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dc.creatorChen, Y.
dc.creatorZhao, J.
dc.date.accessioned2007-05-07T20:42:44Z
dc.date.available2007-05-07T20:42:44Z
dc.date.issued2006
dc.identifier.otherESL-IC-06-11-105
dc.identifier.urihttps://hdl.handle.net/1969.1/5244
dc.description.abstractThis article deals with the heat exchange coefficient varied with pulse frequency in the pulsation tube with different flow forms. The findings show that heat can be exchanged coefficient with the pulse frequency, and it has an optimal frequency. The laminar flow and turbulent flow have approximately the same optimal frequency, i.e., about 8 Hz. When the pulsation source was placed in the upstream and downstream position, the heat transformation was completed dissimilarly. These results are coincident with previous experiments. The article also gives some information on the applications of the heat transformation by pulse flow in the shell and tube heat exchanger.en
dc.format.extent77811 bytesen
dc.format.mimetypeapplication/pdf
dc.language.isoen_US
dc.publisherEnergy Systems Laboratory (http://esl.tamu.edu)
dc.publisherTexas A&M University (http://www.tamu.edu)
dc.subjectpulse flowen
dc.subjectstrong heat transformationen
dc.subjectcomputation fluid dynamicsen
dc.subjectshell and tube heat exchangeren
dc.titleApplications of the Strong Heat Transformation by Pulse Flow in the Shell and Tube Heat Exchangeren


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