Spallation Characteristics of Single Crystal Aluminum with Copper Nanoparticles Based on Atomistic Simulations

被引:8
|
作者
Jiang, Dong-Dong [1 ,2 ]
Chen, Peng-Yu [1 ]
Wang, Pei [1 ]
He, An-Min [1 ]
机构
[1] Inst Appl Phys & Computat Math, Beijing 100094, Peoples R China
[2] China Acad Engn Phys, Grad Sch, Beijing 100088, Peoples R China
关键词
nanocomposite; aluminum; inclusion; spall; shock response; microstructure; molecular dynamics; MOLECULAR-DYNAMICS; FRACTURE; AL; MICROSTRUCTURE; DAMAGE; DEFORMATION; STRENGTH; SIZE; INCLUSIONS; EVOLUTION;
D O I
10.3390/nano11102603
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
In this study, the effects of Cu nanoparticle inclusion on the dynamic responses of single crystal Al during shockwave loading and subsequent spallation processes have been explored by molecular dynamics simulations. At specific impact velocities, the ideal single crystal Al will not produce dislocation and stacking fault structure during shock compression, while Cu inclusion in an Al-Cu nanocomposite will lead to the formation of a regular stacking fault structure. The significant difference of a shock-induced microstructure makes the spall strength of the Al-Cu nanocomposite lower than that of ideal single crystal Al at these specific impact velocities. The analysis of the damage evolution process shows that when piston velocity u(p) <= 2.0 km/s, due to the dense defects and high potential energy at the interface between inclusions and matrix, voids will nucleate preferentially at the inclusion interface, and then grow along the interface at a rate of five times faster than other voids in the Al matrix. When u(p) >= 2.5 km/s, the Al matrix will shock melt or unloading melt, and micro-spallation occurs; Cu inclusions have no effect on spallation strength, but when Cu inclusions and the Al matrix are not fully diffused, the voids tend to grow and coalescence along the inclusion interface to form a large void.
引用
收藏
页数:16
相关论文
共 50 条
  • [21] Atomistic simulations of tension properties for bi-crystal copper with twist grain boundary
    Liu, X. M.
    You, X. C.
    Liu, Z. L.
    Nie, J. F.
    Zhuang, Z.
    JOURNAL OF PHYSICS D-APPLIED PHYSICS, 2009, 42 (03)
  • [22] A methodology to generate crystal-based molecular structures for atomistic simulations
    Negre, Christian F. A.
    Alvarado, Andrew
    Singh, Himanshu
    Finkelstein, Joshua
    Martinez, Enrique
    Perriot, Romain
    JOURNAL OF PHYSICS-CONDENSED MATTER, 2023, 35 (22)
  • [23] Effect of material damage on the spallation threshold of single crystal copper: a molecular dynamics study
    Rawat, S.
    Warrier, M.
    Chaturvedi, S.
    Chavan, V. M.
    MODELLING AND SIMULATION IN MATERIALS SCIENCE AND ENGINEERING, 2012, 20 (01)
  • [24] A metastable phase of shocked bulk single crystal copper: an atomistic simulation study
    Neogi, Anupam
    Mitra, Nilanjan
    SCIENTIFIC REPORTS, 2017, 7
  • [25] R-curve Evaluation of Copper and Nickel Single Crystals Using Atomistic Simulations
    Zhuo, Xiao Ru
    Kim, Jang Hyun
    Beom, Hyeon Gyu
    CRYSTALS, 2018, 8 (12):
  • [26] A metastable phase of shocked bulk single crystal copper: an atomistic simulation study
    Anupam Neogi
    Nilanjan Mitra
    Scientific Reports, 7
  • [27] Investigations on the damping of acoustic vibrations of single gold nanoparticles in water by continuum and atomistic simulations
    Gan, Yong
    Cai, Hao
    MATERIALS TODAY COMMUNICATIONS, 2023, 34
  • [28] Single Crystal Copper Nanocrystallization and Sintered with Silver Nanoparticles
    Zhou Wei
    Zheng Zhen
    Wang Chunqing
    2016 17TH INTERNATIONAL CONFERENCE ON ELECTRONIC PACKAGING TECHNOLOGY (ICEPT), 2016, : 1015 - 1017
  • [29] Atomistic simulations of tensile and bending properties of single-crystal bcc iron nanobeams
    Olsson, Par A. T.
    Melin, Solveig
    Persson, Christer
    PHYSICAL REVIEW B, 2007, 76 (22)
  • [30] Atomistic simulations of displacement cascades in Y2O3 single crystal
    Dholakia, Manan
    Chandra, Sharat
    Valsakumar, M. C.
    Jaya, S. Mathi
    JOURNAL OF NUCLEAR MATERIALS, 2014, 454 (1-3) : 96 - 104