2019
DOI: 10.1063/1.5102063
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Existence and nonlinear stability of convective solutions for almost compressible fluids in Bénard problem

Abstract: We study the nonlinear almost compressible 2D Oberbeck-Boussinesq system, characterized by an extra buoyancy term where the density depends on the pressure, and a corresponding dimensionless parameter β, proportional to the (positive) compressibility factor β 0. The local in time existence of the perturbation to the conductive solution is proved for any "size" of the initial data. However, unlike the classical problem where β 0 = 0, a smallness condition on the initial data is needed for global in time existen… Show more

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Cited by 9 publications
(11 citation statements)
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“…Let us denote by H −1 the dual space of H. We show the following lemma that in the case α < 2π was proved in [2,4] by different arguments. Since F ∈ L 2 (Ω 0 ), by classical elliptic regularity we get that q ∈ W 2,2 (Ω 0 ), and that it satisfies (4.5) along with q 2,2 ≤ C M 2 .…”
Section: Preliminary Resultsmentioning
confidence: 90%
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“…Let us denote by H −1 the dual space of H. We show the following lemma that in the case α < 2π was proved in [2,4] by different arguments. Since F ∈ L 2 (Ω 0 ), by classical elliptic regularity we get that q ∈ W 2,2 (Ω 0 ), and that it satisfies (4.5) along with q 2,2 ≤ C M 2 .…”
Section: Preliminary Resultsmentioning
confidence: 90%
“…Motivated by this important issues, the author jointly with D. Grandi rigorously derived, by perturbative methods from the full set of balance laws, new models where the density, ρ, may depend on both T and p [12,13], while for related ones, the authors addressed well-posedness and stability questions, in [2,4,5]. In particular, in [13], we proposed a new model for thermal convection in a horizontal layer of fluid heated from below with ρ = ρ(T, p).…”
Section: Introductionmentioning
confidence: 99%
“…As is well known, one of the most accepted models in the study of convection problems in fluid mechanics is the socalled Oberbeck-Boussinesq approximation (hereafter denoted by O-B) [1][2][3][4][5]. e latter is characterized by the fact that one keeps the fluid incompressible and allows for density changes only in the buoyancy term of the linear momentum equation, by assuming a linear dependence on temperature.…”
Section: Introductionmentioning
confidence: 99%
“…Notice that (1) tends to the motionless solution for the same problem in the O-B approximation by letting β ⟶ 0. In [4,9,12], the linear and nonlinear stability of r 0 , as well as the existence and uniqueness for the associated "perturbed problem," was investigated. All this work was done in the case of the plane flow.…”
Section: Introductionmentioning
confidence: 99%
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