Abstract
Statistically planar turbulent premixed and stratified flames for different initial intensities of decaying turbulence have been simulated for global equivalence ratios = 0.7 and = 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 T1, the tangential strain rate term T2, the propagation term T3, and the curvature term T4) of the generalised FSD transport equation has been addressed in the context of RANS simulations. It has been found that the turbulent transport term T1 remains small in comparison to the leading order contributions of the tangential strain rate and curvature terms (i.e. T2 and T4, respectively) in the globally stoichiometric cases, but T1 begins to play a more important role in the globally fuel-lean cases. The strain rate term T2 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 T2 decreases with decreasing root-mean-square velocity fluctuations u′ ( ) for a given value of (u′). The contribution of the propagation term T3 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 T3 is comparable in all cases, T3 remains small in comparison to the leading order contributors (i.e. T2 and T4) in the globally stoichiometric cases however it plays a more important role in the globally fuel-lean cases. The curvature term T4 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. = 1.0) flames. Furthermore, it has been demonstrated that the magnitude of T4 decreases with decreasing u′ ( ) for a given value of (u′). Appropriate model expressions have been identified for T1, T2, T3 and T4 based on an a-priori analysis of the DNS data.
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