Fast-flame limit for hydrogen/methane-air mixtures
Autor(a) principal: | |
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Data de Publicação: | 2019 |
Outros Autores: | , , , |
Tipo de documento: | Artigo |
Idioma: | eng |
Título da fonte: | Repositório Institucional da UNESP |
Texto Completo: | http://dx.doi.org/10.1016/j.proci.2018.06.045 http://hdl.handle.net/11449/184293 |
Resumo: | Flame acceleration experiments were performed in a 10cm inner-diameter tube filled with evenly spaced 0.43 blockage ratio orifice plates. The critical mixture composition required for flame acceleration to a fast-flame was measured for four methane/hydrogen fuel-air mixtures at initial temperatures of 298 K, 423 K, and 573 K. These conditions provide a large range in the Zeldovich number between 12 and 28, where the Zeldovich number was calculated from the laminar burning velocity obtained from 1-D flame simulations. The data collapsed very well when the expansion ratio across the flame (calculated at the critical condition) was plotted versus the Zeldovich number. This is consistent with correlation proposed by Dorofeev [7], that was based on experimental data obtained over a narrower Zeldovich number range. For pure hydrogen fuel, the critical expansion ratio was found to be between 2 and 4, and for pure methane the critical expansion ratio was as high as 8, for an initial temperature of 573 K. (C) 2018 The Combustion Institute. Published by Elsevier Inc. All rights reserved. |
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Fast-flame limit for hydrogen/methane-air mixturesFast-flameFlame acceleration criterionHydrogenMethaneFlame acceleration experiments were performed in a 10cm inner-diameter tube filled with evenly spaced 0.43 blockage ratio orifice plates. The critical mixture composition required for flame acceleration to a fast-flame was measured for four methane/hydrogen fuel-air mixtures at initial temperatures of 298 K, 423 K, and 573 K. These conditions provide a large range in the Zeldovich number between 12 and 28, where the Zeldovich number was calculated from the laminar burning velocity obtained from 1-D flame simulations. The data collapsed very well when the expansion ratio across the flame (calculated at the critical condition) was plotted versus the Zeldovich number. This is consistent with correlation proposed by Dorofeev [7], that was based on experimental data obtained over a narrower Zeldovich number range. For pure hydrogen fuel, the critical expansion ratio was found to be between 2 and 4, and for pure methane the critical expansion ratio was as high as 8, for an initial temperature of 573 K. (C) 2018 The Combustion Institute. Published by Elsevier Inc. All rights reserved.Solar TurbinesFundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)Queens Univ, Kingston, ON, CanadaCNRS, INSIS, ICARE, Paris, FranceSao Paulo State Univ, Sao Paulo, BrazilSao Paulo State Univ, Sao Paulo, BrazilFAPESP: 2015/23351-9FAPESP: 2015/25435-5Elsevier B.V.Queens UnivCNRSUniversidade Estadual Paulista (Unesp)Ciccarelli, G.Chaumeix, N.Mendiburu, A. Z. [UNESP]N'Guessan, K.Comandini, A.2019-10-04T11:56:28Z2019-10-04T11:56:28Z2019-01-01info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/article3661-3668http://dx.doi.org/10.1016/j.proci.2018.06.045Proceedings Of The Combustion Institute. New York: Elsevier Science Inc, v. 37, n. 3, p. 3661-3668, 2019.1540-7489http://hdl.handle.net/11449/18429310.1016/j.proci.2018.06.045WOS:000456628600116Web of Sciencereponame:Repositório Institucional da UNESPinstname:Universidade Estadual Paulista (UNESP)instacron:UNESPengProceedings Of The Combustion Instituteinfo:eu-repo/semantics/openAccess2021-10-23T04:16:27Zoai:repositorio.unesp.br:11449/184293Repositório InstitucionalPUBhttp://repositorio.unesp.br/oai/requestopendoar:29462024-08-05T13:31:47.353790Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP)false |
dc.title.none.fl_str_mv |
Fast-flame limit for hydrogen/methane-air mixtures |
title |
Fast-flame limit for hydrogen/methane-air mixtures |
spellingShingle |
Fast-flame limit for hydrogen/methane-air mixtures Ciccarelli, G. Fast-flame Flame acceleration criterion Hydrogen Methane |
title_short |
Fast-flame limit for hydrogen/methane-air mixtures |
title_full |
Fast-flame limit for hydrogen/methane-air mixtures |
title_fullStr |
Fast-flame limit for hydrogen/methane-air mixtures |
title_full_unstemmed |
Fast-flame limit for hydrogen/methane-air mixtures |
title_sort |
Fast-flame limit for hydrogen/methane-air mixtures |
author |
Ciccarelli, G. |
author_facet |
Ciccarelli, G. Chaumeix, N. Mendiburu, A. Z. [UNESP] N'Guessan, K. Comandini, A. |
author_role |
author |
author2 |
Chaumeix, N. Mendiburu, A. Z. [UNESP] N'Guessan, K. Comandini, A. |
author2_role |
author author author author |
dc.contributor.none.fl_str_mv |
Queens Univ CNRS Universidade Estadual Paulista (Unesp) |
dc.contributor.author.fl_str_mv |
Ciccarelli, G. Chaumeix, N. Mendiburu, A. Z. [UNESP] N'Guessan, K. Comandini, A. |
dc.subject.por.fl_str_mv |
Fast-flame Flame acceleration criterion Hydrogen Methane |
topic |
Fast-flame Flame acceleration criterion Hydrogen Methane |
description |
Flame acceleration experiments were performed in a 10cm inner-diameter tube filled with evenly spaced 0.43 blockage ratio orifice plates. The critical mixture composition required for flame acceleration to a fast-flame was measured for four methane/hydrogen fuel-air mixtures at initial temperatures of 298 K, 423 K, and 573 K. These conditions provide a large range in the Zeldovich number between 12 and 28, where the Zeldovich number was calculated from the laminar burning velocity obtained from 1-D flame simulations. The data collapsed very well when the expansion ratio across the flame (calculated at the critical condition) was plotted versus the Zeldovich number. This is consistent with correlation proposed by Dorofeev [7], that was based on experimental data obtained over a narrower Zeldovich number range. For pure hydrogen fuel, the critical expansion ratio was found to be between 2 and 4, and for pure methane the critical expansion ratio was as high as 8, for an initial temperature of 573 K. (C) 2018 The Combustion Institute. Published by Elsevier Inc. All rights reserved. |
publishDate |
2019 |
dc.date.none.fl_str_mv |
2019-10-04T11:56:28Z 2019-10-04T11:56:28Z 2019-01-01 |
dc.type.status.fl_str_mv |
info:eu-repo/semantics/publishedVersion |
dc.type.driver.fl_str_mv |
info:eu-repo/semantics/article |
format |
article |
status_str |
publishedVersion |
dc.identifier.uri.fl_str_mv |
http://dx.doi.org/10.1016/j.proci.2018.06.045 Proceedings Of The Combustion Institute. New York: Elsevier Science Inc, v. 37, n. 3, p. 3661-3668, 2019. 1540-7489 http://hdl.handle.net/11449/184293 10.1016/j.proci.2018.06.045 WOS:000456628600116 |
url |
http://dx.doi.org/10.1016/j.proci.2018.06.045 http://hdl.handle.net/11449/184293 |
identifier_str_mv |
Proceedings Of The Combustion Institute. New York: Elsevier Science Inc, v. 37, n. 3, p. 3661-3668, 2019. 1540-7489 10.1016/j.proci.2018.06.045 WOS:000456628600116 |
dc.language.iso.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
Proceedings Of The Combustion Institute |
dc.rights.driver.fl_str_mv |
info:eu-repo/semantics/openAccess |
eu_rights_str_mv |
openAccess |
dc.format.none.fl_str_mv |
3661-3668 |
dc.publisher.none.fl_str_mv |
Elsevier B.V. |
publisher.none.fl_str_mv |
Elsevier B.V. |
dc.source.none.fl_str_mv |
Web of Science reponame:Repositório Institucional da UNESP instname:Universidade Estadual Paulista (UNESP) instacron:UNESP |
instname_str |
Universidade Estadual Paulista (UNESP) |
instacron_str |
UNESP |
institution |
UNESP |
reponame_str |
Repositório Institucional da UNESP |
collection |
Repositório Institucional da UNESP |
repository.name.fl_str_mv |
Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP) |
repository.mail.fl_str_mv |
|
_version_ |
1808128243153240064 |