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Following the Crystallization Process of Polyethylene Single Chain by Molecular Dynamics: The Role of Lateral Chain Defects

机译:通过分子动力学的聚乙烯单链结晶过程:侧链缺陷的作用

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Langevin molecular dynamics (LMD) simulations have been performed in order to understand the role of the short chain branches (SCB) on the formation of ordered domains by cooling ethylene/a-olefins single chain models. Different long single-chain models (C_(2000)) with 0, 5 and 10 branches each 1000 carbons were selected. The branches were randomly distributed along the backbone chain. Furthermore, C1 (methyl) and C4 (butyl) branches were taken into account. These models mimic the molecular architecture of ethylene/1-butene and ethylene/ 1-hexene random copolymers. The simulations are performed according to the following protocol: 20 random chain conformations for each model were equilibrated at high temperature (T~*=13.3) and then they were cooled in steps of 0.45 until the final temperature (T~*=6.2) by running a total of 35×10~6 LMD steps. The distribution peaks of crystallization for each model were calculated by differentiating the global order parameter with respect to the temperature. The Tc~*(crystallization temperature) decrease as the number of branches increases as it is experimentally observed. The formation of order in the copolymers is affected by the type and amount of the SCB in the backbone of the polymer chain. The stem lenght and crystallization fraction (a) were defined using the local-bond order parameter. Both parameters decrease as the number of branches increase. In all cases here shown, the C4 branches are excluded from the ordered domains. However, we have observed that the methyl branch can be incorporated into the ordered regions. These facts satisfactorily agree with experimental data available in the literature.
机译:已经进行了Langevin分子动力学(LMD)模拟,以了解短链分支(SCB)对通过冷却乙烯/烯烃单链模型形成有序结构域的作用。不同的长单链型号(C_(2000)),选择了0,5和10个分支,每1000个碳都被选中。分支沿骨干链随机分布。此外,考虑C1(甲基)和C4(丁基)分支。这些模型模拟了乙烯/ 1-丁烯和乙烯/ 1-己烯无规共聚物的分子结构。根据以下方案进行模拟:在高温(T〜* = 13.3)下每种模型的20个随机链构象(T〜* = 13.3),然后按照0.45的步长冷却,直至最终温度(t〜* = 6.2)。总共运行35×10〜6 LMD步骤。通过将全局顺序参数与温度区分区来计算每个模型的结晶分布峰。随着分支的数量随着实验观察而增加,TC〜*(结晶温度)降低。共聚物中的顺序的形成受聚合物链的骨架中SCB的类型和量的影响。使用局部键合顺序参数定义茎长度和结晶级分(A)。随着分支的数量增加,两个参数都会减少。在此目明的所有情况下,C4分支被排除在有序域之外。然而,我们观察到甲基分支可以掺入有序区域。这些事实令人满意地同意文献中提供的实验数据。

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