Monte Carlo, density functional theory, and Poisson-Boltzmann theory study of the structure of an electrolyte near an electrode

被引:143
作者
Boda, D
Fawcett, WR
Henderson, D [1 ]
Sokolowski, S
机构
[1] Brigham Young Univ, Dept Chem & Biochem, Provo, UT 84602 USA
[2] Univ Veszprem, Dept Phys Chem, H-8201 Veszprem, Hungary
[3] Univ Calif Davis, Dept Chem, Davis, CA 95616 USA
[4] Marie Curie Sklodowska Univ, Dept Modeling Physicochem Properties, PL-20031 Lublin, Poland
关键词
D O I
10.1063/1.1464826
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Monte Carlo (MC) and density functional theory (DFT) results are reported for an electrolyte, consisting of charged hard spheres of diameter 3 Angstrom with the solvent modeled as a dielectric continuum, near a charged flat uniformly charged electrode. These results are more interesting than the earlier MC results of Torrie and Valleau [J. Chem. Phys. 73, 5807 (1980); J. Phys. Chem. 86, 3251 (1982)] for 4.25 Angstrom spheres because the popular Gouy-Chapman (GC) theory is less successful for this system. The DFT results are in good agreement with the MC results. Both the MC and DFT results show particularly interesting features when the counterions are divalent. For such divalent counterions, the diffuse layer potential passes through a maximum magnitude, then declines, and ultimately has a sign that is opposite to that of the electrode charge. The consequences of this behavior are discussed. In contrast, the well-known GC theory consistently overestimates the magnitude of the diffuse layer potential, does not have any unusual behavior, and is in poor agreement with the simulation results. (C) 2002 American Institute of Physics.
引用
收藏
页码:7170 / 7176
页数:7
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