We introduce a "spatial" Lyapunov exponent to characterize the complex beha
vior of non-chaotic but convectively unstable flow sytems. This complexity
is of spatial type and is due to sensitivity to the boundary conditions. We
show that there exists a relation between the spatial-complexity index we
define and the comoving Lyapunov exponents. In such systems the transition
to chaos, i.e., the occurrence of a positive Lyapunov exponent, can manifes
t itself in two different ways. In the first case (from neither chaotic nor
spatially complex behavior to chaos) one observes the typical scenario; i.
e., as the system size grows up the spectrum of the Lyapunov exponents give
s rise to a density. In the second case (when the chaos develops from a con
vectively unstable situation) one observes only a finite number of positive
Lyapunov exponents. (C) 1999 Elsevier Science B.V. All rights reserved.