Experiments on Collapsing Cylindrical Flames

This article is concerned with the effect of curvature on laminar flame dynamics. This topic is of fundamental interest and it has practical implications in turbulent combustion. It is shown that highly curved premixed flames may be obtained by operating a standard axisymmetric burner in a specific pulsed mode. Collapsing cylindrical flames are observed by submitting the burner to suitably tuned plane pulsations of the flow velocity. The cylindrical flame pattern collapses in an essentially radial motion. In these circumstances the flame cylinder separates unburned inner gases from the burned outer flow. The temporal evolution of the flame may be monitored using schlieren images while the inner flow velocity is determined from particle image velocimetry (PIV). It is shown that these data yield the stretched laminar burning velocity up to very small radii. Models of the stretched laminar burning velocity as a function of curvature are compared to experimental data and Markstein lengths are deduced. These experiments indicate how laminar flames respond to large curvature values. The data gathered may be used to guide modeling efforts in the area of turbulent combustion.

[1]  A. Lipatnikov Some Issues of Using Markstein Number for Modeling Premixed Turbulent Combustion , 1996 .

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

[3]  B. Deshaies,et al.  The velocity of a premixed flame as a function of the flame stretch: An experimental study , 1990 .

[4]  Bernard J. Matkowsky,et al.  Flames as gasdynamic discontinuities , 1982, Journal of Fluid Mechanics.

[5]  P. Clavin,et al.  Premixed flames in large scale and high intensity turbulent flow , 1983 .

[6]  P. Clavin,et al.  Premixed flames with nonbranching chain-reactions (structure and dynamics) , 1987 .

[7]  Alfonso F. Ibarreta,et al.  Measured burning velocities of stretched inwardly propagating premixed flames , 2000 .

[8]  Chung King Law,et al.  An invariant derivation of flame stretch , 1984 .

[9]  M. Z. Haq,et al.  Laminar burning velocity and Markstein lengths of methane–air mixtures , 2000 .

[10]  Piotr Wolanski,et al.  Finding the markstein number using the measurements of expanding spherical laminar flames , 1997 .

[11]  Experimental Study of the Darrieus-Landau instability on an inverted-‘V’ flame, and measurement of the Markstein number , 1999 .

[12]  D. Dunn-Rankin,et al.  Location of the Schlieren Image in Premixed Flames: Axially Symmetrical Refractive Index Fields , 1998 .

[13]  D. Durox,et al.  Concerning the location of the schlieren limit in premixed flames , 2000 .

[14]  P. Gaskell,et al.  Burning Velocities, Markstein Lengths, and Flame Quenching for Spherical Methane-Air Flames: A Computational Study , 1996 .

[15]  Chung King Law,et al.  An integral analysis of the structure and propagation of stretched premixed flames , 1988 .

[16]  Norbert Peters,et al.  Approximations for burning velocities and markstein numbers for lean hydrocarbon and methanol flames , 1997 .

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

[18]  Moshe Matalon,et al.  On Flame Stretch , 1983 .

[19]  F. Lacas,et al.  Flow seeding with an air nebulizer , 1999 .

[20]  Kendrick Aung,et al.  Response to comment by S.C. Taylor and D.B. Smith on “laminar burning velocities and Markstein numbers of hydrocarbon/air flames” , 1995 .

[21]  Bunsen flame hydrodynamics , 1985 .

[22]  Sébastien Ducruix Dynamique des interactions acoustique-combustion , 2001 .

[23]  Gerard M. Faeth,et al.  Laminar burning velocities and Markstein numbers of hydrocarbonair flames , 1993 .

[24]  F. Baillot,et al.  Burning Velocity of Pockets from a Vibrating Flame Experiment , 1997 .