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Secondary instabilities of convection in a shallow cavity

Published online by Cambridge University Press:  26 April 2006

Tzyy-Ming Wang
Affiliation:
Department of Mechanical Engineering, The Ohio State University, 206 West 18th Avenue, Columbus, OH 43210, USA
Seppo A. Korpela
Affiliation:
Department of Mechanical Engineering, The Ohio State University, 206 West 18th Avenue, Columbus, OH 43210, USA

Abstract

Analysis of secondary instabilities of natural convection in a shallow cavity heated from a side has been carried out. For mercury with Prandtl number equal to 0.027 analysis of the primary instabilities by linear theory shows that an instability sets in as transverse cells at Grashof number equal to 9157.6. Instability resulting in oscillatory longitudinal rolls is also possible, their critical Grashof number being equal to 10608.4. The secondary instabilities of the equilibrium states of transverse cells for mercury have been determined. The results show roughly that stable transverse cells with wavelength shorter than the critical become unstable by subharmonic resonance, but the instability for longer cells sets in by a combination resonance. The instability as longitudinal oscillatory rolls reappears at larger values of Grashof number, although slightly delayed by the presence of the transverse cells.

Type
Research Article
Copyright
© 1992 Cambridge University Press

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References

Benjamin, T. B. & Feir, J. E. 1967 The disintegration of wave trains on deep water. Part 1. Theory. J. Fluid Mech. 27, 417430.Google Scholar
Chait, A. & Korpela, S. A. 1989 The secondary flow and its stability for natural convection in a tall vertical enclosure. J. Fluid Mech. 200, 189216.Google Scholar
Clever, R. M. & Busse, F. H. 1974 Transition to time-dependent convection. J. Fluid Mech. 65, 625645.Google Scholar
Drummond, J. E. & Korpela, S. A. 1987 Multicellular natural convection in a shallow cavity. J. Fluid Mech. 148, 245266.Google Scholar
Eckhaus, W. 1965 Studies in Non-linear Stability Theory. Springer.
Gershuni, G. Z., Zhukhovitskii, E. M. & Myznikov, V. M. 1974 Stability of plane-parallel convective fluid flow in a horizontal layer relative to spatial oscillations. J. Appl. Mech. Tech. Phys. 5, 706708.Google Scholar
Gill, A. E. 1974 A theory of thermal oscillations in liquid metals. J. Fluid Mech. 64, 577588.Google Scholar
Hart, J. E. 1972 Stability of thin non-rotating Hadley circulations. J. Atmos. Sci. 29, 687697.Google Scholar
Hart, J. E. 1983 A note on the stability of low-Prandtl-number Hadley circulations. J. Fluid Mech. 132, 271281.Google Scholar
Herbert, Th. 1983 Secondary instability of plane channel flow to subharmonic three-dimensional disturbances. Phys. Fluids 26, 871874.Google Scholar
Herbert, Th. 1988 Secondary instability of boundary layers. Ann. Rev. Fluid Mech. 20, 487526.Google Scholar
Hung, M. C. 1989 Transitions in convection of a low Prandtl number fluid Driven by a horizontal temperature gradient. Ph.D. thesis, The Ohio State University.
Hung, M. C. & Andereck, C. D. 1988 Transitions in convection driven by a horizontal temperature gradient. Phys. Lett. A 132, 253258.Google Scholar
Hurle, D. T. J. 1966 Temperature oscillations in molten metals and their relationship to growth striae in melt-grown crystals. Phil. Mag. 13, 305310.Google Scholar
Hurle, D. T. J., Jakeman, E. & Johnson, C. P. 1974 Convective temperature oscillations in molten gallium. J. Fluid Mech. 64, 565576.Google Scholar
Kelly, R. E. 1967 On the stability of an inviscid shear layer which is periodic in space and time. J. Fluid Mech. 27, 657689.Google Scholar
Klaassen, G. P. & Peltier, W. R. 1989 The role of transverse secondary instabilities in the evolution of free shear layers. J. Fluid Mech. 202, 367402.Google Scholar
Kuo, H. P. & Korpela, S. A. 1988 Stability and finite amplitude natural convection in a shallow cavity with insulated top and bottom and heated from a side. Phys. Fluids 31, 3342.Google Scholar
Kuo, H. P., Korpela, S. A., Chait, A. & Marcus, P. S. 1986 Stability of natural convection in a shallow cavity. In Eight Intl Heat Transfer Conf. San Francisco, vol. 4. pp. 15441544. Hemisphere.
Laure, P. 1987 Etude des mouvements de convection dans une cavité rectangulaire soumise à un gradient de température horizontal. J. Méc. Théor. Appl. 6, 351382.Google Scholar
Marcus, P. S. 1984 Simulation of Taylor-Couette flow. Part 1. Numerical methods and comparison with experiments. J. Fluid Mech. 146, 4564.Google Scholar
Maseev, L. M. 1968 Occurrence of three-dimensional perturbations in a boundary layer. Fluid Dyn. 3, 2324.Google Scholar
Nagata, M. & Busse, F. H. 1983 Three-dimensional tertiary motions in a plane shear layer. J. Fluid Mech. 135, 126.Google Scholar
Pierrehumbert, R. T. & Widnall, S. E. 1982 Secondary instability of wall bounded shear flows. J. Fluid Mech. 114, 347385.Google Scholar
Roux, B., Bontoux, P. & Henry, D. 1984 Numerical and theoretical study of different flow regimes occurring in horizontal fluid layers differentially heated. Lecture Notes in Physics, vol. 230, pp. 134134. Springer.
Stuart, J. T. & DiPrima, R. C. 1978 The Eckhaus and Benjamin-Feir resonance mechanisms. Proc. R. Soc. Lond. A 362, 2741.Google Scholar
Wang, T. M. 1990 Secondary stability and three dimensional natural convection in a shallow cavity, Ph.D. thesis, The Ohio State University.
Wang, T. M. & Korpela, S. A. 1989 Convection rolls in a shallow cavity heated from a side. Phys. Fluids A 1, 947953.Google Scholar