Resistive wall mode stabilization of high-{beta} plasmas in the National Spherical Torus Experiment

The resistive wall mode (RWM) poses a limit to the maximum {beta} that can be sustained in magnetic fusion experiments. RWM stabilization physics at low aspect ratio is studied in high-{beta} National Spherical Torus Experiment (NSTX) [M. Ono, S. M. Kaye, Y.-K. M. Peng et al., Nucl. Fusion 40, 557 (2000)] plasmas ({beta}{sub t} up to 39%; {beta}{sub N} up to 6.8) to understand and alleviate this constraint. Plasmas with increased q in NSTX have been maintained with {beta} above the computed ideal no-wall {beta} limit for more than 20 wall times with no signs of RWM growth in cases where toroidal rotation {omega}{sub {phi}}>{omega}{sub A}/4q{sup 2} across the entire plasma cross section. Plasmas that violate this stability criterion can suffer a RWM induced collapse within a few wall times. This critical rotation profile for stabilization is in agreement with drift-kinetic theory applied to low frequency magnetohydrodynamics modes [A. Bondeson and M. S. Chu, Phys. Plasmas 3, 3013 (1996)]. A toroidally symmetric array of internal sensors has been used to observe n=1-3 RWMs in NSTX. This array consists of B{sub p} and B{sub r} sensors both above and below the midplane at 12 toroidal locations instrumented to detect toroidal mode numbers of n=1-3. RWM perturbations exceeding 30 G have been measured with mode growth rates on the order of 5 ms. Small modes ({delta}B