Volume 42 Issue 3
Apr.  2022
Turn off MathJax
Article Contents
LIU Jun, SUN Zhiyuan, ZHANG Fengguo, WANG Pei. Simulation study of the recompression of metal spallation zone[J]. Explosion And Shock Waves, 2022, 42(3): 033101. doi: 10.11883/bzycj-2021-0262
Citation: LIU Jun, SUN Zhiyuan, ZHANG Fengguo, WANG Pei. Simulation study of the recompression of metal spallation zone[J]. Explosion And Shock Waves, 2022, 42(3): 033101. doi: 10.11883/bzycj-2021-0262

Simulation study of the recompression of metal spallation zone

doi: 10.11883/bzycj-2021-0262
  • Received Date: 2021-06-28
  • Rev Recd Date: 2021-10-28
  • Available Online: 2021-12-29
  • Publish Date: 2022-04-07
  • Metal spallation phenomenon often occurs when shock waves are reflected and unloaded on a free surface. If there is a secondary shock wave impact, the metal spallation zone will be compressed again, and the metal in the tensile state will be gradually recompressed into a dense material until the spallation zone disappears. The above process is referred to as the recompression process of the metal spallation zone. The main difficulty of the recompression process simulation is that the initial tensile state of the spallation zone is hard to be determined, and it is difficult to accurately measure the recompaction state experimentally. These bring great difficulties in verifying the reliability of macro-simulations under complex loading. In this case, direct numerical simulations with the ability to describe the internal details of the spallation zone become an effective means to verify the reliability of the macro-simulation. Firstly, in direct simulation modeling, the initial tensile state of the metal spallation zone is set to three situations: containing only spalls, only holes, and both holes and spalls. After that, through direct numerical simulations of different porosity, recompression rate, number of spalls and number of holes, the recompression states of the metal spallation zone under the corresponding working conditions are statistically obtained. Finally, under the condition that the constitutive model and parameters of the direct simulation and macro-simulation have good comparability, macro-modeling and simulation analysis of the spallation recompression process are carried out. The results show that: if there are spalls in the spallation zone, the macro-simulation can better simulate the recompression process and the state of the metal spallation zone when the mesh fracture post-processing algorithm is "set stress to zero and keep temperature constant". If the initial state of the recompression process contains only holes, then macro-simulations cannot well simulate the recompression process and the recompression state no matter whether the hole collapse forms surface material ejections or not.
  • loading
  • [1]
    HOLTKAMP D B, CLARK D A, FERM E N, et al. A surver of high explosive-induced damage and spall in selected metals using proton radiography [C]// AIP Conference Proceedings: Shock Compression of Condersed Matter, 2003: 477−482. DOI: 10.1063/1.1780281.
    [2]
    HOLTKAMP D B, CLARK D A, CRAIN M D, et al. Development of a non-radiographic spall and damage diagnotic [C]// AIP Conference Proceedings, Shock Compression of Condersed Matter, 2003: 473−476. DOI: 10.1063/1.1780280.
    [3]
    RESSEGUIER T D, SIGNOR L, DRAGON A, et al. Experimental inverstigation of liquid spall in laser shock-loaded tin [J]. Journal of Applied Physics, 2007, 101: 013506. DOI: 10.1063/1.2400800.
    [4]
    张凤国, 刘军, 王裴, 等. 三角波强加载下延性金属多次层裂破坏问题 [J]. 爆炸与冲击, 2018, 38(3): 659–664. DOI: 10.11883/bzycj-2016-0279.

    ZHANG F G, LIU J, WANG P, et al. Multi-spall in ductile metal under triangular impulse loading [J]. Explosion and Shock Waves, 2018, 38(3): 659–664. DOI: 10.11883/bzycj-2016-0279.
    [5]
    贺年丰, 任国武, 陈永涛, 等. 爆轰加载下金属锡层裂破碎数值模拟 [J]. 爆炸与冲击, 2019, 39(4): 042101. DOI: 10.11883/bzycj-2017-0354.

    HE N F, REN G W, CHEN Y T, et al. Numerical simulation on spallation and fragmentation of tin under explosive loading [J]. Explosion and Shock Waves, 2019, 39(4): 042101. DOI: 10.11883/bzycj-2017-0354.
    [6]
    杨扬, 彭志强, 郭昭亮, 等. 滑移爆轰条件下高纯铜的层裂行为 [J]. 材料科学与工程学报, 2016, 34(1): 32–37.

    YANG Y, PENG Z Q, GUO Z L, et al. Spall behaviors of high purity copper under sweeping detonation [J]. Materials Science and Engineering: A, 2016, 34(1): 32–37.
    [7]
    ANDRIOT P, CHAPRON P, LAMBERT V, et al. Influence of melting on shocked free surface behavior using Doppler laser interferometry and X-ray densitometry [C]// AIP Conference Proceedings: Shock Waves in Condensed Matter, 1983: 277−280. DOI: 10.1016/b978-0-444-86904-3.50065-8.
    [8]
    REMIOT C, CHAPRON P, DEMAY B. A flash X-ray radiography diagnostic for studying surface phenomena under shock loading [C]// AIP Conference Proceedings, Shock Waves in Condensed Matter, 1994: 1763−1766. DOI: 10.1063/1.46171.
    [9]
    陈永涛, 胡海波, 汤铁钢, 等. 强冲击加载下铅样品表面微层裂现象诊断 [J]. 中国科学: 物理学 力学 天文学, 2012, 42: 1076–1085.

    CEHN Y T, HU H B, TANG T G, et al. Experimental diagnostic of micro-spall fragments on Pb surface under intense shock [J]. Science China: Physics Mechanics & Astronomy, 2012, 42: 1076–1085.
    [10]
    陈永涛, 任国武, 汤铁钢, 等. 爆轰加载下金属样品的熔化破碎现象诊断 [J]. 物理学报, 2013, 62(11): 116202. DOI: 10.7498/aps.62.116202.

    CHEN Y T, REN G W, TANG T G, et al. Experimental diagnostic of melting fragments under explosive loading [J]. Acta Physica Sinica, 2013, 62(11): 116202. DOI: 10.7498/aps.62.116202.
    [11]
    CHEN Y T, REN G W, TANG T G, et al. Experimental study of micro-spalling fragmentation from melted lead [J]. Shock Waves, 2016, 26: 221–225. DOI: 10.1007/s00193-015-0601-4.
    [12]
    张崇玉, 胡海波, 王 翔. 铅飞层中斜冲击波对碰马赫反射行为实验研究 [J]. 爆炸与冲击, 2019, 39(4): 043102.

    ZHANG C Y, HU H B, WANG X, et al. Experimental study of Mach reflection induced by collision of oblique shock waves in a lead plate [J]. Explosion and Shock Waves, 2019, 39(4): 043102.
    [13]
    XIANG M Z, HU H B, CHEN J. Molecular dynamics studies of thermal dissipation during shock induced spalling [J]. Journal of Applied Physics, 2013, 113(16): 163507–6. DOI: 10.1063/1.4821341.
    [14]
    SEAMAN L, CURRAN D R, SHOCKEY D A. Computational models for ductile and brittle fracture [J]. Journal of Applied Physics, 1976, 47(11): 4814–4826. DOI: 10.1063/1.322523.
    [15]
    GURSON A L. Continuum theory of ductile rupture by void nucleation and growth: Part Ⅰ: yield criteria and flow rules for porous ductile media [J]. Journal of Engineering Materials and Technology, 1977, 99(1): 2–15. DOI: 10.1115/1.3443401.
    [16]
    TONKS D L, ZUREK A K, THISSELL W R. Void coalescence model for ductile damage [C]// AIP Conference Proceedings: Shock Compression of Condensed Matter. 2002: 611–614. DOI: 10.1063/1.1483613.
    [17]
    MOLINARI A, WRIGHT T. A physical model for nucleation and early growth of voids in ductile materials under dynamic loading [J]. Journal of the Mechanics and Physics of Solids, 2005, 53(7): 1476–1504. DOI: 10.1016/j.jmps.2005.02.010.
    [18]
    HERRMANN W. Constitutive equation for the dynamic compaction of ductile porous materials [J]. Journal of Applied Physics, 1969, 40(6): 2490–9. DOI: 10.1063/1.1658021.
    [19]
    CARROLL M M, HOLT A C. Static and dynamic pore-collapse relations for ductile porous materials [J]. Journal of Applied Physics, 1972, 43(4): 1626–36. DOI: 10.1063/1.1661372.
    [20]
    WUENNEMANN K, COLLINS G S, MELOSH H J. A novel porosity model for use in hydrocode simulations: 20050180812 [R].USA: Lunar and Planetary Science Ⅹ Ⅹ Ⅹ Ⅵ, Part 21, 2005.
    [21]
    COLLINS G S, MELOSH H J, WUNNEMANN K, et al. Improvements to the ε-α porous compaction model for simulation impacts into high-porosity solar system objects [J]. International Journal of Impact Engineering, 2011, 38: 434–439. DOI: 10.1016/j.ijimpeng.2010.10.013.
    [22]
    何长江, 于志鲁, 冯其京. 高速碰撞的三维欧拉数值模拟方法 [J]. 爆炸与冲击, 1999, 19(3): 216–221.

    HE C J, YU Z L, FENG Q J. 3D Eulerian numerical simulation method of high speed impact [J]. Explosion and Shock Waves, 1999, 19(3): 216–221.
    [23]
    冯其京, 郝鹏程, 杭义洪, 等. 聚能装药的欧拉数值模拟 [J]. 爆炸与冲击, 2008, 28(2): 138–143. DOI: 10.11883/1001-1455(2008)02-0138-06.

    FENG Q J, HAO P C, HANG Y H, et al. Eulerian numerical simulation of a shaped charge [J]. Explosion and Shock Waves, 2008, 28(2): 138–143. DOI: 10.11883/1001-1455(2008)02-0138-06.
    [24]
    刘军, 王裴, 王言金. L-R两步欧拉方法在铝材料微喷射中的应用 [J]. 高压物理学报, 2014, 28(3): 346–352. DOI: 10.11858/gywlxb.2014.03.013.

    LIU J, WANG P, WANG Y J. Application of L-R two-step Euler method to micro ejection of aluminum [J]. Chinese Journal of High Pressure Physics, 2014, 28(3): 346–352. DOI: 10.11858/gywlxb.2014.03.013.
    [25]
    HE A M, LIU J, LIU C, WANG P. Numerical and theoretical investigation of jet formation in lastic-plastic solids [J]. Journal of Applied Physics, 2018, 124: 185902. DOI: 10.1063/1.5051527.
    [26]
    STEINBERG D J. Equation of state and strength properties of selected materials: UCRL-MA-106439 [R]. USA: Lawrence Livermore National Laboratory, 1991.
    [27]
    WHIRLEY R G, ENGELMANN B E. DYNA2D: a nonlinear, explicit, two dimensional finite element code for solid mechanics: UCRL-MA-110630 [R]. USA : NASA STI Technical Report, 1992.
  • 加载中

Catalog

    通讯作者: 陈斌, bchen63@163.com
    • 1. 

      沈阳化工大学材料科学与工程学院 沈阳 110142

    1. 本站搜索
    2. 百度学术搜索
    3. 万方数据库搜索
    4. CNKI搜索

    Figures(15)  / Tables(2)

    Article Metrics

    Article views (389) PDF downloads(94) Cited by()
    Proportional views
    Related

    /

    DownLoad:  Full-Size Img  PowerPoint
    Return
    Return