Obstacle's effects and their location inside the square cavity on the thermal performance of Cu-Al2O3/H2O hybrid nanofluid

被引:2
|
作者
Hachichi, Farid [1 ]
Belghar, Nourredine [1 ]
Kamel, Chadi [1 ]
Saleh, Momen S. M. [2 ,6 ]
Kadja, Mahfoud [3 ]
Lachi, Mohammed [4 ]
Chamkha, Ali J. [5 ]
机构
[1] Univ Mohamed Khider Biskra, Dept Mech Engn, Lab Mat & Energy Engn, Biskra, Algeria
[2] Univ Tiaret, Dept Mech Engn, Res Lab Ind Technol, Tiaret, Algeria
[3] Univ Freres Mentouri, Dept Mech Engn, Lab Appl Energet & Pollut, Constantine, Algeria
[4] Univ Reims, Dept Mech Engn, MATIM, Reims, France
[5] Kuwait Coll Sci & Technol, Fac Engn, Doha, Kuwait
[6] Univ Tiaret, Res Lab Ind Technol, Tiaret 14000, Algeria
关键词
hybrid nanofluid; obstacle; Rayleigh number; square cavity; thermal performance; MHD MIXED CONVECTION; CU-WATER NANOFLUID; LID-DRIVEN CAVITY; NATURAL-CONVECTION; HEAT SOURCE/SINK; NUMERICAL-SIMULATION; ENCLOSURE; FLOW; LAYER; CYLINDER;
D O I
10.1002/htj.22834
中图分类号
O414.1 [热力学];
学科分类号
摘要
The current study focuses on the effect of obstacles and their positioning within the square cavity (L = H) on heat exchange. This work considers heating the cavity's bottom wall to a steady, high temperature. The top wall of the cavity is adiabatic, while the two vertical side walls are cooled. Four cases are explored under these conditions: the first case is a square-shaped cavity holding a square-shaped obstacle h = l = 0,15 L, while the other three cases, respectively, each include two, three, and four square obstacles. The cavity was filled with Cu-Al2O3/H2O hybrid nanofluid with a volume fraction phi = 0.03. Numerical results for laminar and stationary flow regimes with Rayleigh numbers 10(4) <= Ra <= 10(6). The finite volume approach solves the governing equations numerically. The findings show that the number of square obstacles within the square-shaped cavity significantly impacts heat exchange and hybrid nanofluid flow. The second example, with two square obstacles, improves heat exchange more than other cases with one to four barriers. In the second example, the obstacle location at the plane Y = 0.25H is suitable and helps boost heat transmission of the hybrid nanofluid. The ideal obstacle position in the fourth scenario, which has four square barriers, is at the plane Y = 0.75H.
引用
收藏
页码:3411 / 3430
页数:20
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