Report from the Crystalline rocks & buffer workshop Mattias Åkesson, Clay Technology AB.

Slides:



Advertisements
Similar presentations
Routing System Stability draft-dimitri-grow-rss-01.txt IETF71 - Philadelphia.
Advertisements

Solutions of Nonelectrolytes
Learning Objectives and Fundamental Questions What is thermodynamics and how are its concepts used in petrology? How can heat and mass flux be predicted.
Experimental Investigation and Mathematical Modeling of Cold-Cap Behavior in HLW Melter D. Pierce, J. Chun, P. Hrma, J. Rice, R. Pokorny, M. Schweiger.
Chapter 4 Electrochemical kinetics at electrode / solution interface and electrochemical overpotential.
Sensitivity Analysis In deterministic analysis, single fixed values (typically, mean values) of representative samples or strength parameters or slope.
Conductivity Testing of Unsaturated Soils A Presentation to the Case Western Reserve University May 6, 2004 By Andrew G. Heydinger Department of Civil.
1 International Clay Conference,14-20 June 2009 Hydration sequence for swelling clays F. Salles 1,2, O. Bildstein 1, I. Beurroies 3, J.M. Douillard 2 M.
A modified Lagrangian-volumes method to simulate nonlinearly and kinetically adsorbing solute transport in heterogeneous media J.-R. de Dreuzy, Ph. Davy,
Flow scheme of gas extraction from solids Chapter 3 Supercritical Fluid Extraction from Solids.
1 Miller Similarity and Scaling of Capillary Properties How to get the most out of your lab dollar by cheating with physics.
REACTIVE TRANSPORT MODELING OF THE INTERACTION BETWEEN WATER AND A CEMENTITIOUS GROUT IN A FRACTURE 1 Josep M. Soler, 2 Marja Vuorio, 2 Aimo Hautojärvi.
© 2014 Carl Lund, all rights reserved A First Course on Kinetics and Reaction Engineering Class 3.
The NEA Sorption Project a multinational cooperative program to advance the use of Thermodynamic Sorption Models Mark Fuhrmann U.S. NRC Office of Nuclear.
Carbon Sequestration is the process of trapping CO 2 underground in order to prevent its release into the atmosphere to reduce our impact on the climate.
Development of Dynamic Models Illustrative Example: A Blending Process
1 Miller Similarity and Scaling of Capillary Properties How to get the most out of your lab dollar by cheating with physics.
Summary of results to date B. Garitte and A. Gens 2nd DECOVALEX 2011 workshop, 20 th of October 2008, Wakkanai, Japan Dept. of Geotechnical Engineering.
Magnetic field diffusion in Molecular Clouds Understanding star formation is a central problem of modern astrophysics. In this work we are performing a.
Introduction to GW contamination and
C HAPTER 1 Matter, Energy and Change. What is Chemistry? 1. Is a physical science: looks at nonliving things (rocks, stars, electricity) 2. Is the study.
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.
Task Force meeting #29, Lund, November Task 8 1 Some ideas for continuation of Task 8 Task 8 is intended to lead to:Task 8 is intended to lead to:
Task #8: Hydraulic interaction rock/bentonite Objectives: Scientific understanding of the exchange of water across the bentonite-rock interface. Better.
Catalyst design driven by fundamental research How do we extrapolate from molecular (picoscale) and nanoscale fundamentals to operating catalytic systems?
Chapter Outline: Phase Diagrams
AN ITERATIVE METHOD FOR MODEL PARAMETER IDENTIFICATION 4. DIFFERENTIAL EQUATION MODELS E.Dimitrova, Chr. Boyadjiev E.Dimitrova, Chr. Boyadjiev BULGARIAN.
Summer Course on Exergy and Its Applications EXERGY ANALYSIS of FUEL CELLS C. Ozgur Colpan July 2-4, 2012 Osmaniye Korkut Ata Üniversitesi.
In Engineering --- Designing a Pneumatic Pump Introduction System characterization Model development –Models 1, 2, 3, 4, 5 & 6 Model analysis –Time domain.
Benchtop X-ray Diffraction Spectroscopy Contact: World Agroforestry Centre (ICRAF), P.O. Box Nairobi, Kenya. Tel:
Chemical Thermodynamics II Phase Equilibria
1 Modelling Task 8 EBS Task Force Meeting 16, Lund, 28 November 2012 Dr. David Holton Dr. Steven Baxter
Chapter 1-1 Matter, Measurement,
BsysE595 Lecture Basic modeling approaches for engineering systems – Summary and Review Shulin Chen January 10, 2013.
Discussion on Modeling Stefan Finsterle Earth Sciences Division Lawrence Berkeley National Laboratory 29. Task Force Meeting Lund, Sweden November 29-29,
Advance Chemical Engineering Thermodynamics
A unifying model of cation binding by humic substances Class: Advanced Environmental Chemistry (II) Presented by: Chun-Pao Su (Robert) Date: 2/9/1999.
Density lab 2012 Entry #5 mineral lab #2—leave 3 pages Entry #6 mineral density lab 2/1/12.
Introduction to Chemistry
Physical and Chemical Changes Matter  Matter – anything that has volume or mass. Atoms are the smallest unit of matter!  Volume – anything that takes.
Upscaling of two-phase flow processes in CO 2 geological storage Orlando Silva (1), Insa Neuweiler 2), Marco Dentz (3,4), Jesús Carrera (3,4) and Maarten.
Microstructure and Phase Transformations in Multicomponent Systems
For RH>54%: Two peaks  2 well-defined families of pore sizes Osmotic swelling occurs at RH > 80% in interlayer space compared to RH ~ 54% in mesopores.
DETERMINATION of the SPECIFIC SURFACE AREA in SWELLING CLAYS F. Salles 1, J.M. Douillard 1, O. Bildstein 2, M. Jullien 3 and H. Van Damme 4 (1) ICGM, Université.
Chemical Reaction Engineering Lecture (1) Week 2.
CHBE 452 Lecture 31 Mass Transfer & Kinetics In Catalysis 1.
Sedimentary Materials Sedimentary rocks cover 80% of the earth’s surface but only comprise ~1% of the volume of the crust (they are generally NOT dense.
Cement waste matrix evaluation and modelling of the long-term stability of cementitious waste matrices.
LECTURE 4 FACILITATED DIFFUSION
HYDRATION SEQUENCE of SWELLING CLAYS EXCHANGED with MIXED ALKALI/ALKALI-EARTH CATIONS F. Salles 1, O. Bildstein 2, J.M. Douillard 1, B. Prelot 1, J. Zajac.
Ch 24 pages Lecture 11 – Equilibrium centrifugation.
Role of Theory Model and understand catalytic processes at the electronic/atomistic level. This involves proposing atomic structures, suggesting reaction.
February 13-15, 2006 Hydromechanical modeling of fractured crystalline reservoirs hydraulically stimulated S. Gentier*, X. Rachez**, A. Blaisonneau*,
R Conclusions According to reactive transport calculations carried out in this study,  At an ambient temperature of 25 °C, there will be no obvious mineralogical.
How Do We Characterize and Control Matter Away - Especially Very Far Away - from Equilibrium? Progress on Grand Challenge New Horizons for Grand Challenge.
Oxygen Potential in High Burnup LWR Fuel using Themochimica in MOOSE/BISON Theodore M. Besmann.
Heat Transfer Su Yongkang School of Mechanical Engineering # 1 HEAT TRANSFER CHAPTER 6 Introduction to convection.
Treatment of colloids and related issues in the safety case BELBaR 1 st Workshop, Helsinki 5-7 March Rebecca Beard, NDA RWMD.
1 Basic of thermodynamic by Dr. Srimala room 2.07 Albert Einstein.
Chapter 20 Lecture 35: Entropy and the Second Law of Thermodynamics HW13 (problems):19.3, 19.10, 19.44, 19.75, 20.5, 20.18, 20.28,
Introduction to Modeling Technology Enhanced Inquiry Based Science Education.
Thermodynamics Thermodynamics Thermodynamics Way to calculate if a reaction will occur Way to calculate if a reaction will occur Kinetics Kinetics Way.
3rd DECOVALEX 2011 workshop, 21th of April 2009, , Gyeongju, Korea
Macroscopic Behavior of Expansive Clay Minerals in the Crystalline Swelling Regime William J. Likos, Department of Civil and Environmental Engineering,
Tritium Research in TITA Information Required
Matter and Chemical Change
Physical and Chemical Changes
The Role of Stretching in Slow Axonal Transport
Parameter Space for Amorphous Oxide Semiconductors (AOSs)
Presentation transcript:

Report from the Crystalline rocks & buffer workshop Mattias Åkesson, Clay Technology AB

Workshop divided in four blocks 1.Buffer/backfill hydration and influence of rock 2.THM process understanding 3.Homogenization, pellets, piping and erosion 4.Chemical and mineralogical interactions A number of specific issues were suggested for each block Each block started with an introduction Possible form of output: ProcessesRelevance for PANeed for experimental data Need for code development Need for development of conceptual models

1. Buffer/backfill hydration and influence of rock Introduction: M. Åkesson Specific issues: To what degree can we confidently predict buffer saturation times? Is the degree of uncertainty important from PA point of view? Interaction rock buffer /crystalline host rock: i) Effect of localized water entry (individual fractures inflow); ii) Is it necessary to consider especial properties for the rock/buffer interface? Should we work more intensively towards routine performance of 3D THM numerical analysis or 2D computations are sufficient for our purposes?

Modeling approaches 2D – axisymmetric buffer model

Modeling approaches 2D-axisymmetric backfill model Example of influence of fracture distance

1. Buffer/backfill hydration and influence of rock Discussion PA aspects: –Moderate relevance of time of hydration in itself –Critical that it gets hydrated eventually –Less crucial how long it takes –If hydration is slow, it may have influence on the chemical state of the barrier Rock interaction and interface properties –Planned Äspö project ”BRIE”. Study effects of intersecting fracture. Joint task for EBS and groundwater modelers. –No general need for special interface properties, except perhaps friction elements 3D or 2D modeling –Bounding calculations in 2D, with sensitivity analysis, is sufficient if it can be justified –3D without sensitivity analysis in dangerous - Order of complexity: T, TH, THC, THM

2. THM process understanding Introduction: H.R. Thomas Specific issues: Are there additional phenomena that should be included in our understanding/modelling of the buffer? For instance: i)effect of microstructure evolution; ii)existence of different states of water in the bentonite; iii)existence of a threshold gradient in water flow; iv)thermo-osmosis Can we obtain all required buffer parameters from (small scale) laboratory tests?

2. THM process understanding Discussion –In some experiments the models tend to over predict the rate of hydration –This may be caused by the uncertainty in parameter data –Or by limits in the conceptual models: A number of phenomena has been proposed which may explain these: i) effect of microstructure evolution; ii) existence of different states of water in the bentonite; iii) existence of a threshold gradient in water flow; iv) thermo-osmosis –Confidence building. Scientific approach has a central role,: –Characterize uncertainties; –Extrapolation to very long time scales – thermodynamically grounding & use natural analogs

3. Homogenization, pellets, piping and erosion Introduction: M. Åkesson Specific issues: Do we require better understanding of the THM behaviour of special materials such as pellets or pellet-powder mixtures? Is microstructure evolution especially important in this case? Significance of the processes associated with Homogenization / gaps / erosion / piping of the bentonite buffer. Are potential irreversible effects in large swelling/compression cycles understood?

Comparison with experimental results Maximum fallout Theoretical section Saturated oedometer test CRT void ratio profile Data indicate that hysteretic effects are one cause of remaining heterogeneities

Piping and erosion A model has been derived from erosion tests results, assuming a linear relation in a double logarithmic diagram: where m s = accumulated mass of eroded bentonite (g) m w = accumulated mass of eroding water (g)  = α = 0.65 The current limit that only 1 % of the inflow into one tunnel is allowed from one deposition hole is supported by this model.

3. Homogenization, pellets, piping and erosion Pellets and erosion –Difficulties to predict the water flow through pellets fillings. Influence how fast we must backfill. But, this is possible to test and even to train. –Question about if we should expect homogenization: Yes if it is the same material, but perhaps not if swelling/compression cycles are irreversible –Erosion of pellets depending on salinity, water flow and granularity –Empirical model imply a maximum allowed inflow of 1% of tunnel available pore space into the deposition hole –Grouting is the method to limit the inflow to 1 % of total inflow. –The plug is a therefore an important system component Homogenization –Definition of homogenization: Convergence of densities or keeping the difference in permissible bounds –Irreversible swelling/compression cycles should be expected. –Same phenomena observed in free swelling retention curves The mechanical constitutive laws have a key role, in contrast to conventional THM modeling

4. Chemical and mineralogical interactions Introduction: O. Karnland Specific issues: What are the effects of the characteristics and phenomena of the transient period on the long term state of the buffer? Possible presence of chemical phenomena interacting with THM behaviour and leading to irreversible effects: i) dissolution/precipitation phenomena; ii) cation exchange processes; iii: others?

4. Chemical and mineralogical interactions Introduction Possible mineral reactions Enrichment of substances originating from the saturating groundwater Accessory mineral dissolution/precipitation Montmorillonite surface reactions, Ion - exchange, Na → Ca Colloid release from Na-montmorillonite Montmorillonite alteration, illitization/dissolution Geochemical modeling Microstructure view – Multipore systems The chemical view – Ion equilibrium

0.5 g Wyoming material after 43 days in 100 mL H 2 O Ca- montmorillonite Na- montmorillonite No colloid formation in Ca-montmorillonite

Conceptual view of montmorillonite (bentonite) C1C1 C 2 <<C 1 flux of anions C 3 =0 Chemical view: ion equilibrium with interlayer space Ion equilibrium between montmorillonite interlayer space and an external solution - Consequences for diffusional transport. Birgersson and Karnland, 2008, in press, Geochimica et Cosmochimica Acta, DOI: /j.gca Bentonite solution 1solution 2 C1C1 C 2 =0 flux of anions C 3 =0 Micro-structural view: no anions in interlayer space microstructure Bentonite solution 1solution 2

4. Chemical and mineralogical interactions Discussion Good if different groups have different conceptual understanding Multi-component reactive transport models, not pushed to the same level as THM models

Advances since 2003 Empirical erosion model “Chemical view” of bentonite – conceptual breakthrough Thermodynamic approach Molecular dynamics Significant advances of conceptual understanding of bentonite behavior The large-scale experiments Industrial aspects

Need for further research Bentonite hydration: Identification of processes not included in present formulation THM behavior of pellets and pellets mixtures Piping and erosion Irreversible swelling/compression in large gap filling Chemical issues: implementation of “chemical view” in geochemical codes. Greater integration of THM & C