Why Does the Doppler Effect Differ for Moving Source and Detector?

  • Context: Undergrad 
  • Thread starter Thread starter Charlie X
  • Start date Start date
  • Tags Tags
    Doppler Doppler effect
Click For Summary

Discussion Overview

The discussion revolves around the differences in the Doppler Effect for a moving source versus a moving detector, particularly in the context of sound waves. Participants explore the mathematical formulations, implications of medium properties, and the conceptual understanding of frequency changes based on relative motion.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents the Doppler Effect formula and illustrates it with specific cases, questioning why the frequency changes differently for a moving source versus a moving detector.
  • Another participant expresses uncertainty about deriving the Doppler equation and shares their own formulation, indicating a lack of confidence in their mathematical approach.
  • There is a correction regarding the formula used, with acknowledgment of errors in earlier posts.
  • Some participants discuss the relationship between the source's movement and the frequency of sound waves in the medium, suggesting that the medium plays a crucial role in understanding the Doppler Effect.
  • Questions arise about how the Doppler Effect applies to electromagnetic radiation, with mentions of time dilation and the need for a relative speed approach.
  • Clarifications are made regarding the treatment of wavelength changes due to the source's motion and the implications for frequency calculations.
  • One participant seeks confirmation on the explanation that the frequency in the medium does not depend on the detector's speed, emphasizing the distinction between the frequency indicated by the detector and the frequency in the medium.

Areas of Agreement / Disagreement

Participants express varying levels of understanding and confidence regarding the mathematical formulations and conceptual explanations of the Doppler Effect. There is no consensus on the best approach to explain the differences in frequency changes, and multiple competing views remain regarding the implications of medium properties and the treatment of moving sources and detectors.

Contextual Notes

Some participants note limitations in their understanding of the derivations and the implications of the Doppler Effect, particularly in relation to electromagnetic radiation and the role of the medium in sound propagation.

Charlie X
Messages
5
Reaction score
0
the formula of Doppler Effect
f = fs(v + vd)/(v - vs)
(v = speed of sound; d = detector; s = source)

Simply from this formula, it can be seen that vd has differenct effect on the frequency receiver from vs.
when vd or vs approaches the speed of sound, this difference is pronounced.
make v = 343 m/s, fs = 1 Hz, the the source and detector move towards each other

Case 1
vd = 340 m/s, vs = 0
f = 683/343 = 1.99 Hz
Case 2
vd = 0, vs = 340 m/s,
f = 343/3 = 114 Hz

why would there be a difference? Isn't the source and detector move relative to each other?
my teacher says it has sth to do with medium, but i still don't get it.
 
Physics news on Phys.org
Trying to derive the equation you use from base doppler shift ones, not working for me >,< and I only explain stuff now if I am 100% sure of where the equations come from, to understand how messy mine is, I have produced:

F_{observer} = \frac{V^{2}*F_{source}}{(V-A_{source})(V+B_{observer})} = \frac{V^{2}*F_{Source}}{V^{2}+VB-VA-AB}

Where
A is source velocity
B is observer velocity
V is wave speed
F is Wave frequency

So yeah, I don't trust my math :)
 
Last edited:
May as well wait for a PF guy with more knowledge to pop over the hill annny minute now :)
 
Wrong formula

Indeed, the formula I wrote here was not correct, therefore I deleted it.
 
Last edited:
Yeah, what PieWie said, my equation is just a linear combination of the source moving and the observer moving, but that was my attempt to try and show how your irrational equation actually works I guess, since I went off the suggestion that reletive speed wouldn't work, I just combined the equation twice...I really should have just used relative velocity >,<, to rewrite PieWie's equation for easier reading then going explosive on your teacher.

f_{observed} = f_{source}\leftbracket[\frac{V}{V+V_{Relative}}\rightbracket]

Thanks PieWie ^_^ I too was wondering why the "compression" (Increase in frequency) was disproportionate to the "decompression" (decrease from moving away from source)
 
Charlie X said:
the formula of Doppler Effect
f = fs(v + vd)/(v - vs)
(v = speed of sound; d = detector; s = source)

Simply from this formula, it can be seen that vd has differenct effect on the frequency receiver from vs.
when vd or vs approaches the speed of sound, this difference is pronounced.
make v = 343 m/s, fs = 1 Hz, the the source and detector move towards each other

Case 1
vd = 340 m/s, vs = 0
f = 683/343 = 1.99 Hz
Case 2
vd = 0, vs = 340 m/s,
f = 343/3 = 114 Hz

why would there be a difference? Isn't the source and detector move relative to each other?
my teacher says it has sth to do with medium, but i still don't get it.
To understand why there's a difference, you need to understand how the Doppler formula is derived.

The fundamental difference is that when you (the detector) remain still but the source moves towards you, the speed of sound with respect to you doesn't change. But the frequency does, since the wavelength is getting shorter. If the original wavelength is \lambda_0, the new wavelength is \lambda = \lambda_0 - v_s / f_0. Since for any wave, v = f\lambda, the new frequency is:

f = v/\lambda = v/(\lambda_0 - v_s / f_0) = f_0 \frac{v}{(v - v_s)}

When the source remains fixed but you (the detector) move towards it, the wavelength stays the same but the speed of sound (relative to you) is now v&#039; = v + v_d. Thus the apparent frequency is:

f = v&#039;/\lambda_0 = (v + v_d)/\lambda_0 = f_0 \frac{(v + v_d)}{v}


Of course, if both source and detector are moving, you get the combination of both effects:

f = f_0 \frac{(v + v_d)}{(v - v_s)}


I hope that makes a bit of sense.
 
I don't know weather to love doc'al or slap myself in the face :) or do both, so doc'al, how is this handled with EM Radiation? as the speed is constant in that case, would you just use a relative speed case for that?

EDIT: Oh, and I didnt quite understand:

\lambda = \lambda_0 - v_s / f_0

For my low-level ability, it sort of sounds like your treating the sources movement as a wave emmitter in its own right, but taking the wavelength produced from the sound... is it ok for a deeper explanation? You know I'm a picky little mofo.
 
Last edited:
The F_{0} From the first equation, is equal to the f from the last one, so you substitute the f_{0} in the second equation to give:

f_{final}=f_{0}\bracketleft[\frac{v(v+v_{d})}{v(v-v_{s})}\bracketright] then cancel variables ^^
 
AbedeuS said:
how is this handled with EM Radiation? as the speed is constant in that case, would you just use a relative speed case for that?
It turns out that way, but you also have to factor in time dilation. Read this: Relativistic Doppler Effect

EDIT: Oh, and I didnt quite understand:

\lambda = \lambda_0 - v_s / f_0

For my low-level ability, it sort of sounds like your treating the sources movement as a wave emmitter in its own right, but taking the wavelength produced from the sound... is it ok for a deeper explanation?
The source is the emitter but I am modifying the wavelength since the source is moving with respect to the medium.
You know I'm a picky little mofo.
But cuddly and loveable, I'm sure!
 
  • #10
And I apologise to doc'al, the equation makes perfect sense, since it was the first one i wrote in my notebook, then I used the hyperphysics one, but let me just clarify:

\lambda_{new} = \lambda_{old} - v_{s}*T

and because T=f^{-1} then:

\lambda_{new} = \lambda_{old} - \frac{v_{s}}{f_{0}}
 
  • #11
Sorry I didnt get that one, it was glaring me literally in the face in my PF notebook :), also, not to hiijack, but I did some maths in that "Pascals Principle Headache" post invloving gases rather than liquids, I'd really appreciate if you could have a glance over it whenever you have free time
 
  • #12
AbedeuS said:
And I apologise to doc'al, the equation makes perfect sense, since it was the first one i wrote in my notebook, then I used the hyperphysics one, but let me just clarify:

\lambda_{new} = \lambda_{old} - v_{s}*T

and because T=f^{-1} then:

\lambda_{new} = \lambda_{old} - \frac{v_{s}}{f_{0}}
Exactly right.

AbedeuS said:
Sorry I didnt get that one, it was glaring me literally in the face in my PF notebook :), also, not to hiijack, but I did some maths in that "Pascals Principle Headache" post invloving gases rather than liquids, I'd really appreciate if you could have a glance over it whenever you have free time
I'll give it a look a bit later.
 
  • #13
Charlie X said:
Why would there be a difference? Isn't the source and detector move relative to each other?
my teacher says it has sth to do with medium, but i still don't get it.

If the source moves the sound waves have a different frequency in the medium (compared to when the source would stand still or move with a different velocity).

That is NOT the case for the detector: the frequency in the medium does not depend on the speed of the detector. Note that the frequency that is indicated by the detecor is not equal to the frequency in the medium. So... don't trust a moving sound-detector ;)

Can someone confirm this explanation?
 

Similar threads

  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 14 ·
Replies
14
Views
2K
  • · Replies 12 ·
Replies
12
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 8 ·
Replies
8
Views
1K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
Replies
8
Views
1K