Modeling of turbulent opposed-jet mixing flows with (K)over-tilde-(ε)over-tilde model and second-order closure

被引:15
作者
Chou, CP
Chen, JY
Janicka, J
Mastorakos, E
机构
[1] Univ Calif Berkeley, Dept Mech Engn, Berkeley, CA 94720 USA
[2] Tech Univ Darmstadt, Fachgebiet Energie & Kraftwerkstech, D-64287 Darmstadt, Germany
[3] Univ Cambridge, Dept Engn, Cambridge CB2 1PZ, England
关键词
opposed-jet flow; turbulent scalar mixing; (K)over-tilde-(E)over-tilde; Reynolds stress;
D O I
10.1016/j.ijheatmasstransfer.2003.09.005
中图分类号
O414.1 [热力学];
学科分类号
摘要
A numerical model for turbulent opposed-jet mixing flows is developed with a one-dimensional (1-D) formulation with various turbulence models. Calculations with different combinations of turbulence and scalar models are conducted. The performances of various models are evaluated by extensive comparisons with existing experimental data. The numerical model is then used for studying the dependence of predicted scalar field on exit bulk velocity and turbulence intensity. Model results in general agree well with trends observed experimentally. The importance of nonzero velocity gradient at jet exit on the predicted results is illustrated through exploration runs. The distribution of mechanical-to-scalar time scale ratio, CD, is deduced from results obtained with a Reynolds stress model. The value of CD is found to deviate substantially from the commonly used value of 2, especially when the density variation is large. (C) 2003 Elsevier Ltd. All rights reserved.
引用
收藏
页码:1023 / 1035
页数:13
相关论文
共 32 条
[1]   RATIO OF SCALAR AND VELOCITY DISSIPATION TIME SCALES IN SHEAR-FLOW TURBULENCE [J].
BEGUIER, C ;
DEKEYSER, I ;
LAUNDER, BE .
PHYSICS OF FLUIDS, 1978, 21 (03) :307-310
[2]   PREMIXED FLAMES IN STAGNATING TURBULENCE .3. THE (KAPPA)OVER-TILDE-(EPSILON)OVER-TILDE THEORY FOR REACTANTS IMPINGING ON A WALL [J].
BRAY, KNC ;
CHAMPION, M ;
LIBBY, PA .
COMBUSTION AND FLAME, 1992, 91 (02) :165-186
[3]   PREMIXED FLAMES IN STAGNATING TURBULENCE .1. THE GENERAL FORMULATION FOR COUNTERFLOWING STREAMS AND GRADIENT MODELS FOR TURBULENT TRANSPORT [J].
BRAY, KNC ;
CHAMPION, M ;
LIBBY, PA .
COMBUSTION AND FLAME, 1991, 84 (3-4) :391-410
[4]   Premixed flames in stagnating turbulence part IV: A new theory for the Reynolds stresses and Reynolds fluxes applied to impinging flows [J].
Bray, KNC ;
Champion, M ;
Libby, PA .
COMBUSTION AND FLAME, 2000, 120 (1-2) :1-18
[5]   Premixed flames in stagnating turbulence Part II. The mean velocities and pressure and the Damkohler number [J].
Bray, KNC ;
Champion, M ;
Libby, PA .
COMBUSTION AND FLAME, 1998, 112 (04) :635-653
[6]   REYNOLDS STRESS DESCRIPTION OF OPPOSED AND IMPINGING TURBULENT JETS .2. AXISYMMETRICAL JETS IMPINGING ON NEARBY WALLS [J].
CHAMPION, M ;
LIBBY, PA .
PHYSICS OF FLUIDS, 1994, 6 (05) :1805-1819
[7]   REYNOLDS STRESS DESCRIPTION OF OPPOSED AND IMPINGING TURBULENT JETS .1. CLOSELY SPACED OPPOSED JETS [J].
CHAMPION, M ;
LIBBY, PA .
PHYSICS OF FLUIDS A-FLUID DYNAMICS, 1993, 5 (01) :203-216
[8]  
CHOU CP, 2001, 2 JOINT M US SECT CO
[9]   SEPARATED FLOW COMPUTATIONS WITH THE K-EPSILON-UPSILON(2) MODEL [J].
DURBIN, PA .
AIAA JOURNAL, 1995, 33 (04) :659-664
[10]   On the k-3 stagnation point anomaly [J].
Durbin, PA .
INTERNATIONAL JOURNAL OF HEAT AND FLUID FLOW, 1996, 17 (01) :89-90