Question:

The difference between the apparent frequency of a source of sound as perceived by the observer during its approach and recession is $2\%$ of the frequency of the source. If the speed of sound in air is $ 300\,ms^{-1}$ , the velocity of the source is

Updated On: Jul 5, 2022
  • $1.5\,ms^{-1}$
  • $12\,ms^{-1}$
  • $6\, ms^{-1}$
  • $3\,ms^{-1}$
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The Correct Option is D

Solution and Explanation

When source approaches the observer, the apparent frequency heard by observer is $n'=n\left(\frac{v}{v-v_{s}}\right)$ ...(i) $v_{s}=$ speed of source of sound. During it recession, apparent frequency $n''=n\left(\frac{v}{v +v_{s}}\right)$ ...(ii) Accordingly $n'=n''=\frac{2}{100} n$ (given) $\therefore n\left(\frac{v}{v-v_{s}}\right)=n\left(\frac{v}{v +v_{s}}\right)$ $=\frac{2}{100} n$ or $v\left[\frac{v +v_{s}-v+ v_{s}}{\left(v-v_{s}\right) v +v_{s}}\right]=\frac{2}{100}$ or $\frac{2 v v_{s}}{\left(v-v_{s}\right)\left(v+ v_{s}\right)}=\frac{2}{100}$ or $100\, v v_{s}=v^{2}-v_{s}^{2}$ But speed of sound in air $v=300\, m / s$ $\therefore 30000\, v_{s}=(300)^{2}-v_{s}^{2}$ $\Rightarrow v_{s}^{2}+30000\, v_{s}-90000=0$ $\therefore v_{s}=\frac{-30000 \pm \sqrt{(30000)^{2}+4 \times 90000}}{2}$ $=\frac{-30000 \pm 30006}{2}$ $=\frac{6}{2}=3\, ms ^{-1}$
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Concepts Used:

Electromagnetic waves

The waves that are produced when an electric field comes into contact with a magnetic field are known as Electromagnetic Waves or EM waves. The constitution of an oscillating magnetic field and electric fields gives rise to electromagnetic waves.

Types of Electromagnetic Waves:

Electromagnetic waves can be grouped according to the direction of disturbance in them and according to the range of their frequency. Recall that a wave transfers energy from one point to another point in space. That means there are two things going on: the disturbance that defines a wave, and the propagation of wave. In this context the waves are grouped into the following two categories:

  • Longitudinal waves: A wave is called a longitudinal wave when the disturbances in the wave are parallel to the direction of propagation of the wave. For example, sound waves are longitudinal waves because the change of pressure occurs parallel to the direction of wave propagation.
  • Transverse waves: A wave is called a transverse wave when the disturbances in the wave are perpendicular (at right angles) to the direction of propagation of the wave.