Hostname: page-component-cd9895bd7-p9bg8 Total loading time: 0 Render date: 2024-12-28T22:15:26.675Z Has data issue: false hasContentIssue false

Buoyancy-driven convection in cylindrical geometries

Published online by Cambridge University Press:  29 March 2006

S. F. Liang
Affiliation:
Department of Chemical Engineering, Stanford University, California Present address: Chicago Bridge and Iron, Plainfield, Illinois.
A. Vidal
Affiliation:
Department of Chemical Engineering, Stanford University, California
Andreas Acrivos
Affiliation:
Department of Chemical Engineering, Stanford University, California

Abstract

Numerical solutions to the Boussinesq equations containing a temperature-dependent viscosity are presented for the case of axisymmetric buoyancy-driven convective flow in a cylindrical cell. Two solutions, one with upflow and the other with downflow at the centre of the cell, were found for each set of boundary conditions that were considered. The existence of these two steady-state régimes was verified experimentally for the case of a cylindrical cell having rigid insulating lateral boundaries and isothermal top and bottom planes.

Using a perturbation expansion it is also shown that only one of these solutions remains stable in the subcritical régime. This, however, seems to be confined to a very narrow range of Rayleigh numbers, beyond which, according to all the evidence presently at hand, both solutions are equally stable for those values of the Rayleigh and Prandtl numbers for which axisymmetric motions occur.

Finally, certain fundamental differences between the problem considered here and that of thermal convection in a layer of infinite horizontal extent are briefly discussed.

Type
Research Article
Copyright
© 1969 Cambridge University Press

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

Busse, F. 1967 The stability of finite amplitude cellular convection and its relation to an extremum principle J. Fluid Mech. 30, 62549.Google Scholar
Graham, A. 1933 Shear patterns in an unstable layer of air Phil. Trans. A 232, 28596.Google Scholar
Hurle, D. T. J., Jakeman, E. & Pike, E. R. 1967 On the solution of the Bénard problem with boundaries of finite conductivity Proc. Roy. Soc. A 296, 46975.Google Scholar
Mitchell, W. T. & Quinn, J. A. 1966 Thermal convection in a completely confined fluid layer A.I.Ch.E. J. 12, 111624.Google Scholar
MÜLLER, U. 1965 Untersuchungen an rotationssymmetrischen Zellularkonvektionsströmungen II Beitr. Phys. Atm. 38, 922.Google Scholar
Palm, E. 1960 On the tendency towards hexagonal cells in steady convection J. Fluid Mech. 8, 18392.Google Scholar
Palm, E., Ellingsen, T. & Gjevik, B. 1967 On the occurrence of cellular motion in Bénard convection J. Fluid Mech. 30, 651661.Google Scholar
Palm, E. & ØIANN, H. 1964 Contribution to the theory of cellular thermal convection J. Fluid Mech. 19, 35365.Google Scholar
Pellew, A. & Southwell, R. V. 1940 On maintained convective motion in a fluid heated from below. Proc. Roy. Soc A 176, 31243.Google Scholar
Segel, L. A. 1965 The non-linear interaction of a finite number of disturbances to a layer of fluid heated from below J. Fluid Mech. 21, 35984.Google Scholar
Segel, L. A. & Stuart, J. T. 1962 On the question of the preferred mode in cellular thermal convection J. Fluid Mech. 13, 289306.Google Scholar
Sparrow, E. M., Goldstein, R. J. & Jonsson, V. K. 1964 Thermal instability in a horizontal fluid layer: effect of boundary conditions and non-linear temperature profile. J. Fluid Mech. 18, 51328.CrossRefGoogle Scholar
Tippelskirch, H. VON 1956 Über Konvektionszellen, insbesondere im flüssigen Schwefel Beitr. Phys. Atm. 29, 3754.Google Scholar