Beta-limiting instabilities and global mode stabilization in the National Spherical Torus Experiment

Research on the stability of spherical torus plasmas at and above the no-wall beta limit is being addressed on the National Spherical Torus Experiment [M. Ono , Nucl. Fusion 40, 557 (2000)], that has produced low aspect ratio plasmas, R/asimilar to1.27 at plasma current exceeding 1.4 MA with high energy confinement (TauE/TauE_ITER89P>2). Toroidal and normalized beta have exceeded 25% and 4.3, respectively, in qsimilar to7 plasmas. The beta limit is observed to increase and then saturate with increasing l(i). The stability factor beta(N)/l(i) has reached 6, limited by sudden beta collapses. Increased pressure peaking leads to a decrease in beta(N). Ideal stability analysis of equilibria reconstructed with EFIT [L. L. Lao , Nucl. Fusion 25, 1611 (1985)] shows that the plasmas are at the no-wall beta limit for the n=1 kink/ballooning mode. Low aspect ratio and high edge q theoretically alter the plasma stability and mode structure compared to standard tokamak configurations. Below the no-wall limit, stability calculations show the perturbed radial field is maximized near the center column and mode stability is not highly effected by a nearby conducting wall due to the short poloidal wavelength in this region. In contrast, as beta reaches and exceeds the no-wall limit, the mode becomes strongly ballooning with long poloidal wavelength at large major radius and is highly wall stabilized. In this way, wall stabilization is more effective at higher beta in low aspect ratio geometry. The resistive wall mode has been observed in plasmas exceeding the ideal no-wall beta limit and leads to rapid toroidal rotation damping across the plasma core. (C) 2002 American Institute of Physics.