Hydraulic Fracture: multiscale processes and moving interfaces Anthony Peirce Department of Mathematics University of British Columbia WORKSHOP ON ROCK.

Slides:



Advertisements
Similar presentations
Stable Fluids A paper by Jos Stam.
Advertisements

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.
Lecture 1. How to model: physical grounds
By Paul Delgado. Motivation Flow-Deformation Equations Discretization Operator Splitting Multiphysics Coupling Fixed State Splitting Other Splitting Conclusions.
DEBRIS FLOWS & MUD SLIDES: A Lagrangian method for two- phase flow simulation Matthias Preisig and Thomas Zimmermann, Swiss Federal Institute of Technology.
Numerical Method for Computing Ground States of Spin-1 Bose-Einstein Condensates Fong Yin Lim Department of Mathematics and Center for Computational Science.
Multilevel Incomplete Factorizations for Non-Linear FE problems in Geomechanics DMMMSA – University of Padova Department of Mathematical Methods and Models.
Hydraulic Fracture: multiscale processes and moving interfaces Anthony Peirce Department of Mathematics University of British Columbia Nanoscale Material.
LES Continuity Equation Residual Stress Residual Stress Tensor Anisotropic residual stress tensor Residual kinetic energy Filtered pressure.
1 MODELING OF HYDRAULIC FRACTURES. 2 HYDRAULIC FRACTURES Hydraulic fracturing can be broadly defined as the process by which a fracture initiates and.
Computational Solutions of Helmholtz Equation Yau Shu Wong Department of Mathematical & Statistical Sciences University of Alberta Edmonton, Alberta, Canada.
12/21/2001Numerical methods in continuum mechanics1 Continuum Mechanics On the scale of the object to be studied the density and other fluid properties.
One dimensional models of hydraulic fracture Anthony Peirce (UBC) Collaborators: Jose` Adachi (SLB) Shira Daltrop (UBC) Emmanuel Detournay (UMN) WITS University.
Network and Grid Computing –Modeling, Algorithms, and Software Mo Mu Joint work with Xiao Hong Zhu, Falcon Siu.
Fluvial Landscape Erosion Kirsten Meeker, Bjorn Birnir, Terence Smith, George Merchant
Iterative Solvers for Coupled Fluid-Solid Scattering Jan Mandel Work presentation Center for Aerospace Structures University of Colorado at Boulder October.
Computations of Fluid Dynamics using the Interface Tracking Method Zhiliang Xu Department of Mathematics University of Notre.
A phase field model for binary fluid-surfactant system
Rajai1 y b. 2 APPLICATIONS v Heat and mass transfer rates are enhanced by the oscillation of the surrounding fluid. Useful in combustion, drying and the.
FUNDAMENTAL EQUATIONS, CONCEPTS AND IMPLEMENTATION
Stirling-type pulse-tube refrigerator for 4 K
Multigrid for Nonlinear Problems Ferien-Akademie 2005, Sarntal, Christoph Scheit FAS, Newton-MG, Multilevel Nonlinear Method.
Material point method simulation
60th Annual Meeting Division of Fluid Dynamics A multiscale approach to study the stability of long waves in near-parallel flows S. Scarsoglio #, D.Tordella.
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.
6. Elastic-Plastic Fracture Mechanics
ParCFD Parallel computation of pollutant dispersion in industrial sites Julien Montagnier Marc Buffat David Guibert.
CFD Lab - Department of Engineering - University of Liverpool Ken Badcock & Mark Woodgate Department of Engineering University of Liverpool Liverpool L69.
Efficient Integration of Large Stiff Systems of ODEs Using Exponential Integrators M. Tokman, M. Tokman, University of California, Merced 2 hrs 1.5 hrs.
The role of boundary layers in the large-scale ocean circulation Laure Saint-Raymond ENS & Université Paris 6.
Two Dimensional Hydraulic Fracture Simulations Using FRANC2D
Modeling of Materials Processes using Dimensional Analysis and Asymptotic Considerations Patricio Mendez, Tom Eagar Welding and Joining Group Massachusetts.
Cavitation Models Roman Samulyak, Yarema Prykarpatskyy Center for Data Intensive Computing Brookhaven National Laboratory U.S. Department of Energy
Stirling-type pulse-tube refrigerator for 4 K M. Ali Etaati CASA-Day April 24 th 2008.
Order of Magnitude Scaling of Complex Engineering Problems Patricio F. Mendez Thomas W. Eagar May 14 th, 1999.
Web-based Class Project on Rock Mechanics REPORT PREPARED AS PART OF COURSE CEE 544: ROCK MECHANICS WINTER 2015 SEMESTER INSTRUCTOR: PROFESSOR DIMITRIOS.
Ale with Mixed Elements 10 – 14 September 2007 Ale with Mixed Elements Ale with Mixed Elements C. Aymard, J. Flament, J.P. Perlat.
1 Point-implicit diffusion operator in a moving particle method (MPPM) Yao-Hsin Hwang Department of Marine Engineering National Kaohsiung Marine University.
Large deflection of a supercavitating hydrofoil
The Materials Computation Center, University of Illinois Duane Johnson and Richard Martin (PIs), NSF DMR Time and spacetime finite.
1 Instituto Tecnológico de Aeronáutica Prof. Maurício Vicente Donadon AE-256 Lecture notes: Prof. Maurício V. Donadon NUMERICAL METHODS IN APPLIED STRUCTURAL.
An Integrated Hydrodynamic Approach to River, Sewer and Overland Flow Modelling presented by Andrew Walker Innovyze Ltd.
A Dirichlet-to-Neumann (DtN)Multigrid Algorithm for Locally Conservative Methods Sandia National Laboratories is a multi program laboratory managed and.
Governing Equations Conservation of Mass Conservation of Momentum Velocity Stress tensor Force Pressure Surface normal Computation Flowsheet Grid values.
Controlled CO 2 | Diversified Fuels | Fuel-efficient Vehicles | Clean Refining | Extended Reserves © IFP IEA Collaborative Project on EOR - 30th Annual.
A novel approach for thermomechanical analysis of stationary rolling tires within an ALE-kinematic framework A. Suwannachit and U. Nackenhorst Institute.
A Numerical Solution to the Flow Near an Infinite Rotating Disk White, Section MAE 5130: Viscous Flows December 12, 2006 Adam Linsenbardt.
MULTIFUNCTIONAL COLLABORATIVE MODELING AND ANALYSIS METHODS IN ENGINEERING SCIENCE Jonathan B. Ransom NASA Langley Research Center Mail Stop 240, Hampton,
Klein-Gordon Equation in the Gravitational Field of a Charged Point Source D.A. Georgieva, S.V. Dimitrov, P.P. Fiziev, T.L. Boyadjiev Gravity, Astrophysics.
SPH weekly meeting Free surface flows in Code Saturne Results 23/11/2009 Olivier Cozzi.
F. Fairag, H Tawfiq and M. Al-Shahrani Department of Math & Stat Department of Mathematics and Statistics, KFUPM. Nov 6, 2013 Preconditioning Technique.
M. Khalili1, M. Larsson2, B. Müller1
Topic 3: Constitutive Properties of Tissues
Institute of Mechanics and Advanced Materials An Adaptive Multiscale Method for Modelling of Fracture in Polycrystalline Materials Ahmad Akbari R., Pierre.
Algorithm of the explicit type for porous medium flow simulation
Convection-Dominated Problems
Transient Mixed Flow Modeling Capability in SRH-2D for Culverts and Bridges Yong G. Lai.
From: Toughness-Dominated Hydraulic Fracture in Permeable Rocks
I-2. Power Method and Wielandt Shift II. Multigroup Neutron Diffusion
Convergence in Computational Science
Meros: Software for Block Preconditioning the Navier-Stokes Equations
Robert Shuttleworth Applied Math & Scientific Computation (AMSC)
Adaptive Grid Generation for Magnetically Confined Plasmas
John Drozd Colin Denniston
Numerics for PDE using EXCEL
Konferanse i beregningsorientert mekanikk, Trondheim, Mai, 2005
Objective Numerical methods Finite volume.
L.V. Stepanova Samara State University
What are Multiscale Methods?
Presentation transcript:

Hydraulic Fracture: multiscale processes and moving interfaces Anthony Peirce Department of Mathematics University of British Columbia WORKSHOP ON ROCK MECHANICS AND LOGISTICS IN MINING February 26, 2007 Collaborators: Jose` Adachi (SLB, Houston) Rachel Kuske (UBC) Sarah Mitchell (UBC) Ed Siebrits (SLB, Houston)

2 Outline What is a hydraulic fracture? Mathematical models of hydraulic fracture Scaling and special solutions for 1-2D models Numerical modeling for 2-3D problems Conclusions

3 HF Examples - block caving

4 HF Example – caving (Jeffrey, CSIRO)

5 HF Examples – well stimulation

6 Model EQ 1: Conservation of mass

7 1-2D model and physical processes Fracture Energy Breaking rock Leak-off Viscous energy loss

8 Scaling and dimensionless quantities Rescale: Dimensionless quantities: Governing equations become:

9 Toughness dominated propagation Asymptotic behaviour of the Hilbert transform Large toughness:

10 Viscosity dominated propagation Asymptotic behaviour of the Hilbert transform Large viscosity:

11 HF experiment (Bunger & Jeffrey CSIRO)

12 2-3D HF Equations Elasticity Lubrication Boundary conditions at moving front (non-locality) (free boundary) (non-linearity)

13 Coupled equations – a model problem nn-1n-2n+1n+2 Elasticity Fluid Flow

14 Conditioning of the Jacobian Evolution equation for w: Eigenvalues of AC: Explicit Scheme Use implicit time stepping

15 General first order iterative method Consider solving: using the iterative method Residual errors are damped according to

16 Damping factor Poorly Damped Well Damped

17 Multigrid Methods

18 MG approach for coupled HF Equations

19 MG preconditioning of C coarsening using dual mesh Localized GS smoother

20 Performance of MG Preconditioner ~9.5 x

21 Incomplete LU factorization function [A] = lu(A) [n,n]=size(A); for j=1:n for k=1:j-1 for i=k+1:n A(i,j)=A(i,j)-A(i,k)*A(k,j); end for i=j+1:n A(i,j)=A(i,j)/A(j,j); end return function [A] = basicILUc(A) [n,n]=size(A); for j=1:n for k=1:j-1 if A(k,j) ~=0, for i=k+1:n if A(i,j) ~=0, A(i,j)=A(i,j)-A(i,k)*A(k,j); end for i=j+1:n if A(i,j) ~=0, A(i,j)=A(i,j)/A(j,j); end return

22 Local Jacobian & Fourier Analysis nn-1n-2n+1n+2 Elasticity Fluid Flow

23 Spectrum of AC (AC Loc ) -1

24 Eigenvalues of preconditioners

25 Numerical results for stress jump

26 Numerical results for stress jump

27 Front evolution via the VOF method

28 Time stepping and front evolution Time step loop: VOF loop: Coupled Solution end next VOF iteration next time step

29 Radial Solution

30 Fracture width for modulus contrast Modulus Changes Source

31 Fracture width for stress jump

32 Pressure and width evolution

33 Channel fracture & pinch region

34 Hourglass HF with leakoff

35 Concluding remarks Examples of hydraulic fractures Scaling and physical processes in 1D models  Tip asymptotics: & Numerical models of 2-3D hydraulic fractures  The non-local, nonlinear & free boundary problem  An Eulerian approach and the coupled equations  A multigrid algorithm for the coupled problem  ILU Factorization for the Localized Jacobian  Front evolution via the VOF method Numerical results