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Roderick, N.F.; Payne, S.S.; Peterkin, R.E. Jr.; Frese, M.H.; Hussey, T.W.
Sandia National Labs., Albuquerque, NM (USA)1989
Sandia National Labs., Albuquerque, NM (USA)1989
AbstractAbstract
[en] Simulations of plasma opening switch have been made using two-dimensional, single fluid, magnetohydrodynamic codes HAM and MACH2. A variety of mechanisms for magnetic field penetration have been investigated. These include plasma convection, classical and microturbulent resistive diffusion, and Hall effect transport. We find that plasma microturbulent models are necessary to explain the broad current channels observed in experiments. Both heuristic and consistent microturbulent models are able to explain observed channel widths and penetration features. The best results are obtained for a consistent model that includes the Buneman, ion acoustic, and lower hybrid microturbulent collision frequencies and threshold conditions. Maximum microturbulent collision frequencies of 5 ωp, are typical. Field transport and current channel profiles are in excellent agreement with experimental observations for GAMBLE I, GAMBLE II, and SUPERMITE experiments. Dominant field penetration mechanisms and center of mass plasma motion are current and density dependent. Including the Hall effect enhanced field penetration. Center of mass motion is negligible for the GAMBLE I experiments but significant for the GAMBLE II conditions. Scaling of plasma opening time with switch length and density can be fit by linear representations for lengths from 0.03 m to 0.24 m and ion densities from 1018m-3 to 1.5 times 1019m-3. 15 refs., 7 figs., 1 tab
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1989; 10 p; 5. international conference on megagauss magnetic field generation and related topics; Novosibirsk (USSR); 3-7 Jul 1989; CONF-890710--16-DRAFT; CONTRACT DOE AC04-76DP00789; Available from NTIS, PC A02/MF A01 - OSTI as DE89014491; US Govt. Printing Office Dep
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