Department of Chemical Engineering, Faculty of Chemistry, Sofia University, BG-1164 Sofia, Bulgaria.
Langmuir. 2010 Jan 19;26(2):915-23. doi: 10.1021/la902397w.
Micellar solutions of nonionic surfactants Brij 35 and Tween 20 are confined between two surfaces in a colloidal-probe atomic-force microscope (CP-AFM). The experimentally detected oscillatory forces due to the layer-by-layer expulsion of the micelles agree very well with the theoretical predictions for hard-sphere fluids. While the experiment gives parts of the stable branches of the force curve, the theoretical model allows reconstruction of the full oscillatory curve. Therewith, the strength and range of the ordering could be determined. The resulting aggregation number from the fits of the force curves for Brij 35 is close to 70 and exhibits a slight tendency to increase with the surfactant concentration. The last layer of micelles cannot be pressed out. The measured force-vs-distance curve has nonequilibrium portions, which represent "jumps" from one to another branch of the respective equilibrium oscillatory curve. In the case of Brij 35, at concentrations <150 mM spherical micelles are present and the oscillation period is close to the micelle diameter, slightly decreasing with the rise of concentration. For elongated micelles (at concentration 200 mM), no harmonic oscillations are observed anymore; instead, the period increases with the decrease of film thickness. In the case of Tween 20, the force oscillations are almost suppressed, which implies that the micelles of this surfactant are labile and are demolished by the hydrodynamic shear stresses due to the colloidal-probe motion. The comparison of the results for the two surfactants demonstrates that in some cases the micelles can be destroyed by the CP-AFM, but in other cases they can be stable and behave as rigid particles. This behavior correlates with the characteristic times of the slow micellar relaxation process for these surfactants.
胶束溶液中的非离子表面活性剂 Brij 35 和 Tween 20 被限制在胶体探针原子力显微镜 (CP-AFM) 的两个表面之间。由于胶束逐层排斥而产生的实验检测到的振荡力与硬球流体的理论预测非常吻合。虽然实验给出了力曲线稳定分支的一部分,但理论模型允许重建完整的振荡曲线。由此可以确定有序的强度和范围。从 Brij 35 的力曲线拟合得出的聚集数接近 70,并表现出随表面活性剂浓度略有增加的趋势。最后一层胶束无法被压出。测量的力-距离曲线具有非平衡部分,代表从一个分支到另一个分支的“跳跃”相应的平衡振荡曲线。在 Brij 35 的情况下,在浓度 <150 mM 时存在球形胶束,并且振荡周期接近胶束直径,略微随浓度升高而减小。对于伸长的胶束(在浓度 200 mM 时),不再观察到谐波振荡;相反,周期随膜厚度的减小而增加。在 Tween 20 的情况下,力振荡几乎被抑制,这意味着这种表面活性剂的胶束不稳定,并且由于胶体探针运动引起的流体动力剪切应力而被破坏。两种表面活性剂结果的比较表明,在某些情况下,CP-AFM 可以破坏胶束,但在其他情况下,它们可以稳定并表现为刚性颗粒。这种行为与这些表面活性剂的慢胶束松弛过程的特征时间相关。