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PAllen said:@erbahar ,
Relativistic beaming results from the joint action of two phenomena: aberration, and Doppler. Both occur for radio waves just as readily as visible light. Aberration really has no valid derivation before SR - the one used by Bradley requires a corpuscular theory of light where speed of source affects speed of light, which is c only relative to its emission source. Doppler has a pre-SR derivation, but the predicted amount for a high speed jet would be way too small. Beaming is considered relativistic because it is this joint effect of a pure SR phenomenon and SR augmented Doppler.
Thank you for the insightfull answer. I am going to discuss the physics of the image with my modern physics class next week and want to demonstrate this. I am going to first discuss it in a classical picture. (That is something I always do to explain the phenomenology first not to intimidate them with SR directly which they have to replace their "common sense" with pure math.)
What you pointed out as the Bradley's explanation is just EXACTLY what I mean by Galilean addition of velocities by the way. I didn't know the name and history, thank you for that and also thank you for pointing out the Doppler shift has a secondary (or indirect I can say) effect on the intensity via the relationship of frequency with the energy. That was something I missed also.
I am not totally convinced though that all of these are "pure" SR effects. What I would say pure relativistic is stuff like time dilation, length contraction, redefinition of momentum, energy, etc... (One interesting aspect is that the relationship of frequency with energy is not SR but "pure" QM which is also non-classical anyway)
Thanks again!
Dogan