搜索

x

留言板

尊敬的读者、作者、审稿人, 关于本刊的投稿、审稿、编辑和出版的任何问题, 您可以本页添加留言。我们将尽快给您答复。谢谢您的支持!

姓名
邮箱
手机号码
标题
留言内容
验证码

爆轰加载下弹塑性固体Richtmyer-Meshkov流动的扰动增长规律

殷建伟 潘昊 吴子辉 郝鹏程 胡晓棉

引用本文:
Citation:

爆轰加载下弹塑性固体Richtmyer-Meshkov流动的扰动增长规律

殷建伟, 潘昊, 吴子辉, 郝鹏程, 胡晓棉

A growth study of the Richtmyer-Meshkov flow in the elastoplastic solids under explosive loading

Yin Jian-Wei, Pan Hao, Wu Zi-Hui, Hao Peng-Cheng, Hu Xiao-Mian
PDF
导出引用
  • 研究了冲击波加载弹塑性材料扰动自由面的动力学演化过程,分析了高能炸药爆轰驱动时初始扰动与材料性质对扰动增长的影响.研究结果表明:初始扰动的振幅与波长之比越高,扰动越易增长,强度越高的材料扰动增长幅度越小;扰动增长被抑制时,尖钉的最大振幅与增长速度无量纲数之间存在线性近似关系,进一步理论分析表明尖钉的振幅增长因子与加载压力、初始扰动形态和材料强度有关,该理论关系作为扰动增长规律的线性近似在一定范围内适用于多种金属材料.
    In this paper, a theoretical analysis model is proposed for the linear growth of the Richtmyer-Meshkov instability in elastoplastic solid medium-vacuum interface under the explosion shock wave loading. The analysis of the dynamic evolution of small perturbations shows that after the initial phase inversion, some perturbations would stop growing after they have reached their maximum amplitude, some others would continue to grow and then form jetting from the solid-vacuum interfaces. Numerical simulations show excellent agreement with the experimental results of explosively-driven Richtmyer-Meshkov instability in the sample of copper. The effects of two physical factors on the maximum amplitude of spikes are also studied numerically. The first physical factor is the initial configuration of the perturbation, which is expressed as the time values of the initial wave number and initial amplitude. With increasing the value of the initial configuration, the maximum amplitudes of the spikes would become greater while the growth of perturbations is suppressed. On the other hand, the maximum amplitudes of spikes would become smaller in the solid which has a higher yield strength when the initial configuration keeps unchanged. Further investigations show that the boundary of the stage division between the stable growth and the unstable growth is revealed by a combination parameter form of the two physical factors, which is expressed as the ratio of initial configuration to yield strength. In the stable stage, the linear relation between the non-dimensional maximum amplitude and the non-dimensional maximum growth rate of the spikes is fitted with the coefficient value 0.30, which is very close to 0.29, a theoretical prediction based on the Newton's second law analysis. Considering the shock Hugoniot relations in the elastoplastic medium and the maximum growth rate equation of the Richtmyer-Meshkov instability in ideal fluid, the linear model is improved to add the effects of the loading shockwave pressure and the compression acoustic impedance of the material on the amplitude growth of the spike to the analytical model proposed by the former researchers. Extensive numerical simulations are performed to show that the linear model could accurately describe the growth factor of the spikes in the stable cases in different metal materials, such as copper, aluminum, and stain-less steels. In the numerical analysis of the scope of application of the linear model, a rough estimation of the stage division boundary between the stable and unstable growth is given as 0.8 GPa-1. When the ratio of initial configuration to yield strength is lower than the division boundary, the perturbation growth would be stable and the linear model could describe the growth law of the spikes.
      通信作者: 胡晓棉, hu_xiaomian@iapcm.ac.cn
    • 基金项目: 国家自然科学基金(批准号:11272064)资助的课题.
      Corresponding author: Hu Xiao-Mian, hu_xiaomian@iapcm.ac.cn
    • Funds: Project supported by the National Natural Science Foundation of China (Grant No. 11272064).
    [1]

    Richtmyer R D 1960 Commun. Pure Appl. Math. 13 297

    [2]

    Meshkov E E 1969 Sovit. Fluid Dyn. 4 151

    [3]

    Mikaelian K O 2013 Phys. Rev. E 87 031003

    [4]

    Brouillette M 2002 Annu. Rev. Fluid Mech. 34 445

    [5]

    Piriz A R, Lopez Cela J J, Tahir N A, Hoffmann D H H 2006 Phys. Rev. E 74 037301

    [6]

    Piriz A R, Lopez Cela J J, Cortazar O D, Tahir N A, Hoffmann D H H 2005 Phys. Rev. E 72 056313

    [7]

    Piriz A R, Lopez Cela J J, Tahir N A, Hoffmann D H H 2008 Phys. Rev. E 78 056401

    [8]

    Piriz A R, Lopez Cela J J, Tahir N A 2009 Phys. Rev. E 80 046305

    [9]

    Lopez Ortega A, Lombardini M, Pullin D I, Meiron D I 2014 Phys. Rev. E 89 033018

    [10]

    Remington B A, Rudd E R, Wark J S 2015 Phys. Plasmas 22 090501

    [11]

    Buttler W T, Oro D M, Preston D L, Mikaelian K O, Cherne F J, Hixson R S, Mariam F G, Morris C, Stone J B, Terrones G, Tupa D 2012 J. Fluid Mech. 703 60

    [12]

    Buttler W T, Oro D M, Olsen R T, Cheren F J, Hammerberg J E, Hixson R S, Monfared S K, Pack C L, Rigg P A, Stone J B, Terrones G 2014 J. Appl. Phys. 116 103519

    [13]

    Dimonte G, Terrones G, Cheren F J, Germann T C, Dunpont V, Kadau K, Buttler W T, Oro D M, Morris C, Preston D L 2011 Phys. Rev. Lett. 107 264502

    [14]

    Jensen B J, Cheren F J, Prime M B, Fezzaa K, Iverson A J, Carlson C A, Yeager J D, Ramos K J, Hooks D E, Cooley J C, Dimonte G 2015 J. Appl. Phys. 118 195903

    [15]

    Sun Z F, Xu H, Li Q Z, Zhang C Y 2010 Chin. J. High Pressure Phys. 24 55 (in Chinese)[孙占峰, 徐辉, 李庆忠, 张崇玉2010高压物理学报24 55]

    [16]

    Robinson A C, Swegle J W, 1989 J. Appl. Phys. 66 2838

    [17]

    Zhu J S, Hu X M, Wang P, Chen J, Xu A G 2010 Adv. Mech. 40 400 (in Chinese)[朱建士, 胡晓棉, 王裴, 陈军, 许爱国2010力学进展40 400]

    [18]

    Vogler T J, Chhabildas L C 2006 Int. J. Impact Engng. 33 812

    [19]

    Barton N R, Bernier J V, Becker R, Arsenlis A, Cavallo R, Marian J, Rhee M, Park H S, Remington B A, Olson R T 2011 J. Appl. Phys. 109 073501

    [20]

    Smith R F, Eggert J H, Rudd R E, Swift D C, Blome C A, Collins G W 2011 J. Appl. Phys. 110 123515

    [21]

    Park H S, Rudd R E, Cavallo R M, Barton N R, Arsenlis A, Belof J L, Blobaum K J M, El-dasher B S, Florando J N, Huntington C M, Maddox B R, May M J, Plechaty C, Prisbrey S T, Remington B A, Wallace R J, Wehrenberg C E, Wilson M J, Comley A J, Giraldex E, Nikroo A, Farrell M, Randall G, Gray III G T 2015 Phys. Rev. Lett. 114 065502

    [22]

    Wouchuk J G 2001 Phys. Rev. E 63 056303

    [23]

    Pan H, Wu Z H, Hu X M, Yang K 2013 Chin. J. High Pressure Phys. 27 778 (in Chinese)[潘昊, 吴子辉, 胡晓棉, 杨堃2013高压物理学报27 778]

    [24]

    Pan H, Hu X M, Wu Z H, Dai C D, Wu Q 2012 Acta Phys. Sin. 61 206401 (in Chinese)[潘昊, 胡晓棉, 吴子辉, 戴诚达, 吴强2012物理学报61 206401]

    [25]

    Yu Y Y, Tan H, Hu J B, Dai C D, Chen D N, Wang H R 2008 Acta Phys. Sin. 57 2352 (in Chinese)[俞宇颖, 谭华, 胡建波, 戴诚达, 陈大年, 王焕然2008物理学报57 2352]

    [26]

    Colvin J D, Legrand M, Remington B A, Schurtz G, Weber S V 2003 J. Appl. Phys. 93 5287

  • [1]

    Richtmyer R D 1960 Commun. Pure Appl. Math. 13 297

    [2]

    Meshkov E E 1969 Sovit. Fluid Dyn. 4 151

    [3]

    Mikaelian K O 2013 Phys. Rev. E 87 031003

    [4]

    Brouillette M 2002 Annu. Rev. Fluid Mech. 34 445

    [5]

    Piriz A R, Lopez Cela J J, Tahir N A, Hoffmann D H H 2006 Phys. Rev. E 74 037301

    [6]

    Piriz A R, Lopez Cela J J, Cortazar O D, Tahir N A, Hoffmann D H H 2005 Phys. Rev. E 72 056313

    [7]

    Piriz A R, Lopez Cela J J, Tahir N A, Hoffmann D H H 2008 Phys. Rev. E 78 056401

    [8]

    Piriz A R, Lopez Cela J J, Tahir N A 2009 Phys. Rev. E 80 046305

    [9]

    Lopez Ortega A, Lombardini M, Pullin D I, Meiron D I 2014 Phys. Rev. E 89 033018

    [10]

    Remington B A, Rudd E R, Wark J S 2015 Phys. Plasmas 22 090501

    [11]

    Buttler W T, Oro D M, Preston D L, Mikaelian K O, Cherne F J, Hixson R S, Mariam F G, Morris C, Stone J B, Terrones G, Tupa D 2012 J. Fluid Mech. 703 60

    [12]

    Buttler W T, Oro D M, Olsen R T, Cheren F J, Hammerberg J E, Hixson R S, Monfared S K, Pack C L, Rigg P A, Stone J B, Terrones G 2014 J. Appl. Phys. 116 103519

    [13]

    Dimonte G, Terrones G, Cheren F J, Germann T C, Dunpont V, Kadau K, Buttler W T, Oro D M, Morris C, Preston D L 2011 Phys. Rev. Lett. 107 264502

    [14]

    Jensen B J, Cheren F J, Prime M B, Fezzaa K, Iverson A J, Carlson C A, Yeager J D, Ramos K J, Hooks D E, Cooley J C, Dimonte G 2015 J. Appl. Phys. 118 195903

    [15]

    Sun Z F, Xu H, Li Q Z, Zhang C Y 2010 Chin. J. High Pressure Phys. 24 55 (in Chinese)[孙占峰, 徐辉, 李庆忠, 张崇玉2010高压物理学报24 55]

    [16]

    Robinson A C, Swegle J W, 1989 J. Appl. Phys. 66 2838

    [17]

    Zhu J S, Hu X M, Wang P, Chen J, Xu A G 2010 Adv. Mech. 40 400 (in Chinese)[朱建士, 胡晓棉, 王裴, 陈军, 许爱国2010力学进展40 400]

    [18]

    Vogler T J, Chhabildas L C 2006 Int. J. Impact Engng. 33 812

    [19]

    Barton N R, Bernier J V, Becker R, Arsenlis A, Cavallo R, Marian J, Rhee M, Park H S, Remington B A, Olson R T 2011 J. Appl. Phys. 109 073501

    [20]

    Smith R F, Eggert J H, Rudd R E, Swift D C, Blome C A, Collins G W 2011 J. Appl. Phys. 110 123515

    [21]

    Park H S, Rudd R E, Cavallo R M, Barton N R, Arsenlis A, Belof J L, Blobaum K J M, El-dasher B S, Florando J N, Huntington C M, Maddox B R, May M J, Plechaty C, Prisbrey S T, Remington B A, Wallace R J, Wehrenberg C E, Wilson M J, Comley A J, Giraldex E, Nikroo A, Farrell M, Randall G, Gray III G T 2015 Phys. Rev. Lett. 114 065502

    [22]

    Wouchuk J G 2001 Phys. Rev. E 63 056303

    [23]

    Pan H, Wu Z H, Hu X M, Yang K 2013 Chin. J. High Pressure Phys. 27 778 (in Chinese)[潘昊, 吴子辉, 胡晓棉, 杨堃2013高压物理学报27 778]

    [24]

    Pan H, Hu X M, Wu Z H, Dai C D, Wu Q 2012 Acta Phys. Sin. 61 206401 (in Chinese)[潘昊, 胡晓棉, 吴子辉, 戴诚达, 吴强2012物理学报61 206401]

    [25]

    Yu Y Y, Tan H, Hu J B, Dai C D, Chen D N, Wang H R 2008 Acta Phys. Sin. 57 2352 (in Chinese)[俞宇颖, 谭华, 胡建波, 戴诚达, 陈大年, 王焕然2008物理学报57 2352]

    [26]

    Colvin J D, Legrand M, Remington B A, Schurtz G, Weber S V 2003 J. Appl. Phys. 93 5287

计量
  • 文章访问数:  4372
  • PDF下载量:  220
  • 被引次数: 0
出版历程
  • 收稿日期:  2016-09-03
  • 修回日期:  2017-01-06
  • 刊出日期:  2017-04-05

/

返回文章
返回