Turbulent Premixed Hydrogen/Air Flames.

Abstract : The properties of turbulent premixed flames were investigated both theoretically and experimentally. Attention was limited to hydrogen/air mixtures burning as either turbulent jet flames or a freely propagating flames in isotropic turbulence. The research has application to a variety to premixed turbulent combustion processes: underwater metal cutting at great depth, primary combustors for high-speed airbreathing propulsion systems, afterburners, fuel/ air explosions, and spark-ignition internal combustion engines. Major findings of this phase of the investigation are as follows: (1) effects of preferential diffusion are relevent for flames at high Reynolds number, retarding and enhancing the distortion of the flame surface by turbulence for stable and unstable conditions, respectively; (2) local turbulent burning velocity, flame brush thickness and the fractal dimension of the flame surface all increase with distance from the flameholder, with larger rates of increases at larger turbulence intensities; (3) estimates of flame properties using contemporary turbulence models were only fair because these methods cannot account for effects of preferential diffusion, distance from the flameholder and finite laminar flame speeds; and (4) the stochastic simulation duplicated measured trends of flame surface properties for neutral preferential diffusion conditions (the only case considered) but underestimated effects of turbulence (particularly near the flame tip) due to the limitations of a two-dimensional simulation.

[1]  J. Driscoll,et al.  Flame surface properties of premixed flames in isotropic turbulence : measurements and numerical simulations , 1992 .

[2]  James F. Driscoll,et al.  Preferential Diffusion Effects on the Surface Structure of Turbulent Premixed Hydrogen/Air Flames , 1991 .

[3]  J. Driscoll,et al.  Turbulent Premixed Hydrogen/Air Flames at High Reynolds Numbers , 1990 .

[4]  Frediano V. Bracco,et al.  Fractals and turbulent premixed engine flames , 1989 .

[5]  J. Driscoll,et al.  Measurement of various terms in the turbulent kinetic energy balance within a flame and comparison with theory , 1988 .

[6]  E. G. Groff,et al.  An experimental evaluation of an entrainment flame-propagation model , 1987 .

[7]  Benoit B. Mandelbrot,et al.  Fractal Geometry of Nature , 1984 .

[8]  P. K. Barr,et al.  Stochastic Calculation of Laminar Wrinkled Flame Propagation via Vortex Dynamics , 1983 .

[9]  G. Andrews,et al.  Determination of burning velocity by double ignition in a closed vessel , 1973 .

[10]  E. S. Semenov Measurement of turbulence characteristics in a closed volume with artificial turbulence , 1965 .

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

[12]  G. Adomeit,et al.  The influence of turbulence intensity and laminar flame speed on turbulent flame propagation under engine like conditions , 1991 .

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

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

[15]  P. Clavin Dynamic behavior of premixed flame fronts in laminar and turbulent flows , 1985 .

[16]  E. G. Groff The cellular nature of confined spherical propane-air flames , 1982 .

[17]  K. Bray,et al.  Turbulent flows with premixed reactants , 1980 .