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dc.contributor.authorHsu, Li-Chiehen_US
dc.contributor.authorChen, Ing Younen_US
dc.contributor.authorChyu, Chien-Minen_US
dc.contributor.authorWang, Chi-Chuanen_US
dc.date.accessioned2016-03-28T00:04:11Z-
dc.date.available2016-03-28T00:04:11Z-
dc.date.issued2015-11-01en_US
dc.identifier.issn0894-1777en_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.expthermflusci.2015.06.012en_US
dc.identifier.urihttp://hdl.handle.net/11536/129400-
dc.description.abstractIn this study, single-phase/two-phase frictional characteristics and flow patterns of 900 bends are experimentally investigated. The two bends have inner diameters (D) of 5.5 and 9.5 mm with tube curvature ratio (2R/D) of 5.4 and 4.2, respectively. The bends are installed either an upward, horizontal or downward arrangement. For results concerned with single-phase flow, the bend friction factor (f(B)) is always greater than that of the straight tubes at the same liquid Reynolds number. On the other hand, the f(B) values for D = 9.5 mm with smaller curvature ratio are greater than those of D = 5.5 mm. The resultant two-phase frictional pressure drops of 90 bend are well predicted by the Sanchez Silva et al. [14]\'s correlation. For the two-phase frictional pressure gradient, the upward arrangement is greater than that of the horizontal arrangement due to swirled motion and liquid flow reversal. The flow reversals are observed for upward flow arrangement at specific flow pattern and pressure gradient. However, no swirled motion and liquid flow reversal is seen in the downward arrangement. As mass flux and quality increase, the differences of pressure drop among the three arrangements are getting smaller due to the appreciable offset by the rising flow inertia. Meanwhile, the liquid flow reversal is more evidently observed in the large diameter bend. Flow pattern map showing the region of liquid flow reversal is shown on the diagram of the superficial gas velocity (U-GS) versus superficial liquid velocity (U-LS). The region for liquid flow reversal for D = 9.5 mm is much greater than that of D = 5.5 mm. For D = 5 mm, there is no liquid flow reversal when U-GS is above 2 m/s. On the other hand, the threshold value is raised to 4 m/s for the 9.5 mm internal diameter tube. (C) 2015 Elsevier Inc. All rights reserved.en_US
dc.language.isoen_USen_US
dc.subjectTwo-phase flowen_US
dc.subject90 degrees benden_US
dc.subjectFrictional pressure dropen_US
dc.subjectFlow reversalen_US
dc.titleTwo-phase pressure drops and flow pattern observations in 90 degrees bends subject to upward, downward and horizontal arrangementsen_US
dc.typeArticleen_US
dc.identifier.doi10.1016/j.expthermflusci.2015.06.012en_US
dc.identifier.journalEXPERIMENTAL THERMAL AND FLUID SCIENCEen_US
dc.citation.volume68en_US
dc.citation.spage484en_US
dc.citation.epage492en_US
dc.contributor.department機械工程學系zh_TW
dc.contributor.departmentDepartment of Mechanical Engineeringen_US
dc.identifier.wosnumberWOS:000365361800045en_US
dc.citation.woscount0en_US
Appears in Collections:Articles