Accurate Numerical Treatment of the Source Terms in the Non-linear Shallow Water Equations J.G. Zhou, C.G. Mingham, D.M. Causon and D.M. Ingram Centre.

Slides:



Advertisements
Similar presentations
PARMA UNIVERSITY SIMULATIONS OF THE ISOLATED BUILDING TEST CASE F. AURELI, A. MARANZONI & P. MIGNOSA DICATeA, Parma University Parco Area delle Scienze.
Advertisements

Finite Volume II Philip Mocz. Goals Construct a robust, 2nd order FV method for the Euler equation (Navier-Stokes without the viscous term, compressible)
1 A new iterative technique for solving nonlinear coupled equations arising from nuclear waste transport processes H. HOTEIT 1,2, Ph. ACKERER 2, R. MOSE.
RAMS/BRAMS Basic equations and some numerical issues.
Numerical Simulation of Wave-Seawall Interaction Clive Mingham, Derek Causon, David Ingram and Stephen Richardson Centre for Mathematical Modelling and.
Fluidyn FLOWCOAST FLOOIL 3D Fluid Dynamics Model to Simulate Oil slick movement in coastal waters or rivers FLOOIL.
Numerical Simulation of Benchmark Problem 2
July 11, 2006 Comparison of Exact and Approximate Adjoint for Aerodynamic Shape Optimization ICCFD 4 July 10-14, 2006, Ghent Giampietro Carpentieri and.
Numerical Relativistic Hydrodynamics Luciano Rezzolla SISSA, International School for Advanced Studies, Trieste INFN, Department of Physics, University.
1 Internal Seminar, November 14 th Effects of non conformal mesh on LES S. Rolfo The University of Manchester, M60 1QD, UK School of Mechanical,
Combining the strengths of UMIST and The Victoria University of Manchester Aspects of Transitional flow for External Applications A review presented by.
Shallow water equations in 1D: Method of characteristics
Use of satellite altimeter data for validating large scale hydraulic models Matt Wilson, University of Exeter Doug Alsdorf, Ohio State University Paul.
Knut Vaagsaether, Vegeir Knudsen and Dag Bjerketvedt
1/36 Gridless Method for Solving Moving Boundary Problems Wang Hong Department of Mathematical Information Technology University of Jyväskyklä
Modeling Fluid Phenomena -Vinay Bondhugula (25 th & 27 th April 2006)
Computations of Fluid Dynamics using the Interface Tracking Method Zhiliang Xu Department of Mathematics University of Notre.
A TWO-FLUID NUMERICAL MODEL OF THE LIMPET OWC CG Mingham, L Qian, DM Causon and DM Ingram Centre for Mathematical Modelling and Flow Analysis Manchester.
Numerical Schemes for Advection Reaction Equation Ramaz Botchorishvili Faculty of Exact and Natural Sciences Tbilisi State University GGSWBS,Tbilisi, July.
A finite volume solution method for thermal convection in a spherical shell with strong temperature- und pressure-dependent viscosity CIG Workshop 2005.
CHAPTER 8 APPROXIMATE SOLUTIONS THE INTEGRAL METHOD
© 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the.
FUNDAMENTAL EQUATIONS, CONCEPTS AND IMPLEMENTATION
Tutorial 5: Numerical methods - buildings Q1. Identify three principal differences between a response function method and a numerical method when both.
© Fluent Inc. 9/5/2015L1 Fluids Review TRN Solution Methods.
© Arturo S. Leon, BSU, Spring 2010
Numerical study of wave and submerged breakwater interaction (Data-driven and Physical-based Model for characterization of Hydrology, Hydraulics, Oceanography.
Hybrid WENO-FD and RKDG Method for Hyperbolic Conservation Laws
A Look at High-Order Finite- Volume Schemes for Simulating Atmospheric Flows Paul Ullrich University of Michigan.
Modelling Hydrodynamical Processes of the Pacific Ocean Littoral and the Amur River (the Far Eastern Region of Russia) K. A. Chekhonin Resheach Institute.
A Hybrid Particle-Mesh Method for Viscous, Incompressible, Multiphase Flows Jie LIU, Seiichi KOSHIZUKA Yoshiaki OKA The University of Tokyo,
Solution of the St Venant Equations / Shallow-Water equations of open channel flow Dr Andrew Sleigh School of Civil Engineering University of Leeds, UK.
C M C C Centro Euro-Mediterraneo per i Cambiamenti Climatici COSMO General Meeting - September 8th, 2009 COSMO WG 2 - CDC 1 An implicit solver based on.
Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde How to make a three-dimensional numerical model that.
A Novel Wave-Propagation Approach For Fully Conservative Eulerian Multi-Material Simulation K. Nordin-Bates Lab. for Scientific Computing, Cavendish Lab.,
A conservative FE-discretisation of the Navier-Stokes equation JASS 2005, St. Petersburg Thomas Satzger.
Numerical Schemes for Streamer Discharges at Atmospheric Pressure
Governing equations: Navier-Stokes equations, Two-dimensional shallow-water equations, Saint-Venant equations, compressible water hammer flow equations.
Discontinuous Galerkin Methods Li, Yang FerienAkademie 2008.
Approximate Riemann Solvers for Multi-component flows Ben Thornber Academic Supervisor: D.Drikakis Industrial Mentor: D. Youngs (AWE) Aerospace Sciences.
Discontinuous Galerkin Methods for Solving Euler Equations Andrey Andreyev Advisor: James Baeder Mid.
7. Introduction to the numerical integration of PDE. As an example, we consider the following PDE with one variable; Finite difference method is one of.
The Governing Equations The hydrodynamic model adopted here is the one based on the hydrostatic pressure approximation and the boussinesq approximation,
J.-Ph. Braeunig CEA DAM Ile-de-FrancePage 1 Jean-Philippe Braeunig CEA DAM Île-de-France, Bruyères-le-Châtel, LRC CEA-ENS Cachan
MIKE 11 IntroductionNovember 2002Part 1 Introduction to MIKE 11 Part 1 General Hydrodynamics within MIKE 11 –Basic Equations –Flow Types Numerical Scheme.
© IFP Controlled CO 2 | Diversified fuels | Fuel-efficient vehicles | Clean refining | Extended reserves Écrire ici dans le masque le nom de votre Direction.
COMPUTATIONAL FLUID DYNAMICS (AE 2402) Presented by IRISH ANGELIN S AP/AERO.
FALL 2015 Esra Sorgüven Öner
AMS 691 Special Topics in Applied Mathematics Lecture 8
Discretization Methods Chapter 2. Training Manual May 15, 2001 Inventory # Discretization Methods Topics Equations and The Goal Brief overview.
The Islamic University of Gaza Faculty of Engineering Civil Engineering Department EENV 5326 Groundwater Modeling.
DIMENSIONAL ANALYSIS SECTION 5.
CHANGSHENG CHEN, HEDONG LIU, And ROBERT C. BEARDSLEY
School of Aerospace Engineering MITE Numerical Simulation of Centrifugal Compressor Stall and Surge Saeid NiaziAlex SteinLakshmi N. Sankar School of Aerospace.
Bone Ingrowth in a shoulder prosthesis E.M.van Aken, Applied Mathematics.
X = 2 + t y = t t = x – 2 t = (y + 3)/2 x – 2 = y x – 4 = y + 3 y – 2x + 7 = 0 Finding the Cartesian Equation from a vector equation x = 2.
Implementing Finite Volume Methods 1.  Continue on Finite Volume Methods for Elliptic Equations  Finite Volumes in Two-Dimensions  Poisson’s Equation.
The shallow water equations in geomorphic modeling
Modelling of Marine Systems. Shallow waters Equations.
Computational Fluid Dynamics Lecture II Numerical Methods and Criteria for CFD Dr. Ugur GUVEN Professor of Aerospace Engineering.
Example application – Finite Volume Discretization Numerical Methods for PDEs Spring 2007 Jim E. Jones.
Xing Cai University of Oslo
Modeling of Traffic Flow Problems
A TWO-FLUID NUMERICAL MODEL OF THE LIMPET OWC
© Fluent Inc. 1/10/2018L1 Fluids Review TRN Solution Methods.
Discontinuous Shallow Flow
Finite Volume Method Philip Mocz.
High Accuracy Schemes for Inviscid Traffic Models
Instituto Superior Técnico instituto superior técnico
Presentation transcript:

Accurate Numerical Treatment of the Source Terms in the Non-linear Shallow Water Equations J.G. Zhou, C.G. Mingham, D.M. Causon and D.M. Ingram Centre for Mathematical Modelling and Flow Analysis Department of Computing and Mathematics Manchester Metropolitan University Chester Street, Manchester M1 5GD, U.K.

Outline Introduction Numerics Results Conclusions

Introduction Shallow water equations can be a good model for many flow situations e.g rivers, lakes, estuaries, near shore Realistic problems have variable bathymetry In conservative Godunov schemes it is difficult to balance flux gradients and source terms containing depth leading to errors Surface Gradient Method (SGM) developed to overcome difficulties

Surface Gradient Method Simpler than competitors (e.g Leveque, Vazquez-Cendon) Centred Discretisation Computationally efficient Accurate solutions for wide range of demanding problems e.g. transcritical flow with bores over bumps Solves SWE without source term splitting Can be extended to a Cartesian cut cell framework (AMAZON-CC)

Shallow Water Equations (inviscid) Conserved quantitiesFlux tensor g: acceleration due to gravity, h: water depth,  = g h, V = u i + v j velocity.

Source Terms bed slopewind shearbed friction

Numerical Scheme High resolution, Godunov type Conservative Finite volume (AMAZON-CC uses Cartesian cut cells for automatic boundary fitted mesh) Interface flux via MUSCL reconstruction Riemann flux by HLL approx Riemann solver Surface Gradient Method (SGM) for accurate source term discretisation

Numerical Scheme 1) Predictor: n: time level, i,j: cell index, m: cell side, A: cell area, L m : side vector, F(U m ) interface flux. : discretised source term 2-stage

MUSCL Reconstruction 1-D Cartesian,

Numerical Scheme 2) Corrector: : Riemann flux from HLL approximate Riemann solver

Surface Gradient Method Applying MUSCL to  gives, Uses  rather than h for reconstruction of 

Surface Gradient Method Bathymetry given at cell interfaces. To get required cell centre values assume piecewise linear, Bed slopes approximated by central difference, Scheme retains conservative property

AMAZON-CC Techniques are easily extended to Cartesian cut cell grids AMAZON-CC simulation of a landslide generated tsunami in a fjord

Results What about a 1-D picture v exact soln

Results Seawall modelled using bed slope (left) and solid boundary (right)

Results Fig 2 from Jingous’s paper wind induced circulation

Results Fig 4 from Jingou, overtop sea wall

Conclusions The Surface Gradient Method is a simple way to treat source terms within a conservative Godunov type scheme Results are good for a wide range of demanding test cases The method can be incorporated into a Cartesian cut cell framework (AMAZON-CC)