Three-dimensional magnetohydrodynamic simulations of high-beta plasmas
show that toroidally localized high-n ballooning modes can be driven
unstable by the local pressure steepening that arises from the evoluti
on of low-n modes. Nonlinearly, the high-n mode becomes even more loca
lized and produces a strong local pressure bulge that destroys the flu
x surfaces resulting in a thermal quench. The flux surfaces then recov
er temporarily but now contain large magnetic islands. This scenario i
s supported by experimental data.