磁驱动平面准等熵加载装置、实验技术及应用研究新进展

王桂吉 罗斌强 陈学秒 张旭平 种涛 蔡进涛 谭福利 孙承纬

王桂吉, 罗斌强, 陈学秒, 张旭平, 种涛, 蔡进涛, 谭福利, 孙承纬. 磁驱动平面准等熵加载装置、实验技术及应用研究新进展[J]. 爆炸与冲击, 2021, 41(12): 121403. doi: 10.11883/bzycj-2021-0119
引用本文: 王桂吉, 罗斌强, 陈学秒, 张旭平, 种涛, 蔡进涛, 谭福利, 孙承纬. 磁驱动平面准等熵加载装置、实验技术及应用研究新进展[J]. 爆炸与冲击, 2021, 41(12): 121403. doi: 10.11883/bzycj-2021-0119
WANG Guiji, LUO Binqiang, CHEN Xuemiao, ZHANG Xuping, CHONG Tao, CAI Jintao, TAN Fuli, SUN Chengwei. Recent progress on the experimental facilities, techniques and applications of magnetically driven quasi-isentropic compression[J]. Explosion And Shock Waves, 2021, 41(12): 121403. doi: 10.11883/bzycj-2021-0119
Citation: WANG Guiji, LUO Binqiang, CHEN Xuemiao, ZHANG Xuping, CHONG Tao, CAI Jintao, TAN Fuli, SUN Chengwei. Recent progress on the experimental facilities, techniques and applications of magnetically driven quasi-isentropic compression[J]. Explosion And Shock Waves, 2021, 41(12): 121403. doi: 10.11883/bzycj-2021-0119

磁驱动平面准等熵加载装置、实验技术及应用研究新进展

doi: 10.11883/bzycj-2021-0119
基金项目: 国家自然科学基金(10927201,11327803,11972031,11176002, 10472108,11272295,11002130)
详细信息
    作者简介:

    王桂吉(1977- ),男,博士,研究员,wangguiji@126.com

  • 中图分类号: O383

Recent progress on the experimental facilities, techniques and applications of magnetically driven quasi-isentropic compression

  • 摘要: 利用脉冲大电流装置产生随时间变化平滑上升的磁压力,实现对平面、柱面等不同结构样品的磁驱动准等熵(斜波)压缩,为极端条件下材料动力学研究提供了一种偏离Hugoniot状态热力学路径的加载手段。本文从磁驱动准等熵加载装置、实验技术、数据处理方法等方面综述了磁驱动准等熵加载技术研究近十年的新进展,评述了利用磁驱动准等熵加载技术和方法开展极端条件下材料高压状态方程、高压强度与本构关系、相变与相变动力学等方面研究的进展情况,展望了磁驱动准等熵加载技术发展及其在材料动力学、武器物理和高能量密度物理等方面的应用前景。
  • 图  1  10 MA大电流装置三维效果图

    Figure  1.  Three-dimentional effect of the 10 MA high current facility

    图  2  10 MA大电流装置的典型放电电流曲线

    Figure  2.  Typical discharging current curves of 10 MA high current facility

    图  3  CQ-3装置

    Figure  3.  CQ-3 device

    图  4  CQ-3装置直接短路时的典型放电电流曲线[3]

    Figure  4.  Typical discharging current histories of CQ-3 in short circuits for programmed discharging[3]

    图  5  CQ-7装置实物照片(左)和三维效果设计剖面图(右)

    Figure  5.  Practical photo (left) and conceptual design (right) of CQ-7

    图  6  工作电压±50 kV时CQ-7装置的典型放电电流波形

    Figure  6.  Typical current waveforms of CQ-7 at charging voltage of ±50 kV for programmed discharging

    图  7  Thor装置设计概念(左)及其Thor-96模块装置(右)

    Figure  7.  Conceptual design of Thor (left) and practical photo of Thor-96 (right)

    图  8  Thor装置可实现的放电电流波形

    Figure  8.  Typical current waveforms achieved on Thor

    图  9  铁的热力学相图[37]

    Figure  9.  Thermodynamic phase diagram of Iron[37]

    图  10  磁驱动冲击-准等熵压缩加载

    Figure  10.  Magnetically driven shock-isentropic compression

    图  11  磁驱动斜波压-剪联合加载示意

    Figure  11.  Schematic of magnetically driven ramp wave pressure-shear loadings

    图  12  磁驱动柱面套筒内爆加载示意图

    Figure  12.  Schematic of magnetically driven liner implosion loading

    图  13  传递函数方法的可靠性考核

    Figure  13.  Reliability check of transfer function method for in-situ particle velocity

    图  14  基于特征线反演方法的声速直接计算原理和结果[49]

    Figure  14.  The calculation principle and results of sound speed by inverse characteristics method[49]

    图  15  正向-反向迭代计算流程图

    Figure  15.  Flow chart of forward-backward iterative calculation

    图  16  磁驱动准等熵压缩实验测量LY12铝的声速与应力应变曲线结果[51]

    Figure  16.  Experimental results of LY12 under magnetically-driven quasi-isentropic compression[51]

    图  17  准等熵压缩下LiF的等熵压缩线[54]

    Figure  17.  Isentrope of LiF under quai-isentropic compression[54]

    图  18  准等熵压缩下LiF状态方程的校核[15]

    Figure  18.  Check of equation of state of LiF under quasi-isentropic compression[15]

    图  19  不同形式状态方程计算得到的等熵线与实验结果的比较[56]

    Figure  19.  Comparison between calculated and experimental isentropes based on different equation of states[56]

    图  20  准等熵压缩下钽的高压强度[11]

    Figure  20.  High pressure strength of Tantalum under quasi-isentropic compression[11]

    图  21  准等熵压缩下铍的高压强度[25]

    Figure  21.  High pressure strength of Beryllium under quasi-isentropic compression[25]

    图  22  静水压比较法计算铝的强度[47]

    Figure  22.  Strength of Aluminum calculated by hydro-static pressure comparison[47]

    图  23  静水压比较法计算纯铁的强度[27]

    Figure  23.  Strength of Iron calculated by hydro-static pressure comparison[27]

    图  24  准等熵压缩下PBX-59样品的声速-粒子速度曲线和20GPa内的准等熵压缩线[72]

    Figure  24.  Sound velocity-particle velocity curvers PBX 59 explosive under quasi-isentropic compression and quasi-isentropic compression curves [72]

    图  25  准等熵压缩下铁的相变速度剖面和相变驱动力与加载率关系[74]

    Figure  25.  Phase transition of iron under quasi-isentropic compression[74]

    图  26  不同窗口阻抗时铁的相变波形演化[28]

    Figure  26.  Evolution of phase transition wave profiles of iron with different window impedance[28]

    图  27  冲击-斜波加载下液氘的反射率变化[82]

    Figure  27.  Reflectivity of liquid deuterium under shock-ramp wave compression[82]

    表  1  磁驱动准等熵压缩装置及其技术参数一览表

    Table  1.   Facilities of magnetically driven quasi-isentropic compression

    装置工作电压放电电流/MA上升时间/ns等熵加载
    压力/GPa
    飞片速度/
    (km·s−1
    物理应用技术特点
    Z/ZR数百万伏16~26100~60050043丝阵、套筒内爆、磁驱动准等熵压缩、高速飞片传统的Marx加传输线技术,电流波形多级压缩,多路并联放电,波形可调,装置规模庞大。
    聚龙一号(PTS)数百万伏8~1090丝阵,Z箍缩
    4~7300~70020020磁驱动准等熵压缩、高速飞片
    VELOCE<100 kV3~4400~53010010磁驱动准等熵压缩、高速飞片电容器组储能,通过平板传输线直接对负载放电,装置结构紧凑,运行效率高
    GEPI<100 kV4600100>10
    CQ-4<100 kV~4400~60010012~15
    CQ-3(1)~85 kV~340-800磁驱动准等熵压缩,高速飞片,套筒内爆电容器组储能,通过电缆汇流后进入低漏率防靶室对负载放电,电流波形可调
    CQ-7(2)~120 kV~7200~600 (10%~90%)100~150>15磁驱动准等熵压缩,高速飞片,套筒内爆单极Marx模块储能,通过电缆汇流对负载放电,多路触发放电,电流波形可调
    Thor(3)Thor-96~200 kV4.1250磁驱动准等熵压缩单极Marx模块储能,基于电缆全电路阻抗匹配传输,电流波形可调
    Thor-144~200 kV5.4250
    Thor-288~200 kV6.9250170
     注:(1) CQ-3装置为新技术探索样机,加载压力预计为数GPa至50GPa;(2) CQ-7加载压力为设计值;(3) Thor-288加载压力为设计值。
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  • 收稿日期:  2021-04-21
  • 修回日期:  2021-06-02
  • 网络出版日期:  2021-12-10
  • 刊出日期:  2021-12-05

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