Modelling of the curvature term of the Flame Surface Density transport equation for Reynolds Averaged Navier Stokes simulations

Three-dimensional statistically planar simplified chemistry based Direct Numerical Simulations (DNS) of turbulent premixed flames with wide variations of Karlovitz number Ka , heat release parameter τ and global Lewis number Le have been used for the a-priori modeling of the curvature term of the generalised Flame Surface Density (FSD) transport equation in the context of Reynolds Averaged Navier Stokes (RANS) simulations. The simulation parameters used in the current study have been chosen in such a manner that both the corrugated flamelets and thin reaction zones regime of premixed turbulent combustion have been considered. The curvature term has been split into the contributions arising due to the reaction and normal diffusion components (i.e. 1 T ) and the term arising due to the

[1]  N. Chakraborty,et al.  Effects of Lewis number on flame surface density transport in turbulent premixed combustion , 2011 .

[2]  N. Chakraborty,et al.  Modelling of the tangential strain rate term of the Flame Surface Density transport equation in the context of Reynolds Averaged Navier-Stokes Simulation , 2011 .

[3]  N. Chakraborty,et al.  Effects of Lewis number on turbulent scalar transport and its modelling in turbulent premixed flames , 2009 .

[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]  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 .

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

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

[9]  Charles Meneveau,et al.  A dynamic flame surface density model for large eddy simulation of turbulent premixed combustion , 2004 .

[10]  C. Meneveau,et al.  A power-law flame wrinkling model for LES of premixed turbulent combustion Part I: non-dynamic formulation and initial tests , 2002 .

[11]  RS Cant,et al.  Implications of a flame surface density approach to large eddy simulation of premixed turbulent combustion , 2001 .

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

[13]  Jay P. Gore,et al.  An evaluation of flame surface density models for turbulent premixed jet flames , 1999 .

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

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

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

[17]  Rs Cant,et al.  Turbulent transport in premixed flames , 1994 .

[18]  Thierry Poinsot,et al.  The evolution equation for the flame surface density in turbulent premixed combustion , 1994, Journal of Fluid Mechanics.

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

[20]  Thierry Poinsot,et al.  A comparison of flamelet models for premixed turbulent combustion , 1993 .

[21]  Thierry Poinsot,et al.  Numerical simulations of Lewis number effects in turbulent premixed flames , 1992, Journal of Fluid Mechanics.

[22]  Stephen B. Pope,et al.  Modelling of flamelet surface-to-volume ratio in turbulent premixed combustion , 1991 .

[23]  Thierry Poinsot,et al.  COHERENT FLAMELET MODEL: APPLICATIONS AND RECENT EXTENSIONS , 1990 .

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

[25]  Rs Cant,et al.  Strained laminar flamelet calculations of premixed turbulent combustion in a closed vessel , 1989 .

[26]  Derek Bradley,et al.  Lewis number effects on turbulent burning velocity , 1985 .

[27]  Forman A. Williams,et al.  Effects of molecular diffusion and of thermal expansion on the structure and dynamics of premixed flames in turbulent flows of large scale and low intensity , 1982, Journal of Fluid Mechanics.

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