Department of Applied Physics and COMP Center of Excellence, Aalto University School of Science, P.O. Box 11000, FI-00076 Aalto, Espoo, Finland.
J Chem Phys. 2012 Feb 21;136(7):074901. doi: 10.1063/1.3684880.
A charged Yukawa liquid confined in a slit nanopore is studied in order to understand excluded volume effects in the interaction force between the pore walls. A previously developed self-consistent scheme [S. Buyukdagli, C. V. Achim, and T. Ala-Nissila, J. Stat. Mech. 2011, P05033] and a new simpler variational procedure that self-consistently couple image forces, surface charge induced electric field, and pore modified core interactions are used to this aim. For neutral pores, it is shown that with increasing pore size, the theory predicts a transition of the interplate pressure from an attractive to a strongly repulsive regime associated with an ionic packing state, an effect observed in previous Monte Carlo simulations for hard core charges. We also establish the mean-field theory of the model and show that for dielectrically homogeneous pores, the mean-field regime of the interaction between the walls corresponds to large pores of size d > 4 Å. The role of the range of core interactions in the ionic rejection and interplate pressure is thoroughly analyzed. We show that the physics of the system can be split into two screening regimes. The ionic packing effect takes place in the regime of moderately screened core interactions characterized with the bare screening parameter of the Yukawa potential b ≲ 3/l(B), where l(B) is the Bjerrum length. In the second regime of strongly screened core interactions b ≳ 3/l(B), solvation forces associated with these interactions positively contribute to the ionic rejection driven by electrostatic forces and enhance the magnitude of the attractive pressure. For weakly charged pores without a dielectric discontinuity, core interactions make a net repulsive contribution to the interplate force and also result in oscillatory pressure curves, whereas for intermediate surface charges, these interactions exclusively strengthen the external pressure, thereby reducing the magnitude of the net repulsive interplate force. The pronounced dependence of the interplate pressure and ionic partition coefficients on the magnitude and the range of core interactions indicates excluded volume effects as an important ion specificity and a non-negligible ingredient for the stability of macromolecules in electrolyte solutions.
为了理解纳米孔壁之间相互作用排斥体积效应,研究了受限在狭缝纳米孔中的带电的 Yukawa 液体。采用了先前开发的自洽方案 [S. Buyukdagli、C. V. Achim 和 T. Ala-Nissila,J. Stat. Mech. 2011,P05033] 和一种新的更简单的变分方法,该方法自洽地耦合了镜像力、表面电荷诱导电场和孔修正核相互作用。对于中性孔,研究表明,随着孔径的增大,理论预测出板间压力从吸引转变为强烈排斥,这与先前蒙特卡罗模拟硬核电荷的离子堆积状态有关。我们还建立了该模型的平均场理论,并表明对于介电均匀的孔,壁之间相互作用的平均场状态对应于较大的孔径 d > 4 Å。彻底分析了核相互作用范围对离子排斥和板间压力的影响。我们表明,系统的物理性质可以分为两个屏蔽区域。离子堆积效应发生在具有裸 Yukawa 势屏蔽参数 b ≲ 3/l(B)的中等屏蔽核相互作用区域中,其中 l(B)是 Bjerrum 长度。在强烈屏蔽核相互作用的第二个区域 b ≳ 3/l(B)中,与这些相互作用相关的溶剂化力对静电驱动的离子排斥产生积极贡献,并增强吸引力压力的大小。对于没有介电不连续的弱带电孔,核相互作用对板间力产生净排斥贡献,并且还导致压力曲线振荡,而对于中间表面电荷,这些相互作用仅增强外部压力,从而减小净排斥板间力的大小。板间压力和离子分配系数对核相互作用大小和范围的显著依赖表明排斥体积效应是离子特异性的重要因素,也是电解质溶液中大分子稳定性的重要组成部分。