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NSTX. Supported by. NSTX 2010 Experimental Proposal: Peeling-Ballooning Stability Dependence on Plasma Triangularity. 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 - PowerPoint PPT Presentation
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NSTX 2010 Experimental Proposal:NSTX 2010 Experimental Proposal:Peeling-Ballooning Stability Dependence on Peeling-Ballooning Stability Dependence on
Plasma TriangularityPlasma Triangularity
Aaron Sontag, Oak Ridge National Lab
FY2010 NSTX Research ForumDec. 1-3, 2009
College W&MColorado Sch MinesColumbia UComp-XGeneral AtomicsINELJohns Hopkins ULANLLLNLLodestarMITNova PhotonicsNew York UOld Dominion UORNLPPPLPSIPrinceton UPurdue USNLThink Tank, Inc.UC DavisUC IrvineUCLAUCSDU ColoradoU MarylandU RochesterU WashingtonU Wisconsin
Culham Sci CtrU St. Andrews
York UChubu UFukui U
Hiroshima UHyogo UKyoto U
Kyushu UKyushu Tokai U
NIFSNiigata UU Tokyo
JAEAHebrew UIoffe Inst
RRC Kurchatov InstTRINITI
KBSIKAIST
POSTECHASIPP
ENEA, FrascatiCEA, Cadarache
IPP, JülichIPP, Garching
ASCR, Czech RepU Quebec
NSTXNSTX Supported by
NSTXNSTX A. Sontag - 2010 NSTX Research Forum 1-3 Dec. 2009
Proposal: Alter Peeling-Ballooning Stability Boundary by Varying Plasma Triangularity
• NSTX peeling-ballooning stability inconsistent with ELITE calculations– ELMs observed even though
/(*/2) << 1
• PEST indicates ballooning may be important– max. stable N roughly
proportional to avg.
• Reduced can increase ballooning instability drive– high- opens up 2nd stability at
low A
22
•3 4 5 6 7 8•Normalized Pressure Gradient ()
•1.2
•0.8
•0.4
• Ed
ge
cu
rre
nt
• [(j
ma
x+
jse
p)/
2<
j>]
•0.1
NSTX peeling-ballooning stability as calculated by ELITE for a discharge with Type I ELMs
N
0
5
10
upper
0 0.25 0.5
lower = 0.2
lower = 0.3 lower = 0.4
Ballooning stability as calculated by PEST
NSTXNSTX A. Sontag - 2010 NSTX Research Forum 1-3 Dec. 2009
XP 942 Successfully Affected ELM Stability with lower modification
lower decrease coincident with transition to small ELMs– drsep unchanged until well after
small ELM regime (0.46 s)
• Further reduction needed to approach ballooning boundary– PEST indicates n=3 still most
unstable mode– shot development required going
shape with decreased stability
upper scan also needed
– go to higher , Z0 > 0 plasma, or reduce outer gap
33
NSTXNSTX A. Sontag - 2010 NSTX Research Forum 1-3 Dec. 2009
XP Plan: Continue scan from XP 942, independently varying upper & lower
• Decreased possible with increased outer gap– more modeling required for this scenario
• XP 942 target was low- (~1.9) LSN– difficult to affect upper with large separation from
control coils upper always slightly less than lower
• ISOLVER modeling shows more control of upper achievable at increased-– Use PF1AU to push/pull upper
– Fix PF1s & 2s, PCS control of PF3s & PF5– increase request
• Vary upper at fixed lower
– vary upper squareness request4
0.0 0.5 1.0 1.5 2.0R (m)
-2
-1
0
1
2
Z(m)
NSTXNSTX A. Sontag - 2010 NSTX Research Forum 1-3 Dec. 2009
Duration & Required Diagnostics
• XP could be performed in 1 day
• Required diagnostics– CHERS (beam blips in HHFW-only discharges)– USXR arrays– magnetics– Thomson scattering– EFIT (w/MSE)
– D
• Desired diagnostics– edge reflectometer– two color USXR
5