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What experiments/theory led to the conclusion that light impinging on a moving object at any arbitrary speed( <c) would always arrive at c?
What I want to know is, in the early developmental stages of relativity(ie the work of Lorentz), when and how it was determined that in the case of light hitting a moving object the speeds would no longer be additive/subtractive.
(1) does not, in my opinion, require any postulate from relativity: once emitted the speed of the radiation will be determined solely by μ and ε.
The speed of light,(1) radiating from a moving object
What experiments/theory led to the conclusion that light impinging on a moving object at any arbitrary speed( <c) would always arrive at c? I have struggled with the wording of this question and am still not satisfied with it.
I certainly was not considering LET(aether! God forbid!).
I am somewhat confused by your statement that light emitted by a moving body does not travel at c: suppose an observer measures a body passing by at 0.5c and then this body emits a pulse of light- surely in both the frame of the observer and the frame of the emitter the speed of said light pulse will be c?
One final request, Halc, refresh my ageing brain as to the conflict between Maxwell and Newtonian mechanics.
you did say "light does not radiate from a moving object at c" in reply #9. Am I missing something?
Thanks Halc, you may rename it as you choose and move it