In general, turbulent transport drives a plasma toward a state of turb
ulent equipartition, in which Lagrangian invariants are uniformly dist
ributed. Different invariants decay with different rates, and in tokam
aks the frozen-in law of particles in the poloidal magnetic field surv
ives longer than the corresponding law for the toroidal field, assumin
g that the trapped particles dominate the turbulent transport. Therefo
re, the plasma profiles depend on the safety factor q(r), and the cond
ition for convection of trapped particles is that the shear dq/dr is p
ositive. There are two ways to suppress this convection and thereby en
hance confinement. The first one is to reverse the magnetic shear. The
energy of typical trapped particles then increases outward instead of
inward, which suppresses instabilities. The second method is to elimi
nate the trapped ions by poloidal rotation, and thereby create a trans
port barrier. (C) 1997 American Institute of Physics.