A source producing the sound of frequency 170 Hz is approaching a stationary observer with a velocity of 17 m/s. The apparent change in the wavelength of sound heard by the observer is (speed of sound in air = 340 m/s)
A. 0.1m
B. 0.2m
C. 0.4m
D. 0.5m
Answer
244.8k+ views
Hint:To find the apparent change in wavelength, we find the apparent change in the frequency due to Doppler effect and then using the relation between the wave speed, frequency and the wavelength, we get the apparent change in wavelength of the sound.
Formula used:
\[{f_{ap}} = {f_o}\left( {\dfrac{{v \pm {v_o}}}{{v \pm {v_s}}}} \right)\]
where \[{f_{ap}}\] is the apparent frequency heard by the listener moving with speed \[{v_o}\] with respect to the source which is moving with speed \[{v_s}\], \[{f_o}\] is the original frequency and v is the speed of sound in air.
\[v = f\lambda \]
where v is the speed of the wave, f is the frequency of the wave and \[\lambda \] is the wavelength of the wave.
Complete step by step solution:
It is given that the source of the sound is approaching towards the stationary observer.
The Doppler Effect formula for the sound source moving towards the stationary observer is,
\[{f_{ap}} = {f_o}\left( {\dfrac{v}{{v - {v_s}}}} \right)\]
The speed of sound, v is given as 340 m/s and the original frequency is given as 170 Hz.
So, the apparent frequency is,
\[{f_{ap}} = \left( {170\,Hz} \right)\left( {\dfrac{{340}}{{340 - 17}}} \right) \\ \]
\[\Rightarrow {f_{ap}} = 170 \times \dfrac{{340}}{{323}}Hz \\ \]
\[\Rightarrow {f_{ap}} = 179\,Hz\]
Using the relation between the speed of the wave, frequency and the wavelength we get the initial and final wavelength. By finding differences, we get the change in wavelength.
\[\Delta \lambda = {\lambda _i} - {\lambda _f} \\ \]
\[\Rightarrow \Delta \lambda = \dfrac{v}{{{f_o}}} - \dfrac{v}{{{f_{ap}}}} \\ \]
\[\Rightarrow \Delta \lambda = \left( {\dfrac{{340}}{{170}} - \dfrac{{340}}{{179}}} \right)m \\ \]
\[\therefore \Delta \lambda = 0.10\,m\]
Hence, the apparent change in the wavelength of the sound wave is 0.10 m.
Therefore, the correct option is A.
Note: The Doppler’s effect is for the change in the frequency due to relative motion between the source of the sound and the observer. So, we can’t directly use the Doppler’s effect for the change in wavelength for the mechanical wave-like sound.
Formula used:
\[{f_{ap}} = {f_o}\left( {\dfrac{{v \pm {v_o}}}{{v \pm {v_s}}}} \right)\]
where \[{f_{ap}}\] is the apparent frequency heard by the listener moving with speed \[{v_o}\] with respect to the source which is moving with speed \[{v_s}\], \[{f_o}\] is the original frequency and v is the speed of sound in air.
\[v = f\lambda \]
where v is the speed of the wave, f is the frequency of the wave and \[\lambda \] is the wavelength of the wave.
Complete step by step solution:
It is given that the source of the sound is approaching towards the stationary observer.
The Doppler Effect formula for the sound source moving towards the stationary observer is,
\[{f_{ap}} = {f_o}\left( {\dfrac{v}{{v - {v_s}}}} \right)\]
The speed of sound, v is given as 340 m/s and the original frequency is given as 170 Hz.
So, the apparent frequency is,
\[{f_{ap}} = \left( {170\,Hz} \right)\left( {\dfrac{{340}}{{340 - 17}}} \right) \\ \]
\[\Rightarrow {f_{ap}} = 170 \times \dfrac{{340}}{{323}}Hz \\ \]
\[\Rightarrow {f_{ap}} = 179\,Hz\]
Using the relation between the speed of the wave, frequency and the wavelength we get the initial and final wavelength. By finding differences, we get the change in wavelength.
\[\Delta \lambda = {\lambda _i} - {\lambda _f} \\ \]
\[\Rightarrow \Delta \lambda = \dfrac{v}{{{f_o}}} - \dfrac{v}{{{f_{ap}}}} \\ \]
\[\Rightarrow \Delta \lambda = \left( {\dfrac{{340}}{{170}} - \dfrac{{340}}{{179}}} \right)m \\ \]
\[\therefore \Delta \lambda = 0.10\,m\]
Hence, the apparent change in the wavelength of the sound wave is 0.10 m.
Therefore, the correct option is A.
Note: The Doppler’s effect is for the change in the frequency due to relative motion between the source of the sound and the observer. So, we can’t directly use the Doppler’s effect for the change in wavelength for the mechanical wave-like sound.
Recently Updated Pages
JEE Main 2026 Session 2 City Intimation Slip Releasing Soon

JEE Main 2027 Exam Date, Syllabus, Pattern, Registration, Eligibility & Updates

JEE Main 2026 Question Papers with Solutions PDF – Free Download

Is a Calculator Allowed in JEE Main 2026? Complete NTA Guidelines

JEE Main 2027 Syllabus: Based on Latest NTA Syllabus with PDF Download

JEE Main Exam Countdown Timer: Track Days Until Exam 2026

Trending doubts
JEE Main 2026: Exam Dates, Session 2 Updates, City Slip, Admit Card & Latest News

Ideal and Non-Ideal Solutions Explained for Class 12 Chemistry

Understanding the Angle of Deviation in a Prism

Hybridisation in Chemistry – Concept, Types & Applications

Understanding the Electric Field of a Uniformly Charged Ring

Derivation of Equation of Trajectory Explained for Students

Other Pages
CBSE Class 12 Physics Question Paper 2026: Download SET-wise PDF with Answer Key & Analysis

JEE Advanced Marks vs Ranks 2025: Understanding Category-wise Qualifying Marks and Previous Year Cut-offs

JEE Advanced 2026 - Exam Date (Released), Syllabus, Registration, Eligibility, Preparation, and More

Dual Nature of Radiation and Matter Class 12 Physics Chapter 11 CBSE Notes - 2025-26

JEE Advanced Weightage 2025 Chapter-Wise for Physics, Maths and Chemistry

Understanding Average and RMS Value in Electrical Circuits

