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    Effect of Wettability on Pool Boiling Incipience in Saturated Water

    Source: Journal of Heat Transfer:;2016:;volume( 138 ):;issue: 008::page 80910
    Author:
    Kim, Jinsub
    ,
    Jun, Seongchul
    ,
    Lee, Jungho
    ,
    Lee, Seong Hyuk
    ,
    You, Seung M.
    DOI: 10.1115/1.4033815
    Publisher: 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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      Effect of Wettability on Pool Boiling Incipience in Saturated Water

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    http://yetl.yabesh.ir/yetl1/handle/yetl/161686
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    contributor authorKim, Jinsub
    contributor authorJun, Seongchul
    contributor authorLee, Jungho
    contributor authorLee, Seong Hyuk
    contributor authorYou, Seung M.
    date accessioned2017-05-09T01:30:39Z
    date available2017-05-09T01:30:39Z
    date issued2016
    identifier issn0022-1481
    identifier otherht_138_08_080910.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/161686
    description abstractThree 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).
    publisherThe American Society of Mechanical Engineers (ASME)
    titleEffect of Wettability on Pool Boiling Incipience in Saturated Water
    typeJournal Paper
    journal volume138
    journal issue8
    journal titleJournal of Heat Transfer
    identifier doi10.1115/1.4033815
    journal fristpage80910
    journal lastpage80910
    identifier eissn1528-8943
    treeJournal of Heat Transfer:;2016:;volume( 138 ):;issue: 008
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
    نرم افزار کتابخانه دیجیتال "دی اسپیس" فارسی شده توسط یابش برای کتابخانه های ایرانی | تماس با یابش
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