P. Padilla et E. Velasco, THE ISOTROPIC-NEMATIC TRANSITION FOR THE HARD GAUSSIAN OVERLAP FLUID - TESTING THE DECOUPLING APPROXIMATION, The Journal of chemical physics, 106(24), 1997, pp. 10299-10310
The isotropic-nematic phase transition in a fluid of moderately long m
olecules interacting via a hard Gaussian overlap potential is studied
using the decoupling approximation and computer simulation. Molecules
of length-to-breadth ratios equal to 3 and 5, thought to set the relev
ant range of molecular elongations in real nematic liquid crystals, ar
e considered. The results of the theory (pressure, order parameter, an
d location of the phase transition) and of several of its extensions,
are compared with those from computer simulation, and their relative a
ccuracy assessed. We first study the standard decoupling approximation
, a resummed Onsager virial expansion where only the (exact) second vi
rial coefficient, B-2, is retained, and consider two different mapping
s to perform the resummation: a fluid of equivalent hard spheres and t
he isotropic phase of the hard Gaussian overlap fluid. Whereas the for
mer mapping predicts a phase transition already in qualitative agreeme
nt with simulation, the mapping to the isotropic phase predicts a tran
sition in closer agreement with the simulation result, shifting the lo
cation of the transition to lower pressures. However, the transition i
s overestimated in both cases, which seems to indicate a poor represen
tation of angular correlations. In order to incorporate higher-order c
orrelations, an approximate method is proposed to evaluate the B-3 and
B-4 virial coefficients in the nematic phase numerically. This new in
formation allows us to address two points: (i) the convergence of the
virial series for short molecules, and (ii) the performance of extende
d decoupling approximation theories, incorporating the third and the f
ourth virial coefficients. As expected, inclusion of the high-order vi
rial coefficients improves the results of the corresponding truncated
virial expansion for the largest elongation considered, and provides q
uantitative agreement with the simulations, indicating a fast converge
nce of the virial series. The standard decoupling approximation provid
es results of similar accuracy. Also, the extended decoupling approxim
ation including B-3 improves these results, though the extension to B-
4 degrades the coexistence data slightly, which might indicate that th
e latter misrepresents to some extent the importance of angular correl
ations. In contrast, for molecules with a length-to-breadth ratio of 3
, the truncated virial expansion is still inaccurate, whereas the exte
nded decoupling approximation theories perform better, providing almos
t quantitative agreement with the simulations. As a result of our find
ings, we conclude that in order to improve the standard decoupling app
roximation for fluids of short molecules, it is essential to resum the
virial series using knowledge of the B-3 virial coefficient and also
the B-4 coefficient for the shortest molecules forming nematic phases.
(C) 1997 American Institute of Physics.