Hostname: page-component-cd9895bd7-gxg78 Total loading time: 0 Render date: 2024-12-18T19:02:38.907Z Has data issue: false hasContentIssue false

Nonlinear interactions between convection, rotation and flows with vertical shear

Published online by Cambridge University Press:  21 April 2006

David H. Hathaway
Affiliation:
Space Science Laboratory, NASA/Marshall Space Flight Center, Huntsville, AL 35812
Richard C. J. Somerville
Affiliation:
Scripps Institution of Oceanography, University of California, San Diego, La Jolla, CA 92093

Abstract

A three-dimensional and time-dependent numerical model is used to study the nonlinear interactions between thermal convective motions, rotation, and imposed flows with vertical shear. All cases have Rayleigh numbers of 104 and Prandtl numbers of 1.0. Rotating cases have Taylor numbers of 104.

For the non-rotating cases, the effects of the shear on the convection produce longitudinal rolls aligned with the shear flow and a downgradient flux of momentum. The interaction between the convection and the shear flow decreases the shear in the interior of the fluid layer while adding kinetic energy to the convective motions. For unit Prandtl number the dimensionless flux of momentum is equal to the dimensionless flux of heat.

For rotating cases with vertical rotation vectors, the shear flow favours rolls aligned with the shear and produces a downgradient flux of momentum. However, the Coriolis force turns the flow induced by the convection to produce a more complicated shear that changes direction with height. As in the non-rotating cases, the convective motions become more energetic by extracting energy from the mean flow. For Richardson numbers larger than about − 1.0, the dominant source of eddy kinetic energy is the shear flow rather than buoyancy.

For rotating cases with tilted rotation vectors the results depend upon the direction of the shear. For weak shear, convective rolls aligned with the rotation vector are favoured. When the shear flow is directed to the east along the top, the rolls become broader and the convection weaker. For large shear in this direction, the convective motions are quenched by the competition between the shear flow and the tilted rotation vector. When the shear flow is directed to the west along the top, strong shear produces rolls aligned with the shear. The heat and momentum fluxes become large and can exceed those found in the absence of a tilted rotation vector. Countergradient fluxes of momentum can also be produced.

Type
Research Article
Copyright
© 1986 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

Agee, E. M. 1984 Observations from space and thermal convection: a historical perspective. Bull. Am. Met. Soc. 65, 938949.Google Scholar
Brunt, D. 1951 Experimental cloud formation. Compendium of Meteorology, pp. 1255–1262. Boston: American Meteorological Society.
Busse, F. H. 1982 Thermal convection in rotating systems. Proc. 9th US Nat. Cong. Appl. Mech., Am. Soc. Mech. Eng. pp. 299–305.Google Scholar
Busse, F. H. 1983 Generation of mean flows by thermal convection. Physica 9D, 287299.Google Scholar
Chandrasekhar, S. 1961 Hydrodynamic and Hydromagnetic Stability. Clarendon.
Clever, R. M. & Busse, F. H. 1977 Instabilities of longitudinal convection rolls in an inclined layer. J. Fluid Mech. 81, 107127.Google Scholar
Clever, R. M., Busse, F. H. & Kelly, R. E. 1977 Instabilities of longitudinal convection rolls in Couette flow. Z. angew. Math. Phys. 28, 771783.Google Scholar
Deardorff, J. W. 1965 Gravitational instability between horizontal plates with shear. Phys. Fluids 8, 10271030.Google Scholar
Flasar, F. M. & Gierasch, P. J. 1978 Turbulent convection within rapidly rotating superdiabatic fluids with horizontal temperature gradients. Geophys. Astrophys. Fluid Dyn. 10, 175212.Google Scholar
Hart, J. E. 1971 Transition to a wavy vortex regime in convective flow between inclined plates. J. Fluid Mech. 48, 265271.Google Scholar
Hathaway, D. H. & Somerville, R. C. J. 1983 Three-dimensional simulations of convection in layers with tilted rotation vectors. J. Fluid Mech. 126, 7589.Google Scholar
Hathaway, D. H., Toomre, J. & Gilman, P. A. 1980 Convective instability when the temperature gradient and rotation vector are oblique to gravity. II. Real fluids with effects of diffusion. Geophys. Astrophys. Fluid Dyn. 15, 737.Google Scholar
Ingersoll, A. P. 1966 Convective instabilities in plane Couette flow. Phys. Fluids 9, 682689.Google Scholar
Kuettner, J. P. 1971 Cloud bands in the Earth's atmosphere: observations and theory. Tellus 23, 404425.Google Scholar
Kuo, H. L. 1963 Perturbations of plane Couette flow in stratified fluid and the origin of cloud streets. Phys. Fluids 6, 195211.Google Scholar
LeMone, M. A. 1973 The structure and dynamics of horizontal roll vortices in the planetary boundary layer. J. Atmos. Sci. 30, 10771091.Google Scholar
Lemone, M. A. 1983 Momentum transport by a line of cumulonimbus. J. Atmos. Sci. 40, 18151834.Google Scholar
Lipps, F. B. 1971 Two-dimensional numerical experiments in thermal convection with vertical shear. J. Atmos. Sci. 28, 319.Google Scholar
Somerville, R. C. J. 1971 Benard convection in a rotating fluid. Geophys. Fluid Dyn. 2, 247262.Google Scholar
Somerville, R. C. J. & Gal-Chen, T. 1979 Numerical simulations of convection with mean vertical motion. J. Atmoa. Sci. 36, 805815.Google Scholar
Somerville, R. C. J. & Lipps, F. B. 1973 A numerical study in three space dimensions of Bénard convection in a rotating fluid. J. Atmos. Sci. 30, 590596.Google Scholar
Veronis, G. 1959 Cellular convection with finite amplitude in a rotating fluid. J. Fluid Mech. 5, 401435.Google Scholar
Weiss, N. O. 1964 Convection in the presence of constraints. Phil. Trans. R. Soc. Lond. A 256, 99147.Google Scholar