- #36
ConformalGrpOp
- 50
- 0
Chronos said:Conformal, if you are suggesting variable c casts doubt on all current cosmological models, you are in the good company of notable crackpots - like Thomas Van Flandern. That is not newsworthy. If you presume c is invariant, like the vast majority of mainstream scientists, you get something that resembles the LCDM model. If you know of any generally accepted observational evidence that c is not invariant, please cite your sources instead of rambling on with this nonsense.
Chronos, your post made me chuckle. If by c you refer to the velocity of light in an unobstructed field free space, Maxwell's equations clearly establish the invariance of c and define its velocity. (Ok, so I had to google Thomas Van Flandern. It does seem he was able to make a living being interested in things which would not hold my attention)
What Maxwell's equations do permit, however, is that EM radiation itself may propagate in a metric that is not Minkowskian. To all observers, the velocity of the propagated EM waves will remain invariant, but the wavelengths will not. This means that we cannot, a priori, assume that light propagates within a Minkowskian metric.
What is generally known is that for all observers, the metric of spacetime is locally Minkowskian.
If one looks at the assumptions incorporated into just about every scientifically credible model, if the Michelson-Morley experiment was hypothetically scaled up to say, 120 AU, it would still give a null result. That is, there would be no fringe shift due to wave interference of the recombined beams. (Even that "crack pot" colleague of Peebles, Prof. Hogg acknowledges that we really have never investigated what happens to light beyond the point where the Hubble relation is observable or words to that effect).
But, if, in fact, the light signals traveling across cosmologically relevant distances propagate in a metric that is not Minkowskian, say, for argument's sake, one with a metric that is equivalent (but not necessarily so) and isomorphic to Hubble's relation, the observer is going to interpret the received signals as a red shift. Such a metric would, not be Poincare invariant, but it would be conformal, in the sense that angles are preserved within the metric. If this were the case, then, taking the hypothetical example of the scaled up M-M experiment, the result would not be null and a wave shift would be observed by the interferometer.
Can we preform an analog of such an experiment? Of course we can. It can be done with just one space craft, but I would prefer it to be done with two. So, why don't we perform the experiment and find out about the behavior of light at such distances? Its one thing for Robertson, Eddington, et als. to say, well, we don't have a way to test this, and so, we have to go with what we know, and our lab results suggest that there isn't any observable ether and beyond that, they show that at least at small scales, light doesn't change its behavior as it propagates, ergo, we are left with the Hubble relation, and an expanding universe. But, such a position, in this day in age, is untenable when we clearly have the means to conduct the experiment to resolve the question.
Of course, if you know of some such experiment whereby the data confirms that light propagates across such distances in a metric that is Minkowskian (though it is presumed to be traveling across a universe governed by a metric which is expanding), I would be very grateful if you could direct me to those results, so I could move on to other topics of interest that have absolutely nothing to do with the structure and conformal geometry of the universe. But, I can'd find anything in the literature on the subject at all.
Last edited: