Consumption rate characteristics of a fine-scale unburnt mixture in a turbulent jet premixed flame by high repetition rate PLIF and SPIV
A 10 kHz simultaneous measurement of OH-CH planar laser induced fluorescence (PLIF) and stereoscopic particle image velocimetry (SPIV) is applied to a methane-air turbulent jet premixed flame. The measurement of the flame tip for high Reynolds number conditions shows that isolated fine-scale unburnt...
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The Japan Society of Mechanical Engineers
2016-12-01
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Series: | Journal of Thermal Science and Technology |
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Online Access: | https://www.jstage.jst.go.jp/article/jtst/11/3/11_2016jtst0047/_pdf/-char/en |
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author | Masayasu SHIMURA Ayane JOHCHI Mamoru TANAHASHI |
author_facet | Masayasu SHIMURA Ayane JOHCHI Mamoru TANAHASHI |
author_sort | Masayasu SHIMURA |
collection | DOAJ |
description | A 10 kHz simultaneous measurement of OH-CH planar laser induced fluorescence (PLIF) and stereoscopic particle image velocimetry (SPIV) is applied to a methane-air turbulent jet premixed flame. The measurement of the flame tip for high Reynolds number conditions shows that isolated fine-scale unburnt mixtures, so-called unburnt mixture islands or reactant pockets, are frequently generated. POD analysis shows that the separation of unburnt mixture from the upstream main reactants is the characteristic flame structure. In our previous study (Johchi et al. 2015), the consumption rates of isolated unburnt mixtures are estimated from changes of area of unburnt region detected in OH and CH PLIF images under the assumptions that the isolated unburnt mixtures are spherical and pillar shapes. The most expected consumption rate conditioned by curvature of flame front is about 0.71 m/s, which is much higher than the laminar burning velocity of the corresponding reactants. The consumption rate increases with the decrease of the radius of the isolated reactants. The reason that the consumption rates of the fine-scale isolated unburnt mixtures are much higher than the laminar burning velocity is discussed based on heat conduction in the isolated unburnt mixture by assuming that the heat release from mass difference between going out and coming in the preheat zone increases the mean temperature of remained reactants to consider enhancement of the effect of heat conduction. From the analysis, characteristic scale of fine-scale unburnt mixture in which heat conduction effect is significant is discussed. |
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issn | 1880-5566 |
language | English |
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publishDate | 2016-12-01 |
publisher | The Japan Society of Mechanical Engineers |
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spelling | doaj.art-811048e823d84337aea42b54679b15ef2022-12-22T00:05:16ZengThe Japan Society of Mechanical EngineersJournal of Thermal Science and Technology1880-55662016-12-01113JTST0047JTST004710.1299/jtst.2016jtst0047jtstConsumption rate characteristics of a fine-scale unburnt mixture in a turbulent jet premixed flame by high repetition rate PLIF and SPIVMasayasu SHIMURA0Ayane JOHCHI1Mamoru TANAHASHI2Department of Mechanical Engineering, Tokyo Institute of TechnologyDepartment of Mechanical Engineering, Tokyo Institute of TechnologyDepartment of Mechanical Engineering, Tokyo Institute of TechnologyA 10 kHz simultaneous measurement of OH-CH planar laser induced fluorescence (PLIF) and stereoscopic particle image velocimetry (SPIV) is applied to a methane-air turbulent jet premixed flame. The measurement of the flame tip for high Reynolds number conditions shows that isolated fine-scale unburnt mixtures, so-called unburnt mixture islands or reactant pockets, are frequently generated. POD analysis shows that the separation of unburnt mixture from the upstream main reactants is the characteristic flame structure. In our previous study (Johchi et al. 2015), the consumption rates of isolated unburnt mixtures are estimated from changes of area of unburnt region detected in OH and CH PLIF images under the assumptions that the isolated unburnt mixtures are spherical and pillar shapes. The most expected consumption rate conditioned by curvature of flame front is about 0.71 m/s, which is much higher than the laminar burning velocity of the corresponding reactants. The consumption rate increases with the decrease of the radius of the isolated reactants. The reason that the consumption rates of the fine-scale isolated unburnt mixtures are much higher than the laminar burning velocity is discussed based on heat conduction in the isolated unburnt mixture by assuming that the heat release from mass difference between going out and coming in the preheat zone increases the mean temperature of remained reactants to consider enhancement of the effect of heat conduction. From the analysis, characteristic scale of fine-scale unburnt mixture in which heat conduction effect is significant is discussed.https://www.jstage.jst.go.jp/article/jtst/11/3/11_2016jtst0047/_pdf/-char/enfuel consumption rateturbulent premixed flamereactant pockethigh repetition rate plif and piv |
spellingShingle | Masayasu SHIMURA Ayane JOHCHI Mamoru TANAHASHI Consumption rate characteristics of a fine-scale unburnt mixture in a turbulent jet premixed flame by high repetition rate PLIF and SPIV Journal of Thermal Science and Technology fuel consumption rate turbulent premixed flame reactant pocket high repetition rate plif and piv |
title | Consumption rate characteristics of a fine-scale unburnt mixture in a turbulent jet premixed flame by high repetition rate PLIF and SPIV |
title_full | Consumption rate characteristics of a fine-scale unburnt mixture in a turbulent jet premixed flame by high repetition rate PLIF and SPIV |
title_fullStr | Consumption rate characteristics of a fine-scale unburnt mixture in a turbulent jet premixed flame by high repetition rate PLIF and SPIV |
title_full_unstemmed | Consumption rate characteristics of a fine-scale unburnt mixture in a turbulent jet premixed flame by high repetition rate PLIF and SPIV |
title_short | Consumption rate characteristics of a fine-scale unburnt mixture in a turbulent jet premixed flame by high repetition rate PLIF and SPIV |
title_sort | consumption rate characteristics of a fine scale unburnt mixture in a turbulent jet premixed flame by high repetition rate plif and spiv |
topic | fuel consumption rate turbulent premixed flame reactant pocket high repetition rate plif and piv |
url | https://www.jstage.jst.go.jp/article/jtst/11/3/11_2016jtst0047/_pdf/-char/en |
work_keys_str_mv | AT masayasushimura consumptionratecharacteristicsofafinescaleunburntmixtureinaturbulentjetpremixedflamebyhighrepetitionrateplifandspiv AT ayanejohchi consumptionratecharacteristicsofafinescaleunburntmixtureinaturbulentjetpremixedflamebyhighrepetitionrateplifandspiv AT mamorutanahashi consumptionratecharacteristicsofafinescaleunburntmixtureinaturbulentjetpremixedflamebyhighrepetitionrateplifandspiv |