Wavepacket instability in a rectangular porous channel uniformly heated from below

•We investigate the thermal instability in a porous horizontal rectangular channel.•We consider a parallel flow basic solution for heating from below with uniform flux.•The linear stability of the basic solution is investigated.•Convective/absolute instability is influenced by the upper wall cooling...

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Published inInternational journal of heat and mass transfer Vol. 147; p. 118993
Main Authors Barletta, A., Celli, M., Brandão, P.V., Alves, L.S. de B.
Format Journal Article
LanguageEnglish
Published Oxford Elsevier Ltd 01.02.2020
Elsevier BV
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Summary:•We investigate the thermal instability in a porous horizontal rectangular channel.•We consider a parallel flow basic solution for heating from below with uniform flux.•The linear stability of the basic solution is investigated.•Convective/absolute instability is influenced by the upper wall cooling condition.•An analytical approximate solution exists assuming large Péclet numbers. This paper is aimed to investigate the transition to absolute instability in a porous layer with horizontal throughflow. The importance of this analysis is due to the possible experimental failure to detect growing perturbations which are localised in space and which may be convected away by the throughflow. The instability of the uniform flow in a horizontal rectangular channel subject to uniform heating from below and cooled from above is studied. While the lower wall is modelled as an impermeable isoflux plane, the upper wall is assumed to be impermeable and imperfectly conducting, so that a Robin temperature condition with a given Biot number is prescribed. The sidewalls are assumed to be adiabatic and impermeable. The basic state considered here is a stationary parallel flow with a vertical uniform temperature gradient, namely the typical configuration describing the Darcy–Bénard instability with throughflow. The linear instability of localised wavepackets is analysed, thus detecting the parametric conditions for the transition to absolute instability. The absolute instability is formulated through an eigenvalue problem based on an eighth–order system of ordinary differential equations. The solution is sought numerically by utilising the shooting method. The threshold to absolute instability is detected versus the Péclet number associated with the basic flow rate along the channel.
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content type line 14
ISSN:0017-9310
1879-2189
DOI:10.1016/j.ijheatmasstransfer.2019.118993