Advanced Scenario Development on NSTX D. A. Gates, PPPL For the NSTX Research Team 50th APS-DPP meeting Dallas, TX November 17, 2008 College W&M Colorado.

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Presentation transcript:

Advanced Scenario Development on NSTX D. A. Gates, PPPL For the NSTX Research Team 50th APS-DPP meeting Dallas, TX November 17, 2008 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 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 NSTX Supported by

NSTX APS-DPP 2008 – Advanced scenario development (Gates)November 17, Advanced scenario development incorporates physics understanding to advance ST concept Based on contributions from topical science groups –*MHD - (plasma shaping and RFA/RWM control) –*Boundary - (improved performance with lithium) –Fast particles and *waves - (HHFW heating during H-modes) –Transport and turbulence –Solenoid free startup Scenario modeling focuses activities towards full non- inductive operation –Reduced collisionality increases neutral beam driven current

NSTX APS-DPP 2008 – Advanced scenario development (Gates)November 17, Optimized shape control has enabled access to advanced regimes on NSTX NSTX has achieved record values of plasma shaping –Technology improvements allow control of plasmas with record elongation –PF coil enhancements enable achievement of high triangularity –rtEFIT developed in collaboration with GA enables reliable plasma shape control Improvements in performance clearly associated with plasma shaping 2008 NSTX combines high shaping with high  N giving longest pulse to date –Non-axisymmetric control also important Many shots now limited by available TF flattop 2008  ~ 2.8,  = 0.8, S ~ 40 PF1A coil upgraded S = q 95 (I p /(aB t )) Plot of pulse averaged toroidal  vs. pulse length

NSTX APS-DPP 2008 – Advanced scenario development (Gates)November 17, n=1 RFA/RWM control combined with n=3 error correction increases  and extends pulse Non-axisymmetric feedback algorithm has been developed using unique feedback training scheme –Prevents onset of MHD modes –Plasma rotation is maintained throughout discharge Control statistically raises  and increase pulse length Pulse averaged  N vs. current flat-top Red with control Black w/o control MHD spectrogram with n=1 feedback and n=3 correction MHD spectrogram w/o n=1 feedback and n=3 correction n=1 mode drops  CHERS v t at R = 139cm Red with control Black w/o control Red with control Black w/o control No MHD,  and rotation maintained

NSTX APS-DPP 2008 – Advanced scenario development (Gates)November 17, Solid Lithium Coating Reduces Deuterium Recycling, Suppresses ELMs, Improves Confinement Without ELMs, impurity accumulation increases P rad and Z eff, but despite this Broader T e reduces internal inductance l i and inductive flux consumption LITER Canisters Dual Lithium Evaporators deposit lithium on entire lower divertor, suppressing ELMs, increasing stored energy through the electron channel

NSTX APS-DPP 2008 – Advanced scenario development (Gates)November 17, High toroidal field (0.55T) improves RF coupling in beam heated H-mode plasmas Able to double central electron temperature during high density H-mode with 1.6MW of RF heating power –Lithium coating controls edge density enabling good coupling High TF crucial to RF coupling Opens many possibilities for manipulating q profile during high performance discharges and controlling * RF heating Neutral Beam heating

NSTX APS-DPP 2008 – Advanced scenario development (Gates)November 17, Integrated modeling indicates potential path from best NSTX plasmas towards increased f NICD scenarios Scenarios have: I P = MA B T = kG TSC modeling (C. Kessel) Transient, low n e, high f NBICDTransient, low n e, high f NBICD Low-n e, high-f NBICD n 20 (0) = 0.36  = 2.2 H 98 = 1.1  N = 5.6 q(0)  1 f BS = 35% f NBICD = 55% f NICD = 90%  JB  /  B 2  profiles NSTX highest f NICD n 20 (0) = 0.85  = 2.2 H 98 = 1.1  N = 5.7 q(0)  1.2 f BS = 55-60% f NBICD = 10% f NICD = 65-70%  JB  /  B 2  profiles Total Bootstrap NBICD f BS and f NBICD similar to ST-CTF  JB  /  B 2  profiles High  N, high-f BS n 20 (0) = 0.75  = 2.6 H 98 = 1.4  N = 6.6 q(0) = 1.4 to 2.4 f BS = 75% f NBICD = 25% f NICD = 100% High density, high-  N, high-f BSHigh density, high-  N, high-f BS f BS and f NBICD similar to NHTX Major extrapolations circled

NSTX APS-DPP 2008 – Advanced scenario development (Gates)November 17, NSTX has made rapid progress towards developing attractive advanced operating scenarios In particular, NSTX has: Combined strong shaping with high  Improved MHD stability with n=3 EF correction and n=1 RFA/RWM control Improved confinement with suppressed ELMs using Lithium evaporation Increased central temperatures in advanced scenarios with HHFW  Resulting in longest lasting ST plasma,  pulse = 1.6s ~ 5-6  CR   N > 5 for 3-4  CR Identified a path towards 100% non-inductive sustainment at lower * with integrated scenario modeling These results are very encouraging for proposed future STs such as NHTX, ST-CTF as well as ST reactor concepts such as ARIES-AT