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dc.contributor.authorGriffith, P.en_US
dc.contributor.authorSnyder, George A.en_US
dc.contributor.otherMassachusetts Institute of Technology. Division of Sponsored Research.en_US
dc.contributor.otherMassachusetts Institute of Technology. Heat Transfer Laboratory.en_US
dc.date.accessioned2011-03-04T23:36:45Z
dc.date.available2011-03-04T23:36:45Z
dc.date.issued1964en_US
dc.identifier14072541en_US
dc.identifier.urihttp://hdl.handle.net/1721.1/61488
dc.description.abstractA possible mechanism for the transition between bubbly and slug flow is proposed and tested in a simulated slug flow system. No sudden collapse of slug flow with increasing velocity is found and it is concluded that: a. Slug flow is generally stable at voids greater than 35%. b. Bubbly flow at voids higher than this is a result of entrance conditions. c. Visual observations of bubbly flow in unheated systems at higher voids are most likely faulty. No simple asymptote limit or criterion that would predict the location of the bubbly-slug transition was found.en_US
dc.description.sponsorshipSponsored by the U. S. Atomic Energy Commission DSRen_US
dc.format.extent[35] leaves in various pagings (some unnumbered)en_US
dc.publisherCambridge, Mass. : M.I.T. Division of Sponsored Research, [1964]en_US
dc.relation.ispartofseriesTechnical report (Massachusetts Institute of Technology, Heat Transfer Laboratory) ; no. 29.en_US
dc.subjectBubbles.en_US
dc.subjectPipe -- Fluid dynamics.en_US
dc.subjectHeat -- Transmission.en_US
dc.titleThe bubbly-slug transition in a high velocity two phase flowen_US
dc.typeTechnical Reporten_US


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