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2222材料工程  2015, Vol. 43 Issue (3): 60-66    DOI: 10.11868/j.issn.1001-4381.2015.03.011
  测试与表征 本期目录 | 过刊浏览 | 高级检索 |
不同应变率下纳米多晶Cu/Ni薄膜变形行为的分子动力学模拟
成聪1,2, 陈尚达1,2,*(), 吴勇芝1,2, 黄鸿翔1,2
1 湘潭大学 材料与光电物理学院, 湖南 湘潭 411105
2 湘潭大学 低维材料及其应用技术教育部重点实验室, 湖南 湘潭 411105
Molecular Dynamics Simulations of Deformation Behaviors for Nanocrystalline Cu/Ni Films Under Different Strain Rates
Cong CHENG1,2, Shang-da CHEN1,2,*(), Yong-zhi WU1,2, Hong-xiang HUANG1,2
1 Faculty of Materials, Optoelectronics and Physics, Xiangtan University, Xiangtan 411105, Hunan, China
2 Key Laboratory of Low Dimensional Materials & Application Technology(Ministry of Education), Xiangtan University, Xiangtan 411105, Hunan, China
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摘要 

用分子动力学方法模拟了纳米多晶Cu/Ni薄膜在不同应变率下进行应变加载时的变形行为与力学性能。结果表明:Cu/Ni薄膜在较高的应变率加载情况下具有较高的屈服极限和应变率敏感性(m)。应变率为108s-1时Cu/Ni多层膜的界面上产生孔洞,而应变率为1010s-1时纳米多晶Cu薄膜出现碎裂。在较高的应变率加载条件下,Cu,Ni薄膜中FCC,HCP,OTHER原子团分数变化都很显著,而较小应变率时只有Cu薄膜的结构变化明显。模拟结果还表明,应变率增加有利于堆垛层错的形成,但应变率超过某一值时无序原子团增加会阻碍堆垛层错原子团的生长。

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成聪
陈尚达
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黄鸿翔
关键词 分子动力学纳米多晶Cu/Ni薄膜应变率    
Abstract

Molecular dynamics simulations are carried out to investigate the deformation behaviors and mechanical properties of nanocrystalline Cu/Ni films under conditions of tensile strain at different strain rates. The results indicate that the Cu/Ni films have higher yield strength and higher strain rate sensitivity(m)at the higher strain rate. The nucleation of voids in Cu/Ni multilayers' interface is observed at a strain rate of 108s-1, whereas spallation in nanocrystalline Cu films is appeared at a strain rate of 1010s-1.For the higher strain rate loading conditions, the FCC, HCP, and OTHER atomic groups are changed significantly both in Cu and Ni films. However, striking structural changes are found only in the Cu films under conditions of tensile strain at lower strain rate. The simulation results show that increasing strain rates are benefit to the formation of HCP structure, while if the strain rates exceed a certain value, the increasing disorder atomic groups may impede the growth of HCP atomic groups.

Key wordsmolecular dynamics    nanocrystalline    Cu/Ni film    strain rate
收稿日期: 2013-09-29      出版日期: 2015-03-20
基金资助:国家自然科学基金青年基金(10702058)
通讯作者: 陈尚达     E-mail: chensd@xtu.edu.cn
作者简介: 陈尚达(1976-),男,博士,副教授,主要从事金属薄膜界面微观结构演化与金属薄膜界面结合性能模拟的研究工作,联系地址:湘潭大学材料与光电物理学院(411105),E-mail:chensd@xtu.edu.cn
引用本文:   
成聪, 陈尚达, 吴勇芝, 黄鸿翔. 不同应变率下纳米多晶Cu/Ni薄膜变形行为的分子动力学模拟[J]. 材料工程, 2015, 43(3): 60-66.
Cong CHENG, Shang-da CHEN, Yong-zhi WU, Hong-xiang HUANG. Molecular Dynamics Simulations of Deformation Behaviors for Nanocrystalline Cu/Ni Films Under Different Strain Rates. Journal of Materials Engineering, 2015, 43(3): 60-66.
链接本文:  
http://jme.biam.ac.cn/CN/10.11868/j.issn.1001-4381.2015.03.011      或      http://jme.biam.ac.cn/CN/Y2015/V43/I3/60
Fig.1  Cu/Ni薄膜系统的初始模型,上层为Ni层(橙色-FCC结构、绿色-OTHER、紫色-HCP结构);下层为Cu层(蓝色-FCC结构、黄色-OTHER、红色-HCP结构)
Fig.2  不同应变率下Cu/Ni薄膜系统变形应力-应变曲线
Fig.3  对数坐标平面内Cu/Ni薄膜系统屈服极限-应变率曲线
Fig.4  Cu/Ni薄膜系统在应变率为108s-1
(a),1010s-1(b)时FCC、HCP和晶界结构原子分数随应变变化趋势
Fig.5  应变率为108s-1 时单轴加载纳米多晶Cu/Ni样品截面图
(a)用中心对称参数值P对原子着色,蓝色-完整FCC结构,绿色-部分位错、堆垛层错、孪晶界结构,红色-表面原子;(b)用CNA值对原子进行着色,颜色设置与图1相同;(1)ε=0;(2)ε=0.057;(3)ε=0.058;(4)ε=0.059
Fig.6  应变率为1010s-1 时单轴加载纳米多晶Cu/Ni样品截面图
(a)用中心对称参数值P对原子着色:蓝色-完整FCC结构,绿色-部分位错、堆垛层错、孪晶界结构,红色-表面原子;(b)用CNA值对原子进行着色,颜色设置与图1相同;(1)ε=0;(2)ε=0.0927;(3)ε=0.1126;(4)ε=0.1325
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