Mechanical properties of amorphous metal with dispersed nanocrystalline particles: Molecular dynamics study on crystal volume fraction and size effects

R. Matsumoto, M. Nakagaki
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引用次数: 3

Abstract

Large-scale molecular dynamics simulations of tensile deformation of amorphous metals with nanocrystalline particles were performed in order to clarify the effects of particle size and crystal volume fraction on the deformation property and the strength. It was clarified that the size effects of the particle are very small, whereas the influences of the crystal volume fraction are large. Young’s modulus and the flow stress become large as the crystal volume fraction increases. Even after the yielding of the amorphous phase, the stress of the crystal phase still continues to increase. Thus, the flow stress of the composite increases after yielding, which prevents plastic localization and improves the ductility. When the crystal volume fraction is small, the stress distribution is homogeneous in the particle including near the amorphous-crystal interface. Therefore, possibility of deformation is small, and insideparticle plastic deformation is negligible. When the crystal volume fraction is high, the particle undergoes plastic deformation even with small global deformation. After the yielding of the crystal particle, the flow stress decreases because defects are introduced into the crystal. It is expected that there is an ideal crystal volume fraction that gives the maximum ductility. A Lennard-Jones potential modified to enforce the continuity at the cut-off distance was used as an interatomic potential. The potential parameters were defined based on Inoue’s three basic principles.
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具有分散纳米晶颗粒的非晶金属的力学性能:晶体体积分数和尺寸效应的分子动力学研究
采用分子动力学方法模拟了纳米晶颗粒对非晶态金属拉伸变形的影响,研究了纳米晶颗粒尺寸和晶体体积分数对非晶态金属变形性能和强度的影响。结果表明,颗粒尺寸的影响很小,而晶体体积分数的影响很大。杨氏模量和流动应力随晶体体积分数的增加而增大。即使在非晶相屈服后,晶相的应力仍在继续增大。因此,复合材料屈服后流变应力增大,防止了塑性局部化,提高了延性。当晶体体积分数较小时,颗粒内包括非晶界面附近的应力分布是均匀的。因此,变形的可能性很小,颗粒内的塑性变形可以忽略不计。当晶体体积分数较高时,即使整体变形很小,颗粒也会发生塑性变形。晶体颗粒屈服后,由于在晶体中引入了缺陷,流动应力减小。期望有一个理想的晶体体积分数,使其具有最大的延展性。为了增强截止距离处的连续性,我们使用了经过修正的伦纳德-琼斯势作为原子间势。电位参数是根据井上的三个基本原则定义的。
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