The bubbly-slug transition in a high velocity two phase flow

A 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...

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Bibliographic Details
Main Authors: Griffith, P., Snyder, George A.
Other Authors: Massachusetts Institute of Technology. Division of Sponsored Research.
Format: Technical Report
Published: Cambridge, Mass. : M.I.T. Division of Sponsored Research, [1964] 2011
Subjects:
Online Access:http://hdl.handle.net/1721.1/61488
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author Griffith, P.
Snyder, George A.
author2 Massachusetts Institute of Technology. Division of Sponsored Research.
author_facet Massachusetts Institute of Technology. Division of Sponsored Research.
Griffith, P.
Snyder, George A.
author_sort Griffith, P.
collection MIT
description A 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.
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spelling mit-1721.1/614882019-04-12T11:57:53Z The bubbly-slug transition in a high velocity two phase flow Griffith, P. Snyder, George A. Massachusetts Institute of Technology. Division of Sponsored Research. Massachusetts Institute of Technology. Heat Transfer Laboratory. Bubbles. Pipe -- Fluid dynamics. Heat -- Transmission. A 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. Sponsored by the U. S. Atomic Energy Commission DSR 2011-03-04T23:36:45Z 2011-03-04T23:36:45Z 1964 Technical Report 14072541 http://hdl.handle.net/1721.1/61488 Technical report (Massachusetts Institute of Technology, Heat Transfer Laboratory) ; no. 29. [35] leaves in various pagings (some unnumbered) application/pdf Cambridge, Mass. : M.I.T. Division of Sponsored Research, [1964]
spellingShingle Bubbles.
Pipe -- Fluid dynamics.
Heat -- Transmission.
Griffith, P.
Snyder, George A.
The bubbly-slug transition in a high velocity two phase flow
title The bubbly-slug transition in a high velocity two phase flow
title_full The bubbly-slug transition in a high velocity two phase flow
title_fullStr The bubbly-slug transition in a high velocity two phase flow
title_full_unstemmed The bubbly-slug transition in a high velocity two phase flow
title_short The bubbly-slug transition in a high velocity two phase flow
title_sort bubbly slug transition in a high velocity two phase flow
topic Bubbles.
Pipe -- Fluid dynamics.
Heat -- Transmission.
url http://hdl.handle.net/1721.1/61488
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