2015
DOI: 10.1016/j.cej.2014.11.144
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Discrete particle simulation of solid flow in a three-dimensional blast furnace sector model

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Cited by 64 publications
(26 citation statements)
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“…In addition, it can be found that a vertebral-body deadman exists at the center of the hearth region, and thus, the W shape was obvious at the bottom of the BF model. However, as for the phenomena shown in Figure 3c1, it can be found that when the wall effect was eliminated using the cutting method, the plug flow zone covers most of the area in the BF, which agrees well with the observation shown in the 3D full-circle BF model [27].…”
Section: Vertical Section Of the Solid Flow In The Experimental Bf Modelsupporting
confidence: 85%
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“…In addition, it can be found that a vertebral-body deadman exists at the center of the hearth region, and thus, the W shape was obvious at the bottom of the BF model. However, as for the phenomena shown in Figure 3c1, it can be found that when the wall effect was eliminated using the cutting method, the plug flow zone covers most of the area in the BF, which agrees well with the observation shown in the 3D full-circle BF model [27].…”
Section: Vertical Section Of the Solid Flow In The Experimental Bf Modelsupporting
confidence: 85%
“…Therefore, in future experiments and simulations, the vertical section of the solid flow should be used to analyze the characteristics of the plug and convergence flows, which is consistent with the literature [25,26]. The experimental cutting method can solve the problem of the wall effect on the burden descending in shaft furnaces, which might have important implications for various industrial applications [24][25][26][27].…”
Section: Vertical Section Of the Solid Flow In The Experimental Bf Modelsupporting
confidence: 59%
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“…The torques acting on particle i by particle j include: M t,ij generated by tangential force, M r,ij commonly known as the rolling friction torque. Their expressions have been listed in the previous publications [26,34,[39][40][41]. In the energy governing equation, k i is the number of particles exchanging heat with particle i, Q i,j is the heat flux between particles i and j due to conduction, Q i,f the heat flux by convection between particle i and its local surrounding fluid, and Q i,rad the heat flux between particle i and its surrounding environment by radiation.…”
Section: Governing Equations For Particlesmentioning
confidence: 99%
“…The approach has been used by many investigators to study coal combustion [30,31], air drying [32], olefin polymerization [33] and the heat transfer in packed and fluidized bed [34][35][36]. A number of attempts have also been made to study multiphase flow in a blast furnace by CFD-DEM [37][38][39][40][41], but few studies are carried out on the heat transfer.…”
Section: Introductionmentioning
confidence: 99%