Ideal MHD limited electron temperature in spherical tokamaks

It is well documented that the central electron temperature in the National Spherical Torus Experiment (NSTX) remains largely unchanged as the external heating power, and hence the normalized volume averaged plasma pressure, $\beta$, increases.[D. Stutman, Phys. Rev. Lett. {\bf 102},115002 (2009)]. Here we present a hypothesis that low-n, pressure driven ideal magnetohydrodynamic (MHD) instabilities that are non-disruptive, can break magnetic surfaces in the central region and thereby flatten the electron temperature profiles. We demonstrate this mechanism in a 3D resistive MHD simulation of a NSTX discharge. By varying the toroidal magnetic field strength, and/othe heating power, we show that there is a critical value of $\beta$, above which the central temperature profile no longer peaks on axis.