APPLIED COMPUTATIONAL FLUID DYNAMICS TECHNIQUES

Size: px
Start display at page:

Download "APPLIED COMPUTATIONAL FLUID DYNAMICS TECHNIQUES"

Transcription

1 APPLIED COMPUTATIONAL FLUID DYNAMICS TECHNIQUES AN INTRODUCTION BASED ON FINITE ELEMENT METHODS Second Edition Rainald Löhner Center for Computational Fluid Dynamics, Department of Computational and Data Sciences, College of Sciences, George Mason University, Fairfax, Virginia, USA John Wiley & Sons, Ltd c

2 CONTENTS FOREWORD TO THE SECOND EDITION ACKNOWLEDGEMENTS xiv xvii 1 INTRODUCTION AND GENERAL CONSIDERATIONS The CFD code Porting research codes to an industrial context Scope of the book 5 2 DATA STRUCTURES AND ALGORITHMS Representation of a grid Derived data structures for static data Elements surrounding points - linked lists Points surrounding points Elements surrounding elements Edges External faces Edges of an dement Derived data structures for dynamic data N-trees Sorting and searching Heap lists Proximity in space Bins Binary trees Quadtrees and octrees Nearest-neighbours and graphs Distance to surface 30 3 GRID GENERATION Description of the domain to be gridded Analytical functions Discretedata Variation of dement size and shape Internal measures of grid quality Analytical functions ^ Boxes ) 39

3 CONTENTS Point/line/surface sources Background grids Element size attached to CAD data Adaptive background grids Surface gridding with adaptive background grids Element type Automatic grid generation methods Other grid generation methods The advancing front technique Checking the intersection of faces Data structures to minimize search overheads Additional techniques to increase speed Additional techniques to enhance reliability Delaunay triangulation Circumsphere calculations Data structures to minimize search overheads Boundary recovery Additional techniques to increase speed Additional techniques to enhance reliability and quality Grid improvement Removal of bad elements Laplacian smoothing Grid optimization Selective mesh movement Diagonal swapping Optimal space-filling tetrahedra Grids with uniform cores Volume-to-surface meshing Navier-Stokes gridding techniques Design criteria for RANS gridders Smoothing of surface normals Point distribution along normals Subdivision of prisms into tetrahedra Element removal criteria Filling space with points/arbitrary objects The advancing front space-filling algorithm Point/object placement stencils Boundary consistency checks Maximum compaction techniques Arbitrary objects Deposition patterns Applications Space Shuttle ascend configuration PilotejectingfromF Circleof Willis Generic submarine body 105

4 Vll Ahmed carbody Track PointcloudforF Hopper füled with beans/ellipsoids Cube Med with spheres of different sizes APPROXIMATION THEORY The basic problem Point fitting Weighted residual methods Least-squares formulation Choice of trial functions Constant trial functions in one dimension Linear trial functions in one dimension Quadratic trial functions in one dimension Linear trial functions in two dimensions Quadratic trial functions in two dimensions General properties of shape functions Weighted residual methods with local functions Accuracy and effort Grid estimates APPROXIMATION OF OPERATORS Taxonomy of methods Finite difference methods Finite volume methods Galerkin finite dement methods Petrov-Galerkin finite dement methods Spectral dement methods The Poisson Operator Minimization problem An example Tutorial: code fragment for heat equation Recovery of derivatives First derivatives Second derivatives Higher derivatives DISCRETIZATION IN TIME Explicit schemes Implicit schemes Situations where implicit schemes pay off A word of caution 136

5 Vlll CONTENTS 7 SOLUTION OF LARGE SYSTEMS OF EQUATIONS Direct solvers Gaussian elimination Crout elimination Cholesky elimination Iterative solvers Matrix preconditioning Globalization procedures Multigrid methods The multigrid concept Injection and projection Operators Gridcycling Algorithmic complexity and storage requirements Smoothing An example SIMPLE EULER/NAVIER-STOKES SOLVERS Galerkin approximation Equivalency with FVM Lax-Wendroff(Taylor-Galerkin) Expediting the RHS evaluation Linear elements (triangles, tetrahedra) Solving for the consistent mass matrix Artificial viscosities Boundary conditions Viscous fluxes FLUX-CORRECTED TRANSPORT SCHEMES Algorithmic implementation The limiting procedure Steepening FCT for Taylor-Galerkin schemes Iterative limiting Limiting for Systems of equations Limiting any set of quantities Examples Shocktube Shock diffraction over a wall Summary EDGE-BASED COMPRESSIBLE FLOW SOLVERS The Laplacian Operator First derivatives: first form First derivatives: second form Edge-based schemes for advection-dominated PDEs Exact Riemann solver (Godunov scheme) Approximate Riemann solvers 195

6 IX Scalar limited dissipation Scalar dissipation with pressure sensors Scalar dissipation without gradients Taylor-Galerkin schemes Flux-corrected transport schemes INCOMPRESSIBLE FLOW SOLVERS The advection Operator Integration along characteristics Taylor-Galerkin Edge-based upwinding The divergence Operator Artificial compressibility Temporal discretization: projection schemes Temporal discretization: implicit schemes Temporal discretization of higher order Acceleration to the steady State Local timestepping Reduced pressure iterations Substepping for the advection terms Implicit treatment of the advection terms Projective predictionof pressure increments Examples von Karman vortex street NACA0012wing LPD-17topside flow study DARPA SUBOFF model Generic submarine forebody vortex flow study MESH MOVEMENT The ALE frame of reference Boundary conditions Geometrie conservation law Mesh movement algorithms Smoothingofthevelocityfield Smoothing of the coordinates Prescription via analytic funetions Region of moving elements PDE-based distance funetions Eikonal equation Laplace equation Penalization of deformed elements Special movement techniques for RANS grids Rotating parts/domains 240

7 X CONTENTS 12.9 Applications Multiple spheres PilotejectionfromF Drifting fleet of ships INTERPOLATION Basic Interpolation algorithm Fastest 1-time algorithm: brüte force Fastest iv-time algorithm: octree search Fastest known vicinity algorithm: neighbour-to-neighbour Fastest grid-to-grid algorithm: advancing-front vicinity Layering of brute-force searches Inside-out interpolation Measuring concavity Vectorization Conservative interpolation Conservative and monotonic interpolation Surface-grid-to-surface-grid interpolation Particle-grid interpolation ADAPTIVE MESH REFINEMENT Optimal-mesh criteria Error indicators/estimators Error indicators commonly used Problems with multiple scales Determination of element size and shape Refinement strategies Mesh movement or repositioning (r-methods) Mesh enrichment (h/p-methods) Adaptive remeshing (M-methods) Combinations Tutorial: h-refinement with tetrahedra Algorithmic implementation Examples Convection between concentric cylinders Shock-object interaction in two dimensions Shock-object interaction in three dimensions Shock-structure interaction Object falling into supersonic free stream two dimensions EFFICIENT USE OF COMPUTER HARDWARE Reduction of cache-misses Array access in loops Point renumbering Reordering of nodes within elements Renumbering of edges according to points 306

8 CONTENTS xi Some timings Agglomeration techniques Vector machines Basic edge colouring algorithm Backward/forward strategy Combining vectorizability with data locality Switching algorithm Reduced i/a loops Alternative RHS formation Parallel machines: general considerations Shared-memory parallel machines Local agglomeration Global agglomeration Implementational issues SIMD machines MIMD machines General considerations Load balancing and domain Splitting Parallel flow solvers The effect ofmoore's law on parallel Computing The life cycle of scientific Computing codes Examples The consequences ofmoore's law SPACE-MARCHING AND DEACTIVATION Space-marching Masking of points and edges Renumbering of points and edges Grouping to avoid memory contention Extrapolation of the Solution Treatment of subsonic pockets Measuring convergence Application to transient problems Macro-blocking Examples for space-marching and blocking Deactivation Examples of dynamic deactivation OVERLAPPING GRIDS Interpolation criteria External boundaries and domains Interpolation: initialization Treatment of domains that are partially outside Removal of inactive regions Incremental interpolation Changes to the flow solver 377

9 XÜ CONTENTS 17.8 Examples Sphere in Channel (compressible Euler) Sphere in shear flow (incompressible Navier-Stokes) Spinning missile EMBEDDED AND IMMERSED GRID TECHNIQUES Kinetic treatment of embedded or immersed objects Implementation details Kinematic treatment of embedded surfaces First-order treatment Higher-order treatment Determination of crossed edges Deactivation of interior regions Extrapolation of the Solution Adaptive mesh refinement Load/flux transfer Treatment of gaps or cracks Direct link to particles Examples Sodshocktube Shuttle ascend configuration Blast interaction with a generic ship hüll Generic weapon fragmentation Flow past a sphere Dispersion in an inner city Complex endovascular devices Flow past a VW Golf TREATMENT OF FREE SURFACES Interface fitting methods Free surface discretization Overall scheme Mesh update Examples for surface fitting Practical limitations of free surface fitting Interface capturing methods Extrapolation of the pressure Extrapolation of the velocity Keeping interfaces sharp Imposition of constant mass Deactivation of air region Treatment ofbubbles Adaptive refinement Examples for surface capturing Practical limitations of free surface capturing 448

10 CONTENTS XÜi 20 OPTIMAL SHAPE AND PROCESS DESIGN The general optimization problem Optimization techniques Recursive exhaustive parameter scoping Genetic algorithms Gradient-based algorithms Adjoint solvers Adjoint equations: residuals with first derivatives and source terms Adjoint equations: residuals with second derivatives Jacobians for Euler/Navier-Stokes equations Adjoint solvers Gradient evaluation Geometrie constraints Volume constraint via cost funetion Volume constraint via gradient projeetion Volume constraint via post-processing Approximate gradients Multipoint optimization Representation of surface changes Hierarchical design procedures Topological optimization via porosities Examples Damage assessment for contaminant release External nozzle Wigley hüll KRISO Container ship(kcs) 480 References 481 Index 515

1.2 Numerical Solutions of Flow Problems

1.2 Numerical Solutions of Flow Problems 1.2 Numerical Solutions of Flow Problems DIFFERENTIAL EQUATIONS OF MOTION FOR A SIMPLIFIED FLOW PROBLEM Continuity equation for incompressible flow: 0 Momentum (Navier-Stokes) equations for a Newtonian

More information

Studies of the Continuous and Discrete Adjoint Approaches to Viscous Automatic Aerodynamic Shape Optimization

Studies of the Continuous and Discrete Adjoint Approaches to Viscous Automatic Aerodynamic Shape Optimization Studies of the Continuous and Discrete Adjoint Approaches to Viscous Automatic Aerodynamic Shape Optimization Siva Nadarajah Antony Jameson Stanford University 15th AIAA Computational Fluid Dynamics Conference

More information

NIA CFD Seminar, October 4, 2011 Hyperbolic Seminar, NASA Langley, October 17, 2011

NIA CFD Seminar, October 4, 2011 Hyperbolic Seminar, NASA Langley, October 17, 2011 NIA CFD Seminar, October 4, 2011 Hyperbolic Seminar, NASA Langley, October 17, 2011 First-Order Hyperbolic System Method If you have a CFD book for hyperbolic problems, you have a CFD book for all problems.

More information

Development of a Maxwell Equation Solver for Application to Two Fluid Plasma Models. C. Aberle, A. Hakim, and U. Shumlak

Development of a Maxwell Equation Solver for Application to Two Fluid Plasma Models. C. Aberle, A. Hakim, and U. Shumlak Development of a Maxwell Equation Solver for Application to Two Fluid Plasma Models C. Aberle, A. Hakim, and U. Shumlak Aerospace and Astronautics University of Washington, Seattle American Physical Society

More information

Contents. I The Basic Framework for Stationary Problems 1

Contents. I The Basic Framework for Stationary Problems 1 page v Preface xiii I The Basic Framework for Stationary Problems 1 1 Some model PDEs 3 1.1 Laplace s equation; elliptic BVPs... 3 1.1.1 Physical experiments modeled by Laplace s equation... 5 1.2 Other

More information

Overview and Recent Developments of Dynamic Mesh Capabilities

Overview and Recent Developments of Dynamic Mesh Capabilities Overview and Recent Developments of Dynamic Mesh Capabilities Henrik Rusche and Hrvoje Jasak h.rusche@wikki-gmbh.de and h.jasak@wikki.co.uk Wikki Gmbh, Germany Wikki Ltd, United Kingdom 6th OpenFOAM Workshop,

More information

Computational Fluid Dynamics for Engineers

Computational Fluid Dynamics for Engineers Tuncer Cebeci Jian P. Shao Fassi Kafyeke Eric Laurendeau Computational Fluid Dynamics for Engineers From Panel to Navier-Stokes Methods with Computer Programs With 152 Figures, 19 Tables, 84 Problems and

More information

Solving Partial Differential Equations on Overlapping Grids

Solving Partial Differential Equations on Overlapping Grids **FULL TITLE** ASP Conference Series, Vol. **VOLUME**, **YEAR OF PUBLICATION** **NAMES OF EDITORS** Solving Partial Differential Equations on Overlapping Grids William D. Henshaw Centre for Applied Scientific

More information

The Immersed Interface Method

The Immersed Interface Method The Immersed Interface Method Numerical Solutions of PDEs Involving Interfaces and Irregular Domains Zhiiin Li Kazufumi Ito North Carolina State University Raleigh, North Carolina Society for Industrial

More information

Unstructured Mesh Generation for Implicit Moving Geometries and Level Set Applications

Unstructured Mesh Generation for Implicit Moving Geometries and Level Set Applications Unstructured Mesh Generation for Implicit Moving Geometries and Level Set Applications Per-Olof Persson (persson@mit.edu) Department of Mathematics Massachusetts Institute of Technology http://www.mit.edu/

More information

Development of an Integrated Computational Simulation Method for Fluid Driven Structure Movement and Acoustics

Development of an Integrated Computational Simulation Method for Fluid Driven Structure Movement and Acoustics Development of an Integrated Computational Simulation Method for Fluid Driven Structure Movement and Acoustics I. Pantle Fachgebiet Strömungsmaschinen Karlsruher Institut für Technologie KIT Motivation

More information

Faculty of Mechanical and Manufacturing Engineering, University Tun Hussein Onn Malaysia (UTHM), Parit Raja, Batu Pahat, Johor, Malaysia

Faculty of Mechanical and Manufacturing Engineering, University Tun Hussein Onn Malaysia (UTHM), Parit Raja, Batu Pahat, Johor, Malaysia Applied Mechanics and Materials Vol. 393 (2013) pp 305-310 (2013) Trans Tech Publications, Switzerland doi:10.4028/www.scientific.net/amm.393.305 The Implementation of Cell-Centred Finite Volume Method

More information

The Development of a Navier-Stokes Flow Solver with Preconditioning Method on Unstructured Grids

The Development of a Navier-Stokes Flow Solver with Preconditioning Method on Unstructured Grids Proceedings of the International MultiConference of Engineers and Computer Scientists 213 Vol II, IMECS 213, March 13-15, 213, Hong Kong The Development of a Navier-Stokes Flow Solver with Preconditioning

More information

Multi-Mesh CFD. Chris Roy Chip Jackson (1 st year PhD student) Aerospace and Ocean Engineering Department Virginia Tech

Multi-Mesh CFD. Chris Roy Chip Jackson (1 st year PhD student) Aerospace and Ocean Engineering Department Virginia Tech Multi-Mesh CFD Chris Roy Chip Jackson (1 st year PhD student) Aerospace and Ocean Engineering Department Virginia Tech cjroy@vt.edu May 21, 2014 CCAS Program Review, Columbus, OH 1 Motivation Automated

More information

cuibm A GPU Accelerated Immersed Boundary Method

cuibm A GPU Accelerated Immersed Boundary Method cuibm A GPU Accelerated Immersed Boundary Method S. K. Layton, A. Krishnan and L. A. Barba Corresponding author: labarba@bu.edu Department of Mechanical Engineering, Boston University, Boston, MA, 225,

More information

An Embedded Boundary Method with Adaptive Mesh Refinements

An Embedded Boundary Method with Adaptive Mesh Refinements An Embedded Boundary Method with Adaptive Mesh Refinements Marcos Vanella and Elias Balaras 8 th World Congress on Computational Mechanics, WCCM8 5 th European Congress on Computational Methods in Applied

More information

Lecture 2 Unstructured Mesh Generation

Lecture 2 Unstructured Mesh Generation Lecture 2 Unstructured Mesh Generation MIT 16.930 Advanced Topics in Numerical Methods for Partial Differential Equations Per-Olof Persson (persson@mit.edu) February 13, 2006 1 Mesh Generation Given a

More information

Recent developments for the multigrid scheme of the DLR TAU-Code

Recent developments for the multigrid scheme of the DLR TAU-Code www.dlr.de Chart 1 > 21st NIA CFD Seminar > Axel Schwöppe Recent development s for the multigrid scheme of the DLR TAU-Code > Apr 11, 2013 Recent developments for the multigrid scheme of the DLR TAU-Code

More information

CUDA. Fluid simulation Lattice Boltzmann Models Cellular Automata

CUDA. Fluid simulation Lattice Boltzmann Models Cellular Automata CUDA Fluid simulation Lattice Boltzmann Models Cellular Automata Please excuse my layout of slides for the remaining part of the talk! Fluid Simulation Navier Stokes equations for incompressible fluids

More information

Analysis, extensions and applications of the Finite-Volume Particle Method (FVPM) PN-II-RU-TE Synthesis of the technical report -

Analysis, extensions and applications of the Finite-Volume Particle Method (FVPM) PN-II-RU-TE Synthesis of the technical report - Analysis, extensions and applications of the Finite-Volume Particle Method (FVPM) PN-II-RU-TE-2011-3-0256 - Synthesis of the technical report - Phase 1: Preparation phase Authors: Delia Teleaga, Eliza

More information

Debojyoti Ghosh. Adviser: Dr. James Baeder Alfred Gessow Rotorcraft Center Department of Aerospace Engineering

Debojyoti Ghosh. Adviser: Dr. James Baeder Alfred Gessow Rotorcraft Center Department of Aerospace Engineering Debojyoti Ghosh Adviser: Dr. James Baeder Alfred Gessow Rotorcraft Center Department of Aerospace Engineering To study the Dynamic Stalling of rotor blade cross-sections Unsteady Aerodynamics: Time varying

More information

Introduction to C omputational F luid Dynamics. D. Murrin

Introduction to C omputational F luid Dynamics. D. Murrin Introduction to C omputational F luid Dynamics D. Murrin Computational fluid dynamics (CFD) is the science of predicting fluid flow, heat transfer, mass transfer, chemical reactions, and related phenomena

More information

Finite Volume Discretization on Irregular Voronoi Grids

Finite Volume Discretization on Irregular Voronoi Grids Finite Volume Discretization on Irregular Voronoi Grids C.Huettig 1, W. Moore 1 1 Hampton University / National Institute of Aerospace Folie 1 The earth and its terrestrial neighbors NASA Colin Rose, Dorling

More information

Final Report. Discontinuous Galerkin Compressible Euler Equation Solver. May 14, Andrey Andreyev. Adviser: Dr. James Baeder

Final Report. Discontinuous Galerkin Compressible Euler Equation Solver. May 14, Andrey Andreyev. Adviser: Dr. James Baeder Final Report Discontinuous Galerkin Compressible Euler Equation Solver May 14, 2013 Andrey Andreyev Adviser: Dr. James Baeder Abstract: In this work a Discontinuous Galerkin Method is developed for compressible

More information

CGT 581 G Fluids. Overview. Some terms. Some terms

CGT 581 G Fluids. Overview. Some terms. Some terms CGT 581 G Fluids Bedřich Beneš, Ph.D. Purdue University Department of Computer Graphics Technology Overview Some terms Incompressible Navier-Stokes Boundary conditions Lagrange vs. Euler Eulerian approaches

More information

Shape optimisation using breakthrough technologies

Shape optimisation using breakthrough technologies Shape optimisation using breakthrough technologies Compiled by Mike Slack Ansys Technical Services 2010 ANSYS, Inc. All rights reserved. 1 ANSYS, Inc. Proprietary Introduction Shape optimisation technologies

More information

Particle-based Fluid Simulation

Particle-based Fluid Simulation Simulation in Computer Graphics Particle-based Fluid Simulation Matthias Teschner Computer Science Department University of Freiburg Application (with Pixar) 10 million fluid + 4 million rigid particles,

More information

MESHLESS SOLUTION OF INCOMPRESSIBLE FLOW OVER BACKWARD-FACING STEP

MESHLESS SOLUTION OF INCOMPRESSIBLE FLOW OVER BACKWARD-FACING STEP Vol. 12, Issue 1/2016, 63-68 DOI: 10.1515/cee-2016-0009 MESHLESS SOLUTION OF INCOMPRESSIBLE FLOW OVER BACKWARD-FACING STEP Juraj MUŽÍK 1,* 1 Department of Geotechnics, Faculty of Civil Engineering, University

More information

Numerical Methods in Aerodynamics. Fluid Structure Interaction. Lecture 4: Fluid Structure Interaction

Numerical Methods in Aerodynamics. Fluid Structure Interaction. Lecture 4: Fluid Structure Interaction Fluid Structure Interaction Niels N. Sørensen Professor MSO, Ph.D. Department of Civil Engineering, Alborg University & Wind Energy Department, Risø National Laboratory Technical University of Denmark

More information

Adarsh Krishnamurthy (cs184-bb) Bela Stepanova (cs184-bs)

Adarsh Krishnamurthy (cs184-bb) Bela Stepanova (cs184-bs) OBJECTIVE FLUID SIMULATIONS Adarsh Krishnamurthy (cs184-bb) Bela Stepanova (cs184-bs) The basic objective of the project is the implementation of the paper Stable Fluids (Jos Stam, SIGGRAPH 99). The final

More information

Driven Cavity Example

Driven Cavity Example BMAppendixI.qxd 11/14/12 6:55 PM Page I-1 I CFD Driven Cavity Example I.1 Problem One of the classic benchmarks in CFD is the driven cavity problem. Consider steady, incompressible, viscous flow in a square

More information

Program: Advanced Certificate Program

Program: Advanced Certificate Program Program: Advanced Certificate Program Course: CFD-Vehicle Aerodynamics Directorate of Training and Lifelong Learning #470-P, Peenya Industrial Area, 4th Phase Peenya, Bengaluru 560 058 www.msruas.ac.in

More information

Application of CFD to Industrial Safety Studies (with Prediction Accuracy and Error estimations)

Application of CFD to Industrial Safety Studies (with Prediction Accuracy and Error estimations) School of Mechanical Aerospace and Civil Engineering University of Manchester First Year Transfer Report Application of CFD to Industrial Safety Studies (with Prediction Accuracy and Error estimations)

More information

A Hybrid Cartesian Grid and Gridless Method for Compressible Flows

A Hybrid Cartesian Grid and Gridless Method for Compressible Flows rd AIAA Aerospace Sciences Meeting and Exhibit,, January 5, Reno, Nevada A Hybrid Cartesian Grid and Gridless Method for Compressible Flows Hong Luo and Joseph D. Baum Science Applications International

More information

An adaptive discretization of incompressible flow using a multitude of moving Cartesian grids

An adaptive discretization of incompressible flow using a multitude of moving Cartesian grids An adaptive discretization of incompressible flow using a multitude of moving Cartesian grids R. Elliot English, Linhai Qiu, Yue Yu, Ronald Fedkiw Stanford University, 353 Serra Mall Room 27, Stanford,

More information

Outline. Level Set Methods. For Inverse Obstacle Problems 4. Introduction. Introduction. Martin Burger

Outline. Level Set Methods. For Inverse Obstacle Problems 4. Introduction. Introduction. Martin Burger For Inverse Obstacle Problems Martin Burger Outline Introduction Optimal Geometries Inverse Obstacle Problems & Shape Optimization Sensitivity Analysis based on Gradient Flows Numerical Methods University

More information

Non-Newtonian Transitional Flow in an Eccentric Annulus

Non-Newtonian Transitional Flow in an Eccentric Annulus Tutorial 8. Non-Newtonian Transitional Flow in an Eccentric Annulus Introduction The purpose of this tutorial is to illustrate the setup and solution of a 3D, turbulent flow of a non-newtonian fluid. Turbulent

More information

A higher-order finite volume method with collocated grid arrangement for incompressible flows

A higher-order finite volume method with collocated grid arrangement for incompressible flows Computational Methods and Experimental Measurements XVII 109 A higher-order finite volume method with collocated grid arrangement for incompressible flows L. Ramirez 1, X. Nogueira 1, S. Khelladi 2, J.

More information

Adaptive numerical methods

Adaptive numerical methods METRO MEtallurgical TRaining On-line Adaptive numerical methods Arkadiusz Nagórka CzUT Education and Culture Introduction Common steps of finite element computations consists of preprocessing - definition

More information

Mid-Year Report. Discontinuous Galerkin Euler Equation Solver. Friday, December 14, Andrey Andreyev. Advisor: Dr.

Mid-Year Report. Discontinuous Galerkin Euler Equation Solver. Friday, December 14, Andrey Andreyev. Advisor: Dr. Mid-Year Report Discontinuous Galerkin Euler Equation Solver Friday, December 14, 2012 Andrey Andreyev Advisor: Dr. James Baeder Abstract: The focus of this effort is to produce a two dimensional inviscid,

More information

Lagrangian methods and Smoothed Particle Hydrodynamics (SPH) Computation in Astrophysics Seminar (Spring 2006) L. J. Dursi

Lagrangian methods and Smoothed Particle Hydrodynamics (SPH) Computation in Astrophysics Seminar (Spring 2006) L. J. Dursi Lagrangian methods and Smoothed Particle Hydrodynamics (SPH) Eulerian Grid Methods The methods covered so far in this course use an Eulerian grid: Prescribed coordinates In `lab frame' Fluid elements flow

More information

Partial Differential Equations

Partial Differential Equations Simulation in Computer Graphics Partial Differential Equations Matthias Teschner Computer Science Department University of Freiburg Motivation various dynamic effects and physical processes are described

More information

Compressible Flow in a Nozzle

Compressible Flow in a Nozzle SPC 407 Supersonic & Hypersonic Fluid Dynamics Ansys Fluent Tutorial 1 Compressible Flow in a Nozzle Ahmed M Nagib Elmekawy, PhD, P.E. Problem Specification Consider air flowing at high-speed through a

More information

Coupled Simulation of Flow and Body Motion Using Overset Grids. Eberhard Schreck & Milovan Perić

Coupled Simulation of Flow and Body Motion Using Overset Grids. Eberhard Schreck & Milovan Perić Coupled Simulation of Flow and Body Motion Using Overset Grids Eberhard Schreck & Milovan Perić Contents Dynamic Fluid-Body Interaction (DFBI) model in STAR-CCM+ Overset grids method in STAR-CCM+ Advantages

More information

A Scalable GPU-Based Compressible Fluid Flow Solver for Unstructured Grids

A Scalable GPU-Based Compressible Fluid Flow Solver for Unstructured Grids A Scalable GPU-Based Compressible Fluid Flow Solver for Unstructured Grids Patrice Castonguay and Antony Jameson Aerospace Computing Lab, Stanford University GTC Asia, Beijing, China December 15 th, 2011

More information

NUMERICAL VISCOSITY. Convergent Science White Paper. COPYRIGHT 2017 CONVERGENT SCIENCE. All rights reserved.

NUMERICAL VISCOSITY. Convergent Science White Paper. COPYRIGHT 2017 CONVERGENT SCIENCE. All rights reserved. Convergent Science White Paper COPYRIGHT 2017 CONVERGENT SCIENCE. All rights reserved. This document contains information that is proprietary to Convergent Science. Public dissemination of this document

More information

Lab 9: FLUENT: Transient Natural Convection Between Concentric Cylinders

Lab 9: FLUENT: Transient Natural Convection Between Concentric Cylinders Lab 9: FLUENT: Transient Natural Convection Between Concentric Cylinders Objective: The objective of this laboratory is to introduce how to use FLUENT to solve both transient and natural convection problems.

More information

Multigrid Solvers in CFD. David Emerson. Scientific Computing Department STFC Daresbury Laboratory Daresbury, Warrington, WA4 4AD, UK

Multigrid Solvers in CFD. David Emerson. Scientific Computing Department STFC Daresbury Laboratory Daresbury, Warrington, WA4 4AD, UK Multigrid Solvers in CFD David Emerson Scientific Computing Department STFC Daresbury Laboratory Daresbury, Warrington, WA4 4AD, UK david.emerson@stfc.ac.uk 1 Outline Multigrid: general comments Incompressible

More information

A High-Order Accurate Unstructured GMRES Solver for Poisson s Equation

A High-Order Accurate Unstructured GMRES Solver for Poisson s Equation A High-Order Accurate Unstructured GMRES Solver for Poisson s Equation Amir Nejat * and Carl Ollivier-Gooch Department of Mechanical Engineering, The University of British Columbia, BC V6T 1Z4, Canada

More information

FLOWVISION CFD FREQUENTLY ASKED QUESTIONS

FLOWVISION CFD FREQUENTLY ASKED QUESTIONS FLOWVISION CFD FREQUENTLY ASKED QUESTIONS 1. Installation and Licensing 1.1. Does FlowVision have floating licenses? 1.1.1. Actually all FlowVision licenses have floating capability and no extra fees are

More information

Modeling Unsteady Compressible Flow

Modeling Unsteady Compressible Flow Tutorial 4. Modeling Unsteady Compressible Flow Introduction In this tutorial, FLUENT s density-based implicit solver is used to predict the timedependent flow through a two-dimensional nozzle. As an initial

More information

SPH: Why and what for?

SPH: Why and what for? SPH: Why and what for? 4 th SPHERIC training day David Le Touzé, Fluid Mechanics Laboratory, Ecole Centrale de Nantes / CNRS SPH What for and why? How it works? Why not for everything? Duality of SPH SPH

More information

Computational Fluid Dynamics - Incompressible Flows

Computational Fluid Dynamics - Incompressible Flows Computational Fluid Dynamics - Incompressible Flows March 25, 2008 Incompressible Flows Basis Functions Discrete Equations CFD - Incompressible Flows CFD is a Huge field Numerical Techniques for solving

More information

FEMLAB Exercise 1 for ChE366

FEMLAB Exercise 1 for ChE366 FEMLAB Exercise 1 for ChE366 Problem statement Consider a spherical particle of radius r s moving with constant velocity U in an infinitely long cylinder of radius R that contains a Newtonian fluid. Let

More information

ENERGY-224 Reservoir Simulation Project Report. Ala Alzayer

ENERGY-224 Reservoir Simulation Project Report. Ala Alzayer ENERGY-224 Reservoir Simulation Project Report Ala Alzayer Autumn Quarter December 3, 2014 Contents 1 Objective 2 2 Governing Equations 2 3 Methodolgy 3 3.1 BlockMesh.........................................

More information

Numerical Methods for PDEs. SSC Workgroup Meetings Juan J. Alonso October 8, SSC Working Group Meetings, JJA 1

Numerical Methods for PDEs. SSC Workgroup Meetings Juan J. Alonso October 8, SSC Working Group Meetings, JJA 1 Numerical Methods for PDEs SSC Workgroup Meetings Juan J. Alonso October 8, 2001 SSC Working Group Meetings, JJA 1 Overview These notes are meant to be an overview of the various memory access patterns

More information

Fluent User Services Center

Fluent User Services Center Solver Settings 5-1 Using the Solver Setting Solver Parameters Convergence Definition Monitoring Stability Accelerating Convergence Accuracy Grid Independence Adaption Appendix: Background Finite Volume

More information

Potsdam Propeller Test Case (PPTC)

Potsdam Propeller Test Case (PPTC) Second International Symposium on Marine Propulsors smp 11, Hamburg, Germany, June 2011 Workshop: Propeller performance Potsdam Propeller Test Case (PPTC) Olof Klerebrant Klasson 1, Tobias Huuva 2 1 Core

More information

High-order mesh generation for CFD solvers

High-order mesh generation for CFD solvers High-order mesh generation for CFD solvers M. Turner, D. Moxey, S. Sherwin, J. Peiró Department of Aeronautics, Imperial College London DiPaRT 2015 Annual Meeting, Bristol, UK 17 th November 2015 Overview

More information

A Toolbox of Level Set Methods

A Toolbox of Level Set Methods A Toolbox of Level Set Methods Ian Mitchell Department of Computer Science University of British Columbia http://www.cs.ubc.ca/~mitchell mitchell@cs.ubc.ca research supported by the Natural Science and

More information

Adjoint Solver Advances, Tailored to Automotive Applications

Adjoint Solver Advances, Tailored to Automotive Applications Adjoint Solver Advances, Tailored to Automotive Applications Stamatina Petropoulou s.petropoulou@iconcfd.com 1 Contents 1. Icon s Principal Work in FlowHead 2. Demonstration Cases 3. Icon s Further Development

More information

Module 1: Introduction to Finite Difference Method and Fundamentals of CFD Lecture 13: The Lecture deals with:

Module 1: Introduction to Finite Difference Method and Fundamentals of CFD Lecture 13: The Lecture deals with: The Lecture deals with: Some more Suggestions for Improvement of Discretization Schemes Some Non-Trivial Problems with Discretized Equations file:///d /chitra/nptel_phase2/mechanical/cfd/lecture13/13_1.htm[6/20/2012

More information

Computational Astrophysics 5 Higher-order and AMR schemes

Computational Astrophysics 5 Higher-order and AMR schemes Computational Astrophysics 5 Higher-order and AMR schemes Oscar Agertz Outline - The Godunov Method - Second-order scheme with MUSCL - Slope limiters and TVD schemes - Characteristics tracing and 2D slopes.

More information

Unstructured Mesh Related Issues In Computational Fluid Dynamics (CFD) Based Analysis And Design

Unstructured Mesh Related Issues In Computational Fluid Dynamics (CFD) Based Analysis And Design Unstructured Mesh Related Issues In Computational Fluid Dynamics (CFD) Based Analysis And Design Dimitri J. Mavriplis ICASE NASA Langley Research Center Hampton, VA 23681 USA 11 th International Meshing

More information

Numerical Analysis of Shock Tube Problem by using TVD and ACM Schemes

Numerical Analysis of Shock Tube Problem by using TVD and ACM Schemes Numerical Analysis of Shock Tube Problem by using TVD and Schemes Dr. Mukkarum Husain, Dr. M. Nauman Qureshi, Syed Zaid Hasany IST Karachi, Email: mrmukkarum@yahoo.com Abstract Computational Fluid Dynamics

More information

CFD MODELING FOR PNEUMATIC CONVEYING

CFD MODELING FOR PNEUMATIC CONVEYING CFD MODELING FOR PNEUMATIC CONVEYING Arvind Kumar 1, D.R. Kaushal 2, Navneet Kumar 3 1 Associate Professor YMCAUST, Faridabad 2 Associate Professor, IIT, Delhi 3 Research Scholar IIT, Delhi e-mail: arvindeem@yahoo.co.in

More information

CFD Best Practice Guidelines: A process to understand CFD results and establish Simulation versus Reality

CFD Best Practice Guidelines: A process to understand CFD results and establish Simulation versus Reality CFD Best Practice Guidelines: A process to understand CFD results and establish Simulation versus Reality Judd Kaiser ANSYS Inc. judd.kaiser@ansys.com 2005 ANSYS, Inc. 1 ANSYS, Inc. Proprietary Overview

More information

High-Order Numerical Algorithms for Steady and Unsteady Simulation of Viscous Compressible Flow with Shocks (Grant FA )

High-Order Numerical Algorithms for Steady and Unsteady Simulation of Viscous Compressible Flow with Shocks (Grant FA ) High-Order Numerical Algorithms for Steady and Unsteady Simulation of Viscous Compressible Flow with Shocks (Grant FA9550-07-0195) Sachin Premasuthan, Kui Ou, Patrice Castonguay, Lala Li, Yves Allaneau,

More information

Investigation of cross flow over a circular cylinder at low Re using the Immersed Boundary Method (IBM)

Investigation of cross flow over a circular cylinder at low Re using the Immersed Boundary Method (IBM) Computational Methods and Experimental Measurements XVII 235 Investigation of cross flow over a circular cylinder at low Re using the Immersed Boundary Method (IBM) K. Rehman Department of Mechanical Engineering,

More information

Navier-Stokes & Flow Simulation

Navier-Stokes & Flow Simulation Last Time? Navier-Stokes & Flow Simulation Implicit Surfaces Marching Cubes/Tetras Collision Detection & Response Conservative Bounding Regions backtracking fixing Today Flow Simulations in Graphics Flow

More information

Auto Injector Syringe. A Fluent Dynamic Mesh 1DOF Tutorial

Auto Injector Syringe. A Fluent Dynamic Mesh 1DOF Tutorial Auto Injector Syringe A Fluent Dynamic Mesh 1DOF Tutorial 1 2015 ANSYS, Inc. June 26, 2015 Prerequisites This tutorial is written with the assumption that You have attended the Introduction to ANSYS Fluent

More information

GEOMETRIC TOOLS FOR COMPUTER GRAPHICS

GEOMETRIC TOOLS FOR COMPUTER GRAPHICS GEOMETRIC TOOLS FOR COMPUTER GRAPHICS PHILIP J. SCHNEIDER DAVID H. EBERLY MORGAN KAUFMANN PUBLISHERS A N I M P R I N T O F E L S E V I E R S C I E N C E A M S T E R D A M B O S T O N L O N D O N N E W

More information

Unstructured Grid Numbering Schemes for GPU Coalescing Requirements

Unstructured Grid Numbering Schemes for GPU Coalescing Requirements Unstructured Grid Numbering Schemes for GPU Coalescing Requirements Andrew Corrigan 1 and Johann Dahm 2 Laboratories for Computational Physics and Fluid Dynamics Naval Research Laboratory 1 Department

More information

Fast marching methods

Fast marching methods 1 Fast marching methods Lecture 3 Alexander & Michael Bronstein tosca.cs.technion.ac.il/book Numerical geometry of non-rigid shapes Stanford University, Winter 2009 Metric discretization 2 Approach I:

More information

The Level Set Method. Lecture Notes, MIT J / 2.097J / 6.339J Numerical Methods for Partial Differential Equations

The Level Set Method. Lecture Notes, MIT J / 2.097J / 6.339J Numerical Methods for Partial Differential Equations The Level Set Method Lecture Notes, MIT 16.920J / 2.097J / 6.339J Numerical Methods for Partial Differential Equations Per-Olof Persson persson@mit.edu March 7, 2005 1 Evolving Curves and Surfaces Evolving

More information

Adaptive Mesh Refinement Based on a Posteriori Error Estimation. Martin Juhas

Adaptive Mesh Refinement Based on a Posteriori Error Estimation. Martin Juhas Adaptive Mesh Refinement Based on a Posteriori Error Estimation by Martin Juhas A thesis submitted in conformity with the requirements for the degree of Master of Applied Science Graduate Department of

More information

Modeling Indoor Air Pollution

Modeling Indoor Air Pollution Modeling Indoor Air Pollution This page intentionally left blank Modeling Indoor Air Pollution Darrell W Pepper University of Nevada, Las Vegas, USA David Carrington Los Alamos National Laboratory, USA

More information

Second International Workshop on Scientific Computing and Applications. Kananaskis, Canada, May 28 - June 1, 2000

Second International Workshop on Scientific Computing and Applications. Kananaskis, Canada, May 28 - June 1, 2000 Second International Workshop on Scientific Computing and Applications. Kananaskis, Canada, May 28 - June 1, 2000 Program May 28 (Sunday) 19:00-21:00 Registration and reception Session Chairman: Y. Wong

More information

Parallel High-Order Geometric Multigrid Methods on Adaptive Meshes for Highly Heterogeneous Nonlinear Stokes Flow Simulations of Earth s Mantle

Parallel High-Order Geometric Multigrid Methods on Adaptive Meshes for Highly Heterogeneous Nonlinear Stokes Flow Simulations of Earth s Mantle ICES Student Forum The University of Texas at Austin, USA November 4, 204 Parallel High-Order Geometric Multigrid Methods on Adaptive Meshes for Highly Heterogeneous Nonlinear Stokes Flow Simulations of

More information

Realistic Animation of Fluids

Realistic Animation of Fluids 1 Realistic Animation of Fluids Nick Foster and Dimitris Metaxas Presented by Alex Liberman April 19, 2005 2 Previous Work Used non physics-based methods (mostly in 2D) Hard to simulate effects that rely

More information

An adaptive discretization of incompressible flow using a multitude of moving Cartesian grids

An adaptive discretization of incompressible flow using a multitude of moving Cartesian grids An adaptive discretization of incompressible flow using a multitude of moving Cartesian grids R. Elliot English, Linhai Qiu,YueYu, Ronald Fedkiw Stanford University, 353 Serra Mall Room 27, Stanford, CA

More information

Using a Single Rotating Reference Frame

Using a Single Rotating Reference Frame Tutorial 9. Using a Single Rotating Reference Frame Introduction This tutorial considers the flow within a 2D, axisymmetric, co-rotating disk cavity system. Understanding the behavior of such flows is

More information

This is an author-deposited version published in: Eprints ID: 4362

This is an author-deposited version published in:   Eprints ID: 4362 This is an author-deposited version published in: http://oatao.univ-toulouse.fr/ Eprints ID: 4362 To cite this document: CHIKHAOUI Oussama, GRESSIER Jérémie, GRONDIN Gilles. Assessment of the Spectral

More information

1 Exercise: Heat equation in 2-D with FE

1 Exercise: Heat equation in 2-D with FE 1 Exercise: Heat equation in 2-D with FE Reading Hughes (2000, sec. 2.3-2.6 Dabrowski et al. (2008, sec. 1-3, 4.1.1, 4.1.3, 4.2.1 This FE exercise and most of the following ones are based on the MILAMIN

More information

Pressure Correction Scheme for Incompressible Fluid Flow

Pressure Correction Scheme for Incompressible Fluid Flow AALTO UNIVERSITY School of Chemical Technology CHEM-E7160 Fluid Flow in Process Units Pressure Correction Scheme for Incompressible Fluid Flow Ong Chin Kai 620503 Lee De Ming Benedict 620448 Page 1 Abstract

More information

Navier-Stokes & Flow Simulation

Navier-Stokes & Flow Simulation Last Time? Navier-Stokes & Flow Simulation Pop Worksheet! Teams of 2. Hand in to Jeramey after we discuss. Sketch the first few frames of a 2D explicit Euler mass-spring simulation for a 2x3 cloth network

More information

Introduction to ANSYS CFX

Introduction to ANSYS CFX Workshop 03 Fluid flow around the NACA0012 Airfoil 16.0 Release Introduction to ANSYS CFX 2015 ANSYS, Inc. March 13, 2015 1 Release 16.0 Workshop Description: The flow simulated is an external aerodynamics

More information

Metafor FE Software. 2. Operator split. 4. Rezoning methods 5. Contact with friction

Metafor FE Software. 2. Operator split. 4. Rezoning methods 5. Contact with friction ALE simulations ua sus using Metafor eao 1. Introduction 2. Operator split 3. Convection schemes 4. Rezoning methods 5. Contact with friction 1 Introduction EULERIAN FORMALISM Undistorted mesh Ideal for

More information

The 3D DSC in Fluid Simulation

The 3D DSC in Fluid Simulation The 3D DSC in Fluid Simulation Marek K. Misztal Informatics and Mathematical Modelling, Technical University of Denmark mkm@imm.dtu.dk DSC 2011 Workshop Kgs. Lyngby, 26th August 2011 Governing Equations

More information

Recent applications of overset mesh technology in SC/Tetra

Recent applications of overset mesh technology in SC/Tetra Recent applications of overset mesh technology in SC/Tetra NIA CFD Seminar October 6, 2014 Tomohiro Irie Software Cradle Co., Ltd. 1 Contents Introduction Software Cradle SC/Tetra Background of Demands

More information

Application of Finite Volume Method for Structural Analysis

Application of Finite Volume Method for Structural Analysis Application of Finite Volume Method for Structural Analysis Saeed-Reza Sabbagh-Yazdi and Milad Bayatlou Associate Professor, Civil Engineering Department of KNToosi University of Technology, PostGraduate

More information

Flow in an Intake Manifold

Flow in an Intake Manifold Tutorial 2. Flow in an Intake Manifold Introduction The purpose of this tutorial is to model turbulent flow in a simple intake manifold geometry. An intake manifold is a system of passages which carry

More information

2.7 Cloth Animation. Jacobs University Visualization and Computer Graphics Lab : Advanced Graphics - Chapter 2 123

2.7 Cloth Animation. Jacobs University Visualization and Computer Graphics Lab : Advanced Graphics - Chapter 2 123 2.7 Cloth Animation 320491: Advanced Graphics - Chapter 2 123 Example: Cloth draping Image Michael Kass 320491: Advanced Graphics - Chapter 2 124 Cloth using mass-spring model Network of masses and springs

More information

FAST ALGORITHMS FOR CALCULATIONS OF VISCOUS INCOMPRESSIBLE FLOWS USING THE ARTIFICIAL COMPRESSIBILITY METHOD

FAST ALGORITHMS FOR CALCULATIONS OF VISCOUS INCOMPRESSIBLE FLOWS USING THE ARTIFICIAL COMPRESSIBILITY METHOD TASK QUARTERLY 12 No 3, 273 287 FAST ALGORITHMS FOR CALCULATIONS OF VISCOUS INCOMPRESSIBLE FLOWS USING THE ARTIFICIAL COMPRESSIBILITY METHOD ZBIGNIEW KOSMA Institute of Applied Mechanics, Technical University

More information

Numerical Methods for (Time-Dependent) HJ PDEs

Numerical Methods for (Time-Dependent) HJ PDEs Numerical Methods for (Time-Dependent) HJ PDEs Ian Mitchell Department of Computer Science The University of British Columbia research supported by National Science and Engineering Research Council of

More information

Supersonic Flow Over a Wedge

Supersonic Flow Over a Wedge SPC 407 Supersonic & Hypersonic Fluid Dynamics Ansys Fluent Tutorial 2 Supersonic Flow Over a Wedge Ahmed M Nagib Elmekawy, PhD, P.E. Problem Specification A uniform supersonic stream encounters a wedge

More information

Digital Geometry Processing Parameterization I

Digital Geometry Processing Parameterization I Problem Definition Given a surface (mesh) S in R 3 and a domain find a bective F: S Typical Domains Cutting to a Disk disk = genus zero + boundary sphere = closed genus zero Creates artificial boundary

More information

EVALUATION OF A GENERAL CFD-SOLVER FOR A MICRO-SCALE URBAN FLOW

EVALUATION OF A GENERAL CFD-SOLVER FOR A MICRO-SCALE URBAN FLOW EVALATION OF A GENERAL CFD-SOLVER FOR A MICRO-SCALE RBAN FLOW Jarkko Saloranta and Antti Hellsten Helsinki niversity of Technology, Laboratory of Aerodynamics, Finland INTRODCTION In this work we study

More information

SIMULATION OF PROPELLER-SHIP HULL INTERACTION USING AN INTEGRATED VLM/RANSE SOLVER MODELING.

SIMULATION OF PROPELLER-SHIP HULL INTERACTION USING AN INTEGRATED VLM/RANSE SOLVER MODELING. SIMULATION OF PROPELLER-SHIP HULL INTERACTION USING AN INTEGRATED VLM/RANSE SOLVER MODELING. M.N.Senthil Prakash, Department of Ocean Engineering, IIT Madras, India V. Anantha Subramanian Department of

More information

Navier-Stokes & Flow Simulation

Navier-Stokes & Flow Simulation Last Time? Navier-Stokes & Flow Simulation Optional Reading for Last Time: Spring-Mass Systems Numerical Integration (Euler, Midpoint, Runge-Kutta) Modeling string, hair, & cloth HW2: Cloth & Fluid Simulation

More information