LES/PDF modeling of swirl-stabilized non-premixed methane/air flames with local extinction and re-ignition

被引:16
|
作者
Yu, S. [1 ]
Liu, X. [1 ,3 ]
Bai, X. S. [1 ]
Elbaz, A. M. [2 ,4 ]
Roberts, W. L. [2 ]
机构
[1] Lund Univ, Dept Energy Sci, Div Fluid Mech, S-22100 Lund, Sweden
[2] King Abdullah Univ Sci & Technol, Clean Combust Res Ctr, Thuwal, Saudi Arabia
[3] Harbin Engn Univ, Coll Power & Energy Engn, Harbin 150001, Heilongjiang, Peoples R China
[4] Helwan Univ, Fac Engn, Cairo, Egypt
基金
瑞典研究理事会;
关键词
LES; PDF-ESF; Non-premixed swirl flames; Local extinction; Re-ignition; PROBABILITY DENSITY-FUNCTION; LARGE-EDDY SIMULATIONS; DIRECT NUMERICAL-SIMULATION; CONDITIONAL MOMENT CLOSURE; TURBULENT NONPREMIXED FLAMES; SCALAR DISSIPATION; DIFFUSION FLAME; CONSTANT VOLUME; BLOWOUT LIMITS; JET FLAMES;
D O I
10.1016/j.combustflame.2020.05.018
中图分类号
O414.1 [热力学];
学科分类号
摘要
Turbulent non-premixed flames with local extinction and re-ignition exhibit multiple combustion modes including ignition waves, diffusion flames, partially premixed flames, and ignition-assisted partially pre-mixed flames. The mechanisms of local extinction and re-ignition are not well understood and numerical modeling of multi-mode combustion is a challenging task. In this work, a specially designed swirl-burner was used to study local extinction and re-ignition of non-premixed turbulent methane/air flames. High speed Particle Image Velocimetry (PIV) and laser induced fluorescence of OH radicals (OH-PLIF) mea-surements along with Large Eddy Simulation (LES) were carried out to investigate the mechanisms extinction and re-ignition processes in the burner. LES is based on a transported probability density func-tion model within the framework of Eulerian Stochastic Fields (PDF-ESF). It is found that local extinction occurs when the scalar dissipation rate around the stoichiometric mixture fraction is high. The character-istic time scale for local extinction and re-ignition in the present flames is an order of magnitude longer than the characteristic time scale of diffusion/extinction of laminar flamelets. There are two mechanisms for flame hole re-ignition in the present flames. First, under low degree of local extinction conditions (i.e., for small flame holes surrounded by flames) the flame hole re-ignition is due to the mechanism of turbulent flame folding. Second, under high degree of extinction conditions (i.e., with large regions extinction and lifted flames), re-ignition of the locally extinguished flame is due to the mechanism of ig-nition assisted partially premixed flame propagation. The results show that the PDF-ESF model is capable of simulating the quenching and re-ignition process found in the experiments. (C) 2020 The Combustion Institute. Published by Elsevier Inc. All rights reserved.
引用
收藏
页码:102 / 119
页数:18
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