The effects of a differential flow of the components of a reaction-dif
fusion system which is close to its stability boundary are described w
ithin the long wavelength approximation. In the vicinity of the Hopf b
ifurcation the system's evolution is governed by a complex Ginzburg-La
ndau equation modified by a purely imaginary convective term. If the s
ystem is near the zero real eigenvalue bifurcation, the governing equa
tion is a modified Swift-Hohenberg equation, In both cases the homogen
eous, stable reference steady state may be destabilized by the differe
ntial flow. In the Ginzburg-Landau equation, the destabilization occur
s as long as the flow velocity exceeds some critical value upsilon(cr)
, which tends to zero as the system approaches the Hopf bifurcation. I
n the modified Swift-Hohenberg equation, the flow has either a destabi
lizing or stabilizing effect, depending on the sign of one of the syst
em parameters. Destabilization occurs when the flow velocity exceeds s
ome threshold; however in this case, the threshold remains finite even
at the bifurcation point. In both Ginzburg-Landau and Swift-Hohenberg
equations the differential flow instability produces traveling plane
waves. The stability analysis shows that once a periodic plane wave is
established, its spatial period remains unchanged over a finite range
of the flow velocity and changes in discrete steps - the phenomenon o
f 'wavenumber locking'. Wavenumber locking' is verified in numerical e
xperiments with the Ginzburg-Landau equation. Near Hopf bifurcation, t
he Benjamin-Feir instability may occur. In this case irregular traveli
ng waves are found, but a regular component of the wave pattern surviv
es. Depending on a parameter, the differential flow either promotes or
deters the Benjamin-Feir instability. As a result, the increasing flo
w may switch the periodic wave pattern into a irregular state or, conv
ersely, may stabilize the previously induced irregular pattern and pro
duce periodic waves.