Natural convection in enclosures containing an insulation with a permeable fluid-porous interface

Abstract A numerical study was performed to analyze steady-state natural convective heat transfer in rectangular enclosures vertically divided into a fluid-filled region and a fluid saturated porous region. The interface between the two regions was permeable, allowing the fluid to flow from one region to the other. The vertical boundaries of the enclosures were isothermal and the horizontal boundaries were adiabatic. The flow in the porous region was modeled using the Brinkman-extended Darcy's law to account for no-slip at the walls and the interface. Numerical experiments were performed for different enclosure aspect ratios, Rayleigh numbers, Darcy numbers, thermal conductivity ratios and thicknesses of the porous region. The effects of the governing parameters on heat transfer were established. It was found that, when compared to the case where the fluid and porous regions were separated by an impermeable partition, heat transfer across the enclosure was higher. Also, for certain values of the governing parameters, heat transfer across the enclosure could be minimized by filling the enclosure partially with a porous material instead of filling it entirely.

[1]  C. L. Tien,et al.  Convection in a vertical slot filled with porous insulation , 1977 .

[2]  Claes Bankvall,et al.  Natural convective heat transfer in insulated structures , 1972 .

[3]  G. D. Raithby,et al.  HEAT TRANSFER BY NATURAL CONVECTION ACROSS VERTICAL AIR LAYERS , 1981 .

[4]  Adrian Bejan,et al.  On the boundary layer regime in a vertical enclosure filled with a porous medium , 1979 .

[5]  G. Pinder,et al.  Numerical solution of partial differential equations in science and engineering , 1982 .

[6]  J. W. Elder Numerical experiments with free convection in a vertical slot , 1966, Journal of Fluid Mechanics.

[7]  G. Neale,et al.  Practical significance of brinkman's extension of darcy's law: Coupled parallel flows within a channel and a bounding porous medium , 1974 .

[8]  P. Simpkins,et al.  Convection in a porous layer for a temperature dependent viscosity , 1981 .

[9]  E. Subramanian,et al.  A boundary-layer analysis for natural convection in vertical porous enclosures—use of the Brinkman-extended Darcy model , 1985 .

[10]  R. Pletcher,et al.  Computational Fluid Mechanics and Heat Transfer. By D. A ANDERSON, J. C. TANNEHILL and R. H. PLETCHER. Hemisphere, 1984. 599 pp. $39.95. , 1986, Journal of Fluid Mechanics.

[11]  J. O. Wilkes,et al.  The finite-difference computation of natural convection in a rectangular enclosure , 1966 .

[12]  George M. Homsy,et al.  Convection in a porous cavity , 1978, Journal of Fluid Mechanics.

[13]  Simon Ostrach,et al.  Natural convection in enclosures , 1988 .

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

[15]  F. W. Schmidt,et al.  Heat Transfer by Laminar Natural Convection Within Rectangular Enclosures , 1970 .

[16]  C. Tien,et al.  Numerical Study of High Rayleigh Number Convection in a Vertical Porous Enclosure , 1983 .

[17]  B. Chan,et al.  Natural convection in enclosed porous media with rectangular boundaries , 1970 .

[18]  E. Subramanian,et al.  Natural convection in rectangular enclosures partially filled with a porous medium , 1986 .

[19]  Ashley F. Emery,et al.  Free Convection Through Vertical Plane Layers—Moderate and High Prandtl Number Fluids , 1969 .

[20]  R. Viskanta,et al.  Natural Convection Flow and Heat Transfer Between a Fluid Layer and a Porous Layer Inside a Rectangular Enclosure , 1987 .