RESEARCH ARTICLE

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

  • Zheng WANG 1,2 ,
  • Zai-Sha MAO 1 ,
  • Chao YANG , 1 ,
  • Qinghua ZHANG 1 ,
  • Jingcai CHENG 1
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  • 1. National Engineering Laboratory for Hydrometallurgical Cleaner Production Technology, Institute of Process Engineering, Chinese Academy of Sciences, Beijing 100190, China
  • 2. State Key Laboratory of Chemical Safety and Control, SINOPEC Qingdao Research Institute of Safety Engineering, Qingdao 266071, China

Received date: 24 Sep 2008

Accepted date: 18 Mar 2009

Published date: 05 Sep 2009

Copyright

2014 Higher Education Press and Springer-Verlag Berlin Heidelberg

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.

Cite this article

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[J]. Frontiers of Chemical Science and Engineering, 2009 , 3(3) : 272 -281 . DOI: 10.1007/s11705-009-0023-x

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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