Control of Interface Evolution in Multi-Phase Fluid Flows

Size: px
Start display at page:

Download "Control of Interface Evolution in Multi-Phase Fluid Flows"

Transcription

1 Control of Interface Evolution in Multi-Phase Fluid Flows Markus Klein Department of Mathematics University of Tübingen Workshop on Numerical Methods for Optimal Control and Inverse Problems Garching, Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 1 / 17

2 Contents Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 2 / 17

3 Contents 1 Introduction and Motivation 2 Analysis 3 Numerical Analysis and Computations Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 3 / 17

4 The Model ρ 0 = ρ 1 χ Ω1 + ρ 2 χ Ω2 mixture of two immiscible viscous incompressible fluids in a bounded domain in R 2. Multi-phase flow evolution by Navier Stokes Eq. (cf. [Lions, 1996]) ρy t + ρ[y ]y µ y + p = ρu, y(0) = y 0, (NSE) ρ t + [y ]ρ = 0, ρ(0) = ρ 0, div y = 0 + B.C. Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 4 / 17

5 The Model ρ 0 = ρ 1 χ Ω1 + ρ 2 χ Ω2 mixture of two immiscible viscous incompressible fluids in a bounded domain in R 2. Multi-phase flow evolution by Navier Stokes Eq. (cf. [Lions, 1996]) Minimize Shape Geometry Cost T J(ρ, u) = ρ(t) σ 2 dx dt + β T H 1 (S ρ ) dt + α T u 2 dx dt 0 Ω Ω subject to ρy t + ρ[y ]y µ y + p = ρu, y(0) = y 0, (NSE) ρ t + [y ]ρ = 0, ρ(0) = ρ 0, div y = 0 + B.C. Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 4 / 17

6 Evidence of the geometric functional ρ σ 2 L 2 (Ω T ) ρ σ 2 L 2 (Ω T ) Target σ + T 0 H 1 (S ρ ) Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 5 / 17

7 Evidence of the geometric functional ρ σ 2 L 2 (Ω T ) ρ σ 2 L 2 (Ω T ) Target σ + T 0 H 1 (S ρ ) Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 5 / 17

8 Evidence of the geometric functional ρ σ 2 L 2 (Ω T ) ρ σ 2 L 2 (Ω T ) Target σ + T 0 H 1 (S ρ ) better corners correct geometry Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 5 / 17

9 Application ([Gerbeau et al., 2006]): Aluminium production via electrolysis Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 6 / 17

10 Application ([Gerbeau et al., 2006]): Aluminium production via electrolysis Anods shall not touch the interface! Interface control Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 6 / 17

11 Goals Existence of optimum. (Necessary) first order optimality conditions. Numerical scheme with low order Finite Elements. Convergence of the numerical scheme. Known result Optimization (analysis, no numerics) of L 2 -functional (no geometric term) subject to Stokes equation, cf. [Kunisch and Lu, 2011]. Convergent numerical scheme for equation (low regularity), cf. [Ba nas and Prohl, 2010]. Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 7 / 17

12 Contents 1 Introduction and Motivation 2 Analysis 3 Numerical Analysis and Computations Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 8 / 17

13 Analytical problems and strategy Minimize T J(ρ, u) = ρ(t) σ 2 dx dt + β T H 1 (S ρ ) dt + α T u 2 dx dt 0 Ω Ω subject to ρy t + ρ[y ]y µ y + p = ρu, y(0) = y 0, (NSE) ρ t + [y ]ρ = 0, ρ(0) = ρ 0, div y = 0 + B.C. Problem: Not clear if red term is w.l.s.c., and not clear if corresponding Lagrange multiplier to mass equation exists and is a function. Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 9 / 17

14 Analytical problems and strategy Minimize T J(ρ, u) = ρ(t) σ 2 dx dt + β T H 1 (S ρ ) dt + α T u 2 dx dt 0 Ω Ω subject to ρy t + ρ[y ]y µ y + p = ρu, y(0) = y 0, (NSE) ρ t + [y ]ρ = 0, ρ(0) = ρ 0, div y = 0 + B.C. Problem: Not clear if red term is w.l.s.c., and not clear if corresponding Lagrange multiplier to mass equation exists and is a function. Solution: Add artificial diffusion to equation and approximate Hausdorff measure ( Mortola-Modica, cf. [Braides, 1998]) Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 9 / 17

15 Analytical problems and strategy Minimize J δ (ρ, u) = + β 2 ( δ ρ ) W (ρ) Ω T δ Ω T subject to ρy t + ρ[y ]y µ y + p = ρu, y(0) = y 0, (NSE ε ) ρ t + [y ]ρ ε ρ t = 0, ρ(0) = ρ 0, div y = 0 + B.C. (W 0 double Well functional with W (ρ) = 0 iff ρ = ρ 1 or ρ = ρ 2 ) + Solution: Add artificial diffusion to equation and approximate Hausdorff measure ( Mortola-Modica, cf. [Braides, 1998]) Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 9 / 17

16 Analytic results Theorem (Existence) For δ, ε > 0, there exists at least one minimum and the corresponding Lagrange multipliers belong to some L p (Ω T ) for p > 1. Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 10 / 17

17 Analytic results Theorem (Existence) For δ, ε > 0, there exists at least one minimum and the corresponding Lagrange multipliers belong to some L p (Ω T ) for p > 1. Proof. Key are a priori estimates and regularity for y and ρ and Lagrange multiplier theorem. Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 10 / 17

18 Analytic results Theorem (Existence) For δ, ε > 0, there exists at least one minimum and the corresponding Lagrange multipliers belong to some L p (Ω T ) for p > 1. Proof. Key are a priori estimates and regularity for y and ρ and Lagrange multiplier theorem. Passing to the limit for ε, δ 0? Necessary condition for convergence of the whole system is δ ε. Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 10 / 17

19 Case ε δ: parasitic currents min δ ρ W (ρ) s.t. (NSE ε ). Ω T δ Ω T ρ(t = 0) ρ(t = 0.25) ρ(t = 0.5) Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 11 / 17

20 Case ε δ: parasitic currents min δ ρ W (ρ) s.t. (NSE ε ). Ω T δ Ω T ρ(t = 0) ρ(t = 0.25) ρ(t = 0.5) y(t = 0.05) y(t = 0.15) y(t = 0.35) Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 11 / 17

21 Case ε δ: massive diffusion min δ ρ W (ρ) s.t. (NSE ε ). Ω T δ Ω T ρ(t = 0) ρ(t = 0.5) moderate ε ρ(t = 0.5) big ε Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 12 / 17

22 Contents 1 Introduction and Motivation 2 Analysis 3 Numerical Analysis and Computations Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 13 / 17

23 Strategy Strategy for the discretization Fix δ, ε > 0. Use first discretize, then optimize ansatz with convergent and unconditionally stable scheme, cf. [Ba nas and Prohl, 2010]. Show existence of discrete optimum, derive discrete optimality conditions. Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 14 / 17

24 Strategy Strategy for the discretization Fix δ, ε > 0. Use first discretize, then optimize ansatz with convergent and unconditionally stable scheme, cf. [Ba nas and Prohl, 2010]. Show existence of discrete optimum, derive discrete optimality conditions. Strong coupling of primal and dual variables in the adjoint equation Need to bound strong norms of the primal variables Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 14 / 17

25 Strategy Strategy for the discretization Fix δ, ε > 0. Use first discretize, then optimize ansatz with convergent and unconditionally stable scheme, cf. [Ba nas and Prohl, 2010]. Show existence of discrete optimum, derive discrete optimality conditions. Strong coupling of primal and dual variables in the adjoint equation Need to bound strong norms of the primal variables, in particular show: sup [ Y(t) 2 + h R(t) 2] t [0,T ] T + h Y(t) 2 + d t Y(t) 2 + d t R(t) 2 dt C. 0 Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 14 / 17

26 Strategy Strategy for the discretization Fix δ, ε > 0. Use first discretize, then optimize ansatz with convergent and unconditionally stable scheme, cf. [Ba nas and Prohl, 2010]. Show existence of discrete optimum, derive discrete optimality conditions. Strong coupling of primal and dual variables in the adjoint equation Need to bound strong norms of the primal variables, in particular show: sup [ Y(t) 2 + h R(t) 2] t [0,T ] T + h Y(t) 2 + d t Y(t) 2 + d t R(t) 2 dt C. 0 Bounds for dual variables. Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 14 / 17

27 Main result Theorem (Convergence) There exist y, p, ρ; z, q, η; u : Ω T R (2), such that the solutions of the fully discrete optimality system converge to them in some norms (up to subsequences). The limit functions solve the original fully continuous optimality system. Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 15 / 17

28 Summary Done New geometric functional considered with PDE constraints: Evidence, existence and optimality conditions for δ, ε > 0. Rigorous converence analysis with unconditionally stable scheme for δ, ε > 0. Implementation for δ, ε > 0. Outlook What happens for ε, δ 0? Proofs? Interplay between δ, ε and numerical parameters (time step size k and grid size h)? Surface tension instead of geometric functional? Other models (sharp interface, thin film, etc.)? Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 16 / 17

29 Summary Done New geometric functional considered with PDE constraints: Evidence, existence and optimality conditions for δ, ε > 0. Rigorous converence analysis with unconditionally stable scheme for δ, ε > 0. Implementation for δ, ε > 0. Outlook What happens for ε, δ 0? Proofs? Interplay between δ, ε and numerical parameters (time step size k and grid size h)? Surface tension instead of geometric functional? Other models (sharp interface, thin film, etc.)? Thank you for your attention! Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 16 / 17

30 References I Ba nas, L. and Prohl, A. (2010). Convergent finite element discretization of the multi-fluid nonstationary incompressible magnetohydrodynamics equations. Math. Comp., 79(272): Braides, A. (1998). Approximation of free discontinuity problems. Number 1694 in Lecture notes in mathematics. Springer, Berlin. Gerbeau, J.-F., Le Bris, C., and Lelièvre, T. (2006). Mathematical methods for the magnetohydrodynamics of liquid metals. Numerical mathematics and scientific computation. Oxford University Press. Kunisch, K. and Lu, X. (2011). Optimal control for multi-phase fluid stokes problems. Nonlinear Anal., 74(2): Lions, P.-L. (1996). Mathematical topics in fluid mechanics, volume 1: Incompressible models of Oxford lecture series in mathematics and its applications. Clarendon Press. Markus Klein (U Tübingen) Control of Interface Evolution in Multi-Phase Flows Garching 17 / 17

Discrete Projection Methods for Incompressible Fluid Flow Problems and Application to a Fluid-Structure Interaction

Discrete Projection Methods for Incompressible Fluid Flow Problems and Application to a Fluid-Structure Interaction Discrete Projection Methods for Incompressible Fluid Flow Problems and Application to a Fluid-Structure Interaction Problem Jörg-M. Sautter Mathematisches Institut, Universität Düsseldorf, Germany, sautter@am.uni-duesseldorf.de

More information

Finite Elements for Magnetohydrodynamics and its Optimal Control

Finite Elements for Magnetohydrodynamics and its Optimal Control Finite Elements for Magnetohydrodynamics and its Karl Kunisch Marco Discacciati (RICAM) FEM Symposium Chemnitz September 25 27, 2006 Overview 1 2 3 What is Magnetohydrodynamics? Magnetohydrodynamics (MHD)

More information

Alexei F. Cheviakov. University of Saskatchewan, Saskatoon, Canada. INPL seminar June 09, 2011

Alexei F. Cheviakov. University of Saskatchewan, Saskatoon, Canada. INPL seminar June 09, 2011 Direct Method of Construction of Conservation Laws for Nonlinear Differential Equations, its Relation with Noether s Theorem, Applications, and Symbolic Software Alexei F. Cheviakov University of Saskatchewan,

More information

New Discretizations of Turbulent Flow Problems

New Discretizations of Turbulent Flow Problems New Discretizations of Turbulent Flow Problems Carolina Cardoso Manica and Songul Kaya Merdan Abstract A suitable discretization for the Zeroth Order Model in Large Eddy Simulation of turbulent flows is

More information

Local null controllability of the N-dimensional Navier-Stokes system with N-1 scalar controls in an arbitrary control domain

Local null controllability of the N-dimensional Navier-Stokes system with N-1 scalar controls in an arbitrary control domain Local null controllability of the N-dimensional Navier-Stokes system with N-1 scalar controls in an arbitrary control domain Nicolás Carreño Université Pierre et Marie Curie-Paris 6 UMR 7598 Laboratoire

More information

Convergence of the MAC scheme for incompressible flows

Convergence of the MAC scheme for incompressible flows Convergence of the MAC scheme for incompressible flows T. Galloue t?, R. Herbin?, J.-C. Latche??, K. Mallem????????? Aix-Marseille Universite I.R.S.N. Cadarache Universite d Annaba Calanque de Cortiou

More information

Variable Exponents Spaces and Their Applications to Fluid Dynamics

Variable Exponents Spaces and Their Applications to Fluid Dynamics Variable Exponents Spaces and Their Applications to Fluid Dynamics Martin Rapp TU Darmstadt November 7, 213 Martin Rapp (TU Darmstadt) Variable Exponent Spaces November 7, 213 1 / 14 Overview 1 Variable

More information

Relative entropies, suitable weak solutions, and weak-strong uniqueness for the compressible Navier-Stokes system

Relative entropies, suitable weak solutions, and weak-strong uniqueness for the compressible Navier-Stokes system Relative entropies, suitable weak solutions, and weak-strong uniqueness for the compressible Navier-Stokes system Institute of Mathematics, Academy of Sciences of the Czech Republic, Prague joint work

More information

SECOND ORDER TIME DISCONTINUOUS GALERKIN METHOD FOR NONLINEAR CONVECTION-DIFFUSION PROBLEMS

SECOND ORDER TIME DISCONTINUOUS GALERKIN METHOD FOR NONLINEAR CONVECTION-DIFFUSION PROBLEMS Proceedings of ALGORITMY 2009 pp. 1 10 SECOND ORDER TIME DISCONTINUOUS GALERKIN METHOD FOR NONLINEAR CONVECTION-DIFFUSION PROBLEMS MILOSLAV VLASÁK Abstract. We deal with a numerical solution of a scalar

More information

1 The Stokes System. ρ + (ρv) = ρ g(x), and the conservation of momentum has the form. ρ v (λ 1 + µ 1 ) ( v) µ 1 v + p = ρ f(x) in Ω.

1 The Stokes System. ρ + (ρv) = ρ g(x), and the conservation of momentum has the form. ρ v (λ 1 + µ 1 ) ( v) µ 1 v + p = ρ f(x) in Ω. 1 The Stokes System The motion of a (possibly compressible) homogeneous fluid is described by its density ρ(x, t), pressure p(x, t) and velocity v(x, t). Assume that the fluid is barotropic, i.e., the

More information

From a Mesoscopic to a Macroscopic Description of Fluid-Particle Interaction

From a Mesoscopic to a Macroscopic Description of Fluid-Particle Interaction From a Mesoscopic to a Macroscopic Description of Fluid-Particle Interaction Carnegie Mellon University Center for Nonlinear Analysis Working Group, October 2016 Outline 1 Physical Framework 2 3 Free Energy

More information

Global well-posedness of the primitive equations of oceanic and atmospheric dynamics

Global well-posedness of the primitive equations of oceanic and atmospheric dynamics Global well-posedness of the primitive equations of oceanic and atmospheric dynamics Jinkai Li Department of Mathematics The Chinese University of Hong Kong Dynamics of Small Scales in Fluids ICERM, Feb

More information

Semismooth Newton Methods for an Optimal Boundary Control Problem of Wave Equations

Semismooth Newton Methods for an Optimal Boundary Control Problem of Wave Equations Semismooth Newton Methods for an Optimal Boundary Control Problem of Wave Equations Axel Kröner 1 Karl Kunisch 2 and Boris Vexler 3 1 Lehrstuhl für Mathematische Optimierung Technische Universität München

More information

WELL POSEDNESS OF PROBLEMS I

WELL POSEDNESS OF PROBLEMS I Finite Element Method 85 WELL POSEDNESS OF PROBLEMS I Consider the following generic problem Lu = f, where L : X Y, u X, f Y and X, Y are two Banach spaces We say that the above problem is well-posed (according

More information

NUMERICAL SOLUTION OF CONVECTION DIFFUSION EQUATIONS USING UPWINDING TECHNIQUES SATISFYING THE DISCRETE MAXIMUM PRINCIPLE

NUMERICAL SOLUTION OF CONVECTION DIFFUSION EQUATIONS USING UPWINDING TECHNIQUES SATISFYING THE DISCRETE MAXIMUM PRINCIPLE Proceedings of the Czech Japanese Seminar in Applied Mathematics 2005 Kuju Training Center, Oita, Japan, September 15-18, 2005 pp. 69 76 NUMERICAL SOLUTION OF CONVECTION DIFFUSION EQUATIONS USING UPWINDING

More information

Math background. Physics. Simulation. Related phenomena. Frontiers in graphics. Rigid fluids

Math background. Physics. Simulation. Related phenomena. Frontiers in graphics. Rigid fluids Fluid dynamics Math background Physics Simulation Related phenomena Frontiers in graphics Rigid fluids Fields Domain Ω R2 Scalar field f :Ω R Vector field f : Ω R2 Types of derivatives Derivatives measure

More information

AMS subject classifications. Primary, 65N15, 65N30, 76D07; Secondary, 35B45, 35J50

AMS subject classifications. Primary, 65N15, 65N30, 76D07; Secondary, 35B45, 35J50 A SIMPLE FINITE ELEMENT METHOD FOR THE STOKES EQUATIONS LIN MU AND XIU YE Abstract. The goal of this paper is to introduce a simple finite element method to solve the Stokes equations. This method is in

More information

Chapter 9: Differential Analysis

Chapter 9: Differential Analysis 9-1 Introduction 9-2 Conservation of Mass 9-3 The Stream Function 9-4 Conservation of Linear Momentum 9-5 Navier Stokes Equation 9-6 Differential Analysis Problems Recall 9-1 Introduction (1) Chap 5: Control

More information

Part IV: Numerical schemes for the phase-filed model

Part IV: Numerical schemes for the phase-filed model Part IV: Numerical schemes for the phase-filed model Jie Shen Department of Mathematics Purdue University IMS, Singapore July 29-3, 29 The complete set of governing equations Find u, p, (φ, ξ) such that

More information

LEAST-SQUARES FINITE ELEMENT MODELS

LEAST-SQUARES FINITE ELEMENT MODELS LEAST-SQUARES FINITE ELEMENT MODELS General idea of the least-squares formulation applied to an abstract boundary-value problem Works of our group Application to Poisson s equation Application to flows

More information

Block-Structured Adaptive Mesh Refinement

Block-Structured Adaptive Mesh Refinement Block-Structured Adaptive Mesh Refinement Lecture 2 Incompressible Navier-Stokes Equations Fractional Step Scheme 1-D AMR for classical PDE s hyperbolic elliptic parabolic Accuracy considerations Bell

More information

Chapter 9: Differential Analysis of Fluid Flow

Chapter 9: Differential Analysis of Fluid Flow of Fluid Flow Objectives 1. Understand how the differential equations of mass and momentum conservation are derived. 2. Calculate the stream function and pressure field, and plot streamlines for a known

More information

Conservation Laws: Systematic Construction, Noether s Theorem, Applications, and Symbolic Computations.

Conservation Laws: Systematic Construction, Noether s Theorem, Applications, and Symbolic Computations. Conservation Laws: Systematic Construction, Noether s Theorem, Applications, and Symbolic Computations. Alexey Shevyakov Department of Mathematics and Statistics, University of Saskatchewan, Saskatoon,

More information

A PRACTICALLY UNCONDITIONALLY GRADIENT STABLE SCHEME FOR THE N-COMPONENT CAHN HILLIARD SYSTEM

A PRACTICALLY UNCONDITIONALLY GRADIENT STABLE SCHEME FOR THE N-COMPONENT CAHN HILLIARD SYSTEM A PRACTICALLY UNCONDITIONALLY GRADIENT STABLE SCHEME FOR THE N-COMPONENT CAHN HILLIARD SYSTEM Hyun Geun LEE 1, Jeong-Whan CHOI 1 and Junseok KIM 1 1) Department of Mathematics, Korea University, Seoul

More information

Time-dependent Dirichlet Boundary Conditions in Finite Element Discretizations

Time-dependent Dirichlet Boundary Conditions in Finite Element Discretizations Time-dependent Dirichlet Boundary Conditions in Finite Element Discretizations Peter Benner and Jan Heiland November 5, 2015 Seminar Talk at Uni Konstanz Introduction Motivation A controlled physical processes

More information

The incompressible Navier-Stokes equations in vacuum

The incompressible Navier-Stokes equations in vacuum The incompressible, Université Paris-Est Créteil Piotr Bogus law Mucha, Warsaw University Journées Jeunes EDPistes 218, Institut Elie Cartan, Université de Lorraine March 23th, 218 Incompressible Navier-Stokes

More information

LOCAL WELL-POSEDNESS FOR AN ERICKSEN-LESLIE S PARABOLIC-HYPERBOLIC COMPRESSIBLE NON-ISOTHERMAL MODEL FOR LIQUID CRYSTALS

LOCAL WELL-POSEDNESS FOR AN ERICKSEN-LESLIE S PARABOLIC-HYPERBOLIC COMPRESSIBLE NON-ISOTHERMAL MODEL FOR LIQUID CRYSTALS Electronic Journal of Differential Equations, Vol. 017 (017), No. 3, pp. 1 8. ISSN: 107-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu LOCAL WELL-POSEDNESS FOR AN ERICKSEN-LESLIE S

More information

ON THE STRONG SOLUTIONS OF THE INHOMOGENEOUS INCOMPRESSIBLE NAVIER-STOKES EQUATIONS IN A THIN DOMAIN

ON THE STRONG SOLUTIONS OF THE INHOMOGENEOUS INCOMPRESSIBLE NAVIER-STOKES EQUATIONS IN A THIN DOMAIN ON THE STRONG SOLUTIONS OF THE INHOMOGENEOUS INCOMPRESSIBLE NAVIER-STOKES EQUATIONS IN A THIN DOMAIN XIAN LIAO Abstract. In this work we will show the global existence of the strong solutions of the inhomogeneous

More information

On the local well-posedness of compressible viscous flows with bounded density

On the local well-posedness of compressible viscous flows with bounded density On the local well-posedness of compressible viscous flows with bounded density Marius Paicu University of Bordeaux joint work with Raphaël Danchin and Francesco Fanelli Mathflows 2018, Porquerolles September

More information

Adaptive methods for control problems with finite-dimensional control space

Adaptive methods for control problems with finite-dimensional control space Adaptive methods for control problems with finite-dimensional control space Saheed Akindeinde and Daniel Wachsmuth Johann Radon Institute for Computational and Applied Mathematics (RICAM) Austrian Academy

More information

Goal. Robust A Posteriori Error Estimates for Stabilized Finite Element Discretizations of Non-Stationary Convection-Diffusion Problems.

Goal. Robust A Posteriori Error Estimates for Stabilized Finite Element Discretizations of Non-Stationary Convection-Diffusion Problems. Robust A Posteriori Error Estimates for Stabilized Finite Element s of Non-Stationary Convection-Diffusion Problems L. Tobiska and R. Verfürth Universität Magdeburg Ruhr-Universität Bochum www.ruhr-uni-bochum.de/num

More information

Non-Newtonian Fluids and Finite Elements

Non-Newtonian Fluids and Finite Elements Non-Newtonian Fluids and Finite Elements Janice Giudice Oxford University Computing Laboratory Keble College Talk Outline Motivating Industrial Process Multiple Extrusion of Pastes Governing Equations

More information

Finite difference MAC scheme for compressible Navier-Stokes equations

Finite difference MAC scheme for compressible Navier-Stokes equations Finite difference MAC scheme for compressible Navier-Stokes equations Bangwei She with R. Hošek, H. Mizerova Workshop on Mathematical Fluid Dynamics, Bad Boll May. 07 May. 11, 2018 Compressible barotropic

More information

FDM for parabolic equations

FDM for parabolic equations FDM for parabolic equations Consider the heat equation where Well-posed problem Existence & Uniqueness Mass & Energy decreasing FDM for parabolic equations CNFD Crank-Nicolson + 2 nd order finite difference

More information

1 Introduction. J.-L. GUERMOND and L. QUARTAPELLE 1 On incremental projection methods

1 Introduction. J.-L. GUERMOND and L. QUARTAPELLE 1 On incremental projection methods J.-L. GUERMOND and L. QUARTAPELLE 1 On incremental projection methods 1 Introduction Achieving high order time-accuracy in the approximation of the incompressible Navier Stokes equations by means of fractional-step

More information

A Two-Grid Stabilization Method for Solving the Steady-State Navier-Stokes Equations

A Two-Grid Stabilization Method for Solving the Steady-State Navier-Stokes Equations A Two-Grid Stabilization Method for Solving the Steady-State Navier-Stokes Equations Songul Kaya and Béatrice Rivière Abstract We formulate a subgrid eddy viscosity method for solving the steady-state

More information

Introduction to Finite Volume projection methods. On Interfaces with non-zero mass flux

Introduction to Finite Volume projection methods. On Interfaces with non-zero mass flux Introduction to Finite Volume projection methods On Interfaces with non-zero mass flux Rupert Klein Mathematik & Informatik, Freie Universität Berlin Summerschool SPP 1506 Darmstadt, July 09, 2010 Introduction

More information

Efficient FEM-multigrid solver for granular material

Efficient FEM-multigrid solver for granular material Efficient FEM-multigrid solver for granular material S. Mandal, A. Ouazzi, S. Turek Chair for Applied Mathematics and Numerics (LSIII), TU Dortmund STW user committee meeting Enschede, 25th September,

More information

A Domain Decomposition Method for Quasilinear Elliptic PDEs Using Mortar Finite Elements

A Domain Decomposition Method for Quasilinear Elliptic PDEs Using Mortar Finite Elements W I S S E N T E C H N I K L E I D E N S C H A F T A Domain Decomposition Method for Quasilinear Elliptic PDEs Using Mortar Finite Elements Matthias Gsell and Olaf Steinbach Institute of Computational Mathematics

More information

A STOKES INTERFACE PROBLEM: STABILITY, FINITE ELEMENT ANALYSIS AND A ROBUST SOLVER

A STOKES INTERFACE PROBLEM: STABILITY, FINITE ELEMENT ANALYSIS AND A ROBUST SOLVER European Congress on Computational Methods in Applied Sciences and Engineering ECCOMAS 2004 P. Neittaanmäki, T. Rossi, K. Majava, and O. Pironneau (eds.) O. Nevanlinna and R. Rannacher (assoc. eds.) Jyväskylä,

More information

On Pressure Stabilization Method and Projection Method for Unsteady Navier-Stokes Equations 1

On Pressure Stabilization Method and Projection Method for Unsteady Navier-Stokes Equations 1 On Pressure Stabilization Method and Projection Method for Unsteady Navier-Stokes Equations 1 Jie Shen Department of Mathematics, Penn State University University Park, PA 1682 Abstract. We present some

More information

An Extended Finite Element Method for a Two-Phase Stokes problem

An Extended Finite Element Method for a Two-Phase Stokes problem XFEM project An Extended Finite Element Method for a Two-Phase Stokes problem P. Lederer, C. Pfeiler, C. Wintersteiger Advisor: Dr. C. Lehrenfeld August 5, 2015 Contents 1 Problem description 2 1.1 Physics.........................................

More information

Optimal control in fluid mechanics by finite elements with symmetric stabilization

Optimal control in fluid mechanics by finite elements with symmetric stabilization Computational Sciences Center Optimal control in fluid mechanics by finite elements with symmetric stabilization Malte Braack Mathematisches Seminar Christian-Albrechts-Universität zu Kiel VMS Worshop

More information

Stochastic Shear Thickening Fluids: Strong Convergence of the Galerkin Approximation and the Energy Equality 1

Stochastic Shear Thickening Fluids: Strong Convergence of the Galerkin Approximation and the Energy Equality 1 Stochastic Shear Thickening Fluids: Strong Convergence of the Galerkin Approximation and the Energy Equality Nobuo Yoshida Contents The stochastic power law fluids. Terminology from hydrodynamics....................................

More information

Viscous capillary fluids in fast rotation

Viscous capillary fluids in fast rotation Viscous capillary fluids in fast rotation Centro di Ricerca Matematica Ennio De Giorgi SCUOLA NORMALE SUPERIORE BCAM BASQUE CENTER FOR APPLIED MATHEMATICS BCAM Scientific Seminar Bilbao May 19, 2015 Contents

More information

1. INTRODUCTION 2. PROBLEM FORMULATION ROMAI J., 6, 2(2010), 1 13

1. INTRODUCTION 2. PROBLEM FORMULATION ROMAI J., 6, 2(2010), 1 13 Contents 1 A product formula approach to an inverse problem governed by nonlinear phase-field transition system. Case 1D Tommaso Benincasa, Costică Moroşanu 1 v ROMAI J., 6, 2(21), 1 13 A PRODUCT FORMULA

More information

Vortex-like finite-energy asymptotic profiles for isentropic compressible flows

Vortex-like finite-energy asymptotic profiles for isentropic compressible flows Vortex-like finite-energy asymptotic profiles for isentropic compressible flows L.Miguel Rodrigues Institut Fourier, U.M.R. C.N.R.S. 558 Université de Grenoble I B.P. 74 384 Saint-Martin-d Hères, France

More information

Simulation of free surface fluids in incompressible dynamique

Simulation of free surface fluids in incompressible dynamique Simulation of free surface fluids in incompressible dynamique Dena Kazerani INRIA Paris Supervised by Pascal Frey at Laboratoire Jacques-Louis Lions-UPMC Workshop on Numerical Modeling of Liquid-Vapor

More information

OPTIMAL CONVERGENCE RATES FOR THE COMPRESSIBLE NAVIER-STOKES EQUATIONS WITH POTENTIAL FORCES

OPTIMAL CONVERGENCE RATES FOR THE COMPRESSIBLE NAVIER-STOKES EQUATIONS WITH POTENTIAL FORCES OPTIMAL CONVERGENCE RATES FOR THE COMPRESSIBLE NAVIER-STOKES EQUATIONS WITH POTENTIAL FORCES RENJUN DUAN Department of Mathematics, City University of Hong Kong 83 Tat Chee Avenue, Kowloon, Hong Kong,

More information

INSTITUTE of MATHEMATICS. ACADEMY of SCIENCES of the CZECH REPUBLIC

INSTITUTE of MATHEMATICS. ACADEMY of SCIENCES of the CZECH REPUBLIC INSTITUTEofMATHEMATICS Academy of Sciences Czech Republic INSTITUTE of MATHEMATICS ACADEMY of SCIENCES of the CZECH REPUBLIC On weak solutions to a diffuse interface model of a binary mixture of compressible

More information

An Overview of Fluid Animation. Christopher Batty March 11, 2014

An Overview of Fluid Animation. Christopher Batty March 11, 2014 An Overview of Fluid Animation Christopher Batty March 11, 2014 What distinguishes fluids? What distinguishes fluids? No preferred shape. Always flows when force is applied. Deforms to fit its container.

More information

Mixed Finite Elements Method

Mixed Finite Elements Method Mixed Finite Elements Method A. Ratnani 34, E. Sonnendrücker 34 3 Max-Planck Institut für Plasmaphysik, Garching, Germany 4 Technische Universität München, Garching, Germany Contents Introduction 2. Notations.....................................

More information

Entropy and Relative Entropy

Entropy and Relative Entropy Entropy and Relative Entropy Joshua Ballew University of Maryland October 24, 2012 Outline Hyperbolic PDEs Entropy/Entropy Flux Pairs Relative Entropy Weak-Strong Uniqueness Weak-Strong Uniqueness for

More information

Conservation Laws of Surfactant Transport Equations

Conservation Laws of Surfactant Transport Equations Conservation Laws of Surfactant Transport Equations Alexei Cheviakov Department of Mathematics and Statistics, University of Saskatchewan, Saskatoon, Canada Winter 2011 CMS Meeting Dec. 10, 2011 A. Cheviakov

More information

Nonlinear Diffusion. The Porous Medium Equation. From Analysis to Physics and Geometry

Nonlinear Diffusion. The Porous Medium Equation. From Analysis to Physics and Geometry Nonlinear Diffusion. The Porous Medium Equation. From Analysis to Physics and Geometry Juan Luis Vázquez Departamento de Matemáticas Universidad Autónoma de Madrid http://www.uam.es/personal pdi/ciencias/jvazquez/

More information

Nonlinear elliptic systems with exponential nonlinearities

Nonlinear elliptic systems with exponential nonlinearities 22-Fez conference on Partial Differential Equations, Electronic Journal of Differential Equations, Conference 9, 22, pp 139 147. http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu

More information

INSTITUTE OF MATHEMATICS THE CZECH ACADEMY OF SCIENCES. Homogenization of a non homogeneous heat conducting fluid

INSTITUTE OF MATHEMATICS THE CZECH ACADEMY OF SCIENCES. Homogenization of a non homogeneous heat conducting fluid INSTITUTE OF MATHEMATICS THE CZECH ACADEMY OF SCIENCES Homogenization of a non homogeneous heat conducting fluid Eduard Feireisl Yong Lu Yongzhong Sun Preprint No. 16-2018 PRAHA 2018 Homogenization of

More information

Remarks on the analysis of finite element methods on a Shishkin mesh: are Scott-Zhang interpolants applicable?

Remarks on the analysis of finite element methods on a Shishkin mesh: are Scott-Zhang interpolants applicable? Remarks on the analysis of finite element methods on a Shishkin mesh: are Scott-Zhang interpolants applicable? Thomas Apel, Hans-G. Roos 22.7.2008 Abstract In the first part of the paper we discuss minimal

More information

Nonlinear Diffusion. Porous Medium and Fast Diffusion. From Analysis to Physics and Geometry

Nonlinear Diffusion. Porous Medium and Fast Diffusion. From Analysis to Physics and Geometry Juan L. Vázquez - Nonlinear Diffusion. Porous Medium and Fast Diffusion Equations p. 1/77 Nonlinear Diffusion. Porous Medium and Fast Diffusion. From Analysis to Physics and Geometry Juan Luis Vázquez

More information

NUMERICAL SIMULATION OF INTERACTION BETWEEN INCOMPRESSIBLE FLOW AND AN ELASTIC WALL

NUMERICAL SIMULATION OF INTERACTION BETWEEN INCOMPRESSIBLE FLOW AND AN ELASTIC WALL Proceedings of ALGORITMY 212 pp. 29 218 NUMERICAL SIMULATION OF INTERACTION BETWEEN INCOMPRESSIBLE FLOW AND AN ELASTIC WALL MARTIN HADRAVA, MILOSLAV FEISTAUER, AND PETR SVÁČEK Abstract. The present paper

More information

Lecture Note III: Least-Squares Method

Lecture Note III: Least-Squares Method Lecture Note III: Least-Squares Method Zhiqiang Cai October 4, 004 In this chapter, we shall present least-squares methods for second-order scalar partial differential equations, elastic equations of solids,

More information

Finite Element Techniques for the Numerical Simulation of Two-Phase Flows with Mass Transport

Finite Element Techniques for the Numerical Simulation of Two-Phase Flows with Mass Transport Finite Element Techniques for the Numerical Simulation of Two-Phase Flows with Mass Transport Christoph Lehrenfeld and Arnold Reusken Preprint No. 413 December 2014 Key words: Two-phase flow, mass transport,

More information

A Finite Element Method Using Singular Functions for Poisson Equations: Mixed Boundary Conditions

A Finite Element Method Using Singular Functions for Poisson Equations: Mixed Boundary Conditions A Finite Element Method Using Singular Functions for Poisson Equations: Mixed Boundary Conditions Zhiqiang Cai Seokchan Kim Sangdong Kim Sooryun Kong Abstract In [7], we proposed a new finite element method

More information

Detailed 3D modelling of mass transfer processes in two phase flows with dynamic interfaces

Detailed 3D modelling of mass transfer processes in two phase flows with dynamic interfaces Detailed 3D modelling of mass transfer processes in two phase flows with dynamic interfaces D. Darmana, N.G. Deen, J.A.M. Kuipers Fundamentals of Chemical Reaction Engineering, Faculty of Science and Technology,

More information

A Nonoverlapping Subdomain Algorithm with Lagrange Multipliers and its Object Oriented Implementation for Interface Problems

A Nonoverlapping Subdomain Algorithm with Lagrange Multipliers and its Object Oriented Implementation for Interface Problems Contemporary Mathematics Volume 8, 998 B 0-88-0988--03030- A Nonoverlapping Subdomain Algorithm with Lagrange Multipliers and its Object Oriented Implementation for Interface Problems Daoqi Yang. Introduction

More information

CALCULUS OF VARIATIONS, PARTIAL DIFFERENTIAL EQUATIONS, AND GEOMETRY

CALCULUS OF VARIATIONS, PARTIAL DIFFERENTIAL EQUATIONS, AND GEOMETRY CALCULUS OF VARIATIONS, PARTIAL DIFFERENTIAL EQUATIONS, AND GEOMETRY Fabrice Bethuel Université Pierre et Marie Curie, Paris, France Keywords: Minimization, compactness, minimal surfaces, parameterization,

More information

fluid mechanics as a prominent discipline of application for numerical

fluid mechanics as a prominent discipline of application for numerical 1. fluid mechanics as a prominent discipline of application for numerical simulations: experimental fluid mechanics: wind tunnel studies, laser Doppler anemometry, hot wire techniques,... theoretical fluid

More information

ON SINGULAR PERTURBATION OF THE STOKES PROBLEM

ON SINGULAR PERTURBATION OF THE STOKES PROBLEM NUMERICAL ANALYSIS AND MATHEMATICAL MODELLING BANACH CENTER PUBLICATIONS, VOLUME 9 INSTITUTE OF MATHEMATICS POLISH ACADEMY OF SCIENCES WARSZAWA 994 ON SINGULAR PERTURBATION OF THE STOKES PROBLEM G. M.

More information

ELLIPTIC RECONSTRUCTION AND A POSTERIORI ERROR ESTIMATES FOR PARABOLIC PROBLEMS

ELLIPTIC RECONSTRUCTION AND A POSTERIORI ERROR ESTIMATES FOR PARABOLIC PROBLEMS ELLIPTIC RECONSTRUCTION AND A POSTERIORI ERROR ESTIMATES FOR PARABOLIC PROBLEMS CHARALAMBOS MAKRIDAKIS AND RICARDO H. NOCHETTO Abstract. It is known that the energy technique for a posteriori error analysis

More information

Author(s) Huang, Feimin; Matsumura, Akitaka; Citation Osaka Journal of Mathematics. 41(1)

Author(s) Huang, Feimin; Matsumura, Akitaka; Citation Osaka Journal of Mathematics. 41(1) Title On the stability of contact Navier-Stokes equations with discont free b Authors Huang, Feimin; Matsumura, Akitaka; Citation Osaka Journal of Mathematics. 4 Issue 4-3 Date Text Version publisher URL

More information

20. A Dual-Primal FETI Method for solving Stokes/Navier-Stokes Equations

20. A Dual-Primal FETI Method for solving Stokes/Navier-Stokes Equations Fourteenth International Conference on Domain Decomposition Methods Editors: Ismael Herrera, David E. Keyes, Olof B. Widlund, Robert Yates c 23 DDM.org 2. A Dual-Primal FEI Method for solving Stokes/Navier-Stokes

More information

Space-time XFEM for two-phase mass transport

Space-time XFEM for two-phase mass transport Space-time XFEM for two-phase mass transport Space-time XFEM for two-phase mass transport Christoph Lehrenfeld joint work with Arnold Reusken EFEF, Prague, June 5-6th 2015 Christoph Lehrenfeld EFEF, Prague,

More information

Solving PDEs with freefem++

Solving PDEs with freefem++ Solving PDEs with freefem++ Tutorials at Basque Center BCA Olivier Pironneau 1 with Frederic Hecht, LJLL-University of Paris VI 1 March 13, 2011 Do not forget That everything about freefem++ is at www.freefem.org

More information

Lattice Boltzmann Method for Fluid Simulations

Lattice Boltzmann Method for Fluid Simulations 1 / 16 Lattice Boltzmann Method for Fluid Simulations Yuanxun Bill Bao & Justin Meskas Simon Fraser University April 7, 2011 2 / 16 Ludwig Boltzmann and His Kinetic Theory of Gases The Boltzmann Transport

More information

Approximation of fluid-structure interaction problems with Lagrange multiplier

Approximation of fluid-structure interaction problems with Lagrange multiplier Approximation of fluid-structure interaction problems with Lagrange multiplier Daniele Boffi Dipartimento di Matematica F. Casorati, Università di Pavia http://www-dimat.unipv.it/boffi May 30, 2016 Outline

More information

POD for Parametric PDEs and for Optimality Systems

POD for Parametric PDEs and for Optimality Systems POD for Parametric PDEs and for Optimality Systems M. Kahlbacher, K. Kunisch, H. Müller and S. Volkwein Institute for Mathematics and Scientific Computing University of Graz, Austria DMV-Jahrestagung 26,

More information

ERROR ANALYSIS OF STABILIZED SEMI-IMPLICIT METHOD OF ALLEN-CAHN EQUATION. Xiaofeng Yang. (Communicated by Jie Shen)

ERROR ANALYSIS OF STABILIZED SEMI-IMPLICIT METHOD OF ALLEN-CAHN EQUATION. Xiaofeng Yang. (Communicated by Jie Shen) DISCRETE AND CONTINUOUS doi:1.3934/dcdsb.29.11.157 DYNAMICAL SYSTEMS SERIES B Volume 11, Number 4, June 29 pp. 157 17 ERROR ANALYSIS OF STABILIZED SEMI-IMPLICIT METHOD OF ALLEN-CAHN EQUATION Xiaofeng Yang

More information

GRAND SOBOLEV SPACES AND THEIR APPLICATIONS TO VARIATIONAL PROBLEMS

GRAND SOBOLEV SPACES AND THEIR APPLICATIONS TO VARIATIONAL PROBLEMS LE MATEMATICHE Vol. LI (1996) Fasc. II, pp. 335347 GRAND SOBOLEV SPACES AND THEIR APPLICATIONS TO VARIATIONAL PROBLEMS CARLO SBORDONE Dedicated to Professor Francesco Guglielmino on his 7th birthday W

More information

Asymptotic Behavior of a Hyperbolic-parabolic Coupled System Arising in Fluid-structure Interaction

Asymptotic Behavior of a Hyperbolic-parabolic Coupled System Arising in Fluid-structure Interaction International Series of Numerical Mathematics, Vol. 154, 445 455 c 2006 Birkhäuser Verlag Basel/Switzerland Asymptotic Behavior of a Hyperbolic-parabolic Coupled System Arising in Fluid-structure Interaction

More information

On a variational inequality of Bingham and Navier-Stokes type in three dimension

On a variational inequality of Bingham and Navier-Stokes type in three dimension PDEs for multiphase ADvanced MATerials Palazzone, Cortona (Arezzo), Italy, September 17-21, 2012 On a variational inequality of Bingham and Navier-Stokes type in three dimension Takeshi FUKAO Kyoto University

More information

Suboptimal Open-loop Control Using POD. Stefan Volkwein

Suboptimal Open-loop Control Using POD. Stefan Volkwein Institute for Mathematics and Scientific Computing University of Graz, Austria PhD program in Mathematics for Technology Catania, May 22, 2007 Motivation Optimal control of evolution problems: min J(y,

More information

Modelling of interfaces and free boundaries

Modelling of interfaces and free boundaries University of Regensburg Regensburg, March 2009 Outline 1 Introduction 2 Obstacle problems 3 Stefan problem 4 Shape optimization Introduction What is a free boundary problem? Solve a partial differential

More information

A Least-Squares Finite Element Approximation for the Compressible Stokes Equations

A Least-Squares Finite Element Approximation for the Compressible Stokes Equations A Least-Squares Finite Element Approximation for the Compressible Stokes Equations Zhiqiang Cai, 1 Xiu Ye 1 Department of Mathematics, Purdue University, 1395 Mathematical Science Building, West Lafayette,

More information

Space-time Finite Element Methods for Parabolic Evolution Problems

Space-time Finite Element Methods for Parabolic Evolution Problems Space-time Finite Element Methods for Parabolic Evolution Problems with Variable Coefficients Ulrich Langer, Martin Neumüller, Andreas Schafelner Johannes Kepler University, Linz Doctoral Program Computational

More information

Simulation of T-junction using LBM and VOF ENERGY 224 Final Project Yifan Wang,

Simulation of T-junction using LBM and VOF ENERGY 224 Final Project Yifan Wang, Simulation of T-junction using LBM and VOF ENERGY 224 Final Project Yifan Wang, yfwang09@stanford.edu 1. Problem setting In this project, we present a benchmark simulation for segmented flows, which contain

More information

PROJECTION METHOD III: SPATIAL DISCRETIZATION ON THE STAGGERED GRID

PROJECTION METHOD III: SPATIAL DISCRETIZATION ON THE STAGGERED GRID MATHEMATICS OF COMPUTATION Volume 71, Number 237, Pages 27 47 S 0025-5718(01)01313-8 Article electronically published on May 14, 2001 PROJECTION METHOD III: SPATIAL DISCRETIZATION ON THE STAGGERED GRID

More information

Investigation of an implicit solver for the simulation of bubble oscillations using Basilisk

Investigation of an implicit solver for the simulation of bubble oscillations using Basilisk Investigation of an implicit solver for the simulation of bubble oscillations using Basilisk D. Fuster, and S. Popinet Sorbonne Universités, UPMC Univ Paris 6, CNRS, UMR 79 Institut Jean Le Rond d Alembert,

More information

TRANSPORT IN POROUS MEDIA

TRANSPORT IN POROUS MEDIA 1 TRANSPORT IN POROUS MEDIA G. ALLAIRE CMAP, Ecole Polytechnique 1. Introduction 2. Main result in an unbounded domain 3. Asymptotic expansions with drift 4. Two-scale convergence with drift 5. The case

More information

A Projection FEM for Variable Density Incompressible Flows

A Projection FEM for Variable Density Incompressible Flows Journal of Computational Physics 65, 67 88 (000) doi:0.006/jcph.000.6609, available online at http://www.idealibrary.com on A Projection FEM for Variable Density Incompressible Flows J.-L. Guermond and

More information

On the well-posedness of the Prandtl boundary layer equation

On the well-posedness of the Prandtl boundary layer equation On the well-posedness of the Prandtl boundary layer equation Vlad Vicol Department of Mathematics, The University of Chicago Incompressible Fluids, Turbulence and Mixing In honor of Peter Constantin s

More information

Zdzislaw Brzeźniak. Department of Mathematics University of York. joint works with Mauro Mariani (Roma 1) and Gaurav Dhariwal (York)

Zdzislaw Brzeźniak. Department of Mathematics University of York. joint works with Mauro Mariani (Roma 1) and Gaurav Dhariwal (York) Navier-Stokes equations with constrained L 2 energy of the solution Zdzislaw Brzeźniak Department of Mathematics University of York joint works with Mauro Mariani (Roma 1) and Gaurav Dhariwal (York) LMS

More information

Technische Universität Berlin

Technische Universität Berlin Technische Universität Berlin Institut für Mathematik Regularity of the adjoint state for the instationary Navier-Stokes equations Arnd Rösch, Daniel Wachsmuth Preprint 1-4 Preprint-Reihe des Instituts

More information

Generalized Forchheimer Equations for Porous Media. Part V.

Generalized Forchheimer Equations for Porous Media. Part V. Generalized Forchheimer Equations for Porous Media. Part V. Luan Hoang,, Akif Ibragimov, Thinh Kieu and Zeev Sobol Department of Mathematics and Statistics, Texas Tech niversity Mathematics Department,

More information

Existence of Weak Solutions to a Class of Non-Newtonian Flows

Existence of Weak Solutions to a Class of Non-Newtonian Flows Existence of Weak Solutions to a Class of Non-Newtonian Flows 1. Introduction and statement of the result. Ladyzhenskaya [8]. Newtonian : Air, other gases, water, motor oil, alcohols, simple hydrocarbon

More information

Level Set-based Topology Optimization Method for Viscous Flow Using Lattice Boltzmann Method

Level Set-based Topology Optimization Method for Viscous Flow Using Lattice Boltzmann Method 10 th World Congress on Structural and Multidisciplinary Optimization May 19-24, 2013, Orlando, Florida, USA Level Set-based Topology Optimization Method for Viscous Flow Using Lattice Boltzmann Method

More information

Mathematical analysis of the stationary Navier-Stokes equations

Mathematical analysis of the stationary Navier-Stokes equations Mathematical analysis of the Department of Mathematics, Sogang University, Republic of Korea The 3rd GCOE International Symposium Weaving Science Web beyond Particle Matter Hierarchy February 17-19, 2011,

More information

Local discontinuous Galerkin methods for elliptic problems

Local discontinuous Galerkin methods for elliptic problems COMMUNICATIONS IN NUMERICAL METHODS IN ENGINEERING Commun. Numer. Meth. Engng 2002; 18:69 75 [Version: 2000/03/22 v1.0] Local discontinuous Galerkin methods for elliptic problems P. Castillo 1 B. Cockburn

More information

Hidden Regularity for a Nonlinear Hyperbolic Equation with a Resistance Term

Hidden Regularity for a Nonlinear Hyperbolic Equation with a Resistance Term International Mathematical Forum, 4, 2009, no. 11, 511-520 Hidden Regularity for a Nonlinear Hyperbolic Equation with a Resistance Term G. O. Antunes Instituto de Matemática e Estatística Universidade

More information

GLOBAL WEAK SOLUTION TO THE MAGNETOHYDRODYNAMIC AND VLASOV EQUATIONS

GLOBAL WEAK SOLUTION TO THE MAGNETOHYDRODYNAMIC AND VLASOV EQUATIONS GLOBAL WEAK SOLUTION TO THE MAGNETOHYDRODYNAMIC AND VLASOV EQUATIONS ROBIN MING CHEN, JILONG HU, AND DEHUA WANG Abstract. An initial-boundary value problem for the fluid-particle system of the inhomogeneous

More information

Before we consider two canonical turbulent flows we need a general description of turbulence.

Before we consider two canonical turbulent flows we need a general description of turbulence. Chapter 2 Canonical Turbulent Flows Before we consider two canonical turbulent flows we need a general description of turbulence. 2.1 A Brief Introduction to Turbulence One way of looking at turbulent

More information