Effects of Turbulent Reynolds Number on the Displacement Speed Statistics in the Thin Reaction Zones Regime of Turbulent Premixed Combustion

The effects of turbulent Reynolds number on the statistical behaviour of the displacement speed have been studied using three-dimensional Direct Numerical Simulation of statistically planar turbulent premixed flames. The probability of finding negative values of the displacement speed is found to increase with increasing turbulent Reynolds number when the Damkohler number is held constant. It has been shown that the statistical behaviour of the Surface Density Function, and its strain rate and curvature dependence, plays a key role in determining the response of the different components of displacement speed. Increasing the turbulent Reynolds number is shown to reduce the strength of the correlations between tangential strain rate and dilatation rate with curvature, although the qualitative nature of the correlations remains unaffected. The dependence of displacement speed on strain rate and curvature is found to weaken with increasing turbulent Reynolds number when either Damkohler or Karlovitz number is held constant, but the qualitative nature of the correlation remains unaltered. The implications of turbulent Reynolds number effects in the context of Flame Surface Density (FSD) modelling have also been addressed, with emphasis on the influence of displacement speed on the curvature and propagation terms in the FSD balance equation.

[1]  Tarek Echekki,et al.  Analysis of the contribution of curvature to premixed flame propagation , 1999 .

[2]  T. Poinsot Boundary conditions for direct simulations of compressible viscous flows , 1992 .

[3]  Nilanjan Chakraborty,et al.  Influence of Lewis number on curvature effects in turbulent premixed flame propagation in the thin reaction zones regime , 2005 .

[4]  N. Chakraborty,et al.  Direct Numerical Simulation analysis of the Flame Surface Density transport equation in the context of Large Eddy Simulation , 2009 .

[5]  Tarek Echekki,et al.  Unsteady strain rate and curvature effects in turbulent premixed methane-air flames , 1996 .

[6]  K. Huh,et al.  Roles of displacement speed on evolution of flame surface density for different turbulent intensities and Lewis numbers in turbulent premixed combustion , 2008 .

[7]  N. Chakraborty,et al.  A priori analysis of the curvature and propagation terms of the flame surface density transport equation for large eddy simulation , 2007 .

[8]  M. Klein,et al.  Effects of initial radius on the propagation of premixed flame kernels in a turbulent environment , 2006 .

[9]  N. Chakraborty,et al.  Effects of strain rate and curvature on surface density function transport in turbulent premixed flames in the thin reaction zones regime , 2005 .

[10]  Hong G. Im,et al.  Correlation of Flame Speed with Stretch in Turbulent Premixed Methane/Air Flames , 1997 .

[11]  Bendiks Jan Boersma,et al.  Direct numerical simulation of homogeneous turbulence in combination with premixed combustion at low Mach number modelled by the $G$-equation , 2006, Journal of Fluid Mechanics.

[12]  H. Lugt,et al.  Laminar flow behavior under slip−boundary conditions , 1975 .

[13]  Hong G. Im,et al.  Preferential diffusion effects on the burning rate of interacting turbulent premixed hydrogen-air flames , 2002 .

[14]  N. Chakraborty,et al.  Influence of lewis number on strain rate effects in turbulent premixed flame propagation , 2006 .

[15]  Wolfgang Kollmann,et al.  Pocket formation and the flame surface density equation , 1998 .

[16]  Jacqueline H. Chen,et al.  Comparison of direct numerical simulation of lean premixed methane–air flames with strained laminar flame calculations , 2006 .

[17]  Nilanjan Chakraborty,et al.  Effects of strain rate and curvature on the propagation of a spherical flame kernel in the thin-reaction-zones regime , 2006 .

[18]  Thierry Poinsot,et al.  A Study of the Laminar Flame Tip and Implications for Premixed Turbulent Combustion , 1992 .

[19]  N. Chakraborty Comparison of displacement speed statistics of turbulent premixed flames in the regimes representing combustion in corrugated flamelets and thin reaction zones , 2007 .

[20]  Karl W. Jenkins,et al.  Direct numerical simulation of turbulent flame kernels , 1999 .

[21]  Guy Joulin,et al.  On the response of premixed flames to time-dependent stretch and curvature , 1994 .

[22]  D. Veynante,et al.  Experimental analysis of flamelet models for premixed turbulent combustion , 1994 .

[23]  N. Chakraborty,et al.  Comparison of 2D and 3D density-weighted displacement speed statistics and implications for laser based measurements of flame displacement speed using direct numerical simulation data , 2011 .

[24]  M. Klein,et al.  Stretch rate effects on displacement speed in turbulent premixed flame kernels in the thin reaction zones regime , 2007 .

[25]  Nilanjan Chakraborty,et al.  Unsteady effects of strain rate and curvature on turbulent premixed flames in an inflow-outflow configuration , 2004 .

[26]  M. Klein,et al.  Effects of global flame curvature on surface density function transport in turbulent premixed flame kernels in the thin reaction zones regime , 2009 .

[27]  Thierry Poinsot,et al.  Stretching and quenching of flamelets in premixed turbulent combustion , 1991 .

[28]  E. Hawkes,et al.  The effects of strain rate and curvature on surface density function transport in turbulent premixed methane–air and hydrogen–air flames: A comparative study , 2008 .

[29]  Hideaki Kobayashi,et al.  Relationship between the smallest scale of flame wrinkles and turbulence characteristics of high-pressure, high-temperature turbulent premixed flames , 2002 .

[30]  M. Klein,et al.  Influence of Lewis number on the surface density function transport in the thin reaction zone regime for turbulent premixed flames , 2008 .

[31]  Jacqueline H. Chen,et al.  Statistics of flame displacement speeds from computations of 2-D unsteady methane-air flames , 1998 .

[32]  H. Im,et al.  Stretch effects on the burning velocity of turbulent premixed hydrogen/air flames , 2000 .

[33]  R. Rogallo Numerical experiments in homogeneous turbulence , 1981 .

[34]  Jacqueline H. Chen,et al.  Direct numerical simulation of hydrogen-enriched lean premixed methane–air flames , 2004 .

[35]  K. Bray,et al.  Vorticity in unsteady premixed flames: vortex pair–premixed flame interactions under imposed body forces and various degrees of heat release and laminar flame thickness , 2001 .

[36]  Inge R. Gran,et al.  NEGATIVE FLAME SPEED IN AN UNSTEADY 2-D PREMIXED FLAME: A COMPUTATIONAL STUDY , 1996 .

[37]  D. Veynante,et al.  Experimental analysis of flame surface density models for premixed turbulent combustion , 1996 .

[38]  Thierry Poinsot,et al.  Flame Stretch and the Balance Equation for the Flame Area , 1990 .

[39]  D. Veynante,et al.  Direct numerical simulation analysis of flame surface density concept for large eddy simulation of turbulent premixed combustion , 1998 .

[40]  Jacqueline H. Chen,et al.  Evaluation of models for flame stretch due to curvature in the thin reaction zones regime , 2005 .