Department of Chemistry, Faculty of Sciences, Kyushu University, Fukuoka 812-8581, Japan.
J Phys Chem B. 2011 Jan 27;115(3):471-7. doi: 10.1021/jp1083696. Epub 2010 Dec 30.
The surface tension γ of the aqueous solution of 1H,1H,6H,6H-perfluorohexane-1,6-diol (FC₆diol) and 1H,1H,8H,8H-perfluorooctane-1,8-diol (FC8diol) mixtures was measured as a function of total molality m and composition of FC₈diol in the mixture X₂ at 293.15 K under atmospheric pressure. The γ vs m curves except at X₂ = 0 and 0.05 have a distinct break point due to a phase transition in the adsorbed film. The surface pressure π vs mean area per adsorbed molecule A curves consist of two parts connected by a discontinuous change. The curve was almost vertical just below the phase transition, and the variation of the A value with film composition X(2)(H) was linear corresponding to the fact that FC₆diol and FC₈diol molecules orient parallel to the surface and are densely packed with the same areas of individual condensed films. Above the phase transition, the A value further decreases to around 0.12-0.19 nm² which is much smaller than the cross-sectional area of the fluorocarbon chain, indicating the multilayer formation at the surface. The phase diagram of adsorption (PDA) in the condensed film showed that the m vs film composition X(2)(H) curve is almost linear and the excess Gibbs energy of adsorption g(HE)/RT is at most 0.01, manifesting the ideal mixing of molecules. This is in contrast to a positive deviation (g(HE)/RT ~0.12) observed in the condensed film of the mixture of 1H,1H,2H,2H-perfluorodecanol (FC₁₀OH) and 1H,1H,2H,2H-perfluorododecanol (FC₁₂OH) with perpendicular molecular orientation. The loss of dispersion interaction between different species having different chain lengths is more appreciable in the perpendicular condensed films and thus leads to less miscibility of FC₁₀OH and FC₁₂OH. In the parallel condensed film, on the other hand, FC₆diol and FC₈diol molecules can arrange their position as close as possible to minimize the loss of dispersion interaction. The X(2)(H) value in the multilayer is close to unity, and thus, the multilayer consists of almost FC₈diol molecules which form a multilayer in the single-component system. Furthermore, the condensed monolayer-multilayer phase transition was accompanied by a large increase in surface density of FC₈diol and a small decrease in that of FC₆diol, indicating that FC₈diol molecules pile preferentially to form a multilayer.
在 293.15 K 及大气压下,测定了 1H,1H,6H,6H-全氟己烷-1,6-二醇(FC₆二醇)和 1H,1H,8H,8H-全氟辛烷-1,8-二醇(FC8 二醇)混合物水溶液的表面张力γ与总克分子浓度 m 和混合物中 FC8 二醇的组成 X₂的关系。由于吸附膜中的相转变,γ与 m 的曲线除了在 X₂=0 和 0.05 处外,都有明显的转折点。表面压π与每个吸附分子的平均面积 A 的曲线由两个部分组成,通过不连续的变化连接。在相转变的下方,曲线几乎是垂直的,A 值随膜组成 X(2)(H)的变化是线性的,这对应于 FC₆二醇和 FC8 二醇分子平行于表面取向并且以相同的单个凝聚膜的面积密集排列的事实。在相转变之上,A 值进一步减小到约 0.12-0.19nm²,这远小于氟碳链的截面积,表明表面上形成了多层。凝聚膜中的吸附相图(PDA)表明,m 与膜组成 X(2)(H)的曲线几乎是线性的,吸附的过剩吉布斯自由能 g(HE)/RT 最大为 0.01,表明分子的理想混合。这与在具有垂直分子取向的 1H,1H,2H,2H-全氟癸醇(FC₁₀OH)和 1H,1H,2H,2H-全氟十二醇(FC₁₂OH)混合物的凝聚膜中观察到的正偏差(g(HE)/RT~0.12)形成对比。在具有不同链长的不同物种之间的色散相互作用的损失在垂直凝聚膜中更为明显,因此导致 FC₁₀OH 和 FC₁₂OH 的混溶性降低。另一方面,在平行凝聚膜中,FC₆二醇和 FC₈二醇分子可以将其位置排列得尽可能接近,以最小化色散相互作用的损失。多层中的 X(2)(H)值接近 1,因此,多层几乎由 FC₈二醇分子组成,它们在单一组分系统中形成多层。此外,凝聚单层-多层相变伴随着 FC₈二醇表面密度的大幅增加和 FC₆二醇表面密度的略有下降,表明 FC₈二醇分子优先堆积形成多层。