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In article ,
Dag Oestvang wrote: wrote: I will try to clarify: Unless V to a good approximation appears from a cleverly arranged field of 4-velocities in flat space-time (this is exact in the Milne model), there is no natural way to interpret V in this way if the effects on V of curved space-time on parallel transport is not negligible. That's true. But in the low-redshift limit, the effects on V of curved spacetime on parallel transport *are* negligible. Proof: Try it and see! Neglect spacetime curvature and parallel-transport V. In the low-redshift limit, you get the right answer. Therefore, neglecting spacetime curvature didn't do any harm. Spacetime curvature was negligible. In other words; insofar as the effects on V coming from the curvature of space-time can be neglected it is perfectly all right to interpret V as coming from a field of 4-velocities in flat space-time. But it is not if the size of V depends crucially on space-time curvature. I agree. But again, the last "if" clause is false in the limit I'm considering. Do you think that "the size of V depends crucially on space-time curvature" in an Omega = 0 FRW Universe? (I certainly hope not, since there is no curvature in this spacetime.) How about in an Omega = 10^(-50) FRW Universe? It seems that we mostly agree. This is my position: If the effects of curved space-time on V are negligible then interpretations of spectral shifts as Doppler effects in flat space-time are OK; otherwise not. Do you agree? Yes. But again, the "If" clause is false in the low-redshift limit of an FRW Universe. -Ted -- [E-mail me at , as opposed to .] |
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