NSTX Supported by College W&M Colorado Sch Mines Columbia U Comp-X General Atomics INEL Johns Hopkins U LANL LLNL Lodestar MIT Nova Photonics New York.

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Presentation transcript:

NSTX Supported by College W&M Colorado Sch Mines Columbia U Comp-X 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 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 Effects of Lithium-Coated Plasma-Facing Components on NSTX Discharges Robert Kaita, PPPL For the NSTX Research Team 50th Annual Meeting of the APS Division of Plasma Physics Reunion A, Hyatt Regency Hotel, Dallas, TX November 17, 2008

NSTX 50th Annual Meeting of the APS DPP – Effects of Lithium-Coated PFCs (Kaita)November 17, Introduction Lithium plasma-facing components (PFCs) have potentially attractive features for reactors, e. g., reducing recycling and mitigating effects of high heat and radiation fluxes Dramatic effects of lithium PFCs on plasma performance demonstrated on TFTR, T-11M, FT-U, CDX-U, TJ-II, etc. Recent NSTX experiments have shown significant and recurring benefits of lithium PFCs including: –Reduced plasma density early in discharge –ELM suppression and longer pulse length –Improved energy confinement –Reduced flux consumption –Broader electron temperature profile –Reduced scrapeoff layer plasma density

NSTX 50th Annual Meeting of the APS DPP – Effects of Lithium-Coated PFCs (Kaita)November 17, Two LIThium EvaporatoRs (LITERs) oriented for coating NSTX divertor region with lithium 10 cm

NSTX 50th Annual Meeting of the APS DPP – Effects of Lithium-Coated PFCs (Kaita)November 17, Shutter in front of LITER exit allows rapid interruption of evaporation without cooling oven Helium glow discharge cleaning eliminated between shots –Helium no longer trapped by lithium Plasma 1 s He 6.5 min Plasma 1 s He 6.5 min Continuous Li Evaporation 2007 scenario for lithium deposition 2008 scenario using shutters to block Li deposition Shutter closed 6 min minimum Li 8 min Shutter closed 10 min minimum Li 8 min Li 8 min

NSTX 50th Annual Meeting of the APS DPP – Effects of Lithium-Coated PFCs (Kaita)November 17, ELMs suppressed and discharge duration extended in plasmas with lithium PFC coatings Plasma density reduced early in discharge

NSTX 50th Annual Meeting of the APS DPP – Effects of Lithium-Coated PFCs (Kaita)November 17, Increase in stored energy (W MHD ) with lithium mostly through rise in electron stored energy (W e )

NSTX 50th Annual Meeting of the APS DPP – Effects of Lithium-Coated PFCs (Kaita)November 17, No Li S. Kaye No Li TRANSP analysis indicates increase in edge currentNSTX 50th Annual Meeting of the APS DPP – Effects of Lithium-Coated PFCs (Kaita) 7 November 17, 2008 Higher pedestal gradients raise edge boostrap current –Consistent with “second stability” and ELM suppression

NSTX 50th Annual Meeting of the APS DPP – Effects of Lithium-Coated PFCs (Kaita)November 17, Lithium PFC coatings reduce OH flux consumption Lower average loop voltages mean more efficient flux consumption –Internal inductance decreases as electron temperature profile broadens

NSTX 50th Annual Meeting of the APS DPP – Effects of Lithium-Coated PFCs (Kaita)November 17, Electron temperature profile broadening observed in discharges with lithium PFC coatings (no Li), (260mg Li)

NSTX 50th Annual Meeting of the APS DPP – Effects of Lithium-Coated PFCs (Kaita)November 17, lines fit in this header so I can put too many words in my title Scrapeoff layer profiles indicate density reduction with lithium-coated PFCs and suggests lowered recycling Modeling in progress with UEDGE multi-fluid transport code –Shows variation in magnitude of edge density with recycling coefficient –Presently matches density profile shape only in high Li deposition case Suggests need to include change in transport in simulations Low Li deposition High Li deposition

NSTX 50th Annual Meeting of the APS DPP – Effects of Lithium-Coated PFCs (Kaita)November 17, Lithium coating from stream of lithium powder into scrapeoff layer similar to LITER in effect on plasma performance ~40  m lithium particles dropped from canister above during discharge No lithium; 700mg LITER; 7 mg Powder 0 1 TIME (s) 0 1 TIME (s) Plasma Current (kA)Neutral Beam Power (MW) Stored Energy (J)Average Density (10 19 m -3 )

NSTX 50th Annual Meeting of the APS DPP – Effects of Lithium-Coated PFCs (Kaita)November 17, Summary Recent NSTX experiments have shown improved plasma performance with lithium-coated PFCs –Obtained with lithium evaporation and lithium powder –Helium glow discharge cleaning between shots eliminated for achieving H-mode –Plasma density reduced in early phase of discharge –ELMs suppressed –Energy confinement improved –Discharge length increased –Flux consumption reduced –Electron temperature profile broadened –Scrapeoff layer plasma density reduced Consistent with lowered recycling

NSTX 50th Annual Meeting of the APS DPP – Effects of Lithium-Coated PFCs (Kaita)November 17, 2008 Lithium in porous molybdenum surface to be kept liquid by heated copper substrate Objective is to determine if liquid lithium can sustain deuterium pumping beyond capability of solid lithium coatings Next step in NSTX is to begin investigation of liquid lithium on plasma facing components Liquid Lithium Divertor (LLD) to be installed on lower divertor in

NSTX 50th Annual Meeting of the APS DPP – Effects of Lithium-Coated PFCs (Kaita)November 17, Contributors and acknowledgments *Work supported in part by US DOE Contracts DE-AC02-76CH03073, DE-AC04-94AL85000, DE-AC52-07NA27344, and DE-AC05-00OR22725 H. Kugel 1), J-W. Ahn 2), J. P. Allain 7), M. G. Bell 1), R. Bell 1), J. Boedo 2), C. Bush 3), R. Ellis 1), D. Gates 1), S. Gerhardt 1) T. Gray 1), J. Kallman 1), S. Kaye 1), B. LeBlanc 1), R. Maingi 3), R, Majeski 1), D. Mansfield 1), J. Menard 1), D. Mueller 1), M. Ono 1), S. Paul 1), R. Raman 4), A. L. Roquemore 1), P. W. Ross 1), S. Sabbagh 5), H. Schneider 1), C. H. Skinner 1), V. Soukhanovskii 6), T. Stevenson 1), D. Stotler 1), J. Timberlake 1), W. R. Wampler 8), J. Wang 9), J. Wilgen 3), and L. Zakharov 1) 1) Princeton Plasma Physics Laboratory, Princeton, NJ USA 2) University of California at San Diego, La Jolla, CA USA 3) Oak Ridge National Laboratory, Oak Ridge, TN USA 4) University of Washington, Seattle, WA USA 5) Columbia University, New York, NY USA 6) Lawrence Livermore National Laboratory, Livermore, CA USA 7) Purdue University, School of Nuclear Engineering, West Lafayette, IN USA 8) Sandia National Laboratories, Albuquerque, NM USA 9) Los Alamos National Laboratory, Los Alamos, NM USA See posters NP , NP , NP , and NP on Wednesday morning for more details