A two-dimensional slab model for resistive drift waves in plasmas cons
isting of two coupled nonlinear partial differential equations for the
density perturbation n and the electrostatic potential perturbation p
hi is investigated. The drift waves are linearly unstable, and a quasi
-stationary turbulent state is reached in a finite time, independent o
f the initial conditions. Different regimes of the turbulent state can
be obtained by varying the coupling parameter C, related to the paral
lel electron dynamics. The turbulence is described by using particle t
racking and tools from chaos analysis. The largest Lyapunov exponent l
ambda(1) is calculated for different values of C to quantify the chaot
icity and compared with Lagrangian inverse time scales obtained by tra
cking virtual fluid particles.