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Mechanisms for the ignition of pulverized coal particles

โœ Scribed by V.S. Gururajan; T.F. Wall; R.P. Gupta; J.S. Truelove


Publisher
Elsevier Science
Year
1990
Tongue
English
Weight
726 KB
Volume
81
Category
Article
ISSN
0010-2180

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โœฆ Synopsis


A detailed model for the steady-state combustion of a coal particle considering both surface oxidation and volatile combustion is presented. By solving the model equations in the absence of surface oxidation at various ambient gas temperatures, the homogeneous ignition temperature is determined as the gas temperature at which the mass consumption rate of the particle shows a jump, i.e., a transition from a low-temperature regime with little combustion of volatiles in the boundary layer to a high-temperature regime where essentially all volatiles burn. This ignition temperature is shown to be inversely related to particle size and oxygen concentration, as has been observed experimentally. The application of the flame sheet approximation is shown to overestimate the ignition temperature in most of the cases considered and to predict the incorrect dependence of the ignition temperature on the oxygen concentration. Solution of the model equations considering both surface oxidation and volatile combustion shows that surface oxidation influences the ignition temperature of only small particles or at high oxygen concentrations. When the surface oxidation rate of the particle is high, two ignition jumps, the first due to the heterogeneous mechanism and the second due to the homogeneous mechanism, are observed. NOMENCLATURE OF Ac, Ag, Ap preexponential factor in rp surface oxidation, devolatilization, R and volatile combustion kinetics Cpg specific heat of gas (1.0 kJ/kg K) D ditfusivity of gas (m2/s) T


๐Ÿ“œ SIMILAR VOLUMES


The mechanism of ignition of pulverized
โœ J.B. Howard; R.H. Essenhigh ๐Ÿ“‚ Article ๐Ÿ“… 1965 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 240 KB

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We present a novel experiment to study the ignition of pulverized coal. A dilute stream of particles is dropped into a laminar, upward-flow wind tunnel with a quartz test section. The gas stream is not preheated. A single pulse from a Nd:YAG laser is focused through the tunnel and ignites the fuel.

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