ghwellsjr
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You're welcome.Sugdub said:Thanks for your explanations.
DaleSpam already gave you the complete answer in post #28. Instead of concerning yourself with the black clock which happens to be at rest in a particular IRF, you want to use the Coordinate Time, represented by "t" in his equation. (They may be the same but you still don't want to restrict yourself to any particular clock at rest in an IRF.) In my diagrams, I use a simplified version of his equation which simply means that for the increment of the Coordinate Time grid lines, I determine (or specify) the speed of an object and calculate how much Time Dilation there is for that increment of time and that's how far apart I spread the dots.Sugdub said:...
So IMHO we now have a more realistic specification for what “causes” a different aging. It does not refer any longer to the relative motion between the red and blue clocks, but it spells out the relative motion between the (black) rest clock and each of the moving (red and blue) clocks. However it refers to a peculiar IRF and I guess it can't be extended to any IRF. May be there is a better way to solve this issue...
Once I build a complete scenario in the defining IRF, I can use the Lorentz Transformation process to get to any other IRF moving at any speed within the range of +/- c. That is one reason why you don't want to conceptualize Time Dilation as dependent on or in relation to any other actual clock. It's related to the Coordinate Time of an IRF which may or may not have any clock at rest in it and even if it did, that clock would be subject to the same determination of Time Dilation as any other clock. For example, in the second and fourth diagrams on post #18, there is no clock at rest in those IRF's, and yet the determination of Time Dilation for all the clocks still works.