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单轴拉伸流动下缠结聚乙烯熔体的流动诱导微相分离和结晶的原子模拟以及库恩链段伸长的作用

Atomistic Simulation of Flow-Induced Microphase Separation and Crystallization of an Entangled Polyethylene Melt Undergoing Uniaxial Elongational Flow and the Role of Kuhn Segment Extension.

作者信息

Nafar Sefiddashti Mohammad Hadi, Edwards Brian J, Khomami Bamin

机构信息

Materials Research and Innovation Laboratory, Department of Chemical and Biomolecular Engineering, University of Tennessee, Knoxville, TN 37996, USA.

出版信息

Polymers (Basel). 2023 Apr 9;15(8):1831. doi: 10.3390/polym15081831.

Abstract

Atomistic simulations of the linear, entangled polyethylene CH melt undergoing steady-state and startup conditions of uniaxial elongational flow (UEF) over a wide range of flow strength were performed using a united-atom model for the atomic interactions between the methylene groups constituting the polymer macromolecules. Rheological, topological, and microstructural properties of these nonequilibrium viscoelastic materials were computed as functions of strain rate, focusing on regions of flow strength where flow-induced phase separation and flow-induced crystallization were evident. Results of the UEF simulations were compared with those of prior simulations of planar elongational flow, which revealed that uniaxial and planar flows exhibited essentially a universal behavior, although over strain rate ranges that were not completely equivalent. At intermediate flow strength, a purely configurational microphase separation was evident that manifested as a bicontinuous phase composed of regions of highly stretched molecules that enmeshed spheroidal domains of relatively coiled chains. At high flow strength, a flow-induced crystallization (FIC) occurred, producing a semicrystalline material possessing a high degree of crystallinity and primarily a monoclinic lattice structure. This FIC phase formed at a temperature (450 K) high above the quiescent melting point (≈400 K) and remained stable after cessation of flow for temperature at or below 435 K. Careful examination of the Kuhn segments constituting the polymer chains revealed that the FIC phase only formed once the Kuhn segments had become essentially fully extended under the UEF flow field. Thermodynamic properties such as the heat of fusion and heat capacity were estimated from the simulations and found to compare favorably with experimental values.

摘要

使用联合原子模型来描述构成聚合物大分子的亚甲基之间的原子相互作用,对线性、缠结的聚乙烯CH熔体在很宽的流动强度范围内进行稳态和单轴拉伸流动(UEF)启动条件下的原子模拟。计算了这些非平衡粘弹性材料的流变、拓扑和微观结构性质与应变速率的函数关系,重点关注流动诱导相分离和流动诱导结晶明显的流动强度区域。将UEF模拟结果与之前平面拉伸流动模拟结果进行比较,结果表明,单轴和平面流动表现出基本的通用行为,尽管应变速率范围并不完全相同。在中等流动强度下,明显存在一种纯粹的构型微相分离,表现为一种双连续相,由高度拉伸分子区域和相对卷曲链的球形区域相互交织组成。在高流动强度下,发生了流动诱导结晶(FIC),产生了一种具有高结晶度且主要为单斜晶格结构的半结晶材料。这种FIC相在远高于静态熔点(≈400 K)的温度(450 K)下形成,并且在流动停止后,对于435 K及以下的温度保持稳定。仔细检查构成聚合物链的库恩链段发现,只有在库恩链段在UEF流场下基本完全伸展后,FIC相才会形成。通过模拟估算了诸如熔化热和热容量等热力学性质,发现与实验值相比具有良好的一致性。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ea9f/10146043/afda3d4a1e50/polymers-15-01831-g001.jpg

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