Conflicting Transverse Doppler Shift Equations?

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Discussion Overview

The discussion revolves around conflicting equations for the transverse Doppler shift, as presented in different sources. Participants explore the derivations and implications of these equations, focusing on their application to frequency and wavelength in the context of relativistic effects.

Discussion Character

  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants note that the Wikipedia derivation states v' = γv, while the University of Manitoba presents f' = f0(1-β^2)^(1/2) or f' = f/γ, leading to confusion.
  • One participant suggests that the first equation pertains to wavelength and the second to frequency, indicating a relationship between them since wavelength is the inverse of frequency.
  • Another participant questions the use of E = hv in the Wikipedia derivation, suggesting it implies a relationship between frequency and velocity rather than wavelength.
  • It is mentioned that the equations refer to different "transverse" conditions based on the rest frame of the emitter versus the receiver, highlighting the impact of relativistic aberration.

Areas of Agreement / Disagreement

Participants express confusion over the differing equations and their interpretations, indicating that multiple competing views remain without a clear consensus on which equation applies under what conditions.

Contextual Notes

Participants acknowledge that the equations may refer to different conditions, but the implications of these differences and the definitions of the transverse conditions remain unresolved.

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greswd said:
http://en.wikipedia.org/wiki/List_of_relativistic_equations#Doppler_shift

and

http://www.physics.umanitoba.ca/~souther/waves02/feb0402/sld011.htmIf you look at the derivation on Wikipedia:

v' = γvBut the one on Uni of Manitoba shows:

f' = f0(1-β^2)^(1/2) or f' = f/γ
I'm quite confused.
The first one is for wavelength, the second one is for frequency. Since wavelength is the inverse of frequency, you can change the first one as follows:

v' = γv

1/f' = γ/f

f = γf'

γf' = f

f' = f/γ
 
Last edited:
ghwellsjr said:
greswd said:
http://en.wikipedia.org/wiki/List_of_relativistic_equations#Doppler_shift

and

http://www.physics.umanitoba.ca/~souther/waves02/feb0402/sld011.htm


If you look at the derivation on Wikipedia:

v' = γv


But the one on Uni of Manitoba shows:

f' = f0(1-β^2)^(1/2) or f' = f/γ



I'm quite confused.

The first one is for wavelength, the second one is for frequency. Since wavelength is the inverse of frequency, you can change the first one as follows:

v' = γv

1/f' = γ/f

f = γf'

γf' = f

f' = f/γ

:bugeye:

But in the Wiki derivation they use E = hv. Isn't that the same as E = hf?

Which means that v = f as well, not wavelength?
 
greswd said:
:bugeye:

But in the Wiki derivation they use E = hv. Isn't that the same as E = hf?

Which means that v = f as well, not wavelength?
You're probably right.

I was going by the previous equation in the Wiki article which said:
Doppler shift for emitter and observer moving right towards each other (or directly away):

4099a8aba77dd55b81735edfc1b3e643.png

For an emitter moving towards an observer, the shift in the Doppler frequency is greater than one and yet they imply it is less than one. Since they also include "(or directly away)" without further explanation, I guess they expect the reader to know what they are talking about. Consider the source.

BTW: I'm still waiting for a response from you on your Triplet thread.
 
greswd said:
http://en.wikipedia.org/wiki/List_of_relativistic_equations#Doppler_shift
and
http://www.physics.umanitoba.ca/~souther/waves02/feb0402/sld011.htm

If you look at the derivation on Wikipedia: v' = γv

But the one on Uni of Manitoba shows: f' = f0(1-β^2)^(1/2) or f' = f/γ

I'm quite confused.

Both equations are correct, but they refer to two different "transverse" conditions. One equation defines the transverse condition in terms of the rest frame of the emitter, and the other defines the transverse condition in terms of the rest frame of the receiver. These two conditions are different, because of relativistic aberration. Here's a web page that explains this in detail (toward the bottom of the page):

http://www.mathpages.com/home/kmath587/kmath587.htm
 

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