A Mathematical Theorem on the Onset of Stationary Convection in Couple-Stress Fluid

The thermal instability of a couple-stress fluid heated from below is investigated. Following the linearized stability theory and normal mode analysis, the paper mathematically establishes that the onset of instability at marginal state, cannot manifest itself as stationary convection, if the ther...

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Main Author: Banyal Ajaib Singh
Format: Article
Language:English
Published: Isfahan University of Technology 2013-01-01
Series:Journal of Applied Fluid Mechanics
Subjects:
Online Access:http://jafmonline.net/JournalArchive/download?file_ID=26995&issue_ID=212
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author Banyal Ajaib Singh
author_facet Banyal Ajaib Singh
author_sort Banyal Ajaib Singh
collection DOAJ
description The thermal instability of a couple-stress fluid heated from below is investigated. Following the linearized stability theory and normal mode analysis, the paper mathematically establishes that the onset of instability at marginal state, cannot manifest itself as stationary convection, if the thermal Rayleigh number R and the couple-stress parameter F, 3 satisfy the inequality   2  2 2  2  1  3 F  3 F  1  3 F  1    , and when the couple-stress parameter F is R  2 2 27 F  1  1  3 F    infinitesimally small, R    27 4 4  2    F  , the result which also clearly mathematically established the stabilizing 1  2     character of the couple-stress.
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spelling doaj.art-aaf813ce50274b63b113e39020ec17642022-12-21T23:34:41ZengIsfahan University of TechnologyJournal of Applied Fluid Mechanics1735-36452013-01-0162191196.A Mathematical Theorem on the Onset of Stationary Convection in Couple-Stress FluidBanyal Ajaib Singh0NSCBM, Govt. College Hamirpur (HP) India 177001The thermal instability of a couple-stress fluid heated from below is investigated. Following the linearized stability theory and normal mode analysis, the paper mathematically establishes that the onset of instability at marginal state, cannot manifest itself as stationary convection, if the thermal Rayleigh number R and the couple-stress parameter F, 3 satisfy the inequality   2  2 2  2  1  3 F  3 F  1  3 F  1    , and when the couple-stress parameter F is R  2 2 27 F  1  1  3 F    infinitesimally small, R    27 4 4  2    F  , the result which also clearly mathematically established the stabilizing 1  2     character of the couple-stress.http://jafmonline.net/JournalArchive/download?file_ID=26995&issue_ID=212Thermal convection; Couple-stress fluid; Rayleigh number.
spellingShingle Banyal Ajaib Singh
A Mathematical Theorem on the Onset of Stationary Convection in Couple-Stress Fluid
Journal of Applied Fluid Mechanics
Thermal convection; Couple-stress fluid; Rayleigh number.
title A Mathematical Theorem on the Onset of Stationary Convection in Couple-Stress Fluid
title_full A Mathematical Theorem on the Onset of Stationary Convection in Couple-Stress Fluid
title_fullStr A Mathematical Theorem on the Onset of Stationary Convection in Couple-Stress Fluid
title_full_unstemmed A Mathematical Theorem on the Onset of Stationary Convection in Couple-Stress Fluid
title_short A Mathematical Theorem on the Onset of Stationary Convection in Couple-Stress Fluid
title_sort mathematical theorem on the onset of stationary convection in couple stress fluid
topic Thermal convection; Couple-stress fluid; Rayleigh number.
url http://jafmonline.net/JournalArchive/download?file_ID=26995&issue_ID=212
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