Plasma and neutral dynamics in a simulated tokamak gas target divertor

A stationary, detached ionization front is observed in an experimentally simulated divertor plasma (n≤3×1019 m−3, kT e ≤20 eV) interacting with a hydrogen gas target. With a neutral hydrogen density, n 0≊2×1021 m−3, the electron temperature at the simulated divertor target is reduced to kT e target≊...

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Veröffentlicht in:Physics of Plasmas 1995-08, Vol.2 (8), p.3081-3094
Hauptverfasser: Schmitz, L., Merriman, B., Blush, L., Lehmer, R., Conn, R. W., Doerner, R., Grossman, A., Najmabadi, F.
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Sprache:eng
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Zusammenfassung:A stationary, detached ionization front is observed in an experimentally simulated divertor plasma (n≤3×1019 m−3, kT e ≤20 eV) interacting with a hydrogen gas target. With a neutral hydrogen density, n 0≊2×1021 m−3, the electron temperature at the simulated divertor target is reduced to kT e target≊2.5 eV. Up to 97% of the electron heat flux (≤7 MW/m2) is dissipated by dissociation and ionization losses and hydrogen line radiation. The plasma pressure is observed to peak near the ionization front, and a plasma flow reversal is observed in the region of reversed pressure gradient. Classical momentum flow parallel to the magnetic field and anomalous cross‐field particle transport are found. The plasma flow is strongly damped by ion–neutral collisions and is subsonic. Numerical results from a one‐and‐one‐half dimensional (11/2‐D) coupled plasma–neutral fluid model (incorporating radial particle transport, recycling, and neutral gas injection) agree well with the experimental data, and indicate that the electron heat flow is classical and well described by a harmonic flux limit. The scale length of the parallel plasma pressure gradient in a gas target is found to depend on the neutral density, the electron temperature, and the cross‐field diffusion coefficient.
ISSN:1070-664X
1089-7674
DOI:10.1063/1.871206