Effect of Wettability on Pool Boiling Incipience in Saturated WaterSource: Journal of Heat Transfer:;2016:;volume( 138 ):;issue: 008::page 80910DOI: 10.1115/1.4033815Publisher: The American Society of Mechanical Engineers (ASME)
Abstract: Three different copper surfaces bare, Al2O3 nanocoated, and Polytetrafluoroethylene (PTFE) coated are prepared and tested to examine the effect of wettability on the pool boiling incipience in saturated water at 1 atm. A copper surface is coated with Al2O3 particles ranging 25~43 nm in diameter by immersing the surface in Al2O3/ethanol nanofluid (1g/l) and boiled for 3 min. SEM image in Fig. 1 shows the coated Al2O3 nanoparticles on the copper surface, together with the reference bare surface. PTFE coating is also applied to the copper surface using spin coating method with the mixture of Dupont AF 2400 particles and 3M FC40 solvent. The final coating thickness of the PTFE coating is estimated to be 30 nm. The three surfaces exhibit different static contact angles, 78آ° (bare), 28آ° (nanocoated), and 120آ° (PTFE coated) in Fig. 2, respectively. Wettability affects the boiling incipience heat flux where initial bubble nucleation starts: 15 kW/m2 for the bare surface; 30 kW/m2 for the nanocoated surface; and 2.5 kW/m2 for the PTFE coated surface. Captured images from the high speed camera at 2,000 fps show significantly different bubble shapes and departure frequencies in Fig. 3. During the bubble growth, advancing contact angles are captured and shown qualitatively and found consistent with their static angle measurements for the sessile droplet observed at each surface. The larger bubble is generated on the nanocoated surface compared to that of the bare surface because improved wetting makes promising cavities flood and thus incipience is delayed, resulting in higher superheat. The single bubble life cycle appears to be much longer on the PTFE coated surface due to the increase of the contact angle which becomes hydrophobic (> 90آ°), resulting in lower bubble departure frequency. Successive tests at the same heat flux of 30 kW/m2 confirmed that life cycle on the PTFE coated surface (88.5 ms) is consistently longer than that on the bare surface (16.5 ms) and nanocoated surface (20 ms).
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contributor author | Kim, Jinsub | |
contributor author | Jun, Seongchul | |
contributor author | Lee, Jungho | |
contributor author | Lee, Seong Hyuk | |
contributor author | You, Seung M. | |
date accessioned | 2017-05-09T01:30:39Z | |
date available | 2017-05-09T01:30:39Z | |
date issued | 2016 | |
identifier issn | 0022-1481 | |
identifier other | ht_138_08_080910.pdf | |
identifier uri | http://yetl.yabesh.ir/yetl/handle/yetl/161686 | |
description abstract | Three different copper surfaces bare, Al2O3 nanocoated, and Polytetrafluoroethylene (PTFE) coated are prepared and tested to examine the effect of wettability on the pool boiling incipience in saturated water at 1 atm. A copper surface is coated with Al2O3 particles ranging 25~43 nm in diameter by immersing the surface in Al2O3/ethanol nanofluid (1g/l) and boiled for 3 min. SEM image in Fig. 1 shows the coated Al2O3 nanoparticles on the copper surface, together with the reference bare surface. PTFE coating is also applied to the copper surface using spin coating method with the mixture of Dupont AF 2400 particles and 3M FC40 solvent. The final coating thickness of the PTFE coating is estimated to be 30 nm. The three surfaces exhibit different static contact angles, 78آ° (bare), 28آ° (nanocoated), and 120آ° (PTFE coated) in Fig. 2, respectively. Wettability affects the boiling incipience heat flux where initial bubble nucleation starts: 15 kW/m2 for the bare surface; 30 kW/m2 for the nanocoated surface; and 2.5 kW/m2 for the PTFE coated surface. Captured images from the high speed camera at 2,000 fps show significantly different bubble shapes and departure frequencies in Fig. 3. During the bubble growth, advancing contact angles are captured and shown qualitatively and found consistent with their static angle measurements for the sessile droplet observed at each surface. The larger bubble is generated on the nanocoated surface compared to that of the bare surface because improved wetting makes promising cavities flood and thus incipience is delayed, resulting in higher superheat. The single bubble life cycle appears to be much longer on the PTFE coated surface due to the increase of the contact angle which becomes hydrophobic (> 90آ°), resulting in lower bubble departure frequency. Successive tests at the same heat flux of 30 kW/m2 confirmed that life cycle on the PTFE coated surface (88.5 ms) is consistently longer than that on the bare surface (16.5 ms) and nanocoated surface (20 ms). | |
publisher | The American Society of Mechanical Engineers (ASME) | |
title | Effect of Wettability on Pool Boiling Incipience in Saturated Water | |
type | Journal Paper | |
journal volume | 138 | |
journal issue | 8 | |
journal title | Journal of Heat Transfer | |
identifier doi | 10.1115/1.4033815 | |
journal fristpage | 80910 | |
journal lastpage | 80910 | |
identifier eissn | 1528-8943 | |
tree | Journal of Heat Transfer:;2016:;volume( 138 ):;issue: 008 | |
contenttype | Fulltext |