Abstract

Probability density functions of the components of stretch rate are investigated using a previously-published Direct Numerical Simulation dataset spanning a range of turbulence intensities in the Thin Reaction Zones (TRZ) regime. The dataset was generated by varying the turbulence intensity across five different simulations while maintaining fixed the remaining physico-chemical input parameters such as integral length scale and laminar flame thickness and speed. Across the entire dataset, the joint probability density function of stretch rate and displacement speed displays a distinctive shape with two branches consistent with previous studies at low turbulence intensities. This joint probability density function is analysed further by extracting individual contributions of stretch rate components to determine their relative importance across the branches. The curvature dependence of displacement speed appears to play an important role in shaping these branches. Implications of this result with regard to evaluation of the components of stretch rate in the TRZ regime are discussed.

Highlights

  • Introduction1.1 Flamelet modelling: stretch rate and the displacement speed

  • 1.1 Flamelet modelling: stretch rate and the displacement speedIn flamelet modelling of turbulent premixed flames, the rate at which reactants are transformed into products is a function of the mean stretch rate sof the flame surface [1]

  • The results above suggest that the non-linear contribution of displacement speed sd to the stretch rate sis significant

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Summary

Introduction

1.1 Flamelet modelling: stretch rate and the displacement speed. In flamelet modelling of turbulent premixed flames, the rate at which reactants are transformed into products is a function of the mean stretch rate sof the flame surface [1]. The instantaneous stretch rate sof the flame surface is defined as the fractional rate of change of its area A [2] as follows s ≡ dA , (1) A dt. Turbulence and Combustion (2019) 102:957–971 with the flame surface itself represented by an isosurface of the reaction progress variable c which is defined as c ≡ (YR − Y )/(YR − YP ), (2). At any point on a progress variable isosurface c = c∗, the local instantaneous stretch rate sis written as [3, 4].

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