A specific straight tokamak equilibrium surrounded by vacuum and witho
ut a conducting wall is proved to be stable to all ideal magnetohydrod
ynamic (MHD) modes by analytically evaluating linear stability. The an
alysis starts with a circular-cylindrically symmetric equilibrium whic
h has a piecewise constant current profile. The effect of corruption,
which is of great importance to the stability of axisymmetric modes, i
s taken into account by using perturbation methods. Stability of axisy
mmetric modes is proved by solving the eigenvalue problem up to second
order in the corrugation amplitude. Whereas elliptical corruption (N=
2) leads to instability for arbitrary current density, an equilibrium
with N greater-than-or-equal-to 3 May be stabilized to axisymmetric mo
des by current reversal. To treat nonaxisymmetric global modes, the po
tential energy is evaluated using tokamak scaling. A sufficient stabil
ity criterion is derived according to which the equilibrium is stable
to nonaxisymmetric modes if the current density in the outer plasma ar
ea is reversed and in the center sufficiently peaked, and if the safet
y factor q at the magnetic axis is greater than unity, increasing mono
tonically toward the plasma edge.