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I suppose I was. But I didn't mean to argue, I just wanted to find out what the currently accepted figure was for the size of the universe and be able to give a "reasonable" explanation. Maybe I was being too assumptive.marcus said:It seemed to me earlier that you were arguing for an upperbound on the size (it can't be any larger than such and so) by starting with an idea of the size at the start of expansion and by assuming some kind of bound on the SPEED of expansion.
I'm a big fan of Einstein. I've read up on the original GR translation plus other material. I like to think I stick closer to Einstein than other people do. But they don't always agree that I do.Mainstream cosmology, whatever's based on classic einstein GR, does not HAVE any limit on expansion speed. It can be any finite speed and to talk about the size (of the whole thing) at the start of expansion you have to go outside the bounds of classic 1915 einstein.
Agreed wholeheartedly. But have you ever heard of the Weinberg interpretation? I'd say it's not necessarily the whole theory that breaks down, but some aspect of it, or some interpretation. String Theory has morphed to a huge degree, why can't GR move a little and still stay as GR?as far as we know, singularities do not exist in nature, they only exist where theories break down, so its not meaningful to talk about the starting size in classic GR.
IMHO there are no infinities and no singularities in nature. My goal is to make science more popular. I mean that marcus.they only do that in popularization books, where they talk about the tiny size of what eventually became the observable universe, they never talk about the initial size of the whole thing because the size of a singularity is not well-defined. that's all pop sci anyway.
I definitely don't buy bounce. That's no explanation at all. Going beyond the bounds of "classic 1915 theory" is what Einstein was trying to do, and I try to stick with Einstein, so I suppose that's where I'm going.there are quantized models where you don't have a singularity and then you can talk about the size at the moment of BOUNCE which replaces the singularity, so you can talk about the initial size at the start of expansion but to do it you have to go outside the bounds of the classic 1915 theory, and its hard.
See your earlier point, I guess I was arguing that the ½c² for 13.7 billion years gave an upper bound.So I don't think you or anyone can get a grip on the size of the universe that way----mainly because there is no known bound on the speed of expansion.
I need to give it some thought.I think the only way to get a handle on it is by measuring Omega, essentially measuring the large scale curvature. But if you want, boil your argument down to a brief message that says roughly how it goes and send it PM and I will look at it. I may not be able to comment helpfully, but I'm curious, so you are welcome to do it if you want.
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