chapter 5



THE PHASE DIAGRAM OFHARD SPHEROCYLINDERS

 

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.




Peter Bolhuis
Tue Sep 24 20:44:02 MDT 1996