Well-balanced schemes for the Euler equations with gravitation
|
|
- Austen Miles
- 5 years ago
- Views:
Transcription
1 Well-balanced schemes for the Euler equations with gravitation Roger Käppeli Joint work with S. Mishra
2 Outline Introduction Well-balanced scheme for HydroStatic Equilibrium (HSE) First order Second order Multi-D & further extensions Conclusions Roger Käppeli, Lyon
3 Outline Introduction Well-balanced scheme for HydroStatic Equilibrium (HSE) First order Second order Multi-D & further extensions Conclusions Roger Käppeli, Lyon
4 i) Introduction Stellar life cycle
5 i) Introduction Stellar life cycle
6 i) Introduction Stellar life cycle
7 i) Introduction Core-collapse supernova General idea: Explosion powered by gravitational binding energy of forming compact remnant: GRAVITY BOMB! Roger Käppeli, Lyon 2013 Mass of remnant Radius of remnant 7
8 i) Introduction Core-collapse supernova Roger Käppeli, Lyon
9 i) Introduction Radial profile The problem: (in our simulations) Ability to maintain near hydrostatic equilibrium for a long time! Roger Käppeli, Lyon
10 Outline Introduction Well-balanced scheme for HydroStatic Equilibrium (HSE) First order Second order Multi-D & further extensions Conclusions Roger Käppeli, Lyon
11 ii) WB scheme for HSE Well-balanced scheme for HSE Consider 1D hydrodynamics eqs with gravity Classical solution algorithm: Solve homogeneous eqs with Godunov type method (i.e. solve Riemann problem) Account for source term in second step (split/unsplit) Roger Käppeli, Lyon
12 ii) WB scheme for HSE Well-balanced scheme for HSE (2) Classical solution algorithm: (Local) Lax-Friedrichs HLL (C) Roe Lax (1954), Rusanov (1961) Harten, Lax and van Leer (1983), Toro et al. (1994) Roe (1981) Roger Käppeli, Lyon
13 ii) WB scheme for HSE Well-balanced scheme for HSE (3) Interested in hydrostatic EoS: 13
14 ii) WB scheme for HSE Well-balanced scheme for HSE (3)
15 ii) WB scheme for HSE Well-balanced scheme for HSE (3)
16 ii) WB scheme for HSE Well-balanced scheme for HSE (3)
17 ii) WB scheme for HSE Well-balanced scheme for HSE (3)
18 ii) WB scheme for HSE Well-balanced scheme for HSE (4) The problem: (in our simulations) Ability to maintain near hydrostatic equilibrium for a long time! Roger Käppeli, Lyon
19 ii) WB scheme for HSE Well-balanced scheme for HSE (5) Solutions: at each time Steady state preserving reconstructions, wellbalanced schemes e.g. LeVeque (1998), LeVeque & Bale (1998), Botta et al. (2004), Fuchs et al. (2010), Xing & Shu (2013), Vides et al. (2013) Note: there are many, many more... especially for shallow-water eqs!!! Roger Käppeli, Lyon
20 ii) WB scheme for HSE Well-balanced scheme for HSE (5) Solutions: at each time Steady state preserving reconstructions, wellbalanced schemes e.g. LeVeque (1998), LeVeque & Bale (1998), Botta et al. (2004), Fuchs et al. (2010), Xing & Shu (2013), Vides et al. (2013) Requirements Equilibrium not known in advance (self-gravity) Extensible for general EoS (At least) second order accuracy Preserve Note: there are robustness many, many more... especially shallow-water eqs!!! of base shock for capturing Roger Käppeli, Lyon 2013 scheme 20
21 ii) WB scheme for HSE Well-balanced scheme for HSE (6) Hydrostatic equilibrium Describes only a mechanical equilibrium... Density and pressure not uniquely determined Entropy Temperature Arbitrary entropy or temperature profiles not (physically) stable (convection!) Roger Käppeli, Lyon
22 ii) WB scheme for HSE Well-balanced scheme for HSE (7) Consider constant entropy profile Using the thermodynamic relation Enthalpy Hydrostatic eq.
23 ii) WB scheme for HSE Well-balanced scheme for HSE (8) Perform equilibrium reconstruction:
24 ii) WB scheme for HSE Well-balanced scheme for HSE (9) Well-balanced discretization of momentum source term Roger Käppeli, Lyon 2013 Well-balanced wrt hydrostatic equilibrium! 24
25 ii) WB scheme for HSE Well-balanced scheme for HSE (10) Second order extension: pressure, density Eq. perturbation Stencil: Data Equilibrium Similar to Botta et al. 2004,Fuchs et al Time stepping:
26 ii) WB scheme for HSE Example 1 Hydrostatic atmosphere in a constant gravitational field
27 ii) WB scheme for HSE Example 2 Hydrostatic atmosphere in a constant gravitational field
28 ii) WB scheme for HSE Example 3 Hydrostatic atmosphere in a constant gravitational field
29 Outline Introduction Well-balanced scheme for HydroStatic Equilibrium (HSE) First order Second order Multi-D & further extensions Conclusions Roger Käppeli, Lyon
30 ii) Multi-D & further extensions Multi-dimensional extension Straight forward directional application of HydroStatic Reconstruction Hydrostatic equilibrium: Roger Käppeli, Lyon
31 ii) Multi-D & further extensions Example 4 Polytrope: model star (e.g. main sequence stars, white dwarfs, neutron stars) HSE: Poisson equation: Equation of state Take ~ neutron stars Then there's an exact solution:
32 ii) Multi-D & further extensions Example 4
33 ii) Multi-D & further extensions Example 4
34 ii) Multi-D & further extensions Example 4
35 ii) Multi-D & further extensions Example 4
36 ii) Multi-D & further extensions Example 4
37 ii) Multi-D & further extensions Example 4
38 ii) Multi-D & further extensions Example 4
39 ii) Multi-D & further extensions Well-balanced scheme for HSE Consider constant temperature profile Using the thermodynamic relation Hydrostatic eq. Gibbs free energy
40 ii) Multi-D & further extensions Well-balanced scheme for HSE Interested in numerical hydrostatic equilibrium: Roger Käppeli, HYP2012, Padova 40
41 ii) Multi-D & further extensions Well-balanced scheme for HSE
42 ii) Multi-D & further extensions Well-balanced scheme for HSE
43 ii) Multi-D & further extensions Well-balanced scheme for HSE
44 ii) Multi-D & further extensions Example 5 Hydrostatic atmosphere in a constant gravitational field
45 Conclusions 1D well-balanced scheme for (isentropic, isothermal, arbitrary) hydrostatic equilibrium (for general EoS) Extension to higher-order? Non-zero velocity steady state? (e.g. for steady accretion flow) Multi-D well-balanced scheme for (isentropic, isothermal) hydrostatic equilibrium (for general EoS) Käppeli, Lyon 2013 Thank youroger for your attention!!! 45
Numerical Methods for Hyperbolic and Kinetic Equations
Numerical Methods for Hyperbolic and Kinetic Equations Organizer: G. Puppo Phenomena characterized by conservation (or balance laws) of physical quantities are modelled by hyperbolic and kinetic equations.
More informationA Review on the Numerical Solution of the 1D Euler Equations. Hudson, Justin. MIMS EPrint:
A Review on the Numerical Solution of the D Euler Equations Hudson, Justin 6 MIMS EPrint: 6.9 Manchester Institute for Mathematical Sciences School of Mathematics The University of Manchester Reports available
More informationA new multidimensional-type reconstruction and limiting procedure for unstructured (cell-centered) FVs solving hyperbolic conservation laws
HYP 2012, Padova A new multidimensional-type reconstruction and limiting procedure for unstructured (cell-centered) FVs solving hyperbolic conservation laws Argiris I. Delis & Ioannis K. Nikolos (TUC)
More informationAdaptive Mesh Astrophysical Fluid Simulations on GPU. San Jose 10/2/2009 Peng Wang, NVIDIA
Adaptive Mesh Astrophysical Fluid Simulations on GPU San Jose 10/2/2009 Peng Wang, NVIDIA Overview Astrophysical motivation & the Enzo code Finite volume method and adaptive mesh refinement (AMR) CUDA
More informationLagrangian 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 informationA CONSERVATIVE FRONT TRACKING ALGORITHM
A CONSERVATIVE FRONT TRACKING ALGORITHM Vinh Tan Nguyen, Khoo Boo Cheong and Jaime Peraire Singapore-MIT Alliance Department of Mechanical Engineering, National University of Singapore Department of Aeronautics
More informationTable of contents for: Waves and Mean Flows by Oliver Bühler Cambridge University Press 2009 Monographs on Mechanics. Contents.
Table of contents for: Waves and Mean Flows by Oliver Bühler Cambridge University Press 2009 Monographs on Mechanics. Preface page 2 Part I Fluid Dynamics and Waves 7 1 Elements of fluid dynamics 9 1.1
More informationStability and Pulsations of Wolf - Rayet Stars
Stability and Pulsations of Wolf - Rayet Stars Talk presented on the conference Hydrogen - Deficient Stars Tübingen, September 20, 2007 Wolfgang Glatzel Institut für Astrophysik, Universität Göttingen
More informationLarge Scale Simulation of Cloud Cavitation Collapse
PRACEdays17 Barcelona, May 16-18, 2017 Large Scale Simulation of Cloud Cavitation Collapse Ursula Rasthofer with: Fabian Wermelinger, Petr Karnakov, Panagiotis Hadjidoukas, Petros Koumoutsakos CSElab Computational
More informationMid-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 informationOn the order of accuracy and numerical performance of two classes of finite volume WENO schemes
On the order of accuracy and numerical performance of two classes of finite volume WENO schemes Rui Zhang, Mengping Zhang and Chi-Wang Shu November 29, 29 Abstract In this paper we consider two commonly
More informationComputer simulations using implicit Lagrangian hydrodynamics in 3D
Highlights of Spanish Astrophysics VI, Proceedings of the IX Scientific Meeting of the Spanish Astronomical Society held on September 13-17, 2010, in Madrid, Spain. M. R. Zapatero Osorio et al. (eds.)
More informationCGT 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 informationRK-Time Integration and High-Order Spatial Discretization a New Dynamical Core for the LMK
RK-Time Integration and High-Order Spatial Discretization a New Dynamical Core for the LMK Jochen Förstner Deutscher Wetterdienst, Kaiserleistraße 35, 63067 Offenbach am Main jochen.foerstner@dwd.de COSMO
More informationA mass-conservative version of the semi- Lagrangian semi-implicit HIRLAM using Lagrangian vertical coordinates
A mass-conservative version of the semi- Lagrangian semi-implicit HIRLAM using Lagrangian vertical coordinates Peter Hjort Lauritzen Atmospheric Modeling & Predictability Section National Center for Atmospheric
More informationTechnical Report TR
Technical Report TR-2015-09 Boundary condition enforcing methods for smoothed particle hydrodynamics Arman Pazouki 1, Baofang Song 2, Dan Negrut 1 1 University of Wisconsin-Madison, Madison, WI, 53706-1572,
More informationLecture 1: Finite Volume WENO Schemes Chi-Wang Shu
Lecture 1: Finite Volume WENO Schemes Chi-Wang Shu Division of Applied Mathematics Brown University Outline of the First Lecture General description of finite volume schemes for conservation laws The WENO
More informationSPH: 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 informationLax-Wendroff and McCormack Schemes for Numerical Simulation of Unsteady Gradually and Rapidly Varied Open Channel Flow
Archives of Hydro-Engineering and Environmental Mechanics Vol. 60 (2013), No. 1 4, pp. 51 62 DOI: 10.2478/heem-2013-0008 IBW PAN, ISSN 1231 3726 Lax-Wendroff and McCormack Schemes for Numerical Simulation
More informationInterpolation of gridded data using Geostrophic Balance. Lennon O Naraigh *
Interpolation of gridded data using Geostrophic Balance Lennon O Naraigh * Date: 6 th September 2004 Abstract: In this report, a method of interpolating data from the grid of a global climate model (GCM)
More informationHierarchical Reconstruction for Spectral Volume Method on Unstructured Grids
Hierarchical Reconstruction for Spectral Volume Method on Unstructured Grids Zhiliang Xu, Yingjie Liu and Chi-Wang Shu April 4, 2009 Abstract The hierarchical reconstruction (HR) [, 24] is applied to a
More informationA finite-volume integration method for computing pressure gradient force in general vertical coordinates
Q. J. R. Meteorol. Soc. (1997), 123, pp. 1749-1 762 A finite-volume integration method for computing pressure gradient force in general vertical coordinates By SHIAN-JIANN LIN* University of Maryland,
More informationA third order conservative Lagrangian type scheme on curvilinear meshes for the compressible Euler equations
A third order conservative Lagrangian type scheme on curvilinear meshes for the compressible Euler equations Juan Cheng and Chi-Wang Shu 2 Abstract Based on the high order essentially non-oscillatory (ENO)
More informationFluid-structure Interaction by the mixed SPH-FE Method with Application to Aircraft Ditching
Fluid-structure Interaction by the mixed SPH-FE Method with Application to Aircraft Ditching Paul Groenenboom ESI Group Delft, Netherlands Martin Siemann German Aerospace Center (DLR) Stuttgart, Germany
More informationParticle-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 informationOn the Order of Accuracy and Numerical Performance of Two Classes of Finite Volume WENO Schemes
Commun. Comput. Phys. doi: 8/cicp.99.84s Vol. 9, No. 3, pp. 87-87 March On the Order of Accuracy and Numerical Performance of Two Classes of Finite Volume WENO Schemes Rui Zhang, Mengping Zhang and Chi-Wang
More informationShallow Water Equations:Variable Bed Topography Adam Riley Computer Science (with Industry) 2011/2012
Shallow Water Equations:Variable Bed Topography Adam Riley Computer Science (with Industry) 011/01 The candidate confirms that the work submitted is their own and the appropriate credit has been given
More informationHigh-Order CENO Reconstruction Scheme For Three-Dimensional Unstructured Mesh
High-Order CENO Reconstruction Scheme For Three-Dimensional Unstructured Mesh by Al-Amin Aziz A thesis submitted in conformity with the requirements for the degree of Masters of Applied Science Graduate
More informationFaculty 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 informationTutorial 17. Using the Mixture and Eulerian Multiphase Models
Tutorial 17. Using the Mixture and Eulerian Multiphase Models Introduction: This tutorial examines the flow of water and air in a tee junction. First you will solve the problem using the less computationally-intensive
More information1.6 Smoothed particle hydrodynamics (SPH)
26 Smoothed Particle Hydrodynamics 1.6 Smoothed particle hydrodynamics (SPH) 1.6.1 The SPH method In the SPH method, the state of a system is represented by a set of particles, which possess individual
More informationHigh Order Fixed-Point Sweeping WENO Methods for Steady State of Hyperbolic Conservation Laws and Its Convergence Study
Commun. Comput. Phys. doi:.48/cicp.375.6a Vol., No. 4, pp. 835-869 October 6 High Order Fixed-Point Sweeping WENO Methods for Steady State of Hyperbolic Conservation Laws and Its Convergence Study Liang
More informationImplicit versus Explicit Finite Volume Schemes for Extreme, Free Surface Water Flow Modelling
Archives of Hydro-Engineering and Environmental Mechanics Vol. 51 (2004), No. 3, pp. 287 303 Implicit versus Explicit Finite Volume Schemes for Extreme, Free Surface Water Flow Modelling Michał Szydłowski
More informationRELATIVISTIC HYDRODYNAMIC FLOWS USING SPATIAL AND TEMPORAL ADAPTIVE STRUCTURED MESH REFINEMENT
The Astrophysical Journal Supplement Series, 176:467Y483, 2008 June # 2008. The American Astronomical Society. All rights reserved. Printed in U.S.A. RELATIVISTIC HYDRODYNAMIC FLOWS USING SPATIAL AND TEMPORAL
More informationTutorial: Using Wells and Polygonal Mesh Refinement PetraSim 5
403 Poyntz Avenue, Suite B Manhattan, KS 66502 USA +1.785.770.8511 www.thunderheadeng.com Tutorial: Using Wells and Polygonal Mesh Refinement PetraSim 5 Introduction Wells are a mesh-independent way to
More informationFinal 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 informationDivergence Form for Bed Slope Source Term in Shallow Water Equations
Divergence Form for Bed Slope Source Term in Shallow Water Equations Alessandro Valiani 1 and Lorenzo Begnudelli 2 Abstract: A novel technique is presented for the treatment of the bed slope source terms
More informationAcknowledgements. Prof. Dan Negrut Prof. Darryl Thelen Prof. Michael Zinn. SBEL Colleagues: Hammad Mazar, Toby Heyn, Manoj Kumar
Philipp Hahn Acknowledgements Prof. Dan Negrut Prof. Darryl Thelen Prof. Michael Zinn SBEL Colleagues: Hammad Mazar, Toby Heyn, Manoj Kumar 2 Outline Motivation Lumped Mass Model Model properties Simulation
More informationHigh Order Schemes for CFD: A Review. Juan Cheng 1. Institute of Applied Physics and Computational Mathematics, Beijing , China.
High Order Schemes for CFD: A Review Juan Cheng 1 Institute of Applied Physics and Computational Mathematics, Beijing 100088, China and Chi-Wang Shu 2 Division of Applied Mathematics, Brown University,
More informationIMPROVED WALL BOUNDARY CONDITIONS WITH IMPLICITLY DEFINED WALLS FOR PARTICLE BASED FLUID SIMULATION
6th European Conference on Computational Mechanics (ECCM 6) 7th European Conference on Computational Fluid Dynamics (ECFD 7) 1115 June 2018, Glasgow, UK IMPROVED WALL BOUNDARY CONDITIONS WITH IMPLICITLY
More informationVolume II SENSITIVITY and UNCERTAINTY ANALYSIS. Applications to Large-Scale Systems
Volume II SENSITIVITY and UNCERTAINTY ANALYSIS Applications to Large-Scale Systems TABLE OF CONTENTS I. A COMPARATIVE REVIEW OF SENSITIVITY AND UNCERTAINTY ANALYSIS METHODS FOR LARGE-SCALE SYSTEMS 1 A.
More informationA New Trouble-Cell Indicator for Discontinuous Galerkin Methods for. Hyperbolic Conservation Laws ABSTRACT
A New Trouble-Cell Indicator for Discontinuous Galerkin Methods for Hyperbolic Conservation Laws Guosheng Fu and Chi-Wang Shu ABSTRACT We introduce a new troubled-cell indicator for the discontinuous Galerkin
More informationarxiv: v2 [astro-ph.sr] 20 Nov 2009
Astronomy & Astrophysics manuscript no. paper c ESO 2009 November 20, 2009 A 3D radiative transfer framework: VI. PHOENIX/3D example applications Peter H. Hauschildt 1 and E. Baron 1,2,3 arxiv:0911.3285v2
More informationNUMERICAL INVESTIGATION OF ONE- DIMENSIONAL SHALLOW WATER FLOW AND SEDIMENT TRANSPORT MODEL USING DISCONTINOUOUS GALERKIN METHOD
Clemson University TigerPrints All Dissertations Dissertations 5-2014 NUMERICAL INVESTIGATION OF ONE- DIMENSIONAL SHALLOW WATER FLOW AND SEDIMENT TRANSPORT MODEL USING DISCONTINOUOUS GALERKIN METHOD Farzam
More informationRequirements for a new EOS interface in the Einstein Toolkit
Requirements for a new EOS interface in the Einstein Toolkit Erik Schnetter, 2009-11-03 CIGR Talk Series, Baton Rouge, LA Tuesday, November 3, 2009 CCT: Center for Computation & Technology Discussion Topic
More informationA two-fluid solver for hydraulic applications
A two-fluid solver for hydraulic applications L. Qian, D. M. Causon, D. M. Ingram&C. G. Mingham Department of Computing and Mathematics, I%e Manchester Metropolitan University, Manchester Ml 5 GD, United
More informationSelf-Cultivation System
Development of a Microorganism Incubator using CFD Simulations Self-Cultivation System A comfortable mixing incubator to grow microorganism for agricultural, animal husbandry and ocean agriculture industries
More informationNavier-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 informationAdaptive Discontinuous Galerkin Method for the Shallow Water Equations
INTERNATIONAL JOURNAL FOR NUMERICAL METHODS IN FLUIDS Int. J. Numer. Meth. Fluids 2003; 00:1 20 [Version: 2002/09/18 v1.01] Adaptive Discontinuous Galerkin Method for the Shallow Water Equations Jean-François
More informationNIA 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 informationParallel Adaptive Tsunami Modelling with Triangular Discontinuous Galerkin Schemes
Parallel Adaptive Tsunami Modelling with Triangular Discontinuous Galerkin Schemes Stefan Vater 1 Kaveh Rahnema 2 Jörn Behrens 1 Michael Bader 2 1 Universität Hamburg 2014 PDES Workshop 2 TU München Partial
More informationEssay 1: Dimensional Analysis of Models and Data Sets: Similarity Solutions
Table of Contents Essay 1: Dimensional Analysis of Models and Data Sets: Similarity Solutions and Scaling Analysis 1 About dimensional analysis 4 1.1 Thegoalandtheplan... 4 1.2 Aboutthisessay... 5 2 Models
More informationINTRODUCTION TO HEC-RAS
INTRODUCTION TO HEC-RAS HEC- RAS stands for Hydrologic Engineering Center s River Analysis System By U.S. Army Corps of Engineers One dimensional analysis of : 1. Steady flow 2. Unsteady flow 3. Sediment
More informationc 2005 Society for Industrial and Applied Mathematics
SIAM J. SCI. COMPUT. Vol. 6, No. 3, pp. 785 89 c 5 Society for Industrial and Applied Mathematics A HIGH-RESOLUTION ROTATED GRID METHOD FOR CONSERVATION LAWS WITH EMBEDDED GEOMETRIES CHRISTIANE HELZEL,
More informationc 2011 Society for Industrial and Applied Mathematics
SIAM J. SCI. COMPUT. Vol. 33, No., pp. 588 611 c 011 Society for Industrial and Applied Mathematics VORTICITY PRESERVING FINITE VOLUME SCHEMES FOR THE SHALLOW WATER EQUATIONS ULRIK S. FJORDHOLM AND SIDDHARTHA
More informationCalculate a solution using the pressure-based coupled solver.
Tutorial 19. Modeling Cavitation Introduction This tutorial examines the pressure-driven cavitating flow of water through a sharpedged orifice. This is a typical configuration in fuel injectors, and brings
More informationA-posteriori Diffusion Analysis of Numerical Schemes in Wavenumber Domain
2th Annual CFD Symposium, August 9-1, 218, Bangalore A-posteriori Diffusion Analysis of Numerical Schemes in Wavenumber Domain S. M. Joshi & A. Chatterjee Department of Aerospace Engineering Indian Institute
More informationNumerical Simulation of Tsunami Propagation and Runup: Case study on the South China Sea
Numerical Simulation of Tsunami Propagation and Runup: Case study on the South China Sea By Phung D. Hieu Center for Marine and Ocean-Atmosphere Interaction Research, Vietnam Email: phungdanghieu@vkttv.edu.vn;
More informationCOMPLETE DERIVATION OF 2D SHALLOW-WATER MODEL FROM THE PRIMITIVE EQUATIONS GOVERNING GEOPHYSICAL FLOWS
COMPLETE DERIVATION OF 2D SHALLOW-WATER MODEL FROM THE PRIMITIVE EQUATIONS GOVERNING GEOPHYSICAL FLOWS Muhammad Salihi Bin Abdul Hadi, Mohd Zaini Bin Mustapa & Shahbudin Bin Saad Institute of Oceanography
More informationHomework 4A Due November 7th IN CLASS
CS207, Fall 2014 Systems Development for Computational Science Cris Cecka, Ray Jones Homework 4A Due November 7th IN CLASS Previously, we ve developed a quite robust Graph class to let us use Node and
More informationChapter 1 - Basic Equations
2.20 Marine Hydrodynamics, Fall 2017 Lecture 2 Copyright c 2017 MIT - Department of Mechanical Engineering, All rights reserved. 2.20 Marine Hydrodynamics Lecture 2 Chapter 1 - Basic Equations 1.1 Description
More informationUsing the Eulerian Multiphase Model for Granular Flow
Tutorial 21. Using the Eulerian Multiphase Model for Granular Flow Introduction Mixing tanks are used to maintain solid particles or droplets of heavy fluids in suspension. Mixing may be required to enhance
More informationA Novel Multi-Dimensional Limiter for High-Order Finite Volume Methods on Unstructured Grids
Commun. Comput. Phys. doi:.428/cicp.oa-27-39 Vol. xx, No. x, pp. -28 xxx 2x A Novel Multi-Dimensional Limiter for High-Order Finite Volume Methods on Unstructured Grids Yilang Liu, Weiwei Zhang, and Chunna
More informationDevelopment 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 informationChallenges and recent progress in developing numerical methods for multi-material ALE Hydrocodes
Challenges and recent progress in developing numerical methods for multi-material ALE Hydrocodes ICFD 25 year Anniversary Conference 15-16 th September 2008 Oxford University Andrew Barlow AWE Introduction
More informationMultigrid Third-Order Least-Squares Solution of Cauchy-Riemann Equations on Unstructured Triangular Grids
INTERNATIONAL JOURNAL FOR NUMERICAL METHODS IN FLUIDS Int. J. Numer. Meth. Fluids ; : 6 Prepared using fldauth.cls [Version: /9/8 v.] Multigrid Third-Order Least-Squares Solution of Cauchy-Riemann Equations
More informationComputation of Fictitious Gas Flow with Euler Equations
1 Computation of Fictitious Gas Flow with Euler Equations Pei Li and Helmut Sobieczky DLR Göttingen, Germany Abstract The Fictitious Gas Concept supports some computational design methods to construct
More informationExactPack: A Master Code of Exact Solutions for Code Verification
ExactPack: A Master Code of Exact Solutions for Code Verification Robert L. Singleton Jr. Los Alamos National Laboratory bobs1@lanl.gov Collaborators: Scott Doebling Daniel Israel James Kamm ASME V&V Symposium
More informationAnimation of Fluids. Animating Fluid is Hard
Animation of Fluids Animating Fluid is Hard Too complex to animate by hand Surface is changing very quickly Lots of small details In short, a nightmare! Need automatic simulations AdHoc Methods Some simple
More informationMicrowell Mixing with Surface Tension
Microwell Mixing with Surface Tension Nick Cox Supervised by Professor Bruce Finlayson University of Washington Department of Chemical Engineering June 6, 2007 Abstract For many applications in the pharmaceutical
More informationCOMPARISON OF SEVERAL DIFFERENCE SCHEMES ON 1D AND 2D TEST PROBLEMS FOR THE EULER EQUATIONS
COMPARISON OF SEVERAL DIFFERENCE SCHEMES ON D AND D TEST PROBLEMS FOR THE EULER EQUATIONS RICHARD LISKA AND BURTON WENDROFF Available at http://www-troja.fjfi.cvut.cz/~liska/compareeuler/compare8/ Abstract.
More informationThompson/Ocean 420/Winter 2005 Internal Gravity Waves 1
Thompson/Ocean 420/Winter 2005 Internal Gravity Waves 1 II. Internal waves in continuous stratification The real ocean, of course, is continuously stratified. For continuous stratification, = (z), internal
More informationCarl Leake Embry-Riddle Aeronautical University,
College of Engineering Honors Program 8-11-2016 Testing the Accuracy of Commercial Computational Fluid Dynamics Codes: Vortex Transport by Uniform Flow and Transonic Ringleb Flow Problems Using ANSYS Fluent
More informationBubble Dynamics using Free Surfaces in a VOF framework
Bubble Dynamics using Free Surfaces in a VOF framework Sevilla Meeting: Numerical Challenges in two-phase flows 27 October 2014 Léon MALAN Supervisor: Prof. Stéphane ZALESKI 1 Contents Introduction: Simulation
More informationSmoothed Particle Hydrodynamics
Particle methods Part 1 Smoothed Particle Hydrodynamics Nathan Quinlan Mechanical Engineering 1: SPH 2: Truncation error and consistency of particle methods 3: FVPM CFD is mature Kroll et al. (2002) lift
More informationCFD 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 informationOPEN CHANNEL FLOW. An Introduction. -
OPEN CHANNEL FLOW An Introduction http://tsaad.utsi.edu - tsaad@utsi.edu OUTLINE General characteristics Surface Waves & Froude Number Effects Types of Channel flows The Hydraulic Jump Conclusion General
More informationDevelopment of Compressible-Incompressible Link to Efficiently Model Bubble Dynamics near Floating Body Chao-Tsung Hsiao 1, Georges L.
Development of Compressible-Incompressible Link to Efficiently Model Bubble Dynamics near Floating Body Chao-Tsung Hsiao 1, Georges L. Chahine 1 DYNAFLOW, INC. 1061-J Iron Bridge Road, Jessup, MD 0794,
More informationCHAPTER 3. Elementary Fluid Dynamics
CHAPTER 3. Elementary Fluid Dynamics - Understanding the physics of fluid in motion - Derivation of the Bernoulli equation from Newton s second law Basic Assumptions of fluid stream, unless a specific
More informationThis 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 informationALE and AMR Mesh Refinement Techniques for Multi-material Hydrodynamics Problems
ALE and AMR Mesh Refinement Techniques for Multi-material Hydrodynamics Problems A. J. Barlow, AWE. ICFD Workshop on Mesh Refinement Techniques 7th December 2005 Acknowledgements Thanks to Chris Powell,
More informationCOMPARISON OF CELL-CENTERED AND NODE-CENTERED FORMULATIONS OF A HIGH-RESOLUTION WELL-BALANCED FINITE VOLUME SCHEME: APPLICATION TO SHALLOW WATER FLOWS
XVIII International Conference on Water Resources CMWR 010 J. Carrera (Ed) CIMNE, Barcelona 010 COMPARISON OF CELL-CENTERED AND NODE-CENTERED FORMULATIONS OF A HIGH-RESOLUTION WELL-BALANCED FINITE VOLUME
More informationExample 13 - Shock Tube
Example 13 - Shock Tube Summary This famous experiment is interesting for observing the shock-wave propagation. Moreover, this case uses the representation of perfect gas and compares the different formulations:
More informationNavier-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 informationA SLOPE LIMITING PROCEDURE IN DISCONTINUOUS GALERKIN FINITE ELEMENT METHOD FOR GASDYNAMICS APPLICATIONS
INTERNATIONAL JOURNAL OF NUMERICAL ANALYSIS AND MODELING Volume 2, Number 2, Pages 163 178 c 25 Institute for Scientific Computing and Information A SLOPE LIMITING PROCEDURE IN DISCONTINUOUS GALERKIN FINITE
More informationRobust and Efficient Adaptive Moving Mesh Solution of the 2-D Euler equations
Contemporary Mathematics Robust and Efficient Adaptive Moving Mesh Solution of the -D Euler equations P. A. Zegeling, W. D. de Boer, and H. Z. Tang Abstract. In this paper we describe an adaptive moving
More informationRealtime Water Simulation on GPU. Nuttapong Chentanez NVIDIA Research
1 Realtime Water Simulation on GPU Nuttapong Chentanez NVIDIA Research 2 3 Overview Approaches to realtime water simulation Hybrid shallow water solver + particles Hybrid 3D tall cell water solver + particles
More informationWeighted Essentially Non-oscillatory Schemes on Triangular Meshes 1
Journal of Computational Physics 150, 97 127 (1999) Article ID jcph.1998.6165, available online at http://www.idealibrary.com on Weighted Essentially Non-oscillatory Schemes on Triangular Meshes 1 Changqing
More informationDonna Calhoun. Boise State University
Wave propagation algorithms in two dimensions, adaptive refinement and wellbalancing Donna Calhoun Boise State University PASI 2013 Valparaiso, Chile January 2-13 Plan How do these Riemann solvers make
More informationHigh Order Finite Difference and Finite Volume WENO Schemes and Discontinuous Galerkin Methods for CFD
NASA/CR-200-20865 ICASE Report No. 200- High Order Finite Difference and Finite Volume WENO Schemes and Discontinuous Galerkin Methods for CFD Chi-Wang Shu Brown University, Providence, Rhode Island ICASE
More informationOn the high order FV schemes for compressible flows
Applied and Computational Mechanics 1 (2007) 453-460 On the high order FV schemes for compressible flows J. Fürst a, a Faculty of Mechanical Engineering, CTU in Prague, Karlovo nám. 13, 121 35 Praha, Czech
More informationA new class of central compact schemes with spectral-like resolution II: Hybrid weighted nonlinear schemes. Abstract
A new class of central compact schemes with spectral-like resolution II: Hybrid weighted nonlinear schemes Xuliang Liu 1, Shuhai Zhang, Hanxin Zhang 3 and Chi-Wang Shu 4 Abstract In this paper, we develop
More informationi.e. variable extrapolation along the characteristic propagation directions. This leads to a family of rst and second-order accurate schemes with an i
Cell-centered Genuinely Multidimensional Upwind Algorithms and Structured Meshes P. Van Ransbeeck, Ch. Hirsch Department of Fluid Mechanics Vrije Universiteit Brussel Brussels, Belgium A family of cell-centered
More informationTutorial: Heat and Mass Transfer with the Mixture Model
Tutorial: Heat and Mass Transfer with the Mixture Model Purpose The purpose of this tutorial is to demonstrate the use of mixture model in FLUENT 6.0 to solve a mixture multiphase problem involving heat
More informationA Technique of Treating Negative Weights in WENO Schemes
NASA/CR--63 ICASE Report No. -49 A Technique of Treating Negative Weights in WENO Schemes Jing Shi, Changqing Hu, and Chi-Wang Shu Brown University, Providence, Rhode Island ICASE NASA Langley Research
More informationNavier-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 informationDivergence-Free Smoothed Particle Hydrodynamics
Copyright of figures and other materials in the paper belongs to original authors. Divergence-Free Smoothed Particle Hydrodynamics Bender et al. SCA 2015 Presented by MyungJin Choi 2016-11-26 1. Introduction
More informationThis tutorial illustrates how to set up and solve a problem involving solidification. This tutorial will demonstrate how to do the following:
Tutorial 22. Modeling Solidification Introduction This tutorial illustrates how to set up and solve a problem involving solidification. This tutorial will demonstrate how to do the following: Define a
More informationPiTP Summer School 2009
PiTP Summer School 2009 Plan for my lectures Volker Springel Lecture 1 Basics of collisionless dynamics and the N-body approach Lecture 2 Gravitational solvers suitable for collisionless dynamics, parallelization
More informationSimulation of Flow Development in a Pipe
Tutorial 4. Simulation of Flow Development in a Pipe Introduction The purpose of this tutorial is to illustrate the setup and solution of a 3D turbulent fluid flow in a pipe. The pipe networks are common
More information