GRDixon
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In theory the set of Inertial Reference Frames could consist of an infinite set of rectangular grids and distributed clocks, overlaid and sliding through one another without interference. Let us say we are initially at rest at the Origin of IRF K. Relative to K, the grid of moving frame K’ will be length contracted, etc.
If we switch our rest frame to K’, then it will be the grid of K that is length contracted, etc. At great enough distances from the Origin of K, this would seem to require parts of the K’ grid to move outward, away from the Origins, at speeds faster than c. (And similarly, from the Origin of K’ it would seem distant parts of the K grid must move closer to the Origins at speeds greater than c.)
How can this violation of the rule, that c is the maximum speed of material objects, be resolved?
If we switch our rest frame to K’, then it will be the grid of K that is length contracted, etc. At great enough distances from the Origin of K, this would seem to require parts of the K’ grid to move outward, away from the Origins, at speeds faster than c. (And similarly, from the Origin of K’ it would seem distant parts of the K grid must move closer to the Origins at speeds greater than c.)
How can this violation of the rule, that c is the maximum speed of material objects, be resolved?