Numerical modeling of multiple steady-state convective modes in a tilted porous medium heated from below

被引:16
作者
Guerrero-Martinez, Fernando J. [1 ,4 ]
Karimi, Nader [1 ,2 ]
Ramos, Eduardo [3 ]
机构
[1] Univ Glasgow, Sch Engn, Glasgow G12 8QQ, Lanark, Scotland
[2] Univ Missouri, Sch Comp & Engn, Civil & Mech Engn Dept, Kansas City, MO 64110 USA
[3] Univ Nacl Autonoma Mexico, Renewable Energy Inst, Temixco 62580, Mor, Mexico
[4] Univ Nacl Autonoma Mexico, Inst Geophys, Mexico City 04510, DF, Mexico
基金
英国工程与自然科学研究理事会;
关键词
2D numerical modeling; Porous medium; Free convection; Boussinesq approximation; NATURAL-CONVECTION; ENTROPY GENERATION; SQUARE CAVITY; FLUID;
D O I
10.1016/j.icheatmasstransfer.2018.02.009
中图分类号
O414.1 [热力学];
学科分类号
摘要
Numerical simulations are carried out to determine the steady-state convective modes in a rectangular porous cavity heated from below. The property of multiplicity of solutions for a given set of governing parameters is examined in this paper. The multiple steady-state solutions that appear in a horizontal cavity for a given Rayleigh number are obtained by means of suitable initial conditions. Each of these solutions is then perturbed by increasing the inclination angle in order to identify the transition angle to a different convective mode. It is observed that for an odd-number of convective cells, if the counterclockwise rotating cells dominate the configuration, the Nusselt number increases with the slope angle up to a maximum and then decreases before the transition to single cell convection. Otherwise, if there are more clockwise rotating cells, the Nusselt number decreases monotonically and the configuration becomes unstable. Since multicellular configurations with even number of convective cells have equal number of clockwise and counterclockwise rotating cells, this case presents a single behavior characterized by a decrease in the Nusselt number. The transition angles from multi cellular to single cell convection are found to be as large as 45 degrees when the aspect ratio of the cavity is large, so that this angle is the upper limit to destabilize multicellular convection.
引用
收藏
页码:64 / 72
页数:9
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