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在 Jagla 溶剂中对简单两亲性溶质进行建模。

Modeling simple amphiphilic solutes in a Jagla solvent.

机构信息

Center for Polymer Studies and Department of Physics, Boston University, Boston, Massachusetts 02215, USA.

出版信息

J Chem Phys. 2012 Jan 28;136(4):044511. doi: 10.1063/1.3677185.

Abstract

Methanol is an amphiphilic solute whose aqueous solutions exhibit distinctive physical properties. The volume change upon mixing, for example, is negative across the entire composition range, indicating strong association. We explore the corresponding behavior of a Jagla solvent, which has been previously shown to exhibit many of the anomalous properties of water. We consider two models of an amphiphilic solute: (i) a "dimer" model, which consists of one hydrophobic hard sphere linked to a Jagla particle with a permanent bond, and (ii) a "monomer" model, which is a limiting case of the dimer, formed by concentrically overlapping a hard sphere and a Jagla particle. Using discrete molecular dynamics, we calculate the thermodynamic properties of the resulting solutions. We systematically vary the set of parameters of the dimer and monomer models and find that one can readily reproduce the experimental behavior of the excess volume of the methanol-water system as a function of methanol volume fraction. We compare the pressure and temperature dependence of the excess volume and the excess enthalpy of both models with experimental data on methanol-water solutions and find qualitative agreement in most cases. We also investigate the solute effect on the temperature of maximum density and find that the effect of concentration is orders of magnitude stronger than measured experimentally.

摘要

甲醇是一种两亲性溶质,其水溶液表现出独特的物理性质。例如,混合时的体积变化在整个组成范围内为负,表明存在强烈的缔合。我们探索了 Jagla 溶剂的相应行为,Jagla 溶剂先前已显示出许多与水异常的性质。我们考虑了两种两亲性溶质模型:(i)“二聚体”模型,由一个疏水硬球与一个具有永久键的 Jagla 粒子相连组成;(ii)“单体”模型,是二聚体的极限情况,由同心重叠的硬球和 Jagla 粒子形成。使用离散分子动力学,我们计算了所得溶液的热力学性质。我们系统地改变二聚体和单体模型的参数集,并发现可以很容易地再现甲醇-水体系过量体积随甲醇体积分数的实验行为。我们将两个模型的过量体积和过量焓的压力和温度依赖性与甲醇-水溶液的实验数据进行比较,并在大多数情况下发现定性一致。我们还研究了溶质对最大密度温度的影响,并发现浓度的影响比实验测量的要强几个数量级。

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