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Maingi, R.; Mahdavi, M.A.; Petrie, T.W.
General Atomics, San Diego, CA (United States); Oak Ridge National Lab., TN (United States); Sandia National Labs., Albuquerque, NM (United States); Univ. of California, San Diego, CA (United States). Funding organisation: USDOE Office of Energy Research, Washington, DC (United States)1998
General Atomics, San Diego, CA (United States); Oak Ridge National Lab., TN (United States); Sandia National Labs., Albuquerque, NM (United States); Univ. of California, San Diego, CA (United States). Funding organisation: USDOE Office of Energy Research, Washington, DC (United States)1998
AbstractAbstract
[en] The authors have studied the processes limiting plasma density and successfully achieved discharges with density ∼50% above the empirical Greenwald density limit with H-mode confinement. This was accomplished by density profile control, enabled through pellet injection and divertor pumping. By examining carefully the criterion for MARFE formation, the authors have derived an edge density limit with scaling very similar to Greenwald scaling. Finally, they have looked in detail at the first and most common density limit process in DIII-D, total divertor detachment, and found that the local upstream separatrix density (nesep,det) at detachment onset (partial detachment) increases with the scrape-off layer heating power, Pheat, i.e., nesep,det ∼ Pheat0.76. This is in marked contrast to the line-average density at detachment which is insensitive to the heating power. The data are in reasonable agreement with the Borass model, which predicted that the upstream density at detachment would increase as Pheat0.7
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Aug 1998; 23 p; 13. international conference on plasma surface interactions; San Diego, CA (United States); 18-22 May 1998; CONF-980560--; CONTRACT AC03-89ER51114; AC05-96OR22464; AC04-94AL85000; FG03-95ER54294; ALSO AVAILABLE FROM OSTI AS DE98006222; NTIS; US GOVT. PRINTING OFFICE DEP
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