Extinction of laminar, premixed, counter-flow methane/air flames under unsteady conditions: Effect of H2 addition

被引:21
作者
Cuoci, A. [1 ]
Frassoldati, A. [1 ]
Faravelli, T. [1 ]
Ranzi, E. [1 ]
机构
[1] Politecn Milan, Dipartimento Chim Mat & Ingn Chim G Natta, I-20133 Milan, Italy
关键词
Combustion; Mathematical modeling; Kinetics; Laminar flow; Unsteady flame; Flame extinction; DIFFUSION FLAMES; STRAIN-RATE; HYDROCARBON; COMBUSTION; LIMITS; FUELS;
D O I
10.1016/j.ces.2013.02.009
中图分类号
TQ [化学工业];
学科分类号
0817 ;
摘要
In this paper the extinction of laminar, premixed flames fed with a mixture of methane and hydrogen is numerically modeled in unsteady conditions. The aim of the work is to better understand how the oscillations of the flow field and the addition of hydrogen to the fuel mixture affect the extinction limits of the flame. For this purpose, numerical simulations of laminar, premixed, symmetric counter-flow flames were performed using a detailed kinetic mechanism (similar to 80 species and 1400 reactions). Steady-state conditions were first analyzed and the numerical results were compared with the experimental measurements with satisfactory agreement, showing that the main effect of hydrogen addition is to increase the characteristic extinction limits of the flame. Then, harmonic oscillations were imposed on the inlet velocities, in order to study the response of the flame (in terms of temperature and species) to the unsteadiness of the flow field. The results clearly showed that, as long as the averaged strain rate is smaller than the steady state strain rate, the oscillating flames can always survive instantaneous high strain rates for sufficiently high frequencies. Moreover, the unsteady flames are able to survive to instantaneous strain rates well beyond the corresponding steady-state extinction conditions, especially when the frequency of oscillations is large. Eventually, it was found that the flame behavior under unsteady conditions can be effectively explained using the Stokes' number (i.e. the ratio between the frequency of imposed oscillations and the strain rate of the flame), a dimensionless parameter comparing the characteristic times of the flame and of the imposed disturbances. (C) 2013 Elsevier Ltd. All rights reserved.
引用
收藏
页码:266 / 276
页数:11
相关论文
共 33 条
[1]  
[Anonymous], P COMBUST I
[2]  
Barlow R., 1992, Symposium (International) on Combustion, V24, P231
[3]   Frequency response of counter flow diffusion flames to strain rate harmonic oscillations [J].
Cuoci, A. ;
Frassoldati, A. ;
Faravelli, T. ;
Ranzi, E. .
COMBUSTION SCIENCE AND TECHNOLOGY, 2008, 180 (05) :767-784
[4]   Formation of soot and nitrogen oxides in unsteady counterflow diffusion flames [J].
Cuoci, A. ;
Frassoldati, A. ;
Faravelli, T. ;
Ranzi, E. .
COMBUSTION AND FLAME, 2009, 156 (10) :2010-2022
[5]   Soot formation in unsteady counterflow diffusion flames [J].
Cuoci, A. ;
Frassoldati, A. ;
Faravelli, T. ;
Ranzi, E. .
PROCEEDINGS OF THE COMBUSTION INSTITUTE, 2009, 32 :1335-1342
[6]  
Cuoci A., COMBUST FLA IN PRESS
[7]   THE EFFECT OF STRAIN RATE ON A PREMIXED LAMINAR FLAME [J].
DARABIHA, N ;
CANDEL, SM ;
MARBLE, FE .
COMBUSTION AND FLAME, 1986, 64 (02) :203-217
[8]   Study of transient effects on the extinction limits of an unsteady counterflow diffusion flame [J].
Decroix, ME ;
Roberts, WL .
COMBUSTION SCIENCE AND TECHNOLOGY, 1999, 146 (1-6) :57-84
[9]   Transient flow field effects on soot volume fraction in diffusion flames [J].
Decroix, ME ;
Roberts, WL .
COMBUSTION SCIENCE AND TECHNOLOGY, 2000, 160 (1-6) :165-189
[10]   Unsteady counterflowing strained diffusion flames: Diffusion-limited frequency response [J].
Egolfopoulos, FN ;
Campbell, CS .
JOURNAL OF FLUID MECHANICS, 1996, 318 :1-29