Numerical investigation of the influence of kinetics and shape factor on barium sulfate precipitation in a continuous stirred tank

Zheng WANG, Zai-Sha MAO, Chao YANG, Qinghua ZHANG, Jingcai CHENG

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PDF(481 KB)
Front. Chem. Sci. Eng. ›› 2009, Vol. 3 ›› Issue (3) : 272-281. DOI: 10.1007/s11705-009-0023-x
RESEARCH ARTICLE
RESEARCH ARTICLE

Numerical investigation of the influence of kinetics and shape factor on barium sulfate precipitation in a continuous stirred tank

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Abstract

The effect of kinetics and shape factor on barium sulfate precipitation in a continuous stirred tank has been investigated numerically through solving the standard momentum and mass transport equations in combination with the moment equations for crystal population balance. The numerical method was validated with the literature data. The simulated results include the distribution of the local supersaturation ratio in the reactor, the mean crystal size, and the coefficient of variation. The simulation results show that the value of shape factor used in the model affected greatly the mean crystal size and the moments of the crystal size distribution. The influence of the kinetic expressions on the simulation is also analyzed. It is important to investigate the relationship of the shape factor with the precipitator type and other operation conditions to obtain reliable simulation results and suitable kinetic equations of crystal nucleation and growth rates.

Keywords

stirred tank / numerical simulation / precipitation / shape factor / crystal kinetics

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Zheng WANG, Zai-Sha MAO, Chao YANG, Qinghua ZHANG, Jingcai CHENG. Numerical investigation of the influence of kinetics and shape factor on barium sulfate precipitation in a continuous stirred tank. Front Chem Eng Chin, 2009, 3(3): 272‒281 https://doi.org/10.1007/s11705-009-0023-x

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Acknowledgements

Financial support from the National Natural Science Foundation of China (Grant Nos. 20236050, 50404009 and 50134020), the National Basic Research Priorities Program (No. 2004CB217604) and the National High Technology Research and Development Program of China (Grant No. 2007AA060904) is gratefully acknowledged.
Nomenclature
bwidth of baffle, m
Bnucleation rate, #·m-3·s-1
Cclearance of impeller to tank bottom, m
C.V. coefficient of variation defined by Eq. (9)
cconcentration, kmol·m-3
ddiameter of impeller, m
d32mean particle size, m
Ggrowth rate, m·s-1
Hheight of the tank, m
Kspsolubility product, kmol2·m-6
kturbulent kinetic energy m2·s-2
kvThe volumetric crystal shape factor
L43mean particle size, m
Mcmole mass of the crystal, kg·kmol-1
Mtmass concentration of crystal, kg·m-3
mjjth moment of crystal size distribution, mj·m-3
Nimpeller speed, r·min-1
rradial coordinate, m
Sasupersaturation ratio
Scturbulent Schmidt number
Sgspecific crystal growth rate
Ttank diameter, m
u, v, wvelocity of liquid phase in r, θ, z direction, m·s-1
Xjconversion ratio of ion j
zaxial coordinate, m
μeffeffective viscosity, m2·s-1
Γeffdiffusion coefficient, m2·s-1
ϕgeneral variable
θtangential coordinate, rad
ρsolution density, kg·m-3
ρcrystaldensity, kg·m-3
τmean residence time, s
ϵturbulent energy dissipation rate, W·kg-1
ΔcSupersaturation, kmol·m-3

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