Simultaneous CH-OHPLIF and stereoscopic PIV measurements of turbulent premixed flames

被引:85
作者
Tanahashi, M
Murakami, S
Choi, GM
Fukuchi, Y
Miyauchi, T
机构
[1] Tokyo Inst Technol, Dept Mech & Aerosp Engn, Meguro Ku, Tokyo 1528552, Japan
[2] Pusan Natl Univ, Coll Engn, Sch Mech Engn, Pusan 609735, South Korea
基金
日本学术振兴会;
关键词
laser diagnostics; simultaneous PLIF/PIV; stereoscopic PIV; simultaneous CH-OHPLIF; turbulent premixed flames;
D O I
10.1016/j.proci.2004.08.270
中图分类号
O414.1 [热力学];
学科分类号
摘要
Simultaneous CH and OH planar laser-induced fluorescence (PLIF) and stereoscopic particle image velocimetry (PIV) measurement have been developed to investigate the local flame structure of turbulent premixed flames. In this system, high-speed CMOS cameras were adopted to capture clear stereoscopic particle images without contamination by the flame radiation. The effects of scattering of CH PLIF laser by tracer particles are carefully investigated to improve signal-to-noise ratio in CH fluorescence images. The developed simultaneous two radical concentrations and three-component velocity measurement on a two-dimensional plane was applied to relatively high Reynolds number turbulent premixed flames in a swirl-stabilized combustor. All measurements were conducted for methane-air premixed flames in the corrugated flamelet regime. Simultaneous CH and OH images suggest the presence of the isolated burned gas in the unburned mixture and the isolated unburned mixture in the burned side, which have been predicted by direct numerical simulations. Detailed analysis of simultaneous CH and OH images reveals that the minimum curvature radius of the flame front coincides with the Kolmogorov scale. Strong three-dimensional velocity fluctuations, which are measured by the stereoscopic PIV, imply that misunderstanding of the flame/turbulence interactions would be caused by the analysis of two-component velocity distributions in a cross-section. Furthermore, comparisons of CH-OH PLIF and three-component velocity fields show that the burned gases do not always have high-speed velocity in a relatively high Reynolds number turbulent premixed flame. The Reynolds number dependence of the flame front was clearly captured by the simultaneous CH-OH PLIF and stereoscopic PIV measurements. (c) 2004 Published by Elsevier Inc. on behalf of The Combustion Institute.
引用
收藏
页码:1665 / 1672
页数:8
相关论文
共 34 条
[1]   DIGITAL IMAGING OF REACTION ZONES IN HYDROCARBON AIR FLAMES USING PLANAR LASER-INDUCED FLUORESCENCE OF CH AND C-2 [J].
ALLEN, MG ;
HOWE, RD ;
HANSON, RK .
OPTICS LETTERS, 1986, 11 (03) :126-128
[2]   STEREOSCOPIC PARTICLE IMAGE VELOCIMETRY [J].
ARROYO, MP ;
GREATED, CA .
MEASUREMENT SCIENCE AND TECHNOLOGY, 1991, 2 (12) :1181-1186
[3]   Numerical simulation of premixed turbulent methane combustion [J].
Bell, JB ;
Day, MS ;
Grcar, JF .
PROCEEDINGS OF THE COMBUSTION INSTITUTE, 2002, 29 (02) :1987-1993
[4]  
Böckle S, 2000, P COMBUST INST, V28, P279
[5]   Simultaneous CH planar laser-induced fluorescence and particle imaging velocimetry in turbulent nonpremixed flames [J].
Carter, CD ;
Donbar, JM ;
Driscoll, JF .
APPLIED PHYSICS B-LASERS AND OPTICS, 1998, 66 (01) :129-132
[6]   The mechanism of two-dimensional pocket formation in lean premixed methane-air flames with implications to turbulent combustion [J].
Chen, JH ;
Echekki, T .
COMBUSTION AND FLAME, 1999, 116 (1-2) :15-+
[7]   Reaction zone structure in turbulent nonpremixed jet flames - From CH-OHPLIF images [J].
Donbar, JM ;
Driscoll, JF ;
Carter, CD .
COMBUSTION AND FLAME, 2000, 122 (1-2) :1-19
[8]  
DYER MJ, 1985, P INT C LASER, V84, P211
[9]   ENERGY-TRANSFER PROCESSES IN CH A2-DELTA AND B2-SIGMA- IN AN ATMOSPHERIC-PRESSURE FLAME [J].
GARLAND, NL ;
CROSLEY, DR .
APPLIED OPTICS, 1985, 24 (23) :4229-4237
[10]   Simultaneous measurement of velocity and CH layer distribution in turbulent non-premixed flames [J].
Han, DH ;
Mungal, MG .
PROCEEDINGS OF THE COMBUSTION INSTITUTE, 2000, 28 :261-267