Correlation analysis on volume vorticity and vortex in late boundary layer transition
In this paper, two functions are introduced to describe the turbulence generation in late flow transition. One is called the volume omega bar (volume Ω¯), which represents the flow rotation or vortex strength. The other is called the volume vorticity, which shows the flow statistical fluctuations. A...
Gespeichert in:
Veröffentlicht in: | Physics of fluids (1994) 2018-01, Vol.30 (1) |
---|---|
Hauptverfasser: | , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | |
---|---|
container_issue | 1 |
container_start_page | |
container_title | Physics of fluids (1994) |
container_volume | 30 |
creator | Dong, Xiangrui Tian, Shuling Liu, Chaoqun |
description | In this paper, two functions are introduced to describe the turbulence generation in late flow transition. One is called the volume omega bar (volume Ω¯), which represents the flow rotation or vortex strength. The other is called the volume vorticity, which shows the flow statistical fluctuations. Although they have very different definitions, one is for fluctuation and the other is for rotation, volume Ω¯ and volume vorticity are found highly correlated with a correlation factor greater than 0.9, which means that there is a very close correlation between flow fluctuation and flow rotation (vortex). While the vorticity flux keeps constant in the late flow transition through the integration over any sections either parallel or perpendicular to the flow direction, the volume Ω¯ is greatly increased along the flow direction during the flow transition process. This means that the vortex structures are greatly built up and rotation becomes more and more dominant. On the other hand, the total volume vorticity is also quickly increased, which shows that the fluctuation is stronger. The flow transition is a process with significant volume vorticity increase, which is attributed to two of the following crucial factors: the first one is the lengthening of the vorticity tubes from side boundary due to the vorticity line stretching, distortion, and tangling; the second one is the generation of countless self-closed vorticity rings within the domain. Both the increase of the volume vorticity and the volume Ω¯ can be a significant symbol of the flow transition from the laminar flow to turbulent flow. It also shows that vorticity (tubes or lines) cannot directly represent vortex and should not be simply used as a signal of the turbulent transition process. |
doi_str_mv | 10.1063/1.5009115 |
format | Article |
fullrecord | <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_crossref_primary_10_1063_1_5009115</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2115812048</sourcerecordid><originalsourceid>FETCH-LOGICAL-c292t-c34f89e101adc34a3e7bff889110a27b1146abe90c2001f116b3ceb087e98dc73</originalsourceid><addsrcrecordid>eNp9kEFPwzAMhSMEEmNw4B9U4gRSh510aXJEEwOkSVzYOUrTVMrUNSNpEf33pNvOnPwsf7aeHyH3CAsEzp5xsQSQiMsLMkMQMi8555eTLiHnnOE1uYlxBwBMUj4j25UPwba6d77LdKfbMbqYJf3j22FvUwm9M64f07A-dvY3c12WNmxW-aGrdRhTN9qQ9UF30U2XbslVo9to7851Trbr16_Ve775fPtYvWxyQyXtc8OKRkiLgLpOWjNbVk0jRPIPmpYVYsF1ZSUYCoANIq-YsRWI0kpRm5LNycPp7iH478HGXu38ENIXUdGUgUAKhUjU44kywccYbKMOwe2Tb4WgptQUqnNqiX06sTE9fUzlH_gP6iFs5w</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2115812048</pqid></control><display><type>article</type><title>Correlation analysis on volume vorticity and vortex in late boundary layer transition</title><source>AIP Journals Complete</source><source>Alma/SFX Local Collection</source><creator>Dong, Xiangrui ; Tian, Shuling ; Liu, Chaoqun</creator><creatorcontrib>Dong, Xiangrui ; Tian, Shuling ; Liu, Chaoqun</creatorcontrib><description>In this paper, two functions are introduced to describe the turbulence generation in late flow transition. One is called the volume omega bar (volume Ω¯), which represents the flow rotation or vortex strength. The other is called the volume vorticity, which shows the flow statistical fluctuations. Although they have very different definitions, one is for fluctuation and the other is for rotation, volume Ω¯ and volume vorticity are found highly correlated with a correlation factor greater than 0.9, which means that there is a very close correlation between flow fluctuation and flow rotation (vortex). While the vorticity flux keeps constant in the late flow transition through the integration over any sections either parallel or perpendicular to the flow direction, the volume Ω¯ is greatly increased along the flow direction during the flow transition process. This means that the vortex structures are greatly built up and rotation becomes more and more dominant. On the other hand, the total volume vorticity is also quickly increased, which shows that the fluctuation is stronger. The flow transition is a process with significant volume vorticity increase, which is attributed to two of the following crucial factors: the first one is the lengthening of the vorticity tubes from side boundary due to the vorticity line stretching, distortion, and tangling; the second one is the generation of countless self-closed vorticity rings within the domain. Both the increase of the volume vorticity and the volume Ω¯ can be a significant symbol of the flow transition from the laminar flow to turbulent flow. It also shows that vorticity (tubes or lines) cannot directly represent vortex and should not be simply used as a signal of the turbulent transition process.</description><identifier>ISSN: 1070-6631</identifier><identifier>EISSN: 1089-7666</identifier><identifier>DOI: 10.1063/1.5009115</identifier><identifier>CODEN: PHFLE6</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Boundary layer transition ; Correlation analysis ; Correlation coefficients ; Fluid dynamics ; Fluid flow ; Laminar flow ; Rotation ; Signal processing ; Tangling ; Tubes ; Turbulence ; Turbulent flow ; Variation ; Vortices ; Vorticity</subject><ispartof>Physics of fluids (1994), 2018-01, Vol.30 (1)</ispartof><rights>Author(s)</rights><rights>2018 Author(s). Published by AIP Publishing.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c292t-c34f89e101adc34a3e7bff889110a27b1146abe90c2001f116b3ceb087e98dc73</citedby><cites>FETCH-LOGICAL-c292t-c34f89e101adc34a3e7bff889110a27b1146abe90c2001f116b3ceb087e98dc73</cites><orcidid>0000-0003-3445-5102 ; 0000-0002-0651-9263</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,790,4498,27901,27902</link.rule.ids></links><search><creatorcontrib>Dong, Xiangrui</creatorcontrib><creatorcontrib>Tian, Shuling</creatorcontrib><creatorcontrib>Liu, Chaoqun</creatorcontrib><title>Correlation analysis on volume vorticity and vortex in late boundary layer transition</title><title>Physics of fluids (1994)</title><description>In this paper, two functions are introduced to describe the turbulence generation in late flow transition. One is called the volume omega bar (volume Ω¯), which represents the flow rotation or vortex strength. The other is called the volume vorticity, which shows the flow statistical fluctuations. Although they have very different definitions, one is for fluctuation and the other is for rotation, volume Ω¯ and volume vorticity are found highly correlated with a correlation factor greater than 0.9, which means that there is a very close correlation between flow fluctuation and flow rotation (vortex). While the vorticity flux keeps constant in the late flow transition through the integration over any sections either parallel or perpendicular to the flow direction, the volume Ω¯ is greatly increased along the flow direction during the flow transition process. This means that the vortex structures are greatly built up and rotation becomes more and more dominant. On the other hand, the total volume vorticity is also quickly increased, which shows that the fluctuation is stronger. The flow transition is a process with significant volume vorticity increase, which is attributed to two of the following crucial factors: the first one is the lengthening of the vorticity tubes from side boundary due to the vorticity line stretching, distortion, and tangling; the second one is the generation of countless self-closed vorticity rings within the domain. Both the increase of the volume vorticity and the volume Ω¯ can be a significant symbol of the flow transition from the laminar flow to turbulent flow. It also shows that vorticity (tubes or lines) cannot directly represent vortex and should not be simply used as a signal of the turbulent transition process.</description><subject>Boundary layer transition</subject><subject>Correlation analysis</subject><subject>Correlation coefficients</subject><subject>Fluid dynamics</subject><subject>Fluid flow</subject><subject>Laminar flow</subject><subject>Rotation</subject><subject>Signal processing</subject><subject>Tangling</subject><subject>Tubes</subject><subject>Turbulence</subject><subject>Turbulent flow</subject><subject>Variation</subject><subject>Vortices</subject><subject>Vorticity</subject><issn>1070-6631</issn><issn>1089-7666</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNp9kEFPwzAMhSMEEmNw4B9U4gRSh510aXJEEwOkSVzYOUrTVMrUNSNpEf33pNvOnPwsf7aeHyH3CAsEzp5xsQSQiMsLMkMQMi8555eTLiHnnOE1uYlxBwBMUj4j25UPwba6d77LdKfbMbqYJf3j22FvUwm9M64f07A-dvY3c12WNmxW-aGrdRhTN9qQ9UF30U2XbslVo9to7851Trbr16_Ve775fPtYvWxyQyXtc8OKRkiLgLpOWjNbVk0jRPIPmpYVYsF1ZSUYCoANIq-YsRWI0kpRm5LNycPp7iH478HGXu38ENIXUdGUgUAKhUjU44kywccYbKMOwe2Tb4WgptQUqnNqiX06sTE9fUzlH_gP6iFs5w</recordid><startdate>201801</startdate><enddate>201801</enddate><creator>Dong, Xiangrui</creator><creator>Tian, Shuling</creator><creator>Liu, Chaoqun</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0003-3445-5102</orcidid><orcidid>https://orcid.org/0000-0002-0651-9263</orcidid></search><sort><creationdate>201801</creationdate><title>Correlation analysis on volume vorticity and vortex in late boundary layer transition</title><author>Dong, Xiangrui ; Tian, Shuling ; Liu, Chaoqun</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c292t-c34f89e101adc34a3e7bff889110a27b1146abe90c2001f116b3ceb087e98dc73</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Boundary layer transition</topic><topic>Correlation analysis</topic><topic>Correlation coefficients</topic><topic>Fluid dynamics</topic><topic>Fluid flow</topic><topic>Laminar flow</topic><topic>Rotation</topic><topic>Signal processing</topic><topic>Tangling</topic><topic>Tubes</topic><topic>Turbulence</topic><topic>Turbulent flow</topic><topic>Variation</topic><topic>Vortices</topic><topic>Vorticity</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Dong, Xiangrui</creatorcontrib><creatorcontrib>Tian, Shuling</creatorcontrib><creatorcontrib>Liu, Chaoqun</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physics of fluids (1994)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Dong, Xiangrui</au><au>Tian, Shuling</au><au>Liu, Chaoqun</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Correlation analysis on volume vorticity and vortex in late boundary layer transition</atitle><jtitle>Physics of fluids (1994)</jtitle><date>2018-01</date><risdate>2018</risdate><volume>30</volume><issue>1</issue><issn>1070-6631</issn><eissn>1089-7666</eissn><coden>PHFLE6</coden><abstract>In this paper, two functions are introduced to describe the turbulence generation in late flow transition. One is called the volume omega bar (volume Ω¯), which represents the flow rotation or vortex strength. The other is called the volume vorticity, which shows the flow statistical fluctuations. Although they have very different definitions, one is for fluctuation and the other is for rotation, volume Ω¯ and volume vorticity are found highly correlated with a correlation factor greater than 0.9, which means that there is a very close correlation between flow fluctuation and flow rotation (vortex). While the vorticity flux keeps constant in the late flow transition through the integration over any sections either parallel or perpendicular to the flow direction, the volume Ω¯ is greatly increased along the flow direction during the flow transition process. This means that the vortex structures are greatly built up and rotation becomes more and more dominant. On the other hand, the total volume vorticity is also quickly increased, which shows that the fluctuation is stronger. The flow transition is a process with significant volume vorticity increase, which is attributed to two of the following crucial factors: the first one is the lengthening of the vorticity tubes from side boundary due to the vorticity line stretching, distortion, and tangling; the second one is the generation of countless self-closed vorticity rings within the domain. Both the increase of the volume vorticity and the volume Ω¯ can be a significant symbol of the flow transition from the laminar flow to turbulent flow. It also shows that vorticity (tubes or lines) cannot directly represent vortex and should not be simply used as a signal of the turbulent transition process.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.5009115</doi><tpages>14</tpages><orcidid>https://orcid.org/0000-0003-3445-5102</orcidid><orcidid>https://orcid.org/0000-0002-0651-9263</orcidid></addata></record> |
fulltext | fulltext |
identifier | ISSN: 1070-6631 |
ispartof | Physics of fluids (1994), 2018-01, Vol.30 (1) |
issn | 1070-6631 1089-7666 |
language | eng |
recordid | cdi_crossref_primary_10_1063_1_5009115 |
source | AIP Journals Complete; Alma/SFX Local Collection |
subjects | Boundary layer transition Correlation analysis Correlation coefficients Fluid dynamics Fluid flow Laminar flow Rotation Signal processing Tangling Tubes Turbulence Turbulent flow Variation Vortices Vorticity |
title | Correlation analysis on volume vorticity and vortex in late boundary layer transition |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-02-03T03%3A56%3A24IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Correlation%20analysis%20on%20volume%20vorticity%20and%20vortex%20in%20late%20boundary%20layer%20transition&rft.jtitle=Physics%20of%20fluids%20(1994)&rft.au=Dong,%20Xiangrui&rft.date=2018-01&rft.volume=30&rft.issue=1&rft.issn=1070-6631&rft.eissn=1089-7666&rft.coden=PHFLE6&rft_id=info:doi/10.1063/1.5009115&rft_dat=%3Cproquest_cross%3E2115812048%3C/proquest_cross%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=2115812048&rft_id=info:pmid/&rfr_iscdi=true |