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Structure, thermodynamics and dynamics of confined and supercooled liquids.

机译:密闭和过冷液体的结构,热力学和动力学。

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摘要

Static measures such as density and entropy, which are intimately connected to structure, have featured prominently in modern thinking about the dynamics of the liquid state. In this dissertation, we explore the connections between self-diffusivity, density, available space, and excess entropy in two non-trivial problems in liquid state theory, confined and supercooled liquids.;We present exact simulation data for the relationship between self-diffusivity and excess entropy for a wide range of simple fluids (i.e. hard-sphere, Lennard-Jones and square-well) confined to pores with a variety of different sizes and fluid-wall interations. Our main finding is that, at a given temperature, self-diffusivity of the confined fluids collapses onto the bulk behavior when plotted versus excess entropy. In other words, the only information required to "predict" the implications of confinement for the single-particle dynamics is the bulk fluid behavior at a given temperature and the excess entropy of the confined fluid. This should prove practically useful given that the bulk behavior is well known for these fluid systems, and the excess entropy of the confined fluids can be readily estimated from classical density functional theory.;We also show that the self-diffusivity of the confined fluids approximately collapses onto the data for the corresponding bulk fluid when plotted versus the average packing fraction (which is based on total, rather than center accessible volume). For continuous interaction potentials such as Lennard-Jones, calculation of effective packing fraction requires knowledge of both the number density of the fluid and a temperature-dependent Boltzmann diameter associated with the repulsive part of the interparticle interactions. We suggest a way to calculate this effective diameter, which to a very good approximation, collapse the temperature- and density-dependent data for the self-diffusivity of the bulk Lennard-Jones fluid onto hard-sphere fluid data plotted versus the fluid's effective packing fraction.;Finally, we found that the self-diffusivities of several model systems in their supercooled state also scale exponentially not only with the excess entropy, but also with the two-body contribution to the excess entropy obtained from the pair correlation function of the fluid. The latter observation is particularly interesting because it provides direct evidence of a quantitative link between the dynamics and the average structural order of supercooled liquids. Whether such a connection could indeed be discovered is part of a long-standing question in the study of liquids.
机译:与结构密切相关的诸如密度和熵之类的静态量度在现代关于液态动力学的思考中尤为突出。本文研究了液态理论中两个非平凡问题-密闭和过冷液体-的自扩散率,密度,可用空间和过量熵之间的关系。以及广泛的简单流体(即硬球,伦纳德·琼斯和方阱)的过量熵,这些熵被限制在具有各种不同尺寸和流体壁相互作用的孔隙中。我们的主要发现是,在给定温度下,与过量熵作图时,密闭流体的自扩散性会塌陷到整体行为上。换句话说,“预测”约束对单粒子动力学的影响所需要的唯一信息是给定温度下的整体流体行为以及约束流体的过量熵。鉴于这些流体系统的整体行为众所周知,承压流体的过量熵很容易从经典密度泛函理论中估算出来,因此这应该被证明具有实用性;我们还证明了承压流体的自扩散系数约为相对于平均填充率(基于总体积而不是中心可访问体积)进行绘制时,将相应的散装数据折叠到数据上。对于诸如伦纳德·琼斯这样的连续相互作用势,计算有效堆积分数需要了解流体的数密度和与粒子间相互作用的排斥部分相关的温度相关的玻尔兹曼直径。我们提出了一种计算该有效直径的方法,该方法非常近似地将散装Lennard-Jones流体的自扩散系数的温度和密度相关数据折叠到硬球流体数据相对于流体的有效填充量上最后,我们发现,几个模型系统在其过冷状态下的自扩散率不仅与过量熵成指数关系,而且还与从该体的对相关函数获得的两体对过量熵的贡献有关。体液。后一种观察特别有趣,因为它提供了动力学和过冷液体平均结构顺序之间定量联系的直接证据。是否确实可以发现这样的连接是液体研究中长期存在的问题的一部分。

著录项

  • 作者

    Mittal, Jeetain.;

  • 作者单位

    The University of Texas at Austin.;

  • 授予单位 The University of Texas at Austin.;
  • 学科 Engineering Chemical.;Physics Condensed Matter.;Physics Fluid and Plasma.
  • 学位 Ph.D.
  • 年度 2007
  • 页码 154 p.
  • 总页数 154
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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