Araki Taisuke, Oka Takayuki, Shioya Nobutaka, Hasegawa Takeshi
Laboratory of Chemistry for Functionalized Surfaces, Division of Environmental Chemistry, Institute for Chemical Research, Kyoto University, Gokasho, Uji, Kyoto, 611-0011, Japan.
Anal Sci. 2024 Sep;40(9):1723-1731. doi: 10.1007/s44211-024-00611-w. Epub 2024 Jun 14.
Phase diagram of polytetrafluoroethylene (PTFE) comprises four regions. Phases II and IV are characterized by twisted perfluoroalkyl (R) chains having different twisting rate of 13/6 and 15/7, respectively, while Phase III is characterized by a planer trans-zigzag molecular skeleton like a normal alkyl chain. These are confirmed by X-ray and electron diffraction and have already been established. Unlike these, Phase I is left an unresolved matter. This phase is complicated indeed and is not symbolized by a single molecular structure. At an ambient pressure, Phase I is the temperature region above 30 ºC (303 K), and the helical molecular structure is supposed to be gradually untwisted with an elevating temperature. This untwisting image is roughly suggested by the diffraction, neutron scattering, and thermal expansion techniques, but the conventional approaches have all experimental limitations because the untwisting accompanies disorder (or defect) in the twist along the chain. To explore the transition between two different helical structures of the R chain having disordered structures, vibrational spectroscopic techniques are expected to be an alternative approach. For infrared spectroscopy, for example, the twisting rate of the molecule is simply recognized as a degree of molecular symmetry. Here, we show that the band progression peaks of the CF symmetric stretching vibration mode are quite sensitive and useful for pursuing the molecular symmetry change in Phase I for both peak intensity and position using perfluoro-n-alkanes having different chain length covering both even and odd number of the CF groups.
聚四氟乙烯(PTFE)的相图包含四个区域。II相和IV相的特征分别是扭曲的全氟烷基(R)链,其扭曲率分别为13/6和15/7,而III相的特征是具有像正常烷基链一样的平面反式锯齿形分子骨架。这些已通过X射线和电子衍射得到证实且早已确定。与这些不同的是,I相仍是一个未解决的问题。这个相确实很复杂,不能用单一的分子结构来表征。在环境压力下,I相是温度高于30 ºC(303 K)的区域,并且随着温度升高,螺旋分子结构被认为会逐渐解开扭曲。衍射技术、中子散射技术和热膨胀技术大致表明了这种解开扭曲的图像,但传统方法都存在实验局限性,因为解开扭曲伴随着沿链扭曲的无序(或缺陷)。为了探索具有无序结构的R链的两种不同螺旋结构之间的转变,振动光谱技术有望成为一种替代方法。例如,对于红外光谱,分子的扭曲率可简单地视为分子对称程度。在此,我们表明,使用覆盖CF基团偶数和奇数的不同链长的全氟正构烷烃,CF对称伸缩振动模式的带进展峰对于追踪I相中分子对称变化的峰强度和位置都非常敏感且有用。