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Fluid-to-Particle Heat Transfer in Fluidized Beds

DOI 10.1615/hedhme.a.000172

2.5.5 Fluid-to-particle heat transfer in fluidized beds

A. Introduction, range of fluidization, bed expansion

Fluidization of solid particles by a streaming gas or liquid requires a fluid velocity u in the range

\[\label{eq1} u_{mf}\lt u \lt u_{t}\tag{1}\]

where umf is the so-called minimum fluidization velocity and ut is the terminal velocity. The minimum fluidization velocity umf can be found from a force balance equating the pressure drop of a fixed bed to the weight of the particle (— buoyancy force) per cross-sectional area. Using Ergun's equation (Ergun, 1952) for the pressure drop of the fixed bed, one obtains the Reynolds number Remfpfumfd /ηf as a function of Archimedes number Argd3ρf (ρpρf) ηf2 and void fraction at minimum fluidization ψmf (see Section 148):

\[\label{eq2} \mbox{Re}_{mf}=42.9(1-\psi_{mf})\left[ \sqrt{1+\dfrac{\psi_{mf}^{3}}{(1-\psi_{mf})^{2}}\,\dfrac{\mbox{Ar}}{3,214}}-1\right] \tag{2}\]

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