Graduate School of Science and Engineering, Yamagata University , 1-4-12 Kojirakawa-machi, Yamagata 990-8560, Japan.
Institute for Multidisciplinary Research for Advanced Materials, Tohoku University , 2-1-1 Katahira, Aoba-ku, Sendai 980-8577, Japan.
Langmuir. 2017 Nov 14;33(45):12897-12902. doi: 10.1021/acs.langmuir.7b03160. Epub 2017 Nov 1.
The effect of the content of acid groups on the proton conductivity at the interlayer of polymer-nanosheet assemblies was investigated. For that purpose, amphiphilic poly(N-dodecylacrylamide-co-acrylic acid) copolymers [p(DDA/AA)] with varying contents of AA were synthesized by free radical polymerization. Surface pressure (π)-area (A) isotherms of these copolymers indicated that stable polymer monolayers are formed at the air/water interface for AA mole fraction (n) ≤ 0.49. In all cases, a uniform dispersion of the AA groups in the polymer monolayer was observed. Subsequently, polymer monolayers were transferred onto solid substrates using the Langmuir-Blodgett (LB) technique. X-ray diffraction (XRD) analyses of the multilayer films showed strong Bragg diffraction peaks, suggesting a highly uniform lamellar structure for the multilayer films. The proton conductivity of the multilayer films parallel to the direction of the layer planes were measured by impedance spectroscopy, which revealed that the conductivity increased with increasing values of n. Activation energies for proton conduction of ∼0.3 and 0.42 eV were observed for n ≥ 0.32 and n = 0.07, respectively. Interestingly, the proton conductivity of a multilayer film with n = 0.19 did not follow the Arrhenius equation. These results were interpreted in terms of the average distance between the AA groups (l), and it was concluded that, for n ≥ 0.32, an advanced 2D hydrogen bonding network was formed, while for n = 0.07, l is too long to form such hydrogen bonding networks. The l for n = 0.19 is intermediate to these extremes, resulting in the formation of hydrogen bonding networks at low temperatures, and disruption of these networks at high temperatures due to thermally induced motion. These results indicate that a high proton conductivity with low activation energy can be achieved, even under weakly acidic conditions, by arranging the acid groups at an optimal distance.
研究了酸基团含量对聚合物-纳米片组装体层间质子传导的影响。为此,通过自由基聚合合成了具有不同 AA 含量的两亲性聚(N-十二烷基丙烯酰胺-共-丙烯酸)共聚物 [p(DDA/AA)]。这些共聚物的表面压(π)-面积(A)等温线表明,当 AA 摩尔分数(n)≤0.49 时,在空气/水界面形成稳定的聚合物单分子层。在所有情况下,都观察到 AA 基团在聚合物单层中的均匀分散。随后,使用 Langmuir-Blodgett (LB) 技术将聚合物单层转移到固体基底上。多层膜的 X 射线衍射 (XRD) 分析表明,多层膜具有高度均匀的层状结构,出现强布拉格衍射峰。通过阻抗谱法测量平行于层平面方向的多层膜的质子电导率,结果表明电导率随 n 值的增加而增加。对于 n≥0.32 和 n=0.07,观察到质子传导的活化能分别为 0.3 和 0.42 eV。有趣的是,n=0.19 的多层膜的质子电导率不遵循阿仑尼乌斯方程。这些结果根据 AA 基团之间的平均距离(l)进行解释,结论是对于 n≥0.32,形成了先进的 2D 氢键网络,而对于 n=0.07,l 太长而无法形成这种氢键网络。n=0.19 的 l 处于这两个极端之间,导致在低温下形成氢键网络,以及由于热诱导运动在高温下破坏这些网络。这些结果表明,即使在弱酸性条件下,通过将酸基团排列在最佳距离,可以实现具有低活化能的高质子电导率。