  The QCD phase transition is studied on 32^3x8 quenched lattices. One expects
from simple arguments that the quenched chiral condensate should diverge as the
chiral limit is approached. Previous studies have not been able to observe this
behavior, perhaps due to relatively large lattice spacings used. The topic is
revisited here on N_t=8 lattices, where the physical spacing is approximately
2(Gev^-1).
