The critical conditions for coalescence in phase field simulations of colliding droplets in shear.

Simulations have been performed using the free-energy binary-liquid lattice Boltzmann method with sufficient resolution that the critical capillary number for coalescence was determined for collisions between droplets in simple shear with a small initial offset in the shear gradient direction. The simulations were used to study the behavior of the interacting interfaces and the film between them during collisions over a wide range of capillary numbers with emphasis on near-critical conditions. From these three-dimensional simulations with deforming interfaces, several features of the evolution of the film between the drops were observed. The critical film thickness was determined to be similar to the interface thickness, a power law described the dependence of the minimum film thickness on the capillary number in collisions without coalescece, and an inflection point was found in the dynamics of the minimum distance between drops that eventually coalesce. The rotation of the film and the flow in it were also studied, and a reversal in the flow was found to occur before coalescence. The mobility of the phase field was therefore important in the continued thinning of the film at the points of minimum thickness after the flow reversal. A comparison of the critical capillary number and critical film thickness in the simulations with the values for experiments in confined simple shear indicated that the effective physical radius of the simulated droplets was on the order of several micrometers. The results are significant for simulations of droplet interactions and emulsion flows in complex geometries and turbulence because they demonstrate the necessary scale of the computations and how parameters, such as the interface thickness and phase field mobility, should be selected for accurate results.

[1]  David J. Pine,et al.  Drop deformation, breakup, and coalescence with compatibilizer , 2000 .

[2]  I. Halliday,et al.  A local lattice Boltzmann method for multiple immiscible fluids and dense suspensions of drops , 2011, Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[3]  P. Sheng,et al.  A variational approach to moving contact line hydrodynamics , 2006, Journal of Fluid Mechanics.

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

[5]  D. Juric,et al.  A front-tracking method for the computations of multiphase flow , 2001 .

[6]  W. Agterof,et al.  Experimental Investigation of the Orthokinetic Coalescence Efficiency of Droplets in Simple Shear Flow. , 2001, Journal of colloid and interface science.

[7]  J. E. Hilliard,et al.  Free Energy of a Nonuniform System. I. Interfacial Free Energy , 1958 .

[8]  Ak Allen Chesters The modelling of coalescence processes in fluid-liquid dispersions : a review of current understanding , 1991 .

[9]  David Jacqmin,et al.  Contact-line dynamics of a diffuse fluid interface , 2000, Journal of Fluid Mechanics.

[10]  Jos Derksen,et al.  Lattice Boltzmann simulations of drop deformation and breakup in shear flow , 2014 .

[11]  Clayton D. McAuliffe,et al.  Oil-in-Water Emulsions and Their Flow Properties in Porous Media , 1973 .

[12]  D. Jacqmin Regular Article: Calculation of Two-Phase Navier–Stokes Flows Using Phase-Field Modeling , 1999 .

[13]  Ping Sheng,et al.  Molecular scale contact line hydrodynamics of immiscible flows. , 2003, Physical review. E, Statistical, nonlinear, and soft matter physics.

[14]  Kausik Sarkar,et al.  Effects of viscosity ratio and three dimensional positioning on hydrodynamic interactions between two viscous drops in a shear flow at finite inertia , 2009 .

[15]  J. Yeomans,et al.  Lattice Boltzmann simulations of contact line motion. II. Binary fluids. , 2004, Physical review. E, Statistical, nonlinear, and soft matter physics.

[16]  The effect of geometrical confinement on coalescence efficiency of droplet pairs in shear flow. , 2013, Journal of colloid and interface science.

[17]  Michał Januszewski,et al.  Simulations of gravity-driven flow of binary liquids in microchannels , 2011 .

[18]  S. Guido,et al.  Binary collision of drops in simple shear flow by computer-assisted video optical microscopy , 1998, Journal of Fluid Mechanics.

[19]  Kausik Sarkar,et al.  Spatial ordering due to hydrodynamic interactions between a pair of colliding drops in a confined shear , 2012, 1201.3813.

[20]  J. Bowman,et al.  Asymptote: the Vector Graphics Language , 2008 .

[21]  S. G. Mason,et al.  Particle motions in sheared suspensions. XIV. Coalescence of liquid drops in electric and shear fields , 1962 .

[22]  P. Bhatnagar,et al.  A Model for Collision Processes in Gases. I. Small Amplitude Processes in Charged and Neutral One-Component Systems , 1954 .

[23]  F. Toschi,et al.  Droplet size distribution in homogeneous isotropic turbulence , 2011, 1112.6041.

[24]  L. G. Leal,et al.  The coalescence of two equal-sized drops in a two-dimensional linear flow , 2001 .

[25]  Orest Shardt,et al.  Simulations of droplet coalescence in simple shear flow. , 2012, Langmuir : the ACS journal of surfaces and colloids.

[26]  James J. Feng,et al.  Can diffuse-interface models quantitatively describe moving contact lines? , 2011 .

[27]  S. G. Mason,et al.  Particle motions in sheared suspensions: VIII. Singlets and doublets of fluid spheres , 1959 .

[28]  H. Brenner,et al.  Particle motions in sheared suspensions , 1959 .

[29]  R. G. M. van der Sman,et al.  Emulsion droplet deformation and breakup with Lattice Boltzmann model , 2008, Comput. Phys. Commun..

[30]  Vittorio Cristini,et al.  An adaptive mesh algorithm for evolving surfaces: simulation of drop breakup and coalescence , 2001 .

[31]  Kausik Sarkar,et al.  Pairwise interactions between deformable drops in free shear at finite inertia , 2009 .

[32]  R. Boom,et al.  Lattice Boltzmann simulations of droplet formation in a T-shaped microchannel. , 2006, Langmuir : the ACS journal of surfaces and colloids.

[33]  J. E. Hilliard,et al.  Free Energy of a Nonuniform System. I. Interfacial Free Energy and Free Energy of a Nonuniform System. III. Nucleation in a Two‐Component Incompressible Fluid , 2013 .

[34]  Christopher W. Macosko,et al.  Drop Breakup and Coalescence in Polymer Blends: The Effects of Concentration and Compatibilization , 1995 .

[35]  E. J. Hinch,et al.  Collision of two deformable drops in shear flow , 1997, Journal of Fluid Mechanics.

[36]  Nicolas Bremond,et al.  Decompressing emulsion droplets favors coalescence. , 2008, Physical review letters.

[37]  I. Zawadzki,et al.  Equilibrium raindrop size distributions in tropical rain , 1988 .

[38]  A. Ladd Numerical simulations of particulate suspensions via a discretized Boltzmann equation. Part 2. Numerical results , 1993, Journal of Fluid Mechanics.

[39]  Cyrus K. Aidun,et al.  Lattice-Boltzmann Method for Complex Flows , 2010 .

[40]  H. Stone,et al.  Satellite and subsatellite formation in capillary breakup , 1992, Journal of Fluid Mechanics.

[41]  L. G. Leal,et al.  Viscosity ratio effects on the coalescence of two equal-sized drops in a two-dimensional linear flow , 2005, Journal of Fluid Mechanics.

[42]  David P. Schmidt,et al.  Modeling merging and breakup in the moving mesh interface tracking method for multiphase flow simulations , 2009, J. Comput. Phys..

[43]  J. McLaughlin,et al.  Lattice Boltzmann simulations of flows with fluid–fluid interfaces , 2008 .

[44]  Suppressing the coalescence in the multi-component lattice Boltzmann method , 2011 .

[45]  A. Ladd Numerical simulations of particulate suspensions via a discretized Boltzmann equation. Part 1. Theoretical foundation , 1993, Journal of Fluid Mechanics.

[46]  Vittorio Cristini,et al.  Inertia-induced breakup of highly viscous drops subjected to simple shear , 2003 .