Direct numerical simulations of droplet emulsions in sliding bi-periodic frames using the level-set method See Jo Wook Ryol Hwang*

Slides:



Advertisements
Similar presentations
Impact of Microdrops on Solids James Sprittles & Yulii Shikhmurzaev Failure of conventional models All existing models are based on the contact angle being.
Advertisements

Outline Overview of Pipe Flow CFD Process ANSYS Workbench
Level set based Image Segmentation Hang Xiao Jan12, 2013.
Active Contours, Level Sets, and Image Segmentation
Particle Acceleration Particle t t+dt. Physical Interpretation Total acceleration of a particle Local acceleration Convective acceleration time velocity.
1 FEM study of the faults activation Technische Universität München Joint Advanced Student School (JASS) St. Petersburg Polytechnical University Author:
Introduction: Gravitational forces resulting from microgravity, take off and landing of spacecraft are experienced by individual cells in the living organism.
Dr. Kirti Chandra Sahu Department of Chemical Engineering IIT Hyderabad.
Single-Scale Models: The Cytoskeleton Scientific Computing and Numerical Analysis Seminar CAAM 699.
Results It was found that variations in wettability disturb the flow of adjacent liquid (Fig. 3). Our results suggest that for a given liquid the normal.
Coupling Continuum Model and Smoothed Particle Hydrodynamics Methods for Reactive Transport Yilin Fang, Timothy D Scheibe and Alexandre M Tartakovsky Pacific.
Peyman Mostaghimi, Prof. Martin Blunt, Dr. Branko Bijeljic 16 January 2009, Imperial College Consortium on Pore-Scale Modelling The level set method and.
12/21/2001Numerical methods in continuum mechanics1 Continuum Mechanics On the scale of the object to be studied the density and other fluid properties.
University of North Carolina - Chapel Hill Fluid & Rigid Body Interaction Comp Physical Modeling Craig Bennetts April 25, 2006 Comp Physical.
1 MECH 221 FLUID MECHANICS (Fall 06/07) Tutorial 6 FLUID KINETMATICS.
Preliminary Assessment of Porous Gas-Cooled and Thin- Liquid-Protected Divertors S. I. Abdel-Khalik, S. Shin, and M. Yoda ARIES Meeting, UCSD (March 2004)
16/12/ Texture alignment in simple shear Hans Mühlhaus,Frederic Dufour and Louis Moresi.
James Sprittles ECS 2007 Viscous Flow Over a Chemically Patterned Surface J.E. Sprittles Y.D. Shikhmurzaev.
Pablo Sanz 1, David Pollard 2 and Ronaldo Borja 1 FINITE ELEMENT MODELING OF FRACTURES EVOLUTION DURING FOLDING OF AN ASYMMETRIC ANTICLINE 1 Department.
ABSTRACT Many new devices and applications are being created that involve transporting droplets from one place to another. A common method of achieving.
MCE 561 Computational Methods in Solid Mechanics
Some Aspects of Drops Impacting on Solid Surfaces J.E Sprittles Y.D. Shikhmurzaev EFMC7 Manchester 2008.
Flow and Thermal Considerations
The Finite Element Method
Conservation Laws for Continua
Lecture 16 - Free Surface Flows Applied Computational Fluid Dynamics
Motion and Stress Analysis by Vector Mechanics Edward C. Ting Professor Emeritus of Applied Mechanics Purdue University, West Lafayette, IN National Central.
James Sprittles BAMC 2007 Viscous Flow Over a Chemically Patterned Surface J.E Sprittles Y.D. Shikhmurzaev.
Modelling of the particle suspension in turbulent pipe flow
A Hybrid Particle-Mesh Method for Viscous, Incompressible, Multiphase Flows Jie LIU, Seiichi KOSHIZUKA Yoshiaki OKA The University of Tokyo,
Viscoelasticity While water and air are Newtonian, lots of other common stuff isn’t: –Blood, paint, and many others have nonlinear viscosity (the faster.
1 Department: Material science and engineering Discipline: Finite element method By: Anelia Ivanova To: Prof. V. Iliev Subject : Hydrodynamics Simulation.
MSc Thesis presentation – Thijs Bosma – December 4th 2013
Numerical Simulations of Silverpit Crater Collapse: A Comparison of TEKTON and SALES 2 Gareth Collins, Zibi Turtle, and Jay Melosh LPL, Univ. of Arizona.
© Cambridge University Press 2010 Brian J. Kirby, PhD Sibley School of Mechanical and Aerospace Engineering, Cornell University, Ithaca, NY Powerpoint.
A Numerical Model for Multiphase Flow, I: The Interface Tracking Algorithm Frank Bierbrauer.
A.H. Gosline ( andrewg [at] cim.mcgill.ca) S.E. Salcudean (tims [at] ece.ubc.ca) J. Yan (josephy [at] ece.ubc.ca) Haptic Simulation of Linear Elastic Media.
Dynamics of a compound vesicle*
Introduction to Level Set Methods: Part II
LATTICE BOLTZMANN SIMULATIONS OF COMPLEX FLUIDS Julia Yeomans Rudolph Peierls Centre for Theoretical Physics University of Oxford.
Ale with Mixed Elements 10 – 14 September 2007 Ale with Mixed Elements Ale with Mixed Elements C. Aymard, J. Flament, J.P. Perlat.
Introduction: Lattice Boltzmann Method for Non-fluid Applications Ye Zhao.
Materials Process Design and Control Laboratory Sibley School of Mechanical and Aerospace Engineering 169 Frank H. T. Rhodes Hall Cornell University Ithaca,
Numerical simulation of droplet motion and two-phase flow field in an oscillating container Tadashi Watanabe Center for Computational Science and e-Systems.
Numerical Simulation of Dendritic Solidification
Governing Equations Conservation of Mass Conservation of Momentum Velocity Stress tensor Force Pressure Surface normal Computation Flowsheet Grid values.
A New Discontinuous Galerkin Formulation for Kirchhoff-Love Shells
EPSRC Portfolio Partnership in Complex Fluids and Complex Flows Computational Rheology The Numerical Prediction of Complex Flows of Complex Fluids Gigantic.
Particle-based Viscoelastic Fluid Simulation Simon Clavet Philippe Beaudoin Pierre Poulin LIGUM, Université de Montréal.
Numerical Modeling of Viscoelastic Drops John Gemmer, Millersville University Tobin Isaac, Rice University Mark Sussman, Florida State University.
Environmental Hydrodynamics Lab. Yonsei University, KOREA RCEM D finite element modeling of bed elevation change in a curved channel S.-U. Choi,
1.Fundamental equations and concepts 2.Balanced flow and vortex motion 3.Waves 4.Instabilities 5.Nonlinear phenomena An Introduction to Geophysical Fluid.
Hirophysics.com Some Aspects of Numerical Solutions for Partial Differential Equations Austin Andries University of Southern Mississippi Dr. Hironori Shimoyama.
Relationship between cilia-induced and airflow-induced mucus clearance Sorin Mitran Applied Mathematics UNC Virtual Lung Project August 19, 2008.
Convergence Studies of Turbulent Channel Flows Using a Stabilized Finite Element Method Andrés E. Tejada-Martínez Department of Civil & Environmental Engineering.
An Introduction to Computational Fluids Dynamics Prapared by: Chudasama Gulambhai H ( ) Azhar Damani ( ) Dave Aman ( )
Chapter 1: Basic Concepts
The Soft Matter Engineering Lab Laboratory of Modeling and Simulation of Soft Matter G. D’Avino, T. Tuccillo, S. Nazir, P.L. Maffettone COMPUTING IN SOFT.
I- Computational Fluid Dynamics (CFD-I)
Energy Reduction Through Tribology-2
Chapter 4 Fluid Mechanics Frank White
Part IV: Detailed Flow Structure Chap. 7: Microscopic Balances
Numerical Modeling of Dynamics and Adhesion of Leukocytes
1. Density y Volume,  Mass, m C Elemental Volume,   Mass, m x z.
Numerical Modeling of Fluid Droplet Spreading and Contact Angle Hysteresis Nikolai V. Priezjev, Mechanical Engineering, Michigan State University, MI
CMG Research: Mathematical Modeling of the Dynamics of Multi-scale Phenomena During Folding and Fracturing of Sedimentary Rocks Ronaldo I. Borja, Craig.
Three-Dimensional Fragmentation of Core-Annular Flow
Introduction to Fluid Mechanics
Anthony D. Fick & Dr. Ali Borhan Governing Equations
COMBUSTION ENGINEERING
Presentation transcript:

Direct numerical simulations of droplet emulsions in sliding bi-periodic frames using the level-set method See Jo Wook Ryol Hwang* School of Mechanical Engineering, Andong National University * School of Mechanical and Aerospace Engineering, Gyeongsang National University

Objective Rheology and flow-induced microstructural development in droplet emulsions in viscoelastic fluids by direct numerical simulations  A large number of small drops suspended freely in a viscoelastic fluid.  Fully coupled viscoelastic flow simulation with drops under sliding bi-periodic flows.  A well-defined sliding bi-periodic domain concept with drops is necessary.

 2D, Circular disk-like drops, negligible inertia.  Inertialess drops in viscoelastic fluids in a sliding bi-periodic frame under simple shear.  Sliding bi-periodic frame of simple shear flow

This problem represents a regular configuration of an infinite number of such a configuration in the unbounded domain Question 1: How to find INTERFACES ? Question 2: How to apply INTERFACIAL TENSION ?

Question 1: How to find INTERFACES ? Interface Tracking – Mesh Moves with Interface: Deformation characteristics of spherical bubble collapse in Newtonian fluids near the wall using the Finite Element Method with ALE formulation

 Bowyer-Waston Algorithm Andong National University Advanced Material Processing Lab.

Andong National University Advanced Material Processing Lab.

Node number : 437, element number : 814. Boundary Mark Andong National University Advanced Material Processing Lab.

 Mesh Generation for Two-Phase Fluid Systems  Graphic Display by OpenGL (a) Show Number of Node (b) Show Number of Element(c) Show Number of Material Andong National University Advanced Material Processing Lab.

Normal Stress Balance : Shear Stress Balance : Local Mean Curvature: Interfacial Boundary Conditions by Interface Tracking N T R Liquid Droplet

Question 1: How to find INTERFACES ? Interface Capturing – Fixed Meshes across Interface: VOF: Level Set Method: Diffuse Interface:

Interface capturing based on a fixed mesh. Evolution Equation of the interface in terms of Level Set Function. Interface Capturing by Level Set Method.

Continuum Surface Stress (CSS):  Interfacial tension is treated as a body force  Interfacial tension is treated as an additional stress Continuum Surface Force (CSF): Interfacial Boundary Conditions by Interface Capturing

Governing Equations Computational Domain (Oldroyd-B) B.C. on computational domain Γ : (Sliding bi-periodic frame constraints)

Finite Element Formulation Modification of combined weak formulation of Glowinski et al for right-ring description of particles and sliding bi-periodic frame constraints 1.Both fluid and particle domains are described by the fluid problem; 2. Force-free, torque-free, rigid-body motion is satisfied weakly with the constraint on the particle boundary only; 3.Sliding bi-periodicity is applied weakly through the constraints of the sliding bi-periodic frame; 4.The weak form has been coupled with the DEVSS/DG scheme to solve emulsions in a viscoelastic fluid. 5.The weak form has been coupled with the DG scheme to solve the Level set function.

A single particle of radius r=0.2 in a sliding bi-periodic frame of size 1 x 1 in a Newtonian fluid with Regular configuration of an infinite number of drops of the same size in an unbounded domain Drops do not translate, but rotate with deformation. Good example for study of rheology of emulsion. A Single Drop in Newtonian Fluid

The pressure contour and streamline Convergence to steady shape of deformed drop

Distance function and drop deformation

Time-dependent bulk suspension properties Convergence to steady oscillation  bulk normal stress is zero for Particle-Newtonian medium system  bulk normal stress is not zero for Drop-Newtonian medium system  possibility of viscoelastic effects even for Drop-Newtonian medium system

Two Drops in Newtonian Fluid Two symmetrically located particles of radius 0.2 in a sliding bi-periodic frame Of size 1 x 1 in a Newtonian fluid with

Distance function and drop deformation

Multiple Droplets in Newtonian Fluid

1. Direct numerical methods of drop emulsions in a viscoelastic fluid has been developed and implemented. 2. Incorporation with the Level set scheme for interfacial tension of droplet. 3. Deformation phenomena were observed for a single droplet, and multiple droplets. 4. Bulk normal stress is not zero for Drop- Newtonian medium system. Conclusions