DYNAS Workshop 6,7,8/12/04 Mixed Hybrid Finite Element and Iterative Methods for Flow in Porous Media E. Mouche, C. Le Potier, P. Maugis, L.V. Benet. Commissariat.

Slides:



Advertisements
Similar presentations
1 A parallel software for a saltwater intrusion problem E. Canot IRISA/CNRS J. Erhel IRISA/INRIA Rennes C. de Dieuleveult IRISA/INRIA Rennes.
Advertisements

A parallel scientific software for heterogeneous hydrogeoloy
Yhd Subsurface Hydrology
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.
Infiltration and unsaturated flow Learning objective Be able to calculate infiltration, infiltration capacity and runoff rates using the methods described.
Journée Castem, 25/11/09 Simulation de l’injection de carbone dans un site géologique de séquestration du CO 2 Mohamed HAYEK, Emmanuel MOUCHE and Claude.
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.
1 Modélisation et simulation appliquées au suivi de pollution des nappes phréatiques Jocelyne Erhel Équipe Sage, INRIA Rennes Mesures, Modélisation et.
Stochastic Modeling of Multiphase Transport in Subsurface Porous Media: Motivation and Some Formulations Thomas F. Russell National Science Foundation,
A modified Lagrangian-volumes method to simulate nonlinearly and kinetically adsorbing solute transport in heterogeneous media J.-R. de Dreuzy, Ph. Davy,
z = -50 cm, ψ = -100 cm, h = z + ψ = -50cm cm = -150 cm Which direction will water flow? 25 cm define z = 0 at soil surface h = z + ψ = cm.
Hydrocarbon Migration Istvan Csato University of South Carolina Department of Geological Sciences Petroleum Geology Class 745 Spring 2002.
Features of POLLUSOL Flow model Flow model Homogeneous, Isotropic, Heterogeneous and Anisotropic medium Homogeneous, Isotropic, Heterogeneous and Anisotropic.
1 Miller Similarity and Scaling of Capillary Properties How to get the most out of your lab dollar by cheating with physics.
High performance flow simulation in discrete fracture networks and heterogeneous porous media Jocelyne Erhel INRIA Rennes Jean-Raynald de Dreuzy Geosciences.
Ground-Water Flow and Solute Transport for the PHAST Simulator Ken Kipp and David Parkhurst.
1 A component mode synthesis method for 3D cell by cell calculation using the mixed dual finite element solver MINOS P. Guérin, A.M. Baudron, J.J. Lautard.
Finite-Element-Based Characterisation of Pore- scale Geometry and its Impact on Fluid Flow Lateef Akanji Supervisors Prof. Martin Blunt Prof. Stephan Matthai.
Peyman Mostaghimi, Martin Blunt, Branko Bijeljic 11 th January 2010, Pore-scale project meeting Direct Numerical Simulation of Transport Phenomena on Pore-space.
1 Miller Similarity and Scaling of Capillary Properties How to get the most out of your lab dollar by cheating with physics.
D2011 Project CEA-IRSN Results Alain MILLARD, Frédéric DELERUYELLE Wakkanai, Japan, October 20-23, 2008 Task A - STEPS 0/1.
HYDRUS_1D Sensitivity Analysis Limin Yang Department of Biological Engineering Sciences Washington State University.
Status report on Step1 of Task A, DECOVALEX-2011 modeling for Ventilation Experiment –modeling for Ventilation Experiment By Xiaoyan Liu, Chengyuan Zhang.
Infiltration, Runoff and Stream flow Ali Fares, PhD Watershed Hydrology, NREM 691 UHM-CTAHR-NREM.
Modeling and simulation of deformable porous media Jan Martin Nordbotten Department of Mathematics, University of Bergen, Norway Department of Civil and.
Groundwater Hydraulics Daene C. McKinney
Direct and iterative sparse linear solvers applied to groundwater flow simulations Matrix Analysis and Applications October 2007.
1 Parallel Simulations of Underground Flow in Porous and Fractured Media H. Mustapha 1,2, A. Beaudoin 1, J. Erhel 1 and J.R. De Dreuzy IRISA – INRIA.
Density-Dependent Flows Primary source: User’s Guide to SEAWAT: A Computer Program for Simulation of Three-Dimensional Variable-Density Ground- Water Flow.
1 GROUNDWATER HYDROLOGY AND CONTAMINANT TRANSPORT CEVE 518 P.C. de Blanc C.J. Newell 1.Porosity and Density Continued 2.Saturation and Water Content 3.Darcy.
MODFLOW – Introduction Organization & Main Packages
Soil Water Reading: Applied Hydrology Sections 4.1 and 4.2 Topics
DYNAS 04 Workshop Ph. Ackerer, IMFS - STRASBOURG Some Difficulties in Modeling Water and Solute Transport in Soils Ph. ACKERER IMFS STRASBOURG
Unit 01 : Advanced Hydrogeology Review of Groundwater Flow Malcolm Reeves Civil and Geological Engineering.
CE 394K.2 Hydrology Infiltration Reading AH Sec 5.1 to 5.5 Some of the subsequent slides were prepared by Venkatesh Merwade.
Lecture Notes Applied Hydrogeology
CE 394K.2 Hydrology Infiltration Reading AH Sec 5.1 to 5.5 Some slides were prepared by Venkatesh Merwade Slides 2-6 come from
Figure (p. 235) (a) Cross-section through an unsaturated porous medium; (b) Control volume for development of the continuity equation in an unsaturated.
Darcy’s Law and Flow CIVE Darcy allows an estimate of: the velocity or flow rate moving within the aquifer the average time of travel from the head.
Surface Water Hydrology: Infiltration – Green and Ampt Method
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.,
1 Numerical simulation software LinkFEA Iris Summer Academy 2011 Mengxi WU Institue of Mechanics,CAS 04\09\2011 (WP4)
CE 394K.2 Hydrology Infiltration Reading for Today: AH Sec 4.3 and 4.4 Reading for Thurs: AH Sec 5.1 to 5.5 Subsequent slides prepared by Venkatesh Merwade.
GROUND WATER CONTAMINATION. IMPORTANCE OF GROUND WATER Approximately 99 percent of all liquid fresh water is in underground aquifers At least a quarter.
Geometry Group Summer 08 Series Toon Lenaerts, Bart Adams, and Philip Dutre Presented by Michael Su May
Journées Scientifiques du GNR MOMAS, novembre 2009DM2S/SFME/LSET 1 MPCube Development Ph. Montarnal, Th. Abballe, F. Caro, E. Laucoin, DEN Saclay.
1 GROUNDWATER HYDROLOGY AND CONTAMINANT TRANSPORT CEVE 518 P.C. de Blanc C.J. Newell 1.Hydrologic Cycle and Water Distribution 2.Soil Horizons 3.Aquifers.
Karst and non karst aquifers modelling « MEditerranean Development of Innovative Technologies for integrAted waTer managEment » Kick-off meeting [7th-8th.
ATM 301 Lecture #7 (sections ) Soil Water Movements – Darcy’s Law and Richards Equation.
Darcy’s Law Philip B. Bedient Civil and Environmental Engineering Rice University.
Final Project I. Calibration Drawdown Prediction Particle Tracking
PRESENTATION OF CFD ACTIVITIES IN CV GROUP Daniel Gasser.
CE 3354 Engineering Hydrology Lecture 21: Groundwater Hydrology Concepts – Part 1 1.
Transient Two-dimensional Modeling in a Porous Environment Unsaturated- saturated Flows H. LEMACHA 1, A. MASLOUHI 1, Z. MGHAZLI 2, M. RAZACK 3 1 Laboratory.
Infiltration Equations Fundamental Mass Balance Equation: Darcy’s Law (z direction): Where.
Water Resources Assessment Main Resources – Surface water – Groundwater – Unconventional Tools – Flood routing/delineation models – Runoff models – GIS.
1 Simulation of the Couplex 1 test case and preliminary results of Couplex 2 H. HOTEIT 1,2, Ph. ACKERER 1, R. MOSE 1 1 IMFS STRASBOURG 2 IRISA RENNES 1.
Soil Physics—Past, Present, and Future
Soil Water Balance Reading: Applied Hydrology Sections 4.3 and 4.4
Algorithm of the explicit type for porous medium flow simulation
Darcy’s Law and Richards Equation
Basic Hydrology & Hydraulics: DES 601
Infiltration and unsaturated flow
Gilles Bernard-Michel
Impact of Flowing Formation Water on Residual CO2 Saturations
Confined aquifer storage
Objective Numerical methods Finite volume.
INFILTRATION The downward flow of water from the land surface into the soil medium is called infiltration. The rate of this movement is called the infiltration.
Infiltration and unsaturated flow
CASA Day 9 May, 2006.
Presentation transcript:

DYNAS Workshop 6,7,8/12/04 Mixed Hybrid Finite Element and Iterative Methods for Flow in Porous Media E. Mouche, C. Le Potier, P. Maugis, L.V. Benet. Commissariat à l'Energie Atomique, C.E. de Saclay, Gif sur Yvette Cedex, France

DYNAS Workshop 6,7,8/12/04 Summary l Cast3M Code l Richard’s equation & MHFE Formulation l Iterative resolution l Illustrations l Air Water migration l + Temperature l Conclusion

DYNAS Workshop 6,7,8/12/04 Cast3M (CASTEM2000) http: //www-cast3m.cea.fr) l Finite Element Code (CEA) l PDE : Structural mechanics, Fluid Mechanics, Thermics, … l Object oriented code : Object2 = Operator Object1 (options) l « Toll Box » (500 operators) l 2 languages : user’s (Gibiane) & developer’s (Esope) l Pre & Post processors l FE, MHFE & FV

DYNAS Workshop 6,7,8/12/04 Cast3M (CASTEM2000) l Porous media : Darcy (2d & 3d), Transport equations (adv. disp. diff.), …( See recent paper in computational geosciences 2004, Gilles Bernard Michel et al, about the COUPLEX test case) l Basic brick for multiphase flow : Iterative Solutions For multiphase flow F, G, …

DYNAS Workshop 6,7,8/12/04 Richard’s Equation, Iterative Resolution Mixed Hybrid Finite Element formulation for water flow in unsaturated porous media », C.Le Potier et al., CMWR XII, 1998 MHFE h : head pressure, U : Darcy velocity, C : Capillary capacity, K : permeability, Θ water content FE Mesh (QUA4) Face center Velocity, head MHFE Mesh EFMH (QUAF) Element center, head

DYNAS Workshop 6,7,8/12/04 Richard’s Equation, Iterative Resolution Implicit time discretization & Picard algorithm Time step : n Iterative step : i

DYNAS Workshop 6,7,8/12/04 Richard’s Equation, Iterative Resolution Time step strategy : Parameter (X= C & K) homogeneization : Different types of means : 1) functions of X values on the faces, X=F(X(H face )), X A (arithmetic), X G (geometric), X H (harmonic) or centered value X = X(H center ) MHFE Mesh MHFE (QUAF) Element center; X = X(H center ) Face center; X =F(X(H face ))

DYNAS Workshop 6,7,8/12/04 Infiltration in a Heterogeneous Soil Infiltration Water content 30mn 1 day Overflow Not at Scale Clay lens Infiltration and Recharge of an aquifer in a heterogeneous soil Sand

DYNAS Workshop 6,7,8/12/04 Rainfall on a Slope (Cf DYNAS) Localized Rainfall Uniform Rainfall Runoff T0 T1 Rainfall on a slope (Runoff, Infiltration, Recharge, Overflow), Aquifer Saturation

DYNAS Workshop 6,7,8/12/04 Richard’s Equation, Iterative Resolution 1. Importance of first time step in the convergence process. If well selected, convergence is achieved in 5-10 iterations. 2. Parameter homogeneization : Depending on the situation : Arithmetic mean or centered value. Arithmetic seems to lead to a better precision ?!. 3. No problem with the convective (gravity) term. 4. Heterogeneous media may lead to tough situations : flow from an impervious medium (low hydraulic diffusivity, D=K/C) to a pervious medium (high D) 5. No problem with the unsaturated - saturated transition (see 4.)

DYNAS Workshop 6,7,8/12/04 Air Water Migration w : water, a : air, Hc : Henry’s constant, ρ : density, ω : porosity

DYNAS Workshop 6,7,8/12/04 Air Water Migration w : water, a : air, Hc : Henry’s constant, ρ : density, ω : porosity Rewritten in terms of capillary head & air head pressures

DYNAS Workshop 6,7,8/12/04 Air Water Migration And solved the same way as for Richard’s equation It looks like the matrix system

DYNAS Workshop 6,7,8/12/04 Touma and Vauclin experiment Exp. and num. Analysis of two-phase infiltration in a partially saturated soil, TIPM (1) 1986 « Vertical infiltration in a sandy column with no lateral air flow and with air flow » Air flow No Air flow. The water infiltration is drastically slowed down by air

DYNAS Workshop 6,7,8/12/04 Air mass conservation problem THM and Geoch. Behaviour of clay barrier in radioactive waste repositories, Volckaert et al, CCE Report EUR en 1996 « Vertical infiltration in a sandy column with no air flow and soluble air » Air mass conservationAir Pressure

DYNAS Workshop 6,7,8/12/04 EVEGAS European Project Cannot find the reference ! «Production of a Hydrogen Bubble in a saturated porous media » Does your code see the Cat’s ears ? H2

DYNAS Workshop 6,7,8/12/04 + Temperature : Thermo Hydraulics Physics Numerics

DYNAS Workshop 6,7,8/12/04 Pollock D.W., WRR (22) 1986 « Simulation of Fluid Flow & Energy Transport Processes associated with HLW Disposal in Unsaturated Alluvium » Saturation y. Saturation y. Pollock’s results

DYNAS Workshop 6,7,8/12/04 Conclusion l Iterative methods work quite well. l Not time consuming, as compared to « global » methods (benchmarking with THM codes). l Sometimes grandma’s tricks (choice of good variables) must be introduced l May become very tough with some media such as unsaturated flow in fractured media, geothermy, … l If you do it, have fun ! A paper is in preparation !