Yaroshchuk A E
Institute of Bio-Colloid Chemistry, National Academy of Sciences of Ukraine, Kiev.
Adv Colloid Interface Sci. 2000 Mar 31;85(2-3):193-230. doi: 10.1016/s0001-8686(99)00021-4.
Dielectric exclusion is caused by the interactions of ions with the bound electric charges induced by ions at interfaces between media of different dielectric constants. It is considered as one of mechanisms of nanofiltration. The transport properties of capillary model are expressed through ion distribution and diffusion coefficients. Due to local equilibrium the distribution coefficient is directly related to the excess solvation energy of ion. First, this energy is considered for single ions in single neutral pores in terms of pore size, ion charge, dielectric constants of solvent and membrane matrix and pore geometry. The dielectric exclusion from pores with closed geometry like circular cylinders is shown to be essentially stronger than that from pores with relatively open geometry like slits. Furthermore, the role of finite membrane porosity is analysed for the model of infinite slabs with alternating dielectric constants. The presence of other ions is accounted for within the scope of a mean-field approach, and the screening of dielectric exclusion is thus introduced and considered in some detail. A fixed electric charge is shown to cause additional screening. At the same time the dielectric exclusion makes the Donnan exclusion of ions stronger. Therefore the interaction between those two rejection mechanisms turns out to be non-trivial. Finally, the effect of solvent molecular structure is considered within the scope of non-local electrostatics. It is shown that the solvent non-locality typically results in somewhat stronger dielectric exclusion, however, its most important effect is slowing down the decline of dielectric exclusion with increasing bulk electrolyte concentration.
介电排斥是由离子与不同介电常数介质之间界面处离子诱导产生的束缚电荷相互作用引起的。它被认为是纳滤的机制之一。毛细管模型的传输特性通过离子分布和扩散系数来表示。由于局部平衡,分布系数与离子的过量溶剂化能直接相关。首先,从孔径、离子电荷、溶剂和膜基质的介电常数以及孔的几何形状等方面考虑单个中性孔中单个离子的这种能量。结果表明,具有封闭几何形状(如圆柱体)的孔的介电排斥比具有相对开放几何形状(如狭缝)的孔的介电排斥要强得多。此外,针对具有交替介电常数的无限平板模型分析了有限膜孔隙率的作用。在平均场方法的范围内考虑了其他离子的存在,从而引入并详细考虑了介电排斥的屏蔽作用。固定电荷会引起额外的屏蔽。同时,介电排斥使离子的唐南排斥更强。因此,这两种排斥机制之间的相互作用变得很复杂。最后,在非局部静电学的范围内考虑了溶剂分子结构的影响。结果表明,溶剂的非局部性通常会导致介电排斥稍强一些,然而,其最重要的影响是减缓了介电排斥随本体电解质浓度增加而下降的速度。