Erin S. McGarrity1, Amalie L. Frischknecht2, and Michael E. Mackay1. (1) Dept. of Chemical Engineering & Materials Science, Michigan State University, East Lansing, MI 48824, (2) Sandia National Laboratories, PO Box 5800 MS 1411, Albuquerque, NM 87185-1411
We study the phase behavior of polymer/nanoparticle blends near a substrate using a fluids density functional theory. Initially we model the blends as a mixture of hard spheres and freely jointed hard chains, near a hard wall. There is a first order phase transition present in these blends in which the nanoparticles expel the polymer from the substrate to form a monolayer at a certain nanoparticle concentration. The nanoparticle transition density depends on the length of the polymer, the nanoparticle diameter, and the overall bulk density of the system. The phase transition is due to both packing entropy effects related to size asymmetry between the components, and to the polymer configurational entropy, justifying the so-called “entropic push” observed in experiments. A layered state is found at higher densities which resembles that in colloidal crystals, in which the polymer and nanoparticles form alternating discrete layers. We show that this laminar state has nearly the same free energy as the homogeneously mixed fluid in the bulk and is nucleated by the surface. In addition to these athermal results, we will present preliminary data from calculations in which the polymers, particles, and substrate are attractive.
This work was performed in part at the U.S. Department of Energy, Center for Integrated Nanotechnologies, at Los Alamos National Laboratory (Contract No. DE-AC52-06NA25396) and Sandia National Laboratories (Contract No. DE-AC04-94AL85000).