Front propagation in Rayleigh-Taylor systems with reaction

A special feature of Rayleigh-Taylor systems with chemical reactions is the competition between turbulent mixing and the "burning processes", which leads to a highly non-trivial dynamics. We studied the problem performing high resolution numerical simulations of a 2d system, using a thermal lattice Boltzmann (LB) model. We spanned the various regimes emerging at changing the relative chemical/turbulent time scales, from slow to fast reaction; in the former case we found numerical evidence of an enhancement of the front propagation speed (with respect to the laminar case), providing a phenomeno... Mehr ...

Verfasser: Mauro Sbragaglia
Luca Biferale
Filippo Mantovani
Raffaele Tripiccione
Marcello Pivanti
Fabio Pozzati
Sebastiano Fabio Schifano
Federico Toschi
Andrea Scagliarini
Dokumenttyp: Artikel
Erscheinungsdatum: 2011
Schlagwörter: Netherlands / Digital Humanities and Cultural Heritage / Social Science and Humanities / General Physics and Astronomy
Sprache: unknown
Permalink: https://search.fid-benelux.de/Record/base-26811595
Datenquelle: BASE; Originalkatalog
Powered By: BASE
Link(s) : https://www.openaccessrepository.it/record/139581

A special feature of Rayleigh-Taylor systems with chemical reactions is the competition between turbulent mixing and the "burning processes", which leads to a highly non-trivial dynamics. We studied the problem performing high resolution numerical simulations of a 2d system, using a thermal lattice Boltzmann (LB) model. We spanned the various regimes emerging at changing the relative chemical/turbulent time scales, from slow to fast reaction; in the former case we found numerical evidence of an enhancement of the front propagation speed (with respect to the laminar case), providing a phenomenological argument to explain the observed behaviour. When the reaction is very fast, instead, the formation of sharp fronts separating patches of pure phases, leads to an increase of intermittency in the small scale statistics of the temperature field.