A hybrid lattice Boltzmann and finite difference method for droplet dynamics with insoluble surfactants

Droplet dynamics in microfluidic applications is significantly influenced by surfactants. It remains a research challenge to model and simulate droplet behaviour including deformation, breakup and coalescence, especially in the confined microfluidic environment. Here, we propose a hybrid method to simulate interfacial flows with insoluble surfactants. The immiscible two-phase flow is solved by an improved lattice Boltzmann colour-gradient model which incorporates a Marangoni stress resulting from non-uniform interfacial tension, while the convection–diffusion equation which describes the evolution of surfactant concentration in the entire fluid domain is solved by a finite difference method. The lattice Boltzmann and finite difference simulations are coupled through an equation of state, which describes how surfactant concentration influences interfacial tension. Our method is first validated for the surfactant-laden droplet deformation in a three-dimensional (3D) extensional flow and a 2D shear flow, and then applied to investigate the effect of surfactants on droplet dynamics in a 3D shear flow. Numerical results show that, at low capillary numbers, surfactants increase droplet deformation, due to reduced interfacial tension by the average surfactant concentration, and non-uniform effects from non-uniform capillary pressure and Marangoni stresses. The role of surfactants on the critical capillary number ( $Ca_{cr}$ ) of droplet breakup is investigated for various confinements (defined as the ratio of droplet diameter to wall separation) and Reynolds numbers. For clean droplets, $Ca_{cr}$ first decreases and then increases with confinement, and the minimum value of $Ca_{cr}$ is reached at a confinement of 0.5; for surfactant-laden droplets, $Ca_{cr}$ exhibits the same variation in trend for confinements lower than 0.7, but, for higher confinements, $Ca_{cr}$ is almost a constant. The presence of surfactants decreases $Ca_{cr}$ for each confinement, and the decrease is also attributed to the reduction in average interfacial tension and non-uniform effects, which are found to prevent droplet breakup at low confinements but promote breakup at high confinements. In either clean or surfactant-laden cases, $Ca_{cr}$ first remains almost unchanged and then decreases with increasing Reynolds number, and a higher confinement or Reynolds number favours ternary breakup. Finally, we study the collision of two equal-sized droplets in a shear flow in both surfactant-free and surfactant-contaminated systems with the same effective capillary numbers. It is identified that the non-uniform effects in the near-contact interfacial region immobilize the interfaces when two droplets are approaching each other and thus inhibit their coalescence.

[1]  L. Marino,et al.  The sharp-interface limit of the Cahn–Hilliard/Navier–Stokes model for binary fluids , 2013, Journal of Fluid Mechanics.

[2]  Yin Yang,et al.  A level-set continuum method for two-phase flows with insoluble surfactant , 2012, J. Comput. Phys..

[3]  Johan Sjöblom,et al.  Emulsions and emulsion stability , 1996 .

[4]  Mitsutoshi Nakajima,et al.  Preparation characteristics of oil-in-water emulsions using differently charged surfactants in straight-through microchannel emulsification , 2003 .

[5]  Y. Sui Moving towards the cold region or the hot region? Thermocapillary migration of a droplet attached on a horizontal substrate , 2014 .

[6]  Sauro Succi,et al.  Lattice Boltzmann simulations of phase-separating flows at large density ratios: the case of doubly-attractive pseudo-potentials , 2010 .

[7]  Jian-Jun Xu,et al.  A level-set method for two-phase flows with moving contact line and insoluble surfactant , 2014, J. Comput. Phys..

[8]  Metin Muradoglu,et al.  A front-tracking method for computation of interfacial flows with soluble surfactants , 2008, J. Comput. Phys..

[9]  Chi-Wang Shu,et al.  Efficient Implementation of Weighted ENO Schemes , 1995 .

[10]  Ryutaro Maeda,et al.  Straight-through microchannel devices for generating monodisperse emulsion droplets several microns in size , 2008 .

[11]  Kathleen J. Stebe,et al.  The effects of a diffusion controlled surfactant on a viscous drop injected into a viscous medium , 2007 .

[12]  Howard A. Stone,et al.  Dynamics of Drop Deformation and Breakup in Viscous Fluids , 1994 .

[13]  J. Lowengrub,et al.  A surfactant-conserving volume-of-fluid method for interfacial flows with insoluble surfactant , 2004 .

[14]  I. Halliday,et al.  Improved simulation of drop dynamics in a shear flow at low Reynolds and capillary number. , 2006, Physical review. E, Statistical, nonlinear, and soft matter physics.

[15]  Jie Zhang,et al.  A front tracking method for a deformable intravascular bubble in a tube with soluble surfactant transport , 2006, J. Comput. Phys..

[16]  C M Care,et al.  Lattice Boltzmann algorithm for continuum multicomponent flow. , 2007, Physical review. E, Statistical, nonlinear, and soft matter physics.

[17]  Vittorio Cristini,et al.  Effect of inertia on drop breakup under shear , 2001 .

[18]  Axel Voigt,et al.  A DIFFUSE-INTERFACE APPROACH FOR MODELING TRANSPORT, DIFFUSION AND ADSORPTION/DESORPTION OF MATERIAL QUANTITIES ON A DEFORMABLE INTERFACE. , 2009, Communications in mathematical sciences.

[19]  Albert J. Valocchi,et al.  Pore-scale simulation of liquid CO2 displacement of water using a two-phase lattice Boltzmann model , 2014 .

[20]  Yonghao Zhang,et al.  Lattice Boltzmann modeling of contact angle and its hysteresis in two-phase flow with large viscosity difference. , 2015, Physical review. E, Statistical, nonlinear, and soft matter physics.

[21]  K. Migler,et al.  Droplet−String Deformation and Stability during Microconfined Shear Flow , 2003 .

[22]  Zhilin Li,et al.  A level-set method for interfacial flows with surfactant , 2006, J. Comput. Phys..

[23]  Yan Wang,et al.  Multiphase lattice Boltzmann flux solver for incompressible multiphase flows with large density ratio , 2015, J. Comput. Phys..

[24]  Tianyu Zhang,et al.  Cahn-Hilliard Vs Singular Cahn-Hilliard Equations in Phase Field Modeling , 2009 .

[25]  Vittorio Cristini,et al.  Drop deformation in microconfined shear flow. , 2006, Physical review letters.

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

[27]  Kathleen Feigl,et al.  Simulation and experiments of droplet deformation and orientation in simple shear flow with surfactants , 2007 .

[28]  Yeomans,et al.  Lattice Boltzmann simulation of nonideal fluids. , 1995, Physical review letters.

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

[30]  Joon Sang Lee,et al.  A hybrid lattice Boltzmann model for surfactant-covered droplets , 2011 .

[31]  Haihu Liu,et al.  Modelling thermocapillary migration of a microfluidic droplet on a solid surface , 2015, J. Comput. Phys..

[32]  T. M. Tsai,et al.  Tip streaming from a drop in the presence of surfactants. , 2001, Physical review letters.

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

[34]  Jianhong Xu,et al.  The dynamic mass transfer of surfactants upon droplet formation in coaxial microfluidic devices , 2015 .

[35]  Ming-Chih Lai,et al.  Numerical Simulation of Moving Contact Lines with Surfactant by Immersed Boundary Method , 2010 .

[36]  Rongye Zheng,et al.  Color-gradient lattice Boltzmann model for simulating droplet motion with contact-angle hysteresis. , 2013, Physical review. E, Statistical, nonlinear, and soft matter physics.

[37]  Ming-Chih Lai,et al.  An immersed boundary method for interfacial flows with insoluble surfactant , 2008, J. Comput. Phys..

[38]  Peter Van Puyvelde,et al.  Effect of confinement on the steady-state behavior of single droplets during shear flow , 2007 .

[39]  郑楚光,et al.  Non-equilibrium extrapolation method for velocity and pressure boundary conditions in the lattice Boltzmann method , 2005 .

[40]  Yousef Saad,et al.  Iterative methods for sparse linear systems , 2003 .

[41]  Giacomo Falcucci,et al.  Three-Dimensional Lattice Pseudo-Potentials for Multiphase Flow Simulations at High Density Ratios , 2015 .

[42]  Anja Vananroye,et al.  Review on morphology development of immiscible blends in confined shear flow , 2008 .

[43]  Yi Cheng,et al.  Lattice-Boltzmann method for the simulation of multiphase mass transfer and reaction of dilute species. , 2014, Physical review. E, Statistical, nonlinear, and soft matter physics.

[44]  M. Minale Models for the deformation of a single ellipsoidal drop: a review , 2010 .

[45]  H. Fujita,et al.  Silicon array of elongated through-holes for monodisperse emulsion droplets , 2002 .

[46]  Stefano Ubertini,et al.  Lattice Boltzmann Modeling of Diesel Spray Formation and Break-Up , 2010 .

[47]  B. Shi,et al.  Non-equilibrium extrapolation method for velocity and pressure boundary conditions in the lattice Boltzmann method , 2002 .

[48]  Francesco Greco,et al.  DYNAMICS OF A LIQUID DROP IN A FLOWING IMMISCIBLE LIQUID , 2004 .

[49]  Bing Dai,et al.  The mechanism of surfactant effects on drop coalescence , 2008 .

[50]  Johan Sjoblom,et al.  Emulsions and Emulsion Stability: Surfactant Science Series/61 , 1996 .

[51]  Héctor D. Ceniceros,et al.  The effects of surfactants on the formation and evolution of capillary waves , 2003 .

[52]  Haihu Liu,et al.  Modeling and simulation of thermocapillary flows using lattice Boltzmann method , 2012, J. Comput. Phys..

[53]  S. Herminghaus,et al.  Droplet based microfluidics , 2012, Reports on progress in physics. Physical Society.

[54]  Peng Song,et al.  A diffuse-interface method for two-phase flows with soluble surfactants , 2011, J. Comput. Phys..

[55]  Geoffrey Ingram Taylor,et al.  The formation of emulsions in definable fields of flow , 1934 .

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

[57]  He Zhenmin,et al.  EMC effect on p-A high energy collisions , 1991 .

[58]  Xiaoyi He,et al.  Thermodynamic Foundations of Kinetic Theory and Lattice Boltzmann Models for Multiphase Flows , 2002 .

[59]  J. Yeomans,et al.  Contact line dynamics in binary lattice Boltzmann simulations. , 2008, Physical review. E, Statistical, nonlinear, and soft matter physics.

[60]  S. Succi,et al.  Direct numerical evidence of stress-induced cavitation , 2013, Journal of Fluid Mechanics.

[61]  H. Stone A simple derivation of the time‐dependent convective‐diffusion equation for surfactant transport along a deforming interface , 1990 .

[62]  Patrick D Anderson,et al.  Numerical investigation of the effect of insoluble surfactants on drop deformation and breakup in simple shear flow. , 2006, Journal of colloid and interface science.

[63]  Ali Borhan,et al.  Stability of the shape of a surfactant-laden drop translating at low Reynolds number , 1998 .

[64]  Kazufumi Ito,et al.  Three-dimensional elliptic solvers for interface problems and applications , 2003 .

[65]  Haihu Liu,et al.  Phase-field modeling droplet dynamics with soluble surfactants , 2010, J. Comput. Phys..

[66]  R. Boom,et al.  Coalescence dynamics of surfactant-stabilized emulsions studied with microfluidics , 2012 .

[67]  Remko M. Boom,et al.  Droplet formation in a T-shaped microchannel junction: A model system for membrane emulsification , 2005 .

[68]  Charles D. Eggleton,et al.  Insoluble surfactants on a drop in an extensional flow: a generalization of the stagnated surface limit to deforming interfaces , 1999, Journal of Fluid Mechanics.

[69]  Mitsutoshi Nakajima,et al.  Effects of type and physical properties of oil phase on oil-in-water emulsion droplet formation in straight-through microchannel emulsification, experimental and CFD studies. , 2005, Langmuir : the ACS journal of surfaces and colloids.

[70]  Wei Shyy,et al.  Force evaluation in the lattice Boltzmann method involving curved geometry. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[71]  Yuriko Renardy,et al.  The effects of confinement and inertia on the production of droplets , 2006 .

[72]  S Succi,et al.  Generalized lattice Boltzmann method with multirange pseudopotential. , 2006, Physical review. E, Statistical, nonlinear, and soft matter physics.

[73]  Shan,et al.  Lattice Boltzmann model for simulating flows with multiple phases and components. , 1993, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[74]  D. Rothman,et al.  Diffusion properties of gradient-based lattice Boltzmann models of immiscible fluids. , 2005, Physical review. E, Statistical, nonlinear, and soft matter physics.

[75]  L. Gary Leal,et al.  The Influence of Surfactant on the Deformation and Breakup of a Viscous Drop: The Effect of Surfactant Solubility , 1994 .

[76]  Patrick Patrick Anderson,et al.  Generalized behavior of the breakup of viscous drops in confinements , 2010 .

[77]  Pier Luca Maffettone,et al.  Equation of change for ellipsoidal drops in viscous flow , 1998 .

[78]  Shimon Haber,et al.  Low Reynolds number motion of a droplet in shear flow including wall effects , 1990 .

[79]  S Succi,et al.  Mesoscopic modeling of a two-phase flow in the presence of boundaries: The contact angle. , 2006, Physical review. E, Statistical, nonlinear, and soft matter physics.

[80]  Dieter Bothe,et al.  3D Numerical Modeling of Soluble Surfactant at Fluidic Interfaces Based on the Volume-of-Fluid Method , 2009 .

[81]  J. Baret Surfactants in droplet-based microfluidics. , 2012, Lab on a chip.

[82]  I. Tiselj,et al.  Lattice Boltzmann Method , 2022, Advanced Computational Techniques for Heat and Mass Transfer in Food Processing.

[83]  S. Zaleski,et al.  Lattice Boltzmann model of immiscible fluids. , 1991, Physical review. A, Atomic, molecular, and optical physics.

[84]  Amit Gupta,et al.  Effect of geometry on droplet formation in the squeezing regime in a microfluidic T-junction , 2010 .

[85]  D. Weitz,et al.  Geometrically mediated breakup of drops in microfluidic devices. , 2003, Physical review letters.

[86]  Increased drop formation frequency via reduction of surfactant interactions in flow-focusing microfluidic devices. , 2015, Langmuir : the ACS journal of surfaces and colloids.

[87]  Hongkai Zhao,et al.  An Eulerian Formulation for Solving Partial Differential Equations Along a Moving Interface , 2003, J. Sci. Comput..

[88]  Qinjun Kang,et al.  Three-dimensional lattice Boltzmann model for immiscible two-phase flow simulations. , 2012, Physical review. E, Statistical, nonlinear, and soft matter physics.

[89]  Qinjun Kang,et al.  Multiple-relaxation-time color-gradient lattice Boltzmann model for simulating two-phase flows with high density ratio. , 2016, Physical review. E.

[90]  S. Fielding,et al.  Moving contact line dynamics: from diffuse to sharp interfaces , 2015, Journal of Fluid Mechanics.

[91]  S V Lishchuk,et al.  Lattice Boltzmann algorithm for surface tension with greatly reduced microcurrents. , 2003, Physical review. E, Statistical, nonlinear, and soft matter physics.

[92]  Han E. H. Meijer,et al.  Droplet behavior in the presence of insoluble surfactants , 2004 .

[93]  B. Shi,et al.  Discrete lattice effects on the forcing term in the lattice Boltzmann method. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[94]  V. Cristini,et al.  Theory and numerical simulation of droplet dynamics in complex flows--a review. , 2004, Lab on a chip.

[95]  L. G. Leal,et al.  The effects of surfactants on drop deformation and breakup , 1990, Journal of Fluid Mechanics.

[96]  D. An,et al.  The effects of surfactants on drop deformation and breakup By , 2005 .