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dc.contributor.authorAslangil, Denis
dc.contributor.authorFarley, Zachary
dc.contributor.authorLawrie, Andrew G. W.
dc.contributor.authorBanerjee, Arindam
dc.date.accessioned2022-02-04T23:01:59Z
dc.date.available2022-02-04T23:01:59Z
dc.date.copyright12/1/2020 12:00:00 AM
dc.date.issued2020
dc.identifier.issn0098-2202
dc.identifier.otherfe_142_12_121103.pdf
dc.identifier.urihttp://yetl.yabesh.ir/yetl1/handle/yetl/4275952
dc.description.abstractWe present our findings from a numerical investigation of the acceleration-driven Rayleigh–Taylor Instability, modulated by varying periods without an applied acceleration field. It is well known from studies on shock-driven Richtmyer–Meshkov instability that mixing without external forcing grows with a scaling exponent as ≈t0.20−0.28. When the Rayleigh–Taylor Instability is subjected to varying periods of “zero” acceleration, the structural changes to the mixing layer remain remarkably small. After the acceleration is re-applied, the mixing layer quickly resumes the profile of development it would have had if there had been no intermission. This behavior contrasts in particular with the strong sensitivity that is found to other variable acceleration profiles examined previously in the literature.
dc.publisherThe American Society of Mechanical Engineers (ASME)
dc.titleRayleigh–Taylor Instability With Varying Periods of Zero Acceleration
dc.typeJournal Paper
dc.journal.volume142
dc.journal.issue12
dc.journal.titleJournal of Fluids Engineering
dc.identifier.doi10.1115/1.4048348
dc.journal.fristpage0121103-1
dc.journal.lastpage0121103-8
dc.page8
dc.treeJournal of Fluids Engineering:;2020:;volume( 142 ):;issue: 012
dc.contenttypeFulltext


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