Two coarse-grained models for polymer chains in dense glass-forming polymer
melts are studied by computer simulation: the bond fluctuation model on a
simple cubic lattice is treated by Monte Carlo methods, and a continuum bea
d-spring model with a Lennard-Jones potential between the beads is treated
by means of molecular dynamics. While the dynamics of the two models differ
for short length scales and the associated timescales, the two models beha
ve similarly on mesoscopic spatial and temporal scales. In particular, the
mode-coupling theory of the glass transition can be used to interpret the s
lowing down of the undercooled polymer melt. For the off-lattice model, the
approach to the critical point of mode coupling is studied both at constan
t pressure and constant volume. The lattice model allows a test of the Gibb
s-Di Marzio entropy theory of the glass transition to be carried out, and o
ur finding is that although the entropy does decrease significantly, there
is no 'entropy catastrophe' where the fluid entropy would turn negative. Fi
nally, a forward look at the effects of confinement on the glass transition
in thin-film geometry is given.