where we have factored all of the time
dependence of
R(t) into a(t), leaving the vector
X
with no time dependence, representing the co-moving distance
between the two galaxies. The common convention is to
set a(t) = 1 at the current age of the universe, such that
the physical vector
R(t) is equal to the co-moving
vector
X today.
The history and ultimate fate of the expansion is described
by the function a(t). If the universe contained a lot
of dark matter, called a closed universe, a(t) would rise,
reach a maximum, and then fall. The universe would
suffer a "Big Crunch" in which the galaxies would all
collide at some point in the future. If the universe
contained very little dark matter, called an open universe,
a(t) would rise forever. Galaxies would forever be
moving away from each other, with expansion never
stopping. If the universe contained precisely the
critical density of matter and energy, called a flat
universe, a(t) would rise forever but would approach an
asymptote at some final value. Galaxies would still be
forever moving away from each other, but the expansion of
the universe would approach zero. The following plot
shows these cases.