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首页> 外文期刊>Flow, turbulence and combustion >Statistical analysis and a-priori modelling of flame surface density transport in turbulent stratified flames: A direct numerical simulation study
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Statistical analysis and a-priori modelling of flame surface density transport in turbulent stratified flames: A direct numerical simulation study

机译:湍流分层火焰中火焰表面密度传输的统计分析和先验建模:直接数值模拟研究

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摘要

Statistically planar turbulent premixed and stratified flames for different initial intensities of decaying turbulence have been simulated for global equivalence ratios < φ > = 0.7 and < φ > = 1.0 using three-dimensional simplified chemistry based Direct Numerical Simulations (DNS). The simulation parameters are chosen such that the thin reaction zones regime combustion is realised in all cases and a random bi-modal distribution of equivalence ratio φ is introduced in the unburned gas ahead of the flame to account for the mixture inhomogeneity for stratified flames. The modelling of the unclosed terms (i.e. the turbulent transport term T _1, the tangential strain rate term T _2, the propagation term T _3, and the curvature term T 4) of the generalised FSD transport equation has been addressed in the context of RANS simulations. It has been found that the turbulent transport term T _1 remains small in comparison to the leading order contributions of the tangential strain rate and curvature terms (i.e. T _2 and T _4, respectively) in the globally stoichiometric cases, but T _1 begins to play a more important role in the globally fuel-lean cases. The strain rate term T _2 remains positive throughout the flame brush and acts as a leading order source term for all the flames considered in this analysis. It is has been found that the magnitude of T _2 decreases with decreasing root-mean-square velocity fluctuations u ′ (< φ >) for a given value of < φ > (u ′). The contribution of the propagation term T _3 remains generally positive towards the unburned gas side of the flame brush but assumes generally negative values towards the burned gas side of the flame brush. Moreover, whilst the order of magnitude of the propagation term T _3 is comparable in all cases, T _3 remains small in comparison to the leading order contributors (i.e. T _2 and T _4) in the globally stoichiometric cases however it plays a more important role in the globally fuel-lean cases. The curvature term T _4 acts as a leading order sink term in all cases except towards the unburned gas side of the flame brush in low u ′ globally stoichiometric (i.e. < φ > = 1.0) flames. Furthermore, it has been demonstrated that the magnitude of T 4 decreases with decreasing u ′ (< φ >) for a given value of < φ > (u ′). Appropriate model expressions have been identified for T _1, T _2, T _3 and T _4 based on an a-priori analysis of the DNS data.
机译:使用基于三维简化化学的直接数值模拟(DNS),针对全局等效比<φ> = 0.7和<φ> = 1.0,针对不同的衰减湍流初始强度对统计平面湍流预混和分层火焰进行了模拟。选择模拟参数,以便在所有情况下都实现稀薄的反应区状态燃烧,并且等价比φ的随机双峰分布在火焰之前引入未燃烧气体中,以解决分层火焰的混合物不均匀性。广义FSD输运方程的未封闭项(即湍流输运项T _1,切向应变率项T _2,传播项T _3和曲率项T 4)的建模已在RANS的背景下得到解决。模拟。已经发现,在整体化学计量的情况下,与切向应变率和曲率项(分别为T _2和T _4)的先导贡献相比,湍流输运项T _1仍然很小,但是T _1开始起作用在全球燃油稀少的案例中扮演更重要的角色。应变率项T _2在整个火焰刷中保持为正,并且充当此分析中考虑的所有火焰的前导源项。已经发现,对于给定的值<φ>(u'),T _2的大小随着均方根速度波动u'(<φ>)的减小而减小。传播项T _3对火焰刷的未燃烧气体侧的贡献通常保持为正,但对火焰刷的燃烧气体侧的贡献通常为负。此外,尽管在所有情况下传播项T _3的数量级都是可比的,但与全球化学计量情况下的领先顺序贡献者(即T _2和T _4)相比,T _3仍然很小,但是它起着更重要的作用在全球燃油稀少的情况下。在所有情况下,曲率项T _4都充当前导下沉项,除了在全局化学计量低(即<φ> = 1.0)的低u'火焰中朝向火焰刷的未燃烧气体侧。此外,已经证明,对于给定值<φ>(u′),T 4的大小随着u′(<φ>)的减小而减小。基于对DNS数据的先验分析,已经为T _1,T _2,T _3和T _4确定了合适的模型表达式。

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