A system of equations that couples the rapidly varying fluctuations of
resistive ballooning modes to the slowly varying transport of the den
sity, vorticity and parallel momentum have been derived and solved num
erically. Only a single toroidal mode number is retained in the presen
t work. The low-mode (L-mode) phase consists of strong poloidally asym
metric particle transport driven by resistive ballooning modes, with l
arger flux on The outboard side compared to the inboard side. With the
onset of shear flow driven by a combination of toroidal drive mechani
sms as well as the Reynolds stress, the fluctuations associated with t
he resistive ballooning modes are attenuated leading to a strong reduc
tion in the particle transport. The drop in the particle transport res
ults in steepening of the density profile leading to the high-mode (H-
mode). (C) 1996 American Institute of Physics.