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DOE-HDBK-3010-94
3.0 Liquids; Aqueous Solutions
ligaments formed from surface disruption); droplets generated by all three
droplet generation mechanisms (i.e., bubble bursting, splashing, or foaming).
Three regions as a function of axial distance from the pool surface were identified:
1.
near-surface region: immediate vicinity of surface; entrainment dependent on
height and gas velocity; entrainment consists of all droplets entrained.
2.
momentum-controlled region: intermediate axial distances above pool surface;
entrainment consists of droplets with initial momentum to reach height and
droplets whose terminal velocity is equal to or less than the superficial gas
velocity; three regimes as a function of superficial gas velocity in region:
low gas flux: entrainment small and consists of very fine droplets; Efg
approximately proportional to gas flux.
intermediate gas flux: larger drops ejected from pool; Efg increases with
the 3rd or 4th power of the superficial gas velocity.
high gas flux: large gas slugs form and pool surface highly agitated;
considerable droplets formed by splashing; Efg increases with the 7th to
20th power of the superficial gas velocity.
3.
deposition-controlled region: entrained droplets of size whose terminal velocity
is equal to or less than the superficial gas velocity.
A simple mechanistic model was developed based on the concepts presented above. Due to
the enormous number of droplets generated, the motion of individual droplets could not be
followed individually, and so droplet motion was handled statistically. Important physical
parameters and distribution functions essential to the modeling and calculations were
developed or assumed. Correlations for the height criteria and entrainment in each region
were developed as a function of:
~ jg/[σg ρg2]1/4
dimensionless gas velocity, jg*
=
(3-2)
h/[σ/g ∆ρ]1/2
dimensionless height above surface, h* =
(3-3)
g/[ρg σ (σ/g ∆ρ)1/2]1/2
gas viscosity number, Ng
=
(3-4)
DH/ [σ/g ∆ρ]1/2
dimensionless vessel diameter, D*H
=
(3-5)
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