碳纳米管长度分布对纤维力学性能影响的百万原子计数模拟

C. Cornwell, R. Haskins, J. Allen, C. R. Welch, R. Kirgan
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引用次数: 2

摘要

碳纳米管(CNTs)非凡的力学性能使其成为超级基础材料的首选候选材料。从头算、紧密结合、分子动力学模拟和最近的实验表明,碳纳米管的抗拉强度高达约1550万psi (110 GPa),杨氏模量为1.5亿psi (1 TPa),密度约为80 lbs/ft3 (1.3 g/cm3)。这些特性提供的抗拉强度-重量比和刚度-重量比分别是高强度(100,000 psi)钢的900倍和30倍。构建保持这些特性的宏观材料是具有挑战性的。迄今为止,分子缺陷、空洞、外来夹杂物,特别是弱分子间键阻碍了CNTs形成的宏观材料具有CNTs显著的强度和刚度特性。与碳纳米管相关的范德华力表示碳纳米管之间单位长度的作用力。因此,可以预期排列的碳纳米管之间的结合强度随着重叠长度的增加而增加。真正的细丝可能由具有一定长度分布的碳纳米管组成。为了了解碳纳米管长度分布对排列整齐的碳纳米管细丝的拉伸强度的影响,我们使用桑迪亚实验室的大规模原子/分子大规模并行模拟器(LAMMPS)代码在高性能计算机上进行了一系列淬火分子动力学模拟。每个细丝的横截面由六边形最密填充(HCP)阵列碳纳米管链组成,形成两个HCP环。通过端对端放置(5,5)手性碳纳米管来构建长丝。虽然单手性碳纳米管纤维的选择目前还无法实现,但单手性纤维的使用使我们能够只关注碳纳米管长度对长丝响应的影响。CNTs的长度随机选取,呈高斯分布,平均长度范围为100 ~ 1,600Å。对长度从400到6,400Å的细丝进行了一系列的模拟。对于每个细丝,应变以小增量增加,并在应变增量之间淬灭。记录纤维的总拉伸力,并用于确定纤维的单轴应力-应变响应。模拟结果量化了杨氏模量、抗拉强度和临界应变作为平均碳纳米管长度增加的函数的改进。这是作者所知道的第一个分子动力学模拟,处理现实碳纳米管结构的统计质量。模拟结果被用于指导碳纳米管长丝的分子设计,以实现超(100万psi)强度。如果没有大规模并行的高性能计算平台和优化的分子动力学模拟工具,这些模拟将是不切实际的,甚至可能是不可能的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Million-Atom Count Simulations of the Effects of Carbon Nanotube Length Distributions on Fiber Mechanical Properties
The extraordinary mechanical properties of carbon nanotubes (CNTs) make them prime candidates as a basis for super infrastructure materials. Ab initio, tight binding, and molecular dynamics simulations and recent experiments have shown that CNTs have tensile strengths up to about 15.5 million psi (110 GPa), Young’s modulus of 150 million psi (1 TPa), and density of about 80 lbs/ft3 (1.3 g/cm3). These qualities provide tensile strength-toweight and stiffness-to-weight ratios about 900 times and 30 times, respectively, those of high-strength (100,000- psi) steel. Building macromaterials that maintain these properties is challenging. Molecular defects, voids, foreign inclusions, and, in particular, weak intermolecular bonds have, to date, prevented macromaterials formed from CNTs from having the remarkable strength and stiffness characteristics of CNTs. The van der Waals forces associated with CNTsrepresent a force per unit length between CNTs. Accordingly, one would expect the bond strength between aligned CNTs to increase with overlap length. Real filaments are likely composed of CNTs with some distribution of lengths. To understand the effects that CNT length distributions have on the tensile strength of neat filaments of aligned CNTs, we performed a series of quenched molecular dynamics simulations on high performance computers using Sandia Laboratory’s Large-scale Atomic/Molecular Massively Parallel Simulator (LAMMPS) code. The cross-section of each filament was composed of hexagonal closest-packed (HCP) array CNT strands that formed two HCP rings. The filaments were constructed by placing (5,5) chirality CNTs end to end. While the choice of a single-chirality CNT fiber is currently unrealizable, the use of a singlechirality fiber allowed us to focus only on the effects of CNT lengths on filament response. The lengths of the CNTs were randomly selected to have Gaussian distribution with the average length ranging from 100 to 1,600Å. A series of simulations were performed on filament with lengths ranging from 400 to 6,400Å. For each filament, the strain was increased in small increments and quenched between strain increments. The total tensile force on the filament was recorded and used to determine the uniaxial stress-strain response of the filaments. The results of the simulations quantified the improvements in Young’s modulus, tensile strength, and critical strain as a function of the increase in the average component CNT lengths. These are the first molecular dynamics simulations that the authors are aware of that treat statistical qualities of realistic CNT structures. The simulation results are being used to guide the molecular design of CNT filaments to achieve super (1 million psi) strength. The simulations would be impractical, and perhaps impossible, without massively parallel, highperformance computational platforms and molecular dynamics simulation tools optimized to run on such platforms.
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