Plasma confined in a magnetic dipole is stabilized by the expansion of
the magnetic flux. The stability of low beta electrostatic modes in a
magnetic dipole field is examined when the distribution function is t
o lowest order Maxwellian. It is shown that for sufficiently gentle de
nsity and temperature gradients the configuration would be expected to
be stable to magnetohydrodynamic interchange, as well as to dissipati
ve trapped ion and collisionless trapped particle modes. These results
are applicable to any magnetic configuration for which the curvature
drift frequency exceeds the diamagnetic drift frequency. (C) 1997 Amer
ican Institute of Physics.