2007
DOI: 10.1063/1.2405129
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On the classification of buoyancy-driven chemo-hydrodynamic instabilities of chemical fronts

Abstract: Exothermic autocatalytic fronts traveling in the gravity field can be deformed by buoyancy-driven convection due to solutal and thermal contributions to changes in the density of the product versus the reactant solutions. We classify the possible instability mechanisms, such as Rayleigh-Bénard, Rayleigh-Taylor, and double-diffusive mechanisms known to operate in such conditions in a parameter space spanned by the corresponding solutal and thermal Rayleigh numbers. We also discuss a counterintuitive instability… Show more

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Cited by 43 publications
(44 citation statements)
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“…6 The fact that heat diffuses more rapidly than mass and also the possible competition between antagonistic solutal and thermal buoyancy effects is expected to lead to interesting new dynamics as is the case for fronts traveling in vertical geometries. 20,21 In parallel, this work complements our previous studies 9,10 of the influence of pure Marangoni stresses on the deformation and acceleration of fronts traveling in horizontal layers open to the air but in the absence of gravity. In practice, in such geometries, Marangoni and buoyancy effects will most often both be present.…”
Section: Discussionsupporting
confidence: 76%
See 1 more Smart Citation
“…6 The fact that heat diffuses more rapidly than mass and also the possible competition between antagonistic solutal and thermal buoyancy effects is expected to lead to interesting new dynamics as is the case for fronts traveling in vertical geometries. 20,21 In parallel, this work complements our previous studies 9,10 of the influence of pure Marangoni stresses on the deformation and acceleration of fronts traveling in horizontal layers open to the air but in the absence of gravity. In practice, in such geometries, Marangoni and buoyancy effects will most often both be present.…”
Section: Discussionsupporting
confidence: 76%
“…19 In such a vertical orientation, hydrodynamic flows are due to Rayleigh-Taylor, Rayleigh-Bénard, doublediffusive, or even chemically driven instabilities. 20,21 Flows are triggered typically when the heavier solution lies on top of the lighter one or if double-diffusive effects due to the differential diffusivity of mass and heat are involved. Otherwise, the front remains planar and travels at a reactiondiffusion ͑RD͒ speed v as in a gel.…”
Section: Introductionmentioning
confidence: 99%
“…[19][20][21][22][23][24] Various scenarios of buoyancy-driven instabilities have been shown to arise from the combination of solutal and thermal contributions to the density difference across the front. 9,[25][26][27][28][29] In horizontal geometries, the situation can become even more complicated if the solution is open to air. Indeed, besides possible density gradients, there is an additional source of fluid motions, the Marangoni effects triggered by surface tension gradients at the air-liquid interface.…”
Section: Introductionmentioning
confidence: 99%
“…[4][5][6][7][8][9][10][11][12] In that case, the combination of solutal and thermal contributions to the density jump has been shown to lead to various instability scenarios depending on whether ⌬ S and ⌬ T have the same negative sign ͑coop-erative case͒ or different signs ͑⌬ S Ͼ 0, ⌬ T Ͻ 0, antagonistic case͒. 6,13,14 In thin horizontal solution layers, it is known that convection can also deform the dynamic of autocatalytic fronts or waves. 4,[15][16][17][18][19][20][21] In the case of a simple reaction front propagating horizontally, it has been shown both experimentally 17,18,22 and numerically 16,23 that instead of a gravity current leading to a homogeneous solution, the coupling between reaction, diffusion, and convection triggered by the density difference leads in isothermal conditions to CHAOS 19, 023110 ͑2009͒ one solitary vortex structure deforming the front and speeding it up.…”
Section: Introductionmentioning
confidence: 99%