Theoretically, high-beta (beta similar to 1) tokamaks offer a large fusion
power efficiency advantage over low-beta devices. However, if high-beta tok
amaks are inherently unstable then such devices will never be realized. In
particular, kink modes are thought to be the most serious obstacle to high-
beta operations. High-beta tokamaks are characterized by a very large Shafr
anov shift with a thin "boundary layer" on the outboard side of the device
and a large "core" region of vertical flux surfaces comprising most of the
central volume. In this paper, the energy principle is used to compute the
magnetohydrodynamic internal kink stability of such devices in the large as
pect ratio limit with a low toroidal mode number. A class of internal kink
mode similar to the usual low-beta kink is present; the stability against t
hese modes is computed. A set of parameters describing a kink stable high-b
eta equilibrium is given. Stability is shown to be dependent on the shape o
f the plasma boundary. (C) 2000 American Institute of Physics. [S1070-664X(
00)00510-3].