Experiments on velocity augmentation of spherical flames by grids

Using spherical wire mesh screens with a wire diameter d and a mesh size l, an experimental study was carried out involving homogeneous mixtures of propane/air, ethylene/air, acetylene/air and with oxygen enriched air. Streak photographs of the processes were taken, yielding information on the flame propagation speeds inside and outside the screen. The ratio of the two speeds immediately before and after crossing the screen, α, can be interpreted as practically equivalent (for the same “heat release”) to the ratio of flame velocities relative to the unburned gas, i.e. Values of (α − 1) are correlated with the Reynolds number based on the wire thickness d, density and viscosity of the unburned gas and flame propagation speed inside the wire mesh. The experiments were repeated with two and three spheres of different diameters, e.g. inner screen 9 cm in diameter and outer screen 18 cm in diameter or three screens, 9, 13.5 and 18 cm, respectively. The second screen usually added a factor of 2 on the value of α. The third screen produced very little additional effect. The highest value of α we ever obtained for mixtures with air was about 12 (for acetylene/air). With oxygen enriched air the situation is quite different. If the flame velocity of the laminar flame relative to the unburned gas exceeds 2 m/sec, the value of α may increase up to a level corresponding to detonation.