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STRUCTURE DEVELOPMENT IN SEMICRYSTALLINE DIBLOCK COPOLYMERS CRYSTALLIZING FROM THE ORDERED MELT

机译:有序熔体结晶的半结晶二嵌段共聚物的结构发展

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Time-resolved simultaneous synchrotron small-angle and wide-angle X-ray scattering (SAXS and WAXS) and DSC experiments have been performed on poly(ethylene)-poly(ethylethylene) and poly(ethylene)-poly(ethylene-propylene) diblock copolymers quenched from melts with lamellar and hexagonal-packed cylinder structures. We find that the original microphase-separated morphologies are destroyed due to poly(ethylene) (PE) chain folding upon crystallization. Below the melting temperature, a sample with a volume fraction f(PE) = 0.49 forms a lamellar structure distinct from that in the melt. On quenching, a hexagonal f(PE) = 0.25 sample forms a lamellar structure similar to that of the f(PE) = 0.49 sample, while the hexagonal-packed cylinder structure of an f(PE) = 0.75 sample is also destroyed by crystallization but does not form well-ordered lamellae. The SAXS profiles from crystallized materials are shown to correspond to the sum of scattering from block copolymer lamellae, with up to four orders of reflection, plus a broad peak arising from semicrystalline PE. Analysis of scattering density correlation functions calculated using the SAXS data shows that the PE lamellar thickness is (45 +/- 5) Angstrom for all samples, similar to that observed for PE homopolymer. The WAXS data reveal that PE crystallizes in its usual orthorhombic form in all samples. The relative degree of crystallinity as a function of time after a quench, determined from the SAXS invariant, is fitted by Avrami equations for spherulitic crystallite growth. The Avrami exponent is found to be n = (3.0 +/- 0.1) for all samples, consistent with a nucleation and growth process. [References: 32]
机译:对聚(乙烯)-聚(乙基乙烯)和聚(乙烯)-聚(乙烯-丙烯)二嵌段进行了时间分辨的同步加速器小角度和广角X射线散射(SAXS和WAXS)和DSC实验共聚物是由具有层状和六角形填充圆柱结构的熔体淬火而成的。我们发现原始的微相分离形态被破坏了由于结晶时的聚乙烯(PE)链折叠。在熔融温度以下,体积分数f(PE)= 0.49的样品形成的层状结构不同于熔体中的层状结构。淬火时,六角形的f(PE)= 0.25样品形成类似于f(PE)= 0.49样品的层状结构,而f(PE)= 0.75样品的六角堆积圆柱结构也被结晶破坏但不会形成有序的薄片。显示结晶材料的SAXS轮廓对应于嵌段共聚物薄片的散射总和,具有多达四个反射级,以及半结晶PE产生的宽峰。使用SAXS数据计算得到的散射密度相关函数的分析表明,所有样品的PE层厚度均为(45 +/- 5)埃,类似于对PE均聚物的观察值。 WAXS数据显示,在所有样品中,PE均以其通常的正交晶形式结晶。由SAXS不变量确定的淬灭后相对结晶度随时间变化的函数,通过球晶生长的Avrami方程拟合。发现所有样品的Avrami指数均为n =(3.0 +/- 0.1),与成核和生长过程一致。 [参考:32]

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