Austin0
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Austin0 said:Regarding the lightning strike hitting the rear of the train and tracks;
The source would be the lightning strike. The origens would be the rear of the train and the colocated point on the tracks at the event.
((1)) SO tell me what is the velocity of the source or the origen as measured or assumed in either frame?
Self evidently both frames would measure the origen [coordinate point ] in the other frame as having a velocity relative to their frame but that is not what I was talking about.
((2))Would you argue that the source and origen were not considered at rest within both frames?
Hi Al68Al68 said:(1)The velocity of the source of any light is zero in whichever frame observes identical frequencies in each direction. And very much like The Highlander, "there can be only one".
(2)Absolutely. Both frames logically cannot detect identical frequencies in each direction. Again, "there can be only one".
(In this example, there may actually be multiple sources of light, since light may be emitted from parts of the train and parts of the track. But the above is still true for each light ray.)
Light always has a source, and the velocity of the source is frame dependent. Therefore the frequency of light from any source is frame dependent. That's why the motion of a source of light can be determined from measuring the frequency of the light.
I want to thank you for your clear and specific responce to my points above.
It was very helpful in attaining the realization that I was wrong.
In the confusion of source vs origen and the midstream change from my original concept of spontaneous cosmic occurance to a specific attached source I failed to give the new parameters enough thought.
Having done so I see that I missed the most obvious. Thinking of the source as instantaneous and so without motion in x I completely forgot that from the perspective of the frames it didnt just appear there but the orthogonal frame itself was moving prior to the emission. So in fact both frames would assume an anisotropic wave form.
SO the event [observation] was at rest in both frames but the source within the context of physical source was not.
You were perfectly correct in your conclusion in this case although regarding the two frames in question it was.."There can be only none"
But your logic, which is the logic of the real world ,where conclusions can drawn based on empirical measurements is not always applicable.
Austin0 said:------------------Consider the original spheres "paradox" scenario.
All frames must measure a constant c
All frames must calculate that they remain in the center of the sphere.
---------------Wouldn't the field have to be measured as either isotropic in all frames or anisotropic in all frames??
Otherwise it would not be consistent with their evaluation of being at the center.
If you apply the same real world logic to this case regarding the geometric center of an expanding sphere
It would be incontrovertably true that ;..."There can be only one"
Which I would agree with, but it is not consistent with the view within the frames . Or the assumptions we make looking at all frames from the outside perspective of Minkowski diagrams etc. etc.
In this case if we did assume a cosmic source: from the perspective of any given frame wouldn't they assume they were at rest and therefore the source which just appeared from nowhere would be considered at rest with the expectation of isotropic wave form in all frames??
This thread has undergone a lot of unneccessary argument because of a problem with my original condition of an unattached cosmic light source. With objections based on the real world logic that there can be no such thing.
Yet in Einstein's 1918 gravity based resolution of the twins paradox as reported in your link, there is massive use of dissappearing gravitational fields and magical undefined external forces negating these fields when required .
...But you have no problem accepting these conditions but reject my light source which is actually much more conceivable as a real world possibility.
It appears to me , to paraphrase an old arabic saying:
"You swallowed a camel whole but choked on a gnat"
In any case I have renovated my original conditions:
I now realize that orthogonal motion doesn't change anything and makes computation more complex so I am assuming a frame moving along x such that both frames have a relative velocity of.5c wrt the source frame and .8c wrt each other.
I am in the process of including both Doppler and aberration on top of irradiance falloff.
Is there anything else you can think of?
I can see now that I should do not only the numerical calculations but also Minkowski diagrams for those who don't like verbal descriptions and logic.
SO thanks again for your help and input, But I will make a prediction; If you reach a point of understanding the actual problem I am presenting you will then realize that all this extra complexity is irrelevant as it is all reciprocal and relative. ...IMHO
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