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dc.contributor.authorChen, Ing Younen_US
dc.contributor.authorChen, Chien-Jenen_US
dc.contributor.authorWang, Chi-Chuanen_US
dc.date.accessioned2019-04-02T06:00:07Z-
dc.date.available2019-04-02T06:00:07Z-
dc.date.issued2014-10-01en_US
dc.identifier.issn0017-9310en_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.ijheatmasstransfer.2014.06.023en_US
dc.identifier.urihttp://hdl.handle.net/11536/147779-
dc.description.abstractIn this study, the effects of electrode configuration on the cooling of LED are presented. A total of six needle type electrodes, including sharp, 0.08, 0.12, 0.37, 0.49 R and flat tip, are used to generate ionic wind for cooling of the LED. The effects of electrode configuration, vertical separation height, and tilt angle on the cooling performance of a LED are reported in this study. It is found that the thermal resistance is reduced with the supplied voltage and a maximum 50% reduction is achieved before the spark-over voltage. For the same supplied voltage, the thermal resistance with a larger vertical separation is also higher. However, the operational range is also longer. The effect of tilt angle on the cooling performance of LED depends on the supplied voltage. With a supplied voltage being less than 6.5 kV, it is found that the thermal resistance is increased when the tilt angle is reduced with a tip radius of 0.12 R. However, the trend is reversed when the supplied voltage is higher than 6.5 kV where the thermal resistance of a smaller tilt angle is lower than that of a larger tilt angle. For the same mesh ground, the effect of electrode configurations cast little influence on the final thermal resistance. All the electrodes show an approximately 50% reduction of thermal resistance in association with its original thermal resistance. However, the corresponding threshold voltage and operational voltage differs significantly. The threshold voltage is lowest for the sharp needle and is increased with the rise of tip radius. On the other hand, the corresponding operational range becomes narrower when the tip radius is increased. Yet the spark-over voltage is also insensitive to change of electrode configuration. (C) 2014 Elsevier Ltd. All rights reserved.en_US
dc.language.isoen_USen_US
dc.subjectThermal managementen_US
dc.subjectElectronic equipment coolingen_US
dc.subjectElectrohydrodynamicsen_US
dc.subjectIonic winden_US
dc.subjectThreshold voltageen_US
dc.subjectSpark-over voltageen_US
dc.titleInfluence of electrode configuration on the heat transfer performance of a LED heat sourceen_US
dc.typeArticleen_US
dc.identifier.doi10.1016/j.ijheatmasstransfer.2014.06.023en_US
dc.identifier.journalINTERNATIONAL JOURNAL OF HEAT AND MASS TRANSFERen_US
dc.citation.volume77en_US
dc.citation.spage795en_US
dc.citation.epage801en_US
dc.contributor.department機械工程學系zh_TW
dc.contributor.departmentDepartment of Mechanical Engineeringen_US
dc.identifier.wosnumberWOS:000340302400069en_US
dc.citation.woscount12en_US
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