NSTX XP830 review – J.W. Berkery J.W. Berkery, S.A. Sabbagh, H. Reimerdes Supported by Columbia U Comp-X General Atomics INEL Johns Hopkins U LANL LLNL.

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NSTX XP830 review – J.W. Berkery J.W. Berkery, S.A. Sabbagh, H. Reimerdes Supported by Columbia U Comp-X General Atomics INEL Johns Hopkins U LANL LLNL Lodestar MIT Nova Photonics NYU ORNL PPPL PSI SNL UC Davis UC Irvine UCLA UCSD U Maryland U New Mexico U Rochester U Washington U Wisconsin Culham Sci Ctr Hiroshima U HIST Kyushu Tokai U Niigata U Tsukuba U U Tokyo JAERI Ioffe Inst TRINITI KBSI KAIST ENEA, Frascati CEA, Cadarache IPP, Jülich IPP, Garching U Quebec NSTX Team Review Meeting April 21, 2008 Princeton Plasma Physics Laboratory Department of Applied Physics, Columbia University, New York, NY XP830: Resistive Wall Mode Stabilization Physics – Comparison to Theory

NSTX XP830 review – J.W. Berkery XP830: Resistive Wall Mode Stabilization Physics Goals  Determine stabilization physics - compare between experiment and theory Expand RWM critical rotation profile database – destabilize RWM with n=3 braking Kinetic effects: using University of Rochester code, and possibly MARS-K  Investigate the effect of various rotation profiles on kinetic stabilization Wide range of rotation profiles available, from very broad to peaked with no rotation at the q=2 surface.  Investigate stabilization over the widest possible range of ion collisionality  Make comparisons to DIIID Aspect ratio and trapped ion fraction are expected to be important Addresses  Joule Milestone (2008) and FY2009 milestone (R09-1) “Further understand the physics of RWM stabilization and control as a function of plasma rotation”  ITPA MDC-2: Joint experiments on RWM physics.

NSTX XP830 review – J.W. Berkery RWM Energy Principle – Kinetic Effects (Hu, Betti, and Manickam, PoP 12 (2005) ) (Haney and Freidberg, PoF-B 1 (1989) 1637) PEST Hu/Betti/Manickam

NSTX XP830 review – J.W. Berkery Preliminary NSTX Results from Hu/Betti Code  Strongest kinetic effect: trapped ion precession drift frequency Depends inversely on ion collision frequency Depends on rotation frequency through ω E.

NSTX XP830 review – J.W. Berkery Various Frequencies are Important (profiles at t = 0.601s)

NSTX XP830 review – J.W. Berkery NSTX and DIII-D Rotation Thresholds not Consistent DIII-D Rotation threshold may be dominated by error field. (Sontag, et al., NF 47 (2007) 1005) (G arofalo, et al., NF 47 (2007) 1121) NSTX Not consistent with this model Possibly due to large trapped ion fraction, which may stabilize RWM through kinetic effects.

NSTX XP830 review – J.W. Berkery Setup Shot – Create a Long n=1 Mode Free Period  from Sabbagh’s XP 802, 4/11 Create a long window free of n=1 rotating modes Ramp the n=3 braking field.

NSTX XP830 review – J.W. Berkery Rotation Profiles  Variety of rotation profiles From very broad to peaked with zero rotation at q=2 Created by varying the timing and magnitude of the n=3 DC correction/braking field.

NSTX XP830 review – J.W. Berkery Collisionality  Variation of collisionality Demonstrated by XP619. Accomplished by changing the density (changing B t and I p at fixed q).

NSTX XP830 review – J.W. Berkery Active MHD Spectroscopy Gives a measurement of the growth rate and rotation frequency of a weakly damped, stable RWM. (Reimerdes, et al., PPFC 49 (2007) B349)

NSTX XP830 review – J.W. Berkery XP830: RWM Stabilization Physics - Run plan

NSTX XP830 review – J.W. Berkery Required diagnostics / capabilities  Ability to operate RWM coils in n = 3 configuration  RWM sensors  CHERS toroidal rotation measurement  Thomson scattering  USXR  MSE  Toroidal Mirnov array / between-shots spectrogram with toroidal mode number analysis  Diamagnetic loop Desired diagnostics  FIReTip  Fast camera XP830: RWM Stabilization Physics - Diagnostics