1 Simulation of Micro-channel Flows by Lattice Boltzmann Method LIM Chee Yen, and C. Shu National University of Singapore.

Slides:



Advertisements
Similar presentations
Cosmological Structure Formation A Short Course III. Structure Formation in the Non-Linear Regime Chris Power.
Advertisements

Fluid Mechanics Research Group Two phase modelling for industrial applications Prof A.E.Holdø & R.K.Calay.
MASS TRANSFER TO SPHERE AND HEMISPHERE ELCTRODES BY IMPINGING JET
Open Source Field Operation and Manipulation
Outline Overview of Pipe Flow CFD Process ANSYS Workbench
Basic Governing Differential Equations
ON WIDTH VARIATIONS IN RIVER MEANDERS Luca Solari 1 & Giovanni Seminara 2 1 Department of Civil Engineering, University of Firenze 2 Department of Environmental.
Kazuo Aoki Dept. of Mech. Eng. and Sci. Kyoto University
An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez-Miravete Department of Engineering and Science Rensselaer at Hartford.
Estimation of the Accuracy Obtained from CFD for industrial applications Prepared by Imama Zaidi.
GPU Workshop: July, 2010 Scott Briggs PhD Candidate Civil/Env. Engineering Contaminant Hydrogeology Supervisors: B. E. Sleep and B. W. Karney.
Permeability Prediction of Shale Gas by the Monte Carlo Molecular Simulations at Pore Scale Jun Li Research Engineer ||| Center for Petroleum & Mineral,
Quantification of Laminar flow weakness … P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Instability Analysis of Laminar Flows.
Combining the strengths of UMIST and The Victoria University of Manchester Aspects of Transitional flow for External Applications A review presented by.
Anoop Samant Yanyan Zhang Saptarshi Basu Andres Chaparro
Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Basic Governing Differential Equations CEE 331 June 12, 2015.
Basic Governing Differential Equations
Karin Erbertseder Ferienakademie 2007
1 A Project Presentation for Applied Computational Fluid Dynamics By Reni Raju Finite Element Model of Gas Flow inside a Microchannel MECH
Lecture 7 Exact solutions
Modeling Fluid Phenomena -Vinay Bondhugula (25 th & 27 th April 2006)
Slip to No-slip in Viscous Fluid Flows
Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Basic Governing Differential Equations CEE 331 July 14, 2015 CEE 331 July 14, 2015.
FUNDAMENTAL EQUATIONS, CONCEPTS AND IMPLEMENTATION
If the shock wave tries to move to right with velocity u 1 relative to the upstream and the gas motion upstream with velocity u 1 to the left  the shock.
1 Heat Transfer in Microchannels 11.1 Introduction: Applications Micro-electro-mechanical systems (MEMS): Micro heat exchangers, mixers, pumps, turbines,
Discrete unified gas-kinetic scheme for compressible flows
© Arturo S. Leon, BSU, Spring 2010
Jean-Charles Matéo-Vélez, Frédéric Thivet, Pierre Degond * ONERA - Centre de Toulouse * CNRS - Mathématiques pour l'Industrie et la Physique, Toulouse.
Accelerated Numerical Simulation of Bloodflow in Aneurysms Using Lattice Boltzmann Methods and Multigrid Sarntal Jan Götz.
PTT 204/3 APPLIED FLUID MECHANICS SEM 2 (2012/2013)
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS Compressible Flow Over Airfoils: Linearized Subsonic Flow Mechanical and Aerospace Engineering Department Florida.
1 SIMULATION OF VIBROACOUSTIC PROBLEM USING COUPLED FE / FE FORMULATION AND MODAL ANALYSIS Ahlem ALIA presented by Nicolas AQUELET Laboratoire de Mécanique.
Improved Near Wall Treatment for CI Engine CFD Simulations Mika Nuutinen Helsinki University of Technology, Internal Combustion Engine Technology.
LBM: Approximate Invariant Manifolds and Stability Alexander Gorban (Leicester) Tuesday 07 September 2010, 16:50-17:30 Seminar Room 1, Newton Institute.
Governing equations: Navier-Stokes equations, Two-dimensional shallow-water equations, Saint-Venant equations, compressible water hammer flow equations.
Simulation of Micro Flows by Taylor Series Expansion- and Least Square-based Lattice Boltzmann Method   C. Shu, X. D. Niu, Y. T. Chew and Y. Peng.
A. Vikhansky, Lattice-Boltzmann method for non-Newtonian and non-equilibrium flows Lattice-Boltzmann method for non-Newtonian and non-equilibrium flows.
1 MICRO FLOWS: AN INTRODUCTION Michael Shusser. 2 SIZE RANGES OF MACRO, MICRO, AND NANO DEVICES.
Numerical simulations of thermal counterflow in the presence of solid boundaries Andrew Baggaley Jason Laurie Weizmann Institute Sylvain Laizet Imperial.
Basic Boltzmann Gas Concepts. Kinetic Theory Complete set of position (x) and momentum (p) coordinates for all individual particles gives exact dynamical.
Order of Magnitude Scaling of Complex Engineering Problems Patricio F. Mendez Thomas W. Eagar May 14 th, 1999.
Numerical simulations of inertia-gravity waves and hydrostatic mountain waves using EULAG model Bogdan Rosa, Marcin Kurowski, Zbigniew Piotrowski and Michał.
Introduction: Lattice Boltzmann Method for Non-fluid Applications Ye Zhao.
7.1.1 Hyperbolic Heat Equation
HEAT TRANSFER FINITE ELEMENT FORMULATION
Modeling of the Unsteady Separated Flow over Bilge Keels of FPSO Hulls under Heave or Roll Motions Yi-Hsiang Yu 09/23/04 Copies of movies/papers and today’s.
Information Geometry and Model Reduction Sorin Mitran 1 1 Department of Mathematics, University of North Carolina, Chapel Hill, NC, USA Reconstruction.
FREE CONVECTION 7.1 Introduction Solar collectors Pipes Ducts Electronic packages Walls and windows 7.2 Features and Parameters of Free Convection (1)
Modeling Electromagnetic Fields in Strongly Inhomogeneous Media
1 MULTIPHYSICS December 2009 Lille, FRANCE.
Chapter 3. Instability of the free plane and near – wall plane jet
Environmental Hydrodynamics Lab. Yonsei University, KOREA RCEM D finite element modeling of bed elevation change in a curved channel S.-U. Choi,
May 23, 2006SINS meeting Structure Formation and Particle Mixing in a Shear Flow Boundary Layer Matthew Palotti University of Wisconsin.
An Unified Analysis of Macro & Micro Flow Systems… P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Wall Bound Flows.
Investigation of supersonic and hypersonic laminar shock/boundary-layer interactions R.O. Bura, Y.F.Yao, G.T. Roberts and N.D. Sandham School of Engineering.
An Unified Analysis of Macro & Micro Flow Systems… P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Slip to No-slip in Viscous Fluid.
Basic Boltzmann Gas Concepts
Hamdache Abderrazaq 1*, Belkacem Mohamed 1, Hannoun Nourredine 2
Nonequilibrium statistical mechanics of electrons in a diode
Kinetic Theory.
Viscous Flow in Pipes.
CHAPTER 6 Viscous Flow in Pipes
Kinetic Theory.
Lecture Objectives Review for exam Discuss midterm project
Turbulent Boundary Layer
Bogdan Rosa1, Marcin Kurowski1, Damian Wójcik1,
Two-dimensional Lattice Boltzmann Simulation of Liquid Water Transport
Lattice Boltzmann Simulation of Water Transport in Gas Diffusion Layers of PEMFCs with Different Inlet Conditions Seung Hun Lee1, Jin Hyun Nam2,*, Hyung.
Kinetic Theory.
Presentation transcript:

1 Simulation of Micro-channel Flows by Lattice Boltzmann Method LIM Chee Yen, and C. Shu National University of Singapore

2 Introduction 1. Lattice Boltzmann Method 2. Micro flow Simulation 3. Results and Discussions 4. Conclusions

3 1. Lattice Boltzmann Method Originated from LGCA: i=0,1,…,k Collision term linearized, LBGK model:

4 1. Lattice Boltzmann Method This form is similar to Boltzmann equation with BGK collision term: In discrete velocity space:

5 1. Lattice Boltzmann Method Applying upwind scheme together with Lattice velocity, we have This is exactly standard LBM form is we set.

6 1. Lattice Boltzmann Method To determine, we assume linear relationship between and : We obtain this relationship: In our simplified analysis, we set:

7 1. Lattice Boltzmann Method D2Q9 lattice model is employed. Lattice vectors can be represented by:

8 1. Lattice Boltzmann Method Flow recoveriesEquilibrium functions i = 1, 3, 5, 7 i = 2, 4, 6, 8

9 2. Simulation of Micro Flow is unknown. Channel height, From Kn and relationship of we obtain

Boundary Conditions Equilibrium functions at openings Specular bounce back at solid walls.

Extrapolation Scheme Another boundary treatment scheme Approximating unknown f’s by their f eq ’s. f eq is function of local density and velocities.

12 2. Simulation of Micro Flow Simulation process involves only 2 updating steps: Local collision: Streaming: i = 1,…, 8

13 3. Results and Discussions Qualitative analyses: General profiles of flow properties. Quantitative analyses – pressure and velocity distributions. Normalising, P* = P / P out, P*’ = P* - P* linear, u* = u / u max

General Profiles Pressure distribution Pr=2.0, Kn=0.05. Pressure changes only along the channel, in X direction. Pressure is independent of Y.

General Profiles Pr=2.0, Kn=0.05 Increasing centerline and slip velocities along the channel. Parabolic profile of u across the channel.

General Profiles Pr=2.0, Kn=0.05. Several magnitude smaller. Anti-phase peaks, growing along the channel.

Pressure Distributions Non-linearity of pressure, P’. Rarefaction negates compressibility on micro flow. Less compressibility predicted by both models.

Pressure Distributions Slip flow: Pr=1.88, Kn= Over-prediction by analytical solution Due to insufficient rarefaction taken into account.

Pressure Distributions Transition regime Pr =2.05 and Kn= Over-prediction of analytical solution is more obvious. Present methods are more general.

Slip Velocities According to Arkilic et al, slip at outlet is only dependent on Kn:, is set to 1. Slip along the channel can be written in term of outlet slip:

Slip Velocities where and Slip is generally dependent on the Pr, Kn, and the pressure gradients dP*/dX.

Slip Velocities (Spec) Kn = 0.05 Generally agree with analytical predictions. Convergence of slip at outlet for different Pr’s.

Slip Velocities (Spec) Kn = 0.1 Slip is enhanced by Rarefaction considerably. Convergence of slip at outlet for different Pr’s.

Slip Velocities (U Ext.) Kn = 0.05 Generally predicts less slip than Spec. Convergence of outlet slip is seen.

Slip Velocities (U Ext.) Kn = 0.1 seems to have better agreement at higher Kn. Slip is enhanced as Kn increases.

26 4. Closure Discuss the origin of LBM and its derivation from Boltzmann equation. Present an efficient LBM scheme for simulation of micro flows. Verify our numerical results by comparisons to experimental and analytical work.

27 4. Closure Pressure distribution Negation of compressibility by rarefaction. Insufficient consideration of rarefaction in N-S analytical solution. Slip velocities Slip is function of u * s,o, Pr, and dP*/dX. Convergence of outlet slip for different Pr’s. Kn enhances slip.