Originally posted by Imagine
Relative to Hubble relation, V=R*H:
- Do we have the same problem?
- How is it resolved?-
- Is this resolution could apply to this case?
- Is centripetal acceleration, w2r, could be related to Hubble relation?
IMHO, I would said that "the gravitational field is 1/time", and the particular empty space-time property, second per meter, equal to "1/c".
Imagine, a reply from only one person, myself, may be insufficient. Interestingly enough we do NOT have a problem with superluminal recession speeds-------they simply say that the physical distance between some locations is increasing at a rate > c. Nothing is traveling at such speeds, no transmission of information, no motion as we normally understand it. There is no A that is passing thru the neighborhood of B and observed by B to being going faster than light.
A simple calculation shows that volume-wise the greater part of the observable universe is receding > c. Light now reaching us from objects in some 90% of the observable volume was emitted when those objects were receding at superluminal speed and was initially swept backwards. It is an amazing fact but part of the standard picture cosmologists have agreed on---in this sense it is not controversial, just part of the consensus model.
NON-cosmologists, however, are apt to find it controversial and to want to argue about it.
a short paper by Tamara Davis and Charles Lineweaver discusses this
http://arxiv.org/astro-ph/0011070
-------------------
Now about what Goedel said in 1949, and what Burghardt said in 1996, I have not understood yet. It is possible that Jcsd has understood what they are talking about.
I don't see WHY Burghardt should have declared there was a cutoff. He is not a person of any great stature or reputation as far as I know and maybe he simply made a mistake which no one bothered to correct. I know of no reason to give particular weight to what he says. The case of Goedel is different, but I have not read Goedel-----Goedel may very well have thought that he did not have to apply a cutoff.
I don't yet understand how anyone can model the rotation of the gravitational field, that is to say the metric. Expansion is easy: you just have the metric get larger.
I think Jcsd may understand this and he may be willing to put it in terms you can understand. But I cant.
However I can respond to what you said about the Hubble relation. No cutoff needed there! Just look at the sky and reflect that most of what can in principle be seen there (with the proper instruments) is at present receding at over the speed of light and
was already doing so when it emitted the light now reaching us!