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3D-2D transition in mode-I fracture microbranching in a perturbed hexagonal close-packed lattice

机译:模式-I中的3D-2D过渡在扰动中的断裂微变形   六角密排晶格

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摘要

Mode-I fracture exhibits microbranching in the high velocity regime where thesimple straight crack is unstable. For velocities below the instability,classic modeling using linear elasticity is valid. However, showing theexistence of the instability and calculating the dynamics post-instabilitywithin the linear elastic framework is difficult and controversial. Theexperimental results give several indications that the microbranchingphenomenon is basically a three-dimensional phenomenon. Nevertheless, thetheoretical effort has been focused mostly in two-dimensional modeling. In thiswork we study the microbranching instability using three-dimensional atomisticsimulations, exploring the difference between the 2D and 3D models. We findthat the basic 3D fracture pattern shares similar behavior with the 2D case.Nevertheless, we exhibit a clear 3D-2D transition as the crack velocityincreases, while as long as the microbranches are sufficiently small, thebehavior is pure 3D-behavior, while at large driving, as the size of themicrobranches increases, more 2D-like behavior is exhibited. In addition, in 3Dsimulations, the quantitative features of the microbranches, separating theregimes of steady-state cracks (mirror) and post-instability (mist-hackle) arereproduced clearly, consistent with the experimental findings.
机译:Ⅰ型骨折在简单的直裂纹不稳定的高速区域表现出微分支。对于低于不稳定性的速度,使用线性弹性的经典建模是有效的。然而,在线性弹性框架内显示不稳定性的存在并计算不稳定性的动力学是困难且有争议的。实验结果表明,微支化现象基本上是三维现象。尽管如此,理论上的努力主要集中在二维建模上。在这项工作中,我们使用三维原子模拟研究微分支不稳定性,探索2D模型和3D模型之间的差异。我们发现基本的3D断裂模式与2D情况具有相似的行为。尽管如此,当裂纹速度增加时,我们仍显示出清晰的3D-2D过渡,而只要微分支足够小,则行为就是纯3D行为,而大时在驱动中,随着微分支的尺寸增加,表现出更多的2D样行为。此外,在3D模拟中,与实验结果一致,清晰地再现了微分支的定量特征,分离了稳态裂纹(镜)和后不稳定性(雾-hackle)的区域。

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