Monte-Carlo Simulation of the Ionic Transport of Electrolyte Solutions at High Concentrations Based on the Pseudo-Lattice Model. Issue 7 (1st January 2016)

• Record Type: Journal Article
• Authors: Ozaki, Hiroyuki; Kuratani, Kentaro; Kiyobayashi, Tetsu
• Is Part Of: Journal of the Electrochemical Society. Volume 163:Issue 7(2016)
• Page Start: H576
• Page End: H583
• Publication Date: 2016-01-01
• Subjects: Conductance -- Lattice liquid model -- Random walk -- Transport phenomena; Electrochemistry -- Periodicals; 541.3705
• DOI: 10.1149/2.0941607jes
• Languages: English
• ISSNs: 0013-4651

Abstract

Abstract : The theoretical understanding of the ionic transport in electrolyte solutions is not yet well-established at high concentrations, such as at C /mol · L − 1 > 1. In our present study, two transport phenomena—self-diffusion and ionic conduction—of the electrolyte solution at high concentrations (roughly 0.05 ⩽ C /mol · L − 1 ⩽ 3) are computationally simulated by a kinetic Monte-Carlo scheme. A "swap mechanism" in the three-dimensional pseudo-lattice is proposed to model the movement of ions and solvent, in which only the nearest-neighbor interaction is considered. The energy difference between the before- and after-swap states, based on which the stochastic Monte-Carlo process occurs, is found to be expressed in only two energetic terms; the coulombic repulsion between ions with the identical sign, + ε ii, and the heat of dissolution of the ionic crystal, Δ diss H . The self-diffusion coefficients of both ions and solvent decrease with the increase in the ionic concentration, which qualitatively agree with the experimental observation. The asymmetric bell-shape of the specific conductivity, σ, principally originates from the coulombic repulsion. The ionic concentration at which the maximum σ occurs well coincides with that of the experimentally observed results. The Δ diss H -dependency reveals that, ceteris paribus, σ marks the highest at around − 2 k T < Δ diss H < 0, out of the range of which σ is attenuated by either the ion-ion or ion-solvent interaction. Finally, the limitations in the model are addressed.