Effects of gas liquid ratio on the atomization characteristics of gas-liquid swirl coaxial injectors
To understand the atomization characteristics and atomization mechanism of the gas-liquid swirl coaxial (GLSC) injector, a back-lighting photography technique has been employed to capture the instantaneous spray images with a high speed camera. The diameter and velocity of the droplets in the spray...
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description | To understand the atomization characteristics and atomization mechanism of the gas-liquid swirl coaxial (GLSC) injector, a back-lighting photography technique has been employed to capture the instantaneous spray images with a high speed camera. The diameter and velocity of the droplets in the spray have been characterized with a Dantec Phase Doppler Anemometry (PDA) system. The effects of gas liquid ratio (GLR) on the spray pattern, Sauter mean diameter (SMD), diameter-velocity distribution and mass flow rate distribution were analyzed and discussed. The results show that the atomization of the GLSC injector is dominated by the film breakup when the GLR is small, and violent gas-liquid interaction when the GLR is large enough. The film breakup dominated spray can be divided into gas acceleration region and film breakup region while the violent gas-liquid interaction dominated spray can be divided into the gas acceleration region, violent gas-liquid interaction region and big droplets breakup region. The atomization characteristics of the GLSC injector is significantly influenced by the GLR. From the point of atomization performance, the increase of GLR has positive effects. It decreases the global Sauter mean diameter (GSMD) and varies the SMD distribution from a hollow cone shape (GLR = 0) to an inverted V shape, and finally slanted N shape. However, from the point of spatial distribution, the increase of GLR has negative effects, because the mass flow rate distribution becomes more nonuniform.
•Atomization mechanism of GLSC injector are analyzed.•Atomization is dominated by film breakup when the GLR is small.•Atomization is dominated by gas-liquid interaction when the GLR is large enough.•The SMD distribution shows hollow cone shape, inverted V shape and slanted N shape with different GLR. |
doi_str_mv | 10.1016/j.actaastro.2018.02.026 |
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•Atomization mechanism of GLSC injector are analyzed.•Atomization is dominated by film breakup when the GLR is small.•Atomization is dominated by gas-liquid interaction when the GLR is large enough.•The SMD distribution shows hollow cone shape, inverted V shape and slanted N shape with different GLR.</description><identifier>ISSN: 0094-5765</identifier><identifier>EISSN: 1879-2030</identifier><identifier>DOI: 10.1016/j.actaastro.2018.02.026</identifier><language>eng</language><publisher>Elmsford: Elsevier Ltd</publisher><subject>Acceleration ; Atomization ; Atomizing ; Atoms & subatomic particles ; Breakup ; Droplets ; Flow rates ; Fluids ; Gas-liquid interactions ; Gas-liquid ratio ; Gas-liquid swirl coaxial injector ; Gases ; High speed cameras ; Injectors ; Mass flow rate ; Phase Doppler Anemometer ; Photography ; Sauter mean diameter ; Spatial distribution ; Spray characteristics ; Velocity ; Velocity distribution ; Velocity measurement</subject><ispartof>Acta astronautica, 2018-05, Vol.146, p.24-32</ispartof><rights>2018 IAA</rights><rights>Copyright Elsevier BV May 2018</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c343t-fd075b0b809abc16262acf93a8f5cd105ea3c9868c359895497e1b101ac947d33</citedby><cites>FETCH-LOGICAL-c343t-fd075b0b809abc16262acf93a8f5cd105ea3c9868c359895497e1b101ac947d33</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.actaastro.2018.02.026$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,780,784,3549,27923,27924,45994</link.rule.ids></links><search><creatorcontrib>Kang, Zhongtao</creatorcontrib><creatorcontrib>Li, Qinglian</creatorcontrib><creatorcontrib>Zhang, Jiaqi</creatorcontrib><creatorcontrib>Cheng, Peng</creatorcontrib><title>Effects of gas liquid ratio on the atomization characteristics of gas-liquid swirl coaxial injectors</title><title>Acta astronautica</title><description>To understand the atomization characteristics and atomization mechanism of the gas-liquid swirl coaxial (GLSC) injector, a back-lighting photography technique has been employed to capture the instantaneous spray images with a high speed camera. The diameter and velocity of the droplets in the spray have been characterized with a Dantec Phase Doppler Anemometry (PDA) system. The effects of gas liquid ratio (GLR) on the spray pattern, Sauter mean diameter (SMD), diameter-velocity distribution and mass flow rate distribution were analyzed and discussed. The results show that the atomization of the GLSC injector is dominated by the film breakup when the GLR is small, and violent gas-liquid interaction when the GLR is large enough. The film breakup dominated spray can be divided into gas acceleration region and film breakup region while the violent gas-liquid interaction dominated spray can be divided into the gas acceleration region, violent gas-liquid interaction region and big droplets breakup region. The atomization characteristics of the GLSC injector is significantly influenced by the GLR. From the point of atomization performance, the increase of GLR has positive effects. It decreases the global Sauter mean diameter (GSMD) and varies the SMD distribution from a hollow cone shape (GLR = 0) to an inverted V shape, and finally slanted N shape. However, from the point of spatial distribution, the increase of GLR has negative effects, because the mass flow rate distribution becomes more nonuniform.
•Atomization mechanism of GLSC injector are analyzed.•Atomization is dominated by film breakup when the GLR is small.•Atomization is dominated by gas-liquid interaction when the GLR is large enough.•The SMD distribution shows hollow cone shape, inverted V shape and slanted N shape with different GLR.</description><subject>Acceleration</subject><subject>Atomization</subject><subject>Atomizing</subject><subject>Atoms & subatomic particles</subject><subject>Breakup</subject><subject>Droplets</subject><subject>Flow rates</subject><subject>Fluids</subject><subject>Gas-liquid interactions</subject><subject>Gas-liquid ratio</subject><subject>Gas-liquid swirl coaxial injector</subject><subject>Gases</subject><subject>High speed cameras</subject><subject>Injectors</subject><subject>Mass flow rate</subject><subject>Phase Doppler Anemometer</subject><subject>Photography</subject><subject>Sauter mean diameter</subject><subject>Spatial distribution</subject><subject>Spray characteristics</subject><subject>Velocity</subject><subject>Velocity distribution</subject><subject>Velocity measurement</subject><issn>0094-5765</issn><issn>1879-2030</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNqFkFtLAzEQhYMoWKu_wYDPWyfZW_JYSr1AwRd9DrPZrM2y3bRJ6u3Xm1L1VTgwMMx3DnMIuWYwY8Cq236GOiKG6N2MAxMz4EnVCZkwUcuMQw6nZAIgi6ysq_KcXITQA0DNhZyQdtl1RsdAXUdfMdDB7va2pR6jddSNNK4Nxeg29uuwGaleo095xtsQrf7Fsh8svFs_UO3ww-JA7dgna-fDJTnrcAjm6mdOycvd8nnxkK2e7h8X81Wm8yKPWddCXTbQCJDYaFbxiqPuZI6iK3XLoDSYaykqofNSClkWsjasSSWglkXd5vmU3Bx9t97t9iZE1bu9H1Ok4lDJEiBx6ao-XmnvQvCmU1tvN-g_FQN1qFT16q9SdahUAU-qEjk_kiY98WaNV0FbM2rTWp8-Va2z_3p8AzaehTs</recordid><startdate>201805</startdate><enddate>201805</enddate><creator>Kang, Zhongtao</creator><creator>Li, Qinglian</creator><creator>Zhang, Jiaqi</creator><creator>Cheng, Peng</creator><general>Elsevier Ltd</general><general>Elsevier BV</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7TB</scope><scope>7TG</scope><scope>8FD</scope><scope>FR3</scope><scope>H8D</scope><scope>KL.</scope><scope>L7M</scope></search><sort><creationdate>201805</creationdate><title>Effects of gas liquid ratio on the atomization characteristics of gas-liquid swirl coaxial injectors</title><author>Kang, Zhongtao ; Li, Qinglian ; Zhang, Jiaqi ; Cheng, Peng</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c343t-fd075b0b809abc16262acf93a8f5cd105ea3c9868c359895497e1b101ac947d33</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Acceleration</topic><topic>Atomization</topic><topic>Atomizing</topic><topic>Atoms & subatomic particles</topic><topic>Breakup</topic><topic>Droplets</topic><topic>Flow rates</topic><topic>Fluids</topic><topic>Gas-liquid interactions</topic><topic>Gas-liquid ratio</topic><topic>Gas-liquid swirl coaxial injector</topic><topic>Gases</topic><topic>High speed cameras</topic><topic>Injectors</topic><topic>Mass flow rate</topic><topic>Phase Doppler Anemometer</topic><topic>Photography</topic><topic>Sauter mean diameter</topic><topic>Spatial distribution</topic><topic>Spray characteristics</topic><topic>Velocity</topic><topic>Velocity distribution</topic><topic>Velocity measurement</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kang, Zhongtao</creatorcontrib><creatorcontrib>Li, Qinglian</creatorcontrib><creatorcontrib>Zhang, Jiaqi</creatorcontrib><creatorcontrib>Cheng, Peng</creatorcontrib><collection>CrossRef</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Acta astronautica</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kang, Zhongtao</au><au>Li, Qinglian</au><au>Zhang, Jiaqi</au><au>Cheng, Peng</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effects of gas liquid ratio on the atomization characteristics of gas-liquid swirl coaxial injectors</atitle><jtitle>Acta astronautica</jtitle><date>2018-05</date><risdate>2018</risdate><volume>146</volume><spage>24</spage><epage>32</epage><pages>24-32</pages><issn>0094-5765</issn><eissn>1879-2030</eissn><abstract>To understand the atomization characteristics and atomization mechanism of the gas-liquid swirl coaxial (GLSC) injector, a back-lighting photography technique has been employed to capture the instantaneous spray images with a high speed camera. The diameter and velocity of the droplets in the spray have been characterized with a Dantec Phase Doppler Anemometry (PDA) system. The effects of gas liquid ratio (GLR) on the spray pattern, Sauter mean diameter (SMD), diameter-velocity distribution and mass flow rate distribution were analyzed and discussed. The results show that the atomization of the GLSC injector is dominated by the film breakup when the GLR is small, and violent gas-liquid interaction when the GLR is large enough. The film breakup dominated spray can be divided into gas acceleration region and film breakup region while the violent gas-liquid interaction dominated spray can be divided into the gas acceleration region, violent gas-liquid interaction region and big droplets breakup region. The atomization characteristics of the GLSC injector is significantly influenced by the GLR. From the point of atomization performance, the increase of GLR has positive effects. It decreases the global Sauter mean diameter (GSMD) and varies the SMD distribution from a hollow cone shape (GLR = 0) to an inverted V shape, and finally slanted N shape. However, from the point of spatial distribution, the increase of GLR has negative effects, because the mass flow rate distribution becomes more nonuniform.
•Atomization mechanism of GLSC injector are analyzed.•Atomization is dominated by film breakup when the GLR is small.•Atomization is dominated by gas-liquid interaction when the GLR is large enough.•The SMD distribution shows hollow cone shape, inverted V shape and slanted N shape with different GLR.</abstract><cop>Elmsford</cop><pub>Elsevier Ltd</pub><doi>10.1016/j.actaastro.2018.02.026</doi><tpages>9</tpages></addata></record> |
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subjects | Acceleration Atomization Atomizing Atoms & subatomic particles Breakup Droplets Flow rates Fluids Gas-liquid interactions Gas-liquid ratio Gas-liquid swirl coaxial injector Gases High speed cameras Injectors Mass flow rate Phase Doppler Anemometer Photography Sauter mean diameter Spatial distribution Spray characteristics Velocity Velocity distribution Velocity measurement |
title | Effects of gas liquid ratio on the atomization characteristics of gas-liquid swirl coaxial injectors |
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