'Shallow water equations' presentation slideshows

Secrets of Supercomputing The Conservation Laws Supercomputing Challenge Kickoff October 21-23, 2007

LA-UR-07-6793 Approved for public release; distribution is unlimited. Secrets of Supercomputing The Conservation Laws Supercomputing Challenge Kickoff October 21-23, 2007. I. Background to Supercomputing II. Get Wet! With the Shallow Water Equations Bob Robey - Los Alamos National Laboratory

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I. Background to Supercomputing II. Get Wet! With the Shallow Water Equations

LA-UR-07-6793 Approved for public release; distribution is unlimited. Secrets of Supercomputing The Conservation Laws Supercomputing Challenge Kickoff October 21-23, 2007. I. Background to Supercomputing II. Get Wet! With the Shallow Water Equations Bob Robey - Los Alamos National Laboratory

524 views • 52 slides

MSc Module MTMW14: met.rdg.ac.uk/cag/courses Numerical modelling of atmospheres and oceans

MSc Module MTMW14: www.met.rdg.ac.uk/cag/courses Numerical modelling of atmospheres and oceans. The Basics 1.1 Introduction 1.2 Brief history of numerical weather prediction 1.3 Dynamical equations for the unforced fluid. 1.1 Introduction : Aims of this course.

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MSc Module MTMW14 : Numerical modelling of atmospheres and oceans

MSc Module MTMW14 : Numerical modelling of atmospheres and oceans. Lecture plan for week 1: 1.1 Introduction 1.2 Brief history of numerical weather prediction 1.3 Dynamical equations for the unforced fluid. 1.1 Introduction : Aims of this course.

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Governing Equations IV

Governing Equations IV. by Nils Wedi (room 007; ext. 2657). Thanks to Piotr Smolarkiewicz , Glen Shutts and Peter Bechtold. Introduction and motivation. How do we treat artificial and/or natural boundaries and how do these influence the solution ?

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Governing Equations II: classical approximations and other systems of equations

Governing Equations II: classical approximations and other systems of equations. By Sylvie Malardel (room 10a; ext. 2414) after Nils Wedi (room 007; ext. 2657). Thanks to Clive Temperton, Mike Cullen and Piotr Smolarkiewicz. The continuous set of dry adiabatic equations.

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Real-time Simulations of Bubbles and Foam within a Shallow Water Framework

Real-time Simulations of Bubbles and Foam within a Shallow Water Framework. ?? ??? ???? ??? ??? 2008.3.13. ??. Abstract Introduction Related Work Overview The Shallow Water Equations Simulating Bubbles Spherical vortices Shallow Water Coupling Coalescence and Surface Animation

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345 views • 34 slides

031,02-11-09,TID

Far-field Effects of Tidal Energy Extraction in Puget Sound. ME 523: Energy and Environment Seminar. February 11, 2008. Brian Polagye PhD Candidate University of Washington Department of Mechanical Engineering. 031,02-11-09,TID. Tidal Energy in Puget Sound Modeling Extraction Effects

557 views • 30 slides

Numerical Simulation of Wave-Seawall Interaction

Numerical Simulation of Wave-Seawall Interaction. Clive Mingham, Derek Causon, David Ingram and Stephen Richardson C entre for M athematical M odelling and F low A nalysis, Manchester Metropolitan University, UK. Outline. Background Experimental set up Numerical simulation

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A Look at High-Order Finite-Volume Schemes for Simulating Atmospheric Flows

A Look at High-Order Finite-Volume Schemes for Simulating Atmospheric Flows. Paul Ullrich University of Michigan. Next Generation Climate Models. High-order accurate Move away from latitude-longitude grids Utilize modern hardware (GPUs, Petascale computing) Adaptive mesh refinement?.

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CHAPTER 1: FELIX M. EXNER AND THE ORIGINS OF MORPHODYNAMICS

CHAPTER 1: FELIX M. EXNER AND THE ORIGINS OF MORPHODYNAMICS.

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CHAPTER 1: FELIX M. EXNER AND THE ORIGINS OF MORPHODYNAMICS

CHAPTER 1: FELIX M. EXNER AND THE ORIGINS OF MORPHODYNAMICS.

451 views • 18 slides

CHAPTER 1: FELIX M. EXNER AND THE ORIGINS OF MORPHODYNAMICS

CHAPTER 1: FELIX M. EXNER AND THE ORIGINS OF MORPHODYNAMICS.

348 views • 18 slides

Modelling & Simulation An Introduction

Model A model is a simplified representation of a system at some particular point in time or space intended to promote understanding of the real system. Simulation

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Introduction to geophysical fluid dynamics

Introduction to geophysical fluid dynamics. Lecture I of VI ( C laudio Piani ) Course philosophy , the Navier -Stokes equations, Shallow Water, pressure gradient force, material derivative, continuity, linearization. 2. Course Philosophy .

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I m p a c t o f w i n d o n n a v i g a t i o n

I m p a c t o f w i n d o n n a v i g a t i o n. # W i n d w a v e . . .

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A Look at Two Tsunamis on the BC Coast with the Neptune-Canada Tsunami-meters

A Look at Two Tsunamis on the BC Coast with the Neptune-Canada Tsunami-meters. Richard Thomson (PI-IOS) Isaac Fine (Modelling-IOS) Alexander Rabinovich (Long Waves-IOS) Martin Heeseman (PGC) Earl Davis (PGC) Maxim Krassovski (IOS) NEPTUNE Science DMAS Team Steven Mihaly (IOS).

180 views • 9 slides

Spilling breaker over a beach shelf

Spilling breaker over a beach shelf. Michael Fong. 1D-version of the shallow water equations. Boundary conditions: free for H and UH Initial conditions: Gaussian waveform Topography: slope up to 2 m deep shallow shelf: 1 mm deep. Run with spilling_breaker.m.

97 views • 3 slides