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1-十二烷基-3-甲基咪唑氟氢酸盐(C12MIm(FH)(n)F,n = 1.0-2.3)的相行为及其各向异性离子电导率作为离子液晶电解质。

Phase behavior of 1-dodecyl-3-methylimidazolium fluorohydrogenate salts (C12MIm(FH)(n)F, n = 1.0-2.3) and their anisotropic ionic conductivity as ionic liquid crystal electrolytes.

机构信息

Graduate School of Energy Science, Kyoto University, Yoshida, Kyoto 606-8501, Japan.

出版信息

J Phys Chem B. 2012 Aug 23;116(33):10106-12. doi: 10.1021/jp305228u. Epub 2012 Aug 10.

DOI:10.1021/jp305228u
PMID:22845709
Abstract

The effects of the HF composition, n, in 1-dodecyl-3-methylimidazolium fluorohydrogenate salts (C(12)MIm(FH)(n)F, n = 1.0-2.3) on their physicochemical and structural properties have been investigated using infrared spectroscopy, thermal analysis, polarized optical microscopy, X-ray diffraction, and anisotropic ionic conductivity measurements. The phase diagram of C(12)MIm(FH)(n)F (n vs transition temperature) suggests that C(12)MIm(FH)(n)F is a mixed crystal system that has a boundary around n = 1.9. For all compositions, a liquid crystalline mesophase with a smectic A interdigitated bilayer structure is observed. The temperature range of the mesophase decreases with increasing n value (from 61.8 °C for C(12)MIm(FH)(1.0)F to 37.0 °C for C(12)MIm(FH)(2.3)F). The layer spacing of the smectic structure decreases with increasing n value or increasing temperature. Two structural types with different layer spacings are observed in the crystalline phase (type I, 1.0 ≤ n ≤ 1.9, and type II, 1.9 ≤ n ≤ 2.3). Ionic conductivities parallel and perpendicular to the smectic layers (σ(||) and σ([perpendicular])) increase with increasing n value, whereas the anisotropy of the ionic conductivities (σ(||)/σ([perpendicular])) is independent of the n value, since the thickness of the insulating sheet formed by the dodecyl group remains nearly unchanged.

摘要

已经使用红外光谱、热分析、偏光显微镜、X 射线衍射和各向异性离子电导率测量研究了 HF 组成物 n 在 1-十二烷基-3-甲基咪唑氟氢酸盐(C(12)MIm(FH)(n)F,n = 1.0-2.3)中的物理化学和结构性质的影响。C(12)MIm(FH)(n)F(n 与转变温度的关系)相图表明,C(12)MIm(FH)(n)F 是一种混合晶体系统,在 n = 1.9 左右存在边界。对于所有组成物,均观察到具有层状 A 交错双层结构的液晶中间相。中间相的温度范围随 n 值的增加而降低(从 C(12)MIm(FH)(1.0)F 的 61.8°C 降至 C(12)MIm(FH)(2.3)F 的 37.0°C)。层状结构的层间距随 n 值或温度的增加而减小。在晶相(I 型,1.0 ≤ n ≤ 1.9 和 II 型,1.9 ≤ n ≤ 2.3)中观察到两种具有不同层间距的结构类型。平行和垂直于层状的离子电导率(σ(||)和 σ([perpendicular]))随 n 值的增加而增加,而离子电导率的各向异性(σ(||)/σ([perpendicular]))与 n 值无关,因为由十二烷基形成的绝缘片的厚度几乎保持不变。

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