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Universe size |
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| Jul4-12, 01:17 AM | #18 |
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Universe size
thank you very much for your kind answer George. In fact, I was not particularly afraid by recession velocities higher than c given that this limit does not apply to space expansion, but I just wondered (for other reasons) if Vrec > c were really observed because H has been proven to be lower than H0 in the past (expansion accelerates)
I have an other question with respect to your answer: I wonder why SR is not sufficient for studying the geometry of expanding universe models, supposed to be isotropic and homogeneous as empty. General relativity deals with gravity? |
| Jul4-12, 01:44 AM | #19 |
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SR does not take gravity into account. That was the whole point of GR.
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| Jul4-12, 03:24 AM | #20 |
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Yes. But precisely, all what I read about universe expansion and horizons, begins with a redefinition of the line element of SR (ds2=(cdt)2+a(t)2dl2)
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| Jul5-12, 04:33 PM | #21 |
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Mentor
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| Jul6-12, 01:04 AM | #22 |
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Indeed I was not clear. I just wanted to say that authors talking about light connection rates in the expanding universe never make use of GR, but only derive their conclusions from the simple relationship cdt=a(t)*dl (note there is a typing error of sign in my previous equation). SR seems to be sufficient. Gravity and GR are generally not involved in the universe model used in these studies.
Furthermore, even SR seems to be not observed: calculations using speed substractions such as c-Vrec, rather resemble to classical mechanics ... even if I understood that Vrec is not a genuine speed. |
| Jul6-12, 05:09 AM | #23 |
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The limits of what we can see are about x3 times the current Hubble light-travel-time. A good place to learn about all the different cosmological distances is Professor Ned Wright's Cosmology Tutorial... Ned Wright's Cosmology Tutorial ...which features a handy Java calculator of all sorts of cosmic parameters. So handy that people have referenced it in their papers. |
| Jul6-12, 08:27 AM | #24 |
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Many thanks for these informations
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| Jul6-12, 08:32 AM | #25 |
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Recognitions:
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| Jul6-12, 08:55 AM | #26 |
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But how do you conceive a finite euclidean 3D space? with a peripheral boundary? looks strange
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| Jul6-12, 08:57 AM | #27 |
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| Jul6-12, 10:31 AM | #28 |
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Recognitions:
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| Jul6-12, 11:49 AM | #29 |
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4D torus?
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| Jul6-12, 01:01 PM | #30 |
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Recognitions:
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| Jul6-12, 01:23 PM | #31 |
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I have a naive perception of topology: the number of dimensions of any shape is that of the minimal euclidean space capable of embedding it. Your torus is 4D to me, even for something confined in its surface
the circle is a good example: unidimensional if envisioned from the interior, but in fact genuinely bidimensionnal |
| Jul7-12, 02:53 PM | #32 |
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Mentor
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[tex] \left( \frac{da}{dt} \left(t\right) \right)^2 = H_0^2 \left( \Omega_{m0} a\left(t\right)^{-1} + \Omega_{r0} a\left(t\right)^{-2} + \Omega_{\Lambda 0} a\left(t\right)^2 + 1 - \Omega_{m0} - \Omega_{r0} - \Omega_{\Lambda 0} \right), [/tex] where the constants [itex]\Omega_{m0}[/itex], [itex]\Omega_{r0}[/itex], [itex]\Omega_{\Lambda 0}[/itex] are the current densities (relative to critical density) of matter, radiation, and dark energy, respectively. This equation comes from Einstein's equation of general relativity, i.e., it come form Einstein's theory of gravity. |
| Jul8-12, 01:43 AM | #33 |
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I disagree with you, the scale factor has first been naturally postulated because of the observation of Hubble. You describe one of the multiple a-posteriori attempts to calculate the expansion rate(s) from the universe constituents: (matter/energy and now the more exotic dark energy). These attempts are very interesting from a physical viewpoint but please do not inverse the string. a(t) did not emerge from matter/energy density calculations but was just postulated a-priori. To my knowledge its time-dependence has not been firmly established yet and it is likely to be underlain by different successive functions in the course of cosmic time |
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