Evidences for the existence of the ultimate regime in supergravitational turbulent thermal convection
What is the final state of turbulence when the driving parameter approaches to infinity? For thermal turbulence, in 1962, Kraichnan proposed a so-called ultimate scaling dependence of the heat transport (quantified by the Nusselt number \(\text{Nu}\)) on the Rayleigh number (\(\text{Ra}\)), which ca...
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description | What is the final state of turbulence when the driving parameter approaches to infinity? For thermal turbulence, in 1962, Kraichnan proposed a so-called ultimate scaling dependence of the heat transport (quantified by the Nusselt number \(\text{Nu}\)) on the Rayleigh number (\(\text{Ra}\)), which can be extrapolated to arbitrarily high \(\text{Ra}\). The existence of Kraichnan ultimate scaling has been intensively debated in the past decades. In this work, using a supergravitational thermal convection system, with an effective gravity up to 100 times the Earth's gravity, both Rayleigh number and shear Reynolds number can be boosted due to the increase of the buoyancy driving and the additional Coriolis forces. Over a decade of \(\text{Ra}\) range, we demonstrate the existence of Kraichnan-like ultimate regime with four direct evidences: the ultimate scaling dependence of \(\text{Nu}\) versus \(\text{Ra}\); the appearance of turbulent velocity boundary layer profile; the enhanced strength of the shear Reynolds number; the new statistical properties of local temperature fluctuations. The present findings will greatly improve the understanding of the flow dynamics in geophysical and astrophysical flows. |
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For thermal turbulence, in 1962, Kraichnan proposed a so-called ultimate scaling dependence of the heat transport (quantified by the Nusselt number \(\text{Nu}\)) on the Rayleigh number (\(\text{Ra}\)), which can be extrapolated to arbitrarily high \(\text{Ra}\). The existence of Kraichnan ultimate scaling has been intensively debated in the past decades. In this work, using a supergravitational thermal convection system, with an effective gravity up to 100 times the Earth's gravity, both Rayleigh number and shear Reynolds number can be boosted due to the increase of the buoyancy driving and the additional Coriolis forces. Over a decade of \(\text{Ra}\) range, we demonstrate the existence of Kraichnan-like ultimate regime with four direct evidences: the ultimate scaling dependence of \(\text{Nu}\) versus \(\text{Ra}\); the appearance of turbulent velocity boundary layer profile; the enhanced strength of the shear Reynolds number; the new statistical properties of local temperature fluctuations. The present findings will greatly improve the understanding of the flow dynamics in geophysical and astrophysical flows.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.2110.01224</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Coriolis force ; Earth gravitation ; Fluid flow ; Free convection ; Physics - Fluid Dynamics ; Rayleigh number ; Reynolds number ; Scaling ; Turbulence ; Turbulent boundary layer</subject><ispartof>arXiv.org, 2021-10</ispartof><rights>2021. 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For thermal turbulence, in 1962, Kraichnan proposed a so-called ultimate scaling dependence of the heat transport (quantified by the Nusselt number \(\text{Nu}\)) on the Rayleigh number (\(\text{Ra}\)), which can be extrapolated to arbitrarily high \(\text{Ra}\). The existence of Kraichnan ultimate scaling has been intensively debated in the past decades. In this work, using a supergravitational thermal convection system, with an effective gravity up to 100 times the Earth's gravity, both Rayleigh number and shear Reynolds number can be boosted due to the increase of the buoyancy driving and the additional Coriolis forces. Over a decade of \(\text{Ra}\) range, we demonstrate the existence of Kraichnan-like ultimate regime with four direct evidences: the ultimate scaling dependence of \(\text{Nu}\) versus \(\text{Ra}\); the appearance of turbulent velocity boundary layer profile; the enhanced strength of the shear Reynolds number; the new statistical properties of local temperature fluctuations. The present findings will greatly improve the understanding of the flow dynamics in geophysical and astrophysical flows.</description><subject>Coriolis force</subject><subject>Earth gravitation</subject><subject>Fluid flow</subject><subject>Free convection</subject><subject>Physics - Fluid Dynamics</subject><subject>Rayleigh number</subject><subject>Reynolds number</subject><subject>Scaling</subject><subject>Turbulence</subject><subject>Turbulent boundary layer</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GOX</sourceid><recordid>eNotkMtqwzAQRUWh0JDmA7qqoGun0kiypGUJ6QMC3WRvFHeUKjh2Kskm_fvaSVcDZ-4Ml0PIA2dLaZRizy6ew7AEPgLGAeQNmYEQvDAS4I4sUjowxqDUoJSYEVwP4QvbGhP1XaT5GymeQ8oTop2_gL7J4egy0oj7cEQaWpr6E8Z9dEPILoeudQ3Nfdz1DbZ5uonHkdRdO2A9re_JrXdNwsX_nJPt63q7ei82n28fq5dN4RSoAjVH5yWW6I1WEnagELTmxgpw1gsQxta1sUxIqcrSegNSc15asWMomRdz8nh9e3FQneJYO_5Wk4vq4mJMPF0Tp9j99Jhydej6ONZPFShtgSttlPgD_INiYw</recordid><startdate>20211004</startdate><enddate>20211004</enddate><creator>Jiang, Hechuan</creator><creator>Wang, Dongpu</creator><creator>Liu, Shuang</creator><creator>Sun, Chao</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20211004</creationdate><title>Evidences for the existence of the ultimate regime in supergravitational turbulent thermal convection</title><author>Jiang, Hechuan ; Wang, Dongpu ; Liu, Shuang ; Sun, Chao</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a525-e71eaf4e6ef87542b25e27718932a9f32389cc8903445669f824711693b0e40f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Coriolis force</topic><topic>Earth gravitation</topic><topic>Fluid flow</topic><topic>Free convection</topic><topic>Physics - Fluid Dynamics</topic><topic>Rayleigh number</topic><topic>Reynolds number</topic><topic>Scaling</topic><topic>Turbulence</topic><topic>Turbulent boundary layer</topic><toplevel>online_resources</toplevel><creatorcontrib>Jiang, Hechuan</creatorcontrib><creatorcontrib>Wang, Dongpu</creatorcontrib><creatorcontrib>Liu, Shuang</creatorcontrib><creatorcontrib>Sun, Chao</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection><collection>arXiv.org</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Jiang, Hechuan</au><au>Wang, Dongpu</au><au>Liu, Shuang</au><au>Sun, Chao</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Evidences for the existence of the ultimate regime in supergravitational turbulent thermal convection</atitle><jtitle>arXiv.org</jtitle><date>2021-10-04</date><risdate>2021</risdate><eissn>2331-8422</eissn><abstract>What is the final state of turbulence when the driving parameter approaches to infinity? For thermal turbulence, in 1962, Kraichnan proposed a so-called ultimate scaling dependence of the heat transport (quantified by the Nusselt number \(\text{Nu}\)) on the Rayleigh number (\(\text{Ra}\)), which can be extrapolated to arbitrarily high \(\text{Ra}\). The existence of Kraichnan ultimate scaling has been intensively debated in the past decades. In this work, using a supergravitational thermal convection system, with an effective gravity up to 100 times the Earth's gravity, both Rayleigh number and shear Reynolds number can be boosted due to the increase of the buoyancy driving and the additional Coriolis forces. Over a decade of \(\text{Ra}\) range, we demonstrate the existence of Kraichnan-like ultimate regime with four direct evidences: the ultimate scaling dependence of \(\text{Nu}\) versus \(\text{Ra}\); the appearance of turbulent velocity boundary layer profile; the enhanced strength of the shear Reynolds number; the new statistical properties of local temperature fluctuations. The present findings will greatly improve the understanding of the flow dynamics in geophysical and astrophysical flows.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.2110.01224</doi><oa>free_for_read</oa></addata></record> |
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subjects | Coriolis force Earth gravitation Fluid flow Free convection Physics - Fluid Dynamics Rayleigh number Reynolds number Scaling Turbulence Turbulent boundary layer |
title | Evidences for the existence of the ultimate regime in supergravitational turbulent thermal convection |
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