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On the atomistic mechanisms of grain boundary migration in [0 0 1] twist boundaries: Molecular dynamics simulations

机译:[0 0 1]扭曲边界中晶界迁移的原子机理:分子动力学模拟

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Molecular dynamics simulations were performed to characterize the atomic motions that govern grain boundary migration in a series of twist boundaries. In particular, migration of θ = 36.87° Σ5, θ = 22.63° Σ13, and θ = 40.23° general high angle [0 0 1] twist boundaries driven by stored elastic energy in fcc nickel were investigated. Atomic motions during migration were identified as single-atom jumps and multiple-atom collective motions (including general string-like cooperative motions and special four-atom shuffles) using quantitative string measurement, the self-part of the van Hove correlation function, and an angular distribution function. The simulation results confirmed that collective four-atom shuffle motion was the rate controlling atomic motion during migration of the Σ5 twist boundary. Furthermore, simulations showed no correlation between individual four-atom shuffles, suggesting migration was controlled by random shuffles rather than a propagation of kinks along ledges. As grain boundary local symmetry decreased (i.e., from a low Σ boundary to a high Σ boundary), string-like cooperative atomic motions (not collective shuffle motions) became increasingly important. Both random single-atom jumps and general string-like cooperative motions were dominant during migration of a general non-Σ twist boundary. Simulations also showed that the activation energy for grain boundary migration was well correlated with the average string length occurring within the boundary. This implies that grain boundary drifting velocity is sensitive to factors (e.g., external stresses, impurities) that can alter string motions within a boundary.
机译:进行了分子动力学模拟,以表征控制一系列扭曲边界中晶界迁移的原子运动。特别地,研究了由fcc镍中存储的弹性能驱动的θ= 36.87°Σ5,θ= 22.63°Σ13和θ= 40.23°的一般大角度[0 0 1]扭曲边界的迁移。迁移过程中的原子运动被确定为单原子跳跃和多原子集体运动(包括一般的弦状协作运动和特殊的四原子混洗),其使用了定量弦测量,van Hove相关函数的自部分和角度分布函数。仿真结果证实,集体四原子混洗运动是控制Σ5扭曲边界迁移过程中原子运动的速率。此外,模拟显示单个四原子的混洗之间没有相关性,这表明迁移是由随机混洗控制的,而不是沿壁架的扭结传播。随着晶界局部对称性降低(即,从低Σ边界到高Σ边界),串状协作原子运动(而不是集体拖曳运动)变得越来越重要。在一般的非Σ扭转边界迁移过程中,随机单原子跳跃和一般的串状协作运动均占主导地位。模拟还表明,晶界迁移的活化能与晶界内平均弦长有关。这意味着晶界漂移速度对可能改变边界内弦运动的因素(例如外部应力,杂质)敏感。

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