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dc.contributor.authorJi, Yulong
dc.contributor.authorChu, Lilin
dc.contributor.authorYu, Chunrong
dc.contributor.authorWang, Zongyu
dc.contributor.authorMa, Hongbin
dc.date.accessioned2022-02-04T14:27:35Z
dc.date.available2022-02-04T14:27:35Z
dc.date.copyright2020/02/05/
dc.date.issued2020
dc.identifier.issn0022-1481
dc.identifier.otherht_142_03_030906.pdf
dc.identifier.urihttp://yetl.yabesh.ir/yetl1/handle/yetl/4273696
dc.description.abstractFor an oscillating heat pipe (OHP), the hydraulic diameter must be sufficiently small so that vapor plug and liquid slug can be formed by the capillary action. Therefore, the hydraulic diameter should not exceed a critical value named maximum hydraulic diameter (MHD). In the current research, a glass OHP with a hydraulic diameter of 6 mm was fabricated, and ethanol was used as the working fluid (Figs. 1 and 2). With a hydraulic diameter far exceeding the maximum hydraulic diameter (MHD) defined by dh,max≤{2σBo[(ρl−ρv)g]}1/2, the OHP can function. But the flow pattern is very different from that with a diameter smaller than the MHD, and depends on the filling ratio. When the OHP is charged with a higher filling ratio, the flow pattern is from the bubbly flow to the slug flow as shown in Fig, 3. When the charging ratio is low, the dispersed bubbly flow with many small bubbles generated on the surface was observed, and the dispersed bubbly flow was directly transformed into the annular flow as shown in Fig. 4.
dc.publisherThe American Society of Mechanical Engineers (ASME)
dc.titleVisualization of an Oscillating Heat Pipe with Hydraulic Diameter Far Exceeding the Conventional Maximum Hydraulic Diameter
dc.typeJournal Paper
dc.journal.volume142
dc.journal.issue3
dc.journal.titleJournal of Heat Transfer
dc.identifier.doi10.1115/1.4046117
dc.journal.fristpage30906
dc.page30906
dc.treeJournal of Heat Transfer:;2020:;volume( 142 ):;issue: 003
dc.contenttypeFulltext


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