The diffusive-thermal instability of premixed flames with low unburned-gas temperature under the adiabatic and non-adiabatic conditions

We elucidated the diffusive-thermal instability of premixed flames with low unburned-gas temperature under the adiabatic and non-adiabatic conditions. Numerical calculations of two-dimensional unsteady reactive flows were performed, based on the diffusive-thermal model equation. Lewis numbers smalle...

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Autores principales: Thwe Thwe AUNG, Satoshi KADOWAKI
Formato: article
Lenguaje:EN
Publicado: The Japan Society of Mechanical Engineers 2015
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spelling oai:doaj.org-article:25a6fc9787d249c0a54a86e45db32cbe2021-11-26T06:30:10ZThe diffusive-thermal instability of premixed flames with low unburned-gas temperature under the adiabatic and non-adiabatic conditions2187-974510.1299/mej.14-00460https://doaj.org/article/25a6fc9787d249c0a54a86e45db32cbe2015-09-01T00:00:00Zhttps://www.jstage.jst.go.jp/article/mej/2/5/2_14-00460/_pdf/-char/enhttps://doaj.org/toc/2187-9745We elucidated the diffusive-thermal instability of premixed flames with low unburned-gas temperature under the adiabatic and non-adiabatic conditions. Numerical calculations of two-dimensional unsteady reactive flows were performed, based on the diffusive-thermal model equation. Lewis numbers smaller than unity were adopted, and radiative heat loss was treated. As the unburned-gas temperature became lower, the growth rate decreased and the unstable range narrowed, which was due to the decrease of the burning velocity of a planar flame. As for the growth rate and unstable range normalized by the burning velocity of a planar flame, the former increased and the latter widened. This was due to the enlargement of Zeldovich numbers. Taking account of radiative heat loss, the normalized growth rate was large and the normalized unstable range was wide. This indicated that the heat loss had a pronounced influence on the diffusive-thermal instability of premixed flames with low unburned-gas temperature. Moreover, the cellular-shape flame fronts formed owing to diffusive-thermal instability. The burning velocity of a cellular flame normalized by that of a planar flame increased as the unburned-gas temperature became lower and the heat loss became greater. This was because of the enlargement of Zeldovich numbers and the pronounced influence of heat loss.Thwe Thwe AUNGSatoshi KADOWAKIThe Japan Society of Mechanical Engineersarticlepremixed flamediffusive-thermal instabilitylow temperatureheat losszeldovich numbercellular flameMechanical engineering and machineryTJ1-1570ENMechanical Engineering Journal, Vol 2, Iss 5, Pp 14-00460-14-00460 (2015)
institution DOAJ
collection DOAJ
language EN
topic premixed flame
diffusive-thermal instability
low temperature
heat loss
zeldovich number
cellular flame
Mechanical engineering and machinery
TJ1-1570
spellingShingle premixed flame
diffusive-thermal instability
low temperature
heat loss
zeldovich number
cellular flame
Mechanical engineering and machinery
TJ1-1570
Thwe Thwe AUNG
Satoshi KADOWAKI
The diffusive-thermal instability of premixed flames with low unburned-gas temperature under the adiabatic and non-adiabatic conditions
description We elucidated the diffusive-thermal instability of premixed flames with low unburned-gas temperature under the adiabatic and non-adiabatic conditions. Numerical calculations of two-dimensional unsteady reactive flows were performed, based on the diffusive-thermal model equation. Lewis numbers smaller than unity were adopted, and radiative heat loss was treated. As the unburned-gas temperature became lower, the growth rate decreased and the unstable range narrowed, which was due to the decrease of the burning velocity of a planar flame. As for the growth rate and unstable range normalized by the burning velocity of a planar flame, the former increased and the latter widened. This was due to the enlargement of Zeldovich numbers. Taking account of radiative heat loss, the normalized growth rate was large and the normalized unstable range was wide. This indicated that the heat loss had a pronounced influence on the diffusive-thermal instability of premixed flames with low unburned-gas temperature. Moreover, the cellular-shape flame fronts formed owing to diffusive-thermal instability. The burning velocity of a cellular flame normalized by that of a planar flame increased as the unburned-gas temperature became lower and the heat loss became greater. This was because of the enlargement of Zeldovich numbers and the pronounced influence of heat loss.
format article
author Thwe Thwe AUNG
Satoshi KADOWAKI
author_facet Thwe Thwe AUNG
Satoshi KADOWAKI
author_sort Thwe Thwe AUNG
title The diffusive-thermal instability of premixed flames with low unburned-gas temperature under the adiabatic and non-adiabatic conditions
title_short The diffusive-thermal instability of premixed flames with low unburned-gas temperature under the adiabatic and non-adiabatic conditions
title_full The diffusive-thermal instability of premixed flames with low unburned-gas temperature under the adiabatic and non-adiabatic conditions
title_fullStr The diffusive-thermal instability of premixed flames with low unburned-gas temperature under the adiabatic and non-adiabatic conditions
title_full_unstemmed The diffusive-thermal instability of premixed flames with low unburned-gas temperature under the adiabatic and non-adiabatic conditions
title_sort diffusive-thermal instability of premixed flames with low unburned-gas temperature under the adiabatic and non-adiabatic conditions
publisher The Japan Society of Mechanical Engineers
publishDate 2015
url https://doaj.org/article/25a6fc9787d249c0a54a86e45db32cbe
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