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Rayleigh-Bénard convection in an intermediate-aspect-ratio rectangular container

Published online by Cambridge University Press:  21 April 2006

Paul Kolodner
Affiliation:
AT&T Bell Laboratories, Murray Hill, New Jersey 07974
R. W. Walden
Affiliation:
AT&T Bell Laboratories, Murray Hill, New Jersey 07974
A. Passner
Affiliation:
AT&T Bell Laboratories, Murray Hill, New Jersey 07974
C. M. Surko
Affiliation:
AT&T Bell Laboratories, Murray Hill, New Jersey 07974

Abstract

We report a study of the flow patterns associated with Rayleigh—Bénard convection in rectangular containers of approximate proportions 10 × 5 × 1 at Prandtl numbers σ between 2 and 20. The flow is studied at Rayleigh numbers ranging from the onset of convective flow to the onset of time dependence; Nusselt-number measurements are also presented. The results are discussed in the content of the theory for the stability of a laterally infinite system of parallel rolls. We observed transitions between time-independent flow patterns which depend on roll wavenumber, Rayleigh number and Prandtl number in a manner that is reasonably well described by this theory. For σ [lsim ] 10, the skewed-varicose instability (which leads directly to time dependence in much larger containers) is found to initiate transitions between time-independent patterns. We are then able to study the approach to time dependence in a regime of larger Rayleigh number where the instabilities in the flow are found to have an intrinsic time dependence. In this regime, the onset of time dependence appears to be explained by the recent predictions of Bolton, Busse & Clever for a new set of time-dependent instabilities.

Type
Research Article
Copyright
© 1986 Cambridge University Press

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References

Ahlers, G. 1980 Effect of departures from the Oberbeck—Boussinesq approximation on the heat transport of horizontal convecting fluid layers. J. Fluid Mech. 98, 137148.Google Scholar
Behringer, R. P., Gao, H. & Shaumeyer, J. N. 1983 Time dependence in Rayleigh—BeAnard convection with a variable cylindrical geometry. Phys. Rev. Lett. 50, 11991202.Google Scholar
BergeA, P. 1981 Rayleigh—BeAnard convection in high Prandtl number fluids. In Chaos and Order in Nature (ed. H. Haken), pp. 1424. Springer.
Bolton, E. W., Busse, F. H. & Clever, R. M. 1983 An antisymmetric oscillatory instability of convection rolls. Bull. Am. Phys. Soc. 28, 1399.Google Scholar
Busse, F. H. 1967a The stability of finite amplitude cellular convection and its relation to an extremum principle. J. Fluid Mech. 30, 625649.Google Scholar
Busse, F. H. 1967b On the stability of two-dimensional convection in a layer heated from below. J. Maths & Phys. 46, 140149.Google Scholar
Busse, F. H. 1978 Non-linear properties of thermal convection. Rep. Prog. Phys. 41, 19291967.Google Scholar
Busse, F. H. 1981 Transition to turbulence in Rayleigh—BeAnard convection. In Hydrodynamic Instabilities and the Transition to Turbulence (eds. H. L. Swinney & J. P. Gollub), pp. 97137. Springer.
Busse, F. H. & Clever, R. M. 1979 Instabilities of convection rolls in a fluid of moderate Prandtl number. J. Fluid Mech. 91, 319335.Google Scholar
Busse, F. H. & Whitehead, J. A. 1971 Instabilities of convection rolls in a high Prandtl number fluid. J. Fluid Mech. 47, 305320.Google Scholar
Busse, F. H. & Whitehead, J. A. 1974 Oscillatory and collective instabilities in large Prandtl number convection. J. Fluid Mech. 66, 6779.Google Scholar
Chen, M. M. & Whitehead, J. A. 1968 Evolution of two-dimensional periodic Rayleigh—BeAnard convection cells of arbitrary wave numbers. J. Fluid Mech. 31, 115.Google Scholar
Clever, R. M. & Busse, F. H. 1974 Transition to time-dependent convection. J. Fluid Mech. 65, 625645.Google Scholar
Dubois, M. & BergeA, P. 1980 Experimental evidence for the oscillators in a convective biperiodic regime. Phys. Lett. 76 A, 53–56.Google Scholar
Gao, H. & Behringer, R. P. 1984 Onset of convective time dependence in cylindrical containers. Phys. Rev. A 30, 28372839.Google Scholar
Gollub, J. P. & Benson, S. V. 1980 Many routes to turbulent convection. J. Fluid Mech. 100, 449470.Google Scholar
Gollub, J. P. & McCarriar, A. R. 1982 Convection patterns in Fourier space. Phys. Rev. A 26, 34703476.Google Scholar
Gollub, J. P., McCarriar, A. R. & Steinman, J. F. 1982 Convective pattern evolution and secondary instabilities. J. Fluid Mech. 125, 259281.Google Scholar
Greenside, H. S. & Coughran, W. M. 1984 Nonlinear pattern formation near the onset of Rayleigh—BeAnard convection. Phys. Rev. A 30, 398428.Google Scholar
Matjrer, J. & Libchaber, A. 1980 Effect of the Prandtl number on the onset of turbulence in liquid 4-He. J. Physique Lett. 41, L515L518.Google Scholar
Mueller, K. H., Ahlers, G. & Pobell, F. 1976 Thermal expansion coefficient, scaling, and universality near the superfluid transition of 4-He. Phys. Rev. B 14, 20962118.Google Scholar
Pomeau, Y. & Zaleski, S. 1981 Wavelength selection in one-dimensional cellular structures. J. Physique 42, 516528.Google Scholar
Walden, R. W. 1983 Some new routes to chaos in Rayleigh-BeAnard convection. Phys. Rev. A 27, 12551258.Google Scholar
Walden, R. W. & Ahlers, G. 1981 Non-Boussinesq and penetrative convection in a cylindrical cell. J. Fluid Mech. 109, 89114.Google Scholar
Walden, R. W., Kolodner, P., Passner, A. & Surko, C. M. 1984 Nonchaotic Rayleigh—BeAnard convection with four and five incommensurate frequencies. Phys. Rev. Lett. 53, 242245.Google Scholar
Whitehead, J. A. & Chan, G. L. 1976 Stability of Rayleigh-BeAnard convection rolls and bimodal flow at moderate Prandtl numbers. Dyn. Atmos. Oceans 1, 3349.Google Scholar