Study of the thickness of the liquid film formed by a round water jet impinging on a curved cylindrical wall
An experimental setup has been established to investigate the thickness profiles of the liquid film formed by an oblique round water jet impinging on curved walls. The influence of the jet velocity, jet angle, and radius of curvature of the curved wall on the thickness profile of the liquid film has...
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Veröffentlicht in: | Physics of fluids (1994) 2023-05, Vol.35 (5) |
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creator | Yuan Weiwei Huang, Yong Zhang Hongzhou |
description | An experimental setup has been established to investigate the thickness profiles of the liquid film formed by an oblique round water jet impinging on curved walls. The influence of the jet velocity, jet angle, and radius of curvature of the curved wall on the thickness profile of the liquid film has been investigated. Both on the flat and curved walls, as the jet velocity increases, the mode of the liquid film transitions from laminar to turbulent, and the thickness of the liquid film decreases first and then increases along the flow direction. The transition velocity range for the curved walls with the radius of curvature R = 30 mm is 19.1–25.08 m/s (Re = 10 946–14 373). Both on the flat and curved walls, the thicknesses of the liquid film increase in the downstream part of the liquid film while decreasing in the upstream part, as the jet angle increases. The laminar and turbulent thickness prediction models of liquid film on flat walls were extended to curved walls by replacing the distance away from a stagnation point with the radius of curvature. Predictions obtained by the present models agree well with measurements. Errors of the film thickness between the predictions and measurements along the centerline are mainly less than 20%, and the correlation coefficients (σc) are mainly located in 0.85–0.99. |
doi_str_mv | 10.1063/5.0149122 |
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The influence of the jet velocity, jet angle, and radius of curvature of the curved wall on the thickness profile of the liquid film has been investigated. Both on the flat and curved walls, as the jet velocity increases, the mode of the liquid film transitions from laminar to turbulent, and the thickness of the liquid film decreases first and then increases along the flow direction. The transition velocity range for the curved walls with the radius of curvature R = 30 mm is 19.1–25.08 m/s (Re = 10 946–14 373). Both on the flat and curved walls, the thicknesses of the liquid film increase in the downstream part of the liquid film while decreasing in the upstream part, as the jet angle increases. The laminar and turbulent thickness prediction models of liquid film on flat walls were extended to curved walls by replacing the distance away from a stagnation point with the radius of curvature. Predictions obtained by the present models agree well with measurements. Errors of the film thickness between the predictions and measurements along the centerline are mainly less than 20%, and the correlation coefficients (σc) are mainly located in 0.85–0.99.</description><identifier>ISSN: 1070-6631</identifier><identifier>EISSN: 1089-7666</identifier><identifier>DOI: 10.1063/5.0149122</identifier><identifier>CODEN: PHFLE6</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Correlation coefficients ; Film thickness ; Fluid dynamics ; Hydraulic jets ; Physics ; Prediction models ; Radius of curvature ; Stagnation point</subject><ispartof>Physics of fluids (1994), 2023-05, Vol.35 (5)</ispartof><rights>Author(s)</rights><rights>2023 Author(s). Published under an exclusive license by AIP Publishing.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c362t-a3b45258da7abe6a89873539ddd6582d724626f69406dc6b4f0bcf778374c7dc3</citedby><cites>FETCH-LOGICAL-c362t-a3b45258da7abe6a89873539ddd6582d724626f69406dc6b4f0bcf778374c7dc3</cites><orcidid>0000-0002-0775-5479 ; 0000-0002-3493-3357 ; 0000-0002-3770-0559</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,794,4512,27924,27925</link.rule.ids></links><search><creatorcontrib>Yuan Weiwei</creatorcontrib><creatorcontrib>Huang, Yong</creatorcontrib><creatorcontrib>Zhang Hongzhou</creatorcontrib><title>Study of the thickness of the liquid film formed by a round water jet impinging on a curved cylindrical wall</title><title>Physics of fluids (1994)</title><description>An experimental setup has been established to investigate the thickness profiles of the liquid film formed by an oblique round water jet impinging on curved walls. The influence of the jet velocity, jet angle, and radius of curvature of the curved wall on the thickness profile of the liquid film has been investigated. Both on the flat and curved walls, as the jet velocity increases, the mode of the liquid film transitions from laminar to turbulent, and the thickness of the liquid film decreases first and then increases along the flow direction. The transition velocity range for the curved walls with the radius of curvature R = 30 mm is 19.1–25.08 m/s (Re = 10 946–14 373). Both on the flat and curved walls, the thicknesses of the liquid film increase in the downstream part of the liquid film while decreasing in the upstream part, as the jet angle increases. The laminar and turbulent thickness prediction models of liquid film on flat walls were extended to curved walls by replacing the distance away from a stagnation point with the radius of curvature. Predictions obtained by the present models agree well with measurements. Errors of the film thickness between the predictions and measurements along the centerline are mainly less than 20%, and the correlation coefficients (σc) are mainly located in 0.85–0.99.</description><subject>Correlation coefficients</subject><subject>Film thickness</subject><subject>Fluid dynamics</subject><subject>Hydraulic jets</subject><subject>Physics</subject><subject>Prediction models</subject><subject>Radius of curvature</subject><subject>Stagnation point</subject><issn>1070-6631</issn><issn>1089-7666</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNp90EtLxDAQAOAiCq6rB_9BwJNC1zzaJD3K4gsWPKjnkOahWdtmN0lX-u_tsqseBCFDhpmPGZgsO0dwhiAl1-UMoqJCGB9kEwR5lTNK6eE2ZzCnlKDj7CTGJYSQVJhOsuY59XoA3oL0bsZw6qMzMX4XGrfunQbWNS2wPrRGg3oAEgTfdxp8ymQCWJoEXLty3dv4gO_GturDZqRqaFyng1OyGW3TnGZHVjbRnO3_afZ6d_syf8gXT_eP85tFrgjFKZekLkpcci2ZrA2VvOKMlKTSWtOSY81wQTG1tCog1YrWhYW1soxxwgrFtCLT7GI3dxX8ujcxiaXvQzeuFJhDDktOERzV5U6p4GMMxopVcK0Mg0BQbI8pSrE_5mivdjYql2RyvvvBGx9-oVhp-x_-O_kL3caClg</recordid><startdate>202305</startdate><enddate>202305</enddate><creator>Yuan Weiwei</creator><creator>Huang, Yong</creator><creator>Zhang Hongzhou</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/0000-0002-0775-5479</orcidid><orcidid>https://orcid.org/0000-0002-3493-3357</orcidid><orcidid>https://orcid.org/0000-0002-3770-0559</orcidid></search><sort><creationdate>202305</creationdate><title>Study of the thickness of the liquid film formed by a round water jet impinging on a curved cylindrical wall</title><author>Yuan Weiwei ; Huang, Yong ; Zhang Hongzhou</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c362t-a3b45258da7abe6a89873539ddd6582d724626f69406dc6b4f0bcf778374c7dc3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Correlation coefficients</topic><topic>Film thickness</topic><topic>Fluid dynamics</topic><topic>Hydraulic jets</topic><topic>Physics</topic><topic>Prediction models</topic><topic>Radius of curvature</topic><topic>Stagnation point</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Yuan Weiwei</creatorcontrib><creatorcontrib>Huang, Yong</creatorcontrib><creatorcontrib>Zhang Hongzhou</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>Yuan Weiwei</au><au>Huang, Yong</au><au>Zhang Hongzhou</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Study of the thickness of the liquid film formed by a round water jet impinging on a curved cylindrical wall</atitle><jtitle>Physics of fluids (1994)</jtitle><date>2023-05</date><risdate>2023</risdate><volume>35</volume><issue>5</issue><issn>1070-6631</issn><eissn>1089-7666</eissn><coden>PHFLE6</coden><abstract>An experimental setup has been established to investigate the thickness profiles of the liquid film formed by an oblique round water jet impinging on curved walls. The influence of the jet velocity, jet angle, and radius of curvature of the curved wall on the thickness profile of the liquid film has been investigated. Both on the flat and curved walls, as the jet velocity increases, the mode of the liquid film transitions from laminar to turbulent, and the thickness of the liquid film decreases first and then increases along the flow direction. The transition velocity range for the curved walls with the radius of curvature R = 30 mm is 19.1–25.08 m/s (Re = 10 946–14 373). Both on the flat and curved walls, the thicknesses of the liquid film increase in the downstream part of the liquid film while decreasing in the upstream part, as the jet angle increases. The laminar and turbulent thickness prediction models of liquid film on flat walls were extended to curved walls by replacing the distance away from a stagnation point with the radius of curvature. Predictions obtained by the present models agree well with measurements. Errors of the film thickness between the predictions and measurements along the centerline are mainly less than 20%, and the correlation coefficients (σc) are mainly located in 0.85–0.99.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/5.0149122</doi><tpages>17</tpages><orcidid>https://orcid.org/0000-0002-0775-5479</orcidid><orcidid>https://orcid.org/0000-0002-3493-3357</orcidid><orcidid>https://orcid.org/0000-0002-3770-0559</orcidid><oa>free_for_read</oa></addata></record> |
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source | AIP Journals Complete; Alma/SFX Local Collection |
subjects | Correlation coefficients Film thickness Fluid dynamics Hydraulic jets Physics Prediction models Radius of curvature Stagnation point |
title | Study of the thickness of the liquid film formed by a round water jet impinging on a curved cylindrical wall |
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