Isothermal crystallization kinetics in bulk of olefin-based multiblock copolymers

G. Urciuoli, Odda Ruiz de Ballesteros, Giuseppe Femina, F. Auriemma
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引用次数: 2

Abstract

Isothermal crystallization kinetics of ethylene/1-octene (C2/C8) multiblock copolymers synthesized by chain shuttling technology is investigated. The samples are a reactor blend of segmented chains characterized by alternating crystalline and amorphous blocks with C8 content of 0.5 and 20 mol%, respectively, and statistical distribution of block number/chain and block length. The analysis is carried out after complete removal of a fraction (5–12 wt%), namely consisting of C8-rich blocks, through Kumagawa extraction with boiling diethyl ether. The resultant diethyl ether-insoluble fractions have similar average content of C8 units (≈13–14 mol%) and of crystalline blocks (≈23–27 wt%) but different molecular mass (the number average molecular mass M n is ≈ 60–70 kDa for the samples 1,2 and ≈38 and ≈21 kDa for the samples 3 and 4, respectively). An additional sample with M n ≈ 93 kDa, but a greater average content of C8 units (≈15 mol%) and a smaller content of crystalline blocks (15 wt%) is also analyzed. The crystallization half time of the samples increases with increase of M n and, for each sample, its logarithm increases linearly with a decrease of the undercooling by a factor of -0.155/°C, for the samples 1–4 and −0.031/°C, for the sample 5. Using the classic kinetic crystallization model by Lauritzen and Hoffman, values of energy barrier constant due to contributions from primary nucleation K N and crystal growth K G are extracted. The K N contribution is esteemed to amount to ≈34% of the total barrier assuming regime II for the sample 5 and regime III (or I) for the samples 1–4, to ≈34% for the sample 5 and 67% for the samples 1–4, assuming regime II for all the samples. In all the cases, regardless of the assumed regimes, the K N values of the sample 5 are lower than those of the samples 1–4. As a final remark, the implications of crystallization kinetics on the solid-state morphology are also discussed, considering that transmission electron microscopy (TEM) images present a partially mesophase separated morphology for the samples 1,2, and 5 and a classic lamellar morphology for the samples 3 and 4.
烯烃基多嵌段共聚物的等温结晶动力学
研究了链穿梭法合成乙烯/1-辛烯(C2/C8)多嵌段共聚物的等温结晶动力学。结果表明,C8的含量分别为0.5 mol%和20 mol%,呈晶态和非晶态交替分布,具有块数/链和块长统计分布。分析是在用煮沸乙醚进行熊川萃取,完全去除一部分(5-12 wt%),即由富含c8的块组成后进行的。所得的二乙醚不溶馏分C8单元的平均含量(≈13-14 mol%)和结晶块的平均含量(≈23-27 wt%)相似,但分子质量不同(样品1、2的数平均分子质量mn为≈60-70 kDa,样品3和4分别为≈38和≈21 kDa)。另外一个样品的mn≈93 kDa,但C8单位的平均含量较高(≈15 mol%),晶体块的含量较低(15 wt%)。样品的结晶半时间随mn的增加而增加,对于每个样品,其对数随过冷度的减少而线性增加-0.155/°C,对于样品1-4和- 0.031/°C,对于样品5。利用Lauritzen和Hoffman的经典动力学结晶模型,提取了由初成核K N和晶体生长K G贡献的能垒常数值。假设对样品5和样品1-4的状态II和状态III(或I), K N的贡献被认为相当于总势垒的≈34%,对样品5和样品1-4的贡献分别为≈34%和67%,假设对所有样品的状态II。在所有情况下,无论假设的情况如何,样本5的K - N值低于样本1-4的K - N值。最后,考虑到透射电子显微镜(TEM)图像显示样品1、2和5的部分中间相分离形貌以及样品3和4的经典片层形貌,本文还讨论了结晶动力学对固态形貌的影响。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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