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Scaling of slip avalanches in sheared amorphous materials based on large-scale atomistic simulations

机译:基于大规模原子模拟的剪切非晶材料中滑动雪崩的缩放

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Atomistic simulations of binary amorphous systems with over 4 million atoms are performed. Systems oftwo interatomic potentials of the Lennard-Jones type, LJ12-6 and LJ9-6, are simulated. The athermal quasistaticshearing protocol is adopted, where the shear strain is applied in a stepwise fashion with each step followed byenergy minimization. For each avalanche event, the shear stress drop (σ), the hydrostatic pressure drop (σh),and the potential energy drop (△E) are computed. It is found that, with the avalanche size increasing, the threebecome proportional to each other asymptotically. The probability distributions of avalanche sizes are obtainedand values of scaling exponents fitted. In particular, the distributions follow a power law, P(△U) ~ △U~(−τ) ,where △U is a measure of avalanche sizes defined based on shear stress drops. The exponent τ is 1.25 ± 0.1 forthe LJ12-6 systems, and 1.15 ± 0.1 for the LJ9-6 systems. The value of τ for the LJ12-6 systems is consistentwith that from an earlier atomistic simulation study by Robbins et al. [Phys. Rev. Lett. 109, 105703 (2012)], butthe fitted values of other scaling exponents differ, which may be because the shearing protocol used here differsfrom that in their study.
机译:进行了超过400万原子的二元非晶系统的原子模拟。系统模拟了Lennard-Jones型,LJ12-6和LJ9-6的两个网状模型。滴管Quasistatic采用剪切方案,其中剪切应变以逐步的方式施加,每个步骤后能量最小化。对于每个雪崩事件,剪切应力下降(σ),静液压压降(ΣH),并且计算潜在的能量下降(△e)。发现,随着雪崩大小的增加,三个渐近地变得与彼此成比例。获得雪崩尺寸的概率分布和缩放指数的价值。特别是,分布遵循权力法,P(△U)〜△U〜(-τ),其中△U是基于剪切应力下降定义的雪崩尺寸的衡量标准。指数τ为1.25±0.1LJ12-6系统,LJ9-6系统为1.15±0.1。 LJ12-6系统的τ的值是一致的从罗宾斯等人的早期原子模拟研究中。 [物理。 rev. lett。 109,105703(2012)],但是其他缩放指数的拟合值不同,这可能是因为这里使用的剪切协议不同在他们的研究中。

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    《PHYSICAL REVIEW E》 |2017年第4期|032902.1-032902.12|共12页
  • 作者单位

    Department of Mechanical Science and Engineering University of Illinois at Urbana-Champaign Urbana Illinois 61801 USA;

    Department of Physics Institute for Condensed Matter Theory University of Illinois at Urbana-Champaign Urbana Illinois 61801 USA;

    Department of Mechanical Science and Engineering Institute for Condensed Matter Theory and Beckman Institute University of Illinois at Urbana-Champaign Urbana Illinois 61801 USA;

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