The structure of flame propagating through lycopodium dust clouds has been
investigated experimentally. Upward propagating laminar flames in a vertica
l duct of 1800 mm height and 150x150 mm square cross-section are observed,
and the leading flame front is also visualized using by a high-speed video
camera. Although the dust concentration decreases slightly along the height
of duct, the leading flame edge propagates upwards at a constant velocity.
The maximum upward propagating velocity is 0.50 mis at a dust concentratio
n of 170 g/m(3). Behind the upward propagating flame, some downward propaga
ting flames are also observed. Despite the employment of nearly equal sized
particles and its good dispersability and flowability, the reaction zone i
n lycopodium particles cloud shows the double flame structure in which isol
ated individual burning particles (0.5-1.0 mm in diameter) and the ball-sha
ped flames (2-4 mm in diameter; the combustion time of 4-6 ms) surrounding
several particles are included. The ball-shaped flame appears as a faint fl
ame in which several luminous spots are distributed, and then it turns into
a luminous flame before disappearance. In order to distinguish these ball-
shaped flames from others with some exceptions for merged flames, they are
defined as independent flames in this study. The flame thickness in a lycop
odium dust flame is observed to be 20 mm, about several orders of magnitude
higher than that of a premixed gaseous flame. From the microscopic visuali
zation, it was found that the flame front propagating through lycopodium pa
rticles is discontinuous and not smooth. (C) 2000 Elsevier Science Ltd. All
rights reserved.