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Study of strong temperature mixing in subsonic grid turbulence
Strong temperature mixing in subsonic air turbulence is studied in an open‐circuit wind tunnel with a 0.5 m cross section. The specially constructed heating grid consumes up to 300 kW of electric power at a mean flow velocity of 11 m/sec. The highest mean absolute temperature 〈T〉 reaches 370°K, whil...
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Published in: | The Physics of fluids (1958) 1973-10, Vol.16 (10), p.1587-1598 |
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Language: | English |
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container_end_page | 1598 |
container_issue | 10 |
container_start_page | 1587 |
container_title | The Physics of fluids (1958) |
container_volume | 16 |
creator | Lin, Shih‐Chun Lin, Shao‐Chi |
description | Strong temperature mixing in subsonic air turbulence is studied in an open‐circuit wind tunnel with a 0.5 m cross section. The specially constructed heating grid consumes up to 300 kW of electric power at a mean flow velocity of 11 m/sec. The highest mean absolute temperature
〈T〉
reaches 370°K, while the rms temperature fluctuation
θ′
at midtunnel is typically 6°K. Basic statistics of the temperature field are measured and discussed. It is found, in particular, that (i) the streamwise decay of the normalized mean‐square temperature fluctuation
(θ′ / )
2
is not sensitive to the applied heating rates, suggesting that so far buoyancy contributes little to the dynamics of the turbulence; (ii) the observed decay rates are much higher than those reported by others in the literature and are consistent with the higher drag characteristics of the present grid; (iii) the temperature fluctuation spectrum, when normalized by local fluid properties and dissipation rates, retains a universal form and show an inertial‐convection subrange of limited extent; (iv) the one‐dimensional universal scalar inertial Kolmogoroff constant,
β
1
, determined from such subrange has a value of 0.60±0.06. |
doi_str_mv | 10.1063/1.1694184 |
format | article |
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〈T〉
reaches 370°K, while the rms temperature fluctuation
θ′
at midtunnel is typically 6°K. Basic statistics of the temperature field are measured and discussed. It is found, in particular, that (i) the streamwise decay of the normalized mean‐square temperature fluctuation
(θ′ / < T >)
2
is not sensitive to the applied heating rates, suggesting that so far buoyancy contributes little to the dynamics of the turbulence; (ii) the observed decay rates are much higher than those reported by others in the literature and are consistent with the higher drag characteristics of the present grid; (iii) the temperature fluctuation spectrum, when normalized by local fluid properties and dissipation rates, retains a universal form and show an inertial‐convection subrange of limited extent; (iv) the one‐dimensional universal scalar inertial Kolmogoroff constant,
β
1
, determined from such subrange has a value of 0.60±0.06.</description><identifier>ISSN: 0031-9171</identifier><identifier>EISSN: 2163-4998</identifier><identifier>DOI: 10.1063/1.1694184</identifier><identifier>CODEN: PFLDAS</identifier><language>eng</language><ispartof>The Physics of fluids (1958), 1973-10, Vol.16 (10), p.1587-1598</ispartof><rights>American Institute of Physics</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c262t-ec3b0fad9a01f482d8d16a47283074cca292a1c9a3a1945cd4069e2bc2ce03f93</citedby><cites>FETCH-LOGICAL-c262t-ec3b0fad9a01f482d8d16a47283074cca292a1c9a3a1945cd4069e2bc2ce03f93</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Lin, Shih‐Chun</creatorcontrib><creatorcontrib>Lin, Shao‐Chi</creatorcontrib><title>Study of strong temperature mixing in subsonic grid turbulence</title><title>The Physics of fluids (1958)</title><description>Strong temperature mixing in subsonic air turbulence is studied in an open‐circuit wind tunnel with a 0.5 m cross section. The specially constructed heating grid consumes up to 300 kW of electric power at a mean flow velocity of 11 m/sec. The highest mean absolute temperature
〈T〉
reaches 370°K, while the rms temperature fluctuation
θ′
at midtunnel is typically 6°K. Basic statistics of the temperature field are measured and discussed. It is found, in particular, that (i) the streamwise decay of the normalized mean‐square temperature fluctuation
(θ′ / < T >)
2
is not sensitive to the applied heating rates, suggesting that so far buoyancy contributes little to the dynamics of the turbulence; (ii) the observed decay rates are much higher than those reported by others in the literature and are consistent with the higher drag characteristics of the present grid; (iii) the temperature fluctuation spectrum, when normalized by local fluid properties and dissipation rates, retains a universal form and show an inertial‐convection subrange of limited extent; (iv) the one‐dimensional universal scalar inertial Kolmogoroff constant,
β
1
, determined from such subrange has a value of 0.60±0.06.</description><issn>0031-9171</issn><issn>2163-4998</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1973</creationdate><recordtype>article</recordtype><recordid>eNp9j01LxDAURYMoWEcX_oNsFTq-l8S22Qgy-AUDLtR1SV-SITJthyQF599bmVm7unDv4cJh7BphiVDJO1xipRU26oQVAitZKq2bU1YASCw11njOLlL6BhAKlSzYw0ee7J6Pnqccx2HDs-t3Lpo8Rcf78BPmKgw8TV0ah0B8E4Pl89hNWzeQu2Rn3myTuzrmgn09P32uXsv1-8vb6nFdkqhELh3JDryx2gB61QjbWKyMqkUjoVZERmhhkLSRBrW6J6ug0k50JMiB9Fou2M3hl-KYUnS-3cXQm7hvEdo_8Rbbo_jM3h7YRCGbHMbhH_gXReNYhQ</recordid><startdate>197310</startdate><enddate>197310</enddate><creator>Lin, Shih‐Chun</creator><creator>Lin, Shao‐Chi</creator><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>197310</creationdate><title>Study of strong temperature mixing in subsonic grid turbulence</title><author>Lin, Shih‐Chun ; Lin, Shao‐Chi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c262t-ec3b0fad9a01f482d8d16a47283074cca292a1c9a3a1945cd4069e2bc2ce03f93</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1973</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Lin, Shih‐Chun</creatorcontrib><creatorcontrib>Lin, Shao‐Chi</creatorcontrib><collection>CrossRef</collection><jtitle>The Physics of fluids (1958)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Lin, Shih‐Chun</au><au>Lin, Shao‐Chi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Study of strong temperature mixing in subsonic grid turbulence</atitle><jtitle>The Physics of fluids (1958)</jtitle><date>1973-10</date><risdate>1973</risdate><volume>16</volume><issue>10</issue><spage>1587</spage><epage>1598</epage><pages>1587-1598</pages><issn>0031-9171</issn><eissn>2163-4998</eissn><coden>PFLDAS</coden><abstract>Strong temperature mixing in subsonic air turbulence is studied in an open‐circuit wind tunnel with a 0.5 m cross section. The specially constructed heating grid consumes up to 300 kW of electric power at a mean flow velocity of 11 m/sec. The highest mean absolute temperature
〈T〉
reaches 370°K, while the rms temperature fluctuation
θ′
at midtunnel is typically 6°K. Basic statistics of the temperature field are measured and discussed. It is found, in particular, that (i) the streamwise decay of the normalized mean‐square temperature fluctuation
(θ′ / < T >)
2
is not sensitive to the applied heating rates, suggesting that so far buoyancy contributes little to the dynamics of the turbulence; (ii) the observed decay rates are much higher than those reported by others in the literature and are consistent with the higher drag characteristics of the present grid; (iii) the temperature fluctuation spectrum, when normalized by local fluid properties and dissipation rates, retains a universal form and show an inertial‐convection subrange of limited extent; (iv) the one‐dimensional universal scalar inertial Kolmogoroff constant,
β
1
, determined from such subrange has a value of 0.60±0.06.</abstract><doi>10.1063/1.1694184</doi><tpages>12</tpages></addata></record> |
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title | Study of strong temperature mixing in subsonic grid turbulence |
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