A novel nonequilibrium molecular dynamics, originating in mesoscopic t
heory of suspensions, is introduced to investigate the behavior of mod
el polymeric fluids consisting of several hundred ellipsoids of revolu
tion (spheroids) that interact via the Gay-Berne potential. This dynam
ics is used to generate new microstructural, thermodynamic and rheolog
ical data. The microcanonical equtions of motion for the translational
and angular momenta as well as for mass-centers and orientational uni
t vectors are derived from a Hamiltonian. These expressions are then a
ugmented by SLLOD-like and Gaussian thermostat terms added consistentl
y to equations for both the rotational and translational degrees of fr
eedom; the role of Gaussian thermostat is to maintain constant kinetic
temperature of the assembly of spheroids. The thermodynamic results a
re calculated along one isotherm (nondimensional temperature T maintai
ned at unity). Rheology is investigated for two state points (namely f
or particle number density rho equal to 0.25, 0.4 and T set to 1), tha
t lie well inside the isotropic phase if no external flow is applied.
A state point is defined by the fluid's temperature T, and the concent
ration of particles per unit volume rho. As indicated by snapshots of
molecular configurations, at the intermediate shear rates (nondimensio
nal shear rate approximately 1-2), ellipsoids become aligned to the di
rection of flow and the stress tensor begins to be nonsymmetric. At ev
en higher shear rates, this configuration breaks down leading to the f
ormation of a transitory isotropic-type fluid, and then to the build-u
p of a highly ordered structure exhibiting global orientation of parti
cles in the direction of the vorticity axis. For rho = 0.4, the first
(N1) and the second (N2) normal stress differences are positive and ne
gative respectively, but at low densities (rho = 0.25), N1 becomes sli
ghtly negative. In addition to the stress tensor, we compute the confo
rmation tensor, the order parameter and the components of the pair rad
ial distribution function. At high shear rates the radial distribution
functions become significantly anisotropic. Furthermore, we investiga
te the phenomenon of the stress overshoot at the inception of the simp
le shear flow from a molecular perspective, and study the evolution of
the distribution of translational velocities as a function of the she
ar rate.