Plasma flows during the ablation stage of an over-massed pulsed-power-driven exploding planar wire array

被引:5
作者
Datta, R. [1 ]
Angel, J. [2 ]
Greenly, J. B. [2 ]
Bland, S. N. [3 ]
Chittenden, J. P. [3 ]
Lavine, E. S. [2 ]
Potter, W. M. [2 ]
Robinson, D. [1 ]
Varnish, T. W. O. [1 ]
Wong, E. [1 ]
Hammer, D. A. [2 ]
Kusse, B. R. [2 ]
Hare, J. D. [1 ]
机构
[1] MIT, Plasma Sci & Fus Ctr, Cambridge, MA 02319 USA
[2] Cornell Univ, Lab Plasma Studies, Ithaca, NY 14853 USA
[3] Imperial Coll London, Blackett Lab, London SW7 2BW, England
基金
英国工程与自然科学研究理事会;
关键词
DYNAMICS; PHYSICS;
D O I
10.1063/5.0160893
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
We characterize the plasma flows generated during the ablation stage of an over-massed exploding planar wire array, fielded on the COBRA pulsed-power facility (1 MA peak current, 250 ns rise time). The planar wire array is designed to provide a driving magnetic field (80-100 T) and current per wire distribution (about 60 kA), similar to that in a 10 MA cylindrical exploding wire array fielded on the Z machine. Overmassing the arrays enables continuous plasma ablation over the duration of the experiment without implosion. The requirement to overmass on the Z machine necessitates wires with diameters of 75-100 mu m, which are thicker than wires usually fielded on wire array experiments. To test ablation with thicker wires, we perform a parametric study by varying the initial wire diameter between 33 and 100 mu m. The largest wire diameter (100 mu m) array exhibits early closure of the cathode-wire gap, while the gap remains open over the duration of the experiment for wire diameters between 33 and 75 mu m. Laser plasma interferometry and time-gated extreme-ultraviolet (XUV) imaging are used to probe the plasma flows ablating from the wires. The plasma flows from the wires converge to generate a pinch, which appears as a fast-moving (V approximate to 100 kms(-1)) column of increased plasma density ((n) over bare approximate to 2 x 10(18)cm(-3)) and strong XUV emission. Finally, we compare the results with three-dimensional resistive-magnetohydrodynamic (MHD) simulations performed using the code GORGON, the results of which reproduce the dynamics of the experiment reasonably well. (c) 2023 Author(s). All article content, except where otherwise noted, is licensed under a Creative Commons Attribution (CC BY) license (http:// creativecommons.org/licenses/by/4.0/). https://doi.org/10.1063/5.0160893
引用
收藏
页数:15
相关论文
共 40 条
[1]   Use of linear wire array Z pinches to examine plasma dynamics in high magnetic fields [J].
Bland, SN ;
Lebedev, SV ;
Chittenden, JP ;
Ampleford, DJ ;
Tang, G .
PHYSICS OF PLASMAS, 2004, 11 (11) :4911-4921
[2]   The structure of bow shocks formed by the interaction of pulsed-power driven magnetised plasma flows with conducting obstacles [J].
Burdiak, G. C. ;
Lebedev, S. V. ;
Bland, S. N. ;
Clayson, T. ;
Hare, J. ;
Suttle, L. ;
Suzuki-Vidal, F. ;
Garcia, D. C. ;
Chittenden, J. P. ;
Bott-Suzuki, S. ;
Ciardi, A. ;
Frank, A. ;
Lane, T. S. .
PHYSICS OF PLASMAS, 2017, 24 (07)
[3]   Equilibrium flow structures and scaling of implosion trajectories in wire array Z pinches [J].
Chittenden, JP ;
Lebedev, SV ;
Oliver, BV ;
Yu, EP ;
Cuneo, ME .
PHYSICS OF PLASMAS, 2004, 11 (03) :1118-1127
[4]   The evolution of magnetic tower jets in the laboratory [J].
Ciardi, A. ;
Lebedev, S. V. ;
Frank, A. ;
Blackman, E. G. ;
Chittenden, J. P. ;
Jennings, C. J. ;
Ampleford, D. J. ;
Bland, S. N. ;
Bott, S. C. ;
Rapley, J. ;
Hall, G. N. ;
Suzuki-Vidal, F. A. ;
Marocchino, A. ;
Lery, T. ;
Stehle, C. .
PHYSICS OF PLASMAS, 2007, 14 (05)
[5]   The structure of 3-D collisional magnetized bow shocks in pulsed-power-driven plasma flows [J].
Datta, R. ;
Russell, D. R. ;
Tang, I ;
Clayson, T. ;
Suttle, L. G. ;
Chittenden, J. P. ;
Lebedev, S., V ;
Hare, J. D. .
JOURNAL OF PLASMA PHYSICS, 2022, 88 (06)
[6]   Time-resolved velocity and ion sound speed measurements from simultaneous bow shock imaging and inductive probe measurements [J].
Datta, R. ;
Russell, D. R. ;
Tang, I ;
Clayson, T. ;
Suttle, L. G. ;
Chittenden, J. P. ;
Lebedev, S., V ;
Hare, J. D. .
REVIEW OF SCIENTIFIC INSTRUMENTS, 2022, 93 (10)
[7]  
Datta R., 2022, 64th Annual Meeting of the APS Division of Plasma Physics
[8]   Structure of the dense cores and ablation plasmas in the initiation phase of tungsten wire-array Z pinches [J].
Douglass, J. D. ;
Pikuz, S. A. ;
Shelkovenko, T. A. ;
Hammer, D. A. ;
Bland, S. N. ;
Bott, S. C. ;
McBride, R. D. .
PHYSICS OF PLASMAS, 2007, 14 (01)
[9]   Wire dynamics model of the implosion of nested and planar wire arrays [J].
Esaulov, A. A. ;
Velikovich, A. L. ;
Kantsyrev, V. L. ;
Mehlhorn, T. A. ;
Cuneo, M. E. .
PHYSICS OF PLASMAS, 2006, 13 (12)
[10]   Magnetic field measurements via visible spectroscopy on the Z machine [J].
Gomez, M. R. ;
Hansen, S. B. ;
Peterson, K. J. ;
Bliss, D. E. ;
Carlson, A. L. ;
Lamppa, D. C. ;
Schroen, D. G. ;
Rochau, G. A. .
REVIEW OF SCIENTIFIC INSTRUMENTS, 2014, 85 (11)