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Phase behavior of polymeranoparticle blends near a substrate

机译:基材附近的聚合物/纳米粒子共混物的相行为

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We use the recent fluids density functional theory of Tripathi and Chapman [Phys. Rev. Lett. 94, 087801 (2005); J. Chem. Phys. 122, 094506 (2005)] to investigate the phase behavior of athermal polymeranoparticle blends near a substrate. The blends are modeled 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 surface 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. In addition, 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. (c) 2008 American Institute of Physics.
机译:我们使用Tripathi和Chapman的最新流体密度泛函理论[Phys。牧师94,087801(2005); J.化学物理122,094506(2005)]来研究基材附近无热聚合物/纳米粒子混合物的相行为。共混物建模为硬球和硬壁附近自由连接的硬链的混合物。这些共混物中存在一级相变,其中纳米颗粒将聚合物从表面排出,以一定的纳米颗粒浓度形成单层。纳米粒子的转变密度取决于聚合物的长度,纳米粒子的直径和系统的整体堆积密度。相变既归因于与组分之间的尺寸不对称有关的堆积熵效应,也归因于聚合物构型熵,这证明了在实验中观察到的所谓的“熵推动”是合理的。另外,发现在较高密度下的层状状态类似于在胶体晶体中的状态,其中聚合物和纳米颗粒形成交替的离散层。我们表明,这种层流状态具有与本体中均匀混合的流体几乎相同的自由能,并被表面成核。 (c)2008年美国物理研究所。

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