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Shapes of nonbuoyant round hydrocarbon-fueled laminar-jet diffusion flames in still air
The soot-luminosity boundaries (near the laminar smoke-point condition) of steady nonbuoyant round hydrocarbon/air laminar-jet diffusion flames at microgravity were found from color video images obtained on orbit during three flights of the Space Shuttle Columbia (flights STS-83, STS-94, and STS-107...
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Published in: | Combustion and flame 2005-07, Vol.142 (1), p.1-16 |
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container_title | Combustion and flame |
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creator | Aalburg, C. Diez, F.J. Faeth, G.M. Sunderland, P.B. Urban, D.L. Yuan, Z.-G. |
description | The soot-luminosity boundaries (near the laminar smoke-point condition) of steady nonbuoyant round hydrocarbon/air laminar-jet diffusion flames at microgravity were found from color video images obtained on orbit during three flights of the Space Shuttle Columbia (flights STS-83, STS-94, and STS-107); these test conditions included ethylene- and propane-fueled flames burning in still air at an ambient temperature of 300 K, ambient pressures of 35–130 kPa, jet exit diameters of 0.40–2.70 mm, and jet exit Reynolds numbers of 46–1186 to yield steady round flames, with most of the flames near the laminar smoke-point condition (including flames both emitting and not emitting soot). These results were supplemented by observations of the flame-sheet locations (locations where the local mixture fraction is stoichiometric) of nonbuoyant round soot-free and soot-containing hydrocarbon/air laminar-jet diffusion flames at microgravity found from filtered color images (at the CH line or
430
±
5
nm
) obtained using a 2.2-s free-fall facility; these test conditions included methane-, ethane-, and propane-fueled flames burning in still air at an ambient temperature of 300 K, ambient pressures of 25–98 kPa, jet exit diameters of 0.42–3.25 mm, and jet exit Reynolds numbers of 10–625. Simplified expressions to estimate soot-luminosity boundaries (near the laminar smoke-point condition) and flame-sheet locations were obtained using the classic analysis of D.B. Spalding (Combustion and Mass Transfer, Pergamon, New York, 1979, p. 185), extended empirically to account for the presence of soot luminosity for flames near the laminar smoke-point condition. The extended Spalding analysis provided good correlations of both soot-luminosity boundaries (near the laminar smoke-point condition) and flame-sheet locations for flames having short characteristic residence times where radiative heat losses from the flames were small. These results showed that soot-luminosity lengths near the laminar smoke-point condition were roughly twice as long as the flame-sheet location for both soot-free (blue) and soot-containing flames under comparable conditions due to the presence of luminous soot particles beyond the flame sheet within the fuel-lean portion of the flames. |
doi_str_mv | 10.1016/j.combustflame.2004.12.009 |
format | article |
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430
±
5
nm
) obtained using a 2.2-s free-fall facility; these test conditions included methane-, ethane-, and propane-fueled flames burning in still air at an ambient temperature of 300 K, ambient pressures of 25–98 kPa, jet exit diameters of 0.42–3.25 mm, and jet exit Reynolds numbers of 10–625. Simplified expressions to estimate soot-luminosity boundaries (near the laminar smoke-point condition) and flame-sheet locations were obtained using the classic analysis of D.B. Spalding (Combustion and Mass Transfer, Pergamon, New York, 1979, p. 185), extended empirically to account for the presence of soot luminosity for flames near the laminar smoke-point condition. The extended Spalding analysis provided good correlations of both soot-luminosity boundaries (near the laminar smoke-point condition) and flame-sheet locations for flames having short characteristic residence times where radiative heat losses from the flames were small. These results showed that soot-luminosity lengths near the laminar smoke-point condition were roughly twice as long as the flame-sheet location for both soot-free (blue) and soot-containing flames under comparable conditions due to the presence of luminous soot particles beyond the flame sheet within the fuel-lean portion of the flames.</description><identifier>ISSN: 0010-2180</identifier><identifier>EISSN: 1556-2921</identifier><identifier>DOI: 10.1016/j.combustflame.2004.12.009</identifier><identifier>CODEN: CBFMAO</identifier><language>eng</language><publisher>New York, NY: Elsevier Inc</publisher><subject>Applied sciences ; Boundaries ; Combustion ; Combustion of gaseous fuels ; Combustion. Flame ; Diffusion flames ; Energy ; Energy. Thermal use of fuels ; Exact sciences and technology ; Flame shapes ; Flame structure ; Laminar ; Laminar diffusion flames ; Microgravity ; Nonbuoyant flames ; Soot ; Soot-containing flames ; Space flight ; Space shuttles ; Theoretical studies. Data and constants. Metering</subject><ispartof>Combustion and flame, 2005-07, Vol.142 (1), p.1-16</ispartof><rights>2005 The Combustion Institute</rights><rights>2005 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c302t-9d16694af13cb0d78258b023c287efc41b949e5100832220aaf3b49d2e463023</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=16914754$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Aalburg, C.</creatorcontrib><creatorcontrib>Diez, F.J.</creatorcontrib><creatorcontrib>Faeth, G.M.</creatorcontrib><creatorcontrib>Sunderland, P.B.</creatorcontrib><creatorcontrib>Urban, D.L.</creatorcontrib><creatorcontrib>Yuan, Z.-G.</creatorcontrib><title>Shapes of nonbuoyant round hydrocarbon-fueled laminar-jet diffusion flames in still air</title><title>Combustion and flame</title><description>The soot-luminosity boundaries (near the laminar smoke-point condition) of steady nonbuoyant round hydrocarbon/air laminar-jet diffusion flames at microgravity were found from color video images obtained on orbit during three flights of the Space Shuttle Columbia (flights STS-83, STS-94, and STS-107); these test conditions included ethylene- and propane-fueled flames burning in still air at an ambient temperature of 300 K, ambient pressures of 35–130 kPa, jet exit diameters of 0.40–2.70 mm, and jet exit Reynolds numbers of 46–1186 to yield steady round flames, with most of the flames near the laminar smoke-point condition (including flames both emitting and not emitting soot). These results were supplemented by observations of the flame-sheet locations (locations where the local mixture fraction is stoichiometric) of nonbuoyant round soot-free and soot-containing hydrocarbon/air laminar-jet diffusion flames at microgravity found from filtered color images (at the CH line or
430
±
5
nm
) obtained using a 2.2-s free-fall facility; these test conditions included methane-, ethane-, and propane-fueled flames burning in still air at an ambient temperature of 300 K, ambient pressures of 25–98 kPa, jet exit diameters of 0.42–3.25 mm, and jet exit Reynolds numbers of 10–625. Simplified expressions to estimate soot-luminosity boundaries (near the laminar smoke-point condition) and flame-sheet locations were obtained using the classic analysis of D.B. Spalding (Combustion and Mass Transfer, Pergamon, New York, 1979, p. 185), extended empirically to account for the presence of soot luminosity for flames near the laminar smoke-point condition. The extended Spalding analysis provided good correlations of both soot-luminosity boundaries (near the laminar smoke-point condition) and flame-sheet locations for flames having short characteristic residence times where radiative heat losses from the flames were small. These results showed that soot-luminosity lengths near the laminar smoke-point condition were roughly twice as long as the flame-sheet location for both soot-free (blue) and soot-containing flames under comparable conditions due to the presence of luminous soot particles beyond the flame sheet within the fuel-lean portion of the flames.</description><subject>Applied sciences</subject><subject>Boundaries</subject><subject>Combustion</subject><subject>Combustion of gaseous fuels</subject><subject>Combustion. Flame</subject><subject>Diffusion flames</subject><subject>Energy</subject><subject>Energy. Thermal use of fuels</subject><subject>Exact sciences and technology</subject><subject>Flame shapes</subject><subject>Flame structure</subject><subject>Laminar</subject><subject>Laminar diffusion flames</subject><subject>Microgravity</subject><subject>Nonbuoyant flames</subject><subject>Soot</subject><subject>Soot-containing flames</subject><subject>Space flight</subject><subject>Space shuttles</subject><subject>Theoretical studies. Data and constants. 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Flame</topic><topic>Diffusion flames</topic><topic>Energy</topic><topic>Energy. Thermal use of fuels</topic><topic>Exact sciences and technology</topic><topic>Flame shapes</topic><topic>Flame structure</topic><topic>Laminar</topic><topic>Laminar diffusion flames</topic><topic>Microgravity</topic><topic>Nonbuoyant flames</topic><topic>Soot</topic><topic>Soot-containing flames</topic><topic>Space flight</topic><topic>Space shuttles</topic><topic>Theoretical studies. Data and constants. Metering</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Aalburg, C.</creatorcontrib><creatorcontrib>Diez, F.J.</creatorcontrib><creatorcontrib>Faeth, G.M.</creatorcontrib><creatorcontrib>Sunderland, P.B.</creatorcontrib><creatorcontrib>Urban, D.L.</creatorcontrib><creatorcontrib>Yuan, Z.-G.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Combustion and flame</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Aalburg, C.</au><au>Diez, F.J.</au><au>Faeth, G.M.</au><au>Sunderland, P.B.</au><au>Urban, D.L.</au><au>Yuan, Z.-G.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Shapes of nonbuoyant round hydrocarbon-fueled laminar-jet diffusion flames in still air</atitle><jtitle>Combustion and flame</jtitle><date>2005-07</date><risdate>2005</risdate><volume>142</volume><issue>1</issue><spage>1</spage><epage>16</epage><pages>1-16</pages><issn>0010-2180</issn><eissn>1556-2921</eissn><coden>CBFMAO</coden><abstract>The soot-luminosity boundaries (near the laminar smoke-point condition) of steady nonbuoyant round hydrocarbon/air laminar-jet diffusion flames at microgravity were found from color video images obtained on orbit during three flights of the Space Shuttle Columbia (flights STS-83, STS-94, and STS-107); these test conditions included ethylene- and propane-fueled flames burning in still air at an ambient temperature of 300 K, ambient pressures of 35–130 kPa, jet exit diameters of 0.40–2.70 mm, and jet exit Reynolds numbers of 46–1186 to yield steady round flames, with most of the flames near the laminar smoke-point condition (including flames both emitting and not emitting soot). These results were supplemented by observations of the flame-sheet locations (locations where the local mixture fraction is stoichiometric) of nonbuoyant round soot-free and soot-containing hydrocarbon/air laminar-jet diffusion flames at microgravity found from filtered color images (at the CH line or
430
±
5
nm
) obtained using a 2.2-s free-fall facility; these test conditions included methane-, ethane-, and propane-fueled flames burning in still air at an ambient temperature of 300 K, ambient pressures of 25–98 kPa, jet exit diameters of 0.42–3.25 mm, and jet exit Reynolds numbers of 10–625. Simplified expressions to estimate soot-luminosity boundaries (near the laminar smoke-point condition) and flame-sheet locations were obtained using the classic analysis of D.B. Spalding (Combustion and Mass Transfer, Pergamon, New York, 1979, p. 185), extended empirically to account for the presence of soot luminosity for flames near the laminar smoke-point condition. The extended Spalding analysis provided good correlations of both soot-luminosity boundaries (near the laminar smoke-point condition) and flame-sheet locations for flames having short characteristic residence times where radiative heat losses from the flames were small. These results showed that soot-luminosity lengths near the laminar smoke-point condition were roughly twice as long as the flame-sheet location for both soot-free (blue) and soot-containing flames under comparable conditions due to the presence of luminous soot particles beyond the flame sheet within the fuel-lean portion of the flames.</abstract><cop>New York, NY</cop><pub>Elsevier Inc</pub><doi>10.1016/j.combustflame.2004.12.009</doi><tpages>16</tpages></addata></record> |
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subjects | Applied sciences Boundaries Combustion Combustion of gaseous fuels Combustion. Flame Diffusion flames Energy Energy. Thermal use of fuels Exact sciences and technology Flame shapes Flame structure Laminar Laminar diffusion flames Microgravity Nonbuoyant flames Soot Soot-containing flames Space flight Space shuttles Theoretical studies. Data and constants. Metering |
title | Shapes of nonbuoyant round hydrocarbon-fueled laminar-jet diffusion flames in still air |
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