CFD simulation of solid–liquid stirred tanks

Solid liquid stirred tanks are commonly used in the minerals industry for operations like concentration, leaching, adsorption, effluent treatment, etc. Computational Fluid Dynamics (CFD) is increasingly being used to predict the hydrodynamics and performance of these systems. Accounting for the soli...

Full description

Bibliographic Details
Main Authors: Wadnerkar, Divyamaan, Utikar, Ranjeet, Tade, Moses, Pareek, Vishnu
Format: Journal Article
Published: Elsevier 2012
Subjects:
Online Access:http://hdl.handle.net/20.500.11937/14891
_version_ 1848748744643706880
author Wadnerkar, Divyamaan
Utikar, Ranjeet
Tade, Moses
Pareek, Vishnu
author_facet Wadnerkar, Divyamaan
Utikar, Ranjeet
Tade, Moses
Pareek, Vishnu
author_sort Wadnerkar, Divyamaan
building Curtin Institutional Repository
collection Online Access
description Solid liquid stirred tanks are commonly used in the minerals industry for operations like concentration, leaching, adsorption, effluent treatment, etc. Computational Fluid Dynamics (CFD) is increasingly being used to predict the hydrodynamics and performance of these systems. Accounting for the solid–liquid interaction is critical for accurate predictions of these systems. Therefore, a careful selection of models for turbulence and drag is required. In this study, the effect of drag model was studied. The Eulerian–Eulerian multiphase model is used to simulate the solid suspension in stirred tanks. Multiple reference frame (MRF) approach is used to simulate the impeller rotation in a fully baffled tank. Simulations are conducted using commercial CFD solver ANSYS Fluent 12.1. The CFD simulations are conducted for concentration 1% and 7% v/v and the impeller speeds above the “just suspension speed”.It is observed that high turbulence can increase the drag coefficient as high as forty times when compared with a still fluid. The drag force was modified to account for the increase in drag at high turbulent intensities. The modified drag is a function of particle diameter to Kolmogorov length scale ratio, which, on a volume averaged basis, was found to be around 13 in the cases simulated. The modified drag law was found to be useful to simulate the low solids holdup in stirred tanks. The predictions in terms of velocity profiles and the solids distribution are found to be in reasonable agreement with the literature experimental data. Turbulent kinetic energy, homogeneity and cloud height in the stirred tanks are studied and discussed in the paper. The presence of solids resulted in dampening of turbulence and the maximum deviation was observed in the impeller plane. The cloud height and homogeneity were found to increase with an increase in impeller speed. The work provides an insight into the solid liquid flow in stirred tanks.
first_indexed 2025-11-14T07:09:55Z
format Journal Article
id curtin-20.500.11937-14891
institution Curtin University Malaysia
institution_category Local University
last_indexed 2025-11-14T07:09:55Z
publishDate 2012
publisher Elsevier
recordtype eprints
repository_type Digital Repository
spelling curtin-20.500.11937-148912017-09-13T15:02:13Z CFD simulation of solid–liquid stirred tanks Wadnerkar, Divyamaan Utikar, Ranjeet Tade, Moses Pareek, Vishnu Homogeneity Drag models CFD Hydrodynamic study Solid–liquid suspension Cloud height Stirred tanks Solid liquid stirred tanks are commonly used in the minerals industry for operations like concentration, leaching, adsorption, effluent treatment, etc. Computational Fluid Dynamics (CFD) is increasingly being used to predict the hydrodynamics and performance of these systems. Accounting for the solid–liquid interaction is critical for accurate predictions of these systems. Therefore, a careful selection of models for turbulence and drag is required. In this study, the effect of drag model was studied. The Eulerian–Eulerian multiphase model is used to simulate the solid suspension in stirred tanks. Multiple reference frame (MRF) approach is used to simulate the impeller rotation in a fully baffled tank. Simulations are conducted using commercial CFD solver ANSYS Fluent 12.1. The CFD simulations are conducted for concentration 1% and 7% v/v and the impeller speeds above the “just suspension speed”.It is observed that high turbulence can increase the drag coefficient as high as forty times when compared with a still fluid. The drag force was modified to account for the increase in drag at high turbulent intensities. The modified drag is a function of particle diameter to Kolmogorov length scale ratio, which, on a volume averaged basis, was found to be around 13 in the cases simulated. The modified drag law was found to be useful to simulate the low solids holdup in stirred tanks. The predictions in terms of velocity profiles and the solids distribution are found to be in reasonable agreement with the literature experimental data. Turbulent kinetic energy, homogeneity and cloud height in the stirred tanks are studied and discussed in the paper. The presence of solids resulted in dampening of turbulence and the maximum deviation was observed in the impeller plane. The cloud height and homogeneity were found to increase with an increase in impeller speed. The work provides an insight into the solid liquid flow in stirred tanks. 2012 Journal Article http://hdl.handle.net/20.500.11937/14891 10.1016/j.apt.2012.03.007 Elsevier restricted
spellingShingle Homogeneity
Drag models
CFD
Hydrodynamic study
Solid–liquid suspension
Cloud height
Stirred tanks
Wadnerkar, Divyamaan
Utikar, Ranjeet
Tade, Moses
Pareek, Vishnu
CFD simulation of solid–liquid stirred tanks
title CFD simulation of solid–liquid stirred tanks
title_full CFD simulation of solid–liquid stirred tanks
title_fullStr CFD simulation of solid–liquid stirred tanks
title_full_unstemmed CFD simulation of solid–liquid stirred tanks
title_short CFD simulation of solid–liquid stirred tanks
title_sort cfd simulation of solid–liquid stirred tanks
topic Homogeneity
Drag models
CFD
Hydrodynamic study
Solid–liquid suspension
Cloud height
Stirred tanks
url http://hdl.handle.net/20.500.11937/14891