CFD analysis of turbulence non-homogeneity in mixing vessels: A two-compartment model

Abstract A two-compartment model has been developed for calculating the droplet/particle size distribution in suspension polymerization reactors by taking into account the large spatial variations of the turbulent kinetic energy and its dissipation rate in the vessel. The two-compartment model comprised two mixing zones, namely an impeller zone of high local energy dissipation rates and a circulation zone of low kinetic energy. Computational fluid dynamics (CFD) was employed for generating the spatial distribution of energy dissipation rates within an unbaffled mixing vessel agitated by a flat two-blade impeller. A general methodology was developed for extracting, from the results of the CFD simulations, the volume ratio of the impeller over the circulation zone, the ratio of the average turbulent dissipation rates in the two zones, and the exchange flow rate between the two compartments. The effect of agitation rate, continuous phase viscosity, impeller diameter, and mixing vessel scale on the two-compartment model parameters was elucidated. The two-compartment model was then applied to a non-homogeneous liquid–liquid dispersion process to calculate the time evolution of the droplet size distribution in the mixing vessel. An excellent agreement was obtained between theoretical and experimental results on droplet size distributions obtained from a laboratory-scale reactor operated over a wide range of experimental conditions.

[1]  Lawrence L. Tavlarides,et al.  Description of interaction processes in agitated liquid-liquid dispersions , 1977 .

[2]  Alexander Penlidis,et al.  An Updated Review on Suspension Polymerization , 1997 .

[3]  T. A. Engh,et al.  Flow induced by an impeller in an unbaffled tank—II. Numerical modelling , 1994 .

[4]  John R. Bourne,et al.  Investigation of micromixing in stirred tank reactors using parallel reactions , 1994 .

[5]  Robert S. Cherry,et al.  Cellular response to agitation characterized by energy dissipation at the impeller tip , 1996 .

[6]  Ryszard Pohorecki,et al.  Mixing-precipitation model with application to double feed semibatch precipitation , 1995 .

[7]  A. D. Gosman,et al.  Full flow field computation of mixing in baffled stirred vessels , 1993 .

[8]  M. S. Doulah An Effect of Hold-up on Drop Sizes in Liquid-Liquid Dispersions , 1975 .

[9]  Gerhart Eigenberger,et al.  Applicability of the standard k–ε turbulence model to the dynamic simulation of bubble columns. Part II:: Comparison of detailed experiments and flow simulations , 1999 .

[10]  Costas Kiparissides,et al.  Use of CFD in prediction of particle size distribution in suspension polymer reactors , 1998 .

[11]  A.M.O. Smith,et al.  Turbulence models and their application in hydraulics: W. Rodi, University of Karlsruhe, International Association for Hydraulic Research, Rotterdamseweg 185, 2600 MH Delft, The Netherlands , 1981 .

[12]  Dynamic simulation of agitated liquid-liquid dispersions. II: Experimental determination of breakage and coalescence rates in a stirred tank , 1987 .

[13]  A. W. Nienow,et al.  Impeller Power Numbers in Closed Vessels , 1971 .

[14]  Milorad P. Dudukovic,et al.  Dynamic simulation of bubbly flow in bubble columns , 1999 .

[15]  Suzanne M. Kresta,et al.  Prediction of the three-dimensional turbulent flow in stirred tanks , 1991 .

[16]  van den Cm Bleek,et al.  Eulerian simulations of bubbling behaviour in gas-solid fluidised beds , 1998 .

[17]  Aydin K. Sunol,et al.  Chemical plant fault diagnosis through a hybrid symbolic-connectionist machine learning approach , 1998 .

[18]  R. Torvik,et al.  Modelling of slurry reactors. A fundamental approach , 1990 .

[19]  S. T. Johansen,et al.  Flow induced by an impeller in an unbaffled tank—I. Experimental , 1994 .

[20]  Martin E. Weber,et al.  Flow phenomena in stirred tanks. Part I. The impeller stream , 1975 .

[21]  J. C. Middleton,et al.  Computations of flow fields and complex reaction yield in turbulent stirred reactors, and comparison with experimental data , 1986 .

[22]  L. A. Cutter Flow and turbulence in a stirred tank , 1966 .

[23]  C. M. Stoots,et al.  Flow in the impeller region of a stirred tank , 1989 .

[24]  Ivan Fořt,et al.  Turbulent flow in stirred tanks. Part II: A two‐scale model of turbulence , 1986 .

[25]  Philippe A. Tanguy,et al.  Mixing performance induced by coaxial flat blade-helical ribbon impellers rotating at different speeds , 1997 .

[26]  Piero M. Armenante,et al.  Velocity profiles in a baffled vessel with single or double pitched-blade turbines , 1996 .

[27]  D. Ramkrishna The Status of Population Balances , 1985 .

[28]  N. Markatos,et al.  The mathematical modelling of turbulent flows , 1986 .

[29]  Jos Derksen,et al.  Large eddy simulations on the flow driven by a Rushton turbine , 1999 .

[30]  K. S. Gandhi,et al.  A two-zone model of breakage frequency of drops in stirred dispersions , 1994 .

[31]  D. B. Holmes,et al.  Fluid flow in turbine-stirred, baffled tanks—I: Circulation time , 1964 .

[32]  Vivek V. Ranade,et al.  FLOW GENERATED BY PITCHED BLADE TURBINES II: SIMULATION USING κ-ε MODEL , 1989 .

[33]  Catherine Xuereb,et al.  3-D hydrodynamics in a tank stirred by a double-propeller system and filled with a liquid having evolving rheological properties , 1996 .

[34]  Petr Kadlec,et al.  Distribution of energy dissipation rate in an agitated gas-liquid system , 1993 .

[35]  G. K. Patterson,et al.  Laser-Doppler measurements of turbulent-flow parameters in a stirred mixer , 1989 .

[36]  Marco Vanni,et al.  Aggregation of small particles in turbulent liquid flows , 1996 .

[37]  Costas Tsouris,et al.  Breakage and coalescence models for drops in turbulent dispersions , 1994 .

[38]  Jerzy Bałdyga,et al.  Interactions between mixing on various scales in stirred tank reactors , 1992 .

[39]  A. D. Gosman,et al.  Multidimensional modeling of turbulent two‐phase flows in stirred vessels , 1992 .

[40]  E. Chatzi,et al.  Steady‐state drop‐size distributions in high holup fraction dispersion systems , 1995 .

[41]  Ville Alopaeus,et al.  Simulation of the population balances for liquid-liquid systems in a nonideal stirred tank. Part 1: Description and qualitative validation of the model , 1999 .

[42]  C. K. Harris,et al.  Computational Fluid Dynamics for Chemical Reactor Engineering , 1996 .

[43]  Suzanne M. Kresta,et al.  Importance of using the correct impeller boundary conditions for CFD simulations of stirred tanks , 1994 .

[44]  L. Steiner,et al.  Dynamic simulation of liquid-liquid agitated dispersions—I. Derivation of a simplified model , 1987 .

[45]  Costas Kiparissides,et al.  Prediction of particle size distribution in suspension polymerization reactors: effect of turbulence nonhomogeneity , 2000 .

[46]  L. Tavlarides,et al.  Modeling of turbulent, neutrally buoyant droplet suspensions in liquids , 1987 .

[47]  Cui Yq,et al.  Compartment Mixing Model for Stirred Reactors with Multiple Impellers , 1996 .

[48]  Reuel Shinnar,et al.  On the behaviour of liquid dispersions in mixing vessels , 1961, Journal of Fluid Mechanics.

[49]  Lawrence L. Tavlarides,et al.  Turbulent flow in stirred tanks. Part I: Turbulent flow in the turbine impeller region , 1985 .

[50]  E. Papoutsakis,et al.  Damage mechanisms of suspended animal cells in agitated bioreactors with and without bubble entrainment , 1990, Biotechnology and bioengineering.