A potential model has been developed to study the behaviour of CF, ads
orbed on graphite. To avoid the normal problems in simulating commensu
rate/incommensurate phase transitions, we have studied a patch of 400
molecules in the centre of a periodically repeating box at a total cov
erage of 1/2. The model patch melts, dose to the experimentally predic
ted temperature, from the correct (2 x 2) commensurate solid structure
. At the melting temperature the average intermolecular separation in
the centre of the patch is 4.92 Angstrom, which is that of the commens
urate (2 x 2) structure. The order parameter which measures order with
respect to the perfect (2 x 2) lattice fans sharply at 75 K. The ener
gy minimisations have shown that an important characteristic of this s
ystem is the low barrier to translation, for tripod-down molecules, be
tween the bridge and atop sites. Variations in the order parameter O-1
, which measures the order of the molecules with respect to the surfac
e, indicate that a patch of molecules is not strongly pinned to the su
rface. The molecules at the centre of the patch are observed to make c
oncerted moves between the edge and bridge sites during the course of
simulations. At all temperatures the molecules are observed to be orie
ntationally ordered. Below the melting temperature there is orientatio
nal order both in the plane and out of the plane of the surface. Molec
ules prefer to be tripod-down, and there is a preferred direction in t
he plane of the surface for the CF bonds pointing towards the surface.
The order parameter which measures in-plane order decays to zero appr
oximately 3 K below the observed translational melting temperature, in
dicating that any orientationally disordered phase must exist over a s
mall temperature range just prior to translational melting. Above the
melting temperature the in-plane distribution curves shown some in-pla
ne ordering of the molecules, which is induced by the surface corrugat
ion potential. Energy minimisation calculations indicate that the low-
temperature structure for this model is an incommensurate, hexagonally
close-packed structure with the molecules in the tripod-down orientat
ion. The simulations show no evidence of the phase transitions below 7
3 K observed in the calorimetric studies.