The Hasegawa-Wakatani model equations for resistive drift waves are so
lved numerically for a range of values of the coupling due to the para
llel electron motion. The largest Lyapunov exponent, lambda(1), is cal
culated to quantify the unpredictability of the turbulent flow and com
pared to other characteristic inverse time scales of the turbulence su
ch as the linear growth rate and Lagrangian inverse time scales obtain
ed by tracking virtual fluid particles. The results show a correlation
between lambda(1) and the relative dispersion exponent, lambda(p), as
well as to the inverse Lagrangian integral time scale tau(i)(-1). A d
ecomposition of the flow into two distinct regions with different rela
tive dispersion is recognized as the Weiss decomposition [J. Weiss, Ph
ysica D 48, 273 (1991)]. The regions in the turbulent flow which contr
ibute to lambda(1) are found not to coincide with the regions which co
ntribute most to the relative dispersion of particles. (C) 1996 Americ
an Institute of Physics.