We investigate the structural changes that accompany the stress relaxa
tion in simple liquids by means of nonequilibrium molecular dynamics (
NEMD) simulations. It is shown that during elongational deformation of
the system, the statistical distribution of interacting neighbors abo
ut a given atom in the system, as measured by the mean interatomic dis
tance in an arbitrary direction, becomes ellipsoidal with the largest
semiaxis oriented in the stretch direction. Also, the mean number of p
articles in the distribution is smaller in that direction than normal
to the stretch axis. Therefore, the return to isotropy consists on the
one hand of a return of the spatial distribution of neighbors to the
spherical shape and, on the other hand, of an isotropization of the nu
mber density distribution. These two processes, which take place with
widely different rates, errs shown to be closely related to the two mo
des of stress relaxation characteristic for the simple liquids. The fi
rst of these, which is the fastest and corresponds to the most signifi
cant stress decay, is shown to be related to the fast return of the di
stribution of neighbors to the spherical shape. The second mode is int
imately related to the isotropization of the density distribution on t
he sphere through a quasidiffusional process. (C) 1997 American Instit
ute of Physics.