Ideal magnetohydrodynamic stability to the n=1 and n=2 modes are calculated
for spheromak equilibria in flux conserver shapes, which include a midplan
e gap, conforming outer wall, and concave side walls. The equilibria are fo
rce-free (del xB=lambda(psi)B) but not minimum energy states and, therefore
, have nonuniform lambda(psi) profiles. For each flux conserver shape, the
equilibrium with the most hollow linear lambda(psi) profile is found that i
s stable to the n=1 and n=2 modes. The Mercier beta limit is calculated for
each flux conserver shape using the most hollow current profile constraine
d by the stability boundary. The results show that a stable high <beta > (>
10%) spheromak equilibrium can be produced using a concave flux conserver,
improving energy confinement times and plasma performance. (C) 2000 Americ
an Institute of Physics. [S1070-664X(00)04707-8].