There are also important characteristic time scales that govern the dynamics of globular clusters. These are the crossing time , the relaxation time , and the evaporation time . The crossing time is the typical time required for a star in the cluster to travel the characteristic size of the cluster (typically taken to be the half-mass radius). Thus, , where is a typical velocity ( 10 km/s). The relaxation time is the typical time for gravitational interactions with other stars in the cluster to remove the history of a star’s original velocity. This amounts to the timerequired for gravitational encounters to alter the star’s velocity by an amount comparable to its original velocity. Since the relaxation time is related to the number and strength of the gravitational encounters of a typical cluster star, it is related to the number of stars in the cluster and the average energy of the stars in the cluster. Thus, it can be shown that the mean relaxation time for a cluster is [19, 116]. It should be noted, however, that Figure 1.3 of Spitzer  gives a median and Padmanabhan gives .
The evaporation time for a cluster is the time required for the cluster to dissolve through the gradual loss of stars that gain sufficient velocity through encounters to escape its gravitational potential. In the absence of stellar evolution and tidal interactions with the galaxy, the evaporation time can be estimated by assuming that a fraction of the stars in the cluster are evaporated every relaxation time. Thus, the rate of loss is . The value of can be determined by noting that the escape speed at a point is related to the gravitational potential at that point by . Consequently, the mean-square escape speed in a cluster with density is and references therein for a thorough discussion of these effects. For a globular cluster, , which is comparable to the observed age of globular clusters.
The characteristic time scales differ significantly from each other: . When discussing stellar interactions during a given epoch of globular cluster evolution, it is possible to describe the background structure of the globular cluster in terms of a static model. These models describe the structure of the cluster in terms of a distribution function that can be thought of as providing a probability of finding a star at a particular location in phase-space. The static models are valid over time scales which are shorter than the relaxation time so that gravitational interactions do not have time to significantly alter the distribution function. We can therefore assume . The structure of the globular cluster is then determined by the collisionless Boltzmann equation,
The solutions to Equation (5) are often described in terms of the relative energy per unit mass with the relative potential defined as . The constant is chosen so that there are no stars with relative energy less than 0 (i.e. for and for ). A simple class of solutions to Equation (5),