Affiliation:
1. Department of Mechanical Engineering, University of Minnesota, Minneapolis, MN 55455
Abstract
The onset and development of flow in a thick horizontal layer subject to a near-constant flux heating from below has been studied experimentally. The overall heat-flux-based Rayleigh number, Ra*, ranges from 2 × 108 to 7 × 1010. Flow visualization shows the growth and breakdown of a conduction layer adjacent to the heated surface. Convection is characterized by the release of warm meandering plumes and thermals from a boundary layer. The planform of convection at the heated surface begins with a pattern of small spots suggestive of Be´nard cells. Some of these cells expand, forming a larger cell pattern. This continues until a quasi-steady state is reached in which the former cell boundaries form a slowly moving pattern of warm lines on the heated surface. The lines are believed to be the source of the plumes and thermals. Quantitatively, the onset of convection occurs at a constant (critical) Rayleigh number based on the conduction layer thickness, Raδ. Based on the first observation of fluid motion, this critical Rayleigh number is approximately 1300. Based on the heated surface temperature the critical Rayleigh number is 2700. The nondimensional wavenumber associated with the observed instabilities at the onset of convection is about 2.2.
Subject
Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics,General Materials Science
Reference55 articles.
1. Ahlers
G.
, CrossM. C., HohenbergP. C., and SafranS., 1981, “The Amplitude Equation Near the Convective Threshold: Application to Time-Dependent Heating Experiments,” J. Fluid Mech., Vol. 110, pp. 297–334.
2. Asaeda
T.
, and WatanabeK., 1989, “The Mechanism of Heat Transport in Thermal Convection at High Rayleigh Numbers,” Phys. Fluids A, Vol. 1, pp. 861–867.
3. Be´nard, H., 1900, “Les Tourbillons cellulaires dans une nappe liquide,” Revue ge´ne´rale des Sciences pures et applique´s, Vol. 11, pp. 1261–1271, 1309–1328.
4. Berg
J. C.
, BoudartM., and AcrivosA., 1961, “Natural Convection in Pools of Evaporating Liquids,” J. Fluid Mech., Vol. 24, pp. 721–735.
5. Blair
L. M.
, and QuinnJ. A., 1969, “The Onset of Cellular Convection in a Fluid Layer With Time-Dependent Density Gradients,” J. Fluid Mech., Vol. 36, pp. 385–400.
Cited by
37 articles.
订阅此论文施引文献
订阅此论文施引文献,注册后可以免费订阅5篇论文的施引文献,订阅后可以查看论文全部施引文献