Abstract
We present an investigation on the onset of Darcy–Benard instability in a two-dimensional porous medium saturated with a non-Newtonian fluid and heated from below in the presence of a uniform horizontal pressure gradient. The fluid is taken to be of power-law nature with constant rheological index and temperature-dependent consistency index . A two-dimensional linear stability analysis in the vertical plane yields the critical wavenumber and the generalised critical Rayleigh number as functions of dimensionless problem parameters, with a non-monotonic dependence from and with maxima/minima at given values of , a parameter representing the effects of consistency index variations due to temperature. A series of experiments are conducted in a Hele-Shaw cell of aspect ratio to provide a verification of the theory. Xanthan Gum mixtures (nominal concentration from 0.10 % to 0.20 %) are employed as working fluids with a parameter range and . The experimental critical wavenumber corresponding to incipient instability of the convective cells is derived via image analysis for different values of the imposed horizontal velocity. Theoretical results for critical wavenumber favourably compare with experiments, systematically underestimating their experimental counterparts by 10 % at most. The discrepancy between experiments and theory is more relevant for the critical Rayleigh number, with theory overestimating the experiments by a maximum factor less than two. Discrepancies are attributable to a combination of factors: nonlinear phenomena, possible subcritical bifurcations, and unaccounted-for disturbing effects such as approximations in the rheological model, wall slip, ageing and degradation of the fluid properties.
Highlights
Thermal instability of saturated porous media has been intensively investigated with analytical tools (for a survey see Rees (2000), Nield & Bejan (2013)) since the early studies of Horton & Rogers (1945) and Lapwood (1948), subsequently extended to include parallel horizontal flow (Prats 1966)
We present an investigation on the onset of Darcy–Bénard instability in a twodimensional porous medium saturated with a non-Newtonian fluid and heated from below in the presence of a uniform horizontal pressure gradient
A two-dimensional linear stability analysis in the vertical plane yields the critical wavenumber and the generalised critical Rayleigh number as functions of dimensionless problem parameters, with a non-monotonic dependence from n and with maxima/minima at given values of γ, a parameter representing the effects of consistency index variations due to temperature
Summary
Thermal instability of saturated porous media has been intensively investigated with analytical tools (for a survey see Rees (2000), Nield & Bejan (2013)) since the early studies of Horton & Rogers (1945) and Lapwood (1948), subsequently extended to include parallel horizontal flow (Prats 1966). Recent literature further broadens the analysis to cover non-Newtonian fluids, from power law (Hirata & Ouarzazi 2010; Barletta & Nield 2011; Nield 2011a,b; Alloui et al 2012; Alves & Barletta 2013; Barletta & Storesletten 2016; Celli et al 2017), to Bingham (Rees 2015) or viscoelastic (Hirata et al 2015); this entails additional complexity deriving from fluid rheology. Rayleigh–Bénard convection in porous media has been studied by means of the Hele-Shaw analog model (see, for example, Hartline & Lister (1977), Cherkaoui & Wilcock (2001) and Letelier et al (2016)), originally developed for Newtonian fluids and recently extended to non-Newtonian power-law fluids (Longo, Di Federico & Chiapponi 2015; Ciriello et al 2016): the porous medium is replaced with a small gap between two flat plates; this entails advantages and disadvantages. The onset of convection in viscoplastic fluids, including the effects of wall slip, was analysed by Métivier & Magnin (2011) and Darbouli et al (2013); a more complex scenario, with Carbopol behaving like a single or a double-phase continuum, has been analysed in Métivier, Li & Magnin (2017)
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