UPWARD BUOYANT FILTRATION COMBUSTION

Citation
Ap. Aldushin et al., UPWARD BUOYANT FILTRATION COMBUSTION, Journal of engineering mathematics, 31(2-3), 1997, pp. 205-234
Citations number
20
Categorie Soggetti
Computer Application, Chemistry & Engineering",Mathematics,Engineering
ISSN journal
00220833
Volume
31
Issue
2-3
Year of publication
1997
Pages
205 - 234
Database
ISI
SICI code
0022-0833(1997)31:2-3<205:UBFC>2.0.ZU;2-V
Abstract
Heterogeneous combustion in a porous sample with only the top and bott om ends of the sample open to gas flow is considered. Gas enters the s ample due to buoyant upward convection. That is, ignition at the botto m produces an upwardly propagating filtration combustion wave which in duces hot gas to rise, thus pulling cool, fresh gas containing oxidize r in through the bottom of the sample. The gas moves through the solid products to reach the reaction zone just as in forced forward filtrat ion combustion. In contrast to forced forward filtration combustion, i n which the incoming gas flux is fixed by an external source, here the incoming gas flux is determined by the combustion process itself. Tha t is, the incoming gas flux is determined by the burning temperature w hich in turn is affected by the incoming gas flux. Thus, a feedback me chanism exists which hinders ignition of the samples, but also makes t he wave hard to extinguish, once it has formed. A one-dimensional mode l is analyzed and two types of wave structure, termed reaction-leading and reaction-trailing according as the reaction occurs at the leading or trailing edge of the heated region of the sample, respectively, ar e determined. For each structure, two solution modes are described, te rmed stoichiometric and kinetically controlled, according as the rate of oxygen supply or the kinetics controls propagation of the wave. In each of these four situations, expressions are derived for the evoluti on of the burning temperature, propagation velocity, incoming gas flux , degree of oxidizer consumption and degree of fuel conversion as the wave moves through the sample. In addition, profiles for the temperatu re are described. Analysis of the case where significant heat is lost through the sides of the sample leads to extinction limits and demonst rates the sensitivity of the wave structure to changes in external hea t losses.