Abstract
We present a mechanism of limitation for the possible wave numbers above an instability threshold. This mechanism is experimentally investigated in the interfacial instability of directional viscous fingering in a finite system. It is shown experimentally to be controlled by the divergence of a phase-diffusion constant. Theoretically, this limitation on the low value of the accessible wave numbers is a consequence of the interaction between the fundamental and the first harmonic modes. The analysis of coupled amplitude equations demonstrates theoretically the existence of a divergence of a phase-diffusion constant when approaching the threshold of a parity-breaking instability.
| Original language | English |
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| Pages (from-to) | 565-574 |
| Number of pages | 10 |
| Journal | Physical Review E |
| Volume | 58 |
| Issue number | 1 |
| DOIs | |
| Publication status | Published - 1 Jan 1998 |