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晶界取向差对Ni/NiAl力学性能及塑性变形机制的影响:分子动力学研究

The Effects of Grain Boundary Misorientation on the Mechanical Properties and Mechanism of Plastic Deformation of Ni/NiAl: A Molecular Dynamics Study.

作者信息

Ding Jun, Zhang Sheng-Lai, Tong Quan, Wang Lu-Sheng, Huang Xia, Song Kun, Lu Shi-Qing

机构信息

College of Mechanical Engineering, Chongqing University of Technology, Banan, Chongqing 400054, China.

School of Material Science and Engineering, Hefei University of Technology, Hefei 230009, China.

出版信息

Materials (Basel). 2020 Dec 15;13(24):5715. doi: 10.3390/ma13245715.

Abstract

The effects of grain boundary misorientation angle () on mechanical properties and the mechanism of plastic deformation of the Ni/NiAl interface under tensile loading were investigated using molecular dynamics simulations. The results show that the space lattice arrangement at the interface is dependent on grain boundary misorientations, while the interfacial energy is dependent on the arrangement. The interfacial energy varies in a W pattern as the grain boundary misorientation increases from 0° to 90°. Specifically, the interfacial energy first decreases and then increases in both segments of 0-60° and 60-90°. The yield strength, elastic modulus, and mean flow stress decrease as the interfacial energy increases. The mechanism of plastic deformation varies as the grain boundary misorientation angle () increases from 0° to 90°. When = 0°, the microscopic plastic deformation mechanisms of the Ni and NiAl layers are both dominated by stacking faults induced by Shockley dislocations. When = 30°, 60°, and 80°, the mechanisms of plastic deformation of the Ni and NiAl layers are the decomposition of stacking faults into twin grain boundaries caused by extended dislocations and the proliferation of stacking faults, respectively. When = 90°, the mechanisms of plastic deformation of both the Ni and NiAl layers are dominated by twinning area growth resulting from extended dislocations.

摘要

采用分子动力学模拟方法,研究了晶界取向差()对拉伸载荷下Ni/NiAl界面力学性能及塑性变形机制的影响。结果表明,界面处的空间晶格排列取决于晶界取向差,而界面能则取决于这种排列。随着晶界取向差从0°增加到90°,界面能呈W形变化。具体而言,在0 - 60°和60 - 90°两个区间内,界面能均先减小后增大。屈服强度、弹性模量和平均流动应力随着界面能的增加而降低。随着晶界取向差()从0°增加到90°,塑性变形机制发生变化。当 = 0°时,Ni层和NiAl层的微观塑性变形机制均由肖克利位错诱导的层错主导。当 = 30°、60°和80°时,Ni层和NiAl层的塑性变形机制分别是扩展位错导致层错分解为孪晶界和层错的增殖。当 = 90°时,Ni层和NiAl层的塑性变形机制均由扩展位错导致的孪晶区生长主导。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0c2f/7765284/4ae86c36725a/materials-13-05715-g013.jpg

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