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Power consumption and gas–liquid dispersion in turbulently agitated vessels with vertical dual-array tubular coil baffles

  • Xun Wan , Yasuyuki Takahata und Koji Takahashi EMAIL logo
Veröffentlicht/Copyright: 2. Februar 2016
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Abstract

In this work vertical dual-array tubular coil baffles arranged in groups of four, six or eight were investigated and the results compared with those from four planar baffles. The baffle coefficients for a single phase, along with the power consumption and gas hold-up in the gas–liquid phase of a system with the various baffle configurations for single and triple Rushton turbines are presented. Measurements were carried out using a dish-bottom vessel with an inner diameter of 0.29 m. Two ambient-temperature media were used as the liquid phase, namely, tap water and a 0.5 M Na2SO4 aqueous solution, representing coalescent and non-coalescent liquids, respectively. The results of the single-phase experiment revealed the coil baffles to have lower power numbers; when the baffle coefficient is ≥ 0.12, the mixing efficiency is the same as that for four planar baffles. The power consumption experiment using the gas–liquid phase showed that installing coil baffles prevented a large power draw in all types of media. In addition, the power draw characteristics are affected by the media. It was found that, because of the low KB number, flooding occurred more readily with coil baffles than with planar baffles. Gas–liquid dispersion experiments in an air–water system indicated that, at a low gas flow-rate, the gas hold-up values of the coil baffles were almost 60 % higher than those of the conventional four baffles. However, this phenomenon was not observed in the Na2SO4 aqueous solution because of the existence of dead zones in viscous liquids. Finally, all the data from the power consumption and gas hold-up experiments on the gas–liquid phase were correlated.

Symbols

acoefficient in Eq. (4)
bexponent in Eq. (4)
b′length of impeller bladem
Bwidth of bafflem
cexponent in Eq. (4)
c′distance between baffle and vesselm
Cdistance between bottom impeller and bottom of the tankm
douter diameter of tube of inner coilsm
ddisc diameterm
Ddiameter of impellerm
Flggas flow number
FrFroude number
gacceleration due to gravitym2 s-1
hdistance between impellersm
Hheight of liquidm
Hgliquid height under gassed conditionm
H0liquid height under un-gassed conditionm
Hliquid-level correction coefficientm
KBbaffle coefficient
KBFKB number with complete baffles (KBF = 0.35)
KBNKB number without baffles (KBN = 0)
nbnumber of baffles
Nstirrer speedmin-1
NPpower number [NP = P/(ρLN3D5)]
NPFNP number with complete baffles
NPNNP number without baffles
P0power drawn under un-gassed conditionW
Pgpower drawn under gassed conditionW
PFflooding point
Qggas flow-ratem3 s-1
sgas outlet positionm
tm,99homogenisation time to reach 99 %s
Tdiameter of tankm
Vvolume of liquidm3
VSsuperficial gas velocitymm s-1
wwidth of bladem
Greek Letters
αcoefficient in Eq. (7)
βexponent in Eq. (7)
γexponent in Eq. (7)
εgas hold-up, dimensionless
μviscosity of materialPa s
ρLliquid densitykg m-3
σsurface tensionmN m-1

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Received: 2015-3-1
Revised: 2015-8-5
Accepted: 2015-8-5
Published Online: 2016-2-2
Published in Print: 2016-4-1

© 2015 Institute of Chemistry, Slovak Academy of Sciences

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