首页> 外文会议>2017 IEEE 21st International Conference on Pulsed Power >Surface current density distribution measurements of an electrically exploded foil via B-dot probe array data inversion
【24h】

Surface current density distribution measurements of an electrically exploded foil via B-dot probe array data inversion

机译:通过B点探针阵列数据反演测量电爆炸箔的表面电流密度分布

获取原文
获取原文并翻译 | 示例

摘要

Measurements are presented of the current per unit length as a function of the transverse distance from the center of a water-tamped 80 μm Al foil that narrows to a central width of 15.2 cm as it explodes into warm dense matter by Ohmic heating. Current is delivered from a 36 μF capacitor bank charged to 30 kV and discharged to a peak current of 342 kA in 2.0 μs. The distribution is calculated by the linear regularized inversion of signals from an array of B-dot probes distributed long the foil's central half-width. The probes are far enough away from the foil (1 cm) to be noninvasive and mechanically undisturbed during the time of interest. These results are compared to 3-D MHD ALEGRA simulations of the geometry externally coupled to a two-loop lumped circuit model representing the driver. Surface current density is strongly peaked at the foil edges for low-current calibration tests, where conductivity is essentially constant. It's broadly peaked in the center at peak current for the full energy shot, though, due to the foil fusing first at the edges, which subsequently reduces current density there relative to the center by the time of peak current. There is broad agreement in this regard between the experiment and ALEGRA using thermal and electrical conductivity model SNL Sesame 293731. ALEGRA calculates that current peaks 0.5 μs earlier, though, and with 50 kA higher current. This may be due to error in the conductivity tables or effects not well-modeled, such as an electro-thermal instability that results in higher total resistance, but with a distance scale too small for the present simulation to represent. This work is a revision of that presented at IPPC 2015.
机译:给出了每单位长度的电流的测量值,该电流是距夯实的80μm铝箔中心的横向距离的函数,该铝箔在欧姆加热下爆炸成温暖的致密物质时变窄为中心宽度15.2 cm。电流从充电至30 kV的36μF电容器组输出,并在2.0μs内放电至342 kA的峰值电流。该分布是通过将B点探测器阵列的信号线性正则化反演计算得出的,该探测器分布在金属箔的中央半宽度处。探针与金属箔的距离足够远(1厘米),在感兴趣的时间内无创且不受机械干扰。将这些结果与外部耦合到代表驱动器的两回路集总电路模型的几何图形的3-D MHD ALEGRA仿真进行了比较。在低电流校准测试中,电导率基本恒定,在箔边缘处表面电流密度强烈达到峰值。但是,由于箔片首先在边缘熔断,随后在峰值电流时相对于中心降低了电流密度,因此在整个能量发射时,它在峰值电流处的中心普遍达到峰值。在这方面,使用导热和电导率模型SNL Sesame 293731在ALEGRA和实验之间达成了广泛共识。尽管ALEGRA计算出电流峰值提前了0.5μs,但电流却增加了50 kA。这可能是由于电导率表中的错误或建模效果不佳所致,例如电热不稳定性会导致较高的总电阻,但距离比例太小,无法用当前的模拟表示。这项工作是对IPPC 2015提出的工作的修订。

著录项

  • 来源
  • 会议地点 Brighton(GB)
  • 作者单位

    Air Force Research Laboratory, Directed Energy Directorate, AFRL/RDHP, 3550 Aberdeen Ave. SE, Kirtland AFB, NM 87117-5776 USA;

    Air Force Research Laboratory, Directed Energy Directorate, AFRL/RDHP, 3550 Aberdeen Ave. SE, Kirtland AFB, NM 87117-5776 USA;

    Air Force Research Laboratory, Directed Energy Directorate, AFRL/RDHP, 3550 Aberdeen Ave. SE, Kirtland AFB, NM 87117-5776 USA;

    Air Force Research Laboratory, Directed Energy Directorate, AFRL/RDHP, 3550 Aberdeen Ave. SE, Kirtland AFB, NM 87117-5776 USA;

    Leidos Engineering, Inc., Albuquerque, NM 87106 USA;

    Leidos Engineering, Inc., Albuquerque, NM 87106 USA;

    Leidos Engineering, Inc., Albuquerque, NM 87106 USA;

    Leidos Engineering, Inc., Albuquerque, NM 87106 USA;

    TechFlow Inc., 2155 Louisiana Blvd NE, Suite 4200, Albuquerque, NM 87110-5409 USA;

  • 会议组织
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    Probes; Fuses; Integrated circuit modeling; Current density; Calibration; Conductivity; Wires;

    机译:探头;保险丝;集成电路建模;电流密度;校准;电导率;电线;;

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号