An extension of Carreau and Carreau-Yasuda rheological models to porous media is proposed to study the onset of mixed convection of both pseudoplastic fluids (PF) and dilatant fluids (DF) in a porous layer heated from below in the presence of a horizontal throughflow. In comparison with Newtonian fluids, three more dimensionless parameters are introduced, namely, the Darcy-Weissenberg number Wi, the power-law index n, and the Yasuda parameter a. Temporal stability analysis of the basic state showed that in the absence of a throughflow (Wi = 0), the critical Rayleigh number and the critical wavenumber at the onset of convection are the same as for Newtonian fluids, namely, R a c = 4 π 2 and k c = π, respectively. When the throughflow is added (Wi > 0), it is found that moving transverse rolls (stationary longitudinal rolls) are the dominant mode of the instability for PF (for DF). Furthermore, depending on Wi, two regimes of instability were identified. In the weakly non-Newtonian regime (i.e., W i
CITATION STYLE
Brandão, P. V., Ouarzazi, M. N., Hirata, S. C., & Barletta, A. (2021). Darcy-Carreau-Yasuda rheological model and onset of inelastic non-Newtonian mixed convection in porous media. Physics of Fluids, 33(4). https://doi.org/10.1063/5.0048143
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