Experimental Mechanics ( IF 2.4 ) Pub Date : 2021-04-28 , DOI: 10.1007/s11340-021-00724-7 J. Wei , Q. D. Wang , M. Ebrahimi , L. Zhang , D. D. Yin , H. Y. Jiang , W. J. Ding
Background
High pressure die casting (HPDC) Mg alloy has a hetero-structure in which the microstructures gradually coarsen from the casting surface to the interior, leading to the different elastic–plastic (E-P) transitional behaviors among the layers.
Objective
In this paper, we quantitively determined the diverse E-P transitions among the HPDC layers and related them to the microstructural evolution.
Methods
To investigate independently the E-P transitional behavior of the layer, the surface, middle, and central layers were deliberately sliced in sequence from the casting surface to the interior of the HPDC Mg-4Al-5.7RE (in wt.%) component. The onset and the end of E-P transition in each layer were quantitively determined by cyclic tensile test and Kocks-Mecking analysis, respectively.
Results
It was found that the plastic deformation for all layers occurred in the first unloading loop near zero strain, indicating the start of the E-P transition. With increasing strain, the E-P transition ended first in the middle layer at 0.0081 strain due to the lowest fraction of the second phases and ended last at the small-grained surface layer at 0.0090 strain. Excluding the twinning-dependent anelastic strain, the E-P transitions ended in advance at the strains of 0.0059 and 0.0062 in the middle and surface layer, respectively.
Conclusions
A combination of cyclic tensile test and Kocks-Mecking analysis provided a method to quantitively determine the diverse E-P transitions among the HPDC layers resulted from the hetero-structure regarding grains, the second phases, and twins.
中文翻译:
异质高压压铸镁铝稀土合金的弹塑性转变实验研究
背景
高压压铸(HPDC)镁合金具有异质结构,其中微观结构从铸造表面到内部逐渐变粗,从而导致各层之间不同的弹塑性(EP)过渡行为。
客观的
在本文中,我们定量确定了HPDC层之间的各种EP过渡,并将它们与微观结构演变相关。
方法
为了独立研究该层的EP过渡行为,有意从浇铸表面到HPDC Mg-4Al-5.7RE(按重量%)组分的内部依次对表面层,中间层和中心层进行了切片。通过循环拉伸试验和Kocks-Mecking分析分别定量确定每层中EP转变的开始和结束。
结果
结果发现,所有层的塑性变形均发生在接近零应变的第一个卸载回路中,这表明EP转变开始。随着应变的增加,由于第二相的分数最低,EP过渡首先在中间层以0.0081应变终止,最后在0.0090应变在小晶粒表面层终止。除了依赖孪晶的非弹性应变,EP过渡分别在中层和表层分别以0.0059和0.0062的应变结束。
结论
循环拉伸试验和Kocks-Mecking分析的结合提供了一种定量确定HPDC层中由晶粒,第二相和孪晶的异质结构导致的不同EP转变的方法。