Exploring the Discrepancy in Heat Distribution in the Expanding Universe

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In summary: These variations have been used to measure the rate of expansion of the universe. However, if the universe has been expanding for an infinite amount of time, then the variations should be uniform throughout the universe. However, this is not the case. This is known as the "horizon" problem. Inflation theory offers a solution to this problem. Basically, it suggests that the universe has been expanding for a very long time, but that at some point it reached a point where the various regions of the universe were expanding at different rates. As a result, the regions that were closer to the big bang (and thus had more heat) ended up expanding faster than the regions that were further away. Inflation theory suggests that the uniformity of the variations
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csrichie
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I ran across this on a website. The problem is, because heat spreads out slower than light, when the big bang explodes and expands at the speed of light then there should be unequal heat regions all over the universe. But this is not true according to observation. Why is this so?
 
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csrichie said:
I ran across this on a website. The problem is, because heat spreads out slower than light, when the big bang explodes and expands at the speed of light then there should be unequal heat regions all over the universe. But this is not true according to observation. Why is this so?

The standard explanation is inflation. The problem is known as "the horizon problem". See for instance http://www.astro.ucla.edu/~wright/cosmoall.htm (I'll provide a short quote to point out the specific applicable section).

Any event that influences the temperature of the CMB that we see on the left side of the sky must be within the left-hand yellow region. Any event that affects the temperature of the CMB on the right side of the sky must be within the right-hand yellow region. These regions have no events in common, but the two temperatures are equal to better than 1 part in 10,000. How is this possible? This is known as the "horizon" problem in cosmology.

Inflation

The "inflationary scenario", developed by Starobinsky and by Guth, offers a solution to the flatness-oldness problem and the horizon problem.

The "flatness-oldness" problem (i.e. why omega is close to one) is also explained by inflation.
 
  • #3
That does not make any sense to me, csrichie. Heat is transferred by kinetic and photonic energy, according to current theories. The speed of transfer is interrupted by molecules jostling for a more stable position in the grand scheme of things.
 
  • #4
csrichie said:
... when the big bang explodes and expands at the speed of light ...
Note that the Big Bang was not like a conventional "explosion" (it was, in part, the rapid expansion of all space) Also, it didn't expand at the speed of light (at least, not for more than an instant as you'll see from pervect's info about the inflationary period). Also note that there are observable variations in the cosmic microwave background radiation.
 

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