Finite amplitude convection with changing mean temperature. Part 1. Theory

Author:

Krishnamurti Ruby

Abstract

When a horizontal layer of fluid is heated from below and cooled from above with the mean temperature and physical parameters of the fluid constant, the two-dimensional roll is known to be the stable solution near the critical Rayleigh number. In this study, with the mean temperature changing steadily at a rate η, the Rayleigh number and the velocity and temperature fields governed by the Boussinesq equations are expanded in two parameters: η, and the amplitude ε. Hexagons are shown to be the stable solution near the critical Rayleigh number. The direction of the motion depends upon the sign of η. A finite amplitude instability is possible with an associated hysteresis in the heat flux as the critical Rayleigh number is approached from below or from above.

Publisher

Cambridge University Press (CUP)

Subject

Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics

Reference19 articles.

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2. Malkus, W. V. R. 1964 Course lectures, Summer Study Program in Geophysical Fluid Dynamics,Woods Hole Oceanographic Institution.

3. Chandrasekhar, S. 1961 Hydrodynamic and Hydromagnetic Stability .Oxford:Clarendon Press.

4. Krishnamurti, R. 1968 J. Fluid Mech. 33,457.

5. Debler, W. R. 1966 J. Fluid Mech. 24,165.

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