Experimental study of co-annular jet subjected to transverse disturbances
•Flow field of two coaxially aligned jets is presented.•Transverse flow injection bifurcates the co-annular/secondary jet into two lobes.•Manipulated primary jet velocity reduces 30% more compared to primary jet alone case.•Jet manipulation increases mixing and results in faster spreading for the pr...
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Veröffentlicht in: | Experimental thermal and fluid science 2015-09, Vol.66, p.53-62 |
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creator | Kurup, Arathi Laldinpuii Ölçmen, Semih M. Ahmed, Anwar |
description | •Flow field of two coaxially aligned jets is presented.•Transverse flow injection bifurcates the co-annular/secondary jet into two lobes.•Manipulated primary jet velocity reduces 30% more compared to primary jet alone case.•Jet manipulation increases mixing and results in faster spreading for the primary jet.
The results of an investigation of the flow field of two coaxially aligned jets consisting of an inner primary jet and a co-annular outer jet issuing from a nozzle with convex sidewalls are reported. A transverse flow injection into the co-annular jet was used to shape the co-annular jet flow. In the region between the exits of the two jets, a recirculating toroidal eddy is formed due to opposing pressure gradients. In the presence of transverse injection, the eddy bifurcates into two lobes with radially emanating flow structures that substantially increase the decay of axial velocity and the spread rate to twice the values when compared to the characteristics of the primary jet alone. Measurements of mean velocities and Reynolds stresses were made at the jet Reynolds number of 16,000 with the help of a specially designed two-component Laser-Doppler-Velocimetry system. Topology of the resulting complex flow in view of the measurements is presented and discussed. |
doi_str_mv | 10.1016/j.expthermflusci.2015.03.002 |
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The results of an investigation of the flow field of two coaxially aligned jets consisting of an inner primary jet and a co-annular outer jet issuing from a nozzle with convex sidewalls are reported. A transverse flow injection into the co-annular jet was used to shape the co-annular jet flow. In the region between the exits of the two jets, a recirculating toroidal eddy is formed due to opposing pressure gradients. In the presence of transverse injection, the eddy bifurcates into two lobes with radially emanating flow structures that substantially increase the decay of axial velocity and the spread rate to twice the values when compared to the characteristics of the primary jet alone. Measurements of mean velocities and Reynolds stresses were made at the jet Reynolds number of 16,000 with the help of a specially designed two-component Laser-Doppler-Velocimetry system. Topology of the resulting complex flow in view of the measurements is presented and discussed.</description><identifier>ISSN: 0894-1777</identifier><identifier>EISSN: 1879-2286</identifier><identifier>DOI: 10.1016/j.expthermflusci.2015.03.002</identifier><language>eng</language><publisher>Elsevier Inc</publisher><subject>Co-annular jet ; Decay rate ; Disturbances ; Eddies ; Emission ; Fluid dynamics ; Fluid flow ; Laser-doppler velocimetry ; Nozzles ; Spreads ; Turbulence</subject><ispartof>Experimental thermal and fluid science, 2015-09, Vol.66, p.53-62</ispartof><rights>2015 Elsevier Inc.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c396t-5bd8f25f5ee2100da5e5b21dd3d15109c45c7611b5ae2d39576888712e55973b3</citedby><cites>FETCH-LOGICAL-c396t-5bd8f25f5ee2100da5e5b21dd3d15109c45c7611b5ae2d39576888712e55973b3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S089417771500062X$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,776,780,3537,27901,27902,65306</link.rule.ids></links><search><creatorcontrib>Kurup, Arathi Laldinpuii</creatorcontrib><creatorcontrib>Ölçmen, Semih M.</creatorcontrib><creatorcontrib>Ahmed, Anwar</creatorcontrib><title>Experimental study of co-annular jet subjected to transverse disturbances</title><title>Experimental thermal and fluid science</title><description>•Flow field of two coaxially aligned jets is presented.•Transverse flow injection bifurcates the co-annular/secondary jet into two lobes.•Manipulated primary jet velocity reduces 30% more compared to primary jet alone case.•Jet manipulation increases mixing and results in faster spreading for the primary jet.
The results of an investigation of the flow field of two coaxially aligned jets consisting of an inner primary jet and a co-annular outer jet issuing from a nozzle with convex sidewalls are reported. A transverse flow injection into the co-annular jet was used to shape the co-annular jet flow. In the region between the exits of the two jets, a recirculating toroidal eddy is formed due to opposing pressure gradients. In the presence of transverse injection, the eddy bifurcates into two lobes with radially emanating flow structures that substantially increase the decay of axial velocity and the spread rate to twice the values when compared to the characteristics of the primary jet alone. Measurements of mean velocities and Reynolds stresses were made at the jet Reynolds number of 16,000 with the help of a specially designed two-component Laser-Doppler-Velocimetry system. Topology of the resulting complex flow in view of the measurements is presented and discussed.</description><subject>Co-annular jet</subject><subject>Decay rate</subject><subject>Disturbances</subject><subject>Eddies</subject><subject>Emission</subject><subject>Fluid dynamics</subject><subject>Fluid flow</subject><subject>Laser-doppler velocimetry</subject><subject>Nozzles</subject><subject>Spreads</subject><subject>Turbulence</subject><issn>0894-1777</issn><issn>1879-2286</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNqNkLFOwzAURS0EEqXwDxkYWBL8nDh2JBZUtVCpEgvMlmO_iERpUmynav8eV2Vh6_SWc6_uO4Q8As2AQvncZXjYhW9026afvGkzRoFnNM8oZVdkBlJUKWOyvCYzKqsiBSHELbnzvqOUSgZ0RtbLww5du8Uh6D7xYbLHZGwSM6Z6GKZeu6TDkPip7tAEtEkYk-D04PfoPCa2jQlX68Ggvyc3je49PvzdOflaLT8X7-nm4229eN2kJq_KkPLayobxhiPGAdRqjrxmYG1ugQOtTMGNKAFqrpHZvOKilFIKYMh5JfI6n5Onc-_OjT8T-qC2rTfY93rAcfIKRFGUsoJSXoAC42VRcYjoyxk1bvTeYaN20Yp2RwVUnWSrTv2XrU6yFc1VlB3jq3Mc4-f7Fp2KBEYttnVRnLJje1nRL2WBkXg</recordid><startdate>20150901</startdate><enddate>20150901</enddate><creator>Kurup, Arathi Laldinpuii</creator><creator>Ölçmen, Semih M.</creator><creator>Ahmed, Anwar</creator><general>Elsevier Inc</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7QH</scope><scope>7UA</scope><scope>C1K</scope><scope>F1W</scope><scope>H96</scope><scope>L.G</scope><scope>7TB</scope><scope>7U5</scope><scope>8FD</scope><scope>FR3</scope><scope>H8D</scope><scope>KR7</scope><scope>L7M</scope></search><sort><creationdate>20150901</creationdate><title>Experimental study of co-annular jet subjected to transverse disturbances</title><author>Kurup, Arathi Laldinpuii ; Ölçmen, Semih M. ; Ahmed, Anwar</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c396t-5bd8f25f5ee2100da5e5b21dd3d15109c45c7611b5ae2d39576888712e55973b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Co-annular jet</topic><topic>Decay rate</topic><topic>Disturbances</topic><topic>Eddies</topic><topic>Emission</topic><topic>Fluid dynamics</topic><topic>Fluid flow</topic><topic>Laser-doppler velocimetry</topic><topic>Nozzles</topic><topic>Spreads</topic><topic>Turbulence</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kurup, Arathi Laldinpuii</creatorcontrib><creatorcontrib>Ölçmen, Semih M.</creatorcontrib><creatorcontrib>Ahmed, Anwar</creatorcontrib><collection>CrossRef</collection><collection>Aqualine</collection><collection>Water Resources Abstracts</collection><collection>Environmental Sciences and Pollution Management</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</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>Kurup, Arathi Laldinpuii</au><au>Ölçmen, Semih M.</au><au>Ahmed, Anwar</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Experimental study of co-annular jet subjected to transverse disturbances</atitle><jtitle>Experimental thermal and fluid science</jtitle><date>2015-09-01</date><risdate>2015</risdate><volume>66</volume><spage>53</spage><epage>62</epage><pages>53-62</pages><issn>0894-1777</issn><eissn>1879-2286</eissn><abstract>•Flow field of two coaxially aligned jets is presented.•Transverse flow injection bifurcates the co-annular/secondary jet into two lobes.•Manipulated primary jet velocity reduces 30% more compared to primary jet alone case.•Jet manipulation increases mixing and results in faster spreading for the primary jet.
The results of an investigation of the flow field of two coaxially aligned jets consisting of an inner primary jet and a co-annular outer jet issuing from a nozzle with convex sidewalls are reported. A transverse flow injection into the co-annular jet was used to shape the co-annular jet flow. In the region between the exits of the two jets, a recirculating toroidal eddy is formed due to opposing pressure gradients. In the presence of transverse injection, the eddy bifurcates into two lobes with radially emanating flow structures that substantially increase the decay of axial velocity and the spread rate to twice the values when compared to the characteristics of the primary jet alone. Measurements of mean velocities and Reynolds stresses were made at the jet Reynolds number of 16,000 with the help of a specially designed two-component Laser-Doppler-Velocimetry system. Topology of the resulting complex flow in view of the measurements is presented and discussed.</abstract><pub>Elsevier Inc</pub><doi>10.1016/j.expthermflusci.2015.03.002</doi><tpages>10</tpages></addata></record> |
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subjects | Co-annular jet Decay rate Disturbances Eddies Emission Fluid dynamics Fluid flow Laser-doppler velocimetry Nozzles Spreads Turbulence |
title | Experimental study of co-annular jet subjected to transverse disturbances |
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