Shklovskii B I
Theoretical Physics Institute, University of Minnesota, 116 Church Street Southeast, Minneapolis, Minnesota 55455, USA.
Phys Rev E Stat Phys Plasmas Fluids Relat Interdiscip Topics. 1999 Nov;60(5 Pt B):5802-11. doi: 10.1103/physreve.60.5802.
Screening of a strongly charged macroion by multivalent counterions is considered. It is shown that counterions form a strongly correlated liquid at the surface of the macroion. Cohesive energy of this liquid leads to additional attraction of counterions to the surface, which is absent in conventional solutions of the Poisson-Boltzmann equation. Away from the surface this attraction can be taken into account by a new boundary condition for the concentration of counterions near the surface. The Poisson-Boltzmann equation is solved with this boundary condition for a charged flat surface, a cylinder, and a sphere. In all three cases, screening is much stronger than in the conventional approach. At some critical exponentially small concentration of multivalent counterions in the solution, they totally neutralize the surface charge at small distances from the surface. At larger concentrations they invert the sign of the net macroion charge. The absolute value of the inverted charge density can be as large as 20% of the bare one. In particular, for a cylindrical macroion it is shown that for screening by multivalent counterions, predictions of the Onsager-Manning theory are quantitatively incorrect. The net charge density of the cylinder is smaller than their theory predicts and inverts the sign with a growing concentration of counterions. Moreover, the condensation loses its universality and the net charge linear density depends on the bare one.
考虑了多价抗衡离子对强带电大离子的筛选作用。结果表明,抗衡离子在大离子表面形成强关联液体。该液体的内聚能导致抗衡离子对表面产生额外的吸引力,这在泊松 - 玻尔兹曼方程的传统解中是不存在的。在远离表面处,这种吸引力可通过表面附近抗衡离子浓度的新边界条件来考虑。针对带电平面、圆柱体和球体,在该边界条件下求解泊松 - 玻尔兹曼方程。在所有这三种情况下,筛选作用都比传统方法强得多。在溶液中多价抗衡离子处于某个临界指数小浓度时,它们在距表面小距离处完全中和表面电荷。在更高浓度时,它们使大离子净电荷的符号反转。反转后的电荷密度绝对值可高达裸电荷密度的20%。特别是,对于圆柱形大离子,结果表明对于多价抗衡离子的筛选,昂萨格 - 曼宁理论的预测在定量上是不正确的。圆柱体的净电荷密度小于该理论的预测值,并且随着抗衡离子浓度的增加而反转符号。此外,凝聚失去了其普遍性,净电荷线密度取决于裸电荷线密度。