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3.8 T Fluid–Solid Fluidized Bed Reactors w o-Phase, 195
where:
d p the diameter for spherical particles or the nominal diameter for irre - gular
shaped particles
the density of the fluid
g the gravity acceleration constant (=9.81 m 2 /cm)
the dynamic viscosity of the fluid
the f oidage ed-bed v ix
u s the superficial fluid v elocity
the sphericity of the particle
S
G the superficial mass v . elocity
Note that while the fluid density may be a function of the pressure in the bed in a com-
w
pressible flo, the superficial mass velocity is constant. The Ergun equation in the form
given in eq. (3.450) is more conenient when analyzing the effects of pressure drop in the v
fluid density.
Minimum fluidization velocity
The minimum fluidization velocity can be calculated if the pressure drop in a fluidized
bed (eq. (3.448)) is set equal to the pressure drop in a fed bed (eqs. (3.449) and
ix
(3.450)):
150 1
u 1.75 u 2 1
fm fm fm g ( ) (3.451)
s 2 d p 2 3 fm sp d 3 fm h
or
150 1
G 1.75 G 2 1 1
fm fm fm g ( ) (3.452)
h
s 2 d p 2 3 fm sp d fm
3
where:
h the hydraulic density of the particles
G fm the superf elocity elocity based on the minimum fluidization v icial mass v
fm the voidage at minimum fluidization.
This equation can be expressed as a function of the minimum Reynolds number for flu-
idization ( Re fm ) and the Archimedes number ( Ar ):
(1 ) 1
Ar 150 fm Re fm 1.75 Re fm 2 (3.453)
2 S 3 fm Sf m 3
where
3
d g )
(
Ar p h (3.454)
2