4.4 Article

A numerical analysis on the heat transfer of jet impingement with nanofluid on a concave surface covered with metal porous block

期刊

HEAT AND MASS TRANSFER
卷 56, 期 11, 页码 3071-3083

出版社

SPRINGER
DOI: 10.1007/s00231-020-02902-0

关键词

Numerical analysis; Jet impingement; Concave surface; Metal porous layer; Silica-water nanofluid

资金

  1. Natural Science Foundation of Shanghai, China [19ZR1422400]

向作者/读者索取更多资源

In this paper, combining the bilayer porous metal block of copper (BPMBC) on the concave heating surface and jet impingement of SiO2-H2O nanofluid is utilized in the flow channel. The k-epsilon turbulent model coupled with Brinkman Forchheimer extended Darcy equations are employed to analyze the effects of the SiO2-H2O nanofluid concentration, porosity in the porous monolayer on concave surface, thickness ratio between the upper and lower porous layer in the bilayer porous metal block as well as the curvature of concave surface on the heat transfer. In comparison with pure water as working fluid, the 5.85% rise of average heat transfer coefficient (HTC) can be obtained while the 3.0% SiO2-H2O nanofluid is utilized in the mode. The combining effects of the porosity in the monolayer porous layer and the curvature of concave surface on the heat transfer are related to the heating surface area and convection between the jet nanofluid and heating surface. More heat transfer occurs in the bilayer porous metal block with a larger porosity in the upper layer and a lower porosity in the bottom layer due to the dominant effects of the convection and thermal conductivity respectively in the different porous layers. The effects of the thickness ratio between the upper and lower layer in the bilayer porous metal block on the heat transfer are related to the influencing portion between the surface area and convection. With an increase in the curvature of concave surface from R/L(ratio of concave radius to chordal length) =0.5 to R/L = 1.1, the average Nusselt numbers go up, and their rise rates decrease by the Reynolds number gradually, but the surface area decreases, which causes the average temperature rise of copper block. Besides, the higher average temperature occurs in the mode with a flat plate than that with a concave surface.

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