2016
DOI: 10.5772/61418
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Developments in Combustion Technology

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Cited by 10 publications
(19 citation statements)
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“…As the first approximation, t int can be considered the ignition temperature of the combustible mixture. When t int increases, the temperature difference θ int decreases and the required time τ int increases; according to the results of [24], the drying time of the fuel particle can be ignored. The gradual start of the fuel particles into the heat transfer processes in the flame and the additive dependence of the total heat content are defined by the integral of the distribution function of the deviation probability (3), and it is rational to set the integration limits from minus ∞ to the maximum fuel particle size δ max corresponding to the upper limit of integration U…”
Section: Adapting the Model To Flame Characteristicsmentioning
confidence: 99%
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“…As the first approximation, t int can be considered the ignition temperature of the combustible mixture. When t int increases, the temperature difference θ int decreases and the required time τ int increases; according to the results of [24], the drying time of the fuel particle can be ignored. The gradual start of the fuel particles into the heat transfer processes in the flame and the additive dependence of the total heat content are defined by the integral of the distribution function of the deviation probability (3), and it is rational to set the integration limits from minus ∞ to the maximum fuel particle size δ max corresponding to the upper limit of integration U…”
Section: Adapting the Model To Flame Characteristicsmentioning
confidence: 99%
“…If we assume that the interaction pattern of a burning fuel particle with the furnace atmosphere [23,24] has a surface model, which corresponds to a plane diffusion layer between a spherical particle and the furnace atmosphere, the burnout rate of the particle can be determined at G c = const according to the equation dδ/dτ = −2M c G c /ρ, where M c = 12 kg/kmol is the molar mass of carbon, ρ ≈ 800 kg/m 3 is the density of coke. The flow of burnable carbon in the flat diffusion layer, the most common model layer in simulation of moving burning particles of coal dust is assumed to be a constant to simplify the calculations, which does not contradict the actual conditions of combustion, because the boiler unit in a certain mode for a long time period supply a fuel-air mixture constant, and the fractional composition is determined by the operation of the mill devices and also with a certain mode of operation the boiler unit remains virtually unchanged.…”
Section: Adapting the Model To Flame Characteristicsmentioning
confidence: 99%
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“…The disadvantage of all these works is the consideration of reagents as separate structural parts of the combustion medium, which leads to particular methods [10]. In the theory of heat transfer, a new unified methodology is needed based on a mathematical model that includes the design features of the boiler, the torch continuum as an indivisible whole, and the continuous function of the fractional residue.…”
Section: Introductionmentioning
confidence: 99%