Scaling of nucleate boiling rates from water to liquid helium I: wetting conditions on oxidized copper surfaces

Cryogenics ◽  
1992 ◽  
Vol 32 (5) ◽  
pp. 430-432 ◽  
Author(s):  
K.V. Ravikumar ◽  
V. Dhir ◽  
T.H.K. Frederking
Author(s):  
Ursan Tchouteng Njike ◽  
Samuel Cabrera ◽  
Emma R. McClure ◽  
Van P. Carey

Abstract The work reported in this paper explored the use of machine learning tools to analyze quenching pool boiling data in the nucleate boiling range, near maximum heat flux range, and through the transition boiling range towards the Leidenfrost (minimum heat flux) point. It specifically explores the hypothesis that this sequence is a consequence of progressive dryout of the surface as the wall superheat increases. Machine learning tools are used with a heuristic model of the dryout parametric dependence to extract information about the magnitude of surface dryout as the superheat increases. From experimental data, the machine learning analysis provides an indication of how the dryout transition differs for different surface wetting characteristics and substrate materials. The wetting variations considered ranged from moderately wetted plain aluminum and copper surfaces to highly wetted nanostructured superhydrophilic surfaces. The data examined included aluminum and copper substrates. The results of the machine learning analysis indicate that the properties of the surface substrate can have a significant effect on the progressive surface dryout. In contrast, the surface wetting characteristics had a more limited effect for the surfaces tested. The paper concludes with an assessment of the implications of the findings for developing enhanced surfaces for boiling heat transfer performance.


2015 ◽  
Vol 137 (4) ◽  
Author(s):  
Mohamed S. El-Genk ◽  
Amir F. Ali

Pool boiling experiments are performed to investigate potential enhancement of critical heat flux (CHF) of PF-5060 dielectric liquid on microporous copper (MPC) surfaces and the effect of surface inclination angle. The morphology and microstructure of the MPC surfaces change with thickness. The experiments tested seven 10 × 10 mm MPC surfaces with thicknesses from 80 to 230 μm at inclination angles of 0 deg (upward facing), 60 deg, 90 deg (vertical), 120 deg, 150 deg, 160 deg, 170 deg, and 180 deg (downward facing). CHF increases as the thickness of the surface increases and/or the inclination angle decreases. The values in the upward facing orientation are 36–59% higher than on smooth Cu. For all surfaces, CHF values in the downward facing orientation are approximately 28% of those in the upward facing orientation. A developed CHF correlation, similar to those of Zuber and Kutateladze, accounts for the effects of inclination angle and thickness of the MPC surfaces. It is in good agreement with experimental data to within ±8%. Still photographs of nucleate boiling on the MPC surfaces at different inclinations help the interpretation of the experimental results.


Author(s):  
Jack L. Parker ◽  
Mohamed S. El-Genk

Experiments are performed, which investigated the enhancement in saturation boiling of HFE-7100 dielectric liquid on copper surfaces having a footprint of 10 × 10 mm and four 3 × 3 mm corner pins that are 2, 3 and 5 mm tall. These pins increase the geometrical surface area, by 96%, 144%, and 240%, respectively, and the surfaces are prepared using #400 and #1500 emery papers to investigate the effect of roughness on boiling heat transfer. Still photographs and video footage are recorded of the boiling processes. Nucleate boiling starts at a few isolated sites on the inside of the pins, close to the common line with the base surface, markedly reducing or eliminating the temperature excursion prior to boiling incipience. Measurable enhancements are obtained in both natural convection and nucleate boiling heat transfer. On the plane Cu surfaces prepared with emery paper #1500, the maximum nucleate boiling heat transfer coefficient, based on the foot print area, hB*, is 1.16 W/cm2.K and increases to 1.80, 2.03 and 2.37 W/cm2.K on the surfaces with 2, 3, and 5 mm tall pins. Similarly, the Critical Heat Flux (CHF), based on the foot print area, increases linearly with increased pin height, at a rate of ∼ 32% per mm. Increased surface roughness increases both hB* and CHF by additional 15% and 10% and markedly enhances nucleate boiling heat transfer at high surface superheats (ΔTsat > ∼10 K), but causes only little enhancement at lower superheats.


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