2013
DOI: 10.1016/j.apnum.2012.06.034
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Finite element analysis of a projection-based stabilization method for the Darcy–Brinkman equations in double-diffusive convection

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Cited by 29 publications
(19 citation statements)
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“…Suppose Γ D = ∂Ω\Γ B , where Γ B is a regular open subset of ∂Ω . Consider the following time-dependent Darcy–Brinkman equations in a dimensionless form (Çıbık and Kaya, 2013; Goyeau et al , 1996): where u , p , T and C are the velocity, pressure, temperature and concentration fields, respectively; f u , f T and f C are three source terms. Besides, ν represents the kinematic viscosity; γ T and γ C the thermal diffusivity and mass diffusivity, respectively; Da the Darcy number; g the gravitational acceleration vector; and β T and β C the thermal and solutal expansion coefficients, respectively.…”
Section: Introductionmentioning
confidence: 99%
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“…Suppose Γ D = ∂Ω\Γ B , where Γ B is a regular open subset of ∂Ω . Consider the following time-dependent Darcy–Brinkman equations in a dimensionless form (Çıbık and Kaya, 2013; Goyeau et al , 1996): where u , p , T and C are the velocity, pressure, temperature and concentration fields, respectively; f u , f T and f C are three source terms. Besides, ν represents the kinematic viscosity; γ T and γ C the thermal diffusivity and mass diffusivity, respectively; Da the Darcy number; g the gravitational acceleration vector; and β T and β C the thermal and solutal expansion coefficients, respectively.…”
Section: Introductionmentioning
confidence: 99%
“…For our study, we introduce some important dimensionless parameters used in (Çıbık and Kaya, 2013): the thermal Grashof number GrT=gβTTH3ν2, the solutal Grashof number GrC=gβCCH3ν2, the buoyancy ratio N=βCCβTT, the Prandtl number Pr=νγT, the Schmidt number Sc=νγC, the Lewis number Le=ScPr and the Darcy number Da=KH2, where H , K , △ T and △ C denote the cavity height, permeability, characteristics temperature and concentration differences along the enclosure, respectively. We will use another dimensionless parameter, namely, the thermal Rayleigh number Ra = Gr T PrDa for comparison issues.…”
Section: Introductionmentioning
confidence: 99%
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“…Standard numerical methods for solving singularly perturbed problems are unstable and do not give accurate results due to the perturbation parameter  . If suitable numerical methods such as finite difference method and finite element method [1][2][3][4][5][6][7][8] for solving these problems are developed, then the stable and accurate results are obtained. Therefore, we prefer to apply finite difference method for this problem in this paper.…”
Section: Introductionmentioning
confidence: 99%