Lima Eduardo R A, Tavares Frederico W, Biscaia Evaristo C
Programa de Engenharia Química, COPPE, Universidade Federal do Rio de Janeiro, Rio de Janeiro, CEP 21941-972, RJ-Brazil.
Phys Chem Chem Phys. 2007 Jun 28;9(24):3174-80. doi: 10.1039/b701170a. Epub 2007 May 15.
The double layer forces between spherical colloidal particles, according to the Poisson-Boltzmann (PB) equation, have been accurately calculated in the literature. The classical PB equation takes into account only the electrostatic interactions, which play a significant role in colloid science. However, there are at, and above, biological salt concentrations other non-electrostatic ion specific forces acting that are ignored in such modelling. In this paper, the electrostatic potential profile and the concentration profile of co-ions and counterions near charged surfaces are calculated. These results are obtained by solving the classical PB equation and a modified PB equation in bispherical coordinates, taking into account the van der Waals dispersion interactions between the ions and both surfaces. Once the electrostatic potential is known we calculate the double layer force between two charged spheres. This is the first paper that solves the modified PB equation in bispherical coordinates. It is also the first time that the finite volume method is used to solve the PB equation in bispherical coordinates. This method divides the calculation domain into a certain number of sub-domains, where the physical law of conservation is valid, and can be readily implemented. The finite volume method is implemented for several geometries and when it is applied to solve PB equations presents low computational cost. The proposed method was validated by comparing the numerical results for the classical PB calculations with previous results reported in the literature. New numerical results using the modified PB equation successfully predicted the ion specificity commonly observed experimentally.
根据泊松-玻尔兹曼(PB)方程,文献中已精确计算了球形胶体颗粒之间的双层力。经典的PB方程仅考虑了静电相互作用,而静电相互作用在胶体科学中起着重要作用。然而,在生物盐浓度及以上时,此类模型忽略了其他非静电离子特异性作用力。本文计算了带电表面附近同离子和反离子的静电势分布和浓度分布。这些结果是通过在双球坐标系中求解经典PB方程和修正的PB方程得到的,其中考虑了离子与两个表面之间的范德华色散相互作用。一旦知道了静电势,我们就可以计算两个带电球体之间的双层力。这是第一篇在双球坐标系中求解修正PB方程的论文。这也是首次使用有限体积法在双球坐标系中求解PB方程。该方法将计算域划分为一定数量的子域,在这些子域中物理守恒定律成立,并且易于实现。有限体积法针对几种几何形状进行了实现,并且在应用于求解PB方程时具有较低的计算成本。通过将经典PB计算的数值结果与文献中报道的先前结果进行比较,验证了所提出的方法。使用修正PB方程得到的新数值结果成功地预测了实验中常见的离子特异性。