Arifz
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Does the universe has boundaries?, is it finite?
mathman said:Universe does not have a boundary. Finite or infinite is an open question.
Arifz said:But there is no such thing as infinity in physics !
Arifz said:But there is no such thing as infinity in physics !
phinds said:Oh? Can you prove that? Do you have an accredited references to back up such a categorical statement?
jackmell said:I believe there is a simple solution to this problem and it is based on behavior all through the Universe so I do not believe it is an inappropriate stretch to apply it to the entire Universe: we observe phenomena in the Universe having critical points in their dynamics. Breaching such a point often causes the dynamics of the phenomenon to change qualitatively and by doing so, the rules change. For example asking what does swimming mean beyond the critical point of freezing? What happens to a hydrogen atom beyond the critical point of fussion? In a small section of the ground it looks flat, even my whole yard. But it's not always flat, beyond the horizon the rules change and asking whether the Earth is infinitely flat or we just fall off is simply not following the new rules of a spherical Earth in a gravity field.
Therefore, in regards to a "size" of the universe, I do not think it is unreasonable to suggest at some large "size", a critical point is reached, the rules change, the concept "volume" loses meaning, and asking for a "size" of the Universe beyond that point is simply not following the new rules.
Arifz said:I think the big bang "Theory" can proves it
, however I still don't know what do we mean by "universe", is it the space that we know, or it also inclues beyond space "Vacume !".
What do you call the "No Space/No Time" before the big bang?!
Arifz said:But there is no such thing as infinity in physics !
I can't find a post claiming it does. OTOH, does anyone think it does have a boundary?andrewmh said:the big bang does not prove that there is no boundary to the universe.
But those are not infinities in the physical world, just in mathematical theory.and there can be an infinity. if you follow these two patterns you will notice that they will go on forever
1 2 3 4 5 6 7...
2 4 6 8 10 12...
divide them and you still get a number yet they are both infinitely large.
phinds said:I did not ask what you think, I asked what you can support by science.So you are making a definitive statement about something you can't even define. Now that's REALLY scientific.I don't call it anything since there is no evidence that there was such a thing and it is not part of the big bang theory
andrewmh said:to add to the idea of no space or time before the big bang, well you pretty much said it. there was no time. kind of a hard thought for human logic but time started at t=0 so yes, time does have a beginning.
Ken G said:The answer to that question is, "we have no scientific evidence that the universe is finite." That's it, that's all we can use science to say. /QUOTE]
I think we can go a little further than that. Many/most people would assume that if space has no boundaries then it must be infinite in volume. Science can be used to produce models, consistent with physics as far as is known, in which space can be finite yet unbounded. There may even be implications of such models which could be tested.
It's not terribly relevant, but that doesn't follow. Space could curve back on itself, have finite volume, and still have no boundaries. But the real issue here is, despite looking very hard (and quite possibly as hard as we can ever look), we have no evidence that it does have boundaries, nor do we have any evidence that it does not have boundaries, nor do we have any evidence that it curls back on itself, nor do we have any evidence that it does not curl back on itself. All we know is, what we see looks flat, and we have no idea how long it stays looking flat. That's it, that's the scientific evidence in its entirety.haruspex said:I think we can go a little further than that. Many/most people would assume that if space has no boundaries then it must be infinite in volume.
But making and testing models has nothing to do with answering the OP question. The models we make are intended as idealizations, and the standard idealization is that of a flat infinite universe. That model works quite well. Is that evidence that the universe really is flat and infinite? Of course not. If I am digging a foundation for my house, I'm certainly going to use a model that the surface of the Earth is flat and infinite (in that I will certainly not model any curvature of the Earth), and it will work great for digging my foundation, but I'm never going to conclude that any of this is evidence that the Earth really is flat and infinite.Science can be used to produce models, consistent with physics as far as is known, in which space can be finite yet unbounded. There may even be implications of such models which could be tested.
There is zero evidence that this is the case, and there is also zero evidence that this is not the case. And humanity should be prepared for the possibility that this situation will never change for us, as it seems quite likely at present. Even if efforts to detect a tiny spatial curvature do eventually succeed, it won't require that the universe maintains that same curvature everywhere, that will simply be an idealization of the model, like any other idealization of any other model. It will never be testable as fact, we pretty much already know this.shreyakmath said:The universe is finite but with no boundary. It is similar to a bubble or sphere
Yes, that's the point I was making.Ken G said:... that doesn't follow. Space could curve back on itself, have finite volume, and still have no boundaries.
I'm far from expert in this area, but my understanding is that General Relativity posits a "flat" spacetime, but a finite, curved space, with a compensating curvature in time.nor do we have any evidence that it curls back on itself,
I disagree. The question was "Does it have boundaries? Is it finite?" Establishing that 'finite without boundaries' cannot be ruled out is a partial answer.But making and testing models has nothing to do with answering the OP question.
phinds said:Oh? Can you prove that? Do you have an accredited references to back up such a categorical statement?
No, GR says that in comoving-frame coordinates (which is what is generally used in cosmology to talk about what the universe as a whole is doing), all the observed curvature due to gravity is in the time dimension (associated with cosmological redshifts), none is in the spatial dimension. We say the universe is "spatially flat" in this sense. The observations cannot rule out some small spatial curvature, but they can rule out the idea that the universe curves back on itself over the range that we can observe or in some way test our inferences about-- and of course we have no idea what it does beyond that range. Even if we do detect some small spatial curvature, it would not require that this curvature is maintained beyond what we can observe-- the cosmological principle applies to explanations of what we actually observe, it is not a philosophical claim about what we cannot observe.haruspex said:I'm far from expert in this area, but my understanding is that General Relativity posits a "flat" spacetime, but a finite, curved space, with a compensating curvature in time.
No, the Big Bang model includes neither finiteness nor spatial curvature at present. So the model is one of an infinite universe. However, the model need not make any claims that this is actually true, it just means we have no reason to model finiteness of the universe.I would also have thought that an infinite universe was inconsistent with the Big Bang model, and there is much evidence for that.
I said it could not be ruled out. I also said the alternative could not be ruled out. In fact there is no evidence at all either way. When there is no evidence in favor of a proposition, nor evidence against it, it doesn't leave you with a whole lot more to say, which is the point.I disagree. The question was "Does it have boundaries? Is it finite?" Establishing that 'finite without boundaries' cannot be ruled out is a partial answer.
Ken G said:Even if we do detect some small spatial curvature, it would not require that this curvature is maintained beyond what we can observe-- the cosmological principle applies to explanations of what we actually observe, it is not a philosophical claim about what we cannot observe.
No, the Big Bang model includes neither finiteness nor spatial curvature at present. So the model is one of an infinite universe.
When there is no evidence in favor of a proposition, nor evidence against it, it doesn't leave you with a whole lot more to say, which is the point.
haruspex said:I'm far from expert in this area, but my understanding is that General Relativity posits a "flat" spacetime, but a finite, curved space, with a compensating curvature in time.
Algren said:There is a logic behind the beginning of time. Any events which occurred before the big bang does not affect us or the universe today. There is no need to assign these useless and unknown events with a time. Thats why we have BIG BANG occurred at t=0;
Ken G said:Even if efforts to detect a tiny spatial curvature do eventually succeed, it won't require that the universe maintains that same curvature everywhere, that will simply be an idealization of the model, like any other idealization of any other model. It will never be testable as fact, we pretty much already know this.
Right, and what we find, when we do that, is zero evidence of any spatial curvature, which is consistent with inflation. If inflation is correct, this will always be true, no matter how good our observations get.twofish-quant said:But CMB power spectrums can and do constrain large scale anisotropy. We can directly measure what's in our bubble, we can infer things for some distance outward.
If we detect that, you can throw away inflation completely!Also, if we do detect small scale curvature, this is going to very strongly constrain the details of inflation and we can use that to infer a lot of stuff.
You don't see what I'm saying. LCDM is not a statement about what the universe is really like, it is a good model of the universe. That's a rather important distinction, and cuts right to the heart of what physics and astronomy does! What's more, LCDM is flat, and invokes the cosmological principle, and so it is a model of an infinite universe. Of course these are idealizations, physics deals exclusively in idealizations, it makes models. As I said, that does not mean it asserts the universe is infinite, it means it is an infinite model of the universe. Which is just precisely what it is. Newtonian physics was never an assertion that the universe is deterministic, it was always a deterministic model of the universe, which is quite different.This is incorrect. LCDM doesn't require finiteness, but it doesn't exclude it.
I have never been talking about "what the current model allows." The current model allows for unicorns, space aliens, and teleportation beams. But none of those are included in the current model, because there is no need for them, and no evidence in favor of them. Again this is a rather important distinction.Also whether the current model allows for a finite universe is an observational equation that changes from moment to moment.
Right-- and what got changed is we got a flat model! Which is what I have been talking about all along.Before the discovery of dark energy, the amount of dark matter in the universe was clearly insufficient to close the universe so there was a period of a few years in which the preferred model was infinite and negatively curved.
Then we have dark energy and everything changed.
Ken G said:Right, and what we find, when we do that, is zero evidence of any spatial curvature, which is consistent with inflation. If inflation is correct, this will always be true, no matter how good our observations get.
If we detect that, you can throw away inflation completely!
What's more, LCDM is flat, and invokes the cosmological principle, and so it is a model of an infinite universe.
Ken G said:I'm talking about the evidence that exists today, and the models we build based on that evidence. And that evidence is used to build flat models of an infinite universe-- with no claim whatsoever that this is the truth of the matter, it is just our best model.
Right-- and what got changed is we got a flat model! Which is what I have been talking about all along.
Right, but that's exactly why the CDM model was uniformly rejected by just about everyone. That is in complete contrast with the models of today, with which we often hear the phrase "precision cosmology", and has been related to several Nobel prizes.twofish-quant said:One other thing to note is that before the discovery of "dark energy" in 1998, the best available model (CDM) resulted in a negative curvature model of the universe. It's only after you add dark energy that you get something like a flat universe.
No, that's not true. I was an astronomer in 1995 also, and few thought the universe was not flat, they thought the model was wrong. That's also why there were no Nobel prizes awarded for the CDM model. Indeed, it was considered a huge problem that the flatness parameter came out 0.3, which was way too close to 1 to not be 1 (a flatness less than 1 gets exponentially less flat with time, so to be 0.3 now, it would have had to have been extremely close to 1 in the past, but still strangely different from 1). Even in 1995, inflation was commonly taught, and it was widely expected that the flatness should be 1. The missing energy was just considered a paradox that no one knew how to solve, but made people worried that we were missing something really crucial. Today that is not the sentiment, hence all the Nobel prizes, though of course there are plenty of people still not completely happy with dark energy, and that's why we have some people claiming that you need multiverses to explain it. I'm not banking on that approach myself, however, I just think we are still missing some key physics, but the models of the universe will still be flat (except for local fluctuations with no global significance), and we will just never get to know anything beyond that for the simple reason that we cannot look.Which is why I dispute your statement that a flat universe is *required* for inflation. As of 1995, it was believed that we didn't live in a flat universe, because without dark energy flatness is excluded to pretty high certainty, but that didn't kill off inflation.
I'm not sure where you get that, but it is incorrect. See the WMAP website at http://map.gsfc.nasa.gov/universe/uni_shape.html , where we find quotes like:And I'm saying this is false. If you look at the parameterizations for WMAP, you'll find that the model that they use to calculate observational constraints is not flat.
It comes from modern astronomy textbooks, and websites like the WMAP website I quoted above. So, where are you getting your misinformation, given that you are "keen" to stamp it out?twofish-quant said:Also, I'm interested in where you are getting your information since it's wrong.
Ken G said:It comes from modern astronomy textbooks, and websites like the WMAP website I quoted above.
So, where are you getting your misinformation, given that you are "keen" to stamp it out?
Either one. Just not textbooks expressly designed to investigate speculative areas of astronomy. Such books always appear at the fringes of any science, they are certainly not quackery, but they are usually forgetten in a few decades-- such is the nature of controversial speculation. No doubt there are graduate textbooks on MOND, on loop quantum gravity, and on microscopic black holes.twofish-quant said:Which textbooks? Graduate or undergraduate?
Good luck with that, I'm sure they'll be thrilled to have your expertise weighing in.The WMAP website oversimplifies things. I'll e-mail the maintainers of the site to get it changed.
They told you that eternal inflation is a mainstream consensus idea? I doubt that strongly.1) from the graduate courses that I took in cosmology when I got my Ph.D. in astrophysics
I don't see any quotes from them in your argument. What are you claiming they said, and why don't you think it is making it to the WMAP website?2) from talking with cosmologists and supernova people, include one of the lead co-authors of the WMAP paper, one person that was a co-author on the supernova Ia investigation papers, and one person that has a Nobel prize in physics.
Ken G said:Either one. Just not textbooks expressly designed to investigate speculative areas of astronomy.
No doubt there are graduate textbooks on MOND, on loop quantum gravity and on microscopic black holes.
Good luck with that, I'm sure they'll be thrilled to have your expertise weighing in.
They told you that eternal inflation is a mainstream consensus idea? I doubt that strongly.
I don't see any quotes from them in your argument.
What are you claiming they said, and why don't you think it is making it to the WMAP website?
Obviously, it is very important to detail the issue correctly. The way you have paraphrased my arguments makes me doubt your version would have much resemblance. For one thing, you insist that I'm claiming that inflation implies the universe is flat. Of course it does no such thing, inflation is a model, it does not constrain the universe, rather the universe, in concert with the goals and demonstrable benefits of science, constrains the model. What I'm actually saying is threefold:twofish-quant said:Give me a few days. If I can get you a personal email from one of the three people confirming my points, will you concede the argument? Also, I want to define the question, because I don't want to get into a situation where I bug someone who is busy, get an e-mail, and then you argue that the e-mail doesn't refute your point.
Ken G said:1) For inflation to continue to be regarded as a good model of what really happened in our universe, with no need for anthropic thinking, then curvature must never be detected, and conversely, if curvature is detected, then inflationary models will be up to their ears in anthropic justifications, so much so that much of their original purpose (to escape anthropic thinking) will be lost.
2) The current best model of the universe is a flat, infinite model that obeys the cosmological principle.
Occam's razor contributes significantly to making this our best model.
3) The question "is the universe infinite" could never be answered "yes" by any scientific means imaginable.
We must stop pretending that science can determine truths even after we have discovered that the observations cannot.
Ken G said:... What I'm actually saying is threefold:
1) For inflation to continue to be regarded as a good model of what really happened in our universe, with no need for anthropic thinking, then curvature must never be detected, and conversely, if curvature is detected, then inflationary models will be up to their ears in anthropic justifications, so much so that much of their original purpose (to escape anthropic thinking) will be lost.
2) The current best model of the universe is a flat, infinite model that obeys the cosmological principle. Occam's razor contributes significantly to making this our best model. Its success is by no means a claim that the universe is actually flat or infinite, for indeed no model can ever make such a claim, given that we cannot see far enough to check it, and never will.
3) The question "is the universe infinite" could never be answered "yes" by any scientific means imaginable. It could only be answered "no", and we already know it cannot be so answered, because we already know we cannot see the limit of the universe. Even if we detect some tiny positive curvature, it would only mean that our best model was now a closed finite model, and again by Occam's razor-- not by any testable claim on the actual geometry of the universe that we cannot see. The best model is never a claim on things that observations are moot about, such things are adopted in the model purely based on Occam's razor. We must stop pretending that science can determine truths even after we have discovered that the observations cannot.
These are the three points I have repeated over and over, and I have never said, or thought, anything else of importance to this discussion. Anyone whose opinion you'd like to solicit on those three points would be more than welcome, indeed quite informative. But the way you have characterized my points is completely inaccurate, and framing the issue as you put it above would have no value whatsoever.
Here's the problem. You have an inflation model, and it has some parameter in it, perhaps the shape of some scalar potential function. You then look at the curvature today, run your GR backward until inflation ends, and try to match up what you get. Certainly you can take any current curvature, no matter how close to flat it is, and you'll get an answer to this exercise. The issue is what is the "size of the target" you are trying to match. If current curvature is not detectable at the, say, .0001 level, then you have a vast range of possible curvatures at the end of inflation, you just map from .0001, to 0, all the way back, and what you get is a hugely wide range of possible curvatures at the end of inflation. Now you have some hope that a plausible inflation model, that is consistent with other established physics, will "hit the target."marcus said:That said, you might want to relax your points #1 and #2. I've always understood inflation as having leveled things out enough to be consistent with what we see today. Inflation is consistent with some slight residual curvature.
But I think it would. Look at it this way. Take the model you have in mind, and partition its possible parameters into two sets-- the set that leads to unobservable curvature, and the set that leads to small but observable curvature. Of course throw out the set that we've already falsified because it leads to huge curvature. Really do this, it should be easy enough with whatever model you have in mind. Now ask a simple question-- what is the relative measure of those two sets? Is it not true that the unobservable curvature parameter set has vastly larger measure than the observable curvature set? So how is it not fine tuned if we detect curvature tomorrow? How do you answer the question: why that parameter set and not the other parameter set, if the other one was orders of magnitude larger?The treatment of inflation in Loop cosmology does not require fine-tuning and makes an adequate inflation era highly probable. It is consistent with some curvature and if curvature were detected would not bring on the "anthropery" bogeyman.
It is certainly true that Occam's razor is never clear-cut, but if you just look purely at the model, with no extraneous baggage that says the model is supposed to be the actual reality, then it is clear enough that a model with a non-arbitrary value for the flatness (i.e., flat) is simpler than one with an arbitrarily chosen value of curvature (how do you even give a value to it?). Also, it is much easier to use for doing calculations, which is the key issue I would say.Point #2 is a rather one-sided invocation of Occam, I think. Some people would put Occam on the side of a spatially finite universe, other things equal.
Simplicity of imagining is a different flavor of Occam's razor, it's hard to say if a "best model" is the one that has the fewest arbitrarily chosen parameters (like flat versus some essentially randomly chosen curvature that is not refuted by observation), or the one that is "easiest to picture." My point is that once you are on board with point #3, you are relieved of any philosophical issues with an infinite universe, because you are not claiming the universe is infinite-- you are just fitting what we see to a flat model, like fitting a tangent plane to a manifold where you cannot measure any deviation between the two. The tangent plane is mathematically non-arbitrary, but it is hard to picture because it goes off to infinity in all directions. If we saw that as a bad thing, we could certainly do all of calculus to any precision with circles and spheres of small enough curvature, but we don't, we have lines and planes, because they are mathematically simpler, though harder to picture.I find the finite volume case easier to imagine, simpler.
Neither. It comes from me, but it stems from a logical argument. I summarized that argument again just above. So if you want to critique it, you do better finding an actual flaw in the logic.twofish-quant said:Also just to clarify. Is assertion 1) something you got from someone else or something you made up.
You don't seem to even understand what I'm saying with 1) or 2), so I'm suspicious of your judgements of these points. For example, you insist on claiming that I have said that cosmologists assume the universe is flat. That is so completely different from anything I've said, or even thought, that I have no idea where you are even getting that from, but you can't be reading very carefully.Also one other point is that neither 1) or 2) is "mainstream cosmology."
Ken G said:Now imagine some observation was just done that detects spatial curvature, say it's in the range .0001 to .0002. Play the same game, map that backward to the end of inflation, and now you have only a factor of 2 in parameter space
twofish-quant is saying that he has the hope that a plausible inflation scenario that is based on some atomic scale will rather magically hit this target.
But look at the cost we've had to pay-- first of all, we seem to have gotten really lucky to have hit the target, but that's what we are using to justify faith in our model.
But I think it would. Look at it this way. Take the model you have in mind, and partition its possible parameters into two sets-- the set that leads to unobservable curvature, and the set that leads to small but observable curvature. Of course throw out the set that we've already falsified because it leads to huge curvature. Really do this, it should be easy enough with whatever model you have in mind. Now ask a simple question-- what is the relative measure of those two sets? Is it not true that the unobservable curvature parameter set has vastly larger measure than the observable curvature set? So how is it not fine tuned if we detect curvature tomorrow?
My point is that once you are on board with point #3, you are relieved of any philosophical issues with an infinite universe, because you are not claiming the universe is infinite-- you are just fitting what we see to a flat model, like fitting a tangent plane to a manifold where you cannot measure any deviation between the two.
Ken G said:Neither. It comes from me, but it stems from a logical argument. I summarized that argument again just above. So if you want to critique it, you do better finding an actual flaw in the logic.
For example, you insist on claiming that I have said that cosmologists assume the universe is flat.
That is so completely different from anything I've said, or even thought, that I have no idea where you are even getting that from, but you can't be reading very carefully.
But that's just it, the dark energy has already taken over. So we are pretty much at the curvature "peak" right now. That's the problem with a peak curvature that just happens to be what we can barely measure, why on Earth would life come along at just the time when it can barely measure the curvature? That's the "fine tuning problem" that you would be staring at if curvature is detected, and that's what would steal most of the wind from inflation's sails.twofish-quant said:If the curvature is positive then at some point in the life of the universe it will take all values from 1e-16 to infinity. We happen to catch it at 0.001, but wait a few billion years and it will be 0.002. Then 0.3, then 0.5, then 2, then 1000, then at some point dark energy takes over and it goes down again.
No, not with dark energy.If there is *any* curvature, no matter how small, then the universe at some point in it's life will take all values between that small curvature and infinity.
Exactly, and if curvature is detected, then we will have the fine tuning problem that dark energy is taking over at exactly the point when the curvature is barely detectable by intelligent life. That's just the fine tuning that Weinberg argued is evidence for a multiverse, in relation to the amount of dark energy-- you would be in the exact same boat, but now in regard to curvature instead. You would need an anthropic argument to escape the appearance of fine tuning, and it would have to magically be consistent with the same anthropic argument that is supposed to be what let's dark energy be 10100 time weaker than it "ought to" be. If we reject this is an escape hatch for the inflation theory, then we have no explanation for why the universe has a sense of humor that it will just let us glimpse the curvature before dark energy washes it away.Once the universe starts expanding from *any* small curvature, it will take *all* values between that small number and some limit at which when dark energy takes over.
I agree completely, I don't think resorting to multiple universes is a fair way to make a theory seem palatable or plausible. That's exactly why I claim any inflation proponent should be hoping we never detect curvature, and indeed, should probably even be confident we never will. There's just no reason for the parameters of a working inflationary model to be so well perched at that arbitrary tipping point that would suddenly seem very special indeed.Instead of taking multiple universes, let's just take one.
I don't agree, I think that for the vast majority of ways to set up that universe, the curvature will remain way too small to detect, because the one-two punch of inflation and dark energy will insure that. That holds whether you imagine a cosmological constant or a quintessence-type continuous inflation. You have to really fine tune the combination of inflation and dark energy to both have a universe that inflates enough to be anything like what we see (and, dare I say it, to support life), but still leave a window for detectable curvature for a few billion years out of that vastly aging universe-- exactly when life comes along. That's the problem I've been talking about, this bizarre "glimpse of curvature" phenomenon, which has no "natural" explanation at all, and would sorely tax the whole spirit of using inflation to recover a "natural" feel.You have inflation and it reduces the curvature to some random small number. Now let's evolve the universe. It turns out that for most of the life of the universe, you will have a detectable curvature.
No, a thousand times no. Not only did I never say that, I bent over backward many times over to stress that is exactly not what I am saying.twofish-quant said:You are saying that the best model used by cosmologists assumes a flat universe, and I'm saying that's not the case.
Yes, communication is the hardest thing, so let me repeat again what I have been saying. Cosmologists make models, and they make the models only as complicated as necessary to fit the data. The current models that do that are flat, and use the cosmological principle, so they are infinite models, like a derivative is an infinite model of a function even if the function becomes uncertain outside of some compact region. As I've repeated many times now, no such flat and infinite model can say anything at all about the infiniteness of the universe, indeed I stressed several times (there are at least three threads we are debating, so it's hard to keep track of where!) that the question "is the universe infinite" is fundamentally a question that science could never answer in the positive. But science can certainly, and does, make infinite models, if it has no evidence for making them finite. No such model is a claim on what we cannot observe, nor would there ever be any scientific validity in making any claims on such a region.Communication is difficult, and if you aren't making that assertion, then what assertion you are making.
Never said anything like that, nope. I said LCDM is a flat model, which is a totally different claim. It just says the simplest model that fits what we see is a flat infinite universe model, that is not at all "assuming the universe is flat." We don't make assumptions about the universe, we embed assumptions into models, in order to make good models, not in order to use models to make claims on the universe. The logic goes the other way-- observations of the universe inform our models, our models do not inform the universe that is outside the observations we used to make the model.You have said that LCDM assumes a flat universe, and that's false.
Ken G said:No, a thousand times no. Not only did I never say that, I bent over backward many times over to stress that is exactly not what I am saying. Yes, communication is the hardest thing, so let me repeat again what I have been saying. Cosmologists make models, and they make the models only as complicated as necessary to fit the data. The current models that do that are flat, and use the cosmological principle, so they are infinite models, like a derivative is an infinite model of a function even if the function becomes uncertain outside of some compact region. As I've repeated many times now, no such flat and infinite model can say anything at all about the infiniteness of the universe, indeed I stressed several times (there are at least three threads we are debating, so it's hard to keep track of where!) that the question "is the universe infinite" is fundamentally a question that science could never answer in the positive. But science can certainly, and does, make infinite models, if it has no evidence for making them finite. No such model is a claim on what we cannot observe, nor would there ever be any scientific validity in making any claims on such a region.
Never said anything like that, nope. I said LCDM is a flat model, which is a totally different claim. It just says the simplest model that fits what we see is a flat infinite universe model, that is not at all "assuming the universe is flat." We don't make assumptions about the universe, we embed assumptions into models, in order to make good models, not in order to use models to make claims on the universe. The logic goes the other way-- observations of the universe inform our models, our models do not inform the universe that is outside the observations we used to make the model.
andKen G said:See the WMAP website at http://map.gsfc.nasa.gov/universe/uni_shape.html , where we find quotes like: [. . .]
twofish-quant said:The WMAP website oversimplifies things. I'll e-mail the maintainers of the site to get it changed.
1) from the graduate courses that I took in cosmology when I got my Ph.D. in astrophysics
2) from talking with cosmologists and supernova people, include one of the lead co-authors of the WMAP paper, one person that was a co-author on the supernova Ia investigation papers, and one person that has a Nobel prize in physics.
Right, most likely they believe almost as many different things as their are cosmologists, and indeed they are welcome to hold any personal beliefs they wish, but believing it wouldn't make it science.marcus said:Things are getting clearer. You are not saying that mainstream cosmologists believe the universe is spatially flat, or infinite.
There are always many multiple models in use, for a host of reasons, largely around the "buckshot" principle of doing science. But there is also a clear consensus on what is currently regarded as the best model, the model that is often heard in a sentence with "precision cosmology", and it is a model with no reason to include any curvature, so it doesn't. There's always the interplay between consensus and contrariness in science, and nowhere did I ever say that there is only one cosmological model that ever gets looked at-- I said there is one widely regarded best model, and Nobel prizes have been awarded.You are claiming that the predominant model in use, the LCDM, comes in only one version and that version is spatially infinite with zero curvature.
Actually I have seen curved models invoked many times, my point is that none of those models ever gave us the value, the bang for the buck, that the flat model does. Indeed those models can now be seen to be largely a source of unnecessary complication. Almost all cosmology textbooks, for example, start out with the three possible geometries, and go to great lengths describing their differences, only to throw it all away when they come to describing the currently favored model! It's so much wasted overhead. I've no doubt that electromagnetism textbooks after Maxwell went to great lengths describing all the different ways light might operate in different frames if the speed of light was relative to an aether frame, but at some point, they realized that all that overhead was missing a key simplification that drastically simplified the mathematics of doing calculations-- Einstein's postulate. I'm saying flat models in cosmology are another example of just such a drastically beneficial mathematical simplification, to the point that it is becoming more and more apparent that we should embrace that simplification instead of fighting it every step of the way.If you have never seen a cosmologist use a version of LCDM which has overall slightly positive curvature, then this claim is certainly understandable!
Certainly. And many experiments in the era of Michelson-Morely were aimed at placing an upper bound on how much the speed of light could deviate from c in various frames. But at some point, the mathematical simplicity of a basic unifying postulate overwhelms all that careful overhead, and you just embrace what has been jumping up and down waving its arms at you all the while.However my experience is different from yours. I have seen top level cosmologists use different versions of LCDM, and for example, calculate a lower bound for the radius of curvature for the spatially finite positive curved version of LCDM.
Just as in pre-Einstein days, they took the confidence interval on c very seriously too.In other words, in my experience cosmologists do not jump to premature conclusions, do not gloss over different cases, and instead take the Omega confidence interval very seriously.
And what is the confidence interval on c today? It's not infinitely narrow, right? So does that require we have a "very nearly relativistic" version of physics that we also have to bear in mind, and put in every textbook on relativity theory? Models are intended to be simplifications, there's no "conclusions" that are drawn when we adopt one, certainly not that we are announcing that we are convinced the model should suddenly be regarded as "correct," ignoring the fate of all "correct models" for time immemorial. All it means, when we adopt a particular idealization in some model, is that we are tired of doing extraneous and unnecessary work tracking what is much simpler to just remove from the model. We have simply reached the point of diminishing returns for tracking the complexity, relative to just adopting the simpler postulate. I'm saying cosmology is at that point, but it might take it a little while to make the transition.Since the confidence interval has a substantial range above 1 that necessarily requires a spatial finite (but "nearly" flat) version of LCDM.
A flat Universe from high-resolution maps of the cosmic microwave background radiation
P. de Bernardis et al
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The blackbody radiation left over from the Big Bang has been transformed by the expansion of the Universe into the nearly isotropic 2.73 K cosmic microwave background. Tiny inhomogeneities in the early Universe left their imprint on the microwave background in the form of small anisotropies in its temperature. These anisotropies contain information about basic cosmological parameters, particularly the total energy density and curvature of the Universe. Here we report the first images of resolved structure in the microwave background anisotropies over a significant part of the sky. Maps at four frequencies clearly distinguish the microwave background from foreground emission. We compute the angular power spectrum of the microwave background, and find a peak at Legendre multipole lpeak = (197 plusminus 6), with an amplitude DeltaT200 = (69 plusminus 8) microK. This is consistent with that expected for cold dark matter models in a flat (euclidean) Universe, as favoured by standard inflationary models.
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http://www.nature.com/nature/journal/v404/n6781/full/404955a0.html