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首页> 外文期刊>Polymer: The International Journal for the Science and Technology of Polymers >Analysis of structural changes during plastic deformations of amorphous polyethylene
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Analysis of structural changes during plastic deformations of amorphous polyethylene

机译:非晶态聚乙烯塑性变形过程中的结构变化分析

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Molecular dynamics (MD) simulations have been used to analyze yielding and stress-softening processes during stepped simple tensile loading of bulk amorphous polyethylene (PE) at temperatures (T_(def)) well below the glass transition temperature (T_g). Specimens formed by 20 linear chains of 1000 beads each (2 × 10~4 coarse grained -CH _2- units), with energetics described by a united atom potential, were deformed at T_(def) = 100K. Configurations at axial strains (ε_(xx)) ranging from 0% to 30% were allowed to reach steady state equilibration. Subsequently, configurations in a time period of 5 ps were saved for analysis of their local structure. Local structural characteristics were analyzed using three methods: (i) a geometric description by computing the evolution of self and inter-chain entanglements, the number of bead contacts and the free volume, (ii) the method of Empirical Orthogonal Functions (EOF) to obtain a reduced description of the displacement field at each strain level and the vibration of each bead around its equilibrium position, and (iii) Hardy's method to compute the time averaged local stress tensor to obtain a detailed description of the distribution of internal forces. It was found that at early stages of deformation (ε_(xx) < 13%) the inter-chain entanglement continuously decreases while the self-entanglement showed no significant variation and no distinct patterning. Also the energy content in each eigenmode of the normalized displacement correlation matrix used in the EOF analysis is almost the same for a large portion of the frequency range regardless of the imposed axial strain level. Furthermore, distribution of the local pressure presented a positive expected value at the initial (ε_(xx) = 0%) configuration; the expected value continuously decreases toward the point where the axial stress peaks (ε_(xx) = 13%). The evolution of the number of loosely packed regions (quasi-defects), identified by a negative value of the local pressure, showed three distinct regimes: ε_(xx)(0%-5%), ε_(xx)(5%-13%) and ε_(xx)(13%-30%). The first regime corresponds to the fast nucleation of quasi-defects while the last one showed an inversion in the trend during the stress-softening regime with a moderate decreasing tendency. The three analyses show that the plastic deformation in this amorphous material commences with the nucleation of stress-induced defects without significant changes in the molecular degrees of freedom. Despite the chemical nature and inherent internal structure of the material under study, our findings support Argon et al.'s theory [1-4] as well as that of subsequent investigators [4,5] in that local structural rearrangements exist at locations where particles (beads) forming the material are loosely packed; these regions are termed the local shear transformation zones (STZ).
机译:分子动力学(MD)模拟已被用于分析在远低于玻璃化转变温度(T_g)的温度(T_(def))下,块状无定形聚乙烯(PE)的逐步简单拉伸加载过程中的屈服和应力软化过程。由20条每1000条珠子的线性链(2×10〜4个粗粒-CH _2-单元)形成的标本在T_(def)= 100K时发生变形,并且其能量由统一的原子势描述。使轴向应变(ε_(xx))范围从0%到30%的构型达到稳态平衡。随后,保存了5 ps时间内的配置,以分析其局部结构。使用三种方法分析了局部结构特征:(i)通过计算自身和链间缠结的演化,珠子接触的数量和自由体积的几何描述,(ii)经验正交函数(EOF)的方法获得关于每个应变水平的位移场的简化描述以及每个磁珠在其平衡位置附近的振动,以及(iii)Hardy方法计算时间平均局部应力张量,以获得对内力分布的详细描述。发现在变形的早期阶段(ε_(xx)<13%),链间缠结不断减少,而自缠结没有明显变化,也没有明显的图案。同样,在EOF分析中使用的归一化位移相关矩阵的每个本征模中的能量含量对于大部分频率范围几乎都是相同的,而与施加的轴向应变水平无关。此外,局部压力的分布在初始(ε_(xx)= 0%)配置时呈现正期望值;期望值朝着轴向应力峰值(ε_(xx)= 13%)的位置连续降低。由局部压力的负值确定的松散堆积区域(准缺陷)数量的演变显示出三种不同的状态:ε_(xx)(0%-5%),ε_(xx)(5%- 13%)和ε_(xx)(13%-30%)。第一个状态与准缺陷的快速成核相对应,而最后一个状态在应力软化过程中显示出趋势的倒置,并有中等程度的下降趋势。三种分析表明,这种无定形材料的塑性变形始于应力诱发缺陷的形核,而分子自由度没有明显变化。尽管所研究材料的化学性质和固有的内部结构,我们的发现仍支持Argon等人的理论[1-4]以及后来的研究者的理论[4,5],因为该结构在以下位置存在局部结构重排形成材料的颗粒(珠子)松散堆积;这些区域称为局部剪切转变带(STZ)。

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