Performance and Quality Analysis of Interpolation Methods for Coupling
|
|
- Corey Wilson
- 6 years ago
- Views:
Transcription
1 Performance and Quality Analysis of Interpolation Methods for Coupling Neda Ebrahimi Pour, Sabine Roller
2 Outline Motivation Coupling Approaches Interpolation/Evaluation Results of Investigation Summary 11/10/17 2
3 Motivation More and more complex devices à Better understanding of the physical phenomena à Improvements in product design in the engineering field Important: Applications involve multi-physics and multi-scales 11/10/17 3
4 Strategy Simulating whole problem with one solver à too expensive Partitioned coupling à splitting whole domain in subdomains - according physical phenomenon à Solving each domain according to its requirements - equations, element size etc. 11/10/17 4
5 Partitioned Coupling APES Navier-Stokes equations FV 2 nd order Euler equations DG 4-8 th order Linearized Euler equations DG 8-64 th order Coupling different domains with different numerical methods (Finite Volume, Discontinuous Galerkin) e.g. FSA-Interaction Coupled simulation with spatial discretization 11/10/17 5
6 Coupling Types Matching Non-matching à Data mapping from one side to the other Op2on 1: Interpola2on (scheme independent) Op2on 2: Evalua2on of polynomial (scheme dependent, e.g. DG) à Matching coupling à Non-matching coupling - same grid size - different grid size - same scheme order - different scheme order à same number of coupling points à different number of coupling points 11/10/17 6
7 Two coupling approaches 1) precice An external library Treats solver as a black-box Different coupling strategies Parallel/ serial explicit, Implicit quasi newton methods Different data-mapping methods Nearest-Neighbor, Nearest-Projection, Radial-Basis-Function B. Gatzhammer, B. Uekermann (München), F. Lindner, M. Mehl (Stuttgart) 11/10/17 7
8 Interpolation Methods 1a) Nearest-Neighbour 1b) Nearest-Projection A A B B + nearest No computation neighbour ma + 2 nd order accuracy - 1 st order accuracy - provide neighborhood - not suitable for non-matching information coupling 11/10/17 8
9 1c) Radial-Basis-Function s(x) = NX i=1 i '(kx x i k)+q(x) φ : basis func2on x i : point, which has to be evaluated q(x) : global linear func2on s(x) : interpolant + No neighborhood information needed + Different basis-functions available - Linear equation system has to be solved - Condition number depends on point distribution (equidistant/non-equidistant) e.g. basis function: Gaussian function p ln(10 9 ) shape-parameter: a = m h m : average number of points to cover h: average distance between points 11/10/17 9
10 Two coupling approaches 2) APESmate Integrated approach in APES Evaluation of polynomial Data-mapping according to scheme order Accuracy depends on scheme order Aotus Configuration with Lua Shepherd Deployment Scripts Seeder Mesh Generation APES Adaptable Poly-Engineering Simulator TreElM Octree Mesh Infrastructure Ateles Discontinuous Galerkin Muriqui Space-Time DG APESmate Coupling of APES solvers Musubi Lattice Boltzmann K. Masilamani, V. Krupp, H. Klimach, S. Roller (Siegen) Harvester Post-Processing Analysis 11/10/17 10
11 Results: Testcase 11/10/17 11
12 Results: Convergence Study O(2) O(4) O(8) O(12) O(14) 10 1 O(3) O(6) O(10) O(16) O(32) Monolithic simula2on - Varia2on of the element size and scheme order 10 2 L2error Calcula2on of the L2error from simula2on and analy2cal solu2on Elementsize Chosen element size / L2error for coupling two domains 11/10/17 12
13 Testcases: Testcase 1 Inner: Outer: Testcase 2 Inner: Outer: Testcase 3 Inner: Outer: Testcase 4 Inner: Outer: Scheme Order Number of Points O(3) O(4) O(3) O(6) O(3) O(8) O(3) O(14) Number of Elements /10/17 13
14 Testcase: Gaussian Pressure Pulse 11/10/17 14
15 Testcase: Gaussian Pressure Pulse Domain: 5 x 5 x 5 Halfwidth: 0.25 Inner domain: 1 x 1 x 1 Amplitude: /10/17 15
16 Results: Interpolation/Evaluation method NP RBF AP ESmate L2error Highest error with NP Can we reduce the L2error by choosing a different Increasing error with point distribu2on? RBF Constant error with APESmate Scheme Order 11/10/17 16
17 Results: Equidistant Points for Radial-Basis- Function Providing equidistant points for the interpola2on 11/10/17 17
18 Results: Radial-Basis-Function RBF RBF RBF EQ EQ Computational L2error T ime [s] Scheme Order Increasing error for RBF with non-equidistant points Decreasing error with equidistant point distribu2on Increasing computa2onal cost for RBF with equidistant pointd 11/10/17 18
19 Results: Oversampling for Nearest-Projection Oversampling factor of 2 11/10/17 19
20 Results: Nearest-Projection NP NP factor=2 NP EQ NP EQfactor= Increasing error, when using oversampling for non-equidistant points L2error Decreasing error with increasing oversampling factor for equidistant points Scheme Order 11/10/17 20
21 Results: L2error for all methods NP NP EQfactor=3 RBF EQ RBF AP ESmate Highest error with NP and non-equidistant points L2error Error APESmate and NP almost constant over scheme order RBF with equidistant points à decreasing error Scheme Order 11/10/17 21
22 Results: Computational cost 10 3 NP RBF NP EQfactor=3 RBF EQ AP ESmate RBF with equidistant points à highest cost Computational T ime [s] 10 2 NP with non-equidistant points à lows cost APESmate à increasing cost with increasing scheme order Scheme Order 11/10/17 22
23 Results: Performance (Weak Scaling) Nearest-Projec2on Radial-Basis-Func2on APESmate Testcase 1 Testcase 2 Testcase 3 Testcase 4 Testcase 1 Testcase 2 Testcase 3 Testcase 4 Testcase 1 Testcase 2 Testcase 3 Testcase Computational Time Computational Time 10 3 Computational Time np rocs np rocs np rocs 11/10/17 23
24 Results: Performance (Weak Scaling) NP RBF AP ESmate 10 4 Computational T ime np rocs 11/10/17 24
25 Summary Coupling Tool precice Method Error Computa2onal cost RBF non-equidistant Increase with scheme order points Increasing with Decrease when using scheme order When RBF equidistant coupling different points solvers equidistant à precice points with Nearest- Projec2on interpola2on NP non-equidistant Increase when using Increasing with When points using our solvers à oversampling APESmate provides factor very good scheme results order NP equidistant points Decrease with oversampling factor Increasing with scheme order and oversampling factor APESmate Evalua2on of the polynomial Scheme dependent Increasing with scheme order 11/10/17 25
26 Thank you for your attention 11/10/17 26
Locally Linearized Euler Equations in Discontinuous Galerkin with Legendre Polynomials
Locally Linearized Euler Equations in Discontinuous Galerkin with Legendre Polynomials Harald Klimach, Michael Gaida, Sabine Roller harald.klimach@uni-siegen.de 26th WSSP 2017 Motivation Fluid-Dynamic
More informationTIME STEPPING ALGORITHMS FOR PARTITIONED MULTI-SCALE MULTI-PHYSICS IN PRECICE
6th European Conference on Computational Mechanics (ECCM 6 7th European Conference on Computational Fluid Dynamics (ECFD 7 1115 June 2018, Glasgow, UK TIME STEPPING ALGORITHMS FOR PARTITIONED MULTI-SCALE
More informationRadial Basis Functions generated Finite Differences (RBF-FD) for Solving High-Dimensional PDEs in Finance
1 / 27 Radial Basis Functions generated Finite Differences (RBF-FD) for Solving High-Dimensional PDEs in Finance S. Milovanović, L. von Sydow Uppsala University Department of Information Technology Division
More informationChapter 6. Finite Element Method. Literature: (tiny selection from an enormous number of publications)
Chapter 6 Finite Element Method Literature: (tiny selection from an enormous number of publications) K.J. Bathe, Finite Element procedures, 2nd edition, Pearson 2014 (1043 pages, comprehensive). Available
More informationPseudospectral Methods For Op2mal Control. Jus2n Ruths March 27, 2009
Pseudospectral Methods For Op2mal Control Jus2n Ruths March 27, 2009 Introduc2on Pseudospectral methods arose to find solu2ons to Par2al Differen2al Equa2ons Recently adapted for Op2mal Control Key Ideas
More informationComputational Science and Engineering (Int. Master s Program) Conjugate Heat Transfer with the Multiphysics Coupling Library precice
Computational Science and Engineering (Int. Master s Program) Technische Universität München Master s Thesis Conjugate Heat Transfer with the Multiphysics Coupling Library precice Author: Lucía Cheung
More informationAn Efficient Low Memory Implicit DG Algorithm for Time Dependent Problems
An Efficient Low Memory Implicit DG Algorithm for Time Dependent Problems P.-O. Persson and J. Peraire Massachusetts Institute of Technology 2006 AIAA Aerospace Sciences Meeting, Reno, Nevada January 9,
More informationA note on accurate and efficient higher order Galerkin time stepping schemes for the nonstationary Stokes equations
A note on accurate and efficient higher order Galerkin time stepping schemes for the nonstationary Stokes equations S. Hussain, F. Schieweck, S. Turek Abstract In this note, we extend our recent work for
More informationSKA machine learning perspec1ves for imaging, processing and analysis
1 SKA machine learning perspec1ves for imaging, processing and analysis Slava Voloshynovskiy Stochas1c Informa1on Processing Group University of Geneva Switzerland with contribu,on of: D. Kostadinov, S.
More informationMeasurement of the meridional flow from eigenfunc5on perturba5ons
Measurement of the meridional flow from eigenfunc5on perturba5ons Ariane Schad, Markus Roth Kiepenheuer- Ins5tut für Sonnenphysik Solar Subsurface Flows from Helioseismology: Problems and Prospects Helioseismology
More informationNavier Stokes Solvers. Length (Log meters) Particle Methods. Density (Log n/n 0. Knudsen number =1/10 2. Dense Gas
Mesh and Algorithm Reænement Alejandro L. Garcia Center for Comp. Sciences and Engineering Lawrence Berkeley National Laboratory and Dept. Physics, San Jose State University Collaborators: Berni Alder
More informationFounda'ons of Large- Scale Mul'media Informa'on Management and Retrieval. Lecture #4 Similarity. Edward Chang
Founda'ons of Large- Scale Mul'media Informa'on Management and Retrieval Lecture #4 Similarity Edward Y. Chang Edward Chang Foundations of LSMM 1 Edward Chang Foundations of LSMM 2 Similar? Edward Chang
More informationImplicit Solution of Viscous Aerodynamic Flows using the Discontinuous Galerkin Method
Implicit Solution of Viscous Aerodynamic Flows using the Discontinuous Galerkin Method Per-Olof Persson and Jaime Peraire Massachusetts Institute of Technology 7th World Congress on Computational Mechanics
More informationFaster Kinetics: Accelerate Your Finite-Rate Combustion Simulation with GPUs
Faster Kinetics: Accelerate Your Finite-Rate Combustion Simulation with GPUs Christopher P. Stone, Ph.D. Computational Science and Engineering, LLC Kyle Niemeyer, Ph.D. Oregon State University 2 Outline
More informationCFD Based Optimization of a Vertical Axis Wind Turbine
SCHOOL OF ENGINEERING INSTITUTE FOR ENERGY SYSTEMS CFD Based Optimization of a Vertical Axis Wind Turbine Emmanouil Falagkaris Supervisory Team Prof. David Ingram, Dr Ignazio Maria Viola, Dr Daniel Friedrich
More informationUnsupervised Learning: K- Means & PCA
Unsupervised Learning: K- Means & PCA Unsupervised Learning Supervised learning used labeled data pairs (x, y) to learn a func>on f : X Y But, what if we don t have labels? No labels = unsupervised learning
More informationNumerical Programming I (for CSE)
Technische Universität München WT 1/13 Fakultät für Mathematik Prof. Dr. M. Mehl B. Gatzhammer January 1, 13 Numerical Programming I (for CSE) Tutorial 1: Iterative Methods 1) Relaxation Methods a) Let
More informationPartititioned Methods for Multifield Problems
Partititioned Methods for Multifield Problems Joachim Rang, 22.7.215 22.7.215 Joachim Rang Partititioned Methods for Multifield Problems Seite 1 Non-matching matches usually the fluid and the structure
More informationOn the efficiency of the Peaceman-Rachford ADI-dG method for wave-type methods
On the efficiency of the Peaceman-Rachford ADI-dG method for wave-type methods Marlis Hochbruck, Jonas Köhler CRC Preprint 2017/34 (revised), March 2018 KARLSRUHE INSTITUTE OF TECHNOLOGY KIT The Research
More informationZFS - Flow Solver AIA NVIDIA Workshop
ZFS - Flow Solver AIA NVIDIA Workshop Andreas Lintermann, Matthias Meinke, Wolfgang Schröder Institute of Aerodynamics and Chair of Fluid Mechanics RWTH Aachen University Outline Softwareproject ZFS (applications
More informationThe Lattice Boltzmann method for hyperbolic systems. Benjamin Graille. October 19, 2016
The Lattice Boltzmann method for hyperbolic systems Benjamin Graille October 19, 2016 Framework The Lattice Boltzmann method 1 Description of the lattice Boltzmann method Link with the kinetic theory Classical
More information(0, 0), (1, ), (2, ), (3, ), (4, ), (5, ), (6, ).
1 Interpolation: The method of constructing new data points within the range of a finite set of known data points That is if (x i, y i ), i = 1, N are known, with y i the dependent variable and x i [x
More informationDiscontinuous Galerkin Methods
Discontinuous Galerkin Methods Joachim Schöberl May 20, 206 Discontinuous Galerkin (DG) methods approximate the solution with piecewise functions (polynomials), which are discontinuous across element interfaces.
More informationA STUDY OF MULTIGRID SMOOTHERS USED IN COMPRESSIBLE CFD BASED ON THE CONVECTION DIFFUSION EQUATION
ECCOMAS Congress 2016 VII European Congress on Computational Methods in Applied Sciences and Engineering M. Papadrakakis, V. Papadopoulos, G. Stefanou, V. Plevris (eds.) Crete Island, Greece, 5 10 June
More informationDeriva'on of The Kalman Filter. Fred DePiero CalPoly State University EE 525 Stochas'c Processes
Deriva'on of The Kalman Filter Fred DePiero CalPoly State University EE 525 Stochas'c Processes KF Uses State Predic'ons KF es'mates the state of a system Example Measure: posi'on State: [ posi'on velocity
More informationThe hybridized DG methods for WS1, WS2, and CS2 test cases
The hybridized DG methods for WS1, WS2, and CS2 test cases P. Fernandez, N.C. Nguyen and J. Peraire Aerospace Computational Design Laboratory Department of Aeronautics and Astronautics, MIT 5th High-Order
More informationGuangye Chen, Luis Chacón,
JIFT workshop! Oct. 31, 2014 New Orleans, LA.! Guangye Chen, Luis Chacón, CoCoMANs team Los Alamos National Laboratory, Los Alamos, NM 87545, USA gchen@lanl.gov 1 Los Alamos National Laboratory Motivation
More informationChapter 2 Interpolation
Chapter 2 Interpolation Experiments usually produce a discrete set of data points (x i, f i ) which represent the value of a function f (x) for a finite set of arguments {x 0...x n }. If additional data
More informationA method to reduce load imbalances in simulations of phase change processes with FS3D
A method to reduce load imbalances in simulations of phase change processes with FS3D Johannes Müller Philipp Offenhäuser Martin Reitzle Workshop on Sustained Simulation Performance HLRS, Stuttgart, Germany
More informationAnalysis and modelling of the effective reaction rate in a developing mixing layer using OpenFOAM R libraries
Analysis and modelling of the effective reaction rate in a developing mixing layer using OpenFOAM R libraries Karol Wedolowski 1,2, Konrad Bajer 1,2, Kamil Kwiatkowski 1,2 1 Faculty of Physics, University
More informationNumerical analysis of heat conduction problems on 3D general-shaped domains by means of a RBF Collocation Meshless Method
Journal of Physics: Conference Series PAPER OPEN ACCESS Numerical analysis of heat conduction problems on 3D general-shaped domains by means of a RBF Collocation Meshless Method To cite this article: R
More informationHp-Adaptivity on Anisotropic Meshes for Hybridized Discontinuous Galerkin Scheme
Hp-Adaptivity on Anisotropic Meshes for Hybridized Discontinuous Galerkin Scheme Aravind Balan, Michael Woopen and Georg May AICES Graduate School, RWTH Aachen University, Germany 22nd AIAA Computational
More informationCOMP 562: Introduction to Machine Learning
COMP 562: Introduction to Machine Learning Lecture 20 : Support Vector Machines, Kernels Mahmoud Mostapha 1 Department of Computer Science University of North Carolina at Chapel Hill mahmoudm@cs.unc.edu
More informationShock Capturing for Discontinuous Galerkin Methods using Finite Volume Sub-cells
Abstract We present a shock capturing procedure for high order Discontinuous Galerkin methods, by which shock regions are refined in sub-cells and treated by finite volume techniques Hence, our approach
More informationTheory, Solution Techniques and Applications of Singular Boundary Value Problems
Theory, Solution Techniques and Applications of Singular Boundary Value Problems W. Auzinger O. Koch E. Weinmüller Vienna University of Technology, Austria Problem Class z (t) = M(t) z(t) + f(t, z(t)),
More informationOUTLINE ffl CFD: elliptic pde's! Ax = b ffl Basic iterative methods ffl Krylov subspace methods ffl Preconditioning techniques: Iterative methods ILU
Preconditioning Techniques for Solving Large Sparse Linear Systems Arnold Reusken Institut für Geometrie und Praktische Mathematik RWTH-Aachen OUTLINE ffl CFD: elliptic pde's! Ax = b ffl Basic iterative
More informationNational Taiwan University
National Taiwan University Meshless Methods for Scientific Computing (Advisor: C.S. Chen, D.L. oung) Final Project Department: Mechanical Engineering Student: Kai-Nung Cheng SID: D9956 Date: Jan. 8 The
More informationMultigrid Methods and their application in CFD
Multigrid Methods and their application in CFD Michael Wurst TU München 16.06.2009 1 Multigrid Methods Definition Multigrid (MG) methods in numerical analysis are a group of algorithms for solving differential
More informationComputational Fluid Dynamics-1(CFDI)
بسمه تعالی درس دینامیک سیالات محاسباتی 1 دوره کارشناسی ارشد دانشکده مهندسی مکانیک دانشگاه صنعتی خواجه نصیر الدین طوسی Computational Fluid Dynamics-1(CFDI) Course outlines: Part I A brief introduction to
More informationOn the choice of abstract projection vectors for second level preconditioners
On the choice of abstract projection vectors for second level preconditioners C. Vuik 1, J.M. Tang 1, and R. Nabben 2 1 Delft University of Technology 2 Technische Universität Berlin Institut für Mathematik
More informationA Central Compact-Reconstruction WENO Method for Hyperbolic Conservation Laws
A Central Compact-Reconstruction WENO Method for Hyperbolic Conservation Laws Kilian Cooley 1 Prof. James Baeder 2 1 Department of Mathematics, University of Maryland - College Park 2 Department of Aerospace
More informationTermination criteria for inexact fixed point methods
Termination criteria for inexact fixed point methods Philipp Birken 1 October 1, 2013 1 Institute of Mathematics, University of Kassel, Heinrich-Plett-Str. 40, D-34132 Kassel, Germany Department of Mathematics/Computer
More informationBreaking Computational Barriers: Multi-GPU High-Order RBF Kernel Problems with Millions of Points
Breaking Computational Barriers: Multi-GPU High-Order RBF Kernel Problems with Millions of Points Michael Griebel Christian Rieger Peter Zaspel Institute for Numerical Simulation Rheinische Friedrich-Wilhelms-Universität
More informationCSE446: Linear Regression Regulariza5on Bias / Variance Tradeoff Winter 2015
CSE446: Linear Regression Regulariza5on Bias / Variance Tradeoff Winter 2015 Luke ZeElemoyer Slides adapted from Carlos Guestrin Predic5on of con5nuous variables Billionaire says: Wait, that s not what
More informationFinite Element Solver for Flux-Source Equations
Finite Element Solver for Flux-Source Equations Weston B. Lowrie A thesis submitted in partial fulfillment of the requirements for the degree of Master of Science in Aeronautics Astronautics University
More informationFEM techniques for nonlinear fluids
FEM techniques for nonlinear fluids From non-isothermal, pressure and shear dependent viscosity models to viscoelastic flow A. Ouazzi, H. Damanik, S. Turek Institute of Applied Mathematics, LS III, TU
More informationAircra& Damping Deriva/ve Es/ma/on Using STAR CCM+
Aircra& Damping Deriva/ve Es/ma/on Using STAR CCM+ Angelo Lerro, Ph.D. Student at Politecnico di Torino Michele Visone, CFD Manager at Blue Engineering Italy Noordwijk, 22/03/2011 Summary Introduc/on Maneuvers
More informationPROJECTION METHODS FOR DYNAMIC MODELS
PROJECTION METHODS FOR DYNAMIC MODELS Kenneth L. Judd Hoover Institution and NBER June 28, 2006 Functional Problems Many problems involve solving for some unknown function Dynamic programming Consumption
More informationMachine Learning. Kernels. Fall (Kernels, Kernelized Perceptron and SVM) Professor Liang Huang. (Chap. 12 of CIML)
Machine Learning Fall 2017 Kernels (Kernels, Kernelized Perceptron and SVM) Professor Liang Huang (Chap. 12 of CIML) Nonlinear Features x4: -1 x1: +1 x3: +1 x2: -1 Concatenated (combined) features XOR:
More informationReal-Space Renormalisation
Real-Space Renormalisation LMU München June 23, 2009 Real-Space Renormalisation of the One-Dimensional Ising Model Ernst Ising Real-Space Renormalisation of the One-Dimensional Ising Model Ernst Ising
More informationNonlinear Iterative Solution of the Neutron Transport Equation
Nonlinear Iterative Solution of the Neutron Transport Equation Emiliano Masiello Commissariat à l Energie Atomique de Saclay /DANS//SERMA/LTSD emiliano.masiello@cea.fr 1/37 Outline - motivations and framework
More informationModeling radiocarbon in the Earth System. Radiocarbon summer school 2012
Modeling radiocarbon in the Earth System Radiocarbon summer school 2012 Outline Brief introduc9on to mathema9cal modeling Single pool models Mul9ple pool models Model implementa9on Parameter es9ma9on What
More informationCS 6140: Machine Learning Spring What We Learned Last Week 2/26/16
Logis@cs CS 6140: Machine Learning Spring 2016 Instructor: Lu Wang College of Computer and Informa@on Science Northeastern University Webpage: www.ccs.neu.edu/home/luwang Email: luwang@ccs.neu.edu Sign
More informationSOE3213/4: CFD Lecture 1
What is CFD SOE3213/4: CFD Lecture 1 3d 3d Computational Fluid Dynamics { use of computers to study uid dynamics. Solve the Navier-Stokes Equations (NSE) : r:u = 0 Du Dt = rp + r 2 u + F 4 s for 4 unknowns,
More informationCosmological N-Body Simulations and Galaxy Surveys
Cosmological N-Body Simulations and Galaxy Surveys Adrian Pope, High Energy Physics, Argonne Na3onal Laboratory, apope@anl.gov CScADS: Scien3fic Data and Analy3cs for Extreme- scale Compu3ng, 30 July 2012
More informationA6523 Modeling, Inference, and Mining Jim Cordes, Cornell University
A6523 Modeling, Inference, and Mining Jim Cordes, Cornell University Lecture 23 Birthday problem comments Construc
More informationProgress in Numerical Methods at ECMWF
Progress in Numerical Methods at ECMWF EWGLAM / SRNWP October 2016 W. Deconinck, G. Mengaldo, C. Kühnlein, P.K. Smolarkiewicz, N.P. Wedi, P. Bauer willem.deconinck@ecmwf.int ECMWF November 7, 2016 2 The
More informationSpace-time domain decomposition for a nonlinear parabolic equation with discontinuous capillary pressure
Space-time domain decomposition for a nonlinear parabolic equation with discontinuous capillary pressure Elyes Ahmed, Caroline Japhet, Michel Kern INRIA Paris Maison de la Simulation ENPC University Paris
More informationStability constants for kernel-based interpolation processes
Dipartimento di Informatica Università degli Studi di Verona Rapporto di ricerca Research report 59 Stability constants for kernel-based interpolation processes Stefano De Marchi Robert Schaback Dipartimento
More informationA unifying model for fluid flow and elastic solid deformation: a novel approach for fluid-structure interaction and wave propagation
A unifying model for fluid flow and elastic solid deformation: a novel approach for fluid-structure interaction and wave propagation S. Bordère a and J.-P. Caltagirone b a. CNRS, Univ. Bordeaux, ICMCB,
More informationLattice Boltzmann Method
3 Lattice Boltzmann Method 3.1 Introduction The lattice Boltzmann method is a discrete computational method based upon the lattice gas automata - a simplified, fictitious molecular model. It consists of
More informationA recovery-assisted DG code for the compressible Navier-Stokes equations
A recovery-assisted DG code for the compressible Navier-Stokes equations January 6 th, 217 5 th International Workshop on High-Order CFD Methods Kissimmee, Florida Philip E. Johnson & Eric Johnsen Scientific
More informationIndefinite and physics-based preconditioning
Indefinite and physics-based preconditioning Jed Brown VAW, ETH Zürich 2009-01-29 Newton iteration Standard form of a nonlinear system F (u) 0 Iteration Solve: Update: J(ũ)u F (ũ) ũ + ũ + u Example (p-bratu)
More informationEfficient 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 informationWRF- Hydro Development and Performance Tes9ng
WRF- Hydro Development and Performance Tes9ng Wei Yu, David Gochis, David Yates Research Applica9ons Laboratory Na9onal Center for Atmospheric Research Boulder, CO USA Scien9fic Mo9va9on How does terrain
More informationZonal modelling approach in aerodynamic simulation
Zonal modelling approach in aerodynamic simulation and Carlos Castro Barcelona Supercomputing Center Technical University of Madrid Outline 1 2 State of the art Proposed strategy 3 Consistency Stability
More informationRobust Domain Decomposition Preconditioners for Abstract Symmetric Positive Definite Bilinear Forms
www.oeaw.ac.at Robust Domain Decomposition Preconditioners for Abstract Symmetric Positive Definite Bilinear Forms Y. Efendiev, J. Galvis, R. Lazarov, J. Willems RICAM-Report 2011-05 www.ricam.oeaw.ac.at
More informationSimulation of Unsaturated Flow Using Richards Equation
Simulation of Unsaturated Flow Using Richards Equation Rowan Cockett Department of Earth and Ocean Science University of British Columbia rcockett@eos.ubc.ca Abstract Groundwater flow in the unsaturated
More informationPREDICTIVE SIMULATION OF UNDERWATER IMPLOSION: Coupling Multi-Material Compressible Fluids with Cracking Structures
PREDICTIVE SIMULATION OF UNDERWATER IMPLOSION: Coupling Multi-Material Compressible Fluids with Cracking Structures Kevin G. Wang Virginia Tech Patrick Lea, Alex Main, Charbel Farhat Stanford University
More informationCode MIGALE state- of- the- art
Code MIGALE state- of- the- art A. Colombo HiOCFD4 4th International Workshop on High- Order CFD Method Foundation for Research and Technology Hellas (FORTH), Heraklion (Crete) 4th June 2016 1 with the
More informationSolving 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 informationThere are no simple turbulent flows
Turbulence 1 There are no simple turbulent flows Turbulent boundary layer: Instantaneous velocity field (snapshot) Ref: Prof. M. Gad-el-Hak, University of Notre Dame Prediction of turbulent flows standard
More informationAccelerating incompressible fluid flow simulations on hybrid CPU/GPU systems
Accelerating incompressible fluid flow simulations on hybrid CPU/GPU systems Yushan Wang 1, Marc Baboulin 1,2, Karl Rupp 3,4, Yann Fraigneau 1,5, Olivier Le Maître 1,5 1 Université Paris-Sud, France 2
More informationAn arbitrary lagrangian eulerian discontinuous galerkin approach to fluid-structure interaction and its application to cardiovascular problem
An arbitrary lagrangian eulerian discontinuous galerkin approach to fluid-structure interaction and its application to cardiovascular problem Yifan Wang University of Houston, Department of Mathematics
More informationThe Rigid Rotor Problem: A quantum par7cle confined to a sphere Spherical Harmonics. Reading: McIntyre 7.6
The Rigid Rotor Problem: A quantum par7cle confined to a sphere Spherical Harmonics Reading: McIntyre 7.6 Legendre s equa7on (m = 0) The series must be finite! If the series is not finite, the polynomial
More informationRBF-FD Approximation to Solve Poisson Equation in 3D
RBF-FD Approximation to Solve Poisson Equation in 3D Jagadeeswaran.R March 14, 2014 1 / 28 Overview Problem Setup Generalized finite difference method. Uses numerical differentiations generated by Gaussian
More informationAProofoftheStabilityoftheSpectral Difference Method For All Orders of Accuracy
AProofoftheStabilityoftheSpectral Difference Method For All Orders of Accuracy Antony Jameson 1 1 Thomas V. Jones Professor of Engineering Department of Aeronautics and Astronautics Stanford University
More informationHybridized Discontinuous Galerkin Methods
Hybridized Discontinuous Galerkin Methods Theory and Christian Waluga Joint work with Herbert Egger (Uni Graz) 1st DUNE User Meeting, Stuttgart Christian Waluga (AICES) HDG Methods October 6-8, 2010 1
More informationA High Order Conservative Semi-Lagrangian Discontinuous Galerkin Method for Two-Dimensional Transport Simulations
Motivation Numerical methods Numerical tests Conclusions A High Order Conservative Semi-Lagrangian Discontinuous Galerkin Method for Two-Dimensional Transport Simulations Xiaofeng Cai Department of Mathematics
More informationReduced Models for Process Simula2on and Op2miza2on
Reduced Models for Process Simulaon and Opmizaon Yidong Lang, Lorenz T. Biegler and David Miller ESI annual meeng March, 0 Models are mapping Equaon set or Module simulators Input space Reduced model Surrogate
More informationSpace-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 informationNumerical Methods in Biomedical Engineering
Numerical Methods in Biomedical Engineering Lecture s website for updates on lecture materials: h5p://9nyurl.com/m4frahb Individual and group homework Individual and group midterm and final projects (Op?onal)
More informationIMPLEMENTATION OF A PARALLEL AMG SOLVER
IMPLEMENTATION OF A PARALLEL AMG SOLVER Tony Saad May 2005 http://tsaad.utsi.edu - tsaad@utsi.edu PLAN INTRODUCTION 2 min. MULTIGRID METHODS.. 3 min. PARALLEL IMPLEMENTATION PARTITIONING. 1 min. RENUMBERING...
More informationJacobian-Free Newton Krylov Discontinuous Galerkin Method and Physics-Based Preconditioning for Nuclear Reactor Simulations
INL/CON-08-14243 PREPRINT Jacobian-Free Newton Krylov Discontinuous Galerkin Method and Physics-Based Preconditioning for Nuclear Reactor Simulations International Conference on Reactor Physics, Nuclear
More informationSome Advances on Isogeometric Analysis at KAUST
Some Advances on Isogeometric Analysis at KAUST Victor M. Calo Applied Mathema=cs & Computa=onal Science Earth Science & Engineering King Abdullah University of Science and Technology Joint work with:
More informationComparison of numerical schemes for multiphase reactive transport
Énergies renouvelables Production éco-responsable Transports innovants Procédés éco-efficients Ressources durables Comparison of numerical schemes for multiphase reactive transport T. Faney, A. Michel,
More informationPalindromic Discontinuous Galerkin Method
Palindromic Discontinuous Galerkin Method David Coulette, Emmanuel Franck, Philippe Helluy, Michel Mehrenberger, Laurent Navoret To cite this version: David Coulette, Emmanuel Franck, Philippe Helluy,
More informationPOD-based Reduced Order Models for Parameterized PDEs
POD-based Reduced Order Models for Parameterized PDEs Florian De Vuyst florian.de-vuyst@ecp.fr Ecole Centrale Paris Laboratoire Mathématiques Appliquées aux Systèmes July 2008 the 1st Outline 1. Setting
More informationA Linear Multigrid Preconditioner for the solution of the Navier-Stokes Equations using a Discontinuous Galerkin Discretization. Laslo Tibor Diosady
A Linear Multigrid Preconditioner for the solution of the Navier-Stokes Equations using a Discontinuous Galerkin Discretization by Laslo Tibor Diosady B.A.Sc., University of Toronto (2005) Submitted to
More informationApproximate tensor-product preconditioners for very high order discontinuous Galerkin methods
Approximate tensor-product preconditioners for very high order discontinuous Galerkin methods Will Pazner 1 and Per-Olof Persson 2 1 Division of Applied Mathematics, Brown University, Providence, RI, 02912
More informationPseudospectral and High-Order Time-Domain Forward Solvers
Pseudospectral and High-Order Time-Domain Forward Solvers Qing H. Liu G. Zhao, T. Xiao, Y. Zeng Department of Electrical and Computer Engineering Duke University DARPA/ARO MURI Review, August 15, 2003
More informationFISIKA KOMPUTASI (COMPUTATIONAL PHYSICS) Ishafit Program Studi Pendidikan Fisika Universitas Ahmad Dahlan
FISIKA KOMPUTASI (COMPUTATIONAL PHYSICS) Ishafit Program Studi Pendidikan Fisika Universitas Ahmad Dahlan What is Computational Science What is Computational Physics Reference: Resource Letter CP-2: Computational
More informationPart 1. The diffusion equation
Differential Equations FMNN10 Graded Project #3 c G Söderlind 2016 2017 Published 2017-11-27. Instruction in computer lab 2017-11-30/2017-12-06/07. Project due date: Monday 2017-12-11 at 12:00:00. Goals.
More informationLocal 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 informationThe Riccati transformation method for linear two point boundary problems
Chapter The Riccati transformation method for linear two point boundary problems The solution algorithm for two point boundary value problems to be employed here has been derived from different points
More informationStable and high-order accurate finite difference schemes on singular grids
Center for Turbulence Research Annual Research Briefs 006 197 Stable and high-order accurate finite difference schemes on singular grids By M. Svärd AND E. van der Weide 1. Motivation and objectives The
More informationParallel Linear Solvers for Simula6ons of Reactor Thermal Hydraulics
Parallel Linear Solvers for Simula6ons of Reactor Thermal Hydraulics Y. Yan 1, S.P. Antal 2, B. Edge 2, D.E. Keyes 1, D. Shaver 2, I.A. Bolotnov 3 and M.Z. Podowski 2 1 Columbia University, New York, NY,
More informationStabilization and Acceleration of Algebraic Multigrid Method
Stabilization and Acceleration of Algebraic Multigrid Method Recursive Projection Algorithm A. Jemcov J.P. Maruszewski Fluent Inc. October 24, 2006 Outline 1 Need for Algorithm Stabilization and Acceleration
More informationHadronic contribu-ons to (g 2) μ from La4ce QCD: Results from the Mainz group
Hadronic contribu-ons to (g 2) μ from La4ce QCD: Results from the Mainz group Hartmut Wi4g PRISMA Cluster of Excellence, Ins6tute for Nuclear Physics and Helmholtz Ins6tute Mainz Interna-onal Workshop
More informationA Strategy for the Development of Coupled Ocean- Atmosphere Discontinuous Galerkin Models
A Strategy for the Development of Coupled Ocean- Atmosphere Discontinuous Galerkin Models Frank Giraldo Department of Applied Math, Naval Postgraduate School, Monterey CA 93943 Collaborators: Jim Kelly
More information