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Quantification of organoclay dispersion and lamellar morphology in poly(propylene)–clay nanocomposites with small angle X-ray scattering

机译:小角度X射线散射对聚丙烯-粘土纳米复合材料中有机粘土分散体和层状形态的定量

摘要

Intensity profiles of small angle X-ray scattering (SAXS) curves were analyzed to simultaneously gain quantitative information on nanoclay dispersion as well as lamellar ordering in polypropylene–clay nanocomposites. Different types of PP nanocomposites prepared with PP homopolymer (HPP), random propylene–ethylene copolymer (RCP) and a high impact polypropylene–ethylene propylene rubber (ICP) were analyzed. Various one-dimensional models for stacked structures were applied on Lorentz corrected SAXS spectra to derive long period, thicknesses of alternating high and low electron density layers and their distributions, and the number of stacks for both nanoclay and PP lamellae. We applied a mixed thickness distribution model comprising combined Gaussian and exponential for a simple stack of finite thickness, which was found to explain the experimental data better for both nanoclay tactoids and lamellar stacks, compared to simple Gaussian and exponential thickness distributions. Long period X and number of stacks N were derived as important parameters signifying changes in levels of nanoclay exfoliation in PP. Among the three types of polypropylenes studied, better nanoclay exfoliation was obtained for the high impact ICP grade compared to HPP and RCP. Complete exfoliation of nanoclay was achieved in ICP matrix, employing a masterbatch processing route. Moreover, role of nanoclay as a γ nucleating agent was evident from small and wide angle X-ray analyses, and was seen strongly in RCP. Changes in lamellar structure of PP as a result of nanoclay incorporation, double population consisting of both α and γ polytypes in the nanocomposites from that of a primarily α population in neat polymer matrices, were also analyzed in detail with the mixed thickness distribution model, thereby demonstrating its usefulness.
机译:分析了小角X射线散射(SAXS)曲线的强度曲线,以同时获得有关纳米粘土分散体以及聚丙烯-粘土纳米复合材料中层状有序性的定量信息。分析了由PP均聚物(HPP),无规丙烯-乙烯共聚物(RCP)和高抗冲聚丙烯-乙烯丙烯橡胶(ICP)制备的不同类型的PP纳米复合材料。在Lorentz校正的SAXS光谱上应用了各种堆叠结构的一维模型,以得出长周期,交替的高和低电子密度层的厚度及其分布以及纳米粘土和PP薄片的堆叠数。我们对有限厚度的简单堆栈应用了包含高斯和指数组合的混合厚度分布模型,与简单的高斯和指数厚度分布相比,发现该模型可以更好地解释纳米粘土触针和层状堆栈的实验数据。得出了长周期X和堆积数N作为表示PP中纳米粘土剥落水平变化的重要参数。在所研究的三种类型的聚丙烯中,与HPP和RCP相比,高抗冲ICP级的纳米粘土剥离效果更好。采用母料加工路线,在ICP基质中实现了纳米粘土的完全剥离。此外,从小角度和广角X射线分析中可以明显看出纳米粘土作为γ成核剂的作用,并且在RCP中得到了强烈的体现。还通过混合厚度分布模型详细分析了纳米粘土掺入导致PP的层状结构变化,由纳米复合物中的α和γ多型组成的双种群与纯聚合物基质中的主要α种群的双种群。证明其有用性。

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