The behavior of gravitational phase transitions in a system of concentric,
spherical, mass shells that interact via their mutual and self gravitation
is investigated. The nature of the transition in the microcanonical, canoni
cal, and grand canonical ensembles is studied both theoretically in terms o
f the mean field limit and by dynamical simulation. Transitions between a q
uasiuniform state and a centrally concentrated state are predicted by mean
field theory for the microcanonical and canonical ensembles, and this is su
pported by dynamical simulation. For the grand canonical ensemble, mean fie
ld theory predicts that no transition takes place, and that the thermodynam
ically stable state is always the uniform one. Again, this is supported by
simulations under various initial distributions of mass, even when the syst
em is initialized in a collapsed state. In addition to testing the predicti
ons of the mean field theory and studying the effects of finite size scalin
g,dynamical simulation allowed us to examine the behavior of temporal and p
ositional correlations which are predicted to vanish in the mean field Limi
t.