完整後設資料紀錄
DC 欄位 | 值 | 語言 |
---|---|---|
dc.contributor.author | Chen, C. A. | en_US |
dc.contributor.author | Lin, T. F. | en_US |
dc.contributor.author | Yan, Wei-Mon | en_US |
dc.date.accessioned | 2017-04-21T06:56:33Z | - |
dc.date.available | 2017-04-21T06:56:33Z | - |
dc.date.issued | 2017-03 | en_US |
dc.identifier.issn | 0017-9310 | en_US |
dc.identifier.uri | http://dx.doi.org/10.1016/j.ijheatmasstransfer.2016.10.014 | en_US |
dc.identifier.uri | http://hdl.handle.net/11536/133151 | - |
dc.description.abstract | The time periodic saturated boiling heat transfer in a horizontal annulus was investigated experimentally where the walls are under an oscillating heat flux. The fluid enters the duct with zero vapor quality (saturated liquid state). The amplitude of the imposed heat flux oscillation Delta q varies from 0% to 50% of mean imposed heat flux (q) over bar and four different periods of heat flux oscillation t(p) including 20, 30, 60 and 120 s are applied to the system. The measured data display that when the applied heat flux is close to that for the onset of stable flow boiling, intermittent flow boiling appears in which nucleate boiling on the heated surface only exists in a partial interval of each periodic cycle and the heat flux oscillation does not noticeably affect the time-average boiling curves and heat transfer coefficients. Besides, the heated wall temperature and evaporating flow pattern are found to oscillate periodically in time as well and at the same frequency as the imposed heat flux oscillation. Furthermore, in the persistent boiling the resulting oscillation amplitudes of the heated surface temperature, heat transfer coefficient gets larger for a longer period and larger amplitude of the imposed heat flux oscillation and for a higher mean imposed heat flux. The substantial time lag in the heated surface temperature oscillation is observed. In the first half of the periodic cycle in which the heat flux reduces with time, after the time lag the heated wall temperature decreases with time. The inverse processes occur in the second half of the cycle in which imposed heat flux increases with time. Finally, flow regime maps are provided to explain the boundaries separating different boiling regimes for the R-134a saturated boiling in the duct. (C) 2016 Elsevier Ltd. All rights reserved. | en_US |
dc.language.iso | en_US | en_US |
dc.subject | Time periodic saturated flow boiling | en_US |
dc.subject | Heat transfer | en_US |
dc.subject | R-134a | en_US |
dc.subject | Heat flux oscillation | en_US |
dc.subject | Mini-channel | en_US |
dc.title | Time periodic saturated flow boiling heat transfer of R-134a in a narrow annular duct due to heat flux oscillation | en_US |
dc.identifier.doi | 10.1016/j.ijheatmasstransfer.2016.10.014 | en_US |
dc.identifier.journal | INTERNATIONAL JOURNAL OF HEAT AND MASS TRANSFER | en_US |
dc.citation.volume | 106 | en_US |
dc.citation.spage | 35 | en_US |
dc.citation.epage | 46 | en_US |
dc.contributor.department | 機械工程學系 | zh_TW |
dc.contributor.department | Department of Mechanical Engineering | en_US |
dc.identifier.wosnumber | WOS:000393015000005 | en_US |
顯示於類別: | 期刊論文 |