Flow structure of a low aspect ratio wall-mounted airfoil operating in a low Reynolds number flow
•Flow-field across the span of a low aspect ratio wall-mounted airfoil was studied.•Laminar separation and transitional laminar separation were observed.•Mean and fluctuating velocity field varied across the span at lifting conditions.•Near-wake vortex shedding varies with spanwise location and angl...
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Veröffentlicht in: | Experimental thermal and fluid science 2018-12, Vol.99, p.94-116 |
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description | •Flow-field across the span of a low aspect ratio wall-mounted airfoil was studied.•Laminar separation and transitional laminar separation were observed.•Mean and fluctuating velocity field varied across the span at lifting conditions.•Near-wake vortex shedding varies with spanwise location and angle of attack.•A region of spanwise shear with weak dependency on angle of attack was observed.
Measurements on a wall-mounted NACA 0012 airfoil with an aspect ratio (AR) of 0.5 operating in the low Reynolds number (274,000, based on chord) regime were performed. Measurements included oil flow visualizations and velocity data obtained with a combination of pitot and hotwire probes. Three different geometric angles of attack (αg) equal to 0°, 5°, and 10° were considered and the effective angles of attack corresponding to these were quantified through measurements of the velocity vector in the potential flow around the airfoil. The flow around such a low AR airfoil is complex and can be three-dimensional across the span due to strong interaction between the junction, airfoil, and tip flows. In the mid-span region of the airfoil, laminar separation with and without reattachment was present on the suction-side and pressure-side respectively. The pressure-side separation, which is located near the trailing-edge, leads to vortex shedding in the near-wake of the airfoil. The character of this shedding, however, is different between αg = 5° and 10°. Towards the airfoil root (at 25% span), this shedding is supressed by the turbulent junction flow. Towards the free-end of the airfoil (at 75% span), shedding is observed even in the absence of pressure-side laminar separation and may be attributed to the interaction between the spanwise tip flow and the suction-side separation bubble. The airfoil boundary layer in this region is also thinner compared to that at the mid-span point. Further towards the airfoil tip (at 90% span), the shedding still exists; however, its intensity and character are modified by the dominant vortex dynamics. In proximity to the airfoil tip, the velocity and turbulence are affected by both the primary and secondary vorticity for the highest angle of attack studied. |
doi_str_mv | 10.1016/j.expthermflusci.2018.07.019 |
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Measurements on a wall-mounted NACA 0012 airfoil with an aspect ratio (AR) of 0.5 operating in the low Reynolds number (274,000, based on chord) regime were performed. Measurements included oil flow visualizations and velocity data obtained with a combination of pitot and hotwire probes. Three different geometric angles of attack (αg) equal to 0°, 5°, and 10° were considered and the effective angles of attack corresponding to these were quantified through measurements of the velocity vector in the potential flow around the airfoil. The flow around such a low AR airfoil is complex and can be three-dimensional across the span due to strong interaction between the junction, airfoil, and tip flows. In the mid-span region of the airfoil, laminar separation with and without reattachment was present on the suction-side and pressure-side respectively. The pressure-side separation, which is located near the trailing-edge, leads to vortex shedding in the near-wake of the airfoil. The character of this shedding, however, is different between αg = 5° and 10°. Towards the airfoil root (at 25% span), this shedding is supressed by the turbulent junction flow. Towards the free-end of the airfoil (at 75% span), shedding is observed even in the absence of pressure-side laminar separation and may be attributed to the interaction between the spanwise tip flow and the suction-side separation bubble. The airfoil boundary layer in this region is also thinner compared to that at the mid-span point. Further towards the airfoil tip (at 90% span), the shedding still exists; however, its intensity and character are modified by the dominant vortex dynamics. In proximity to the airfoil tip, the velocity and turbulence are affected by both the primary and secondary vorticity for the highest angle of attack studied.</description><identifier>ISSN: 0894-1777</identifier><identifier>EISSN: 1879-2286</identifier><identifier>DOI: 10.1016/j.expthermflusci.2018.07.019</identifier><language>eng</language><publisher>Philadelphia: Elsevier Inc</publisher><subject>Aerodynamics ; Angle of attack ; Boundary layer ; Boundary layers ; Fluid dynamics ; Fluid flow ; Horseshoe vortex ; Laminar separation ; Low aspect ratio ; Low aspect ratio airfoil ; Low Reynolds number flow ; Membrane separation ; Potential flow ; Pressure ; Ratio analysis ; Reynolds number ; Separation ; Strong interactions (field theory) ; Suction ; Tip vortex ; Turbulence ; Turbulent flow ; Velocity ; Vortex shedding ; Vortices ; Vorticity</subject><ispartof>Experimental thermal and fluid science, 2018-12, Vol.99, p.94-116</ispartof><rights>2018 Elsevier Inc.</rights><rights>Copyright Elsevier Science Ltd. Dec 2018</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c412t-b15f5687daae9fa6ecd7e379f314f0b66adaf0e50b59255e5a57b857a994dc3c3</citedby><cites>FETCH-LOGICAL-c412t-b15f5687daae9fa6ecd7e379f314f0b66adaf0e50b59255e5a57b857a994dc3c3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.expthermflusci.2018.07.019$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,780,784,3550,27924,27925,45995</link.rule.ids></links><search><creatorcontrib>Awasthi, M.</creatorcontrib><creatorcontrib>Moreau, D.J.</creatorcontrib><creatorcontrib>Doolan, C.J.</creatorcontrib><title>Flow structure of a low aspect ratio wall-mounted airfoil operating in a low Reynolds number flow</title><title>Experimental thermal and fluid science</title><description>•Flow-field across the span of a low aspect ratio wall-mounted airfoil was studied.•Laminar separation and transitional laminar separation were observed.•Mean and fluctuating velocity field varied across the span at lifting conditions.•Near-wake vortex shedding varies with spanwise location and angle of attack.•A region of spanwise shear with weak dependency on angle of attack was observed.
Measurements on a wall-mounted NACA 0012 airfoil with an aspect ratio (AR) of 0.5 operating in the low Reynolds number (274,000, based on chord) regime were performed. Measurements included oil flow visualizations and velocity data obtained with a combination of pitot and hotwire probes. Three different geometric angles of attack (αg) equal to 0°, 5°, and 10° were considered and the effective angles of attack corresponding to these were quantified through measurements of the velocity vector in the potential flow around the airfoil. The flow around such a low AR airfoil is complex and can be three-dimensional across the span due to strong interaction between the junction, airfoil, and tip flows. In the mid-span region of the airfoil, laminar separation with and without reattachment was present on the suction-side and pressure-side respectively. The pressure-side separation, which is located near the trailing-edge, leads to vortex shedding in the near-wake of the airfoil. The character of this shedding, however, is different between αg = 5° and 10°. Towards the airfoil root (at 25% span), this shedding is supressed by the turbulent junction flow. Towards the free-end of the airfoil (at 75% span), shedding is observed even in the absence of pressure-side laminar separation and may be attributed to the interaction between the spanwise tip flow and the suction-side separation bubble. The airfoil boundary layer in this region is also thinner compared to that at the mid-span point. Further towards the airfoil tip (at 90% span), the shedding still exists; however, its intensity and character are modified by the dominant vortex dynamics. In proximity to the airfoil tip, the velocity and turbulence are affected by both the primary and secondary vorticity for the highest angle of attack studied.</description><subject>Aerodynamics</subject><subject>Angle of attack</subject><subject>Boundary layer</subject><subject>Boundary layers</subject><subject>Fluid dynamics</subject><subject>Fluid flow</subject><subject>Horseshoe vortex</subject><subject>Laminar separation</subject><subject>Low aspect ratio</subject><subject>Low aspect ratio airfoil</subject><subject>Low Reynolds number flow</subject><subject>Membrane separation</subject><subject>Potential flow</subject><subject>Pressure</subject><subject>Ratio analysis</subject><subject>Reynolds number</subject><subject>Separation</subject><subject>Strong interactions (field theory)</subject><subject>Suction</subject><subject>Tip vortex</subject><subject>Turbulence</subject><subject>Turbulent flow</subject><subject>Velocity</subject><subject>Vortex shedding</subject><subject>Vortices</subject><subject>Vorticity</subject><issn>0894-1777</issn><issn>1879-2286</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNqNkEFLxDAQhYMouK7-h4BeW5O0aRrwIourwoIgeg5pOtGUtqlJ67r_3i67F2-eBt6894b5ELqhJKWEFrdNCj_D-Amhs-0UjUsZoWVKREqoPEELWgqZMFYWp2hBSpknVAhxji5ibAghJaNkgfS69VscxzCZcQqAvcUa7yUdBzAjDnp0Hm912yadn_oRaqxdsN612A-w3_Yf2PXH0Cvset_WEfdTV0HAdhYv0ZnVbYSr41yi9_XD2-op2bw8Pq_uN4nJKRuTinLLi1LUWoO0ugBTC8iEtBnNLamKQtfaEuCk4pJxDlxzUZVcaCnz2mQmW6LrQ-8Q_NcEcVSNn0I_n1SMMiZEnkkyu-4OLhN8jAGsGoLrdNgpStQeqmrUX6hqD1URoWaoc3x9iMP8ybeDoGYH9AZqF2Zcqvbuf0W_I-yLUw</recordid><startdate>201812</startdate><enddate>201812</enddate><creator>Awasthi, M.</creator><creator>Moreau, D.J.</creator><creator>Doolan, C.J.</creator><general>Elsevier Inc</general><general>Elsevier Science Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7QH</scope><scope>7TB</scope><scope>7U5</scope><scope>7UA</scope><scope>8FD</scope><scope>C1K</scope><scope>FR3</scope><scope>H8D</scope><scope>KR7</scope><scope>L7M</scope></search><sort><creationdate>201812</creationdate><title>Flow structure of a low aspect ratio wall-mounted airfoil operating in a low Reynolds number flow</title><author>Awasthi, M. ; Moreau, D.J. ; Doolan, C.J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c412t-b15f5687daae9fa6ecd7e379f314f0b66adaf0e50b59255e5a57b857a994dc3c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Aerodynamics</topic><topic>Angle of attack</topic><topic>Boundary layer</topic><topic>Boundary layers</topic><topic>Fluid dynamics</topic><topic>Fluid flow</topic><topic>Horseshoe vortex</topic><topic>Laminar separation</topic><topic>Low aspect ratio</topic><topic>Low aspect ratio airfoil</topic><topic>Low Reynolds number flow</topic><topic>Membrane separation</topic><topic>Potential flow</topic><topic>Pressure</topic><topic>Ratio analysis</topic><topic>Reynolds number</topic><topic>Separation</topic><topic>Strong interactions (field theory)</topic><topic>Suction</topic><topic>Tip vortex</topic><topic>Turbulence</topic><topic>Turbulent flow</topic><topic>Velocity</topic><topic>Vortex shedding</topic><topic>Vortices</topic><topic>Vorticity</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Awasthi, M.</creatorcontrib><creatorcontrib>Moreau, D.J.</creatorcontrib><creatorcontrib>Doolan, C.J.</creatorcontrib><collection>CrossRef</collection><collection>Aqualine</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Water Resources Abstracts</collection><collection>Technology Research Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Experimental thermal and fluid science</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Awasthi, M.</au><au>Moreau, D.J.</au><au>Doolan, C.J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Flow structure of a low aspect ratio wall-mounted airfoil operating in a low Reynolds number flow</atitle><jtitle>Experimental thermal and fluid science</jtitle><date>2018-12</date><risdate>2018</risdate><volume>99</volume><spage>94</spage><epage>116</epage><pages>94-116</pages><issn>0894-1777</issn><eissn>1879-2286</eissn><abstract>•Flow-field across the span of a low aspect ratio wall-mounted airfoil was studied.•Laminar separation and transitional laminar separation were observed.•Mean and fluctuating velocity field varied across the span at lifting conditions.•Near-wake vortex shedding varies with spanwise location and angle of attack.•A region of spanwise shear with weak dependency on angle of attack was observed.
Measurements on a wall-mounted NACA 0012 airfoil with an aspect ratio (AR) of 0.5 operating in the low Reynolds number (274,000, based on chord) regime were performed. Measurements included oil flow visualizations and velocity data obtained with a combination of pitot and hotwire probes. Three different geometric angles of attack (αg) equal to 0°, 5°, and 10° were considered and the effective angles of attack corresponding to these were quantified through measurements of the velocity vector in the potential flow around the airfoil. The flow around such a low AR airfoil is complex and can be three-dimensional across the span due to strong interaction between the junction, airfoil, and tip flows. In the mid-span region of the airfoil, laminar separation with and without reattachment was present on the suction-side and pressure-side respectively. The pressure-side separation, which is located near the trailing-edge, leads to vortex shedding in the near-wake of the airfoil. The character of this shedding, however, is different between αg = 5° and 10°. Towards the airfoil root (at 25% span), this shedding is supressed by the turbulent junction flow. Towards the free-end of the airfoil (at 75% span), shedding is observed even in the absence of pressure-side laminar separation and may be attributed to the interaction between the spanwise tip flow and the suction-side separation bubble. The airfoil boundary layer in this region is also thinner compared to that at the mid-span point. Further towards the airfoil tip (at 90% span), the shedding still exists; however, its intensity and character are modified by the dominant vortex dynamics. In proximity to the airfoil tip, the velocity and turbulence are affected by both the primary and secondary vorticity for the highest angle of attack studied.</abstract><cop>Philadelphia</cop><pub>Elsevier Inc</pub><doi>10.1016/j.expthermflusci.2018.07.019</doi><tpages>23</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Aerodynamics Angle of attack Boundary layer Boundary layers Fluid dynamics Fluid flow Horseshoe vortex Laminar separation Low aspect ratio Low aspect ratio airfoil Low Reynolds number flow Membrane separation Potential flow Pressure Ratio analysis Reynolds number Separation Strong interactions (field theory) Suction Tip vortex Turbulence Turbulent flow Velocity Vortex shedding Vortices Vorticity |
title | Flow structure of a low aspect ratio wall-mounted airfoil operating in a low Reynolds number flow |
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