Flame/turbulence interaction in ammonia/air premixed flames at high karlovitz numbers

被引:7
|
作者
Xu, Leilei [1 ]
Fan, Qingshuang [2 ]
Liu, Xin [2 ]
Cai, Xiao [3 ]
Subash, Arman Ahamed [2 ]
Brackmann, Christian [2 ]
Li, Zhongshan [2 ]
Alden, Marcus [2 ]
Bai, Xue-Song [1 ]
机构
[1] Lund Univ, Div Fluid Mech, S-22100 Lund, Sweden
[2] Lund Univ, Div Combust Phys, S-22100 Lund, Sweden
[3] Xi An Jiao Tong Univ, State Key Lab Multiphase Flow Power Engn, Xian 710049, Peoples R China
基金
瑞典研究理事会;
关键词
Ammonia flame; Regimes; Turbulence; fl ame interaction; Distributed reactions; Karlovitz number; Bai); REACTION ZONE; PROPAGATION; TURBULENCE; SPEED;
D O I
10.1016/j.proci.2022.09.010
中图分类号
O414.1 [热力学];
学科分类号
摘要
Turbulent premixed flames subjected to extreme levels of turbulence exhibit reaction zone broadening and thinning. Instantaneous flame structures visualized using advanced laser diagnostic methods have shown significantly different behaviours of flame/turbulence interaction in jet flames stabilized on burners of different sizes. This paper aims to reconcile the controversy about flame broadening on burners of different sizes. Premixed ammonia/air flames are investigated owing to the importance of ammonia in the future carbonfree energy system. Due to the low laminar flame speed of ammonia/air mixture, the intensity of turbulence ( u ' /S L ) can be 5 times higher than that of methane/air flames at the same jet velocities. Planar laser-induced fluorescence (PLIF) imaging and large eddy simulation based on detailed chemical kinetics are carried out to systematically study the structures of ammonia/air premixed jet flames under extreme levels of turbulence conditions, with u ' /S L up to 240 and Karlovitz number up to 3019. Consistent with the observation in methane/air jet flames reported in the literature, the reaction zones of premixed ammonia/air jet flames show significantly different behaviour on burners of different sizes under similar Karlovitz number conditions. It is found that reaction zone broadening in jet flames is a spatially evolving process, not only depending on the local eddy/flame interaction but also on the upstream history. The onset of distributed reaction zones is found to take place at positions located several jet orifice diameters above the burner and thereafter eddies are self-produced in the reaction layer due to the continuous vortex stretch interacting in the layer and broadening the reaction zone. The flames on a large burner have turbulence eddies of larger integral length scales that do not fit directly inside the reaction zones, and as such the eddies could not broaden the reaction zones.& COPY; 2022 The Author(s). Published by Elsevier Inc. on behalf of The Combustion Institute. This is an open access article under the CC BY license ( http://creativecommons.org/licenses/by/4.0/ )
引用
收藏
页码:2289 / 2298
页数:10
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