蒙脱土填充聚酯薄膜的界面效应

L. Sahu, N. D'Souza
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引用次数: 3

摘要

薄支撑和非支撑薄膜的行为已被证明与体聚合物不同。另外,高表面积填料,如蒙脱土层状硅酸盐(MLS),可以改善性能。在这项研究中,我们研究了聚乙烯对苯二甲酸乙二醇酯(PET)薄膜与MLS。用椭偏仪测定了其热膨胀率和玻璃化转变温度。结果表明,随着MLS浓度的增加,薄膜和厚膜平台的玻璃化转变下降。对于中等厚度,发现MLS聚合物界面对特征长度的影响不大。随着MLS存在的增加,液层厚度减小。大约60纳米。从实验结果中,他们观察到随着烷基链长度从甲基增加到正辛烷基,薄膜的tg和CTE与体膜的偏差显著减小。他们认为溶剂的加入增加了协同段的长度。利用聚合物物理学(分子迁移率)和聚合物混溶性(相互作用)的结合,Pham和Green(10)通过三层模型解释了相互矛盾的T - g -厚度结果。在衬底旁边,聚合物链弯曲和折叠导致密度更高,迁移率降低和玻璃化转变温度更高。在自由表面,预期密度更低,迁移率更高,玻璃化转变更低。高迁移率是由于诸如解纠缠、约束效应或链端偏析等熵效应导致弛豫时间的增加。在自由表面和靠近基体的区域之间,聚合物链具有中等的迁移率。当衬底-聚合物相互作用不相互作用时,衬底层的厚度低于衬底-聚合物相互作用高度时的厚度。其结果是,非相互作用涂层中的中间区域比相互作用体系中的中间区域厚。在前者中,玻璃化转变随膜厚的增加而增加。自由表面迁移率占主导地位,导致tg随膜厚的减小而减小。在衬底-聚合物发生正相互作用的薄膜中,由于迁移率较低的层占主导地位,玻璃化转变随着薄膜厚度的增加而减少。
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Interfacial Effects in Montmorillonite Filled Polyester Thin Films
The behavior of thin supported and non-supported films has been shown to be distinct from the bulk polymer. Separately, high surface area fillers such as montomorillonite layered silicates (MLS) result in improved properties. In this study, we investigate thin films of polyethylene terephthalate (PET) with MLS. The thermal expansivity and glass transi- tion temperature (T g ) were determined using ellipsometry. The results show that with increasing MLS concentration, the glass transition drops for the thin and thick film plateaus. For intermediate thicknesses, a modest influence of the MLS polymer interface on the characteristic length is found. The liquid layer thickness decreases with increased MLS presence. approximately 60 nm. From the experimental results they observed the significant reduction in deviation in T g and CTE of thin film from bulk film as the alkyl chain length was increased from methyl to n-octyl. They attributed to increase in the cooperative segmental length with the addi- tion of solvent. Utilizing a combination of polymer physics (molecular mobility) and polymer miscibility (interactions), Pham and Green (10) explain the contradictory T g -thickness results via a three layer model. Next to a substrate, the poly- mer chains bend and fold over leading to higher density, decreased mobility and higher glass transition temperatures. At the free surface, lower density, higher mobility and lower glass transitions are to be expected. The higher mobility re- sults from an increase in relaxation time due to entropic ef- fects such as disentanglements, confinement effects or by chain-end segregation. Between the free surface and the re- gion close to the substrate, polymer chains have intermediate mobility. When the substrate-polymer interaction is non in- teracting, the thickness of the substrate layer is lower than when there is a high degree of substrate-polymer interaction. The consequence is that the intermediate region in a non- interacting coating is thicker than in an interacting system. In the former the glass transition increases with increasing film thickness. The free surface mobility dominates leading to decreased T g 's with decreasing film thickness. In a film where positive substrate-polymer interactions occur, the glass transition decreases with increasing film thickness as the lower mobility layer dominates.
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