Numerical simulation of fluid dynamics in the stirred tank by the SSG Reynolds Stress Model

Nana QI, Hui WANG, Kai ZHANG, Hu ZHANG

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PDF(537 KB)
Front. Chem. Sci. Eng. ›› 2010, Vol. 4 ›› Issue (4) : 506-514. DOI: 10.1007/s11705-010-0508-7
RESEARCH ARTICLE
RESEARCH ARTICLE

Numerical simulation of fluid dynamics in the stirred tank by the SSG Reynolds Stress Model

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Abstract

The Speziale, Sarkar and Gatski Reynolds Stress Model (SSG RSM) is utilized to simulate the fluid dynamics in a full baffled stirred tank with a Rushton turbine impeller. Four levels of grid resolutions are chosen to determine an optimised number of grids for further simulations. CFD model data in terms of the flow field, trailing vortex, and the power number are compared with published experimental results. The comparison shows that the global fluid dynamics throughout the stirred tank and the local characteristics of trailing vortices near the blade tips can be captured by the SSG RSM. The predicted mean velocity components in axial, radial and tangential direction are also in good agreement with experiment data. The power number predicted is quite close to the designed value, which demonstrates that this model can accurately calculate the power number in the stirred tank. Therefore, the simulation by using a combination of SSG RSM and MRF impeller rotational model can accurately model turbulent fluid flow in the stirred tank, and it offers an alternative method for design and optimisation of stirred tanks.

Keywords

stirred tank / fluid dynamics / numerical simulation / SSG Reynolds Stress Model / MRF

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Nana QI, Hui WANG, Kai ZHANG, Hu ZHANG. Numerical simulation of fluid dynamics in the stirred tank by the SSG Reynolds Stress Model. Front Chem Eng Chin, 2010, 4(4): 506‒514 https://doi.org/10.1007/s11705-010-0508-7

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Acknowledgements

Financial support from the Major State Basic Research Development Program of China (973 Program, Grant No. 2005CB221205) was gratefully acknowledged. Ms. Qi would like to acknowledge financial support from the China Scholarship Council (CSC) during her stay at the University of Adelaide, Australia.
Nomenclature
Bsum of body force, N/m3
cµRsϵRSconstants in the SSG RSM
csconstant in the SSG RSM
cϵ1,cϵ2constants in the SSG RSM
Cs1,Cs2Constants in the SSG RSM
Cr1~Cr5constants in the SSG RSM
ddiameter of the impeller, m
Ddiameter of Rushton turbine, m
Fexternal force, N/m3
Hheight of the tank, m
Idefdefault turbulent intensity of 5%, m2/s2
Nrotation speed, 1/s
Nppower number
ppressure, Pa
Rdiameter of the tank, m
Tinner diameter of the tank, m
Tqtotal torque, N·m
uturbulent velocity, m/s
Uaverage velocity, m/s
wbaffle width, m
Greek letters
δKronecker delta, when i=j, δ=1; when i≠j, δ=0
eturbulence dissipation rate, m2/s3
κturbulence kinetic energy per unit mass, m2/s2
µviscosity, Pa ·s
ξbulk viscosity, Pa ·s
rdensity, kg/m3
ϕijpressure-strain correlation in the SSG model, kg · m /s3
Subscripts
i, j, kCartesian coordinate direction vector

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