Interaction of turbulence and scalar fields in premixed flames

The interaction of turbulence with progress variable, c, field in a premixed flame is studied. This interaction is characterized by the correlation c,ieijc,j¯, where the overbar denotes an appropriate averaging process, c,i is the gradient of c in spatial direction i and eij is the turbulence strain rate. The importance of this term is recognized via a transport equation for the square of the magnitude of the scalar gradient in turbulent premixed flames. It is also shown that the above correlation forms a natural part of the tangential strain rate which appears in the flame surface density, Σ, equation. It is well known that this correlation is negative signifying the scalar gradient production by incompressible turbulence via the preferential alignment of the scalar gradient with the most compressive principal strain rate. This physical picture is commonly adopted for turbulent premixed flames also. Contrary to this, analyses of direct numerical simulation data for a turbulent premixed flame having flame...

[1]  Stephen B. Pope,et al.  Computations of turbulent combustion: Progress and challenges , 1991 .

[2]  Denis Veynante,et al.  Turbulent combustion modeling , 2002, VKI Lecture Series.

[3]  A. Kerstein,et al.  Alignment of vorticity and scalar gradient with strain rate in simulated Navier-Stokes turbulence , 1987 .

[4]  Roland Borghi,et al.  Towards an extended scalar dissipation equation for turbulent premixed combustion , 2003 .

[5]  R. Cant,et al.  Scalar transport modelling in large eddy simulation of turbulent premixed flames , 2002 .

[6]  G. Batchelor,et al.  The effect of homogeneous turbulence on material lines and surfaces , 1952, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[7]  Thierry Poinsot,et al.  Direct numerical simulation of H2/O2/N2 flames with complex chemistry in two-dimensional turbulent flows , 1994, Journal of Fluid Mechanics.

[8]  Nedunchezhian Swaminathan,et al.  Effect of dilatation on scalar dissipation in turbulent premixed flames , 2005 .

[9]  Robert W. Bilger,et al.  Some Aspects of Scalar Dissipation , 2004 .

[10]  Robert McDougall Kerr,et al.  Higher-order derivative correlations and the alignment of small-scale structures in isotropic numerical turbulence , 1983, Journal of Fluid Mechanics.

[11]  N. Peters,et al.  Numerical Simulation of Turbulent Flame Structure with Non-unity Lewis Number , 1987 .

[12]  Stephen B. Pope,et al.  The evolution of surfaces in turbulence , 1988 .

[13]  G. Batchelor Small-scale variation of convected quantities like temperature in turbulent fluid Part 1. General discussion and the case of small conductivity , 1959, Journal of Fluid Mechanics.

[14]  Nedunchezhian Swaminathan,et al.  Structure of nonpremixed reaction zones in numerical isotropic turbulence , 1996 .

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

[16]  Nedunchezhian Swaminathan,et al.  Interdependence of the Instantaneous Flame Front Structure and the Overall Scalar Flux in Turbulent Premixed Flames , 1997 .

[17]  Christopher J. Rutland,et al.  Direct simulations of premixed turbulent flames with nonunity Lewis numbers , 1993 .

[18]  R. Borghi,et al.  Turbulent premixed combustion: Further discussions on the scales of fluctuations , 1990 .

[19]  Martin R. Maxey,et al.  Small‐scale features of vorticity and passive scalar fields in homogeneous isotropic turbulence , 1991 .

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

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

[22]  Rs Cant,et al.  Scalar transport modeling in large eddy simulation of turbulent premixed flames , 2002 .

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

[24]  S. Elghobashi,et al.  Mixing characteristics of an inhomogeneous scalar in isotropic and homogeneous sheared turbulence , 1992 .

[25]  J. Gore,et al.  An evaluation of combined flame surface density and mixture fraction models for nonisenthalpic premixed turbulent flames , 1999 .

[26]  T. Poinsot,et al.  Theoretical and numerical combustion , 2001 .

[27]  S. Candel,et al.  Applications of direct numerical simulation to premixed turbulent combustion , 1995 .

[28]  Thierry Mantel,et al.  A new model of premixed wrinkled flame propagation based on a scalar dissipation equation , 1994 .

[29]  Robert W. Bilger,et al.  Experimental investigation of three-dimensional flame-front structure in premixed turbulent combustion-I: Hydrocarbon/air Bunsen flames , 2002 .

[30]  S. Elghobashi,et al.  Effects of gravity on turbulent nonpremixed flames , 1999 .

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

[32]  C. Gibson Fine Structure of Scalar Fields Mixed by Turbulence. I. Zero‐Gradient Points and Minimal Gradient Surfaces , 1968 .

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

[34]  S. Elghobashi,et al.  On the alignment of strain, vorticity and scalar gradient in turbulent, buoyant, nonpremixed flames , 1998 .

[35]  Peter Diamessis,et al.  Interaction of vorticity, rate-of-strain, and scalar gradient in stratified homogeneous sheared turbulence , 2000 .

[36]  D. Veynante,et al.  Gradient and counter-gradient scalar transport in turbulent premixed flames , 1997, Journal of Fluid Mechanics.

[37]  Robert W. Bilger,et al.  Scalar gradient and related quantities in turbulent premixed flames , 1997 .

[38]  Clemens F. Kaminski,et al.  Curvature and wrinkling of premixed flame kernels?comparisons of OH PLIF and DNS data , 2005 .

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

[40]  A. Leonard,et al.  Scalar dissipation and mixing in turbulent reacting flows , 1991 .

[41]  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 .

[42]  Otto Zeman,et al.  Modeling Buoyancy Driven Mixed Layers , 1976 .

[43]  M. Glauser,et al.  Theoretical and Computational Fluid Dynamics the Structure of Inhomogeneous Turbulence in Variable Density Nonpremixed Flames 1 , 2022 .

[44]  W. Cocke Turbulent Hydrodynamic Line Stretching: Consequences of Isotropy , 1969 .

[45]  R. Bilger Conditional moment closure modelling and advanced laser measurements , 1993 .

[46]  Comments on “Turbulent Hydrodynamic Line Stretching: Consequences of Isotropy” , 1970 .