Departments of Chemical & Biomolecular Engineering and Materials Science & Engineering, North Carolina State University , Raleigh, North Carolina 27695, United States.
Langmuir. 2017 Sep 12;33(36):8856-8868. doi: 10.1021/acs.langmuir.7b02017. Epub 2017 Aug 29.
Two polystyrene-b-poly(ethylene oxide) (PS-b-PEO) diblock copolymers differing in molecular mass (49 and 78 kDa) but possessing the same PEO cylindrical morphology are examined to elucidate their molecular dynamics. Of particular interest here is the molecular motion of the PEO blocks involved in the rigid amorphous fraction (RAF). An analysis of complementary thermal calorimetry and X-ray scattering data confirms the presence of microphase-separated morphology as well as semicrystalline structure in each copolymer. Molecular motion within the copolymer systems is monitored by dielectric and nuclear magnetic resonance spectroscopies. The results reported herein reveal the existence of two local Arrhenius-type processes attributed to the noncooperative local motion of PEO segments involved in fully amorphous and rigid amorphous PEO microphases. In both systems, two structural relaxations governed by glass-transition phenomena are identified and assigned to cooperative segmental motion in the fully amorphous phase (the α process) and the RAF (the α process). We measure the temperature dependence of the dynamics associated with all of the processes mentioned above and propose that these local processes are associated with corresponding cooperative segmental motion in both copolymer systems. In marked contrast to the thermal activation of the α process as discerned in both copolymers, the α process appears to be a sensitive probe of the copolymer nanostructure. That is, the copolymer with shorter PEO blocks exhibits more highly restricted cooperative dynamics of PEO segments in the RAF, which can be explained in terms of the greater constraint imposed by the glassy PS matrix on the PEO blocks comprising smaller cylindrical microdomains.
两种聚苯乙烯-聚(环氧乙烷)(PS-b-PEO)嵌段共聚物,其分子量不同(49 和 78 kDa),但具有相同的 PEO 圆柱形态,用于阐明其分子动力学。特别感兴趣的是涉及刚性无定形部分(RAF)的 PEO 嵌段的分子运动。互补热焓和 X 射线散射数据分析证实了每种共聚物中存在微相分离形态和半结晶结构。通过介电和核磁共振光谱监测共聚物体系内的分子运动。本文报道的结果表明,存在两种局部 Arrhenius 型过程,归因于完全无定形和刚性无定形 PEO 微相中涉及的 PEO 段的非协同局部运动。在这两种体系中,都识别并分配了两个由玻璃化转变现象控制的结构弛豫,这归因于完全无定形相(α 过程)和 RAF(α 过程)中的协同分子链段运动。我们测量了与上述所有过程相关的动力学的温度依赖性,并提出这些局部过程与两个共聚物体系中相应的协同分子链段运动有关。与在两种共聚物中都能识别出的α过程的热激活形成鲜明对比的是,α过程似乎是共聚物纳米结构的敏感探针。也就是说,具有较短 PEO 嵌段的共聚物在 RAF 中表现出 PEO 段的协同动力学受到更大的限制,这可以用玻璃态 PS 基质对包含较小圆柱微区的 PEO 嵌段施加的更大约束来解释。