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ramcg1
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Assume that c is the maximum velocity of electromagnetic radiation in an inertial frame of reference centred upon the source of the elecromagnetic radiation.
Assign an interface (boundary layer) between adjacent inertial frames of reference such that the velocity of the electromagnetic radiation changes to the maximum velocity of electromagnetic radiation in that inertial frame of reference, which is again c.
Then relativity becomes the rules of physical interaction between adjacent interfaces.
Time, mass and length become invarient.
Any velocity is possible so classical motion can also be applied to relative motion between source and observer.
You can observe a source traveling >> c if enough frame of reference interfaces exist between source and observer
If you think this an interesting concept follow the following link for more information and a play with the applets before replying.
http://members.iinet.net.au/~ramcg1/Others/Relativity/Fun%20With%20Relativity.html
http://members.iinet.net.au/~ramcg1/Others/Relativity/Relativity%20Applets.html
Assign an interface (boundary layer) between adjacent inertial frames of reference such that the velocity of the electromagnetic radiation changes to the maximum velocity of electromagnetic radiation in that inertial frame of reference, which is again c.
Then relativity becomes the rules of physical interaction between adjacent interfaces.
Time, mass and length become invarient.
Any velocity is possible so classical motion can also be applied to relative motion between source and observer.
You can observe a source traveling >> c if enough frame of reference interfaces exist between source and observer
If you think this an interesting concept follow the following link for more information and a play with the applets before replying.
http://members.iinet.net.au/~ramcg1/Others/Relativity/Fun%20With%20Relativity.html
http://members.iinet.net.au/~ramcg1/Others/Relativity/Relativity%20Applets.html
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