Annu. Rev. Astron. Astrophys. 1991. 29:
239-274
Copyright © 1991 by . All rights reserved |

The dynamical time scale in an elliptical galaxy ranges from less than
10^{5}
years in the central regions to more than 10^{9} years in the
outskirts. With
the possible exception of the inner nucleus, the two-body relaxation time is
everywhere much larger than a Hubble time. Thus, an elliptical galaxy is a
collisionless stellar system. The time scale for differential precession
between neighboring orbits is usually of the order of 5-10 dynamical times,
and becomes comparable to a Hubble time beyond a few optical radii. As a
result, the inner regions of elliptical galaxies are likely to be in
equilibrium, in agreement with their regular and smooth optical appearance,
but the outer regions probably have not experienced sufficient phase-mixing
to have reached equilibrium.

The structure and dynamics of a collisionless stellar system are determined
completely by the phase-space distribution function *f*(**r**,
**v**, *t*),
which gives the distribution of the stars in the system over position **r**
and velocity **v** as a function of time *t*. The distribution function
must be non-negative, and satisfy the collisionless Boltzmann equation. In an
equilibrium model ð*f* / ð*t* = 0. Integration of
*f* over all
velocities gives the density distribution (**r**) of the system. By
Jeans' theorem, *f* depends on the phase-space coordinates **r**
and **v** only through the isolating integrals of motion admitted by
the gravitational potential of the system
(179,
220,
but see 40).
Any collisionless dynamical model can be scaled in mass, radius
and central velocity dispersion, but only two of these three parameters can be
chosen freely, because of the constraint provided by the virial theorem
(48).