Volume 40 Issue 3
Mar.  2020
Turn off MathJax
Article Contents
KAN Mingxian, WANG Ganghua, XIAO Bo, DUAN Shuchao, ZHANG Zhaohui. Simulation on magnetically-driven one-sided flyer plate experiments[J]. Explosion And Shock Waves, 2020, 40(3): 033304. doi: 10.11883/bzycj-2019-0103
Citation: KAN Mingxian, WANG Ganghua, XIAO Bo, DUAN Shuchao, ZHANG Zhaohui. Simulation on magnetically-driven one-sided flyer plate experiments[J]. Explosion And Shock Waves, 2020, 40(3): 033304. doi: 10.11883/bzycj-2019-0103

Simulation on magnetically-driven one-sided flyer plate experiments

doi: 10.11883/bzycj-2019-0103
  • Received Date: 2019-04-01
  • Rev Recd Date: 2019-11-18
  • Available Online: 2020-02-25
  • Publish Date: 2020-03-01
  • The numerical simulation of magnetically driven one-sided flyer plate experiment usually does not take into account the influences of cathode motion and ablation width in the thickness direction on the boundary magnetic field. Hence, one-sided computational model was usually applied to simulate magnetically driven one-sided flyer plate experiment. In order to understand the reason why magnetically driven one-sided flyer plate experiment can be simulated by one-sided computational model, magnetically driven one-sided flyer plate experiment (experiment PTS-061 with a 0.972-mm-thick aluminum flyer plate and experiment PTS-064 with a 1.041-mm-thick aluminum flyer plate) were simulated by two-sided computational model. In the experiments with experiment PTS-061 and PTS-064, displacement of thin flyer plate current-loading surface increases with time; displacement of thick cathode current-loading surface does not increases with time, and remains basically unchanged with small displacement in the middle and late stage of experiments. At the end of experiment PTS-061, displacement of thin flyer plate current-loading surface is 4.9 mm, and displacement of thick cathode current-loading surface is only 1.7 mm. At the end of experiment PTS-064, displacement of thin flyer plate current-loading surface is 4.1 mm, and displacement of thick cathode current-loading surface is only 0.9 mm. The reason of one-sided computational model can be adopted in magnetically driven one-sided flyer plate experiment is not that cathode plate position remains unchanged, but instead that cathode current-loading surface has smaller displacement remaining basically unchanged in the middle and later stage of experiments, and the displacement of thin flyer plate current-loading surface has a greater influence on the boundary magnetic field that of thick cathode current-loading surface in the late stage of experiments.
  • loading
  • [1]
    KNUDSON M D, LEMKE R W, HAYES D B, et al. Near-absolute Hugoniot measurements in aluminum to 500 GPa using a magnetically accelerated flyer plate technique [J]. Journal of Applied Physics, 2003, 94(7): 4420–4431. DOI: 10.1063/1.1604967.
    [2]
    LEMKE R W, KNUDSON M D, BLISS D E, et al. Magnetically accelerated, ultrahigh velocity flyer plates for shock wave experiments [J]. Journal of Applied Physics, 2005, 98: 073530. DOI: 10.1063/1.2084316.
    [3]
    KNUDSON M D, HANSON D L, BAILEY J E, et al. Equation of state measurements in liquid Deuterium to 70 GPa [J]. Physical Review Letters, 2001, 87: 225501. DOI: 10.1103/PhysRevLett.87.225501.
    [4]
    KNUDSON M D, HANSON D L, BAILEY J E, et al. Use of a wave reverberation technique to infer the density compression of shocked liquid deuterium to 75 GPa [J]. Physical Review Letters, 2003, 90: 035505. DOI: 10.1103/PhysRevLett.90.035505.
    [5]
    KNUDSON M D, HANSON D L, BAILEY J E, et al. Principal Hugoniot, reverberating wave, and mechanical reshock measurements of liquid deuterium to 400 GPa using plate impact techniques [J]. Physical Review B, 2004, 69: 144209. DOI: 10.1103/PhysRevB.69.144209.
    [6]
    LEMKE R W, KNUDSON M D, HALL C A, et al. Characterization of magnetically accelerated flyer plates [J]. Physics of Plasmas, 2003, 10(4): 1092–1099. DOI: 10.1063/1.1554740.
    [7]
    LEMKE R W, KNUDSON M D, DAVIS J P. Magnetically driven hyper-velocity launch capability at the Sandia Z accelerator [J]. International Journal of Impact Engineering, 2011, 38(6): 480–485. DOI: 10.1016/j.ijimpeng.2010.10.019.
    [8]
    DAVIS J P, BROWN J L, KNUDSON M D, et al. Analysis of shockless dynamic compression data on solids to multi-megabar pressures: application to tantalum [J]. Journal of Applied Physics, 2014, 116: 204903. DOI: 10.1063/1.4902863.
    [9]
    KAN M X, ZHANG Z H, XIAO B, et al. Simulation of magnetically driven flyer plate experiments with an improved magnetic field boundary formula [J]. High Energy Density Physics, 2018, 26: 38–43. DOI: 10.1016/j.hedp.2017.12.002.
    [10]
    DENG J J, XIE W P, FENG S P, et al. Initial performance of the Primary Test Stand [J]. IEEE TPS, 2013, 41(10): 2580–2583.
    [11]
    但加坤, 任晓东, 黄显宾, 等. Z箍缩内爆产生的电磁脉冲辐射 [J]. 物理学报, 2013, 62(24): 245201. DOI: 10.7498/aps.62.245201.

    DAN J K, REN X D, HUANG X B, et al. Electromagnetic pulse emission produced by Z pinch implosions [J]. Acta Physica Sinica, 2013, 62(24): 245201. DOI: 10.7498/aps.62.245201.
    [12]
    郭帅, 王贵林, 张朝辉, 等. 聚龙一号装置准等熵压缩实验负载优化研究 [J]. 强激光与粒子束, 2016, 28(1): 015015. DOI: 10.11884/HPLPB201628.015015.

    GUO S, WANG G L, ZHANG Z H, et al. Optimization of load configurations for isentropic compression experiments on PTS [J]. High Power Laser and Particle Beams, 2016, 28(1): 015015. DOI: 10.11884/HPLPB201628.015015.
    [13]
    王贵林, 张朝辉, 郭帅, 等. 聚龙一号装置上铜的准等熵压缩线测量实验研究 [J]. 强激光与粒子束, 2016, 28(5): 055010. DOI: 10.11884/HPLPB201628.055010.

    WANG G L, ZHANG Z H, GUO S, et al. Experimental measurement of quasi-isentrope for copper on PTS [J]. High Power Laser and Particle Beams, 2016, 28(5): 055010. DOI: 10.11884/HPLPB201628.055010.
    [14]
    阚明先, 蒋吉昊, 王刚华, 等. 套筒内爆ALE方法二维MHD数值模拟 [J]. 四川大学学报, 2007, 44(1): 91–96. DOI: 10.3969/j.issn.0490-6756.2007.01.020.

    KAN M X, JIANG J H, WANG G H, et al. ALE simulation 2D MHD for liner [J]. Journal of Sichuan University, 2007, 44(1): 91–96. DOI: 10.3969/j.issn.0490-6756.2007.01.020.
    [15]
    阚明先, 王刚华, 赵海龙, 等. 磁驱动飞片二维磁流体力学数值模拟 [J]. 强激光与粒子束, 2013, 25(8): 2137–2141. DOI: 10.3788/HPLPB20132508.2137.

    KAN M X, WANG G H, ZHAO H L, et al. Two dimensional magneto-hydrodynamic simulations of magnetically accelerated flyer plates [J]. High Power Laser and Particle Beams, 2013, 25(8): 2137–2141. DOI: 10.3788/HPLPB20132508.2137.
    [16]
    杨龙, 王刚华, 阚明先, 等. 基于MDSC程序的Z箍缩内爆单温和三温模拟分析 [J]. 高压物理学报, 2016, 30(1): 64–70. DOI: 10.11858/gywlxb.2016.01.010.

    YANG L, WANG G H, KAN M X, et al. A numerical simulation analysis of mono-temperature and tri-temperature models by MDSC program Z-pinch implosion [J]. Chinese Journal of High Pressure Physics, 2016, 30(1): 64–70. DOI: 10.11858/gywlxb.2016.01.010.
    [17]
    阚明先, 张朝辉, 段书超, 等. “聚龙一号”装置上磁驱动铝飞片实验的数值模拟 [J]. 强激光与粒子束, 2015, 27(12): 125001. DOI: 10.11884/HPLPB201527.125001.

    KAN M X, ZHANG Z H, DUAN S C, et al. Numerical simulation of magnetically driven aluminum flyer plate on PTS accelerator [J]. High Power Laser and Particle Beams, 2015, 27(12): 125001. DOI: 10.11884/HPLPB201527.125001.
    [18]
    阚明先, 段书超, 王刚华, 等. 自由面被烧蚀磁驱动飞片的数值模拟 [J]. 强激光与粒子束, 2017, 29(4): 045003. DOI: 10.11884/HPLPB201729.160482.

    KAN M X, DUAN S C, WANG G H, et al. Numerical simulation of magnetically driven flyer plate of ablated free surface [J]. High Power Laser and Particle Beams, 2017, 29(4): 045003. DOI: 10.11884/HPLPB201729.160482.
    [19]
    阚明先, 王刚华, 赵海龙, 等. 金属电阻率模型 [J]. 爆炸与冲击, 2013, 33(3): 282–286. DOI: 10.11883/1001-1145(2013)03-0282-05.

    KAN M X, WANG G H, ZHAO H L, et al. Electrical resistivity model for metals [J]. Explosion and Shock Waves, 2013, 33(3): 282–286. DOI: 10.11883/1001-1145(2013)03-0282-05.
  • 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(13)  / Tables(1)

    Article Metrics

    Article views (5535) PDF downloads(72) Cited by()
    Proportional views
    Related

    /

    DownLoad:  Full-Size Img  PowerPoint
    Return
    Return