Extinction and structure of ultra lean premixed flame formed in opposite flow

Yuji Yahagi, Masao Takeuchi

研究成果: Article

2 引用 (Scopus)

抄録

Extinction and structure of ultra lean premixed flame formed in opposite flow has been studied experimentally. Two different concentration mixtures, extremely lean premixed gas and lean premixed gas, impinged on each other. The bulk stretch rate were varied from 80-s to 270-s, and the Lewis number (Le) were varied from 0.99 to 1.85. The local stretch rate due to flow divergence and the stagnation point were estimated by measuring the centerline velocity profile with LDV and the reaction zone was identified by OH profiles using PLIF (Planar Laser-Induced Fluorescence). The extinction behavior depends on the mixture property and the flow strain rate. For small strain rate and Le>1, the extinction limit is nearly constant regardless'of super lean premixed gas condition. On the other hand, for Le<1 and the strain rate large, ultra lean premixed gas interacts with lean premixed gas and the stable region extends to the lower fuel concentration zone.

元の言語English
ページ(範囲)1108-1114
ページ数7
ジャーナルNihon Kikai Gakkai Ronbunshu, B Hen/Transactions of the Japan Society of Mechanical Engineers, Part B
65
発行部数631
出版物ステータスPublished - 1999
外部発表Yes

Fingerprint

premixed flames
extinction
strain rate
Strain rate
Gases
gases
Lewis numbers
stagnation point
laser induced fluorescence
divergence
flow velocity
velocity distribution
Fluorescence
Lasers
profiles

ASJC Scopus subject areas

  • Mechanical Engineering
  • Condensed Matter Physics

これを引用

@article{89affad6eaba4e7ebb3893ebd2ff01f7,
title = "Extinction and structure of ultra lean premixed flame formed in opposite flow",
abstract = "Extinction and structure of ultra lean premixed flame formed in opposite flow has been studied experimentally. Two different concentration mixtures, extremely lean premixed gas and lean premixed gas, impinged on each other. The bulk stretch rate were varied from 80-s to 270-s, and the Lewis number (Le) were varied from 0.99 to 1.85. The local stretch rate due to flow divergence and the stagnation point were estimated by measuring the centerline velocity profile with LDV and the reaction zone was identified by OH profiles using PLIF (Planar Laser-Induced Fluorescence). The extinction behavior depends on the mixture property and the flow strain rate. For small strain rate and Le>1, the extinction limit is nearly constant regardless'of super lean premixed gas condition. On the other hand, for Le<1 and the strain rate large, ultra lean premixed gas interacts with lean premixed gas and the stable region extends to the lower fuel concentration zone.",
keywords = "Combustion phenomena, Extinction, Heat loss, Internal combustion engine, Lewis number, Opposite flow, Premixed combustion, Ultra lean combustion",
author = "Yuji Yahagi and Masao Takeuchi",
year = "1999",
language = "English",
volume = "65",
pages = "1108--1114",
journal = "Nihon Kikai Gakkai Ronbunshu, B Hen/Transactions of the Japan Society of Mechanical Engineers, Part B",
issn = "0387-5016",
publisher = "Japan Society of Mechanical Engineers",
number = "631",

}

TY - JOUR

T1 - Extinction and structure of ultra lean premixed flame formed in opposite flow

AU - Yahagi, Yuji

AU - Takeuchi, Masao

PY - 1999

Y1 - 1999

N2 - Extinction and structure of ultra lean premixed flame formed in opposite flow has been studied experimentally. Two different concentration mixtures, extremely lean premixed gas and lean premixed gas, impinged on each other. The bulk stretch rate were varied from 80-s to 270-s, and the Lewis number (Le) were varied from 0.99 to 1.85. The local stretch rate due to flow divergence and the stagnation point were estimated by measuring the centerline velocity profile with LDV and the reaction zone was identified by OH profiles using PLIF (Planar Laser-Induced Fluorescence). The extinction behavior depends on the mixture property and the flow strain rate. For small strain rate and Le>1, the extinction limit is nearly constant regardless'of super lean premixed gas condition. On the other hand, for Le<1 and the strain rate large, ultra lean premixed gas interacts with lean premixed gas and the stable region extends to the lower fuel concentration zone.

AB - Extinction and structure of ultra lean premixed flame formed in opposite flow has been studied experimentally. Two different concentration mixtures, extremely lean premixed gas and lean premixed gas, impinged on each other. The bulk stretch rate were varied from 80-s to 270-s, and the Lewis number (Le) were varied from 0.99 to 1.85. The local stretch rate due to flow divergence and the stagnation point were estimated by measuring the centerline velocity profile with LDV and the reaction zone was identified by OH profiles using PLIF (Planar Laser-Induced Fluorescence). The extinction behavior depends on the mixture property and the flow strain rate. For small strain rate and Le>1, the extinction limit is nearly constant regardless'of super lean premixed gas condition. On the other hand, for Le<1 and the strain rate large, ultra lean premixed gas interacts with lean premixed gas and the stable region extends to the lower fuel concentration zone.

KW - Combustion phenomena

KW - Extinction

KW - Heat loss

KW - Internal combustion engine

KW - Lewis number

KW - Opposite flow

KW - Premixed combustion

KW - Ultra lean combustion

UR - http://www.scopus.com/inward/record.url?scp=2142707643&partnerID=8YFLogxK

UR - http://www.scopus.com/inward/citedby.url?scp=2142707643&partnerID=8YFLogxK

M3 - Article

AN - SCOPUS:2142707643

VL - 65

SP - 1108

EP - 1114

JO - Nihon Kikai Gakkai Ronbunshu, B Hen/Transactions of the Japan Society of Mechanical Engineers, Part B

JF - Nihon Kikai Gakkai Ronbunshu, B Hen/Transactions of the Japan Society of Mechanical Engineers, Part B

SN - 0387-5016

IS - 631

ER -