Ra. Satnoianu et al., DIFFERENTIAL-FLOW-INDUCED INSTABILITY IN A CUBIC AUTOCATALATOR SYSTEM, Journal of engineering mathematics, 33(1), 1998, pp. 77-102
The formation of spatio-temporal stable patterns is considered for a r
eaction-diffusion-convection system based upon the cubic autocatalator
, A + 2B --> 3B, B --> C, with the reactant A being replenished by the
slow decay of some precursor P via the simple step P --> A. The react
ion is considered in a differential-flow reactor in the form of a ring
. It is assumed that the reactant A is immobilised within the reactor
and the autocatalyst B is allowed to flow through the reactor with a c
onstant velocity as well as being able to diffuse. The linear stabilit
y of the spatially uniform steady state (a, b) = (mu(-1), mu), where a
and b are the dimensionless concentrations of the reactant A and auto
catalyst B, and mu is a parameter reflecting the initial concentration
of the precursor P, is discussed first. It is shown that a necessary
condition for the bifurcation of this steady state to stable, spatiall
y non-uniform, flow-generated patterns is that the flow parameter phi
> phi(c)(mu, lambda) where phi(c)(mu, lambda) is a (strictly positive)
critical value of phi and lambda is the dimensionless diffusion coeff
icient of the species B and also reflects the size of the system. Valu
es of phi(c) at which these bifurcations occur are derived in terms of
mu and lambda. Further information about the nature of the bifurcatin
g branches (close to their bifurcation points) is obtained from a weak
ly nonlinear analysis. This reveals that both supercritical and subcri
tical Hopf bifurcations are possible. The bifurcating branches are the
n followed numerically by means of a path-following method, with the p
arameter phi as a bifurcation parameter, for representatives values of
mu and lambda. It is found that multiple stable patterns can exist an
d that it, is also possible that any of these can lose stability throu
gh secondary Hopf bifurcations. This typically gives rise to spatio-te
mporal quasiperiodic transients through which the system is ultimately
attracted to one of the remaining available stable patterns.