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Equation of motion and subsonic-transonic transitions of rectilinear edge dislocations: A collective-variable approach

机译:直线边缘位错的运动方程和亚音速-跨音速跃迁:集体变量方法

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A theoretical framework is proposed to derive a dynamic equation motion for rectilinear dislocations within isotropic continuum elastodynamics. The theory relies on a recent dynamic extension of the Peierls-Nabarro equation, so as to account for core-width generalized stacking-fault energy effects. The degrees of freedom of the solution of the latter equation are reduced by means of the collective-variable method, well known in soliton theory, which we reformulate in a way suitable to the problem at hand. Through these means, two coupled governing equations for the dislocation position and core width are obtained, which are combined into one single complex-valued equation of motion, of compact form. The latter equation embodies the history dependence of dislocation inertia. It is employed to investigate the motion of an edge dislocation under uniform time-dependent loading, with focus on the subsonic/transonic transition. Except in the steady-state supersonic range of velocities-which the equation does not address-our results are in good agreement with atomistic simulations on tungsten. In particular, we provide an explanation for the transition, showing that it is governed by a loading-dependent dynamic critical stress. The transition has the character of a delayed bifurcation. Moreover, various quantitative predictions are made, that could be tested in atomistic simulations. Overall, this work demonstrates the crucial role played by core-width variations in dynamic dislocation motion.
机译:提出了一个理论框架来导出各向同性连续弹性力学中直线错位的动力学方程运动。该理论依赖于Peierls-Nabarro方程的最新动态扩展,以解决核宽度广义堆垛层错能量效应。后一种方程的解的自由度通过孤子理论中众所周知的集体变量方法降低,我们以适合当前问题的方式重新制定了该变量。通过这些手段,获得了用于位错位置和芯宽度的两个耦合的控制方程,这些方程被组合成一个紧凑形式的单个复数值运动方程。后一个方程体现了位错惯性的历史依赖性。它被用来研究边缘错位在均匀的时间依赖性载荷下的运动,重点是亚音速/跨音速过渡。除了在速度的稳态超音速范围内(方程式未解决)以外,我们的结果与钨的原子模拟非常吻合。特别是,我们对过渡进行了解释,表明该过渡受与载荷有关的动态临界应力的控制。过渡具有分叉延迟的特征。此外,做出了各种定量预测,可以在原子模拟中进行测试。总的来说,这项工作证明了核心宽度变化在动态位错运动中所起的关键作用。

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