Abstract
The linear and the nonlinear dynamics of open unstable flow in a finite domain of size L is studied on a modified supercritical Ginzburg-Landau equation. When the advection term is nonzero, the bifurcation to a finite-amplitude state occurs when the instability is absolute, even for large L. The standard weakly nonlinear theory is limited to a control parameter domain of size varying as L-5 due to the nonnormality of the linear evolution operator. The fully nonlinear solution is given and two generic cases are discussed: a supercritical case in which the instability is absolute and a subcritical case in which the instability is solely convective. The subcritical case gives a mathematical example of a bypass transition due to transient growth. The supercritical case allows a fully quantitative comparison, including the effect of the domain size, with results obtained by Büchel et al. for the size of the bifurcated solutions in the Taylor-Couette problem with throughflow.
| Original language | English |
|---|---|
| Pages (from-to) | 2977-2983 |
| Number of pages | 7 |
| Journal | Physics of Fluids |
| Volume | 11 |
| Issue number | 10 |
| DOIs | |
| Publication status | Published - 1 Jan 1999 |
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