We present comprehensive results from constant NVT and constant NPT Monte C
arlo simulations of particles interacting via a biaxial variant of the Gay-
Berne potential which we term the Internally Rotated Gay-Berne (IRGB) poten
tial. The IRGB potential may be considered to be a single-site approximatio
n to the interaction between two zig-zag shaped molecules, the extent of th
is molecular biaxiality being characterized by an internal rotation angle d
elta. We find that increasing the value of delta frustrates the formation o
f orientationally ordered phases, all phase transitions being shifted to lo
wer temperatures and higher densities. Additionally, for delta greater than
or equal to 30 degrees, the smectic B phase is replaced by the tilted smec
tic J phase. The smectic A phase, in contrast, is destabilized completely f
or sufficiently large delta, with neither smectic A nor its tilted equivale
nt, smectic C, being observed. This suggests that models for smectic C-form
ation which are based on biaxial intermolecular attractions may not offer t
he best route to obtaining this phase. (C) 2000 American Institute of Physi
cs. [S0021-9606(00)50636-9].