The combined, finite time effects of molecular diffusion and chaotic advect
ion on a finite distribution of scalar are studied in the context of time p
eriodic, recirculating flows with variable stirring frequency. Comparison o
f two disparate frequencies with identical advective fluxes indicates that
diffusive effects are enhanced for slower oscillations. By examining the ge
ometry of the chaotic advection in both high and low frequency limits, the
flux function and the width of the stochastic zone are found to have a univ
ersal frequency dependence for a broad class of flows. Furthermore, such sy
stems possess an adiabatic transport mechanism which results in the establi
shment of a ''Lagrangian steady state,'' where only the asymptotically inva
riant core remains after a single advective cycle. At higher frequencies, t
ransport due to chaotic advection is confined to exchange along the perimet
er of the recirculating region. The effects of molecular diffusion on the t
otal transport are different in these two cases and it is argued and demons
trated numerically that increasing the diffusion coefficient tin some presc
ribed range) leads to a dramatic increase in the transport only for low fre
quency stirring. The frequency dependence of the total, long time transport
of a limited amount of scalar is more involved since faster stirring leads
to smaller invariant core sizes. (C) 1999 American Institute of Physics. [
S1070-6631(99)04308-1].