Matsuoka Keisuke, Yoshimura Tomokazu, Shikimoto Takashi, Hamada Juri, Yamawaki Mika, Honda Chikako, Endo Kazutoyo
Department of Physical Chemistry, Showa Pharmaceutical University, Higashi-Tamagawagakuen 3-3165, Machida, Tokyo 194-8543, Japan.
Langmuir. 2007 Oct 23;23(22):10990-4. doi: 10.1021/la701525c. Epub 2007 Sep 8.
The size and shape of novel partially fluorinated gemini surfactant 1,2-bis[dimethyl-(3-perfluoroalkyl-2-hydroxypropyl)ammonium]ethane bromide (CnFC3-2-C3CnF, where n=4, 6, and 8) were investigated in aqueous solution by means of light scattering and transmission electron microscopy (TEM). The sizes of these molecular aggregates changed with increasing carbon number of the alkyl chain and concentration. For example, the apparent hydrodynamic radius by dynamic light scattering was 18 nm at a concentration of cmcx5 for n=4, 115 nm at the cmcx15 for n=6, and 62 nm at the cmcx30 for n=8, at 298.2 K. The shapes of CnFC3-2-C3CnF aggregates drastically changed with the alkyl chain length; the aggregates were mainly in the form of large or irregular small aggregates (n=4), string-like aggregates (n=6), and vesicles (n=8). The bromide-ion activity was measured using a bromide-ion-selective electrode to determine the degree of counterion binding to the aggregates. The degree of counterion binding to aggregate was very small compared with that in the typical hydrogenated gemini surfactants. These results indicated that the small curvature of large aggregates was not influenced by an electrostatic repulsion between the cationic head groups in the case of the bulky molecular volume of fluorinated gemini surfactants.
通过光散射和透射电子显微镜(TEM)研究了新型部分氟化双子表面活性剂1,2-双[二甲基-(3-全氟烷基-2-羟丙基)铵]乙烷溴化物(CnFC3-2-C3CnF,其中n = 4、6和8)在水溶液中的尺寸和形状。这些分子聚集体的尺寸随烷基链碳原子数和浓度的增加而变化。例如,在298.2 K时,对于n = 4,在cmcx5浓度下通过动态光散射测得的表观流体动力学半径为18 nm;对于n = 6,在cmcx15浓度下为115 nm;对于n = 8,在cmcx30浓度下为62 nm。CnFC3-2-C3CnF聚集体的形状随烷基链长度急剧变化;聚集体主要为大的或不规则的小聚集体(n = 4)、串状聚集体(n = 6)和囊泡(n = 8)的形式。使用溴离子选择性电极测量溴离子活性,以确定抗衡离子与聚集体的结合程度。与典型的氢化双子表面活性剂相比,抗衡离子与聚集体的结合程度非常小。这些结果表明,在氟化双子表面活性剂分子体积较大的情况下,大聚集体的小曲率不受阳离子头基之间静电排斥的影响。