2002
DOI: 10.1002/1521-3986(200204)42:2/4<181::aid-ctpp181>3.0.co;2-0
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Simulation of Edge Plasmas in DIII-D Double-Null Configurations

Abstract: We present fluid model simulation results for the edge plasma in the DIII‐D tokamak with unbalanced double‐null magnetic configurations, including cross field drifts. Input parame‐ters are typical of low‐power operation in DIII‐D. For high‐recycling the plasma tends to be detached from all divertor plates. Midplane plasma and electric field profiles are relatively insensitive to the magnetic imbalance. Divertor heat flux profiles exhibit sharp peaks due to cross‐field drifts when the ion grad‐B drift direction… Show more

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Cited by 5 publications
(4 citation statements)
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“…However, it has been found experimentally that the up/down asymmetry of the power and particle exhaust is very sensitive to the up/down magnetic balance. UEDGE modeling, which is consistent with the experimental results, indicate 13 that the in/out and up/down particle and power asymmetries are determined entirely by the effects of classical plasma drifts [57].…”
Section: D Model (Uedge)supporting
confidence: 79%
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“…However, it has been found experimentally that the up/down asymmetry of the power and particle exhaust is very sensitive to the up/down magnetic balance. UEDGE modeling, which is consistent with the experimental results, indicate 13 that the in/out and up/down particle and power asymmetries are determined entirely by the effects of classical plasma drifts [57].…”
Section: D Model (Uedge)supporting
confidence: 79%
“…Implementation of these drift effects for all operating modes of DIII-D is ongoing. Inclusion of the drift effects is crucial when modeling double null configurations [56,57]. The use of the double null configuration has been proposed as a means of increasing the wetted surface area over which power is exhausted in advanced tokamak modes [58].…”
Section: D Model (Uedge)mentioning
confidence: 99%
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“…First, small variations in the magnetic balance near the DN shape have sizable effects on the poloidal distributions of heat and particle fluxes at the divertor targets [2,3], the edge localized mode (ELM)-driven particle pulses at the divertor targets [4] and the poloidal distribution of plasma recycling [5]. Second, ion particle drifts in the scrape-off layer (SOL) and divertor(s), such as B × ∇B and E × B drifts [6][7][8], also contribute to the formation of these poloidal 'asymmetries' [9,10]. The particle flows that result from these drifts have long been suspected of playing important roles in edge-and divertor plasma behaviour and are being actively investigated, e.g.…”
Section: Introductionmentioning
confidence: 99%