An empirical potential energy function, comprising two- and three-body
terms, has been derived for aluminium. This potential reproduces the
experimental energies and relaxations of the (111), (110) and (100) su
rfaces of fee Al to a high degree of accuracy. The melting of bulk fcc
Al and its low index surfaces has been studied in detail by employing
Monte Carlo simulation techniques. Melting has been defined in terms
of a number of calculated quantities: order parameters, density profil
es and radial distribution functions. The many-body potential overesti
mates the bulk melting temperature (T-m approximate to 1275+/-25 K) by
approximately 37% but reproduces the sharp melting transition observe
d experimentally. To obtain a melting point in agreement with experime
nt we would need to lower the energy scaling parameter (determined fro
m room temperature data) by 37%. The potential also indicates that the
relatively open (110) surface melts about 200 K below the bulk, while
the denser (100) surface does not melt until T-m. These findings are
again in good agreement with experiment and with previous calculations
. (C) 1997 Elsevier Science BV.