Doppler Effect inconsistent in terms of relative velocities

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Discussion Overview

The discussion revolves around the Doppler Effect, specifically addressing the perceived frequency of sound in two scenarios: one where a sound source (a car) is moving towards a stationary observer, and another where the observer is moving towards a stationary sound source. Participants explore the differences in calculated frequencies and the underlying principles of sound propagation in a medium.

Discussion Character

  • Debate/contested
  • Mathematical reasoning
  • Technical explanation

Main Points Raised

  • One participant presents a scenario with a moving car and a stationary observer, calculating a perceived frequency of 103.125 Hz.
  • In a contrasting scenario where the observer moves towards a stationary car, the same participant calculates a perceived frequency of 103.0303 Hz, questioning the discrepancy between the two results.
  • Another participant asserts that the two situations are fundamentally different due to the movement of sound relative to the air in one case and the observer's movement relative to the air in the other.
  • A later reply emphasizes that sound travels through air, establishing an absolute reference frame, which differs from the relativistic Doppler effect for light, where motion is relative.
  • One participant reiterates the initial example and elaborates on the mechanics of wave propagation in a medium, explaining how the source's motion affects the timing of wave emissions and their arrival at the observer.

Areas of Agreement / Disagreement

Participants do not reach a consensus, as there are competing views on the nature of the Doppler Effect in the two scenarios discussed. Some participants argue that the differences in perceived frequency are due to the reference frame of sound propagation, while others challenge this interpretation.

Contextual Notes

The discussion highlights the importance of understanding the medium through which sound travels and the implications of relative motion in different contexts. There are unresolved aspects regarding the application of the Doppler Effect equations and the assumptions made in each scenario.

memoguy
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Hi all!

Let me use an example to make this clear. There is a car traveling directly toward a man at 10m/s. The car is pressing down its horn, producing a frequency of 100hz. The speed of sound is 330 m/s. What frequency does the man hear?

Ok, so we can use the equation:
f_observer=( (v+v_o)/(v-v_s ) ) * f_source
Where v=330, v_o=0 & v_s = 10
Thus f_observer = 103.125

But, if the car was still and the observer moved toward the car at 10m/s we could say:
f_observer=( (v+v_o)/(v-v_s ) ) * f_source
Where v=330, v_o=10, v_s =0
thus f_observer = 103.0303...

103.0303 does not equal 103.125.

Why is there a difference, surely these two things could be the same.
 
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The two situations are not the same. In one, the sound source is moving relative to the air. In the other, the observer is moving relative to the air.

To see the difference, think about extreme situations, like
(1) the source is moving towards the observer at twice the speed of sound (660 m/s)
(2) the observer is moving towards the source at 660 m/s
 
memoguy said:
surely these two things could be the same.

No, they are not the same. Sound moves through air so all speeds are measured relative to air which gives us an absolute reference frame. Motion is not relative here. Compare that with the relativistic Doppler effect for electromagnetic waves (light).
f_o=f_s \sqrt \frac{c+v_{rel}}{c-v_{rel}},
where v_{rel} is the relative speed between source and observer. Here there is no medium and the speed of the source is measured relative to the observer. Motion is relative here.
 
memoguy said:
Hi all!

Let me use an example to make this clear. There is a car traveling directly toward a man at 10m/s. The car is pressing down its horn, producing a frequency of 100hz. The speed of sound is 330 m/s. What frequency does the man hear?

Ok, so we can use the equation:
f_observer=( (v+v_o)/(v-v_s ) ) * f_source
Where v=330, v_o=0 & v_s = 10
Thus f_observer = 103.125

But, if the car was still and the observer moved toward the car at 10m/s we could say:
f_observer=( (v+v_o)/(v-v_s ) ) * f_source
Where v=330, v_o=10, v_s =0
thus f_observer = 103.0303...

103.0303 does not equal 103.125.

Why is there a difference, surely these two things could be the same.

Sound waves, travel with constant speed in the medium (when pressure, temperature, humidity.. are constant). So when the source is moving it emits a wave, travel some distance and emits again (time between emissions is time period of the wave.)
So the source gets closer to the observer and the second wave has shorter distance to go and it arrives sooner than if the source was stationary.
The speed of the wave relative to observer is the same as this with stationary source(wave can not move in the medium slower or faster ) => speed of sound in the medium.

When the source is stationary and observer is moving, the speed of wave relative to him is the sum of his speed and waves speed (they are traveling against each other and wave travels with the speed of sound in the medium)

dopp.gif


http://hyperphysics.phy-astr.gsu.edu/hbase/sound/dopp.html
 

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