chapter 5
We have mapped out the complete phase diagram of hard spherocylinders
as a function of the length-to-width ratio . Special
computational techniques were required to locate phase transitions in
the limit
and in the close-packing limit for
. The phase boundaries of five different phases
were established: the isotropic fluid, the liquid crystalline
smectic A and nematic phases, the orientationally-ordered solids ---
in AAA and ABC stacking --- and the plastic or rotator solid. The
rotator phase is unstable for
0.35 and the AAA crystal
becomes unstable for lengths smaller than
7. The triple
points isotropic-smectic-A-solid and isotropic-nematic-smectic-A are
estimated to occur at
=3.1 and
=3.5 respectively. For the
low
region, a modified version of the Gibbs-Duhem integration
method was used to calculate the isotropic-solid coexistence
curves. This method was also applied to the isotropic-nematic transition for
10. For large
the simulation results approach the predictions
of the Onsager theory. In the limit
simulations were performed by application of a scaling technique. The
nematic-smectic-A transition for
appears to
be continuous. As the nematic-smectic-A transition is certainly of
first order nature for
5, the tri-critical point is
presumably located between
region, the plastic solid to aligned solid transition is first
order. Using a mapping of the dense sphero-cylinder system on a
lattice model, the initial slope of the coexistence curve could even
be computed in the close packing limit.