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- 30 Jan 2006
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- 427
Visage said:OK. lets clear this up.
For ANY observer, light will always travel at c. No ifs, no buts, no maybes.
Always.
Apparent paradoxes like 'What ahppens if you turn the lights on while travelling at c' are a result of applying galilean transformations to objects in relative motion - simply put, saying 'If object A travels away from me at 10 mph in a given direction, and object b travels away from object a at 20mph in the same direction, then object b is travelling away from me at 30mph'.
That doesnt work when the magnitude of velocities involved approach c. The basic reason for this is that velocity of an object in a given frame is defined as the rate of change of distance with respect to time of that object, in that frame.
The simple derivations of SR between inertial frames shows that, in frames moving with respect to an observer, time is observed to flow at a different rate than the frame in which the observer is situated.
It is the notion that conversion between frames is galilean that creates the apparent paradox. Once you use lorentzian transforms the figures resolve themselves and all is well.
(The apparent contradiction between high speed - lorentzian and low speed - galilean is reconciled by the fact that the lorentzian transform reduce to their gallilean counterparts for small values of v).
Didn't i try to explain something like this, but without the funny words? (any word with a Z just aint right!)
Might have been a bit simplified but i think it sort off had the gist.
What i'm now interested in is for massive objects momentum is m(u)*u
what values does the m and u represent?