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Phys. Rev. E 64, 046307 (2001) [13 pages]

Front propagation in laminar flows

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M. Abel1,4, A. Celani2, D. Vergni1,3, and A. Vulpiani1,3
1Dipartimento di Fisica, Universitá di Roma “La Sapienza” Piazzale Aldo Moro 2, I-00185 Roma, Italy
2CNRS, INLN, 1361 Route des Lucioles, F-06560 Valbonne, France
3INFM unità di Roma “La Sapienza” Piazzale Aldo Moro 2, I-00185 Roma, Italy
4University of Potsdam, Am Neuen Palias 19, 14469 Potsdam, Germany

Received 13 June 2001; published 25 September 2001

The problem of front propagation in flowing media is addressed for laminar velocity fields in two dimensions. Three representative cases are discussed: stationary cellular flow, stationary shear flow, and percolating flow. Production terms of Fisher-Kolmogorov-Petrovskii-Piskunov type and of Arrhenius type are considered under the assumption of no feedback of the concentration on the velocity. Numerical simulations of advection-reaction-diffusion equations have been performed by an algorithm based on discrete-time maps. The results show a generic enhancement of the speed of front propagation by the underlying flow. For small molecular diffusivity, the front speed Vf depends on the typical flow velocity U as a power law with an exponent depending on the topological properties of the flow, and on the ratio of reactive and advective time scales. For open-streamline flows we find always VfU, whereas for cellular flows we observe VfU1/4 for fast advection and VfU3/4 for slow advection.

© 2001 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevE.64.046307
DOI:
10.1103/PhysRevE.64.046307
PACS:
47.27.Qb, 47.70.Fw