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http://en.wikipedia.org/wiki/Relativ...Doppler_effect
"Assume the observer and the source are moving away from each other with a relative velocity v (v is negative if the observer and the source are moving toward each other). Considering the problem in the reference frame of the source, suppose one wavefront arrives at the observer. The next wavefront is then at a distance L=c/f_s away from him (where L is the wavelength, f_s is the frequency of the wave the source emitted, and c is the speed of light). (...) Lo/Ls=f_s/f_o=..." The equation Lo/Ls=f_s/f_o characterizes the RELATIVISTIC Doppler effect only - its raison d'être is Divine Albert's 1905 whim (the speed of light is constant and that's it). For any wave other than a light wave the wavelength measured in the frame of the observer, Lo, does not vary with the speed of the observer so in the case of a stationary source and a moving observer the relevant equation is c'/ c=f_o/f_s, where c'=c-v is the speed of the wave relative to the observer. It can be shown that, even for light waves, Lo/Ls=f_s/f_o is contradictory so c'/c=f_o/f_s is the only plausible equation. Let us assume that Einsteinians are correct in that Lo somehow varies with the speed of the observer (so that the speed of light could gloriously remain constant yes we all believe in relativity, relativity, relativity). Initially both the source and the observer are stationary so Lo=Ls holds good. Then the source starts moving with speed v and we notice that Ls, the wavelength measured in the frame of the source, remains unchanged (this is not valid for waves other than light waves). Since the observer has not moved, Lo remains unchanged as well, in accordance with our assumption. That is, Lo=Ls holds good again. Of the two equations, Lo/Ls=f_s/f_o and c'/c=f_o/f_s, only the latter is compatible with Lo=Ls. Pentcho Valev |
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