Hydrodynamic difference between inline and batch operation of a rotor-stator mixer head - A CFD approach

Rotor-stator mixers (RSMs) can be operated in either batch or inline mode. When operating a rotor-stator geometry in batch mode, it typically experiences an order of magnitude higher volumetric flow through the stator than in inline mode. This is expected to cause differences in the flow and turbulence in the rotor-stator region. This study uses computational fluid dynamics (CFD) to study the hydrodynamic differences in and near the stator hole as a function of volumetric flow rates between those experienced in inline and batch modes of operation. It is concluded that both radial flow profiles and turbulent kinetic energy across a range of rotor speeds and flow rates can be described by a velocity ratio: average tangential fluid velocity in the stator hole divided by the rotor tip speed. Moreover, the position where dissipation of turbulent kinetic energy takes place—and hence the effective region of dispersion or mixing—differs between the two modes of operation. The relative importance of the two regions can be described in terms of the velocity ratio and the transition can be predicted based on the relative power input due to rotational and pumping power of the mixer. This study provides a starting point for understanding differences between emulsification efficiency between inline and batch modes of operation with relevance for both equipment design and process scale-up. (Less)

[1]  Wei Li,et al.  LDA measurements and CFD simulations of an in‐line high shear mixer with ultrafine teeth , 2014 .

[2]  Gül Özcan-Taşkin,et al.  Power and flow characteristics of three rotor-stator heads , 2011 .

[3]  A. Håkansson,et al.  Model emulsions to study the mechanism of industrial mayonnaise emulsification , 2016 .

[4]  T. Shih,et al.  A new k-ϵ eddy viscosity model for high reynolds number turbulent flows , 1995 .

[5]  A. Pacek,et al.  Flow pattern, periodicity and energy dissipation in a batch rotor–stator mixer , 2008 .

[6]  Adam J. Kowalski,et al.  Scaling up of silverson rotor–stator mixers , 2011 .

[7]  Adam J. Kowalski,et al.  Power consumption characteristics of an in-line silverson high shear mixer , 2012 .

[8]  Adam J. Kowalski,et al.  Power characteristics of in-line rotor stator mixers , 2014 .

[9]  S. Pope Turbulent Flows: FUNDAMENTALS , 2000 .

[10]  Y. Liao,et al.  A literature review of theoretical models for drop and bubble breakup in turbulent dispersions , 2009 .

[11]  A. Kowalski,et al.  Droplet break-up by in-line Silverson rotor–stator mixer , 2011 .

[12]  Lasse Rosendahl,et al.  Characteristics of batch rotor–stator mixer performance elucidated by shaft torque and angle resolved PIV measurements , 2011 .

[13]  Tetsu Kamiya,et al.  Evaluation Method of Homogenization Effect for Different Stator Configurations of Internally Circulated Batch Rotor-Stator Mixers , 2010 .

[14]  Richard V. Calabrese,et al.  Drop breakup in turbulent stirred‐tank contactors. Part I: Effect of dispersed‐phase viscosity , 1986 .

[15]  Adam J. Kowalski,et al.  Expression for turbulent power draw of an in-line Silverson high shear mixer , 2011 .

[16]  A. Pacek,et al.  The effect of stator geometry on the flow pattern and energy dissipation rate in a rotor-stator mixer , 2009 .

[17]  A. Pacek,et al.  The effect of scale and interfacial tension on liquid–liquid dispersion in in-line Silverson rotor–stator mixers☆ , 2013 .

[18]  Arno Kwade,et al.  Scale-up of the power draw of inline-rotor–stator mixers with high throughput , 2015 .

[19]  W. Li,et al.  High shear mixers: A review of typical applications and studies on power draw, flow pattern, energy dissipation and transfer properties , 2012 .

[20]  Michael Yianneskis,et al.  Observations on the Distribution of Energy Dissipation in Stirred Vessels , 2000 .

[21]  J. Hinze Fundamentals of the hydrodynamic mechanism of splitting in dispersion processes , 1955 .