If we consider a simple case where the radius, R, of a sphere inside the Universe is steadily increasing with time then the volume will increase as the radius cubed. Hence the number density (number of particles divided by the volume) of both the matter and the photons will go as R-3 . However, in the case of the photons, the temperature also decreases with R and so their energy declines. This leads to the general condition that
for the the matter and radiation energy densities, respectively.
Figure 2.10 Schematic representation
of the faster fall off in the energy density of radiation
compared to that of matter in and expanding and cooling
Universe. The point where the two energy densities are equal
is indicated. This point, called recombination, is fully
discussed in Chapter 3.
|
The radiation dominated era leads to an immediate problem which is discussed in more detail in Chapter 3. Recall that the ratio of photons to matter particles in our Universe is about one billion to one. When the temperature of the Universe is high, the radiation pressure is also high and this radiation pressure can physically effect matter. As matter tries to clump due to gravity, the high radiation pressure intercedes and prevents the clumping. In fact, the radiation pressure is attempting to smooth out the distribution of matter. If this was completely successful then the distribution of matter would be perfectly smooth and there would be no net gravity felt by one particle towards another (recall this was Newton's solution to the problem of the collapsing Universe). If there is no net gravity then there would be no galaxy formation (and you wouldn't have to be reading this sentence). The great challenge in understanding galaxy formation is understanding how density fluctuations can maintain their integrity and grow during the radiation dominated era of the Universe. As we will see, this may well demand the existence of dark matter.