晶体中存在孔隙或空位时奥氏体的理论强度:分子动力学研究

I. Zorya, G. Poletaev, R. Rakitin
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引用次数: 0

摘要

采用分子动力学方法研究了不同直径的孔隙以及相应的单个空位浓度对不同温度下奥氏体理论强度的影响。模型中的变形是通过 20 米/秒的恒定剪切速率进行的。我们考虑了沿两个方向的剪切:[2] 和 [111]。计算奥氏体晶胞的形状为长 14.0 nm、高 14.0 nm、宽 5.1 nm 的矩形平行长方体。为了描述原子间的相互作用,使用了 Lau EAM 势,它很好地再现了奥氏体的结构、能量和弹性特征。在考虑的两个剪切方向上获得的应力-应变曲线具有相似的形式。在没有位错源的情况下,塑性变形是通过形成位错偶极子(具有相反布尔格斯矢量的位错)来实现的。孔隙的存在大大降低了奥氏体的屈服强度。在这种情况下,研究发现,随机散布在计算单元体积中的单个空位也会导致屈服强度降低,但降低程度当然不如孔隙。变形过程中位错的释放通常是通过在两个滑移面上同时形成位错环来实现的。在低温条件下,孔隙和空位对屈服强度的影响更大。随着温度的升高,缺陷对形成位错的临界应力的影响减小。随着孔隙大小和空位浓度的增加,屈服强度也随之降低。在这种情况下,直径为 1 纳米以下的孔隙的依赖性最强。在所考虑的范围内,空位浓度对屈服强度的影响相对更平滑,几乎呈线性关系。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Theoretical strength of austenite in the presence of a pore or vacancies in the crystal: Molecular dynamics study
The molecular dynamics method was used to study the influence of pores of different diameters, as well as the corresponding concentration of individual vacancies, on the theoretical strength of austenite at different temperatures. The deformation in the model was carried out by shear at a cons­tant rate of 20 m/s. We considered a shear along two directions: [ \(\bar 1\ \bar 1\) 2] and [111]. The computational austenite cell had the shape of a rectangular parallelepiped 14.0 nm long, 14.0 nm high, and 5.1 nm wide. To describe interatomic interactions, the Lau EAM potential was used, which reproduces well the structural, energy, and elastic characteristics of austenite. The stress-strain curves obtained for both considered shear directions had a similar form. In the absence of dislocation sources, plastic deformation was carried out by the formation of dislocation dipoles (dislocations with opposite Burgers vectors). The presence of a pore significantly reduced the yield strength of austenite. In this case, it was found that single vacancies randomly scattered over the volume of the computational cell also lead to a decrease in the yield strength, but, of course, not as much as the pore. The emission of dislocations during deformation occurred by the formation of dislocation loops, as a rule, in two slip planes at once. The effect of pores and vacancies on the yield strength was stronger at low temperatures. As the temperature increased, the effect of defects on the critical stress at which dislocations were formed decreased. With an increase in the pore size, as well as the concentration of vacancies, the yield strength decreased. In this case, the strongest dependence was observed for pores up to 1 nm in diameter. The influence of the concentration of vacancies in the considered range on the yield strength turned out to be comparatively smoother and almost linear.
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