2020
DOI: 10.1007/s10915-020-01305-x
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A Fully-Mixed Formulation for the Steady Double-Diffusive Convection System Based upon Brinkman–Forchheimer Equations

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Cited by 15 publications
(15 citation statements)
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“…In what follows we consider the model introduced in [28] (see also [13,Section 2]), which is given by a steady double-diffusive convection system in a fluid saturated porous medium. More precisely, we focus on solving the coupling of the incompressible Brinkman-Forchheimer and double-diffusion equations, which reduces to finding a velocity field u, a pressure field p, a temperature field φ 1 and a concentration field φ 2 , the latter two defining a vector φ := (φ 1 , φ 2 ), such that…”
Section: The Model Problemmentioning
confidence: 99%
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“…In what follows we consider the model introduced in [28] (see also [13,Section 2]), which is given by a steady double-diffusive convection system in a fluid saturated porous medium. More precisely, we focus on solving the coupling of the incompressible Brinkman-Forchheimer and double-diffusion equations, which reduces to finding a velocity field u, a pressure field p, a temperature field φ 1 and a concentration field φ 2 , the latter two defining a vector φ := (φ 1 , φ 2 ), such that…”
Section: The Model Problemmentioning
confidence: 99%
“…Next, in order to derive a new fully-mixed formulation for (2.1)-(2.5), and unlike [13], we do not employ any augmentation procedure and simply proceed as in [17] (see also [18]). More precisely, we now introduce as further unknowns the velocity gradient t, the pseudostress tensor σ, the temperature/concentration gradient t j , and suitable auxiliary variables ρ j depending on t j , u, and φ j , all of which are defined, respectively, by…”
Section: The Model Problemmentioning
confidence: 99%
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