Experimental study of current loss and plasma formation in the Z machine post-hole convolute

The Z pulsed-power generator at Sandia National Laboratories drives high energy density physics experiments with load currents of up to 26 MA. Z utilizes a double post-hole convolute to combine the current from four parallel magnetically insulated transmission lines into a single transmission line j...

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Main Authors: M. R. Gomez, R. M. Gilgenbach, M. E. Cuneo, C. A. Jennings, R. D. McBride, E. M. Waisman, B. T. Hutsel, W. A. Stygar, D. V. Rose, Y. Maron
Format: Article
Language:English
Published: American Physical Society 2017-01-01
Series:Physical Review Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevAccelBeams.20.010401
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author M. R. Gomez
R. M. Gilgenbach
M. E. Cuneo
C. A. Jennings
R. D. McBride
E. M. Waisman
B. T. Hutsel
W. A. Stygar
D. V. Rose
Y. Maron
author_facet M. R. Gomez
R. M. Gilgenbach
M. E. Cuneo
C. A. Jennings
R. D. McBride
E. M. Waisman
B. T. Hutsel
W. A. Stygar
D. V. Rose
Y. Maron
author_sort M. R. Gomez
collection DOAJ
description The Z pulsed-power generator at Sandia National Laboratories drives high energy density physics experiments with load currents of up to 26 MA. Z utilizes a double post-hole convolute to combine the current from four parallel magnetically insulated transmission lines into a single transmission line just upstream of the load. Current loss is observed in most experiments and is traditionally attributed to inefficient convolute performance. The apparent loss current varies substantially for z-pinch loads with different inductance histories; however, a similar convolute impedance history is observed for all load types. This paper details direct spectroscopic measurements of plasma density, temperature, and apparent and actual plasma closure velocities within the convolute. Spectral measurements indicate a correlation between impedance collapse and plasma formation in the convolute. Absorption features in the spectra show the convolute plasma consists primarily of hydrogen, which likely forms from desorbed electrode contaminant species such as H_{2}O, H_{2}, and hydrocarbons. Plasma densities increase from 1×10^{16}  cm^{−3} (level of detectability) just before peak current to over 1×10^{17}  cm^{−3} at stagnation (tens of ns later). The density seems to be highest near the cathode surface, with an apparent cathode to anode plasma velocity in the range of 35–50  cm/μs. Similar plasma conditions and convolute impedance histories are observed in experiments with high and low losses, suggesting that losses are driven largely by load dynamics, which determine the voltage on the convolute.
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spelling doaj.art-5063c56130814a39a27f74637b49b0872022-12-21T22:24:16ZengAmerican Physical SocietyPhysical Review Accelerators and Beams2469-98882017-01-0120101040110.1103/PhysRevAccelBeams.20.010401Experimental study of current loss and plasma formation in the Z machine post-hole convoluteM. R. GomezR. M. GilgenbachM. E. CuneoC. A. JenningsR. D. McBrideE. M. WaismanB. T. HutselW. A. StygarD. V. RoseY. MaronThe Z pulsed-power generator at Sandia National Laboratories drives high energy density physics experiments with load currents of up to 26 MA. Z utilizes a double post-hole convolute to combine the current from four parallel magnetically insulated transmission lines into a single transmission line just upstream of the load. Current loss is observed in most experiments and is traditionally attributed to inefficient convolute performance. The apparent loss current varies substantially for z-pinch loads with different inductance histories; however, a similar convolute impedance history is observed for all load types. This paper details direct spectroscopic measurements of plasma density, temperature, and apparent and actual plasma closure velocities within the convolute. Spectral measurements indicate a correlation between impedance collapse and plasma formation in the convolute. Absorption features in the spectra show the convolute plasma consists primarily of hydrogen, which likely forms from desorbed electrode contaminant species such as H_{2}O, H_{2}, and hydrocarbons. Plasma densities increase from 1×10^{16}  cm^{−3} (level of detectability) just before peak current to over 1×10^{17}  cm^{−3} at stagnation (tens of ns later). The density seems to be highest near the cathode surface, with an apparent cathode to anode plasma velocity in the range of 35–50  cm/μs. Similar plasma conditions and convolute impedance histories are observed in experiments with high and low losses, suggesting that losses are driven largely by load dynamics, which determine the voltage on the convolute.http://doi.org/10.1103/PhysRevAccelBeams.20.010401
spellingShingle M. R. Gomez
R. M. Gilgenbach
M. E. Cuneo
C. A. Jennings
R. D. McBride
E. M. Waisman
B. T. Hutsel
W. A. Stygar
D. V. Rose
Y. Maron
Experimental study of current loss and plasma formation in the Z machine post-hole convolute
Physical Review Accelerators and Beams
title Experimental study of current loss and plasma formation in the Z machine post-hole convolute
title_full Experimental study of current loss and plasma formation in the Z machine post-hole convolute
title_fullStr Experimental study of current loss and plasma formation in the Z machine post-hole convolute
title_full_unstemmed Experimental study of current loss and plasma formation in the Z machine post-hole convolute
title_short Experimental study of current loss and plasma formation in the Z machine post-hole convolute
title_sort experimental study of current loss and plasma formation in the z machine post hole convolute
url http://doi.org/10.1103/PhysRevAccelBeams.20.010401
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