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"Questionable" article in Scientific American? |
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| Jan6-10, 10:16 PM | #18 |
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"Questionable" article in Scientific American? |
| Jan6-10, 10:57 PM | #19 |
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[tex]f(t) = t[/tex]For a more realistic function, I'll have to give the differential equation [tex]\frac{df}{dt}= \sqrt{0.27 f^{-1} + 0.73 f^2}[/tex]The differential equation has a problem when t=0. In fact, it has a singularity. But that's okay. We can just let the differential equation define f for positive values of t, with boundary conditions so that f(t) approaches 0 in the limit as t approaches 0. When f is very small, df/dt is large, so it aligns very closely with [tex]f(t) = (1.5 t \sqrt{0.27})^{2/3}[/tex]in the neighbourhood of 0. We call this function "scale factor", and usually add a couple of constants to scale f and t as we choose, but the above functions will do. Now. Imagine an infinite 3D cartesian space with specks laid out in an infinite 3D grid pattern, one at every point with integer co-ordinates. This represents a static infinite flat space, filled with evenly spaced galaxies. To apply expansion, suppose that the specks are moving apart from each other, so that this is their position at a time t when f(t) = 1. Give each speck a name (x,y,z) corresponding to its co-ordinates at this time, and at all OTHER times, suppose that the speck is located at (x.f(t), y.f(t), x.f(t)). Voila. This is expansion. The speck at location (0,0,0) never moves, and all the others move away from it, with a velocity that is the product of their distance when the scale factor was equal to 1, sqrt(x2+y2+z2), and to the function f(t). Of course, you can also convert the co-ordinates to see where all the specks are relative to any other speck; and curiously, no matter which speck you pick as your origin, the expansion looks exactly the same. Each speck would see itself as the center of the expansion. Also, as you run time backwards towards 0, you always have a perfectly spaced rectangular grid, with distances of f(t) between the points. At t = 0, of course, there's a singularity. Every point is at zero; which introduces a strange kind of discontinuity. At every other time, the grid is infinite and expanding. That's the flat Big Bang model: flat meaning we can use nice simple cartesian co-ordinates like this. Cheers -- sylas PS. Sorry for being so fast. I've been monitoring the forum and happened to see your post. Yes, the Big Bang involves "superluminary" expansion, in the sense that the distance between widely separated specks (or galaxies) can be greater than the speed of light; in fact there's no limit on the speed of separation. Ignore this detail; it is not actually in conflict with relativity and why it isn't is a question for another time. Finding the path of a photon moving between specks in this simple model can be fun; pick your velocity c and just make sure the photon is always moving at this speed relative to any speck it is moving past. Don't worry about anything special in the way of relativistic conversions; they don't matter. The technique outlined in this postscript works. |
| Jan6-10, 11:38 PM | #20 |
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In any case, you seem to be going from a finite perspective to an infinite one; something that you said couldn't happen in the "Flat universe?" thread. While the math seems to work after the strange discontinuity, does the physics work? Looking backwards in time we are going from galaxies to quarks. Are quantum level phenomenon describable in the simple expanding grid you described given the uncertainty of position/momentum? |
| Jan7-10, 12:21 AM | #21 |
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Big Bang cosmology is basically a "classical" theory in physics, involving general relativity for space and time and gravity. You can then talk about particles in the universe with quantum mechanics (nucleosynthesis, for example). The theory involves the universe expanding (in precisely the sense given above; everything moving apart from everything else) and then over time the rate of expansion changes and the energy densities drop all according to classical physics up to the present day. Big Bang cosmology doesn't actually explain the "initial moment" or the singularity. It just says that the universe starts out from a state of extreme density that we can't describe very well, and it cools and expands from then to now.... and the rate of expansion if extrapolated backwards has this singularity. The great issue now is to have a physics which doesn't fall to pieces in this way. But there's not any need to go from finite to infinite. We really don't know if the universe is finite or infinite; but whichever it is, it has always been thus. Personally I have a profound philosophical inclination to finite... but that's not science. I know others have a philosophical inclination in the other way. We really won't have a good handle on that until we get some kind of unification of relativity and quantum physics. Cheers -- sylas |
| Jan7-10, 12:50 AM | #22 |
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| Jan7-10, 01:40 AM | #23 |
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Recognitions:
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| Jan7-10, 01:58 AM | #24 |
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The Dirac delta is an unusual beast; not really a function in the usual sense; but more particularly it isn't a model for the universe. There is no model of the universe which goes from finite to infinite. I've explained multiple times now the case for conventional cosmological Big Bang models, which may be either finite or infinite; they never change from one to the other. What you mean by the last sentence is really unclear. Under the assumptions I have given... an infinite flat homogenous topologically simple universe ... the existence of an infinite number of "twins" is pretty much inevitable. The good old ΛCDM model is of this form, if you take curvature as identically zero and extend homogeneity arbitrarily beyond the visible horizon. If by probability of "finding" a given collection of atoms you mean the probability of you meeting your own twin; sure... but that isn't what we've been talking about. Cheers -- sylas |
| Jan7-10, 11:45 AM | #25 |
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EDIT: OK, for an infinite number of twins you can define a non zero probability of a twin in an infinite universe. |
| Jan7-10, 12:07 PM | #26 |
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| Jan7-10, 05:06 PM | #27 |
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There is a perfectly adequate physical theory for an expanding universe, which covers both the case of an infinite universe and a finite universe. I have said this repeatedly and in some detail. What science does not have is a unified theory of physics applicable to the conditions of extreme density in the very very early universe. That is, we can handle the expansion, but not the point of origin. The theory for the expanding universe works just fine, and it not limited to either finite or infinite cases. Sylas |
| Jan8-10, 08:16 AM | #28 |
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| Jan8-10, 08:26 AM | #29 |
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| Feb17-10, 12:51 AM | #30 |
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from philosophy to science, there is a long path to go. we are curious so we speculate about things. a scientific jouranl has tired to inspire people to go through that path. i think that this curiousity is leading scientists and philosophors to move forward. i am also living for those unsolved questions but I think that we should act collectively for enormous mutual benefit and economies of scale.
if you donot agree we can correct each other. |
| Feb27-10, 03:42 AM | #31 |
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While the article seemed pretty far out, perhaps the name Max Tegmark was the reason for publishing? |
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