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Atomistic simulation study of the shear-band deformation mechanism in Mg-Cu metallic glasses

机译:mg-Cu金属玻璃剪切带变形机制的原子模拟研究

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摘要

We have simulated plastic deformation of a model Mg-Cu metallic glass in order to study shear banding. In uniaxial tension, we find a necking instability occurs rather than shear banding. We can force the latter to occur by deforming in plane strain, forbidding the change of length in one of the transverse directions. Furthermore, in most of the simulations a notch is used to initiate shear bands, which lie at a 45 degrees angle to the tensile loading direction. The shear bands are characterized by the Falk and Langer local measure of plastic deformation D-min(2), averaged here over volumes containing many atoms. The D-min(2) profile has a peak whose width is around 10 nm; this width is largely independent of the strain rate. Most of the simulations were, at least nominally, at 100 K, about T-g/3 for this system. The development of the shear bands takes a few tens of ps, once plastic flow has started, more or less independent of strain rate. The shear bands can also be characterized using a correlation function defined in terms of D-min(2), which, moreover, can detect incipient shear bands in cases where they do not fully form. By averaging the kinetic energy over small regions, the local temperature can be calculated, and this is seen to be higher in the shear bands by about 50-100 K. Increases in temperature appear to initiate from interactions of the shear bands with the free surfaces and with each other, and are delayed somewhat with respect to the localization of plastic flow itself. We observe a slight decrease in density, up to 1%, within the shear band, which is consistent with notions of increased free volume or disorder within a plastically deforming amorphous material.
机译:为了研究剪切带,我们模拟了模型的Mg-Cu金属玻璃的塑性变形。在单轴张力下,我们发现发生颈缩不稳定性而不是剪切带。我们可以通过使平面应变变形来强制后者发生,从而禁止横向方向之一上的长度变化。此外,在大多数模拟中,都使用一个缺口来引发剪切带,该剪切带与拉伸载荷方向成45度角。剪切带的特征在于塑性变形的D-min(2)的Falk和Langer局部量度,此处是包含许多原子的体积的平均值。 D-min(2)轮廓的峰宽约为10 nm;该宽度在很大程度上与应变率无关。对于该系统,大多数模拟至少在名义上为100 K,约为T-g / 3。一旦开始塑性流动,剪切带的发展就需要几十ps,或多或少地与应变率无关。剪切带还可以使用根据D-min(2)定义的相关函数来表征,此外,在不完全形成剪切带的情况下,该函数可以检测初期剪切带。通过在小区域上平均动能,可以计算出局部温度,并且在剪切带中可以看到局部温度高出约50-100K。温度的升高似乎是由剪切带与自由表面的相互作用引起的彼此之间,并且在塑性流本身的定位方面有所延迟。我们观察到剪切带内的密度略有下降,最高降低了1%,这与塑性变形的非晶态材料中自由体积或无序性增加的观点一致。

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