Equilibrium Melting Temperature of the Hexagonal Crystals of Polybutene-1 and Its Copolymer

聚丁烯 层状结构 结晶学 材料科学 四方晶系 差示扫描量热法 小角X射线散射 Crystal(编程语言) 熔点 结晶 战术性 晶体结构 散射 热力学 化学 聚合物 聚合 复合材料 光学 物理 程序设计语言 计算机科学
作者
Yanan Qin,Ying Lu,V. M. Litvinov,Yongfeng Men
出处
期刊:Macromolecules [American Chemical Society]
卷期号:56 (12): 4705-4714 被引量:2
标识
DOI:10.1021/acs.macromol.3c00297
摘要

TheLamellar structures of form I in polymorphic isotactic polybutene-1 (iPB-1) and forms I and I′ in butene-1/ethylene random copolymer (iPB-1/C2) were investigated by studying their melting behavior using the combination of small-angle X-ray scattering (SAXS) and fast scanning chip calorimetry (FSC) techniques. Hexagonal form I was transformed from tetragonal form II obtained by crystallization of a homogeneous melt of iPB-1 and iPB-1/C2. Hexagonal form I′ was crystallized directly from a heterogeneous melt of iPB-1/C2. Despite the same hexagonal crystallographic structure, forms I and I′ have obviously distinct melting behaviors due to different ways of crystal formation. Well-defined linear dependences of the melting temperature against the reciprocal lamellar thickness were observed for forms I and I′ with frozen chain mobility in crystals. The slopes of the thus obtained melting lines for forms I and I′ are different. Their extrapolations to imaginary infinitely large lamellar thickness provide the equilibrium melting temperature Tm∞ for forms I and I′, which is associated with the stability of the lamellar crystals. In spite of crystal defects in form I′, a higher Tm∞ is observed for this form in iPB-1/C2 than Tm∞ for form I in both iPB-1 and iPB-1/C2. The difference in Tm∞ indicates a less perfect structure of form I crystal lamellae that is caused by the fragmentation of form II crystal lamellae during the polymorphic phase transition from form II to I. The lamellae broke into crystal blocks along the lamellar direction. The smaller lateral sizes of the fragmented lamellae clearly induce a decrease in the stability of crystals, as expressed in a lower Tm∞ for form I.
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