Vg. Mavrantzas et An. Beris, A hierarchical model for surface effects on chain conformation and rheology of polymer solutions. I. General formulation, J CHEM PHYS, 110(1), 1999, pp. 616-627
The flow behavior of polymer solutions near a solid surface (either neutral
or adsorbing) is modeled through a new, hierarchical (macroscopic and micr
oscopic) approach which enables the thermodynamically consistent extension
of equilibrium (static) considerations to nonequilibrium (flow) conditions.
The approach involves two steps: First, the set of primary, independent, v
ariables defining the state of the system at the macroscopic level is chose
n, and a complete set of transport and constitutive equations is constructe
d for them through a two fluid, Hamiltonian model. In the present work, the
macroscopic variables include the polymer chain concentration, the macrosc
opic fluid velocity, and the conformation tensor (defined as the tensor of
the second moment of the chain end-to-end vector). The governing equations
involve the (extended) free energy or Hamiltonian of the system, H, and are
valid both in the bulk of the fluid and in the interfacial region. Thus, t
o solve them one needs to specify H. This is done in a second step, by invo
king a microscopic model, which consistently takes into account the simulta
neous effect on chain conformations of both the solid boundary and the impo
sed flow field. Solid boundary effects are taken into account in the soluti
on of a diffusion equation for the chain propagator G(r, n; r(0)) which rep
resents the weighted probability that an n-segment long chain which starts
at r(0) will end at position r. Flow field effects are taken into account t
hrough the definition of a generalized propagator G'(r, n; r(0), alpha), wh
ich further depends on the apparent strain tensor alpha, representing chain
deformation effects due to flow. The present part of the paper describes t
he general formulation of the approach and its relevance with previous work
s. Results from applying the methodology to the case of a polymer solution
flowing past a purely repulsive surface (a wall) are presented in the secon
d part of this work. (C) 1999 American Institute of Physics. [S0021-9606(99
)50701-0].