Effect of 3-D fields on edge power/particle fluxes between and during ELMs (XP1026) A. Loarte, J-W. Ahn, J. M. Canik, R. Maingi, and J.-K. Park and the.

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Presentation transcript:

Effect of 3-D fields on edge power/particle fluxes between and during ELMs (XP1026) A. Loarte, J-W. Ahn, J. M. Canik, R. Maingi, and J.-K. Park and the NSTX Research Team NSTX Team Review B252, PPPL July 23, 2010 NSTX Supported by College W&M Colorado Sch Mines Columbia U CompX General Atomics INEL Johns Hopkins U LANL LLNL Lodestar MIT Nova Photonics New York U Old Dominion U ORNL PPPL PSI Princeton U Purdue U SNL Think Tank, Inc. UC Davis UC Irvine UCLA UCSD U Colorado U Illinois U Maryland U Rochester U Washington U Wisconsin Culham Sci Ctr U St. Andrews York U Chubu U Fukui U Hiroshima U Hyogo U Kyoto U Kyushu U Kyushu Tokai U NIFS Niigata U U Tokyo JAEA Hebrew U Ioffe Inst RRC Kurchatov Inst TRINITI KBSI KAIST POSTECH ASIPP ENEA, Frascati CEA, Cadarache IPP, Jülich IPP, Garching ASCR, Czech Rep U Quebec

NSTX BP Group Review – Effect of 3-D fields on divertor profiles between and during ELMs (Loarte)July 23, Motivation XP 1046 (Ahn): Effect of 3-D fields below ELM triggering threshold XP 1048 (Park): Effect of 3-D fields on ELM characteristics with q 95 scan ELM control in ITER is required for a large range of plasma conditions, not only for flat top of 15 MA Q DT =10 scenario  Dependences of the applied 3-D field effects on divertor power/particle fluxes on plasma parameters need to be determined to understand consequences for ITER stationary conditions and controlled ELM power fluxes  Compatibility with scenario requirements to be checked: acceptable stationary power flux (high n e divertor), erosion, Characterization of 3-D field effect above the ELM triggering threshold with parameter scan (I 3-D, ν* e, q 95, etc)

NSTX BP Group Review – Effect of 3-D fields on divertor profiles between and during ELMs (Loarte)July 23, Best aligned 3-D magnetic perturbation from XP1048 VAC3D modeling for NSTX expects different ratio of non- resonant to resonant components for different q 95  Smaller ratio for lower q 95 is expected. Use the result of XP1048 to figure out best aligned 3-D field perturbation  Parameter scan at this alignment NSTX q 95 ~10 NSTX q 95 ~6 J.-K. Park

NSTX BP Group Review – Effect of 3-D fields on divertor profiles between and during ELMs (Loarte)July 23, 2010 I p scan at constant q 95  Higher I p tends to make the ELM size bigger and likely increase radial transport during ELMs  Will need to vary B t to keep q 95 constant Pedestal collisionality scan  Apply 3-D field at different density levels  Effects on power deposition between ELMs and at ELMs  Change of P NBI can further change the pedestal collisionality SOL plasma collisionality scan/divertor density scan  Apply divertor D 2 gas puffing to change SOL/divertor plasma conditions 3-D field coil current scan above the ELM threshold  Higher coil current tends to produce more frequent ELMs. Need to investigate impact on divertor profiles of smaller ELMs at similar P ped and divertor conditions Parameter scan at best alignment 4

NSTX BP Group Review – Effect of 3-D fields on divertor profiles between and during ELMs (Loarte)July 23, 2010 Establish lowest q 95 (~6) discharge (140000) to obtain best aligned 3-D field spectrum with ELM triggering. Scan 3 coil current levels (eg, 1, 1.5, and 2kA)  Total of 3 shots Perform I p scan at constant q 95 (~6). Try three I p values, 700, 900, 1100kA  Total of 3 shots SOL plasma collisionality scan. Try two divertor D 2 gas levels (3000 and 1500Torr of Bay E GIS), 2 shots for each plasma condition  Total of 4 shots Pedestal collisionality scan. Apply 3-D field blips at three time slices during the density ramp-up in the H-mode. Try 2 NBI power levels (P NBI =2, 5-6MW), Ip  Total of 2 shots Misalign 3-D field coil spectrum by changing q 95, i.e.  q 95 = 2, by the means of Bt change (0.45T and 0.55T) at fixed Ip (700kA)  Total of 3 shots Shot plan 5