Direct Lagrangian Simulations of a Mixing Layer by the Transport-Element Method

Results are presented of Direct Lagrangian Simulations (DLS) of an unsteady, two-dimensional planar mixing layer by means of the "transport-element method." The simulated results are used to understand the mixing behavior in a non-reacting flow, and to assess the limiting rate of the reactant conversion in a layer under the influence of a non-heat releasing reaction of the type A + B -> Products. Both unforced and harmonically forced layers are considered. It is shown that harmonic perturbation results in a significant enhancement of mixing at initial stages of the flow development. However, it does not have a substantial influence at later stages. In all the cases considered the statistical results generated by DLS are shown to compare well with experimental data. Therefore, based on the DLS results the extent of validity of some of the turbulence closures of reacting flows is assessed. With this assessment it is demonstrated that the limiting rate of reactant conversion can be accurately predicted by the use of a Beta density model for the probability distribution of an appropriately defined Shvab-Zeldovich variable. Also, it is shown that the gradient diffusion model works reasonably well in accounting for the effects of turbulent convective fluxes.

[1]  F. Browand,et al.  Vortex pairing : the mechanism of turbulent mixing-layer growth at moderate Reynolds number , 1974, Journal of Fluid Mechanics.

[2]  O. Reynolds III. An experimental investigation of the circumstances which determine whether the motion of water shall be direct or sinuous, and of the law of resistance in parallel channels , 1883, Proceedings of the Royal Society of London.

[3]  A. Ghoniem,et al.  Lagrangian simulation of a reacting mixing layer at low heat release , 1988 .

[4]  B. Launder,et al.  Mathematical Models of turbulence , 1972 .

[5]  John G. Proakis,et al.  Probability, random variables and stochastic processes , 1985, IEEE Trans. Acoust. Speech Signal Process..

[6]  H. L. Toor Mass transfer in dilute turbulent and non‐turbulent systems with rapid irreversible reactions and equal diffusivities , 1962 .

[7]  A. Chorin Numerical study of slightly viscous flow , 1973, Journal of Fluid Mechanics.

[8]  Christopher R. Anderson,et al.  A VORTEX METHOD FOR FLOWS WITH SLIGHT DENSITY VARIATIONS , 1985 .

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

[10]  Andrew J. Majda,et al.  High order accurate vortex methods with explicit velocity kernels , 1985 .

[11]  C. K. Madnia,et al.  Reactant conversion in homogeneous turbulence: Mathematical modeling, computational validations, and practical applications , 1992 .

[12]  M. Mcpherson,et al.  Introduction to fluid mechanics , 1997 .

[13]  S.N.B. Murthy,et al.  Turbulent Free Shear Layer Mixing and Combustion , 1991 .

[14]  P. Dimotakis Two-dimensional shear-layer entrainment , 1986 .

[15]  J. Sethian A brief overview of vortex methods , 1990 .

[16]  Juan I. Ramos,et al.  Probability Density Function Calculations in Turbulent Chemically Reacting Round Jets, Mixing Layers and One-Dimensional Reactors , 1985 .

[17]  A. Ghoniem,et al.  Numerical study of the dynamics of a forced shear layer , 1987 .

[18]  J. Marsden,et al.  A mathematical introduction to fluid mechanics , 1979 .

[19]  Manoochehr Koochesfahani,et al.  Mixing and chemical reactions in a turbulent liquid mixing layer , 1986, Journal of Fluid Mechanics.

[20]  C. Bowman,et al.  The structure of a chemically reacting plane mixing layer , 1986, Journal of Fluid Mechanics.

[21]  P. Givi,et al.  Direct numerical simulations of a two-dimensional reacting, spatially developing mixing layer by a spectral-element method , 1989 .

[22]  Peyman Givi,et al.  Some Current Issues In The Analysis Of Reacting Shear Layers: Computational Challenges , 1992 .

[23]  Ian Proudman,et al.  Boundary Layer Theory (fourth edition). By H. SCHLICHTINO. New York: McGraw-Hill, 1960. 647 pp. £6. 8s. , 1962, Journal of Fluid Mechanics.

[24]  A. Ghoniem,et al.  On mixing, baroclinicity, and the effect of strain in a chemically-reacting shear layer , 1988 .

[25]  P. Givi Model-free simulations of turbulent reactive flows , 1989 .

[26]  P. Moin,et al.  Numerical Simulation of Turbulent Flows , 1984 .

[27]  Alexandre J. Chorin,et al.  Discretization of a vortex sheet, with an example of roll-up☆ , 1973 .

[28]  R. S. Burington Handbook of mathematical tables and formulas , 1933 .

[29]  R. W. Bilger,et al.  Turbulent flows with nonpremixed reactants , 1980 .

[30]  Chien-Cheng Chang Random vortex methods for the Navier-Stokes equations , 1988 .

[31]  James J. Riley,et al.  Progress in direct numerical simulations of turbulent reacting flows , 1989 .

[32]  A. Roshko,et al.  On density effects and large structure in turbulent mixing layers , 1974, Journal of Fluid Mechanics.

[33]  Ahmed F. Ghoniem,et al.  Grid-free simulation of diffusion using random walk methods , 1985 .

[34]  Chih-Ming Ho,et al.  Subharmonics and vortex merging in mixing layers , 1982, Journal of Fluid Mechanics.

[35]  Chih-Ming Ho,et al.  Perturbed Free Shear Layers , 1984 .

[36]  P. Givi,et al.  Mixing and Chemical Reactions in a Spatially Developing Mixing Layer , 1988 .

[37]  Ahmed F. Ghoniem,et al.  Numerical simulation of a thermally stratified shear layer using the vortex element method , 1988 .

[38]  Steven H. Frankel,et al.  Modeling of the reactant conversion rate in a turbulent shear flow , 1992 .

[39]  R. Caflisch Mathematical aspects of vortex dynamics , 1989 .