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首页> 外文期刊>The Journal of Chemical Physics >The isotropic-nematic and nematic-nematic phase transition of binary mixtures of tangent hard-sphere chain fluids: An analytical equation of state
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The isotropic-nematic and nematic-nematic phase transition of binary mixtures of tangent hard-sphere chain fluids: An analytical equation of state

机译:切向硬球链流体二元混合物的各向同性和向列向列相变:状态分析方程

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An analytical equation of state (EoS) is derived to describe the isotropic (I) and nematic (N) phase of linear- and partially flexible tangent hard-sphere chain fluids and their mixtures. The EoS is based on an extension of Onsager's second virial theory that was developed in our previous work [T. van Westen, B. Oyarzún, T. J. H. Vlugt, and J. Gross, J. Chem. Phys. 139, 034505 (2013)]. Higher virial coefficients are calculated using a Vega-Lago rescaling procedure, which is hereby generalized to mixtures. The EoS is used to study (1) the effect of length bidispersity on the I-N and N-N phase behavior of binary linear tangent hard-sphere chain fluid mixtures, (2) the effect of partial molecular flexibility on the binary phase diagram, and (3) the solubility of hard-sphere solutes in I- and N tangent hard-sphere chain fluids. By changing the length bidispersity, two types of phase diagrams were found. The first type is characterized by an I-N region at low pressure and a N-N demixed region at higher pressure that starts from an I-N-N triphase equilibrium. The second type does not show the I-N-N equilibrium. Instead, the N-N region starts from a lower critical point at a pressure above the I-N region. The results for the I-N region are in excellent agreement with the results from molecular simulations. It is shown that the N-N demixing is driven both by orientational and configurational/ excluded volume entropy. By making the chains partially flexible, it is shown that the driving force resulting from the configurational entropy is reduced (due to a less anisotropic pairexcluded volume), resulting in a shift of the N-N demixed region to higher pressure. Compared to linear chains, no topological differences in the phase diagram were found. We show that the solubility of hard-sphere solutes decreases across the I-N phase transition. Furthermore, it is shown that by using a liquid crystal mixture as the solvent, the solubility difference can by maximized by tuning the composition. Theoretical results for the Henry's law constant of the hard-sphere solute are in good agreement with the results from molecular simulation.
机译:导出了状态分析方程(EoS),以描述线性和部分柔性切线硬球链流体及其混合物的各向同性(I)和向列相(N)。 EoS基于Onsager的第二病毒论理论的扩展,该理论是我们先前的工作[T. van Westen,B.Oyarzún,T.J.H.Vlugt和J.Gross,J.Chem。物理139,034505(2013)]。使用Vega-Lago重标度程序计算较高的病毒系数,在此将其概括为混合物。 EoS用于研究(1)长度双分散性对二元线性正切硬球链流体混合物的IN和NN相行为的影响;(2)部分分子柔性对二元相图的影响;和(3 )硬球溶质在I和N切线硬球链流体中的溶解度。通过改变长度双分散度,发现了两种类型的相图。第一种类型的特征是从I-N-N三相平衡开始的低压I-N区和高压N-N混合区。第二种类型不显示I-N-N平衡。取而代之的是,N-N区从一个较低的临界点开始,压力高于I-N区。 I-N区的结果与分子模拟的结果非常吻合。结果表明,N-N混合是由定向和构型/排除体积熵驱动的。通过使链部分地挠曲,表明了由于结构熵引起的驱动力减小了(由于各向异性对的排除体积减小了),导致了N-N混合区向较高压力的移动。与线性链相比,在相图中未发现拓扑差异。我们表明,硬球溶质的溶解度在I-N相变过程中降低。此外,显示出通过使用液晶混合物作为溶剂,可以通过调整组成来使溶解度差最大化。硬球溶质的亨利定律常数的理论结果与分子模拟的结果非常吻合。

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