Soot structure and flow characteristics in turbulent non-premixed methane flames stabilised on a bluff-body

被引:3
作者
Rowhani, Amir [1 ]
Sun, Zhiwei [1 ]
Chinnici, Alfonso [1 ]
Medwell, Paul R. [1 ]
Nathan, Graham J. [1 ]
Dally, Bassam B. [2 ]
机构
[1] Univ Adelaide, Sch Mech Engn, Adelaide, SA 5005, Australia
[2] King Abdullah Univ Sci & Technol KAUST, Clean Combust Res Ctr CCRC, Thuwal 239556900, Saudi Arabia
基金
澳大利亚研究理事会;
关键词
Soot; Methane; Bluff-body; LII; PIV; SIMULTANEOUS PLANAR MEASUREMENTS; LASER-INDUCED INCANDESCENCE; VOLUME FRACTION; DIFFUSION FLAMES; JET; TEMPERATURE; EVOLUTION; BEHAVIOR; FIELDS;
D O I
10.1016/j.fuel.2023.128118
中图分类号
TE [石油、天然气工业]; TK [能源与动力工程];
学科分类号
0807 ; 0820 ;
摘要
The soot properties of methane in turbulent regimes are not well characterised but are highly desirable. Methane is the main constituent of natural gas that is broadly used in many industrial combustors. Investigation of turbulent methane flames under well-defined boundary conditions is therefore useful for interpreting soot formation in practical burners and can be used for further model development. This study presents a joint experimental and numerical study of a series of turbulent non-premixed bluff-body flames fuelled with pure methane for three values of the momentum flux ratio of fuel jet to co-flowing air. Soot volume fraction (SVF) and flowfield are measured simultaneously using planar laser-induced incandescence (P-LII) and 2D-polarised particle image velocimetry (P-PIV). Additionally, time-averaged temperature, mixture fraction, OH and C2H2 concentrations are estimated numerically using RANS models. The global flame structure for all three flames features a recirculation zone with a double-vortex structure, a jet-propagating zone, and a neck zone connecting the two regions. The soot distribution within the recirculation zone shows clear distinct features, which is attributed to the mean mixture fraction distribution in this zone. Increasing the momentum flux ratio shifts the location of the mean stoichiometric mixture fraction to the rich inner vortex core, leading to a distinct peak of the total integrated soot in the inner vortex of the recirculation zone that is not observed in other cases. Also, it is deduced that the soot inception starts earlier in the recirculation zone for the flame with the highest momentum flux ratio and in the jet zone for the other two flames. Much higher soot concentration and lower intermittency are found with ethylenebased flames stabilised on the same burner and with the same operating conditions. In addition, the study has generated a database of soot and flowfield results, which can be helpful for future model validations.
引用
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页数:10
相关论文
共 43 条
[1]  
Agosta A, GLOBAL GAS OUTLOOK 2
[2]  
[Anonymous], 2021, INT SOOT FLAM ISF WO
[3]  
Ansys fluent, ANSYS FLUENT RELEASE
[4]   EFFECT OF MOLECULAR-STRUCTURE ON INCIPIENT SOOT FORMATION [J].
CALCOTE, HF ;
MANOS, DM .
COMBUSTION AND FLAME, 1983, 49 (1-3) :289-304
[5]  
Castaldi MJ, 1996, TWENTY-SIXTH SYMPOSIUM (INTERNATIONAL) ON COMBUSTION, VOLS 1 AND 2, P693
[6]   Soot concentration and primary particle size in swirl-stabilized non-premixed turbulent flames of ethylene and air [J].
Chatterjee, Sandipan ;
Gulder, Omer L. .
EXPERIMENTAL THERMAL AND FLUID SCIENCE, 2018, 95 :73-80
[7]   Soot formation with C1 and C2 fuels using an improved chemical mechanism for PAH growth [J].
Chernov, Victor ;
Thomson, Murray J. ;
Dworkin, Seth B. ;
Slavinskaya, Nadezhda A. ;
Riedel, Uwe .
COMBUSTION AND FLAME, 2014, 161 (02) :592-601
[8]   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
[9]   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
[10]   Instantaneous and mean compositional structure of bluff-body stabilized nonpremixed flames [J].
Dally, BB ;
Masri, AR ;
Barlow, RS ;
Fiechtner, GJ .
COMBUSTION AND FLAME, 1998, 114 (1-2) :119-148