Rayleigh–Bénard convection in tall rectangular enclosures

Natural convection in air-filled, 2-D rectangular enclosures heated from below and cooled from above is studied numerically under the assumption of adiabatic sidewalls. A computational model based on the SIMPLE-C algorithm is used for solving the mass, momentum, and energy transfer governing equations. Simulations are performed for different values of the height-to-width aspect ratio of the enclosure in the range 2⩽A⩽6, by progressively increasing and successively decreasing the Rayleigh number in the range 103⩽Ra⩽2×106. After the departure from motionless conduction takes place, the following flow-pattern evolution is detected: one-cell steady → two-cell steady → two-cell periodic → one-to-three-cell periodic → three-cell periodic. At each bifurcation, either abrupt or smooth changes in the Nusselt number are found to occur, according to whether the flow-transition is either sudden or more gradual. Hysteresis phenomena occurrence is documented. The effects of tilting the enclosure upon the stability of the different flow structures are also analysed.

[1]  Robert B. Kinney,et al.  Time‐dependent natural convection in a square cavity: Application of a new finite volume method , 1990 .

[2]  Orhan Aydm Transient natural convection in rectangular enclosures heated from one side and cooled from above , 1999 .

[3]  Alexander Yu. Gelfgat,et al.  Different Modes of Rayleigh–Bénard Instability in Two- and Three-Dimensional Rectangular Enclosures , 1999 .

[4]  Francesc Giralt,et al.  Natural convection in a cubical cavity heated from below at low rayleigh numbers , 1996 .

[5]  Francesc Giralt,et al.  Flow transitions in laminar Rayleigh–Bénard convection in a cubical cavity at moderate Rayleigh numbers , 1999 .

[6]  E. Koschmieder,et al.  Bénard cells and Taylor vortices , 1993 .

[7]  Kwang-Tzu Yang,et al.  Rayleigh-Bénard Convection in a Small Aspect Ratio Enclosure: Part I—Bifurcation to Oscillatory Convection , 1993 .

[8]  Suhas V. Patankar,et al.  Recent Developments in Computational Heat Transfer , 1988 .

[9]  Kwang-Tzu Yang,et al.  Transitions and Bifurcations in Laminar Buoyant Flows in Confined Enclosures , 1988 .

[10]  Kwang-Tzu Yang,et al.  Rayleigh-Bénard Convection in a Small Aspect Ratio Enclosure: Part II—Bifurcation to Chaos , 1993 .

[11]  J. P. V. Doormaal,et al.  ENHANCEMENTS OF THE SIMPLE METHOD FOR PREDICTING INCOMPRESSIBLE FLUID FLOWS , 1984 .

[12]  M. Hortmann,et al.  Finite volume multigrid prediction of laminar natural convection: Bench-mark solutions , 1990 .

[13]  W. Rohsenow,et al.  Handbook of Heat Transfer Fundamentals , 1985 .

[14]  R. L. Frederick,et al.  Spatial and thermal features of three dimensional Rayleigh-Bénard convection , 1994 .

[15]  Edward A. Spiegel,et al.  Rayleigh‐Bénard Convection: Structures and Dynamics , 1998 .

[16]  J. P. Hartnett,et al.  Handbook of Heat Transfer Fundamentals (Second Edition) , 1986 .

[17]  J. Gollub,et al.  Many routes to turbulent convection , 1980, Journal of Fluid Mechanics.

[18]  Kwang-Tzu Yang,et al.  Thermal convection in small enclosures: an atypical bifurcation sequence , 1995 .

[19]  S. Patankar Numerical Heat Transfer and Fluid Flow , 2018, Lecture Notes in Mechanical Engineering.

[20]  S. Fauve,et al.  Period doubling cascade in mercury, a quantitative measurement , 1982 .

[21]  D. Spalding,et al.  A calculation procedure for heat, mass and momentum transfer in three-dimensional parabolic flows , 1972 .

[22]  G. D. Davis Natural convection of air in a square cavity: A bench mark numerical solution , 1983 .