Investigation of a turbulent flame speed closure approach for premixed flame calculations

被引:37
作者
Dinkelacker, F [1 ]
Hölzler, S [1 ]
机构
[1] Univ Erlangen Nurnberg, Lehrstuhl Tech Thermodynam, D-91058 Erlangen, Germany
关键词
premixed turbulent flames; numerical modelling; turbulent name speed closure; comparison with experimental data;
D O I
10.1080/00102200008947339
中图分类号
O414.1 [热力学];
学科分类号
摘要
A computational model for turbulent premixed gaseous combustion is investigated, where the combustion process is modelled in terms of a single transport equation for a reaction progress variable c. Turbulent closure of the source term of the progress variable is based on a model, where the turbulent flame speed is used in an extension to a field variable. In order to check the model, numerical results are compared with experimental data from a turbulent premixed V-shaped flame, where the conditions of the approaching turbulent flow and of the chemical processes have been varied separately. Regarding the simple structure of this model, it is found to predict the flame shape and flame width sufficiently well, Additionally, three other relations from the literature for the turbulent flame speed variable have been tested within this approach, showing that experimentally determined flame speed relations have to be reduced in order to be used within this flame speed closure. Furthermore, the influence of the formal structure of the reaction term ((w) over bar (c) similar to \(V) over bar (c) over bar \) is compared with that of two other possible approaches ((w) over bar (c) similar to (c) over bar (1 - (c) over bar)/L-y, and (w) over barc similar to min[(1 - (c) over bar), (c) over bar, y]). While the experimental flame shape has straight boundaries, for the parabolic approach a concave bounded flame shape is found, if the length scale L-y is hold constant. This can be understood by analyzing the reaction rate integral across the flame brush.
引用
收藏
页码:321 / 340
页数:20
相关论文
共 25 条
[1]   APPLICATION OF A REYNOLDS STRESS, STRETCHED FLAMELET, MATHEMATICAL-MODEL TO COMPUTATIONS OF TURBULENT BURNING VELOCITIES AND COMPARISON WITH EXPERIMENTS [J].
BRADLEY, D ;
GASKELL, PH ;
GU, XJ .
COMBUSTION AND FLAME, 1994, 96 (03) :221-248
[2]  
Bradley D., 1992, Symp. (Int.) Combust, V24, P247, DOI [DOI 10.1016/S0082-0784(06)80034-2, 10.1016/S0082-0784(06)80034-2]
[3]  
Bray K. N. C., 1980, Turbulent reacting flows, P115
[4]   UNIFIED MODELING APPROACH FOR PREMIXED TURBULENT COMBUSTION .1. GENERAL FORMULATION [J].
BRAY, KNC ;
LIBBY, PA ;
MOSS, JB .
COMBUSTION AND FLAME, 1985, 61 (01) :87-102
[5]   STUDIES OF THE TURBULENT BURNING VELOCITY [J].
BRAY, KNC .
PROCEEDINGS OF THE ROYAL SOCIETY-MATHEMATICAL AND PHYSICAL SCIENCES, 1990, 431 (1882) :315-335
[6]  
Buschmann A, 1996, TWENTY-SIXTH SYMPOSIUM (INTERNATIONAL) ON COMBUSTION, VOLS 1 AND 2, P437
[7]  
Dinkelacker F, 1998, TWENTY-SEVENTH SYMPOSIUM (INTERNATIONAL) ON COMBUSTION, VOLS 1 AND 2, P857
[8]   A COMPARISON OF FLAMELET MODELS FOR PREMIXED TURBULENT COMBUSTION [J].
DUCLOS, JM ;
VEYNANTE, D ;
POINSOT, T .
COMBUSTION AND FLAME, 1993, 95 (1-2) :101-117
[9]   LAMINAR FLAME SPEEDS OF METHANE AIR MIXTURES UNDER REDUCED AND ELEVATED PRESSURES [J].
EGOLFOPOULOS, FN ;
CHO, P ;
LAW, CK .
COMBUSTION AND FLAME, 1989, 76 (3-4) :375-391
[10]  
FLUENT, 1996, COMPUTATIONAL FLUID