Guerrero-García G Iván, González-Tovar Enrique, Chávez-Páez Martín
Instituto de Física, Universidad Autónoma de San Luis Potosí, 78000 San Luis Potosí, S.L.P., México.
Phys Rev E Stat Nonlin Soft Matter Phys. 2009 Aug;80(2 Pt 1):021501. doi: 10.1103/PhysRevE.80.021501. Epub 2009 Aug 12.
Monte Carlo simulations of a spherical macroion, surrounded by a size-asymmetric electrolyte in the primitive model, were performed. We considered 1:1 and 2:2 salts with a size ratio of 2 (i.e., with coions twice the size of counterions), for several surface charge densities of the macrosphere. The radial distribution functions, electrostatic potential in all the space and at the Helmholtz surfaces, and integrated charge are reported. We compare these simulational data with original results obtained from the Ornstein-Zernike integral equation, supplemented by the hypernetted chain-hypernetted chain (HNC-HNC) and hypernetted chain-mean spherical approximation (HNC-MSA) closures, and with the corresponding calculations using the modified Gouy-Chapman and unequal-radius modified Gouy-Chapman theories. The HNC-HNC and HNC-MSA integral equations formalisms show good concordance with Monte Carlo "experiments," whereas the notable limitations of point-ion approaches are evidenced. Most importantly, the simulations confirm our previous theoretical predictions of the nondominance of the counterions in the size-asymmetric spherical electrical double layer [J. Chem. Phys. 123, 034703 (2005)], the appearance of anomalous curvatures at the outer Helmholtz plane, and the enhancement of the charge reversal and screening at high colloidal surface charge densities due to the ionic size asymmetry.
我们对原始模型中被尺寸不对称电解质包围的球形大离子进行了蒙特卡罗模拟。对于几种不同表面电荷密度的大球体,我们考虑了尺寸比为2的1:1和2:2盐(即,同离子大小是反离子的两倍)。报告了径向分布函数、整个空间以及亥姆霍兹表面处的静电势,还有积分电荷。我们将这些模拟数据与通过奥恩斯坦 - 泽尔尼克积分方程获得的原始结果进行比较,该方程由超网链 - 超网链(HNC - HNC)和超网链 - 平均球近似(HNC - MSA)封闭条件补充,同时也与使用修正的古伊 - 查普曼理论和不等半径修正的古伊 - 查普曼理论进行的相应计算结果进行比较。HNC - HNC和HNC - MSA积分方程形式与蒙特卡罗“实验”结果显示出良好的一致性,而点离子方法的显著局限性也得到了证明。最重要的是,模拟结果证实了我们之前的理论预测:在尺寸不对称的球形双电层中反离子并不占主导地位[《化学物理杂志》123, 034703 (2005)];在外亥姆霍兹平面出现异常曲率;以及由于离子尺寸不对称,在高胶体表面电荷密度下电荷反转和屏蔽作用增强。