Modeling of flame-generated turbulence based on direct numerical simulation databases

被引:91
|
作者
Nishiki, S [1 ]
Hasegawa, T
Borghi, R
Himeno, R
机构
[1] Nagoya Inst Technol, Grad Sch Engn, Dept Environm Technol & Urban Planning, Nagoya, Aichi, Japan
[2] Nagoya Univ, Ctr Integrated Res Sci & Engn, Nagoya, Aichi, Japan
[3] Univ Aix Marseille 2, ESM2, F-13284 Marseille 07, France
[4] CNRS, LMA, Marseille, France
[5] RIKEN, Inst Phys & Chem Res, Adv Comp Ctr, Div Comp & Informat, Wako, Saitama, Japan
基金
日本学术振兴会;
关键词
D O I
10.1016/S1540-7489(02)80246-2
中图分类号
O414.1 [热力学];
学科分类号
摘要
Turbulent premixed flames propagating in homogeneous isotropic turbulent flows were simulated directly with a single-step irreversible reaction. Two cases were calculated, case H, with a high-density ratio of flame rho(u)/rho(b) = 7.53, and case L, low-density ratio of flame rho(u)/rho(b) = 2.50, while u'/u(L) was nearly equal to unity. We obtained databases of fully developed stationary turbulent flames. These databases were investigated by analyzing the transport equation for turbulent kinetic energy to study flame-generated turbulence and its models. We found that turbulent fluctuations of all components, especially the streamwise component, were amplified in the flame brush and that flame-generated turbulence increased for a larger density ratio of the flame. Analysis based on the Favre-averaged transport equation for turbulent kinetic energy showed that pressure-related terms produced kinetic energy in the flame brush, the mean pressure gradient term was most important in case H and the pressure work term was most important in case L. On the other hand, the diffusion and dissipation term and velocity gradient term decreased kinetic energy. Next, modeling of the important terms in the balance equations were discussed. The mean pressure gradient term, pressure dilatation term, and additional dissipation components were modeled and compared with the direct numerical simulation (DNS) results. The mean pressure gradient term was modeled,with assumption on the density, and the model was in good agreement with DNS. The other two terms were also modeled by scaling, and these models mimicked DNS well.
引用
收藏
页码:2017 / 2022
页数:6
相关论文
共 50 条
  • [41] Effect of turbulence modeling on VIV numerical simulation
    Wanderley, Juan B. V.
    Souza, Gisele H. B.
    Levi, Carlos
    Proceedings of the 24th International Conference on Offshore Mechanics and Arctic Engineering - 2005 - Vol 1, Pts A and B, 2005, : 175 - 184
  • [42] Comparison of Flame Propagation Statistics Extracted from Direct Numerical Simulation Based on Simple and Detailed Chemistry-Part 1: Fundamental Flame Turbulence Interaction
    Keil, Felix Benjamin
    Amzehnhoff, Marvin
    Ahmed, Umair
    Chakraborty, Nilanjan
    Klein, Markus
    ENERGIES, 2021, 14 (17)
  • [43] Direct numerical simulation of turbulence in the wake of a metal foam
    Corsini, Roberto
    Stalio, Enrico
    INTERNATIONAL COMMUNICATIONS IN HEAT AND MASS TRANSFER, 2020, 115
  • [45] High-resolution direct numerical simulation of turbulence
    Kaneda, Y
    Ishihara, T
    JOURNAL OF TURBULENCE, 2006, 7 (20): : 1 - 17
  • [46] Direct numerical simulation of turbulence and microphysics in the Pi Chamber
    MacMillan, Theodore
    Shaw, Raymond A.
    Cantrell, Will H.
    Richter, David H.
    PHYSICAL REVIEW FLUIDS, 2022, 7 (02):
  • [47] Direct numerical simulation of particle-turbulence interaction
    Li, C
    Mosyak, A
    Hetsroni, G
    INTERNATIONAL JOURNAL OF MULTIPHASE FLOW, 1999, 25 (02) : 187 - 200
  • [48] Direct numerical simulation of turbulence in a square annular duct
    Xu, Hongyi
    JOURNAL OF FLUID MECHANICS, 2009, 621 : 23 - 57
  • [49] Direct numerical simulation of axisymmetric wakes embedded in turbulence
    Rind, Elad
    Castro, Ian P.
    JOURNAL OF FLUID MECHANICS, 2012, 710 : 482 - 504
  • [50] Direct numerical simulation of canonical shock/turbulence interaction
    Larsson, Johan
    Lele, Sanjiva K.
    PHYSICS OF FLUIDS, 2009, 21 (12) : 1 - 12