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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Series: | International Journal of Mathematics and Mathematical Sciences |
Online Access: | http://dx.doi.org/10.1155/S0161171201004811 |
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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 |
work_keys_str_mv |
AT dnriahi finiteamplitudethermalconvectionwithvariablegravity AT albertthsui finiteamplitudethermalconvectionwithvariablegravity |
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1725303557673975808 |