Abstract
We study the pattern selection and the dynamics of a bifurcating system such as Taylor-Couette flow or Rayleigh-Bénard convection, subject to an externally imposed cross flow using the complex Ginzburg-Landau equation as a qualitative model. We show that the bifurcation scenario is radically modified by the introduction of a cross flow, and that a nonlinear global mode, i.e., a nonlinear oscillating solution in a semi-infinite domain [0,+∞), with a homogeneous condition at x=0, exists only when the basic state is linearly absolutely unstable. We derive the scaling law for the characteristic growth size, which varies as ε−1/2(ε being the criticality parameter), and compares satisfactorily with numerical and experimental results from the literature.
| Original language | English |
|---|---|
| Pages (from-to) | 2666-2669 |
| Number of pages | 4 |
| Journal | Physical Review Letters |
| Volume | 79 |
| Issue number | 14 |
| DOIs | |
| Publication status | Published - 1 Jan 1997 |
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