1 Challenge the future Steel ball dropped into very fine sand (YouTube)

Slides:



Advertisements
Similar presentations
Continuum Simulation Monday, 9/30/2002. Class Progress Visualization: abstract concept (stress,2D, 3D), mechanical field Stochastic simulations: random.
Advertisements

Transfer coefficient algorithm for small mass nodes in material point method Xia Ma, Balaji Jayaraman, Paul T. Giguere and Duan Z. Zhang CartaBlanca Team.
ASME-PVP Conference - July
Workshop on Numerical Methods for Multi-material Fluid Flows, Prague, Czech Republic, September 10-14, 2007 Sandia is a multiprogram laboratory operated.
By: Rachel Sorna and William weinlandt
1 Numerical Simulation for Flow in 3D Highly Heterogeneous Fractured Media H. Mustapha J. Erhel J.R. De Dreuzy H. Mustapha INRIA, SIAM Juin 2005.
Chapter 8 Elliptic Equation.
By Paul Delgado. Motivation Flow-Deformation Equations Discretization Operator Splitting Multiphysics Coupling Fixed State Splitting Other Splitting Conclusions.
Pore-Pressure Generation During CPT Probe Advancement By Michael Fitzgerald.
STRESS ANALYSIS OF MULTIPLY FRACTURED POROUS ROCKS Exadaktylos, G. & Liolios P. TUC) ENK , 3F-Corinth, WP5, Task 5.2, Technical University Crete.
Dr. Kirti Chandra Sahu Department of Chemical Engineering IIT Hyderabad.
“LIQUEFACTION” Prepared By: Husni M. Awwad Talal Z. Zammar
LECTURE SERIES on STRUCTURAL OPTIMIZATION Thanh X. Nguyen Structural Mechanics Division National University of Civil Engineering
Session: Computational Wave Propagation: Basic Theory Igel H., Fichtner A., Käser M., Virieux J., Seriani G., Capdeville Y., Moczo P.  The finite-difference.
A Study of Flow in a Corrugated Channel Xin Kai Li Institute of Simulation Sciences De Montfort University Leicester UK.
Finite-Element-Based Characterisation of Pore- scale Geometry and its Impact on Fluid Flow Lateef Akanji Supervisors Prof. Martin Blunt Prof. Stephan Matthai.
FEM and X-FEM in Continuum Mechanics Joint Advanced Student School (JASS) 2006, St. Petersburg, Numerical Simulation, 3. April 2006 State University St.
Advanced Computer Graphics (Fall 2010) CS 283, Lecture 23: Physical Simulation 2 Ravi Ramamoorthi Most slides.
The problem to be solved is specified in a) the physical domain and b) the discretized domain used by FEA Governing principle law :
CHE/ME 109 Heat Transfer in Electronics LECTURE 12 – MULTI- DIMENSIONAL NUMERICAL MODELS.
Finite Element Method in Geotechnical Engineering
A Concept of Environmental Forecasting and Variational Organization of Modeling Technology Vladimir Penenko Institute of Computational Mathematics and.
Lecture 34 - Ordinary Differential Equations - BVP CVEN 302 November 28, 2001.
Numerical modeling of rock deformation: 13 FEM 2D Viscous flow
Finite Difference Methods to Solve the Wave Equation To develop the governing equation, Sum the Forces The Wave Equation Equations of Motion.
© 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the.
Introduction to virtual engineering László Horváth Budapest Tech John von Neumann Faculty of Informatics Institute of Intelligent Engineering.
The Finite Element Method A Practical Course
Variants of the 1D Wave Equation Jason Batchelder 6/28/07.
Haptics and Virtual Reality
EVALUATION OF A FAST NUMERICAL SOLUTION OF THE 1D RICHARD’S EQUATION AND INCLUSION OF VEGETATION PROCESSES Varado N., Ross P.J., Braud I., Haverkamp R.,
PDE simulations with adaptive grid refinement for negative streamers in nitrogen Carolynne Montijn Work done in cooperation with: U. Ebert W. Hundsdorfer.
Solution techniques Martin Ellison University of Warwick and CEPR Bank of England, December 2005.
Ale with Mixed Elements 10 – 14 September 2007 Ale with Mixed Elements Ale with Mixed Elements C. Aymard, J. Flament, J.P. Perlat.
The Configuration Factors between Ring Shape Finite Areas in Cylinders and Cones Cosmin DAN, Gilbert DE MEY.
HEAT TRANSFER FINITE ELEMENT FORMULATION
Mallett Technology, Inc.
Effect of nonlinearity on Head-Tail instability 3/18/04.
MODAL ANALYSIS OF DISCRETE SDOF SYSTEMS 1. Linear spring N/m Model file1DOF.SLDASM MaterialAISI 1020 RestraintsFixed base Restraints preventing.
Material Point Method Solution Procedure Wednesday, 10/9/2002 Map from particles to grid Interpolate from grid to particles Constitutive model Boundary.
Numerical methods 1 An Introduction to Numerical Methods For Weather Prediction by Mariano Hortal office 122.
G Z Mentor: Bill Kells Investigating a Parametric Instability in the LIGO Test Masses Hans Bantilan (Carleton College) for the LIGO Scientific.
Simple numerical scheme for modelling of nonlinear pulse propagation in coupled microring resonators Anna Sterkhova, Jiří Petráček, Jaroslav Luksch ICTON.
25-26 January Bochum, Germany Luc Hantcherli - Philip Eisenlohr - Franz Roters – Dierk Raabe and Collaboration between: Mechanical twinning in crystal.
14 - finite element method
/14:00 1 Literature Study Jeroen Wille.
Stability Investigation of a Difference Scheme for Incompressible Navier—Stokes Equations D. Chibisov, V. Ganzha, E.W. Mayr, E.V. Vorozhtsov.
Finite element mesh and load definition
CHAPTER 2 - EXPLICIT TRANSIENT DYNAMIC ANALYSYS
Finite Element Method in Geotechnical Engineering
Convection-Dominated Problems
The DisCrete-Continual Finite Element Method in Engineering
Simple FD Gerard T. Schuster.
Prof. Pavel A. Akimov, Prof. Marina L. Mozgaleva
Mechanical Engineering at Virginia Tech
Tarmat Layer Geo-mechanical Behavior under Producing Oilfield
Deflated Conjugate Gradient Method
John Drozd Colin Denniston
Implementation of 2D stress-strain Finite Element Modeling on MATLAB
Solutions of the Schrödinger equation for the ground helium by finite element method Jiahua Guo.
What is the future of applied mathematics? Chris Budd.
Your Title Goes Here, All Words With Three or More Letters Capitalized
By Heather Huenison and Allan Dolovich University of Saskatchewan
Analytical Tools in ME Course Objectives
Konferanse i beregningsorientert mekanikk, Trondheim, Mai, 2005
Objective Numerical methods Finite volume.
Finite elements Pisud Witayasuwan.
Linear strain triangular Tieme Willems
Apply discontinous Galerkin method to Einstein equations
Continuum Simulation Monday, 9/30/2002.
Presentation transcript:

1 Challenge the future Steel ball dropped into very fine sand (YouTube)

2 Challenge the future Simulation of sphere being shot into clay-like material (Al-Kafaji)

3 Challenge the future Stability analysis of a simplified 2-phase formulation in Geomechanics Miriam Mieremet Thursday, 8 January 2015

4 Challenge the future Content 1.Problem: Numerical instability with 2-phase MPM 2.Approach: Simplifications and methods 3.Study: Stability analysis with simplified 2-phase FEM 4.Conclusion 5.Outlook

5 Challenge the future Problem: Numerical instability with 2-phase MPM Cone Penetration Test (myv-sg.nl)

6 Challenge the future Numerical instability with 2-phase MPM 2-phase continuum Solid phase Water phase

7 Challenge the future 2-phase formulation Numerical instability with 2-phase MPM

8 Challenge the future Numerical instability with 2-phase MPM Material Point Method & Euler Cromer Method Initial configuration Calculation stepResetting the mesh

9 Challenge the future Numerical instability with 2-phase MPM Simulation of CPT with MPM (Ceccato) Stability Criterion 1-phase Unexpected instability 2-phase High permeability: Stable Low permeability: Unstable What is the right stability criterion?

10 Challenge the future Approach: Simplifications and methods

11 Challenge the future Simplifications and methods Problem:Study: Large deformationsSmall deformations Three dimensionsOne dimension 2-phaseSimplified 2-phase

12 Challenge the future Problem:Study: MPMFEM Tetrahedral elementsLinear elements Simplifications and methods

13 Challenge the future Stability analysis Von Neumann Method Matrix Method Simplifications and methods

14 Challenge the future Study: Stability analysis with simplified 2-phase FEM Oedometer Test

15 Challenge the future Variables velocity of solid phase velocity of water phase effective stress pore pressure Stability analysis with simplified 2-phase FEM

16 Challenge the future 2-phase formulation Stability analysis with simplified 2-phase FEM

17 Challenge the future Simplified 2-phase formulation Stability analysis with simplified 2-phase FEM

18 Challenge the future Finite Element space discretization Stability analysis with simplified 2-phase FEM

19 Challenge the future Euler Cromer time discretization Stability analysis with simplified 2-phase FEM

20 Challenge the future Von Neumann Method Space discretization Time discretization Error equation Fourier decomposition Stability analysis with simplified 2-phase FEM

21 Challenge the future Stability analysis with simplified 2-phase FEM Stability criterion Amplitude equation

22 Challenge the future Matrix Method Space discretization Error equation Eigenvalue decomposition Time discretization Stability analysis with simplified 2-phase FEM

23 Challenge the future Stability analysis with simplified 2-phase FEM Stability criterion Error equation

24 Challenge the future Stability analysis with simplified 2-phase FEM Compare analytical and numerical solution with

25 Challenge the future Stability analysis with simplified 2-phase FEM Compare analytical and numerical solution with

26 Challenge the future Conclusion Familiarization with geomechanical problems Investigation of 1- and 2-phase formulation Implementation in Matlab Literature study on stability analysis

27 Challenge the future Conclusion Stability criterion for simplified 2-phase FEM:

28 Challenge the future Outlook Stability analysis with 2-phase FEM (1D) Stability analysis with 2-phase FEM (3D) Study impact of…  Local Damping  Mass Scaling  Strain smoothening Introduction of stability criterion into Deltares MPM code