McGarrity E S, Frischknecht A L, Frink L J D, Mackay M E
Department of Chemical Engineering & Materials Science, Michigan State University, East Lansing, Michigan, 48824-1226, USA.
Phys Rev Lett. 2007 Dec 7;99(23):238302. doi: 10.1103/PhysRevLett.99.238302.
We investigate the phase behavior of athermal polymer-nanoparticle blends near a substrate. We apply a recent fluids density functional theory of Tripathi and Chapman to a simple model of the blend as a mixture of hard spheres and freely jointed hard chains, near a hard wall. We find that there is a first-order phase transition in which the nanoparticles expel the polymer from the surface to form a monolayer. The nanoparticle transition density depends on the length of the polymer and the overall bulk density of the system. The effect is due both to packing entropy effects related to size asymmetry between the components and to the polymer configurational entropy. The simplicity of the system allows us to understand the so-called "entropic-push" observed in experiments.
我们研究了在基底附近无热聚合物 - 纳米颗粒共混物的相行为。我们将Tripathi和Chapman最近提出的流体密度泛函理论应用于一种简单的共混物模型,该模型将共混物视为硬球和自由连接硬链的混合物,处于硬壁附近。我们发现存在一级相变,其中纳米颗粒将聚合物从表面排挤出去以形成单层。纳米颗粒的转变密度取决于聚合物的长度和系统的整体体密度。这种效应既归因于与组分间尺寸不对称相关的堆积熵效应,也归因于聚合物的构象熵。该系统的简单性使我们能够理解在实验中观察到的所谓“熵推”现象。