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Received December 14, 2000
Accepted March 16, 2001
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Transition Velocity and Bed Expansion of Two-Phase (Liquid-Solid) Fluidization Systems
Department of Chemical Engineering and Energy & Environment Research Center, Korea Advanced Institute of Science and Technology, Daejeon 305-701, Korea
dhlee@mail.kaist.ac.kr
Korean Journal of Chemical Engineering, May 2001, 18(3), 347-351(5), 10.1007/BF02699176
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Abstract
Hydrodynamic transition experiments for two-phase (liquid-solid), both upward and downward, liquid flow systems were performed in a 127-mm diameter column. The particles were 3.2-mm polymer (1,280 kg/m(3)), 5.8-mm polyethylene (910, 930, 946 kg/m(3)), 5.5-mm polystyrene (1,021 kg/m(3)) and 6.0-mm glass (2,230 kg/m(3)) spheres, with water, aqueous glycerol solution and silicone oil as liquids. The dimensionless pressure gradient increases initially with increasing liquid velocity, but decreases gradually with increasing liquid velocity beyond Ulmf due to bed expansion. The non-dimensionalized pressure gradient using the liquid/solid mixture density increases with increasing liquid velocity and then reaches a constant value close to unity beyond U(lmf). The minimum fluidization Reynolds number for liquid-solid system increases with increasing Archimedes number including both heavier and lighter than the density of the liquid phase. Ulmf should be the same for both upward and downward fluidization systems since the Ergun equation is based on the main assumption that drag force of the superficial liquid velocity, Ulmf, is equal to the net difference between gravitational and buoyancy forces.
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