Understanding electrode plasma formation on wires and thin foils via vacuum ultraviolet spectroscopy of desorbed surface contaminants
ORAL
Abstract
Power flow studies on the 30-MA, 100-ns Z facility at Sandia National Labs have shown that plasma in the facility’s magnetically insulated transmission lines can result in a loss of current delivered to the load.1 During the current pulse, thermal energy deposition into the electrodes causes neutral surface contaminant layers to desorb, ionize, and form plasma in the anode-cathode gap.2,3 We suspect that as the electrode thickness decreases relative to the skin depth of the current pulse (50−100 µm for aluminum and 100-500 µm for stainless steel, for a 100−500-ns pulse), the thermal energy delivered to the surface contaminant layers increases, and thus, faster desorption rates.
We review experimental results on a smaller scaled facility (≤ 1 MA) to characterize the contaminants using the plasma temperature, density, and determination of the species and their ionized states during surface desorption. These results are collected from a vacuum ultraviolet spectrometer developed to measure the spectra from wires and foils of varying thicknesses (5 µm – 1 mm) and materials (aluminum and stainless steel). To quickly compare theoretical values to experimental results, a newly developed, semi-analytic desorption and heating model is then used.
1. W.A. Stygar et al., Phys. Rev. S.T.-A.B. 12, 120401 (2009)
2. M.R. Gomez et al., Phys. Rev. A.B. 20, 010401 (2017)
3. T.J. Smith et al., Rev. Sci. Inst. 92, 053550 (2021)
We review experimental results on a smaller scaled facility (≤ 1 MA) to characterize the contaminants using the plasma temperature, density, and determination of the species and their ionized states during surface desorption. These results are collected from a vacuum ultraviolet spectrometer developed to measure the spectra from wires and foils of varying thicknesses (5 µm – 1 mm) and materials (aluminum and stainless steel). To quickly compare theoretical values to experimental results, a newly developed, semi-analytic desorption and heating model is then used.
1. W.A. Stygar et al., Phys. Rev. S.T.-A.B. 12, 120401 (2009)
2. M.R. Gomez et al., Phys. Rev. A.B. 20, 010401 (2017)
3. T.J. Smith et al., Rev. Sci. Inst. 92, 053550 (2021)
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Presenters
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Trevor J Smith
University of Michigan
Authors
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Trevor J Smith
University of Michigan
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Mark D Johnston
University of New Mexico
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Nicholas M Jordan
University of Michigan
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Michael E Cuneo
Sandia National Laboratories
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Jens Schwarz
Sandia National Laboratories
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Ryan D McBride
University of Michigan