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TABLE 12.3
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Security Layer (Optional) Part 8 TCP/IP Transport Layer Parts 11 & 12 Physical Media & Media
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In either case, the difference between ntot and 1 is an increasing function of time. That means that the flat geometry is an unstable situation for the Universe; if there is any deviation from it then the Universe will very quickly become more and more curved. Consequently, for the Universe to be so close to flat even at its large present age means that at very early times it must have been extremely close to the flat geometry. An alternative way to see this is to remember that the densities of matter and radiation reduce with expansion as l/a 3 and l/a 4 respectively. These are both faster reductions than the curvature term k/ a 2 . So if the curvature term is not to totally dominate in the present Universe, it must have begun much smaller than the other terms. The equations for In tot - 11 derived above stop being valid once the curvature or cosmological constant terms are no longer negligible, since we used the a(t) solutions for the flat geometry to derive them. But they are fine to give us an approximate idea of what the problem is. For extra ease let's assume that the Universe always has only radiation in it. Using the equations above, we can ask how close to one the density parameter must have been at various early times, based on the constraint today (to ~ 4 x 10 17 sec). At decoupling (t ~ 10 13 sec), we need
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12.6 Applications of GrACE
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