Danov K D, Kralchevsky P A, Denkov N D, Ananthapadmanabhan K P, Lips A
Laboratory of Chemical Physics and Engineering, Faculty of Chemistry, University of Sofia, 1164 Sofia, Bulgaria.
Adv Colloid Interface Sci. 2006 Jan 31;119(1):17-33. doi: 10.1016/j.cis.2005.09.003. Epub 2005 Nov 23.
Here, we apply the detailed theoretical model of micellar kinetics from part 1 of this study to the case of surfactant adsorption at a quiescent interface, i.e., to the relaxation of surface tension and adsorption after a small initial perturbation. Our goal is to understand why for some surfactant solutions the surface tension relaxes as inverse-square-root of time, 1/t(1/2), but two different expressions for the characteristic relaxation time are applicable to different cases. In addition, our aim is to clarify why for other surfactant solutions the surface tension relaxes exponentially. For this goal, we carried out a computer modeling of the adsorption process, based on the general system of equations derived in part 1. This analysis reveals the existence of four different consecutive relaxation regimes (stages) for a given micellar solution: two exponential regimes and two inverse-square-root regimes, following one after another in alternating order. Experimentally, depending on the specific surfactant and method, one usually registers only one of these regimes. Therefore, to interpret properly the data, one has to identify which of these four kinetic regimes is observed in the given experiment. Our numerical results for the relaxation of the surface tension, micelle concentration and aggregation number are presented in the form of kinetic diagrams, which reveal the stages of the relaxation process. At low micelle concentrations, "rudimentary" kinetic diagrams could be observed, which are characterized by merging of some stages. Thus, the theoretical modeling reveals a general and physically rich picture of the adsorption process. To facilitate the interpretation of experimental data, we have derived convenient theoretical expressions for the time dependence of surface tension and adsorption in each of the four regimes.
在此,我们将本研究第一部分中详细的胶束动力学理论模型应用于表面活性剂在静态界面的吸附情况,即小初始扰动后的表面张力松弛和吸附过程。我们的目标是理解为何对于某些表面活性剂溶液,表面张力以时间的平方根倒数,即1/t(1/2)的形式松弛,但对于不同情况,特征松弛时间有两种不同的表达式适用。此外,我们的目的是阐明为何对于其他表面活性剂溶液,表面张力呈指数松弛。为实现这一目标,我们基于第一部分推导的通用方程组对吸附过程进行了计算机建模。该分析揭示了给定胶束溶液存在四种不同的连续松弛机制(阶段):两种指数机制和两种平方根倒数机制,交替依次出现。在实验中,根据具体的表面活性剂和方法,通常只能记录到这些机制中的一种。因此,为了正确解释数据,必须确定在给定实验中观察到的是这四种动力学机制中的哪一种。我们给出了表面张力、胶束浓度和聚集数松弛的数值结果,以动力学图的形式呈现,这些图揭示了松弛过程的各个阶段。在低胶束浓度下,可以观察到“基本的”动力学图,其特征是某些阶段合并。因此,理论建模揭示了吸附过程的一个普遍且物理内容丰富的图景。为便于解释实验数据,我们推导了四种机制中每种机制下表面张力和吸附随时间变化的方便的理论表达式。