The ideal magnetohydrodynamic (MHD) stability limits of low aspect rat
io tokamak plasmas are computed numerically for plasmas with a range o
f cylindrical safety factors q, normalized plasma pressures beta, elo
ngations kappa and central safety factors q(0). Four distinct regimes
are optimized, namely: (a) low-q plasmas with q(0) = 1.1 with and wit
hout a stabilizing wall, (b) low-q plasmas with no wall and 1.1 < q(0
) < 2, (c) high-beta, high bootstrap fraction plasmas at moderate kapp
a requiring a wall and edge current drive and (d) high-beta, very high
bootstrap fraction plasmas with moderate to high kappa requiring a st
abilizing wall but little external current drive. A stable equilibrium
is found at an aspect ratio of A = 1.4 and an elongation of kappa = 3
.0, with 99.3% of the current provided by the plasma pressure and beta
= 45%. Special attention is paid to the issues of numerical convergen
ce and the proper definition of bootstrap current fraction.