Competition between merging and bifurcation in the generalized Rayleigh-Taylor instability
The nonlinear evolution of bubble and spike fronts growing through the generalized Rayleigh-Taylor instability are studied by numerical simulations and by solving an extension of Alon's [Phys. Rev. E 48, 1008 (1993)2470-004510.1103/PhysRevE.48.1008] statistical model based on the asymptotic velocity of a single-mode bubble and the merging bubble process. In this work, the generalized Rayleigh-Taylor instability includes a frictional force due to collision with a secondary fluid. Depending on its strength the behavior during the nonlinear stage leads to two different regimes: the first is the classical inertial case where the bubble front is known to grow as h∝t^{2} and evolves towards large structures, and the second is the collisional case where the front grows as h∝t and maintains structures of relatively constant size. In this new regime, the importance of adding the bifurcation process, the opposite process of merging, is highlighted.
Authors
- B. Bernecker (ORCID: https://orcid.org/0000-0002-0600-1448)
- B. Canaud (ORCID: https://orcid.org/0009-0000-4342-7635)
- Q. Cauvet (ORCID: https://orcid.org/0000-0002-3575-1563)
Institutions
- Commissariat à l'Énergie Atomique et aux Énergies Alternatives (FR)
- Université Paris-Saclay (FR)
- CEA DAM Île-de-France (FR)
Publication Details
- Journal
- Physical review. E
- Published
- 2024-11-05
- DOI
- https://doi.org/10.1103/physreve.110.055201
- Primary Topic
- Particle Dynamics in Fluid Flows
- Type
- article
- Field-Weighted Citation Impact
- 0.00