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电荷不对称硬球离子流体中的临界现象。

Criticality in charge-asymmetric hard-sphere ionic fluids.

作者信息

Aqua Jean-Noël, Banerjee Shubho, Fisher Michael E

机构信息

Institute for Physical Science and Technology, University of Maryland, College Park, Maryland 20742 USA.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2005 Oct;72(4 Pt 1):041501. doi: 10.1103/PhysRevE.72.041501. Epub 2005 Oct 4.

DOI:10.1103/PhysRevE.72.041501
PMID:16383379
Abstract

Phase separation and criticality are analyzed in z:1 charge-asymmetric ionic fluids of equisized hard spheres by generalizing the Debye-Hückel approach combined with ionic association, cluster solvation by charged ions, and hard-core interactions, following lines developed by Fisher and Levin for the 1:1 case (i.e., the restricted primitive model). Explicit analytical calculations for 2:1 and 3:1 systems account for ionic association into dimers, trimers, and tetramers and subsequent multipolar cluster solvation. The reduced critical temperatures, Tc* (normalized by z), decrease with charge asymmetry, while the critical densities increase rapidly with . The results compare favorably with simulations and represent a distinct improvement over all current theories such as the mean spherical approximation, symmetric Poisson-Boltzmann theory, etc. For z not equal to 1, the interphase Galvani (or absolute electrostatic) potential difference, Deltaphi(T), between coexisting liquid and vapor phases is calculated and found to vanish as absolute value (T-Tc) beta when T-->Tc-with, since our approximations are classical, beta = (1/2). Above Tc, the compressibility maxima and so-called k-inflection loci (which aid the fast and accurate determination of the critical parameters) are found to exhibit a strong z dependence.

摘要

通过推广德拜 - 休克尔方法,并结合离子缔合、带电离子的簇溶剂化以及硬核相互作用,对大小均等的硬球构成的z:1电荷不对称离子流体中的相分离和临界性进行了分析,遵循费舍尔和莱文针对1:1情况(即限制原始模型)所发展的思路。对2:1和3:1体系进行的显式解析计算考虑了离子缔合成二聚体、三聚体和四聚体以及随后的多极簇溶剂化。约化临界温度(T_c^*)(以z归一化)随电荷不对称性降低,而临界密度随[此处原文缺失相关内容]迅速增加。结果与模拟结果吻合良好,并且相较于诸如平均球近似、对称泊松 - 玻尔兹曼理论等所有当前理论有显著改进。对于(z\neq1)的情况,计算了共存液相和汽相之间的相间伽伐尼(或绝对静电)电位差(\Delta\phi(T)),发现当(T\rightarrow T_c^-)时,其绝对值以((T - T_c)^{\beta})的形式消失,由于我们的近似是经典的,所以(\beta=(1/2))。在(T_c)之上,发现压缩率最大值以及所谓的(k)拐点轨迹(有助于快速准确地确定临界参数)呈现出强烈的(z)依赖性。

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