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Frontiers in Energy

ISSN 2095-1701

ISSN 2095-1698(Online)

CN 11-6017/TK

Postal Subscription Code 80-972

2018 Impact Factor: 1.701

Front Energ    2011, Vol. 5 Issue (1) : 75-82    https://doi.org/10.1007/s11708-010-0014-0
RESEARCH ARTICLE
Experimental study of the effects of structured surface geometry on water spray cooling performance in non-boiling regime
Minghou LIU(), Yaqing WANG, Dong LIU, Kan XU, Yiliang CHEN
Department of Thermal Science and Energy Engineering, University of Science and Technology of China, Hefei 230027, China
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Abstract

Experiments were conducted to study the effects of enhanced surfaces on heat transfer performance during water spray cooling in non-boiling regime. The surface enhancement is straight fin. The structures were machined on the top surface of heated copper blocks with a cross-sectional area of 10 mm×10 mm. The spray was performed using Unijet full cone nozzles with a volumetric flux of 0.044–0.053 m3/(m2·s) and a nozzle height of 17 mm. It is found that the heat transfer is obviously enhanced for straight fin surfaces relative to the flat surface. However, the increment decreases as the fin height increases. For flat surface and enhanced surfaces with a fin height of 0.1 mm and 0.2 mm, as the coolant flux increases, the heat flux increases as well. However, for finned surface with a height of 0.4 mm, the heat flux is not sensitive to the coolant volumetric flux. Changed film thickness and the form of water/surface interaction due to an enhanced surface structure (different fin height) are the main reasons for changing of the local heat transfer coefficient.

Keywords spray cooling      finned surface      heat transfer     
Corresponding Author(s): LIU Minghou,Email:mhliu@ustc.edu.cn   
Issue Date: 05 March 2011
 Cite this article:   
Minghou LIU,Yaqing WANG,Dong LIU, et al. Experimental study of the effects of structured surface geometry on water spray cooling performance in non-boiling regime[J]. Front Energ, 2011, 5(1): 75-82.
 URL:  
https://academic.hep.com.cn/fie/EN/10.1007/s11708-010-0014-0
https://academic.hep.com.cn/fie/EN/Y2011/V5/I1/75
Fig.1  Experimental setup
Fig.2  Schematic diagram of heat-target
Fig.3  Schematic diagram of simulated temperature
pressure/ MPavolumetric flux/(m3·m-2·s-1)diameter d32/μmvelocity v / (m·s-1)droplet flux n/s-1spray angle θ/(°)
0.300.044112.319.7468981953.3
0.350.049110.921.6537036155.6
0.400.053107.723.9585792657.2
Tab.1  Parameters of nozzles atomization
Fig.4  Enhanced surfaces
(a) CCD image; (b) Geometry of enhanced surface
a/mmb/mmc/mmS/cm2
channel 10.10.20.31.38
channel 20.20.20.31.76
channel 30.40.20.32.52
smooth0001
Tab.2  Dimensions of surfaces
Fig.5  Heat flux as a function of surface temperature and water volumetric flux
(a) Flat surface; (b) straight-finned surface with a height of 0.1 mm; (c) straight-finned surface with a height of 0.2 mm; (d) straight-finned surface with a height of 0.4 mm
Fig.6  Heat flux as a function of surface temperature and channel height
(a)=0.044 m/(m·s); (b)=0.049 m/(m·s); (c)=0.053 m/(m·s)
heat flux enhancement (0.044 m3/(m2·s))heat flux enhancement (0.049 m3/(m2·s))heat flux enhancement(0.053 m3/(m2·s))area enhancement
channel 139.039.54138
channel 253.067.07276
channel 331.622.018152
Tab.3  Effects of surface structure on heat flux (surface temperature =50°C)
unit: %
fin heightθm/θb
channel 1 (a=0.1 mm)0.976
channel 2 (a=0.2 mm)0.943
channel 3 (a=0.4 mm)0.932
Tab.4  / for enhanced structures
Fig.7  Heat transfer coefficient as a function of surface temperature and channel height for different volumetric flux
(a) =0.044 m/(m·s), (b) =0.049 m/(m·s)
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