L=3⇒vL=12\frac{v}{4L} = 3 \Rightarrow \frac{v}{L} = 12.
  2. Open pipe L3\frac{L}{3}, fundamental: 3v2L=18\frac{3v}{2L} = 18 Hz
  3. Closed pipe 3L3L, fundamental: v12L=1\frac{v}{12L} = 1 Hz
  4. Beats =18−1=17= 18 - 1 = 17. So the answer is (b) 17.
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Q482MHT CET 2024 · 16 MAY · SHIFT 2Easy

Beats · Beat frequency from two waves

Two sound waves having frequencies 250 Hz and 256 Hz superimpose to produce beat wave. The resultant beat wave has intensity maximum at t=0t = 0. After how much time an intensity will be minimum produced at the same point?

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Answer: (d)

  1. Beat frequency =256−250=6 Hz= 256 - 250 = 6\text{ Hz}, beat period T=16 sT = \frac{1}{6}\text{ s}
  2. A minimum comes half a beat period after a maximum: t=T2=112 st = \frac{T}{2} = \frac{1}{12}\text{ s}
  3. So the answer is (d) 112 s\frac{1}{12}\text{ s}.
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Q483MHT CET 2024 · 11 MAY · SHIFT 2Easy

Beats · Beat frequency from two waves

If the two waves of same amplitude, having frequencies 340 Hz and 335 Hz, are moving in same direction, then the time interval between two successive maxima formed (in second) is

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Answer: (b)

  1. Beat frequency =340−335=5 Hz= 340 - 335 = 5\text{ Hz}
  2. Interval between successive maxima =15=0.2 s= \frac{1}{5} = 0.2\text{ s}
  3. So the answer is (b) 0.2.
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Q484MHT CET 2024 · 10 MAY · SHIFT 1Easy

Beats · Beat frequency from two waves

Two sound waves having displacements x1=2sin⁡(1000πt)x_1 = 2\sin(1000\pi t) and x2=3sin⁡(1006πt)x_2 = 3\sin(1006\pi t), when interfere, produce

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Answer: (c)

  1. f1=1000π2π=500 Hzf_1 = \frac{1000\pi}{2\pi} = 500\text{ Hz}, f2=1006π2π=503 Hzf_2 = \frac{1006\pi}{2\pi} = 503\text{ Hz}, so 3 beats/s
  2. Maximum amplitude =2+3=5= 2 + 3 = 5, so Imax∝52=25I_{max} \propto 5^2 = 25 units
  3. So the answer is (c) 3 beats/s with maximum intensity 25 units.
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Q485MHT CET 2024 · 4 MAY · SHIFT 1Easy

Beats · Beat frequency from two waves

Two waves Y1=0.25sin⁡316tY_1 = 0.25\sin 316t and Y2=0.25sin⁡310tY_2 = 0.25\sin 310t are propagating along the same direction. The number of beats produced per second are

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Answer: (b)

  1. Beat frequency =ω1−ω22π=316−3102π= \frac{\omega_1 - \omega_2}{2\pi} = \frac{316 - 310}{2\pi}
  2. =62π=3π= \frac{6}{2\pi} = \frac{3}{\pi} per second
  3. So the answer is (b) 3π\frac{3}{\pi}.
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Q486MHT CET 2024 · 4 MAY · SHIFT 2Easy

Beats · Series of tuning forks

A set of 28 turning forks is arranged in an increasing order of frequencies. Each fork produces ' xx ' beats per second with the preceding fork and the last fork is an octave of the first. If the frequency of the 1212th fork is 152 Hz, the value of ' xx ' (no. of beats per second) is

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Answer: (b)

  1. Last (28th) fork =f+27x=2f⇒f=27x= f + 27x = 2f \Rightarrow f = 27x
  2. 12th fork =f+11x=38x=152⇒x=4= f + 11x = 38x = 152 \Rightarrow x = 4
  3. So the answer is (b) 4.
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Q487MHT CET 2024 · 11 MAY · SHIFT 1Medium

Beats · Loading, filing and unknown frequency

The frequency of two tuning forks A and B are respectively 1.4%1.4\% more and 2.6%2.6\% less than that of the tuning fork C. When A and B are sounded together, 10 beats are produced in 1 second. The frequency of tuning fork C is

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Answer: (a)

  1. nA=1.014 nCn_A = 1.014\,n_C, nB=0.974 nCn_B = 0.974\,n_C
  2. nA−nB=0.04 nC=10n_A - n_B = 0.04\,n_C = 10
  3. nC=250 Hzn_C = 250\text{ Hz}
  4. So the answer is (a) 250 Hz.
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Q488MHT CET 2024 · 2 MAY · SHIFT 1Medium

Beats · Beats with strings and sonometer wires

A wire under tension 225 N produces 6 beats per second when it is tuned with a fork. When the tension changes to 256 N, it is again tuned with the same tuning fork, the number of beats remain unchanged. The frequency of tuning fork will be

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Answer: (b)

  1. f∝Tf \propto \sqrt{T}: 225=15\sqrt{225} = 15, 256=16\sqrt{256} = 16.
  2. Same beats, so at 225 N the wire gives n−6n - 6 and at 256 N it gives n+6n + 6.
  3. n−6n+6=1516⇒16n−96=15n+90\dfrac{n - 6}{n + 6} = \dfrac{15}{16} \Rightarrow 16n - 96 = 15n + 90
  4. n=186 Hzn = 186\text{ Hz}. So the answer is (b) 186 Hz.
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Q489JEE Main 2024 · 1 FEB · SHIFT 1Medium

Beats · Beats with strings and sonometer wires

A tuning fork resonates with a sonometer wire of length 1 m1\text{ m} stretched with a tension of 6 N6\text{ N}. When the tension in the wire is changed to 54 N54\text{ N}, the same tuning fork produces 12 beats per second with it. The frequency of the tuning fork is ________________ Hz\text{Hz}.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 6

  1. f∝Tf \propto \sqrt{T}; at 6 N the wire is in unison with the fork, so f=nf = n.
  2. At 54 N: f′=n54/6=3nf' = n\sqrt{54/6} = 3n.
  3. 3n−n=12⇒n=6 Hz3n - n = 12 \Rightarrow n = 6\text{ Hz}
  4. So the frequency of the fork is 6 Hz6\text{ Hz}.
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Q490MHT CET 2024 · 15 MAY · SHIFT 1Medium

Beats · Beats with organ pipes

An open organ pipe of length ' ll ' is sounded together with another open organ pipe of length (l+l1)(l + l_1) in their fundamental modes. Speed of sound in air is ' VV '. The beat frequency heard will be ( l1<<l)l_1 << l)

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Answer: (b)

  1. Open pipe fundamental: f=V2lf = \frac{V}{2l}.
  2. Beats =V2l−V2(l+l1)=Vl12l(l+l1)= \frac{V}{2l} - \frac{V}{2(l+l_1)} = \frac{Vl_1}{2l(l+l_1)}
  3. Since l1≪ll_1 \ll l, l(l+l1)≈l2l(l+l_1) \approx l^2, so beats ≈Vl12l2\approx \frac{Vl_1}{2l^2}.
  4. So the answer is (b) Vl12l2\frac{Vl_1}{2l^2}.
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Q491JEE Main 2024 · 27 JAN · SHIFT 2Medium

Beats · Beats with organ pipes

A closed organ pipe 150 cm150\text{ cm} long gives 7 beats per second with an open organ pipe of length 350 cm350\text{ cm}, both vibrating in fundamental mode. The velocity of sound is __________ m/s\text{m/s}.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 294

  1. Closed pipe: fc=v4×1.5=v6f_c = \frac{v}{4 \times 1.5} = \frac{v}{6}; open pipe: fo=v2×3.5=v7f_o = \frac{v}{2 \times 3.5} = \frac{v}{7}.
  2. Beats: v6−v7=v42=7\frac{v}{6} - \frac{v}{7} = \frac{v}{42} = 7
  3. v=294v = 294 m/s
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Q492MHT CET 2023 · 12 MAY · SHIFT 1Easy

Beats · Series of tuning forks

41 tuning forks are arranged in increasing order of frequency such that each produces 5 beats/second with next tuning fork. If frequency of last tuning fork is double that of frequency of first fork. Then frequency of first and last fork is

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Answer: (b)

  1. Last (41st) fork =f+40×5=f+200= f + 40 \times 5 = f + 200
  2. f+200=2f⇒f=200 Hzf + 200 = 2f \Rightarrow f = 200\text{ Hz}, last =400 Hz= 400\text{ Hz}
  3. So the answer is (b) 200, 400 Hz200,\ 400\text{ Hz}.
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Q493MHT CET 2023 · 12 MAY · SHIFT 1Medium

Beats · Beat frequency from two waves

Two sounding sources send waves at certain temperature in air of wavelength 50 cm50\text{ cm} and 50.5 cm50.5\text{ cm} respectively. The frequency of sources differ by 6 Hz6\text{ Hz}. The velocity of sound in air at same temperature is

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Answer: (b)

  1. n1−n2=vλ1−vλ2=6n_1 - n_2 = \dfrac{v}{\lambda_1} - \dfrac{v}{\lambda_2} = 6 with λ1=0.50 m\lambda_1 = 0.50\text{ m}, λ2=0.505 m\lambda_2 = 0.505\text{ m}.
  2. v⋅0.0050.50×0.505=6v \cdot \dfrac{0.005}{0.50 \times 0.505} = 6
  3. v=6×0.25250.005=303 m/sv = \dfrac{6 \times 0.2525}{0.005} = 303\text{ m/s}
  4. So the answer is (b) 303 m/s303\text{ m/s}.
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Q494MHT CET 2023 · 14 MAY · SHIFT 2Medium

Beats · Beats with strings and sonometer wires

A sonometer wire 49 cm49\text{ cm} long is in unison with a tuning fork of frequency 'nn'. If the length of the wire is decreased by 1 cm1\text{ cm} and it is vibrated with the same tuning fork, 6 beats are heard per second. The value of 'nn' is

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Answer: (b)

  1. f∝1Lf \propto \dfrac{1}{L}: the 48 cm wire gives n+6n + 6.
  2. n×49=(n+6)×48n \times 49 = (n + 6) \times 48
  3. n=6×48=288 Hzn = 6 \times 48 = 288\text{ Hz}
  4. So the answer is (b) 288 Hz.
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Q495MHT CET 2023 · 13 MAY · SHIFT 2Medium

Beats · Beats with strings and sonometer wires

When two tuning forks are sounded together, 5 beats per second are heard. One of the forks is in unison with 0.97 m0.97\text{ m} length of sonometer wire and the other is in unison with 0.96 m0.96\text{ m} length of the same wire. The frequencies of the two tuning forks are

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Answer: (d)

  1. f∝1Lf \propto \dfrac{1}{L}: f1×0.97=f2×0.96f_1 \times 0.97 = f_2 \times 0.96, with f2−f1=5f_2 - f_1 = 5.
  2. f1(0.970.96−1)=5⇒f1=5×0.960.01=480 Hzf_1\left(\dfrac{0.97}{0.96} - 1\right) = 5 \Rightarrow f_1 = \dfrac{5 \times 0.96}{0.01} = 480\text{ Hz}
  3. f2=485 Hzf_2 = 485\text{ Hz}
  4. So the answer is (d) 480 Hz, 485 Hz.
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Q496MHT CET 2023 · 12 MAY · SHIFT 2Medium

Beats · Beats with strings and sonometer wires

A tuning fork gives 3 beats with 50 cm50\text{ cm} length of sonometer wire. If the length of the wire is shortened by 1 cm1\text{ cm}, the number of beats is still the same. The frequency of the fork is

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Answer: (c)

  1. f∝1Lf \propto \dfrac{1}{L}: 50 cm wire gives n−3n - 3, 49 cm wire gives n+3n + 3.
  2. (n−3)×50=(n+3)×49(n - 3) \times 50 = (n + 3) \times 49
  3. 50n−150=49n+147⇒n=297 Hz50n - 150 = 49n + 147 \Rightarrow n = 297\text{ Hz}
  4. So the answer is (c) 297 Hz.
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Q497JEE Main 2022 · 26 JUN · SHIFT 2Easy

Beats · Series of tuning forks

A set of 20 tuning forks is arranged in a series of increasing frequencies. If each fork gives 4 beats with respect to the preceding fork and the frequency of the last fork is twice the frequency of the first, then the frequency of last fork is _________ Hz.

Numerical answer type. Work it out, then open the answer.

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Answer: 152

  1. Last (20th) fork =f+19×4=f+76= f + 19 \times 4 = f + 76
  2. f+76=2f⇒f=76 Hzf + 76 = 2f \Rightarrow f = 76\text{ Hz}
  3. Last fork =2×76=152 Hz= 2 \times 76 = 152\text{ Hz}
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Q498JEE Main 2022 · 28 JUN · SHIFT 1Medium

Beats · Beat frequency from two waves

The velocity of sound in a gas, in which two wavelengths 4.08 m and 4.16 m produce 40 beats in 12s, will be:

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Answer: (d)

  1. Beat frequency =4012=103 Hz= \dfrac{40}{12} = \dfrac{10}{3}\text{ Hz}.
  2. v(14.08−14.16)=103⇒v⋅0.084.08×4.16=103v\left(\dfrac{1}{4.08} - \dfrac{1}{4.16}\right) = \dfrac{10}{3} \Rightarrow v \cdot \dfrac{0.08}{4.08 \times 4.16} = \dfrac{10}{3}
  3. v=10×16.973×0.08≈707.2 m/sv = \dfrac{10 \times 16.97}{3 \times 0.08} \approx 707.2\text{ m/s}
  4. So the answer is (d) 707.2 m s−1707.2\text{ m s}^{-1}.
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Q499MHT CET 2021 · 23 SEP · SHIFT 2Easy

Beats · Beat frequency from two waves

Two sound waves having wavelengths 5.0 m5.0\text{ m} and 5.5 m5.5\text{ m} propagate in a gas with velocity 300 m/s\text{m/s}. The number of beats produced per second is

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Answer: (a)

  1. f=vλf = \frac{v}{\lambda}: f1=3005.0=60 Hzf_1 = \frac{300}{5.0} = 60\text{ Hz}, f2=3005.5=54.5 Hzf_2 = \frac{300}{5.5} = 54.5\text{ Hz}
  2. Beats =60−54.5≈5.5= 60 - 54.5 \approx 5.5 per second, nearest option is 6
  3. So the answer is (a) six.
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Q500MHT CET 2021 · 23 SEP · SHIFT 1Easy

Beats · Beat frequency from two waves

Two waves Y1=0.25sin⁡316tY_1 = 0.25\sin 316t and Y2=0.25sin⁡310tY_2 = 0.25\sin 310t are propagation same direction. The number of beats produced per second are

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Answer: (a)

  1. Beat frequency =ω1−ω22π=316−3102π= \frac{\omega_1 - \omega_2}{2\pi} = \frac{316 - 310}{2\pi}
  2. =62π=3π= \frac{6}{2\pi} = \frac{3}{\pi} per second
  3. So the answer is (a) 3π\frac{3}{\pi}.
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Q501MHT CET 2021 · 20 SEP · SHIFT 2Easy

Beats · Beat frequency from two waves

Beats are produced by waves y1=asin⁡2000πty_1 = a\sin 2000\pi t and y2=asin⁡2008πty_2 = a\sin 2008\pi t. The number of beats heard per second is

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Answer: (a)

  1. f1=2000π2π=1000 Hzf_1 = \frac{2000\pi}{2\pi} = 1000\text{ Hz}, f2=2008π2π=1004 Hzf_2 = \frac{2008\pi}{2\pi} = 1004\text{ Hz}
  2. Beats per second =1004−1000=4= 1004 - 1000 = 4
  3. So the answer is (a) 4.
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Q502JEE Main 2021 · 26 FEB · SHIFT 2Easy

Beats · Loading, filing and unknown frequency

A tuning fork A of unknown frequency produces 5 beats/s with a fork of known frequency 340 Hz. When fork A is filed, the beat frequency decreases to 2 beats/s. What is the frequency of fork A?

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Answer: (a)

  1. 5 beats with 340 Hz, so nA=335n_A = 335 or 345 Hz345\text{ Hz}.
  2. Filing raises the frequency of AA, and the beats fall to 2.
  3. Beats fall only if nA<340n_A < 340: 335→338 Hz335 \to 338\text{ Hz} gives 2 beats.
  4. So the answer is (a) 335 Hz.
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Q503MHT CET 2021 · 20 SEP · SHIFT 1Medium

Beats · Loading, filing and unknown frequency

The frequencies of three tuning forks A,BA, B and CC are related as nA>nB>nCn_A > n_B > n_C. When the forks AA and BB are sounded together, the number of beats produced per second is 'n1n_1'. When forks AA and CC are sounded together the number of beats produced per second is 'n2n_2'. How may beats are produced per second when forks BB and CC are sounded together?

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Answer: (c)

  1. nA−nB=n1n_A - n_B = n_1 and nA−nC=n2n_A - n_C = n_2.
  2. Subtract: nB−nC=n2−n1n_B - n_C = n_2 - n_1.
  3. So the answer is (c) n2−n1n_2 - n_1.
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Q504MHT CET 2021 · 24 SEP · SHIFT 1Medium

Beats · Beats with strings and sonometer wires

A sonometer wire of length 25 cm vibrates in unison with a tuning fork. When its length is decreased by 1 cm, 6 beats are heard per second. What is the frequency of the tuning fork?

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Answer: (d)

  1. f∝1Lf \propto \dfrac{1}{L}: the 24 cm wire gives n+6n + 6.
  2. n×25=(n+6)×24n \times 25 = (n + 6) \times 24
  3. n=6×24=144 Hzn = 6 \times 24 = 144\text{ Hz}
  4. So the answer is (d) 144 Hz.
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Q505MHT CET 2021 · 24 SEP · SHIFT 2Medium

Beats · Beats with organ pipes

A closed organ pipe and an open organ pipe of same length produce 2 beats per second when they are set into vibrations together in fundamental mode. The length of open pipe is now halved and that of closed pipe is doubled. The number of beats produced per second will be

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Answer: (d)

  1. Open: fo=v2Lf_o = \frac{v}{2L}; closed: fc=v4Lf_c = \frac{v}{4L}; beats v4L=2⇒vL=8\frac{v}{4L} = 2 \Rightarrow \frac{v}{L} = 8.
  2. Open pipe halved: fo′=vL=8f_o' = \frac{v}{L} = 8 Hz
  3. Closed pipe doubled: fc′=v8L=1f_c' = \frac{v}{8L} = 1 Hz
  4. Beats =8−1=7= 8 - 1 = 7. So the answer is (d) 7.
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Q506MHT CET 2020 · 16 OCT · SHIFT 1Easy

Beats · Beat frequency from two waves

Two waves Y1=0.25sin⁡316tY_1 = 0.25\sin 316t and Y2=0.25sin⁡310tY_2 = 0.25\sin 310t are propagating along the same direction. The number of beats produced per second are

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Answer: (c)

  1. Beat frequency =ω1−ω22π=316−3102π= \frac{\omega_1 - \omega_2}{2\pi} = \frac{316 - 310}{2\pi}
  2. =62π=3π= \frac{6}{2\pi} = \frac{3}{\pi} per second
  3. So the answer is (c) 3π\frac{3}{\pi}.
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Q507MHT CET 2020 · 19 OCT · SHIFT 2Easy

Beats · Loading, filing and unknown frequency

A tuning fork AA produces 5 beats per second with a tuning fork of frequency 480 Hz. When a little wax is stuck to a prong of fork AA, the number of beats heard per second becomes 2. What is the frequency of tuning fork AA before the wax is stuck to it?

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Answer: (d)

  1. 5 beats with 480 Hz, so nA=480±5=485n_A = 480 \pm 5 = 485 or 475 Hz475\text{ Hz}.
  2. Wax lowers the frequency of AA, and the beats fall from 5 to 2.
  3. Beats fall only if nAn_A moves closer to 480, so nA>480n_A > 480: 485→482 Hz485 \to 482\text{ Hz} gives 2 beats.
  4. So the answer is (d) 485 Hz.
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Q508NEET 2020 · PHASE 1Easy

Beats · Beats with strings and sonometer wires

In a guitar, two strings A and B made of same material are slightly out of tune and produce beats of frequency 6 Hz. When tension in B is slightly decreased, the beat frequency increases. If the frequency of A is 530 Hz, the original frequency of B will be:

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Answer: (a)

  1. fB=530±6=536f_B = 530 \pm 6 = 536 or 524 Hz524\text{ Hz}.
  2. Decreasing tension lowers fBf_B (f∝Tf \propto \sqrt{T}), and the beats increase.
  3. Beats increase only if fBf_B moves away from 530, so fB<530f_B < 530.
  4. So the answer is (a) 524 Hz.
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Q509MHT CET 2019 · 3 MAY · SHIFT 1Easy

Beats · Beat frequency from two waves

For formation of beats, two sound notes must have

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Answer: (d)

  1. Beats need a small frequency difference (nearly equal frequencies), not equal frequencies
  2. Equal amplitudes give zero intensity at minima, so beats are clearly heard
  3. So the answer is (d) nearly equal frequencies and equal amplitudes.
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Q510JEE Main 2019 · 10 APR · SHIFT 2Medium

Beats · Beat frequency from two waves

The correct figure that shows, schematically, the wave pattern produced by superposition of two waves of frequencies 9 Hz and 11 Hz, is:

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Answer: (c)

  1. Beat frequency =11−9=2 Hz= 11 - 9 = 2\text{ Hz}, so beat period =0.5 s= 0.5\text{ s}.
  2. At t=0t = 0 both waves are in phase, so the amplitude is maximum at t=0,0.5,1,1.5,2 st = 0, 0.5, 1, 1.5, 2\text{ s}.
  3. Amplitude is zero midway, at t=0.25,0.75,… st = 0.25, 0.75, \dots\text{ s}: 4 beats in 2 s.
  4. Only figure (c) shows this. So the answer is (c).
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Q511JEE Main 2018 · 16 APR · SHIFT 1EasyOld syllabus

Beats · Beats with strings and sonometer wires

Two sitar strings, A and B, playing the note 'Dha' are slightly out of tune and produce beats of frequency 5 Hz. The tension of the string B s slightly increased and the beat frequency is found to decrease by 3Hz. If the frequency of A is 425 Hz, the original frequency of B is:

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Answer: (b)

  1. fB=425±5=430f_B = 425 \pm 5 = 430 or 420 Hz420\text{ Hz}.
  2. Increasing tension raises fBf_B, and the beats fall to 5−3=2 Hz5 - 3 = 2\text{ Hz}.
  3. So fB<425f_B < 425: 420→423 Hz420 \to 423\text{ Hz}.
  4. So the answer is (b) 420 Hz.
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Q512JEE Main 2018 · 15 APR · SHIFT 2Medium

Beats · Beats with strings and sonometer wires

5 beats / second are heard when a tuning fork is sounded with a sonometer wire under tension, when the length of the sonometer wire is either 0.95 m or 1 m. The frequency of the fork will be:

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Answer: (a)

  1. f∝1Lf \propto \dfrac{1}{L}: 0.95 m wire gives n+5n + 5, 1 m wire gives n−5n - 5.
  2. (n+5)×0.95=(n−5)×1(n + 5) \times 0.95 = (n - 5) \times 1
  3. 0.05n=9.75⇒n=195 Hz0.05n = 9.75 \Rightarrow n = 195\text{ Hz}
  4. So the answer is (a) 195 Hz.
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Q513JEE Main 2018 · 15 APR · SHIFT 1Medium

Beats · Beats with organ pipes

A tuning fork vibrates with frequency 256 Hz256\text{ Hz} and gives one beat per second with the third normal mode of vibration of an open pipe. What is the length of the pipe? (Speed of sound in air is 340 ms−1340\text{ ms}^{-1})

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Answer: (d)

  1. Third normal mode of an open pipe: f=3v2Lf = \frac{3v}{2L}.
  2. 1 beat/s with 256 Hz, so f=255f = 255 Hz or 257257 Hz.
  3. With f=255f = 255 Hz: L=3×3402×255=2L = \frac{3 \times 340}{2 \times 255} = 2 m =200= 200 cm (257 Hz gives 198.4 cm, not an option).
  4. So the answer is (d) 200200 cm.
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Q514NEET 2016 · PHASE 2Easy

Beats · Beat frequency from two waves

Three sound waves of equal amplitudes have frequencies (n −- 1), n, (n + 1). They superimpose to give beats. The number of beats produced per second will be

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Answer: (d)

  1. Adding the three waves: y=Asin⁡(2πnt)[1+2cos⁡(2πt)]y = A\sin(2\pi nt)\left[1 + 2\cos(2\pi t)\right]
  2. Amplitude A(1+2cos⁡2πt)A(1 + 2\cos 2\pi t) repeats every 1 s; in each second ∣1+2cos⁡2πt∣|1 + 2\cos 2\pi t| has two maxima (at cos⁡=1\cos = 1 and cos⁡=−1\cos = -1)
  3. So 2 beats per second: the answer is (d) 2.
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Q515JEE Main 2013 · 9 APR · SHIFT 1Medium

Beats · Beat frequency from two waves

When two sound waves travel in the same direction in a medium, the displacements of a particle located at 'x' at time 't' is given by:

y1=0.05cos⁡(0.50πx−100πt)y_1 = 0.05\cos(0.50\pi x - 100\pi t)

y2=0.05cos⁡(0.46πx−92πt)y_2 = 0.05\cos(0.46\pi x - 92\pi t)

where y1, y2y_1,\ y_2 and x are in meters and t in seconds. The speed of sound in the medium is:

Show answer and solution

Answer: (b)

  1. Wave speed v=ωkv = \dfrac{\omega}{k}.
  2. Wave 1: v=100π0.50π=200 m/sv = \dfrac{100\pi}{0.50\pi} = 200\text{ m/s}
  3. Wave 2: v=92π0.46π=200 m/sv = \dfrac{92\pi}{0.46\pi} = 200\text{ m/s} (same medium, same speed).
  4. So the answer is (b) 200 m/s.
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Q516NEET 2013Medium

Beats · Loading, filing and unknown frequency

A source of unknown frequency gives 4 beats/s when sounded with a source of known frequency 250 Hz. The second harmonic of the source of unknown frequency gives five beats per second, when sounded with a source of frequency 513 Hz. The unknown frequency is

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Answer: (c)

  1. n=250±4=254n = 250 \pm 4 = 254 or 246 Hz246\text{ Hz}.
  2. Second harmonic 2n=5082n = 508 or 492 Hz492\text{ Hz}.
  3. With 513 Hz: 513−508=5513 - 508 = 5 beats (492 gives 21).
  4. So the answer is (c) 254 Hz.
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Q517NEET 2012 · AIPMT · PRELIMSEasy

Beats · Beat frequency from two waves

Two sources of sound placed close to each other, are emitting progressive waves given by y1 = 4sin600π\pit and y2 = 5sin608π\pit

An observer located near these two sources of sound will hear

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Answer: (d)

  1. f1=600π2π=300 Hzf_1 = \frac{600\pi}{2\pi} = 300\text{ Hz}, f2=608π2π=304 Hzf_2 = \frac{608\pi}{2\pi} = 304\text{ Hz}, so 4 beats/s
  2. ImaxImin=(5+4)2(5−4)2=81:1\frac{I_{max}}{I_{min}} = \frac{(5+4)^2}{(5-4)^2} = 81 : 1
  3. So the answer is (d) 4 beats per second with intensity ratio 81 : 1.
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Q518NEET 2011 · AIPMT · MAINSMedium

Beats · Beats with strings and sonometer wires

Two identical piano wires, kept under the same tension T have a fundamental frequency of 600 Hz. The fractional increase in the tension of one of the wires which will lead to occurrence of 6 beats/s when both the wires oscillate together would be

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Answer: (b)

  1. f∝T⇒Δff=12ΔTTf \propto \sqrt{T} \Rightarrow \dfrac{\Delta f}{f} = \dfrac{1}{2}\dfrac{\Delta T}{T}
  2. Δff=6600=0.01\dfrac{\Delta f}{f} = \dfrac{6}{600} = 0.01
  3. ΔTT=0.02\dfrac{\Delta T}{T} = 0.02
  4. So the answer is (b) 0.02.
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Q519NEET 2010 · AIPMT · PRELIMSEasy

Beats · Beats with strings and sonometer wires

A tuning fork of frequency 512 Hz makes 4 beats per second with the vibrating string of a piano. The beat frequency decreases to 2 beats per sec when the tension in the piano string is slightly increased. The frequency of the piano string before increasing the tension was

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Answer: (d)

  1. String frequency =512±4=516= 512 \pm 4 = 516 or 508 Hz508\text{ Hz}.
  2. Increasing tension raises the string frequency, and the beats fall to 2.
  3. So the string was below 512: 508→510 Hz508 \to 510\text{ Hz}.
  4. So the answer is (d) 508 Hz.
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Q520JEE Main 2009 · AIEEEEasy

Beats · Beat frequency from two waves

Three sound waves of equal amplitudes have frequencies (v−1), v, (v+1).(v-1),\ v,\ (v+1). They superpose to give beats. The number of beats produced per second will be:

Show answer and solution

Answer: (b)

  1. Adding the three waves: y=Asin⁡(2πvt)[1+2cos⁡(2πt)]y = A\sin(2\pi vt)\left[1 + 2\cos(2\pi t)\right]
  2. Amplitude A(1+2cos⁡2πt)A(1 + 2\cos 2\pi t) repeats every 1 s; in each second ∣1+2cos⁡2πt∣|1 + 2\cos 2\pi t| has two maxima (at cos⁡=1\cos = 1 and cos⁡=−1\cos = -1)
  3. So 2 beats per second: the answer is (b) 22.
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Q521NEET 2009 · AIPMTMedium

Beats · Beats with strings and sonometer wires

Each of the two strings of length 51.6 cm and 49.1 cm are tensioned separately by 20 N force. Mass per unit length of both the strings is same and equal to 1 g/m. When both the strings vibrate simultaneously the number of beats is

Show answer and solution

Answer: (a)

  1. v=T/μ=20/10−3=141.4 m/sv = \sqrt{T/\mu} = \sqrt{20/10^{-3}} = 141.4\text{ m/s}
  2. f=v2Lf = \dfrac{v}{2L}: f1=141.42×0.491≈144.0 Hzf_1 = \dfrac{141.4}{2 \times 0.491} \approx 144.0\text{ Hz}, f2=141.42×0.516≈137.0 Hzf_2 = \dfrac{141.4}{2 \times 0.516} \approx 137.0\text{ Hz}
  3. Beats =144.0−137.0≈7= 144.0 - 137.0 \approx 7
  4. So the answer is (a) 7.
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Q522NEET 2006 · AIPMTEasy

Beats · Beat frequency from two waves

Two sound waves with wavelengths 5.0 m and 5.5. m respectively, each propagate in a gas with velocity 330 m/s. We expect the following number of beats per second.

Show answer and solution

Answer: (a)

  1. f=vλf = \frac{v}{\lambda}: f1=3305.0=66 Hzf_1 = \frac{330}{5.0} = 66\text{ Hz}, f2=3305.5=60 Hzf_2 = \frac{330}{5.5} = 60\text{ Hz}
  2. Beats per second =66−60=6= 66 - 60 = 6
  3. So the answer is (a) 6.
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Q523NEET 2005 · AIPMTEasy

Beats · Beat frequency from two waves

Two vibrating tuning forks produce progressive waves given by y1=4sin⁡500πty_1 = 4\sin 500\pi t and y2=2sin⁡506πty_2 = 2\sin 506\pi t. Number of beats produced per minute is

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Answer: (b)

  1. f1=500π2π=250 Hzf_1 = \frac{500\pi}{2\pi} = 250\text{ Hz}, f2=506π2π=253 Hzf_2 = \frac{506\pi}{2\pi} = 253\text{ Hz}
  2. Beats =3= 3 per second =3×60=180= 3 \times 60 = 180 per minute
  3. So the answer is (b) 180.
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Q524JEE Main 2005 · AIEEEEasy

Beats · Loading, filing and unknown frequency

When two tuning forks (fork 11 and fork 22) are sounded simultaneously, 44 beats per second are heated. Now, some tape is attached on the prong of the fork 22 When the tuning forks are sounded again, 66 beats per second are heard. If the frequency of fork 11 is 200 Hz200\text{ Hz}, then what was the original frequency of fork 22?

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Answer: (d)

  1. 4 beats with 200 Hz, so n2=204n_2 = 204 or 196 Hz196\text{ Hz}.
  2. Tape (loading) lowers n2n_2, and the beats rise from 4 to 6.
  3. Beats rise only if n2n_2 moves away from 200, so n2<200n_2 < 200: 196→194 Hz196 \to 194\text{ Hz} gives 6 beats.
  4. So the answer is (d) 196 Hz196\text{ Hz}.
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Q525JEE Main 2003 · AIEEEEasy

Beats · Beats with strings and sonometer wires

A tuning fork of known frequency 256 Hz256\text{ Hz} makes 55 beats per second with the vibrating string of a piano. The beat frequency decreases to 22 beats per second when the tension in the piano string is slightly increased. The frequency of the piano string before increasing the tension was

Show answer and solution

Answer: (c)

  1. String frequency =256±5 Hz= 256 \pm 5\text{ Hz}.
  2. Increasing tension raises the string frequency, and the beats fall from 5 to 2.
  3. So the string was below 256: 251→254 Hz251 \to 254\text{ Hz}.
  4. So the answer is (c) 256−5 Hz256 - 5\text{ Hz}.
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Q526JEE Main 2002 · AIEEEEasy

Beats · Loading, filing and unknown frequency

A tuning fork arrangement (pair) produces 44 beats/sec with one fork of frequency 288 cps288\text{ cps} A little wax is placed on the unknown fork and it then produces 22 beats/sec. The frequency of the unknown fork is

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Answer: (b)

  1. 4 beats with 288 cps, so n=292n = 292 or 284 cps284\text{ cps}.
  2. Wax lowers nn, and the beats fall to 2, so nn was above 288.
  3. 292→290 cps292 \to 290\text{ cps} gives 2 beats.
  4. So the answer is (b) 292 cps292\text{ cps}.
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Q527JEE Main 2002 · AIEEEEasy

Beats · Loading, filing and unknown frequency

When temperature increases, the frequency of a tuning fork

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Answer: (b)

  1. Frequency of a fork depends on the elasticity of its material.
  2. On heating, the Young's modulus decreases (and the prongs lengthen), so the fork vibrates more slowly.
  3. So the answer is (b) decreases.
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Q528NEET 1999 · AIPMTMedium

Beats · Beat frequency from two waves

Two waves of wavelength 50 cm50\text{ cm} and 51 cm51\text{ cm} produce 1212 beats/s. The speed of sound is

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Answer: (a)

  1. v0.50−v0.51=12\dfrac{v}{0.50} - \dfrac{v}{0.51} = 12
  2. v⋅0.010.50×0.51=12⇒v=12×0.2550.01v \cdot \dfrac{0.01}{0.50 \times 0.51} = 12 \Rightarrow v = \dfrac{12 \times 0.255}{0.01}
  3. v=306 m/sv = 306\text{ m/s}
  4. So the answer is (a) 306 m/s306\text{ m/s}.
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Q529NEET 1995 · AIPMTMedium

Beats · Loading, filing and unknown frequency

A source of sound gives 5 beats per second, when sounded with another source of frequency 100 second−1100\text{ second}^{-1}. The second harmonic of the source, together with a source of frequency 205 sec−1205\text{ sec}^{-1} gives 5 beats per second. What is the frequency of the source?

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Answer: (a)

  1. n=100±5=105n = 100 \pm 5 = 105 or 95 s−195\text{ s}^{-1}.
  2. Second harmonic 2n=2102n = 210 or 190 s−1190\text{ s}^{-1}.
  3. With 205: 210−205=5210 - 205 = 5 beats (190 gives 15).
  4. So the answer is (a) 105 second−1105\text{ second}^{-1}.
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Q530NEET 1994 · AIPMTMedium

Beats · Loading, filing and unknown frequency

A source of frequency υ\upsilon gives 5 beats/second when sounded with a source of frequency 200 Hz200\text{ Hz}. The second harmonic of frequency 2υ2\upsilon of source gives 10 beats/second when sounded with a source of frequency 420 Hz420\text{ Hz}. The value of υ\upsilon is

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Answer: (a)

  1. υ=200±5=205\upsilon = 200 \pm 5 = 205 or 195 Hz195\text{ Hz}.
  2. 2υ=4102\upsilon = 410 or 390 Hz390\text{ Hz}.
  3. With 420 Hz: 420−410=10420 - 410 = 10 beats (390 gives 30).
  4. So the answer is (a) 205 Hz205\text{ Hz}.
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Q531NEET 1992 · AIPMTEasy

Beats · Beat frequency from two waves

For production of beats the two sources must have

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Answer: (b)

  1. Beats occur whenever two waves of slightly different frequencies superpose
  2. Equal amplitude or same phase is not required (equal amplitude only makes them clearer)
  3. So the answer is (b) different frequencies.
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Q532MHT CET 2026 · 13 MAY · SHIFT 1Easy

Doppler Effect · Moving source

A whistle sends out 256 waves in a second. If the whistle approaches the observer with velocity (13)rd\left(\frac{1}{3}\right)^{rd} of the velocity of sound in air. The number of waves per second observer will receive is

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Answer: (a)

  1. Source approaching: n′=nvv−vsn' = n\frac{v}{v - v_s}.
  2. n′=256×vv−v/3=256×32n' = 256 \times \frac{v}{v - v/3} = 256 \times \frac{3}{2}
  3. n′=384n' = 384 waves per second. So the answer is (a) 384384.
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Q533MHT CET 2026 · 12 MAY · SHIFT 1Easy

Doppler Effect · Moving source

A whistle giving out 400400 Hz approaches a stationary observer at a speed of 3434 m/s. The frequency heard by the observer (in Hz) is nearly (speed of sound=340= 340 m/s)

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Answer: (c)

  1. Source approaching: n′=nvv−vsn' = n\frac{v}{v - v_s}.
  2. n′=400×340340−34=400×340306n' = 400 \times \frac{340}{340 - 34} = 400 \times \frac{340}{306}
  3. n′≈444n' \approx 444 Hz. So the answer is (c) 444444.
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Q534MHT CET 2026 · 20 APR · SHIFT 1Easy

Doppler Effect · Moving source

A train is moving towards a stationary observer with speed 3434 m/s. A train sounds a whistle of frequency 450450 Hz. If the speed of sound is 340340 m/s, the frequency heard by the observer in Hz is

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Answer: (c)

  1. Source approaching: n′=nvv−vsn' = n\frac{v}{v - v_s}.
  2. n′=450×340306=450×109n' = 450 \times \frac{340}{306} = 450 \times \frac{10}{9}
  3. n′=500n' = 500 Hz. So the answer is (c) 500500.
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Q535MHT CET 2026 · 14 MAY · SHIFT 1Easy

Doppler Effect · Moving observer

An observer moves towards a stationary source of sound with a velocity (15)th\left(\frac{1}{5}\right)^{th} of the velocity of sound. The percentage increase in the apparent frequency is

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Answer: (c)

  1. Observer approaching: n′=nv+vovn' = n\frac{v + v_o}{v}.
  2. n′=nv+v/5v=1.2nn' = n\frac{v + v/5}{v} = 1.2n
  3. Increase =20%= 20\%. So the answer is (c) 20%20\%.
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Q536MHT CET 2026 · 16 APR · SHIFT 2Easy

Doppler Effect · Source and observer both moving

A person observes two moving trains. 'A' reaching the station and 'B' leaving the station with equal speed of 30m/s. If both trains emit sounds with frequency 300 Hz, (speed of sound = 330 m/s) difference of frequencies heard by the person will be

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Answer: (c)

  1. Train A approaching: fA=300×330330−30=330f_A = 300 \times \frac{330}{330 - 30} = 330 Hz.
  2. Train B receding: fB=300×330330+30=275f_B = 300 \times \frac{330}{330 + 30} = 275 Hz.
  3. Difference =330−275=55= 330 - 275 = 55 Hz. So the answer is (c) 5555 Hz.
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Q537MHT CET 2026 · 11 APR · SHIFT 2Medium

Doppler Effect · Moving source

A source of sound is moving towards a stationary observer with velocity 'VSV_S' and then moves away with velocity 'VSV_S'. Assume that medium through which the sound waves travel is at rest. If 'V' is the velocity of sound and 'n' is the frequency emitted by the source then the difference between the apparent frequencies heard by the observer is

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Answer: (a)

  1. Approaching: n1=nVV−Vsn_1 = \dfrac{nV}{V - V_s}; receding: n2=nVV+Vsn_2 = \dfrac{nV}{V + V_s}.
  2. n1−n2=nV (V+Vs)−(V−Vs)V2−Vs2=2nVVsV2−Vs2n_1 - n_2 = nV\,\dfrac{(V+V_s) - (V-V_s)}{V^2 - V_s^2} = \dfrac{2nVV_s}{V^2 - V_s^2}
  3. So the answer is (a).
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Q538MHT CET 2026 · 16 APR · SHIFT 1Medium

Doppler Effect · Moving observer

When the observer moves towards a stationary source with velocity 'V1V_1 ', the apparent frequency of the emitted note is 'F1F_1 '. When the observer moves away from the source with velocity 'V1V_1', the apparent frequency is 'F2F_2'. If 'V' is the speed of sound in air and F1/F2=2F_1/F_2 = 2, then V/V1=V/V_1 =

Show answer and solution

Answer: (b)

  1. Observer moving: F1=F V+V1VF_1 = F\,\dfrac{V + V_1}{V}, F2=F V−V1VF_2 = F\,\dfrac{V - V_1}{V}.
  2. F1F2=V+V1V−V1=2⇒V=3V1\dfrac{F_1}{F_2} = \dfrac{V + V_1}{V - V_1} = 2 \Rightarrow V = 3V_1
  3. So the answer is (b) 3.
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Q539MHT CET 2026 · 13 MAY · SHIFT 2Medium

Doppler Effect · Beats from the Doppler effect

Two sirens situated one km apart are producing sound of frequency 330330 Hz. The observer starts moving from one siren to the other with a speed of 22 m/s. If the speed of sound is 330330 m/s, What will be the beat frequency heard by the observer?

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Answer: (b)

  1. Observer moves away from one siren and towards the other with u=2u = 2 m/s.
  2. Towards: f1=fv+uv=330×332330=332f_1 = f\frac{v+u}{v} = 330 \times \frac{332}{330} = 332 Hz
  3. Away: f2=fv−uv=330×328330=328f_2 = f\frac{v-u}{v} = 330 \times \frac{328}{330} = 328 Hz
  4. Beat frequency =f1−f2=4= f_1 - f_2 = 4 Hz
  5. So the answer is (b) 44 Hz.
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Q540MHT CET 2025 · 25 APR · SHIFT 2Easy

Doppler Effect · Moving source

At what speed should a source of sound move so that the observer finds the apparent frequency equal to half the original frequency?

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Answer: (d)

  1. A lower frequency means the source moves away: n′=nVV+vsn' = n\frac{V}{V + v_s}.
  2. n2=nVV+vs⇒V+vs=2V\frac{n}{2} = n\frac{V}{V + v_s} \Rightarrow V + v_s = 2V
  3. vs=Vv_s = V, moving away from the observer. So the answer is (d) V.
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Q541MHT CET 2025 · 25 APR · SHIFT 1Easy

Doppler Effect · Moving source

A sound source is moving towards a stationary observer with (110)\left(\frac{1}{10}\right)th the speed of sound, The ratio of apparent to real frequency is

Show answer and solution

Answer: (a)

  1. Source approaching: n′n=vv−vs\frac{n'}{n} = \frac{v}{v - v_s}.
  2. n′n=vv−v/10=109\frac{n'}{n} = \frac{v}{v - v/10} = \frac{10}{9}
  3. So the answer is (a) 109\frac{10}{9}.
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Q542MHT CET 2025 · 19 APR · SHIFT 1Easy

Doppler Effect · Moving source

When source of sound moves towards a stationary observer, the apparent frequency heard by him

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Answer: (b)

  1. A moving source crowds its waves together in front: λ′=v−vsn\lambda' = \frac{v - v_s}{n}, smaller than λ\lambda.
  2. With the speed of sound unchanged, n′=vλ′n' = \frac{v}{\lambda'} is larger.
  3. So the answer is (b): frequency increases while wavelength decreases.
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Q543MHT CET 2025 · 23 APR · SHIFT 1Easy

Doppler Effect · Moving observer

An observer moves towards a stationary source of sound with a velocity of one fifth of the velocity of sound. The percentage increase in the apparent frequency is

Show answer and solution

Answer: (c)

  1. Observer approaching: n′=nv+vovn' = n\frac{v + v_o}{v}.
  2. n′=n(1+15)=1.2nn' = n\left(1 + \frac{1}{5}\right) = 1.2n
  3. Increase =20%= 20\%. So the answer is (c) 20%20\%.
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Q544MHT CET 2025 · 5 MAY · SHIFT 2Easy

Doppler Effect · Source and observer both moving

A person observes two moving trains. First reaching the station and another leaves the station with equal speed of 30 m/s30\text{ m/s}. If both trains emit sounds of frequency 300 Hz, difference of frequencies heard by the person will be (speed of sound in air 330 m/s330\text{ m/s})

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Answer: (c)

  1. Approaching train: f1=300×330300=330f_1 = 300 \times \frac{330}{300} = 330 Hz.
  2. Receding train: f2=300×330360=275f_2 = 300 \times \frac{330}{360} = 275 Hz.
  3. Difference =55= 55 Hz. So the answer is (c) 55 Hz.
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Q545MHT CET 2025 · 22 APR · SHIFT 2Easy

Doppler Effect · Source and observer both moving

When source of sound and observer both are moving towards each other, the observer will hear

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Answer: (c)

  1. Approaching each other: n′=nv+vov−vs>nn' = n\frac{v + v_o}{v - v_s} > n, so frequency is higher.
  2. The moving source compresses the waves ahead of it: λ′=v−vsn<λ\lambda' = \frac{v - v_s}{n} < \lambda.
  3. So the answer is (c): high frequency, low wavelength.
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Q546MHT CET 2025 · 26 APR · SHIFT 2Medium

Doppler Effect · Moving observer

When the observer moves towards a stationary source with velocity V1V_1, the apparent frequency of emitted note is F1F_1. When observer moves away from the source with velocity V1V_1, the apparent frequency is F2F_2. If V is the velocity of sound in air and F1/F2=2F_1/F_2 = 2 then V/V1V/V_1 is equal to

Show answer and solution

Answer: (a)

  1. Observer moving: F1=F V+V1VF_1 = F\,\dfrac{V + V_1}{V}, F2=F V−V1VF_2 = F\,\dfrac{V - V_1}{V}.
  2. V+V1V−V1=2⇒V=3V1\dfrac{V + V_1}{V - V_1} = 2 \Rightarrow V = 3V_1
  3. So the answer is (a) 3.
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Q547MHT CET 2025 · 20 APR · SHIFT 1Medium

Doppler Effect · Moving observer

When an observer moves towards a stationary source with velocity ' V1V_1 ', the apparent frequency of emitted note is ' F1F_1 '. When observer moves away from stationary source with velocity ' V1V_1 ' the apparent frequency is ' F2F_2 '. If ' v ' is velocity of sound in air and F1F2=2\frac{F_1}{F_2} = 2, then VV1\frac{V}{V_1} is equal to

Show answer and solution

Answer: (c)

  1. Observer moving: F1=F V+V1VF_1 = F\,\dfrac{V + V_1}{V}, F2=F V−V1VF_2 = F\,\dfrac{V - V_1}{V}.
  2. V+V1V−V1=2⇒V=3V1\dfrac{V + V_1}{V - V_1} = 2 \Rightarrow V = 3V_1
  3. So the answer is (c) 3.
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Q548MHT CET 2025 · 26 APR · SHIFT 1Medium

Doppler Effect · Source and observer both moving

A source of sound emits sound wave of frequency ' f ' and moves towards an observer with a velocity V3\frac{V}{3} where V is the velocity of sound. If the observer moves away from the source with a velocity V5\frac{V}{5} the apparent frequency heard by him will be

Show answer and solution

Answer: (c)

  1. Observer moving away, source approaching: f′=f V−VoV−Vsf' = f\,\dfrac{V - V_o}{V - V_s}.
  2. f′=f V−V/5V−V/3=f 4/52/3=65ff' = f\,\dfrac{V - V/5}{V - V/3} = f\,\dfrac{4/5}{2/3} = \dfrac{6}{5}f
  3. So the answer is (c) 65f\dfrac{6}{5}f.
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Q549MHT CET 2025 · 23 APR · SHIFT 2Medium

Doppler Effect · Source and observer both moving

If a source emitting waves of frequency ' FF ' moves towards an observer with a velocity V3\frac{V}{3} and the observer moves away from the source with a velocity V4\frac{V}{4}, the apparent frequency as heard by the observer will be ( V=V = velocity of sound)

Show answer and solution

Answer: (a)

  1. Observer moving away, source approaching: F′=F V−VoV−VsF' = F\,\dfrac{V - V_o}{V - V_s}.
  2. F′=F V−V/4V−V/3=F 3/42/3=98FF' = F\,\dfrac{V - V/4}{V - V/3} = F\,\dfrac{3/4}{2/3} = \dfrac{9}{8}F
  3. So the answer is (a) 98F\dfrac{9}{8}F.
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Q550MHT CET 2025 · 21 APR · SHIFT 2Difficult

Doppler Effect · Moving observer

A vehicle starts from rest and accelerates along straight path at 2 m/s22\text{ m/s}^2. At the starting point of the vehicle, there is a stationary electric siren. How far has the vehicle nearly gone when the driver hears the siren at 94%94\% of its value when the vehicle was at rest?

(speed of sound =330 m/s= 330\text{ m/s})

Show answer and solution

Answer: (a)

  1. Observer moving away from a stationary source: f′=fv−uvf' = f\frac{v-u}{v}
  2. 0.94=330−u330⇒u=0.06×330=19.80.94 = \frac{330 - u}{330} \Rightarrow u = 0.06 \times 330 = 19.8 m/s
  3. From rest: s=u22a=(19.8)22×2≈98s = \frac{u^2}{2a} = \frac{(19.8)^2}{2 \times 2} \approx 98 m
  4. So the answer is (a) 98 m.
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Q551MHT CET 2024 · 3 MAY · SHIFT 2Easy

Doppler Effect · Moving observer

An observer moves towards a stationary source of sound with a velocity of one-fifth of the velocity of sound. The percentage increase in the apparent frequency is

Show answer and solution

Answer: (c)

  1. Observer approaching: n′=nv+vovn' = n\frac{v + v_o}{v}.
  2. n′=n(1+15)=1.2nn' = n\left(1 + \frac{1}{5}\right) = 1.2n
  3. Increase =20%= 20\%. So the answer is (c) 20%20\%.
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Q552MHT CET 2024 · 4 MAY · SHIFT 2Easy

Doppler Effect · Source and observer both moving

A train sounding a whistle of frequency 510 Hz approaches a station at 72 km/hr72\text{ km/hr}. The frequency of the note heard by an observer on the platform as the train (1) approaches the station and then (2) recedes the station are respectively (in hertz) (velocity of sound in air =320 m/s= 320\text{ m/s})

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Answer: (a)

  1. 7272 km/h =20= 20 m/s.
  2. Approaching: n1=510×320320−20=544n_1 = 510 \times \frac{320}{320 - 20} = 544 Hz
  3. Receding: n2=510×320320+20=480n_2 = 510 \times \frac{320}{320 + 20} = 480 Hz
  4. So the answer is (a) 544,480544, 480.
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Q553MHT CET 2024 · 11 MAY · SHIFT 1Medium

Doppler Effect · Moving observer

With what velocity an observer should move relative to a stationary source so that a sound of triple the frequency of source is heard by an observer?

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Answer: (d)

  1. Observer moving towards a stationary source: f′=f v+uvf' = f\,\dfrac{v + u}{v}.
  2. 3f=f v+uv⇒u=2v3f = f\,\dfrac{v + u}{v} \Rightarrow u = 2v
  3. So the answer is (d) twice the speed of sound, towards the source.
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Q554MHT CET 2024 · 10 MAY · SHIFT 1Medium

Doppler Effect · Moving observer

When the listener moves towards stationary source with velocity ' V1V_1 ', the apparent frequency of emitted note is ' F1F_1 '. When observer moves away from the source with velocity ' V1V_1 ', apparent frequency is ' F2F_2 '. If V is the velocity of sound in air and F1F2=2\frac{F_1}{F_2} = 2 then VV1\frac{V}{V_1} is

Show answer and solution

Answer: (b)

  1. Observer moving: F1=F V+V1VF_1 = F\,\dfrac{V + V_1}{V}, F2=F V−V1VF_2 = F\,\dfrac{V - V_1}{V}.
  2. V+V1V−V1=2⇒V=3V1\dfrac{V + V_1}{V - V_1} = 2 \Rightarrow V = 3V_1
  3. So the answer is (b) 3.
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Q555MHT CET 2024 · 16 MAY · SHIFT 2Medium

Doppler Effect · Source and observer both moving

A source and listener are both moving towards each other with speed V10\frac{V}{10}. (where V is speed of sound) If the frequency of sound note emitted by the source is ' nn ', then the frequency heard by the listener would be nearly

Show answer and solution

Answer: (b)

  1. Both approaching: n′=n V+VoV−Vsn' = n\,\dfrac{V + V_o}{V - V_s}.
  2. n′=n 1+0.11−0.1=119n≈1.22nn' = n\,\dfrac{1 + 0.1}{1 - 0.1} = \dfrac{11}{9}n \approx 1.22n
  3. So the answer is (b) 1.22n1.22n.
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Q556MHT CET 2024 · 3 MAY · SHIFT 1Medium

Doppler Effect · Source and observer both moving

The pitch of a whistle of an engine appears to drop by 30%30\% of original value when it passes a stationary observer. If the speed of sound in air is 350 ms−1350\text{ ms}^{-1}, then the speed of engine in ms−1\text{ms}^{-1} is

Show answer and solution

Answer: (d)

  1. After passing, the engine recedes and the heard pitch is 70% of the original: f′=f vv+u=0.7ff' = f\,\dfrac{v}{v + u} = 0.7f.
  2. 350=0.7(350+u)⇒350+u=500350 = 0.7(350 + u) \Rightarrow 350 + u = 500
  3. So the answer is (d) u=150 m/su = 150\text{ m/s}.
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Q557MHT CET 2024 · 15 MAY · SHIFT 1Medium

Doppler Effect · Reflection from a wall or moving obstacle

The driver of a car travelling with a speed ' V1V_1 ' m/s\text{m/s} towards a wall sounds a siren of frequency ' nn ' Hz. If the velocity of sound in air is V m/sV\text{ m/s}, then the frequency of sound reflected from the wall and as heard by the driver, in Hz, is

Show answer and solution

Answer: (a)

  1. Wall receives n1=n VV−V1n_1 = n\,\dfrac{V}{V - V_1} (source approaching).
  2. Wall re-emits n1n_1; driver approaches it: n′=n1 V+V1V=(V+V1V−V1)nn' = n_1\,\dfrac{V + V_1}{V} = \left(\dfrac{V + V_1}{V - V_1}\right)n
  3. So the answer is (a).
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Q558MHT CET 2024 · 2 MAY · SHIFT 2Medium

Doppler Effect · Reflection from a wall or moving obstacle

The driver of a car travelling with a speed ' V1V_1 ' m/s\text{m/s} towards a wall sounds a siren of frequency ' nn ' Hz. If the velocity of sound in air is ' V ' m/s\text{m/s}, then the frequency of the sound reflected from the wall and as heard by the driver in Hz is

Show answer and solution

Answer: (c)

  1. Wall receives n1=n VV−V1n_1 = n\,\dfrac{V}{V - V_1} (source approaching).
  2. Wall re-emits n1n_1; driver approaches it: n′=n1 V+V1V=(V+V1V−V1)nn' = n_1\,\dfrac{V + V_1}{V} = \left(\dfrac{V + V_1}{V - V_1}\right)n
  3. So the answer is (c).
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Q559MHT CET 2023 · 14 MAY · SHIFT 2Easy

Doppler Effect · Moving source

A source of sound is moving towards a stationary observer with (110)\left(\frac{1}{10}\right)th the of the speed of sound. The ratio of apparent to real frequency is

Show answer and solution

Answer: (a)

  1. Source approaching: n′n=vv−vs\frac{n'}{n} = \frac{v}{v - v_s}.
  2. n′n=vv−v/10=109\frac{n'}{n} = \frac{v}{v - v/10} = \frac{10}{9}
  3. So the answer is (a) 10:910 : 9.
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Q560JEE Main 2023 · 25 JAN · SHIFT 2EasyOld syllabus

Doppler Effect · Moving source

A train blowing a whistle of frequency 320 Hz approaches an observer standing on the platform at a speed of 66 m/s. The frequency observed by the observer will be (given speed of sound = 330 ms −1-1) __________ Hz.

Numerical answer type. Work it out, then open the answer.

Show answer and solution

Answer: 400

  1. Source approaching: n′=nvv−vsn' = n\frac{v}{v - v_s}.
  2. n′=320×330330−66=320×330264n' = 320 \times \frac{330}{330 - 66} = 320 \times \frac{330}{264}
  3. n′=400n' = 400 Hz
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Q561MHT CET 2023 · 13 MAY · SHIFT 1Easy

Doppler Effect · Source and observer both moving

A passenger is sitting in a train which is moving fast. The engine of the train blows a whistle of frequency 'nn'. If the apparent frequency of sound heard by the passenger is 'ff' then

Show answer and solution

Answer: (a)

  1. The passenger and the engine move together, so there is no relative motion between source and listener.
  2. No Doppler shift: f=nf = n.
  3. So the answer is (a) f=nf = n.
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Q562MHT CET 2023 · 9 MAY · SHIFT 1Easy

Doppler Effect · Source and observer both moving

When both source and listener are approaching each other the observed frequency of sound is given by (VL(V_L and VSV_S is the velocity of listener and source respectively, n0=n_0 = radiated frequency)

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Answer: (a)

  1. Listener moving towards the source raises the received rate: numerator V+VLV + V_L.
  2. Source moving towards the listener shortens the wavelength: denominator V−VsV - V_s.
  3. n=n0[V+VLV−Vs]n = n_0\left[\frac{V + V_L}{V - V_s}\right]. So the answer is (a).
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Q563JEE Main 2023 · 11 APR · SHIFT 2EasyOld syllabus

Doppler Effect · Source and observer both moving

A car P travelling at 20 ms−120\text{ ms}^{-1} sounds its horn at a frequency of400 Hz400\text{ Hz}. Another car QQ is travelling behind the first car in the same direction with a velocity 40 ms−140\text{ ms}^{-1}. The frequency heard by the passenger of the car QQ is approximately [Take, velocity of sound =360 ms−1= 360\text{ ms}^{-1} ]

Show answer and solution

Answer: (c)

Q40 m/sP20 m/ssound P to Q
  1. Sound travels backward from P to Q. Q moves towards P (towards the sound): numerator v+40v + 40.
  2. P moves away from Q: denominator v+20v + 20.
  3. n′=400×360+40360+20=400×400380n' = 400 \times \frac{360 + 40}{360 + 20} = 400 \times \frac{400}{380}
  4. n′≈421n' \approx 421 Hz. So the answer is (c) 421 Hz.
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Q564JEE Main 2023 · 8 APR · SHIFT 1EasyOld syllabus

Doppler Effect · Source and observer both moving

The engine of a train moving with speed 10 ms−110\text{ ms}^{-1} towards a platform sounds a whistle at frequency 400 Hz400\text{ Hz}. The frequency heard by a passenger inside the train is: (neglect air speed. Speed of sound in air =330 ms−1= 330\text{ ms}^{-1})

Show answer and solution

Answer: (c)

  1. The passenger moves with the engine at the same velocity, so there is no relative motion between source and listener.
  2. No Doppler shift: frequency heard =400= 400 Hz.
  3. So the answer is (c) 400 Hz.
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Q565JEE Main 2023 · 29 JAN · SHIFT 1EasyOld syllabus

Doppler Effect · Source and observer both moving

A person observes two moving trains, 'A' reaching the station and 'B' leaving the station with equal speed of 30 m/s30\text{ m/s}. If both trains emit sounds with frequency 300 Hz300\text{ Hz}, (Speed of sound: 330 m/s330\text{ m/s}) approximate difference of frequencies heard by the person will be:

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Answer: (b)

  1. Train A approaching: fA=300×330300=330f_A = 300 \times \frac{330}{300} = 330 Hz.
  2. Train B receding: fB=300×330360=275f_B = 300 \times \frac{330}{360} = 275 Hz.
  3. Difference =55= 55 Hz. So the answer is (b) 55 Hz.
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Q566MHT CET 2023 · 11 MAY · SHIFT 1Medium

Doppler Effect · Source and observer both moving

A car sounding a horn of frequency 1000 Hz1000\text{ Hz} passes a stationary observer. The ratio of frequencies of the horn noted by the observer before and after passing the car is 11:911 : 9. If the speed of sound is 'vv', the speed of the car is

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Answer: (d)

  1. Before: f1=f vv−uf_1 = f\,\dfrac{v}{v - u}; after: f2=f vv+uf_2 = f\,\dfrac{v}{v + u}, so f1f2=v+uv−u\dfrac{f_1}{f_2} = \dfrac{v + u}{v - u}.
  2. v+uv−u=119⇒9v+9u=11v−11u⇒20u=2v\dfrac{v + u}{v - u} = \dfrac{11}{9} \Rightarrow 9v + 9u = 11v - 11u \Rightarrow 20u = 2v
  3. So the answer is (d) u=v/10u = v/10.
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Q567MHT CET 2023 · 10 MAY · SHIFT 1Medium

Doppler Effect · Source and observer both moving

Consider the Doppler effect in two cases. In the first case, an observer moves towards a stationary source of sound with a speed of 50 m/s50\text{ m/s}. In the second case, the observer is at rest and the source moves towards the observer with the same speed of 50 m/s50\text{ m/s}. Then the frequency heard by the observer will be

[velocity of sound in air =330 m/s= 330\text{ m/s}.]

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Answer: (b)

  1. Observer moving: f1=f 330+50330≈1.15ff_1 = f\,\dfrac{330 + 50}{330} \approx 1.15f.
  2. Source moving: f2=f 330330−50≈1.18ff_2 = f\,\dfrac{330}{330 - 50} \approx 1.18f.
  3. So the answer is (b) more in the second case.
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Q568JEE Main 2023 · 6 APR · SHIFT 1MediumOld syllabus

Doppler Effect · Reflection from a wall or moving obstacle

A person driving car at a constant speed of 15 m/s15\text{ m/s} is approaching a vertical wall. The person notices a change of 40 Hz40\text{ Hz} in the frequency of his car's horn upon reflection from the wall. The frequency of horn is _______________ Hz\text{Hz}.

(Given: Speed of sound: 330 m/s330\text{ m/s})

Numerical answer type. Work it out, then open the answer.

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Answer: 420

  1. Echo frequency f′=f v+uv−u=f 345315f' = f\,\dfrac{v + u}{v - u} = f\,\dfrac{345}{315}.
  2. Change f′−f=f 30315=40f' - f = f\,\dfrac{30}{315} = 40
  3. f=40×31530=420 Hzf = \dfrac{40 \times 315}{30} = 420\text{ Hz}
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Q569JEE Main 2022 · 27 JUN · SHIFT 1EasyOld syllabus

Doppler Effect · Moving observer

An observer moves towards a stationary source of sound with a velocity equal to one-fifth of the velocity of sound. The percentage change in the frequency will be:

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Answer: (a)

  1. Observer approaching: n′=nv+vovn' = n\frac{v + v_o}{v}.
  2. n′=n(1+15)=1.2nn' = n\left(1 + \frac{1}{5}\right) = 1.2n
  3. Change =20%= 20\%. So the answer is (a) 20%.
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Q570JEE Main 2022 · 28 JUL · SHIFT 1EasyOld syllabus

Doppler Effect · Reflection from a wall or moving obstacle

The frequency of echo will be __________ Hz if the train blowing a whistle of frequency 320 Hz is moving with a velocity of 36 km/h towards a hill from which an echo is heard by the train driver. Velocity of sound in air is 330 m/s.

Numerical answer type. Work it out, then open the answer.

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Answer: 340

  1. Train speed u=36 km/h=10 m/su = 36\text{ km/h} = 10\text{ m/s}.
  2. Echo heard by the driver: f′=f v+uv−u=320×340320f' = f\,\dfrac{v+u}{v-u} = 320 \times \dfrac{340}{320}
  3. f′=340 Hzf' = 340\text{ Hz}
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Q571JEE Main 2022 · 26 JUL · SHIFT 1MediumOld syllabus

Doppler Effect · Source and observer both moving

When a car is approaching the observer, the frequency of horn is 100 Hz100\text{ Hz}. After passing the observer, it is 50 Hz50\text{ Hz}. If the observer moves with the car, the frequency will be x3 Hz\frac{x}{3}\text{ Hz} where x=x = ________________.

Numerical answer type. Work it out, then open the answer.

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Answer: 200

  1. 100=f vv−u100 = f\,\dfrac{v}{v - u} and 50=f vv+u50 = f\,\dfrac{v}{v + u}, so v+uv−u=2⇒u=v3\dfrac{v + u}{v - u} = 2 \Rightarrow u = \dfrac{v}{3}.
  2. Actual frequency f=100 v−uv=100×23=2003 Hzf = 100\,\dfrac{v - u}{v} = 100 \times \dfrac{2}{3} = \dfrac{200}{3}\text{ Hz}.
  3. Moving with the car there is no relative motion, so the observer hears 2003 Hz\dfrac{200}{3}\text{ Hz}.
  4. x=200x = 200
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Q572JEE Main 2022 · 30 JUN · SHIFT 1DifficultOld syllabus

Doppler Effect · Source and observer both moving

An employee of a factory moving away from his workplace by a car listens to the siren of the factory. He drives the car at the speed of 72 kmh−1{}^{-1} in the direction of wind which is blowing at 72 kmh−1{}^{-1} speed. Frequency of siren is 720 Hz. The employee hears an apparent frequency of ____________ Hz.

(Assume speed of sound to be 340 ms−1{}^{-1})

Numerical answer type. Work it out, then open the answer.

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Answer: 680

  1. Car speed == wind speed =72= 72 km/h =20= 20 m/s, both away from the factory.
  2. Wind adds to sound speed along its direction: v′=340+20=360v' = 340 + 20 = 360 m/s
  3. Observer moving away: f′=fv′−uv′=720×360−20360f' = f\frac{v' - u}{v'} = 720 \times \frac{360 - 20}{360}
  4. f′=680f' = 680 Hz
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Q573JEE Main 2022 · 25 JUL · SHIFT 1DifficultOld syllabus

Doppler Effect · Beats from the Doppler effect

An observer is riding on a bicycle and moving towards a hill at 18 kmh−118\text{ kmh}^{-1}. He hears a sound from a source at some distance behind him directly as well as after its reflection from the hill. If the original frequency of the sound as emitted by source is 640 Hz640\text{ Hz} and velocity of the sound in air is 320 m/s320\text{ m/s}, the beat frequency between the two sounds heard by observer will be _____________ Hz\text{Hz}.

Numerical answer type. Work it out, then open the answer.

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Answer: 20

SourceObserver5 m/sHilldirect 630 Hzreflected 650 Hz
  1. Observer speed u=18u = 18 km/h =5= 5 m/s, towards the hill and away from the source.
  2. Direct sound (observer moving away): f1=640×320−5320=630f_1 = 640 \times \frac{320 - 5}{320} = 630 Hz
  3. Reflected sound reaches the hill at 640640 Hz (hill at rest); observer moves towards it: f2=640×320+5320=650f_2 = 640 \times \frac{320 + 5}{320} = 650 Hz
  4. Beat frequency =650−630=20= 650 - 630 = 20 Hz
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Q574JEE Main 2021 · 27 AUG · SHIFT 1EasyOld syllabus

Doppler Effect · Source and observer both moving

Two cars X and Y are approaching each other with velocities 36 km/h and 72 km/h respectively. The frequency of a whistle sound as emitted by a passenger in car X, heard by the passenger in car Y is 1320 Hz. If the velocity of sound in air is 340 m/s, the actual frequency of the whistle sound produced is .................. Hz.

Numerical answer type. Work it out, then open the answer.

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Answer: 1210

  1. vX=36v_X = 36 km/h =10= 10 m/s (source), vY=72v_Y = 72 km/h =20= 20 m/s (observer), approaching.
  2. n′=nv+vov−vs⇒1320=n×340+20340−10=n×360330n' = n\frac{v + v_o}{v - v_s} \Rightarrow 1320 = n \times \frac{340 + 20}{340 - 10} = n \times \frac{360}{330}
  3. n=1320×330360=1210n = 1320 \times \frac{330}{360} = 1210 Hz
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Q575JEE Main 2021 · 26 AUG · SHIFT 1EasyOld syllabus

Doppler Effect · Source and observer both moving

A source and a detector move away from each other in absence of wind with a speed of 20 m/s with respect to the ground. If the detector detects a frequency of 1800 Hz of the sound coming from the source, then the original frequency of source considering speed of sound in air 340 m/s will be ............... Hz.

Numerical answer type. Work it out, then open the answer.

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Answer: 2025

  1. Moving apart: n′=nv−vov+vsn' = n\frac{v - v_o}{v + v_s}.
  2. 1800=n×340−20340+20=n×891800 = n \times \frac{340 - 20}{340 + 20} = n \times \frac{8}{9}
  3. n=1800×98=2025n = 1800 \times \frac{9}{8} = 2025 Hz
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Q576JEE Main 2021 · 20 JUL · SHIFT 1MediumOld syllabus

Doppler Effect · Reflection from a wall or moving obstacle

The frequency of a car horn encountered a change from 400 Hz to 500 Hz, when the car approaches a vertical wall. If the speed of sound is 330 m/s. Then the speed of car is ___________ km/h.

Numerical answer type. Work it out, then open the answer.

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Answer: 132

  1. Echo: 500400=330+u330−u\dfrac{500}{400} = \dfrac{330 + u}{330 - u}
  2. 5(330−u)=4(330+u)⇒9u=330⇒u=36.67 m/s5(330 - u) = 4(330 + u) \Rightarrow 9u = 330 \Rightarrow u = 36.67\text{ m/s}
  3. u=36.67×3.6=132 km/hu = 36.67 \times 3.6 = 132\text{ km/h}
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Q577JEE Main 2021 · 24 FEB · SHIFT 2MediumOld syllabus

Doppler Effect · Beats from the Doppler effect

Two cars are approaching each other at an equal speed of 7.2 km/hr. When they see each other, both blow horns having frequency of 676 Hz. The beat frequency heard by each driver will be ___________ Hz. [Velocity of sound in air is 340 m/s.]

Numerical answer type. Work it out, then open the answer.

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Answer: 8

  1. Speed of each car =7.2= 7.2 km/h =2= 2 m/s.
  2. Each driver is an observer approaching a source approaching him: f′=fv+uv−uf' = f\frac{v+u}{v-u}
  3. f′=676×342338=684f' = 676 \times \frac{342}{338} = 684 Hz
  4. Beat frequency =684−676=8= 684 - 676 = 8 Hz
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Q578MHT CET 2020 · 16 OCT · SHIFT 2Medium

Doppler Effect · Reflection from a wall or moving obstacle

An obstacle is moving towards the source with velocity vv. The sound is reflected from the obstacle. If cc is the speed of sound and λ\lambda is the wavelength, then the wavelength of the reflected wave λr\lambda_r is

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Answer: (a)

  1. Obstacle as moving observer: f1=f c+vcf_1 = f\,\dfrac{c + v}{c}.
  2. Obstacle as moving source towards the original source: fr=f1 cc−v=f c+vc−vf_r = f_1\,\dfrac{c}{c - v} = f\,\dfrac{c + v}{c - v}.
  3. λr=cfr=(c−vc+v)λ\lambda_r = \dfrac{c}{f_r} = \left(\dfrac{c - v}{c + v}\right)\lambda
  4. So the answer is (a).
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Q579JEE Main 2020 · 5 SEP · SHIFT 2MediumOld syllabus

Doppler Effect · Reflection from a wall or moving obstacle

A driver in a car, approaching a vertical wall notices that the frequency of his car horn, has changed from 440 Hz to 480 Hz, when it gets reflected from the wall. If the speed of sound in air is 345 m/s, then the speed of the car is:

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Answer: (b)

  1. Echo: 480440=1211=345+u345−u\dfrac{480}{440} = \dfrac{12}{11} = \dfrac{345 + u}{345 - u}
  2. 12(345−u)=11(345+u)⇒23u=345⇒u=15 m/s12(345 - u) = 11(345 + u) \Rightarrow 23u = 345 \Rightarrow u = 15\text{ m/s}
  3. 15×3.6=54 km/h15 \times 3.6 = 54\text{ km/h}
  4. So the answer is (b) 54 km/hr.
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Q580JEE Main 2020 · 4 SEP · SHIFT 2MediumOld syllabus

Doppler Effect · Reflection from a wall or moving obstacle

The driver of a bus approaching a big wall notices that the frequency of his bus's horn changes from 420 Hz to 490 Hz when he hears it after it gets reflected from the wall. Find the speed of the bus if speed of the sound is 330 ms–1.

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Answer: (a)

  1. Echo: 490420=76=330+u330−u\dfrac{490}{420} = \dfrac{7}{6} = \dfrac{330 + u}{330 - u}
  2. 7(330−u)=6(330+u)⇒13u=330⇒u≈25.4 m/s7(330 - u) = 6(330 + u) \Rightarrow 13u = 330 \Rightarrow u \approx 25.4\text{ m/s}
  3. 25.4×3.6≈91 km/h25.4 \times 3.6 \approx 91\text{ km/h}
  4. So the answer is (a) 91 km/h.
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Q581JEE Main 2020 · 6 SEP · SHIFT 1DifficultOld syllabus

Doppler Effect · Moving source

A sound source S is moving along a straight track with speed v, and is emitting, sound of frequency v0 (see figure). An observer is standing at a finite distance, at the point O, from the track. The time variation of frequency heard by the observer is best represented by:

(t0 represents the instant when the distance between the source and observer is minimum)

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Answer: (d)

  1. Heard frequency ν=ν0vsoundvsound−vcos⁡θ\nu = \frac{\nu_0 v_{sound}}{v_{sound} - v\cos\theta}, where θ\theta is the angle between the source velocity and the line to O.
  2. Far before O: θ≈0\theta \approx 0, so ν\nu is maximum and nearly constant, above ν0\nu_0.
  3. As the source passes, cos⁡θ\cos\theta falls smoothly from +1+1 to −1-1, so ν\nu decreases continuously, through about ν0\nu_0 near t0t_0.
  4. Far after O: ν\nu levels off at a minimum below ν0\nu_0.
  5. So the answer is (d), the smooth decreasing curve.
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Q582JEE Main 2020 · 7 JAN · SHIFT 2DifficultOld syllabus

Doppler Effect · Beats from the Doppler effect

A stationary observer receives sound from two identical tuning forks, one of which approaches and the other one recedes with the same speed (much less than the speed of sound). The observer hears 2 beats/sec. The oscillation frequency of each tuning fork is v0 = 1400 Hz and the velocity of sound in air is 350 m/s. The speed of each tuning fork is close to:

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Answer: (c)

  1. Approaching fork: f1=ν0vv−uf_1 = \nu_0\frac{v}{v - u}; receding fork: f2=ν0vv+uf_2 = \nu_0\frac{v}{v + u}
  2. For u≪vu \ll v: beats =f1−f2≈2ν0uv= f_1 - f_2 \approx \frac{2\nu_0 u}{v}
  3. 2=2×1400×u350=8u⇒u=142 = \frac{2 \times 1400 \times u}{350} = 8u \Rightarrow u = \frac{1}{4} m/s
  4. So the answer is (c) 14\frac{1}{4} m/s.
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Q583JEE Main 2019 · 9 APR · SHIFT 2EasyOld syllabus

Doppler Effect · Source and observer both moving

Two cars A and B are moving away from each other in opposite directions. Both the cars are moving with a speed of 20 ms–1 with respect to the ground. If an observer in car A detects a frequency 2000 Hz of the sound coming from car B, what is the natural frequency of the sound source in car B?

(speed of sound in air = 340 ms–1) :-

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Answer: (c)

  1. Moving apart: n′=nv−vov+vsn' = n\frac{v - v_o}{v + v_s}.
  2. 2000=n×340−20340+20=n×892000 = n \times \frac{340 - 20}{340 + 20} = n \times \frac{8}{9}
  3. n=2000×98=2250n = 2000 \times \frac{9}{8} = 2250 Hz. So the answer is (c) 2250 Hz.
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Q584JEE Main 2019 · 10 APR · SHIFT 2MediumOld syllabus

Doppler Effect · Moving source

A source of sound S is moving with a velocity of 50 m/s towards a stationary observer. The observer measures the frequency of the source as 1000 Hz. What will be the apparent frequency of the source when it is moving away from the observer after crossing him? (Take velocity of sound in air is 350 m/s)

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Answer: (a)

  1. Approaching: 1000=f 350350−50⇒f=1000×300350≈857 Hz1000 = f\,\dfrac{350}{350 - 50} \Rightarrow f = \dfrac{1000 \times 300}{350} \approx 857\text{ Hz}.
  2. Receding: f′=f 350350+50=1000×300400f' = f\,\dfrac{350}{350 + 50} = 1000 \times \dfrac{300}{400}
  3. So the answer is (a) 750 Hz.
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Q585JEE Main 2019 · 10 JAN · SHIFT 1MediumOld syllabus

Doppler Effect · Moving source

A train moves towards a stationary observer with speed 34 m/s. The train sounds a whistle and its frequency registered by the observer is ƒ1. If the speed of the train is reduced to 17 m/s, the frequency registered is ƒ2. If speed of sound is 340 m/s, then the ratio ƒ1/ƒ2 is -

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Answer: (a)

  1. Source approaching: f′=f vv−uf' = f\,\dfrac{v}{v - u}, so f1f2=v−u2v−u1\dfrac{f_1}{f_2} = \dfrac{v - u_2}{v - u_1}.
  2. f1f2=340−17340−34=323306=1918\dfrac{f_1}{f_2} = \dfrac{340 - 17}{340 - 34} = \dfrac{323}{306} = \dfrac{19}{18}
  3. So the answer is (a) 19/18.
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Q586JEE Main 2019 · 10 APR · SHIFT 1MediumOld syllabus

Doppler Effect · Moving observer

A stationary source emits sound waves of frequency 500 Hz. Two observers moving along a line passing through the source detect sound to be of frequencies 480 Hz and 530 Hz. Their respective speeds are, in ms–1, (Given speed of sound = 300 m/s)

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Answer: (a)

  1. 480 Hz is lower, so that observer moves away: 480=500 300−u1300⇒u1=12 m/s480 = 500\,\dfrac{300 - u_1}{300} \Rightarrow u_1 = 12\text{ m/s}.
  2. 530 Hz is higher, so that observer moves towards: 530=500 300+u2300⇒u2=18 m/s530 = 500\,\dfrac{300 + u_2}{300} \Rightarrow u_2 = 18\text{ m/s}.
  3. So the answer is (a) 12, 18.
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Q587JEE Main 2019 · 9 JAN · SHIFT 2MediumOld syllabus

Doppler Effect · Moving observer

A musician using an open flute of length 50 cm producess second harmonic sound waves. A person runs towards the musician from another end of hall at a speed of 10 km/h. If the wave speed is 330 m/s, the frequency heard by the running person shall be close to:

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Answer: (a)

  1. Open pipe, second harmonic: f=2v2L=2×3302×0.5=660 Hzf = \dfrac{2v}{2L} = \dfrac{2 \times 330}{2 \times 0.5} = 660\text{ Hz}.
  2. Runner speed u=10 km/h≈2.78 m/su = 10\text{ km/h} \approx 2.78\text{ m/s}.
  3. f′=660×330+2.78330≈665.6 Hzf' = 660 \times \dfrac{330 + 2.78}{330} \approx 665.6\text{ Hz}
  4. So the answer is (a) 666 Hz.
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Q588JEE Main 2019 · 12 APR · SHIFT 1MediumOld syllabus

Doppler Effect · Reflection from a wall or moving obstacle

A submarine (A) travelling at 18 km/hr is being chased along the line of its velocity by another submarine (B) travelling at 27 km/hr. B sends a sonar signal of 500 Hz to detect A and receives a reflected sound of frequency vv. The value of vv is close to: (Speed of sound in water =1500 ms–1)

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Answer: (b)

  1. vB=27 km/h=7.5 m/sv_B = 27\text{ km/h} = 7.5\text{ m/s} (chasing), vA=18 km/h=5 m/sv_A = 18\text{ km/h} = 5\text{ m/s} (ahead, same direction).
  2. A receives: f1=500 1500−51500−7.5=500 14951492.5f_1 = 500\,\dfrac{1500 - 5}{1500 - 7.5} = 500\,\dfrac{1495}{1492.5} (A moves away, B moves towards).
  3. B receives the echo: f2=f1 1500+7.51500+5=f1 1507.51505f_2 = f_1\,\dfrac{1500 + 7.5}{1500 + 5} = f_1\,\dfrac{1507.5}{1505}
  4. f2≈500×1.00334≈501.7 Hzf_2 \approx 500 \times 1.00334 \approx 501.7\text{ Hz}
  5. So the answer is (b) 502 Hz.
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Q589JEE Main 2019 · 12 APR · SHIFT 2MediumOld syllabus

Doppler Effect · Beats from the Doppler effect

Two sources of sound S1 and S2 produce sound waves of same frequency 660 Hz. A listener is moving from source S1 towards S2 with a constant speed u m/s and he hears 10 beats/s. The velocity of sound is 330 m/s. Then, u equals:

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Answer: (d)

  1. Moving away from S1S_1: f1=fv−uvf_1 = f\frac{v-u}{v}; moving towards S2S_2: f2=fv+uvf_2 = f\frac{v+u}{v}
  2. Beats =f2−f1=2fuv= f_2 - f_1 = \frac{2fu}{v}
  3. 10=2×660×u330=4u⇒u=2.510 = \frac{2 \times 660 \times u}{330} = 4u \Rightarrow u = 2.5 m/s
  4. So the answer is (d) 2.5 m/s.
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Q590NEET 2017EasyOld syllabus

Doppler Effect · Source and observer both moving

Two cars moving in opposite directions approach each other with speed of 22 ms−1{}^{-1} and 16.5 m s−1{}^{-1} respectively. The driver of the first car blows a horn having a frequency 400 Hz. The frequency heard by the driver of the second car is (velocity of sound is 340 m s−1{}^{-1})

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Answer: (c)

  1. Both approaching: n′=nv+vov−vsn' = n\frac{v + v_o}{v - v_s}, with vs=22v_s = 22 m/s, vo=16.5v_o = 16.5 m/s.
  2. n′=400×340+16.5340−22=400×356.5318n' = 400 \times \frac{340 + 16.5}{340 - 22} = 400 \times \frac{356.5}{318}
  3. n′≈448n' \approx 448 Hz. So the answer is (c) 448 Hz.
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Q591JEE Main 2017MediumOld syllabus

Doppler Effect · Moving observer

An observer is moving with half the speed of light towards a stationary microwave source emitting waves at frequency 10 GHz. What is the frequency of the microwave measured by the observer? (speed of light = 3 ×108 ms–1)

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Answer: (d)

  1. For light use the relativistic Doppler formula: f′=f1+β1−βf' = f\sqrt{\dfrac{1 + \beta}{1 - \beta}} with β=0.5\beta = 0.5.
  2. f′=101.50.5=103≈17.3 GHzf' = 10\sqrt{\dfrac{1.5}{0.5}} = 10\sqrt{3} \approx 17.3\text{ GHz}
  3. So the answer is (d) 17.3 GHz.
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Q592JEE Main 2016 · 9 APR · SHIFT 1MediumOld syllabus

Doppler Effect · Source and observer both moving

Two engines pass each other moving in opposite directions with uniform speed of 30 m/s. One of them is blowing a whistle of frequency 540 Hz. Calculate the frequency heard by driver of second engine before they pass each other. Speed of sound is 330 m/sec:

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Answer: (c)

  1. Before passing, both engines approach each other: f′=f v+vov−vsf' = f\,\dfrac{v + v_o}{v - v_s}.
  2. f′=540×330+30330−30=540×360300f' = 540 \times \dfrac{330 + 30}{330 - 30} = 540 \times \dfrac{360}{300}
  3. So the answer is (c) 648 Hz.
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Q593NEET 2016 · PHASE 1MediumOld syllabus

Doppler Effect · Reflection from a wall or moving obstacle

A siren emitting a sound of frequency 800 Hz moves away from an observer towards a cliff at a speed of 15 m s−1{}^{-1}. Then, the frequency of sound that the observer hears in the echo reflected from the cliff is

(Take velocity of sound in air = 330 m s−1{}^{-1})

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Answer: (a)

  1. The siren approaches the cliff, so the cliff receives f1=f vv−uf_1 = f\,\dfrac{v}{v - u}.
  2. The stationary cliff reflects f1f_1 unchanged to the stationary observer.
  3. f1=800×330315≈838 Hzf_1 = 800 \times \dfrac{330}{315} \approx 838\text{ Hz}
  4. So the answer is (a) 838 Hz.
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Q594JEE Main 2016 · 10 APR · SHIFT 1DifficultOld syllabus

Doppler Effect · Beats from the Doppler effect

A toy-car, blowing its horn, is moving with a steady speed of 5 m/s, away from a wall. An observer, towards whom the toy car is moving, is able to hear 5 beats per second. If the velocity of sound in air is 340 m/s, the frequency of the horn of the toy car is close to:

Show answer and solution

Answer: (d)

  1. Direct sound (car approaching observer): f1=fvv−uf_1 = f\frac{v}{v - u}
  2. Wall receives fvv+uf\frac{v}{v + u} (car receding from wall) and reflects it unchanged to the observer: f2=fvv+uf_2 = f\frac{v}{v + u}
  3. Beats =f1−f2≈2fuv= f_1 - f_2 \approx \frac{2fu}{v}
  4. 5=2×f×5340⇒f=1705 = \frac{2 \times f \times 5}{340} \Rightarrow f = 170 Hz
  5. So the answer is (d) 170 Hz.
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Q595NEET 2015 · AIPMTMediumOld syllabus

Doppler Effect · Moving source

A source of sound S emitting waves of frequency 100 Hz and an observer O are located at some distance from each other. The source is moving with a speed of 19.4 m s−1{}^{-1} at an angle of 60° with the source observer line as shown in the figure. The observer is at rest. The apparent frequency observed by the observer (velocity of sound in air 330 m s−1{}^{-1}), is

Figure

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Answer: (d)

  1. Only the velocity component along the source–observer line matters: u=19.4cos⁡60∘=9.7 m/su = 19.4\cos 60^\circ = 9.7\text{ m/s} towards O.
  2. f′=f vv−u=100×330330−9.7=33000320.3f' = f\,\dfrac{v}{v - u} = 100 \times \dfrac{330}{330 - 9.7} = \dfrac{33000}{320.3}
  3. f′≈103 Hzf' \approx 103\text{ Hz}
  4. So the answer is (d) 103 Hz.
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Q596JEE Main 2015 · 10 APR · SHIFT 1MediumOld syllabus

Doppler Effect · Reflection from a wall or moving obstacle

A bat moving at 10 ms−1{}^{-1} towards a wall sends a sound signal of 8000 Hz towards it. On reflection it hears a sound of frequency f. The value of f in Hz is close to (speed of sound = 320 ms−1{}^{-1})

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Answer: (b)

  1. Echo heard by the bat moving towards the wall: f=f0 v+uv−uf = f_0\,\dfrac{v + u}{v - u}.
  2. f=8000×330310≈8516 Hzf = 8000 \times \dfrac{330}{310} \approx 8516\text{ Hz}
  3. So the answer is (b) 8516 Hz.
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Q597JEE Main 2015 · 11 APR · SHIFT 1DifficultOld syllabus

Doppler Effect · Source and observer both moving

A source of sound emits sound waves at frequency f0. It is moving towards an observer with fixed speed vvs (vvs < vv, where vv is the speed of the sound in air). If the observer were to move towards the source with speed vv0, one of the following two graphs (A and B) will give the correct variation of the frequency f heard by the observer as vv0 is changed.

Figure

The variation of f with vv0 is given correctly by:

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Answer: (a)

  1. Both approaching: f=f0v+v0v−vs=f0vv−vs+f0v−vsv0f = f_0\frac{v + v_0}{v - v_s} = \frac{f_0 v}{v - v_s} + \frac{f_0}{v - v_s}v_0
  2. ff is linear in v0v_0 with a positive intercept, which is graph A.
  3. Slope =f0v−vs= \frac{f_0}{v - v_s}
  4. So the answer is (a).
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Q598JEE Main 2015DifficultOld syllabus

Doppler Effect · Source and observer both moving

A train is moving on a straight track with speed 20 ms−1.20\text{ ms}^{-1}. It is blowing its whistle at the frequency of 1000 Hz1000\text{ Hz}. The percentage change in the frequency heard by a person standing near the track as the train passes him is (speed of sound =320 ms−1= 320\text{ ms}^{-1}) close to:

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Answer: (d)

  1. Approaching: f1=1000×320320−20≈1066.7f_1 = 1000 \times \frac{320}{320 - 20} \approx 1066.7 Hz
  2. Receding: f2=1000×320320+20≈941.2f_2 = 1000 \times \frac{320}{320 + 20} \approx 941.2 Hz
  3. Percentage change =f1−f2f1×100=125.51066.7×100≈12%= \frac{f_1 - f_2}{f_1} \times 100 = \frac{125.5}{1066.7} \times 100 \approx 12\%
  4. So the answer is (d) 12%12\%.
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Q599JEE Main 2014 · 11 APR · SHIFT 1EasyOld syllabus

Doppler Effect · Beats from the Doppler effect

Two factories are sounding their sirens at 800 Hz. A man goes from one factory to other at a speed of 2 m/s. The velocity of sound is 320 m/s. The number of beats heard by the person in one second will be:

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Answer: (d)

  1. Moving from one source to the other: beats =2fuv= \dfrac{2fu}{v}.
  2. =2×800×2320=10= \dfrac{2 \times 800 \times 2}{320} = 10
  3. So the answer is (d) 10.
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Q600NEET 2014 · AIPMTMediumOld syllabus

Doppler Effect · Source and observer both moving

A speeding motorcyclist sees traffic jam ahead him. He slows down to 36 km hour−1{}^{-1}. He finds that traffic has eased and a car moving ahead of him at 18 km hour−1{}^{-1} is honking at a frequency of 1392 Hz. If the speed of sound is 343 m s−1{}^{-1}, the frequency of the honk as heard by him will be

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Answer: (c)

  1. Motorcyclist (observer) =36 km/h=10 m/s= 36\text{ km/h} = 10\text{ m/s} towards the car; car (source) =18 km/h=5 m/s= 18\text{ km/h} = 5\text{ m/s} away from him.
  2. f′=f v+vov+vs=1392×343+10343+5=1392×353348f' = f\,\dfrac{v + v_o}{v + v_s} = 1392 \times \dfrac{343 + 10}{343 + 5} = 1392 \times \dfrac{353}{348}
  3. f′≈1412 Hzf' \approx 1412\text{ Hz}
  4. So the answer is (c) 1412 Hz.
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Q601JEE Main 2014 · 12 APR · SHIFT 1DifficultOld syllabus

Doppler Effect · Moving source

A source of sound A emitting waves of frequency 1800 Hz is falling towards ground with a terminal speed vv. The observer B on the ground directly beneath the source receives waves of frequency 2150 Hz, The source A receives waves, reflected from ground, of frequency nearly: (Speed of sound = 343 m/s)

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Answer: (b)

  1. At B (source approaching): 2150=1800×343343−v⇒v≈55.82150 = 1800 \times \frac{343}{343 - v} \Rightarrow v \approx 55.8 m/s
  2. Ground reflects 21502150 Hz; A is an observer moving towards it at vv.
  3. f=2150×343+55.8343≈2500f = 2150 \times \frac{343 + 55.8}{343} \approx 2500 Hz
  4. So the answer is (b) 2500 Hz.
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Q602NEET 2013EasyOld syllabus

Doppler Effect · Beats from the Doppler effect

Two sources P and Q produce notes of frequency 660 Hz. each. A listener moves from P to Q with a speed of 1 ms−1{}^{-1}. If the speed of sound is 330 m/s, then the number of beats heard by the listener per second will be

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Answer: (a)

  1. Moving towards Q: fQ=f v+uvf_Q = f\,\dfrac{v+u}{v}; moving away from P: fP=f v−uvf_P = f\,\dfrac{v-u}{v}.
  2. Beats =fQ−fP=2fuv=2×660×1330= f_Q - f_P = \dfrac{2fu}{v} = \dfrac{2 \times 660 \times 1}{330}
  3. So the answer is (a) 4 beats per second.
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Q603JEE Main 2013 · 22 APR · SHIFT 1MediumOld syllabus

Doppler Effect · Beats from the Doppler effect

A and B are two sources generating sound waves. A listener is situated at C. The frequency of the source at A is 500 Hz. A, now, moves towards C with a speed 4 m/s. The number of beats heard at C is 6. When A moves away from C with speed 4 m/s, the number of beats heard at C is 18. The speed of sound is 340 m/s. The frequency of the source at B is:

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Answer: (c)

  1. A approaching C: fA=500×340340−4=500×340336≈506f_A = 500 \times \frac{340}{340-4} = 500 \times \frac{340}{336} \approx 506 Hz
  2. A receding from C: fA′=500×340344≈494f_A' = 500 \times \frac{340}{344} \approx 494 Hz
  3. Beats: ∣506−fB∣=6|506 - f_B| = 6 and ∣494−fB∣=18|494 - f_B| = 18
  4. Both hold only for fB=512f_B = 512 Hz.
  5. So the answer is (c) 512 Hz.
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Q604NEET 2012 · AIPMT · MAINSMediumOld syllabus

Doppler Effect · Reflection from a wall or moving obstacle

A train moving at a speed of 220 m s−1{}^{-1} towards a stationary object, emits a sound of frequency 1000 Hz. Some of the sound reaching the object gets reflected back to the train as echo. The frequency of the echo as detected by the driver of the train is

(Speed of sound in air is 330 m s−1{}^{-1})

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Answer: (c)

  1. Echo heard by a driver moving towards the reflector: f′=f v+uv−uf' = f\,\dfrac{v + u}{v - u}.
  2. f′=1000×330+220330−220=1000×550110f' = 1000 \times \dfrac{330 + 220}{330 - 220} = 1000 \times \dfrac{550}{110}
  3. So the answer is (c) 5000 Hz.
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Q605NEET 2009 · AIPMTEasyOld syllabus

Doppler Effect · Reflection from a wall or moving obstacle

The driver of a car travelling with speed 30 m/s towards a hill sounds a horn of frequency 600 Hz. If the velocity of sound in air is 330 m/s, the frequency of reflected sound as heard by driver is

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Answer: (b)

  1. The hill receives the horn from a source approaching it, then reflects it back to the driver, who is an observer approaching the hill.
  2. n′=nv+vcv−vcn' = n\frac{v + v_c}{v - v_c}
  3. n′=600×330+30330−30=600×360300=720n' = 600 \times \frac{330 + 30}{330 - 30} = 600 \times \frac{360}{300} = 720 Hz
  4. So the answer is (b) 720 Hz.
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Q606JEE Main 2009 · AIEEEDifficultOld syllabus

Doppler Effect · Moving observer

A motor cycle starts from rest and accelerates along a straight path at 2 m/s2.2\text{ m/s}^2. At the starting point of the motor cycle there is a stationary electric siren. How far has the motor cycle gone when the driver hears the frequency of the siren at 94%94\% of its value when the motor cycle was at rest? (Speed of sound =330 ms−1= 330\text{ ms}^{-1})

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Answer: (a)

  1. Observer moving away from a stationary source: f′=fv−uvf' = f\frac{v-u}{v}
  2. 0.94=330−u330⇒u=19.80.94 = \frac{330 - u}{330} \Rightarrow u = 19.8 m/s
  3. From rest: s=u22a=(19.8)24≈98s = \frac{u^2}{2a} = \frac{(19.8)^2}{4} \approx 98 m
  4. So the answer is (a) 9898 m.
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Q607JEE Main 2006 · AIEEEMediumOld syllabus

Doppler Effect · Moving source

A whistle producing sound waves of frequencies 9500 Hz9500\text{ Hz} and above is approaching a stationary person with speed v ms−1.v\text{ ms}^{-1}. The velocity of sound in air is 300 ms−1.300\text{ ms}^{-1}. If the person can hear frequencies upto a maximum of 10,000 Hz,10{,}000\text{ Hz}, the maximum value of vv upto which he can hear whistle is

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Answer: (c)

  1. The lowest emitted frequency (9500 Hz) must not exceed 10000 Hz after the shift.
  2. 10000=9500×300300−v⇒300−v=28510000 = 9500 \times \dfrac{300}{300 - v} \Rightarrow 300 - v = 285
  3. So the answer is (c) v=15 m/sv = 15\text{ m/s}.
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Q608JEE Main 2005 · AIEEEEasyOld syllabus

Doppler Effect · Moving observer

An observer moves towards a stationary source of sound, with a velocity one-fifth of the velocity of sound. What is the percentage increase in the apparent frequency?

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Answer: (c)

  1. Observer approaching: n′=nv+vovn' = n\frac{v + v_o}{v}.
  2. n′=n(1+15)=1.2nn' = n\left(1 + \frac{1}{5}\right) = 1.2n
  3. Increase =20%= 20\%. So the answer is (c) 20%20\%.
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Q609NEET 2004 · AIPMTEasyOld syllabus

Doppler Effect · Reflection from a wall or moving obstacle

A car is moving towards a high cliff. The driver sounds a horn of frequency ff. The reflected sound heard by the driver has frequency 2f2f. If v is the velocity of sound, then the velocity of the car, in the same velocity units, will be

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Answer: (b)

  1. Echo from a cliff heard by a driver moving at uu: f′=f v+uv−uf' = f\,\dfrac{v+u}{v-u}.
  2. f′=2f⇒v+u=2v−2u⇒3u=vf' = 2f \Rightarrow v + u = 2v - 2u \Rightarrow 3u = v
  3. So the answer is (b) u=v/3u = v/3.
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Q610NEET 2003 · AIPMTEasyOld syllabus

Doppler Effect · Moving observer

An observer moves towards a stationary source of sound with a speed 1/5th of the speed of sound. The wavelength and frequency of the source emitted are λ\lambda and ff respectively. The apparent frequency and wavelength recorded by the observer are respectively

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Answer: (b)

  1. Observer approaching: f′=fv+v/5v=1.2ff' = f\frac{v + v/5}{v} = 1.2f.
  2. The source is at rest, so the waves in air are not compressed: the wavelength stays λ\lambda.
  3. So the answer is (b) 1.2f1.2f, λ\lambda.
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Q611NEET 2002 · AIPMTMediumOld syllabus

Doppler Effect · Moving source

A whistle revolves in a circle with angular speed ω\omega = 20 rad/s using a string of length 50 cm. If the frequency of sound from the whistle is 385 Hz, then what is the minimum frequency heard by an observer which is far away from the centre (velocity of sound == 340 m/s)

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Answer: (b)

  1. Speed of the whistle u=ωr=20×0.5=10 m/su = \omega r = 20 \times 0.5 = 10\text{ m/s}.
  2. Minimum frequency when the whistle moves directly away: fmin=f vv+u=385×340350f_{min} = f\,\dfrac{v}{v + u} = 385 \times \dfrac{340}{350}
  3. fmin=374 Hzf_{min} = 374\text{ Hz}
  4. So the answer is (b) 374 Hz.
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Q612NEET 2000 · AIPMTEasyOld syllabus

Doppler Effect · Beats from the Doppler effect

Two stationary sources each emitting waves of wavelength λ\lambda, an observer moves from one source to another with velocity u. Then number of beats heard by him

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Answer: (a)

  1. Source frequency f=v/λf = v/\lambda.
  2. Approaching one source: f v+uvf\,\dfrac{v+u}{v}; leaving the other: f v−uvf\,\dfrac{v-u}{v}.
  3. Beats =2fuv=2uλ= \dfrac{2fu}{v} = \dfrac{2u}{\lambda}
  4. So the answer is (a) 2uλ\dfrac{2u}{\lambda}.
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Q613NEET 1998 · AIPMTEasy

Doppler Effect · Moving source

A vehicle, with a horn of frequency nn is moving with a velocity of 30 m/s30\text{ m/s} in a direction perpendicular to the straight line joining the observer and the vehicle. The observer perceives the sound to have a frequency n+n1n + n_1. Then (if the sound velocity in air is 300 m/s300\text{ m/s})

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Answer: (b)

  1. Doppler shift depends only on the velocity component along the line joining source and observer.
  2. The vehicle moves perpendicular to this line, so that component is zero.
  3. So n′=nn' = n, i.e. n1=0n_1 = 0. So the answer is (b).
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Q614NEET 1991 · AIPMTMedium

Doppler Effect · Source and observer both moving

Two trains move towards each other with the same speed. The speed of sound is 340 m/s340\text{ m/s}. If the height of the tone of the whistle of one of them heard on the other changes to 9/89/8 times, then the speed of each train should be

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Answer: (a)

  1. Both approaching with speed uu: f′f=340+u340−u=98\dfrac{f'}{f} = \dfrac{340 + u}{340 - u} = \dfrac{9}{8}.
  2. 2720+8u=3060−9u⇒17u=3402720 + 8u = 3060 - 9u \Rightarrow 17u = 340
  3. So the answer is (a) u=20 m/su = 20\text{ m/s}.
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