Buyukdagli Sahin, Manghi Manoel, Palmeri John
UPS, Laboratoire de Physique Théorique (IRSAMC), Université de Toulouse, CNRS, LPT (IRSAMC), F-31062 Toulouse, France.
Phys Rev E Stat Nonlin Soft Matter Phys. 2010 Apr;81(4 Pt 1):041601. doi: 10.1103/PhysRevE.81.041601. Epub 2010 Apr 1.
A variational theory is developed to study electrolyte solutions, composed of interacting pointlike ions in a solvent, in the presence of dielectric discontinuities and charges at the boundaries. Three important and nonlinear electrostatic effects induced by these interfaces are taken into account: surface charge induced electrostatic field, solvation energies due to the ionic cloud, and image-charge repulsion. Our variational equations thus go beyond the mean-field theory, or weak coupling limit, where thermal fluctuations overcome electrostatic correlations, and allows one to reach the opposite strong coupling limit, where electrostatic interactions induced by interfaces dominate. The influence of salt concentration, ion valency, dielectric jumps, and surface charge is studied in two geometries. (i) A single neutral dielectric interface (e.g., air-water or electrolyte-membrane) with an asymmetric electrolyte. A charge separation and thus an electrostatic field get established due to the different image-charge repulsions for coions and counterions. Both charge distributions and surface tension are computed and compared to previous approximate calculations. For symmetric electrolyte solutions close to a charged surface, two zones are characterized. In the first one, in contact with the surface and with size proportional to the logarithm of the coupling parameter, strong image forces and strong coupling impose a total ion exclusion, while in the second zone the mean-field approach applies. (ii) A symmetric electrolyte confined between two dielectric interfaces as a simple model of ion rejection from nanopores in membranes. The competition between image-charge repulsion and attraction of counterions by the membrane charge is studied. For small surface charge, the counterion partition coefficient decreases with increasing pore size up to a critical pore size, contrary to neutral membranes. For larger pore sizes, the whole system behaves like a neutral pore. For strong coupling and small pore size, coion exclusion is total and the counterion partition coefficient is solely determined by global electroneutrality. A quantitative comparison is made with a previous approach, where image and surface charge effects were smeared out in the pore. It is shown that the variational method allows one to go beyond the constant Donnan potential approximation, with deviations stronger at high ion concentrations or small pore sizes. The prediction of the variational method is also compared with MC simulations and good agreement is observed.
发展了一种变分理论来研究电解质溶液,该溶液由溶剂中相互作用的点状离子组成,存在介电不连续性和边界电荷。考虑了这些界面引起的三种重要的非线性静电效应:表面电荷感应静电场、离子云引起的溶剂化能以及镜像电荷排斥。因此,我们的变分方程超越了平均场理论或弱耦合极限,在弱耦合极限中热涨落克服了静电关联,并且使人们能够达到相反的强耦合极限,在该极限中界面引起的静电相互作用占主导。在两种几何结构中研究了盐浓度、离子价、介电跃变和表面电荷的影响。(i) 具有不对称电解质的单个中性介电界面(例如,空气 - 水或电解质 - 膜)。由于同离子和反离子的镜像电荷排斥不同,会形成电荷分离并因此建立静电场。计算了电荷分布和表面张力,并与先前的近似计算进行了比较。对于靠近带电表面的对称电解质溶液,可分为两个区域。在第一个区域中,与表面接触且尺寸与耦合参数的对数成正比,强镜像力和强耦合导致完全离子排斥,而在第二个区域中适用平均场方法。(ii) 限制在两个介电界面之间的对称电解质,作为膜中纳米孔离子排斥的简单模型。研究了镜像电荷排斥与膜电荷对反离子吸引力之间的竞争。对于小表面电荷,反离子分配系数随着孔径增加到临界孔径而减小,这与中性膜相反。对于较大的孔径,整个系统的行为类似于中性孔。对于强耦合和小孔径,同离子完全排斥,反离子分配系数仅由整体电中性决定。与先前的方法进行了定量比较,在先前的方法中,镜像和表面电荷效应在孔中被模糊处理。结果表明,变分方法能够超越恒定唐南电位近似,在高离子浓度或小孔径下偏差更大。变分方法的预测结果也与蒙特卡罗模拟进行了比较,观察到了良好的一致性。