On numerical stability analysis of double-diffusive convection in confined enclosures
The onset of thermosolutal convection and finite-amplitude flows, due to vertical gradients of heat and solute, in a horizontal rectangular enclosure are investigated analytically and numerically. Dirichlet or Neumann boundary conditions for temperature and solute concentration are applied to the tw...
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Published in | Journal of fluid mechanics Vol. 433; pp. 209 - 250 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Cambridge, UK
Cambridge University Press
25.04.2001
|
Subjects | |
Online Access | Get full text |
ISSN | 0022-1120 1469-7645 |
DOI | 10.1017/S0022112000003451 |
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Abstract | The onset of thermosolutal convection and finite-amplitude flows, due to vertical
gradients of heat and solute, in a horizontal rectangular enclosure are investigated
analytically and numerically. Dirichlet or Neumann boundary conditions for temperature
and solute concentration are applied to the two horizontal walls of the
enclosure, while the two vertical ones are assumed impermeable and insulated. The
cases of stress-free and non-slip horizontal boundaries are considered. The governing
equations are solved numerically using a finite element method. To study the linear
stability of the quiescent state and of the fully developed flows, a reliable numerical
technique is implemented on the basis of Galerkin and finite element methods. The
thresholds for finite-amplitude, oscillatory and monotonic convection instabilities are
determined explicitly in terms of the governing parameters. In the diffusive mode
(solute is stabilizing) it is demonstrated that overstability and subcritical convection
may set in at a Rayleigh number well below the threshold of monotonic instability,
when the thermal to solutal diffusivity ratio is greater than unity. In an infinite layer
with rigid boundaries, the wavelength at the onset of overstability was found to be a
function of the governing parameters. Analytical solutions, for finite-amplitude convection,
are derived on the basis of a weak nonlinear perturbation theory for general
cases and on the basis of the parallel flow approximation for a shallow enclosure
subject to Neumann boundary conditions. The stability of the parallel flow solution
is studied and the threshold for Hopf bifurcation is determined. For a relatively large
aspect ratio enclosure, the numerical solution indicates horizontally travelling waves
developing near the threshold of the oscillatory convection. Multiple confined steady
and unsteady states are found to coexist. Finally, note that all the numerical solutions
presented in this paper were found to be stable. |
---|---|
AbstractList | The onset of thermosolutal convection and finite-amplitude flows, due to vertical
gradients of heat and solute, in a horizontal rectangular enclosure are investigated
analytically and numerically. Dirichlet or Neumann boundary conditions for temperature
and solute concentration are applied to the two horizontal walls of the
enclosure, while the two vertical ones are assumed impermeable and insulated. The
cases of stress-free and non-slip horizontal boundaries are considered. The governing
equations are solved numerically using a finite element method. To study the linear
stability of the quiescent state and of the fully developed flows, a reliable numerical
technique is implemented on the basis of Galerkin and finite element methods. The
thresholds for finite-amplitude, oscillatory and monotonic convection instabilities are
determined explicitly in terms of the governing parameters. In the diffusive mode
(solute is stabilizing) it is demonstrated that overstability and subcritical convection
may set in at a Rayleigh number well below the threshold of monotonic instability,
when the thermal to solutal diffusivity ratio is greater than unity. In an infinite layer
with rigid boundaries, the wavelength at the onset of overstability was found to be a
function of the governing parameters. Analytical solutions, for finite-amplitude convection,
are derived on the basis of a weak nonlinear perturbation theory for general
cases and on the basis of the parallel flow approximation for a shallow enclosure
subject to Neumann boundary conditions. The stability of the parallel flow solution
is studied and the threshold for Hopf bifurcation is determined. For a relatively large
aspect ratio enclosure, the numerical solution indicates horizontally travelling waves
developing near the threshold of the oscillatory convection. Multiple confined steady
and unsteady states are found to coexist. Finally, note that all the numerical solutions
presented in this paper were found to be stable. The onset of thermosolutal convection and finite-amplitude flows, due to vertical gradients of heat and solute, in a horizontal rectangular enclosure are investigated analytically and numerically. Dirichlet or Neumann boundary conditions for temperature and solute concentration are applied to the two horizontal walls of the enclosure, while the two vertical ones are assumed impermeable and insulated. The cases of stress-free and non-slip horizontal boundaries are considered. The governing equations are solved numerically using a finite element method. To study the linear stability of the quiescent state and of the fully developed flows, a reliable numerical technique is implemented on the basis of Galerkin and finite element methods. The thresholds for finite-amplitude, oscillatory and monotonic convection instabilities are determined explicitly in terms of the governing parameters. In the diffusive mode (solute is stabilizing) it is demonstrated that overstability and subcritical convection may set in at a Rayleigh number well below the threshold of monotonic instability, when the thermal to solutal diffusivity ratio is greater than unity. In an infinite layer with rigid boundaries, the wavelength at the onset of overstability was found to be a function of the governing parameters. Analytical solutions, for finite-amplitude convection, are derived on the basis of a weak nonlinear perturbation theory for general cases and on the basis of the parallel flow approximation for a shallow enclosure subject to Neumann boundary conditions. The stability of the parallel flow solution is studied and the threshold for Hopf bifurcation is determined. For a relatively large aspect ratio enclosure, the numerical solution indicates horizontally travelling waves developing near the threshold of the oscillatory convection. Multiple confined steady and unsteady states are found to coexist. Finally, note that all the numerical solutions presented in this paper were found to be stable. [PUBLICATION ABSTRACT] |
Author | VASSEUR, P. HASNAOUI, M. MAMOU, M. |
Author_xml | – sequence: 1 givenname: M. surname: MAMOU fullname: MAMOU, M. organization: Institute for Aerospace Research, National Research Council, Ottawa, Ontario, K1A 0R6, Canada – sequence: 2 givenname: P. surname: VASSEUR fullname: VASSEUR, P. organization: Department of Mechanical Engineering, Ecole Polytechnique of Montreal, C.P. 6079, Succ. ‘Down-Town’ Montreal, Quebec, H3C 3A7, Canada – sequence: 3 givenname: M. surname: HASNAOUI fullname: HASNAOUI, M. organization: Physics Department, MFE Laboratory, Faculty of Sciences Semlalia, BP 2390, Marrakesh, Morocco |
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Keywords | Temperature distribution Convective instabilities Cellular convection Oscillatory instability Thermohaline convection Digital simulation Bifurcation Cavity flow Analytical solution Heat transfer Concentration distribution Double diffusion |
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Snippet | The onset of thermosolutal convection and finite-amplitude flows, due to vertical
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SubjectTerms | Boundaries Boundary conditions Convection Convection and heat transfer Exact sciences and technology Fluid dynamics Fundamental areas of phenomenology (including applications) Physics Stability analysis Turbulent flows, convection, and heat transfer |
Title | On numerical stability analysis of double-diffusive convection in confined enclosures |
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