Sigma Percentile
JEE Advanced (1984)
LEVELJEE Main

Animated Solution for Physics - Waves: A source of sound of frequency is placed inside water. The speed of sound in water is and in air it is . The frequency of sound recorded by an observer who is standing in air is

Select Answer:

Visualized Solution

Visualizing the Setup

  • A sound source of frequency is submerged in water.
  • An observer is standing in the air above the water surface.
  • The speed of sound in water is .
  • The speed of sound in air is .

The Core Principle of Wave Frequency

  • Frequency is a fundamental characteristic of the wave source.
  • It represents the rate of vibration of the source particles.
  • When a wave transitions from one medium to another, the boundary particles are forced to vibrate at the same rate.
  • Therefore, frequency remains constant during refraction/transmission: .

Listing the Given Parameters

  • Source frequency:
  • Speed of sound in water:
  • Speed of sound in air:

Calculating Wavelength in Water

  • Using the wave speed relation:
  • Wavelength in water:
  • Substituting the values:

Calculating Wavelength in Air

  • Wavelength in air:
  • Substituting the values:
  • Notice that the wavelength decreases as the speed decreases, keeping the frequency constant.

Concluding the Recorded Frequency

  • Since frequency is independent of the medium, the frequency heard by the observer is exactly the source frequency.
  • Recorded frequency:
  • This matches Option (d).

The Way Forward

  • If the source or observer were moving, we would apply the Doppler effect.
  • However, the change in frequency in that case is due to relative motion, not the change of medium.
  • Always distinguish between medium-dependent properties () and source-dependent properties ().

The Sigma Insight: Reflection and Transmission of Waves

Solution Diagram

Analyzing the Setup

Imagine you are standing on the edge of a quiet swimming pool. Deep below the surface, an underwater speaker is playing a pure tone of frequency . As the sound waves travel upwards, they cross the boundary between water and air, eventually reaching your ears.
We are given the following physical parameters: - Frequency of the source in water: - Speed of sound in water: - Speed of sound in air:
Our goal is to determine the frequency of the sound wave recorded by you, the observer standing in the air.

The Master Principle

Source vs. Medium
To solve this problem, we must understand a fundamental truth of wave mechanics: frequency is a characteristic of the source, not the medium.
When a wave is generated, the source vibrates at a specific rate. For our speaker, it pushes the surrounding water molecules back and forth exactly times every second. These water molecules then push the adjacent molecules, propagating the wave outward.
When the wave reaches the water-air interface, the water molecules at the boundary vibrate at and force the adjacent air molecules to vibrate at the exact same rate. The air molecules have no choice but to oscillate at the frequency of the driving force.
Therefore, as a wave transitions from one medium to another, its frequency remains absolutely constant:

What Actually Changes? Wavelength and Speed

While the frequency remains unchanged, the speed of the wave is determined strictly by the properties of the medium (such as elasticity and density). Since sound travels much slower in air () than in water (), the wave must slow down.
To maintain the fundamental wave relationship:
the wavelength must adjust proportionally to the change in speed.
Let's calculate the wavelength in both media to see this beautiful symmetry.
In water:
In air:
Notice that as the wave enters the air, its speed decreases by a factor of (from to ), and consequently, its wavelength also shrinks by a factor of (from to ).
This perfect scaling ensures that the frequency—the number of wave crests passing a point per second—remains exactly .

Final Conclusion

Since the frequency of the sound wave does not change when crossing the boundary, the observer in the air hears the exact same frequency as emitted by the source.
Thus, the correct option is (d).

Similar Questions

JEE Advanced 1991
LEVELJEE Advanced

The displacement of the medium in a sound wave is given by the equation where , and are positive constants. The wave is reflected by an obstacle situated at . The intensity of the reflected wave is times that of the incident wave. (a) What are the wavelength and frequency of incident wave? (b) Write the equation for the reflected wave. (c) In the resultant wave formed after reflection, find the maximum and minimum values of the particle speeds in the medium. (d) Express the resultant wave as a superposition of a standing wave and a travelling wave. What are the positions of the antinodes of the standing wave? What is the direction of propagation of travelling wave?

JEE Advanced 2012
LEVELJEE Main

A person blows into open-end of a long pipe. As a result, a high-pressure pulse of air travels down the pipe. When this pulse reaches the other end of the pipe,

* Multiple Correct Options
(A)
a high-pressure pulse starts travelling up the pipe, if the other end of the pipe is open.
(B)
a low-pressure pulse starts travelling up the pipe, if the other end of the pipe is open.
(C)
a low-pressure pulse starts travelling up the pipe, if the other end of the pipe is closed.
(D)
a high-pressure pulse starts travelling up the pipe, if the other end of the pipe is closed.
JEE Advanced 1998
LEVELJEE Main

A string of length and mass is tightly clamped at its ends. The tension in the string is . Identical wave pulses are produced at one end at equal intervals of time . The minimum value of , which allows constructive interference between successive pulses, is

(A)
(B)
(C)
(D)
JEE Advanced 1999
LEVELJEE Advanced

A long wire is made by joining two wires and of equal radii. has length and mass . has length and mass . The wire is under a tension of . A sinusoidal wave pulse of amplitude is sent along the wire from the end . No power is dissipated during the propagation of the wave pulse. Calculate (a) the time taken by the wave pulse to reach the other end and (b) the amplitude of the reflected and transmitted wave pulse after the incident wave pulse crosses the joint .