Originally posted by wolram
the expansion of the universe is generaly excepted but what
governes this expansion? and what would be the outcome if
if the "control" for expansion differed by x%
best wishes
the expansion is governed by a simple formula called Friedmann
and the "control" for the expansion is energy density
for the greatest simplification assume space is flat (which they tell us is true to within a percent or so, good enough for government work) and pretend all the constants like G and c are equal to one.
Then Friedman says the square of the expansion rate H is equal to 8pi/3 times the density
John Baez recommends a trick that even makes the 8pi go away---theoreticians like the maximum mental economy and comfort.
So if you do things his way and sweep the 8pi under the rug (and why not get rid of the 3 as well while we're at it) then the square of the expansion rate H is just EQUAL to the density.
BTW negative expansion is contraction. So the equation
H
2 = density
has two solutions a positive H and a negative contraction-rate H.
There is also a second Friedmann equation we can call Mrs. Friedmann which governs the rate H changes
It is also very simple, like this one, and the "control" term
is - (density + 3 X pressure)
that is, minus the quantity (density plus 3 times the pressure)
well if you look out at night you see that the average density in space is pretty sparse and you can imagine the pressure is incredibly skimpy and almost completely negligible
But the two equations have a heck of a lot of space to work with and a whole lot of time and they arent in a hurry, so these things
we think of as almost zero (what kind of average density and pressure do you get from a few stars scattered about?) nevertheless WORK in the long run and do control things
(in the slick tight-lipped way that differential equations control things, never quite revealing how they do it)
best wishes to you in return