Finite amplitude thermal convection with variable gravity

Finite amplitude thermal convection is studied in a horizontal layer of infinite Prandtl number fluid with a variable gravity. For the present study, gravity is restricted to vary quadratically with respect to the vertical variable. A perturbation technique based on a small parameter, which is a mea...

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Main Authors: D. N. Riahi, Albert T. Hsui
Format: Article
Language:English
Published: Hindawi Limited 2001-01-01
Series:International Journal of Mathematics and Mathematical Sciences
Online Access:http://dx.doi.org/10.1155/S0161171201004811
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spelling doaj-647157da591d484b98d11f24992cca772020-11-25T00:36:55ZengHindawi LimitedInternational Journal of Mathematics and Mathematical Sciences0161-17121687-04252001-01-0125315316510.1155/S0161171201004811Finite amplitude thermal convection with variable gravityD. N. Riahi0Albert T. Hsui1Department of Theoretical and Applied Mechanics, 216 Talbot Laboratory, 104 S. Wright Street, University of Illinois at Urbana-Champaign, Urbana 61801, IL, USADepartment of Geology, 245 Natural History Building, 1301 W. Green St., University of Illinois at Urbana-Champaign, Urbana 61801, IL, USAFinite amplitude thermal convection is studied in a horizontal layer of infinite Prandtl number fluid with a variable gravity. For the present study, gravity is restricted to vary quadratically with respect to the vertical variable. A perturbation technique based on a small parameter, which is a measure of the ratio of the vertical to horizontal dimensions of the convective cells, is employed to determine the finite amplitude steady solutions. These solutions are represented in terms of convective modes whose amplitudes can be either small or of order unity. Stability of these solutions is investigated with respect to three dimensional disturbances. A variable gravity function introduces two non-dimensional parameters. For certain range of values of these two parameters, double or triple cellular structure in the vertical direction can be realized. Hexagonal patterns are preferred for sufficiently small amplitude of convection, while square patterns can become dominant for larger values of the convective amplitude. Variable gravity can also affect significantly the wavelength of the cellular pattern and the onset condition of the convective motion.http://dx.doi.org/10.1155/S0161171201004811
collection DOAJ
language English
format Article
sources DOAJ
author D. N. Riahi
Albert T. Hsui
spellingShingle D. N. Riahi
Albert T. Hsui
Finite amplitude thermal convection with variable gravity
International Journal of Mathematics and Mathematical Sciences
author_facet D. N. Riahi
Albert T. Hsui
author_sort D. N. Riahi
title Finite amplitude thermal convection with variable gravity
title_short Finite amplitude thermal convection with variable gravity
title_full Finite amplitude thermal convection with variable gravity
title_fullStr Finite amplitude thermal convection with variable gravity
title_full_unstemmed Finite amplitude thermal convection with variable gravity
title_sort finite amplitude thermal convection with variable gravity
publisher Hindawi Limited
series International Journal of Mathematics and Mathematical Sciences
issn 0161-1712
1687-0425
publishDate 2001-01-01
description Finite amplitude thermal convection is studied in a horizontal layer of infinite Prandtl number fluid with a variable gravity. For the present study, gravity is restricted to vary quadratically with respect to the vertical variable. A perturbation technique based on a small parameter, which is a measure of the ratio of the vertical to horizontal dimensions of the convective cells, is employed to determine the finite amplitude steady solutions. These solutions are represented in terms of convective modes whose amplitudes can be either small or of order unity. Stability of these solutions is investigated with respect to three dimensional disturbances. A variable gravity function introduces two non-dimensional parameters. For certain range of values of these two parameters, double or triple cellular structure in the vertical direction can be realized. Hexagonal patterns are preferred for sufficiently small amplitude of convection, while square patterns can become dominant for larger values of the convective amplitude. Variable gravity can also affect significantly the wavelength of the cellular pattern and the onset condition of the convective motion.
url http://dx.doi.org/10.1155/S0161171201004811
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