Three-dimensional nonlinear simulations of collisional plasma turbulen
ce are presented to model the behavior of the edge region of tokamak d
ischarges. Previous work is extended by including electron temperature
fluctuations (T) over tilde(e). The basic paradigm that turbulence an
d transport are controlled by resistive ballooning modes in low temper
ature plasma and nonlinearly driven drift wave turbulence in higher te
mperature regimes persists in the new system. Parallel thermal conduct
ion strongly suppresses the ability of the electron temperature gradie
nt del T-e to drive the turbulence and transport everywhere except the
very low temperature edge of the resistive ballooning regime. As a co
nsequence, over most of the resistive ballooning regime only the densi
ty gradient drives the turbulence and the temperature fluctuations are
convected as a passive scalar. In the drift wave regime only the dens
ity gradient acts to drive the nonlinear instability and the temperatu
re fluctuations have a relatively strong stabilizing influence on the
turbulence due to an enhanced damping of density and potential fluctua
tions resulting from local electron heating. (C) 1997 American Institu
te of Physics.