Theoretical Chemistry Section, Chemistry Group, Bhabha Atomic Research Centre, Mumbai 400 085, India.
J Phys Chem B. 2011 Sep 22;115(37):10903-10. doi: 10.1021/jp203779t. Epub 2011 Aug 25.
The effect of ionic size on the diffuse layer characteristics of a cylindrical electric double layer is studied using density functional theory and Monte Carlo simulations for the restricted primitive model and solvent primitive model. The double layer is comprised of an infinitely long, rigid, impenetrable charged cylinder also referred to as the polyion, located at the center of a cylindrical cell containing the electrolyte, which is composed of charged hard spheres and the solvent molecules as neutral hard spheres (in the case of the solvent primitive model). The diameters of all the hard spheres are taken to be the same. The theory is based on a partially perturbative scheme, where perturbation is used to approximate the ionic interactions and the hard sphere contribution is treated within the weighted density approach. The Monte Carlo simulations are performed in the canonical ensemble. The zeta potential profiles as a function of the polyion surface charge density are presented for cylindrical double layers at different ionic concentrations, ionic valences, and different hard sphere (ionic and the solvent) diameters of 2, 3, and 4 Å. The theory agrees quite well with the simulation results for a wide range of system parametric conditions and is capable of showing the maximum and minimum in the zeta potential value for systems having divalent counterions. The steric effects due to the presence of solvent molecules play a major role in characterizing the zeta potential and the ionic density profiles. A noticeable change in the concavity of the zeta potential plots with increasing particle size at very low concentrations of monovalent electrolytes is suggestive of the occurrence of infinite differential capacitance for such systems.
使用密度泛函理论和蒙特卡罗模拟对受限原始模型和溶剂原始模型研究了离子大小对圆柱形电双层扩散层特性的影响。双层由一个无限长、刚性、不可穿透的带电圆柱组成,也称为聚离子,位于包含电解质的圆柱形单元的中心,电解质由带电硬球和溶剂分子组成(在溶剂原始模型的情况下)。所有硬球的直径都相同。该理论基于部分微扰方案,其中微扰用于近似离子相互作用,硬球贡献在加权密度方法内进行处理。蒙特卡罗模拟在正则系综中进行。给出了不同离子浓度、离子价和不同硬球(离子和溶剂)直径为 2、3 和 4 Å 的圆柱形双层中 zeta 势随聚离子表面电荷密度的分布。该理论与模拟结果在广泛的系统参数条件下非常吻合,并且能够显示具有二价抗衡离子的系统中 zeta 势值的最大值和最小值。由于溶剂分子的存在而产生的空间位阻效应在表征 zeta 势和离子密度分布方面起着重要作用。在单价电解质的非常低浓度下,zeta 势图的凹度随粒径的增加而显著变化,这表明此类系统存在无限微分电容。