The three-dimensional stability of finite-amplitude convection in a layered porous medium heated from below

Author:

Rees D. A. S.,Riley D. S.

Abstract

Landau–Ginzburg equations are derived and used to study the three-dimensional stability of convection in a layered porous medium of infinite horizontal extent. Criteria for the stability of convection with banded or square planform are determined and results are presented for two-layer and symmetric three-layer systems. In general the neutral curve is uni-modal and parameter space is divided into regions where either rolls or square cells are stable. For certain ranges of parameters, however, the neutral curve is bimodal and there exists a locus of parameters where two modes with different wavenumbers have simultaneous onset.

Publisher

Cambridge University Press (CUP)

Subject

Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics

Reference43 articles.

1. Kvernvold, O. & Tyvand, P. A. 1980 Dispersion effects on thermal convection in porous media.J. Fluid Mech. 99,673–686.

2. Rees, D. A. S. & Riley, D. S. 1989b The effects of boundary imperfections on convection in a saturated porous layer: non-resonant wavelength excitation..Proc. R. Soc. Lond. A421,303–329.

3. Palm, E. , Weber, J. E. & Kvernvold, O. 1972 On steady convection in a porous medium.J. Fluid Mech. 54,153–161.

4. Pillatsis, G. , Taslim, M. E. & Narusawa, U. 1987 Thermal instability of a fluid-saturated porous medium bounded by thin fluid layers. Trans. ASME C: J. Heat Transfer 109,677–682.

5. Rees, D. A. S. & Riley, D. S. 1989a The effects of boundary imperfections on convection in a saturated porous layer: near-resonant wavelength excitation.J. Fluid Mech. 199,133–154.

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