聚(ε-己内酯)/聚(苯乙烯-丙烯腈)共混物中带状球粒的形态

Chun Wang, R. Thomann, J. Kressler, Y. Thomann, K. Crämer, B. Stühn, P. Svoboda, T. Inoue
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引用次数: 9

摘要

采用光学显微镜、扫描电子显微镜、环境扫描电子显微镜和原子力显微镜以及小角x射线散射等方法研究了聚(ε-己内酯)与聚(苯乙烯-丙烯腈)共混物中带状球粒的存在。测量结果表明,片层被限制在从球粒中心沿径向周期性弯曲的原纤维中。原纤维在侧面也有规则的间距。在原子力显微镜下,可以观察到高锰酸蚀后的单片弯曲。通过温度跳变实验,利用偏振光显微镜可以直接观察到靠近球晶生长前沿的非晶态物质的富集。生长球晶表面排除的非晶态物质呈液滴状。这可能是弯曲过程开始的主要原因,因为结果是在球晶和周围熔体之间的界面处作用在生长的片上的应力分布不均匀。通过小角度x射线散射实验和显微观察,可以发现共混物中的非晶态物质存在于三个区域:(1)在片层之间,(2)在片层间区域被排除,但在球晶内,(3)非晶态物质含量高,可以从球晶中排除。球晶的带状周期性作为结晶温度的函数可以用两种模型来描述,要么基于(i)垂直于螺旋位错轴线的片层固有扭曲,要么基于(ii)非晶材料远离片层生长面扩散的依赖关系和结晶速率的温度依赖关系。这两种模型都在非常低的过冷温度下失效,接近于条带完全消失的温度。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Morphology of banded spherulites in poly(ε-caprolactone)/poly(styrene-ran-acrylonitrile) blends

The occurrence of banded spherulites in blends of poly(ε-caprolactone) with poly(styrene-ran-acrylonitrile) is studied by means of optical-, scanning electron-, environmental scanning electron-, and atomic force-microscopy as well as smallangle X-ray scattering. The measurements reveal that lamellae are confined in fibrils that bend periodically from the center of spherulites in a radial direction. The fibrils show also a regular spacing in the lateral direction. Single bent lamellae can be observed by atomic force microscopy after permanganic etching. The enrichment of amorphous material near to the growth front of the spherulites can be directly observed by polarized light microscopy after temperature jump experiments. The excluded amorphous material on the surface of the growing spherulites has the shape of droplets. This might be the main reason for the initiation of the bending process because the result is a non-uniform stress distribution acting on the growing lamellae at the interface between spherulites and the surrounding melt. The amorphous material of the blends can be found in three areas as observed by small-angle X-ray scattering experiments and microscopical methods: (i) between the lamellae, (ii) excluded from the interlamellar region but within the spherulite, and (iii) for high contents of non-crystallizable material, it can be excluded from the spherulite. The banding periodicity of spherulites as a function of the crystallization temperature can be described in terms of two models, based either (i) on the inherent twisting of lamellae perpendicular to the axis of a screw dislocation or (ii) on the dependence of the diffusion of amorphous material away from the growth front of lamellae and the temperature dependence of the rate of crystallization. Both models fail at very low supercoolings near to temperatures where the banding disappears completely.

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