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CMS WORKSHOP LECTURES Volume 21 FILLING THE GAPS – FROM MICROSCOPIC PORE STRUCTURES TO TRANSPORT PROPERTIES IN SHALES THE CLAY MINERALS SOCIETY Joseph W. Stucki, Series Editor and Editor in Chief University of Illinois Urbana, IL 61801-4798, USA Thorsten Scha ¨fer 1 , Reiner Dohrmann 2 , and H.C. Greenwell 3 , Volume Editors 1 Karlsruhe Institute of Technology (KIT), Institute for Nuclear Waste Disposal (INE), P.O. Box 3640, D-76021 Karlsruhe, Germany; 2 Federal Institute for Geosciences and Natural Resources (BGR), State Authority of Mining, Energy and Geology (LBEG), Stilleweg 2, D-30655 Hannover, Germany; and 3 Department of Earth Sciences, Durham University, South Road, Durham, DH1 3LE, UK

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CMS WORKSHOP LECTURES

Volume 21

FILLING THE GAPS – FROMMICROSCOPIC PORE

STRUCTURES TO TRANSPORTPROPERTIES IN SHALES

THE CLAY MINERALS SOCIETY

Joseph W. Stucki, Series Editor and Editor in Chief

University of Illinois

Urbana, IL 61801-4798, USA

Thorsten Schafer1, Reiner Dohrmann2, and H.C. Greenwell3, Volume Editors1 Karlsruhe Institute of Technology (KIT), Institute for Nuclear Waste Disposal (INE), P.O. Box 3640,

D-76021 Karlsruhe, Germany; 2 Federal Institute for Geosciences and Natural Resources (BGR),

State Authority of Mining, Energy and Geology (LBEG), Stilleweg 2, D-30655 Hannover, Germany; and3 Department of Earth Sciences, Durham University, South Road, Durham, DH1 3LE, UK

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CMS WORKSHOP LECTURES

VOLUME 21

FILLING THE GAPS – FROM MICROSCOPIC PORE STRUCTURES TO

TRANSPORT PROPERTIES IN SHALES

Organized By

Thorsten Schafer

Karlsruhe Institute of Technology, Germany

Reiner Dohrmann

State Authority of Mining, Energy, and Geology (LBEG), Germany

Federal Institute for Geosciences and Natural Resources (BGR), Germany

H.C. Greenwell

Department of Earth Sciences, Durham University, UK

Kevin Murphy

The Clay Minerals Society

Contributors

Guillaume Desbois, Structural Geology, Tectonics and Geomechanics, EMR, RWTH Aachen

University, Lochnerstr. 4-20, D-52056 Aachen, Germany

Christopher R. Clarkson, Department of Geoscience, University of Calgary, 2500 University

Drive NW, Calgary, Alberta, Canada T2N 1N4

Andrew Aplin, Department of Earth Sciences, Science Laboratories, South Road, Durham Univer-

sity, Durham, DH1 3LE, UK

Christian Schurig, Chair of Soil Science, Wissenschaftszentrum Weihenstephan, Technische Uni-

versitat Munchen, 85350 Freising-Weihenstephan, Germany

Tony Lanzirotti, Center for Advanced Radiation Source, The University of Chicago, Chicago, IL

60637, USA

Fred Mosselmans, Science Division, Diamond Light Source, Harwell Campus, Didcot, Oxon

OX11 ODE, UK

Marc Fleury, IFP Energies nouvelles, 1, avenue de Bois-Preau, 92852 Rueil-Malmaison, France

Edo Boek, Department of Chemical Engineering, Imperial College, London SW7 2AZ, UK

Daniel Grolimund, Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen-PSI,

Switzerland

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Benjamin Rotenberg, Sorbonne Universites, UPMC Univ. Paris 06, UMR 8234 PHENIX, Paris,

France

Christophe Tournassat, Water, Environment and Ecotechnology Division, French Geological

Survey (BRGM), Orleans, 45060, France

Gioacchino Viggiani, Universite Grenoble Alpes and CNRS, Laboratoire 3SR, Saint Martin

d’Heres, France

Rosanne Murray, Department of Earth Sciences, Science Laboratories, South Road, Durham

University, Durham DH1 3LE, UK

Pieter Bertier, Clay & Interface Mineralogy, RWTH-Aachen University, Bunsenstr. 8, D-52072

Aachen, Germany

Stephan Kaufhold, BGR, Bundesanstalt fur Geowissenschaften und Rohstoffe, Stilleweg 2,

D-30655 Hannover, Germany

Paul Marschall, National Cooperative for the Disposal of Radioactive Waste, 5430 Wettingen,

Switzerland

Frank Friedrich, Karlsruhe Institute of Technology, Institute for Nuclear Waste Disposal (INE),

Hermann-von-Helmholtz-Platz 1, D-76344 Eggenstein-Leopoldshafen, Germany

Katarzyna Gorniak, AGH University of Science and Technology, Faculty of Geology, Geophysics

and Environmental Protection, al. Mickiewicza 30, Krakow, 30-059, Poland

Pierre Dick, IRSN - Institut de Radioprotection et de Surete Nucleaire, BP 17, F-92262 Fontenay-

aux-Roses, France

Nicola Rigonat, The University of Edinburgh, Grant Institute of GeoSciences, James Hutton

Road, Edinburgh EH9 3FE, UK

Yukio Tachi, Japan Atomic Energy Agency, 4-33 Muramatsu, Tokai-mura, Ibaraki, 319-1194,

Japan

Kenji Yotsuji, Japan Atomic Energy Agency, 4-33, Muramatsu, Tokai-mura, Ibaraki, 319-1194,

Japan

Published by

The Clay Minerals Society

3635 Concorde Pkwy Suite 500

Chantilly, VA 20151-1125, USA

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Copyright # 2016 The Clay Minerals Society

All rights reserved. No part of this book may be reproduced by any mechanical, photographic, or

electronic process or in the form of photographic recording, nor may it be stored in a retrieval

system, transmitted, or otherwise copied for public or private use without written permission

from the publisher. For information on this and other volumes in the CMS Workshop Lectures

Series, write The Clay Minerals Society, 3635 Concorde Pkwy Suite 500, Chantilly, VA

20151-1125 USA or go to www.clays.org.

Citations of articles in this volume are properly referenced as follows:

CLARKSON, C.R. and SOLANO, N.A. (2016) Combined use of neutron-scattering, fluid-invasion,

and image-analysis techniques to assess pore structure, accessibility, and connectivity in tight

rock. Pp. 15–31 in: Filling the Gaps – from Microscopic Pore Structures to Transport

Properties in Shales (T. Schafer, R. Dohrmann, and H.C. Greenwell, editors). CMS Workshop

Lectures, 21. The Clay Minerals Society, Chantilly, Virginia, USA.

Library of Congress Catalog Number

ISBN - 978-1-881208-46-4

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THE CLAY MINERALS SOCIETY

The Clay Minerals Society (CMS) was organized in 1963 to stimulate research and to

disseminate information relating to all aspects of the science and technology of clays

and other fine-grained minerals. It sponsors an annual Clay Conference where research

and invited papers are presented in technical sessions and special symposia. Field trips

are organized to important occurrences of clays in regions near the Conference locations

and to industrial sites of clay production and application. In conjunction with its annual

meetings, workshops are held on technical subjects of interest to clay researchers and

technologists. CMS publishes Clays and Clay Minerals, which is the leading inter-

national journal in the field of clay science. In this journal are presented the latest scien-

tific investigations in all areas of the field and from all parts of the world, along with

timely review articles and announcements of new publications on clays and other

fine-grained minerals.

CMS also sponsors the Source Clays Repository, which is now well established as the

provider of clay samples to a plethora of research groups world wide and to teachers of

clay science. It also offers other clay-related publications to its members at a discount

over publisher’s list prices.

Its multi-disciplinary membership includes agronomists, microbiologists, surface

chemists, physicists, geologists, mineralogists, geochemists, material scientists, soil

scientists, crystallographers, sedimentologists, economic geologists, colloid chemists,

ceramicists, rheologists, petroleum engineers, and geotechnical engineers, thereby offer-

ing members the opportunity to exchange ideas and results with fellow researchers

having widely different backgrounds and expertise.

For information on joining the Society and subscribing to Clays and Clay Minerals,

contact:

The Clay Minerals Society

Society Office

3635 Concorde Pkwy Suite 500

Chantilly, VA 20151-1125

Phone: (703) 652-9960

FAX: (703) 652-9951

www.clays.org

E-mail: [email protected]

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Preface

THORSTEN SCHAFER1, REINER DOHRMANN

2, and H. C. GREENWELL3

1Karlsruhe Institute of Technology (KIT), Institute for Nuclear Waste Disposal (INE),

P.O. Box 3640, D-76021 Karlsruhe, Germany2Federal Institute for Geosciences and Natural Resources (BGR),

State Authority of Mining, Energy and Geology (LBEG), Stilleweg 2,

D-30655 Hannover, Germany3Department of Earth Sciences, Durham University,

South Road, Durham DH1 3LE, UK

1. Introduction

This CMS Workshop Lecture Series (WLS) volume is intended to give a summary of the

current state-of-the-art of different spectroscopy and microscopy methods, as presented

during a workshop held in conjunction with the EUROCLAY 2015 conference in Edin-

burgh, UK, on the 5th of July 2015. This workshop was initiated by the NEA Clay

Club, The Clay Minerals Society, and the Euroclay conference series. This EUROCLAY

2015 workshop is a continuation of the very successful workshop “Clays under Nano- to

Microscopic resolution” which took place from 6th–8th September 2011 in Karlsruhe

and documents new developments and the progress made over the past four years

concerning research in low-permeability, clay-rich, geological formations (NEA-CLAY-

CLUB, 2013). The workshop also provided an excellent opportunity for exchange of

knowledge with research communities concerned with the safe long-term management

of radioactive waste within argillaceous sediments, and with shale gas and oil exploration.

A wide spectrum of argillaceous media are being considered in Nuclear Energy

Agency (NEA) member countries for the purpose of the passive long-term management

of radioactive wastes. This includes variously indurated clay-rich bedrock formations to

host and enclose a Deep Geologic Repository and clays used as engineered barrier

materials to create durable repository seals. In this context, the NEA established in

1990 a Working Group on Argillaceous Media, known informally as the ‘Clay Club.’

The Clay Club examines those various argillaceous rocks that are being considered

for the deep disposal of radioactive waste, ranging from soft clays to indurated

shales. These low-permeability rocks exhibit petrophysical, hydrogeologic, and geome-

chanical properties, among others, which allow them to behave as long-lived passive

barriers to the movement of water and solutes on timescales relevant to the safety of

a Deep Geologic Repository (i.e. 1 Ma) (Dohrmann et al., 2013).

In addition, the shale-gas and oil community is interested in the characterization of

sedimentary formations (i.e. black shales) from the core- to nano-scale, focusing on

clay/brine/organic interfaces and understanding how pore space evolves and affects

the transport and production potential of the shale system. Through characterization

of fundamental properties such as nanopore/micropore connectivity, all the way up

to understanding transport and mechanical fracture properties of whole rock units,

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both communities (radioactive waste disposal, and shale gas and oil) are studying the

geological materials with a shared set of tools, from quantum mechanics and molecular

dynamics computer simulations, through advanced microscopy and diffraction methods,

up to tri-axial mechanical tests and large-scale mass-transport models.

Very generally speaking, these clay rocks are composed of fine-grained minerals

showing pore sizes from ,2 nm (micropores) up to .50 nm (macropores). Pores of

between 2 and 50 nm are mesopores. The fluid migration, solute transport, and mechan-

ical properties are largely determined by this microstructure (Figure 1), the spatial

arrangement of the minerals, and the porewater chemical composition. Examples

include anion-accessible (‘geochemical’) porosity and macroscopic membrane effects

(chemical osmosis, hyper-filtration), geomechanical properties, and the characteristics

of two-phase flow properties (relevant for gas transport).

In shale oil/gas systems, the role of clay minerals in creating porosity and controlling

organic-matter distribution is of keen interest, as well as larger-scale phenomena such as

how diagenesis affects the mechanical properties of the shale-gas unit. Linking our

knowledge to: (1) increased confidence in our understanding of material properties/phenomena used in a typical repository safety case, and (2) how best to up-scale the

nano-scale understanding/knowledge are essential.

2. Short summary of research examples presentedduring the workshop

The one-day workshop was subdivided into five sessions with a two-hour poster

session during lunch, which fostered active exchange between students and experts

in the field.

Figure 1. A schematic diagram showing how a multi-scale approach connects mineralogy, porosity, and

transport properties in argillaceous media (Figure reproduced from NEA-CLAYCLUB, 2013, with permission).

VIII

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The five general topics included:

. Pore structure and connectivity

. Chemical information under high spatial resolution

. Gas/water and ion mobility in tight formations

. Upscaling and implementation in model approaches

. Rock mechanics

The rock formations covered within the workshop included host rocks considered for the

deep geological disposal of radioactive waste, such as the Opalinus Clay, the Boom

Clay, the Callovo-Oxfordian argillite, and from the generic underground research

tunnel within the Toarcian shales. Furthermore, sedimentary formations investigated

in the context of oil and gas reservoirs included the Cardium Formation in western

Canada, natural siliciclastic mudstones from the London Clay formation, Oligocene

Grybov marls, Posidonia shales, and Kimmeridge shales and mine tailings (McLean

Lake Tailing Management Facility; TMF). To complete this list, research results also

covered bentonite (MX-80) and minerals such as biotite, illite, and boehmite.

2.1. Pore-structure and connectivity (physical imaging)

The Rheinisch-Westfalische Technische Hochschule Aachen University (Germany)

group (Jop Klaver) gave an overview of complementary methods working at different

scales, providing a conceptual ‘toolbox’ for the characterization of the clay microstruc-

ture. Information about the 3D fracture network, the mineral fabric, and the macropor-

osity can be obtained by micro-computed tomography (mCT), but is clearly limited in

resolution (mm range). Combining mCT with broad ion beam scanning electron

microscopy (BIB-SEM), on the other hand, can give information on pore morphology

and the identification of elementary islands in 2D at the nm scale. If these methods

are further combined with focused ion beam transmission electron microscopy (FIB-

TEM), 3D information on pore connectivity and elementary island representative

under nm-scale resolution can be achieved. A critical point in this type of investigation

is the preservation of the pore structure and connectivity during sample preparation

(drying). Several impregnation methods are discussed in the literature (Pret et al.,

2004; Robinet et al., 2015) and the Aachen group favors the Woods metal (WM) injec-

tion (Woods metal is an alloy of 50.0% bismuth, 26.7% lead, 13.3% tin, and 10.0%

cadmium) liquid at elevated temperatures of 708C (Klaver et al., 2015). The authors

encountered unfilled WM regions and interpret them as artefacts during the WM injec-

tion process closing accessible pore throats (see Desbois et al., 2016, this volume). With

respect to future studies, a comparison with methods such as nuclear magnetic reson-

ance (NMR) or small-angle neutron scattering studies (SANS) should be performed

to tackle and quantify the artefacts.

Using a combination of SANS and ultra-small angle neutron scattering (USANS),

fluid invasion, and imaging methods, pore structure, accessibility, and connectivity

for multiple Cardium Formation tight oil samples have been investigated by Chris

IX

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Clarkson and co-workers from the University of Alberta. On the microlithofacies scale

down to the mm level, the mapping of permeability, porosity, and microhardness has

been performed using computed tomography (CT), mCT, and optical microscopy on

core samples. This information is combined with macroscale work (formation scale)

on the meter to kilometer scale using seismic surveys, well testing, and well logging

(Clarkson and Solano, 2016, this volume).

In a further step, these data are combined with information on the sub-microlithofa-

cies scale using several methods (e.g. SEM, TEM, mercury intrusion porosimetry (MIP),

low-pressure nitrogen adsorption (LPAN2), or CO2 adsorption (LPACO2), He pycnome-

try, Hg intrusion and especially SANS/USANS). The scattering intensity profiles

obtained by SANS/USANS measurements revealed a broad pore-size distribution

with pore accessibility varying strongly with pore size. The scattering intensity profiles

follow a slope of –3 on a log-log scale, which indicates a power-law scattering charac-

teristic of a very rough (fractal) pore-matrix interface.

All images (except for TEM) shown in Figure 2 were taken from reservoir samples

obtained from a tight oil reservoir within the Cardium Formation (depth of �1470 m)

(Pembina Field) in western Canada. One surprising result is that the accessibility

is smaller for larger pore sizes, a finding consistent with Hg intrusion results. High-

resolution SEM imaging has in fact revealed that disconnected pores appear within

mineral grains, possibly explaining the SANS/USANS results. The SANS/USANS

interpretations may be affected by the assumption of a two-component system (spherical

poresþ average mineral phase), however. Mineral mapping using energy-dispersive

X-ray spectroscopy (EDX) suggests that additional components (strong scattering

accessory mineral phases, e.g. siderite) may be present which could affect significantly

the SANS/USANS-derived porosity, pore-size distribution, and pore-accessibility

calculations. A multi-component system will be tried in future work and differences

will be quantified using the more conventional two-component model.

The spherical pore-model assumption used to calculate the pore-size distribution

from the SANS/USANS scattering profiles was discussed indirectly by Aplin and

co-workers, who focused on the permeability estimates from pore size data (see contri-

bution Aplin et al., 2016, this volume) which clearly revealed that a reasonable corre-

lation between the measured and modeled permeability could only be obtained

assuming an elongated wedge-shaped geometry (see also Yang and Aplin, 2007).

In the poster session, Bertier et al. (2016, this volume) presented a critical discussion

about the use of N2 physisorption for the characterization of the pore structure of shales

by addressing some common pitfalls and misconceptions related to the interpretation

of physisorption data. Using measurements from a set of nine Opalinus Clay samples,

N2 physisorption values were compared with other methods such as He-pycnometry,

MIP, fluid saturation (Archimedes), and USANS. The authors concluded that the

results could be used for the analysis of the pore structure of shales and mudrocks,

but they should be interpreted with caution.

The pore system of a potential German gas shale (four different Posidonia shales)

with different levels of maturity was evaluated critically by Kaufhold et al. (2016,

this volume). The most important question concerning shale-gas production and

X

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Figure 2. Use of imaging methods to visualize geologic structures controlling flow at the core- and finer-scale

(taken from Clarkson and Solano, 2016, this volume). The upper panel illustrates use of core photography (left)

for imaging microfacies distribution and X-ray micro-computed tomography (XRmCT, middle and right) for

imaging bulk-density contrasts in core plugs (sampled from a large whole-core sample). The middle and lower

left panels illustrate the use of backscatter imaging from SEM for imaging micro- to nano-scale pore structures

and their associations. The panel on the lower right illustrates use of transmission electron microscopy (TEM)

for imaging nano-scale structures (Jiang et al., 1997; reproduced with permission). Pores and porous regions in

the XRmCT and BSE/SEM images are represented by the darker areas.

XI

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porosity relates to the diameter needed to provide gas migration. The authors compared

their results with data published on gas shales which are known to be productive.

Although both direct microscopical methods and indirect methods based on gas adsorp-

tion or MIP were applied, most of the pores within the clays and shales were too small to

be detected by any of the direct methods. Natural gas in micropores may be bound too

strongly to liberate it without low-pressure/vacuum. For gas production, either meso- or

macropores may be important. The authors concluded that the potential of the Posidonia

shale for gas production, of course, has to be proven by shale-gas production tests.

Microstructural insights into petrophysical characteristics of indurated clays were

given by Marschall et al. (2016, this volume), who characterized core samples from

the Opalinus Clay using TEM, FIB nanotomography (FIB-nt), and CT with image pro-

cessing procedures. Results were compared with MIP, nitrogen adsorption/desorption

measurements (‘BET’), sieving methods, X-ray diffraction (XRD), and triaxial

testing. The authors found that the macroscopic (poro-elastic) deformation behavior

of the Opalinus Clay was reproduced fairly well by geomechanical modelling on the

microscopic scale. In addition, new insight was gained with regard to the role of

small mesopores (2–10 nm), which essentially control the macroscopic deformation be-

havior of the indurated clay.

Apart from clay formations, the development of deep geological repositories for long-

term radioactive waste management is also foreseen in crystalline rocks. Multi-barrier

repository concepts for crystalline rocks require geotechnical barrier systems based

on compacted bentonites (Sellin and Leupin, 2014) which, depending on the compaction

efficiency, contain regions of different densities, and were studied using FIB-nT (e.g.

Keller et al., 2014). In the poster session, hydration experiments with cation-exchanged

Febex bentonite samples studied using an environmental SEM (ESEM) were presented

by Friedrich et al. (2016, this volume). The main finding was that the Sr-exchanged form

showed significantly more swelling at low relative humidity.

2.2. Chemical information under high spatial resolution

To obtain chemical information under high spatial resolution to the mm level and

even the sub-mm level, the research field clearly benefited from the developments

made over the past decade using synchrotron radiation, but not exclusively, as shown

in the presentation by Christian Schurig (see Schurig et al., 2016, this volume) from

the group of Ingrid Kogel-Knabner at the Technical University Munich (Germany).

The authors used nano-scale stable isotope mass spectrometry (NanoSIMS) to charac-

terize the isotopic composition of mineral-associated natural organic matter in

complex soil structures. Here, for example, synchrotron-based Scanning Transmission

X-ray Microscopy (STXM), with a spatial resolution in the 20 nm range and working

on different element absorption edges (Brandt et al., 2012; Kretzschmar and Schafer,

2005), could give complementary information on the general organic structure or

metal oxidation state and isotopic composition. The NanoSIMS presentation also

pointed out clearly that for accurate SIMS stable isotope analysis the polishing relief

XII

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should be less than a few pm, which has to be evaluated by using an optical surface pro-

filometer (Kita et al., 2009).

Two synchrotron beamlines were presented in detail in the oral lectures, the GeoSoil-

EnviroCARS (GSECARS) at the Advanced Photon Source (APS, Chicago, Illinois,

USA) Sector 13 by Tony Lanzirotti (see Lanzirotti et al., 2016, this volume) and the

I18 Beamline of the Diamond light source, UK, by Fred Mosselmans (see Mosselmans

et al., 2016, this volume). The examples given in both presentations were not restricted

to clay systems alone, but showed clearly the potential for clay-dominated systems

(Lange et al., 2010). Improvements included synchronous micro-diffraction capabilities

at high spatial resolution and high speed coupled with micro X-ray fluorescence (mXRF)

mapping at GSECARS.

2.3. Gas/water and ion mobility in low-permeability formations

Nuclear magnetic resonance studies by the group of Marc Fleury (Institute France

Petrol; IFP Energies nouvelles; Rueil-Malmaison, France) demonstrated that water is

surprisingly highly mobile, even when strongly confined in nanopores and despite a

strong affinity with the solid surface. From these NMR studies, the primary factor gov-

erning diffusion in a compacted system seems to be porosity, while the texture or the

pore network details play a secondary role. For small pores in the 1–100 nm range,

unimodal or multimodal NMR relaxation time distribution can provide simple criteria

to characterize connectivity between different compartments of the pore network

system at a time scale corresponding to the life-time of the magnetization and for

length scales of the order 1 mm or larger. In the interlayer space of smectites, the orien-

tation of water molecules can be observed using specific NMR protocols and show the

strong affinity of water with the solid surface (Fleury et al., 2016, this volume).

The presentation by Edo Boek (2016, this volume) demonstrated clearly that the

segmentation of mCT data for the determination of transport properties in fractured

shales using Lattice Boltzmann (LB) and molecular dynamics (MD) simulations must

be used with care and the CT resolution must be taken into account. Here, the parallel

plate model results corresponded to the LB results, but were much higher (15.3–

44.6 Darcy) than the experimental results. For the measured permeability of

1 mDarcy in the example given, the measured aperture would be in the range of

�3.7 mm based on cubic law estimates, which was clearly below the resolution

of the CT dataset (here 13.7 mm resolution) and shows the limitations depending on

the question to be tackled.

The last presentation in this session, given by Daniel Grolimund from PSI-SLS (Gro-

limund et al., 2016, this volume), focused on the migration behavior of redox-sensitive

Se(IV) and monovalent Cs in Opalinus Clay. A multiple-method approach was used

including classical tomography for the structural properties, mXRF, mXRD, chemical

tomography, and mLA-ICP-MS for the chemical properties, neutron studies for the

fluid properties, and macroscopic studies to determine the sorption and diffusion prop-

erties. The random-walk simulations of Cs migration were compared with 3D measure-

ments and showed a very good comparability.

XIII

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Transferring information from high spatial resolution to the large scales of a site

(Figure 1) is the goal of these studies. Two posters focused on this scale. Gorniak

(2016, this volume) studied the pore space in the impure chalk-type source rocks of

the Oligocene Grybow Marls (Outer Carpathians, Poland) using SEM. The author con-

cluded that the origin of the clay and the eogenetic overgrowth calcite cementation influ-

enced the pathway of burial diagenesis and, thus, the pore-space evolution in the impure

chalk. The internal architecture and permeability structures of faults in shale formations

were studied by Dick et al. (2016, this volume). The authors showed that microfractures

govern the matrix porosity in the damage zone and exert an increasingly dominant role

on fluid flow along the boundary between fault core and fault damage zone.

A third poster presented an innovative tool for monitoring of the water chemistry

evolution in bentonite buffer materials using magnets (Rigonat et al., 2016, this

volume). NdFeB magnets were mixed with powdered Na-bentonite, then held at 708Cfor 5 months). Results revealed different degrees of corrosion in the magnets but the

swelling clay minerals were not degraded.

2.4. Upscaling and implementation in modeling approaches

Detailed sensitivity analysis solving the Poisson-Boltzmann equation for swelling and

non-swelling clay materials by the group of Christophe Tournassat and colleagues

from BRGM (French Geological Survey) and Lawrence Berkeley National Laboratory

(USA) based on the three key parameters that affect model predictions of anion exclu-

sion in clay media, namely the pore-size distribution of clay media, the distance of

closest approach of ions to the clay surface, and the accessibility of sub-nanometer-

wide clay-mineral interlayer spaces to anions, highlighted the significant impact of

pore-size distribution on anion-accessible porosity. The calculations show that all

three model assumptions significantly impact values predicted for the anion accessible

porosity. As a consequence, macroscopic measurements of anion exclusion in clay

media cannot be used to test any of the three model assumptions independently from

the other two (Tournassat et al., 2016, this volume).

While recent developments in advanced nano-imaging techniques can provide

detailed views of the microstructure of non-swelling materials, determination of

the microstructure of swelling clays remains a challenge because important additional

information must be obtained at the nm to sub-nm scale. In addition, the accuracy of

ion-distribution models such as the modified Gouy-Chapman (MGC) model in sub-nan-

ometer-wide interlayer nanopores is not known for compacted clay systems in which

overlapping electrical double layers (EDL) are important, particularly with regard to

anion accessibility to the interlayer space. Clearly, additional insights from MD simu-

lations are needed to better constrain macroscopic scale models (cf. Newton and

Sposito, 2015). In natural clay-rocks, where both swelling and non-swelling clay min-

erals are present (smectite, illite, and interstratified clay minerals), the characterization

of the pore-size distribution (from the mm to the nm scale) is a necessary step to accu-

rately predict ion-concentration distributions. Finally, the authors noted that other

sources of uncertainty must be better understood, including the domain of validity of

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the MGC model for complex electrolyte compositions and the fraction of the surface

charge that is screened by the Stern layer.

Overall, the characterization of the pore-size distribution and pore shapes is a necess-

ary step to predict accurately the ion distribution and mobility in the pore space. New

results on changes in celestine precipitation-induced porosity in compacted illite

could demonstrate that anions can be excluded completely from the smallest pores

within a compacted illite material, whereas transport of tritium (water) is still observa-

ble, clearly showing the absence of full porosity clogging (Chagneau et al., 2015).

Benjamin Rotenberg presented a pore network model for spatial dimensions of

.1 mm based on LB or analytical solutions for the pores and channels in the domain

range �1–10 nm taking into account electro-kinetic effects in charged porous media

(see Obliger et al., 2016, this issue). Heterogeneity and couplings can be taken into

account, but caution is needed concerning “effective single channels” to predict macro-

scopic properties. The model cannot currently be used to predict desaturation, clogging,

or thermal gradients; and the parameterization for natural claystones (Callovo-Oxfor-

dian argillite) is currently in progress in order to constrain the model as much as possible

with experimental information.

In the poster session, two posters from the Japan Atomic Energy Agency and Chiba

University, Japan, focused on modeling approaches in radwaste-relevant systems. Tachi

et al. (2016, this issue) studied diffusion and sorption in the argillaceous rock from the

Horonobe Underground Research Laboratory, Japan, and compared their modeling

results with batch tests. Yotsuji et al. (2016, this issue) developed a model taking into

account multiple pore structures in compacted bentonite such as inter-layer and inter-

particle pores, particularly for anionic species.

2.5. Rock mechanics

The concept of deep geological repositories for the disposal of radioactive waste relies

in part on the long-term low permeability of the host and enclosing rock. As the per-

meability is influenced by mechanical damage, the characterization of damage mechan-

isms of the host rock (at multiple scales) is important.

A first approach is developed to characterize strain localization at the scale of a lab-

oratory specimen (a few centimeters). The group of Cino Viggiani (University Joseph

Fourier, Grenoble, France) presented new results obtained with a new true triaxial

apparatus that allows observation of a rock specimen under loading via X-ray CT and

3D digital image correlation (3D-DIC). Here, the development between the previous

workshop in 2011, with cell dimensions of 10 mm diameter resulting in a voxel size

of 7 mm (laboratory 3SR) and a maximum cell pressure of 10 MPa, could be compared

to the current state-of-the-art measurements using an in situ tri-axial compression test

cell with a specimen diameter of 1.3 mm and a height of 2.5 mm resulting in a voxel

size of 0.7 mm (ERSF, beamline ID19).

The strain field in the sample, and its evolution up to and beyond strain localization,

can be measured by digital image correlation (DIC) of photographs taken through a hard

transparent window. Tests in plane-strain compression have been performed, starting

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from isotropic stress states at several mean stress levels. Results of the time evolution of

the pattern of localization in the specimens are shown. Strain localization appears to

start well before the stress peak, sometime at �50% of the stress peak, by very numer-

ous parallel and conjugated shear bands. This early strain localization, to the authors’

knowledge, has never been observed in rocks before. The number of active bands,

then, decreases progressively during subsequent loading, down to a very few bands at

the peak and during strain softening. It is also possible to demonstrate how localization

is influenced by confining pressure. The experimental results are analyzed systemati-

cally in terms of fields of shear and volumetric strains.

The second approach focuses on a smaller scale – the scale of mineral inclusions

embedded in a clay matrix where the inclusion size is a few microns. Studying the mech-

anisms of deformation at this scale is a challenge (clay cracking, de-cohesion of

inclusions, etc. . .); understanding the mechanisms at a relevant scale for understanding

the substantial evolution of some of the physical properties such as fluid permeability

is essential, however. The focus of this study was to characterize the mechanisms of

deformation at the small scale during loading experiments by combining X-ray

micro-tomography and DIC. Where the microstructure of the material is relatively

well understood (Robinet et al., 2012), relatively few attempts have been made to

Figure 3. (Upper) Reconstructions (ID19) at different steps of loading of a clay-rock specimen (1 mm

diameter). (Lower) Shear-strain fields of the increments of loading, obtained by 3D-DIC. Figure from

Viggiani et al. (2015), used with permission.

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develop new experimental techniques to investigate the micro-scale mechanics of clay

rocks in order to feed multi-scale numerical models. Optical microscopy was used

recently by Wang et al. (2013). Viggiani and coworkers used 3D-DIC to measure the

evolution of strain fields at the micro scale from X-ray mCT images (with a spatial res-

olution of 0.7 mm) of specimens tested at ESRF (ID 19) (Figure 3, Viggiani et al., 2015).

In the second presentation given by Roseanne Murray (Durham University), the focus

was on the architecture and frictional properties of faults in shale. The main implications

from the data presented were: (1) gouges demonstrate limited ability to nucleate seismic

events. Slow fracture/fault propagation will affect the rate at which new fracture areas

are created and may limit oil and gas production. (2) Brine-saturated gouges can reduce

frictional stability locally and enhance frictional healing, in comparison to wet and dry

gouges, which facilitate oil and gas production by the creation of large fracture areas.

(3) Fluid composition may vary between basins and, thus, their rate and state properties.

Careful analysis must, therefore, be completed prior to reservoir stimulation.

Rock-mechanics studies at high resolution are very important; experimental con-

ditions are challenging and only a few groups have entered this field of research,

however.

3. Conclusions

The EUROCLAY 2015 workshop demonstrated the advanced application of experi-

mental techniques such as neutron diffraction and scattering, m-XAFS, nanoSIMS,

TEM, AFM, nano-XCT, BIB-SEM, and NMR, etc., to yield new and fundamental

insights into physical/chemical processes acting on the solid phase on a microscopic

scale, i.e. down to the molecular scale. Despite such continued advances, the lack of

standardized procedures for specific approaches to sample preparation and preservation

is evident. Further uncertainties exist surrounding ‘institutional’ codes that are used for

post-processing data, such as segmentation and image reprocessing. These very critical

steps of sample selection (representation), sample preparation, and sample preservation

prior to chemical analysis require increased attention to avoid artefacts and over-

interpretation of data. Future improvements could lead to a type of standardized protocol

for compacted clay materials, which would reduce uncertainties related to the aspects

mentioned above.

In the same manner, guidelines for data segmentation, noise filtering, and post-

processing in the form of correlation/distribution, together with a catalog of criteria

to rank the techniques available for clay systems, would optimize the scientific

output. The workshop has clearly fostered communications between experimentalists

and modelers and this needs to continue in order to clarify which kinds of data are

needed and which are available at different scales (element distribution, chemical

formula, binding environment).

Molecular-modeling techniques will allow elucidation, at an atomic scale, of the

mechanisms of radionuclide sorption onto clay minerals, of interfacial water structuring,

and of the migration behavior of solutes (anion, cation) through compacted clays. All

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these new methods will result in an improved understanding of these systems and will

help to further identify and reduce conservatism in mass transport models. Furthermore,

conceptual approaches were demonstrated throughout this workshop into how these

microscopic results may be upscaled to scales in space and time relevant to performance

assessments. This is work in progress.

Finally, the use of complementary analytical techniques has been shown to be most

successful for most of the applications, bearing in mind the limitations of each analytical

method. The interest in chemical evolution over time might, however, constrain the

application of techniques to non-destructive methods. The combination of destructive

and non-destructive methods is, however, sometimes needed to obtain full quantitative

information. It must also be stated clearly that the resolution reached so far is sometimes

insufficient to clearly discriminate different processes, but rapid instrumental develop-

ment is underway, which might overcome this problem in the near future.

Acknowledgments

The NEA Clay Club members from Belgium (FANC, ONDRAF/NIRAS, SCK . CEN),

Canada (NWMO/SGDN), France (ANDRA, IRSN), Germany (GRS, BGR, KIT-INE),

Hungary (PURAM), Japan (JAEA, NUMO), The Netherlands (COVRA), Spain

(ENRESA), Switzerland (ENSI, Nagra, University Bern), the UK (NDA), and the

United States of America (LBNL) are gratefully acknowledged for their financial or

in-kind contribution to this project. The authors are grateful for the support of the Euro-

clay organizing team, Stephen Hillier and Kevin Murphy, and the Geological Society

(UK) for student support of the workshop poster session. Those who helped by review-

ing the chapters which follow are thanked for their work and listed below, after the

reference list.

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List of Referees

Richard Anderson

Andy Aplin

Frank Bourdelle

Biqiong Chen

Pablo Cubillas

Guillaume Desbois

Katja Emmerich

Eric Ferrage

Mahnaz Firouzi

Istvan Furo

Dawn Geatches

Sylvain Grangeon

Matthias Halisch

Sabine Hartog

Jason Heath

Michael Holmboe

Stephan Kaufhold

Christopher Jeans

Ruth Kips

Catherine Lerouge

Michael Plotze

Tobias Reich

Jean-Charles Robinet

Teresa Roncal-Herrero

Benjamin Rotenberg

Michel Schlegel

Hua Shao

Christopher Spiers

James Suter

Kevin Taylor

Ilka Wallis

Christoph Weidner

Sue Wirick

Laurent Wouters

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Contents

Chapter 1. Investigation of microstructures in naturally and experimentallydeformed reference clay rocks using innovative methods in scanning electron

microscopy......................................................................................................................1

by GUILLAUME DESBOIS, SUSANNE HEMES, BEN LAURICH, MAARTJE HOUBEN,JOP KLAVER, NADINE HOHNE, JANOS L. URAI, GIOACCHINO VIGGIANI,

and PIERRE BESUELLE

1. Introduction ................................................................................................................2

2. Toolbox to investigate relevant microstructures in mudstone ..................................2

2.1. Combination of X-ray tomography, and

BIB/FIB-SEM analyses .................................................................................. 2

2.2. Preservation of hydrated microstructures by

FIB/BIB-cryo-SEM ........................................................................................ 4

2.3. Combining Wood’s metal impregnation and BIB-SEM ................................ 5

3. Applications to reference clay rocks for research ....................................................6

3.1. Microstructures in undeformed clays.............................................................. 6

3.2. Investigation of deformation mechanisms in brittle and plastic

clays deformed in the laboratory .................................................................... 8

3.3. Microstructures in a natural fault zone of Opalinus Clay

(URL, Mont Terri, Switzerland) .................................................................. 10

4. Conclusions ..............................................................................................................11

Acknowledgments ........................................................................................................12

References......................................................................................................................12

Chapter 2. Combined use of neutron-scattering, fluid-invasion, and

image-analysis techniques to assess pore structure, accessibility,

and connectivity in tight rock ....................................................................................15by CHRISTOPHER R. CLARKSON and NISAEL A. SOLANO

1. Introduction ..............................................................................................................15

2. Samples and methods ..............................................................................................20

3. Results ......................................................................................................................22

4. Discussion ................................................................................................................25

5. Conclusions ..............................................................................................................29

Acknowledgments ........................................................................................................30

References......................................................................................................................30

Chapter 3. Observations of pore systems of natural siliciclastic

mudstones ....................................................................................................................33by ANDREW C. APLIN and JULIAN K.S. MOORE

1. Introduction ..............................................................................................................33

2. Mud deposition ........................................................................................................34

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3. Mudstone grain and pore-size distributions ............................................................35

4. Pore size and permeability ......................................................................................39

5. Conclusions ..............................................................................................................41

Acknowledgments ........................................................................................................42

References......................................................................................................................42

Chapter 4. Spatially resolved quantification by NanoSIMS of organicmatter sorbed to (clay) minerals................................................................................45

by CHRISTIAN SCHURIG, THOMAS SCHRANK, CARSTEN W. MULLER, CARMEN

HOSCHEN, JOHANN LUGMEIER, LYDIA POHL, and INGRID KOGEL-KNABNER

1. Introduction ..............................................................................................................45

2. Materials and methods..............................................................................................46

2.1. Sample material ............................................................................................ 46

2.2. Bulk analyses ................................................................................................ 46

2.3. SEM and NanoSIMS analyses ...................................................................... 47

2.4. Data analysis: scaling factors ........................................................................ 47

3. Results and discussion..............................................................................................48

4. Conclusions ..............................................................................................................49

Acknowledgments ........................................................................................................51

References......................................................................................................................51

Chapter 5. High-speed, coupled micro-beam XRD/XRF/XAFS mappingat GSECARS: APS Beamline 13-ID-E......................................................................53

by ANTONIO LANZIROTTI, MATT NEWVILLE, LORI MANOUKIAN, and KARINA LANGE

1. Introduction ..............................................................................................................53

2. Materials and methods..............................................................................................54

3. Results and discussion..............................................................................................57

3.1. McClean lake tailings management facility, Saskatchewan, Canada .......... 57

3.2. Lagunas Norte Au-Ag-Cu Mine, Peru .......................................................... 60

Conclusions....................................................................................................................63

Acknowledgments ........................................................................................................63

References......................................................................................................................63

Chapter 6. Microscopic X-ray imaging techniques applied to mineralsystems and catalyst particles ....................................................................................65

by J.F.W. MOSSELMANS, C.I. PEARCE, W.R. BOWER, R.A.D. PATTRICK,

S.W.T. PRICE, A.M. BEALE, A.P. SIMS, and L. BARRIO

1. Introduction ..............................................................................................................65

2. Experimental ............................................................................................................67

2.1. Phyllosilicates ................................................................................................ 67

2.2. Catalysts ........................................................................................................ 67

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3. Results and discussion..............................................................................................69

3.1. Biotite ............................................................................................................ 69

3.2. Montmorillonite ............................................................................................ 71

3.3. Pt catalyst particle ........................................................................................ 72

3.4. Co catalyst particle ........................................................................................ 73

4. Summary ..................................................................................................................73

Acknowledgments ........................................................................................................75

References......................................................................................................................75

Chapter 7. Water mobility and structure in natural clay systems ........................79by MARC FLEURY, ERIC KOHLER, and LOIC BARRE

1. Introduction ..............................................................................................................79

1.1. Probing mobility with NMR techniques ...................................................... 80

2. Water in the interlayer space of smectites ..............................................................83

3. Conclusion ................................................................................................................85

Acknowledgments ........................................................................................................86

References......................................................................................................................86

Chapter 8. Multi-scale imaging and transport properties in shales from

experiments and molecular dynamics simulations ..................................................87by NATHAN WELCH, JOHN CRAWSHAW, and EDO BOEK

1. Introduction ..............................................................................................................87

2. Experimental section ................................................................................................88

3. Molecular dynamics simulation ..............................................................................92

3.1. Simulation model .......................................................................................... 93

3.2. Interaction potential model............................................................................ 93

3.3. Molecular dynamics simulations .................................................................. 94

3.4. Results: diffusion of water and cations ........................................................ 95

3.5. Comparison with experimental transport coefficients .................................. 98

4. Conclusions ............................................................................................................100

Acknowledgments ......................................................................................................101

References....................................................................................................................101

Chapter 9. Microscopic chemical imaging: a key to understand ionmobility in tight formations......................................................................................105

by D. GROLIMUND, H.A.O. WANG, L.R. VAN LOON, F. MARONE, N. DIAZ,

A. KAESTNER, and A. JAKOB

1. Introduction ............................................................................................................105

2. Microscopic chemical imaging ..............................................................................1063. Chemical imaging of ion mobility in tight formations..........................................108

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3.1. One-dimensional reactive transport pattern ................................................ 108

3.2. Two-dimensional reactive transport pattern .............................................. 109

3.3. Three-dimensional reactive transport pattern ............................................ 114

4. Neutron imaging ....................................................................................................119

5. Conclusions and outlook ........................................................................................121

Acknowledgments ......................................................................................................122

References....................................................................................................................123

Chapter 10. Upscaling electrokinetic transport in clays with lattice

Boltzmann and pore network models......................................................................129

by AMAEL OBLIGER, MARIE JARDAT, DANIEL COELHO, SAMIR BEKRI, andBENJAMIN ROTENBERG

1. Introduction ............................................................................................................129

2. Electrokinetics at the sample scale ........................................................................131

3. Electrokinetics on the pore scale ..........................................................................131

4. Numerical homogenization via a pore network model ........................................132

5. Transport coefficients at the sample scale ............................................................133

6. Conclusion ..............................................................................................................133

Acknowledgments ......................................................................................................134

References....................................................................................................................134

Chapter 11. Impact of microstructure on anion exclusion in

compacted clay media ..............................................................................................137

by CHRISTOPHE TOURNASSAT, STEPHANE GABOREAU, JEAN-CHARLES ROBINET,IAN C. BOURG, and CARL I. STEEFEL

1. Introduction ............................................................................................................137

2. Poisson-Boltzmann models of ion distribution in the

electrical double layer ............................................................................................138

2.1. Non-overlapping diffuse layer in 1:1

electrolyte (e.g. NaCl) ................................................................................ 138

2.2. Compacted clay systems with overlapping

diffuse layers in 1:1 electrolyte .................................................................. 139

2.3. Clay systems with multivalent or high-salinity electrolytes ...................... 140

3. Microstructural parameters affecting macroscopic

ion distribution........................................................................................................140

3.1. Porosity calculation: where the solid ends and the

pore begins .................................................................................................. 140

3.1.1. Mean layer density .......................................................................... 140

3.1.2. Effective thickness of hydrated clay layers .................................... 142

3.2. Distance of closest approach and total exclusion volumes ........................ 142

3.3. Pore-size distribution .................................................................................. 143

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4. Sensitivity of anion-exclusion predictions to microstructural

parameters ..............................................................................................................143

4.1. Modeling strategy ........................................................................................ 143

4.2. Ion-concentration distribution in compacted

montmorillonite samples ............................................................................ 144

4.3. Ion-concentration distribution in compacted illite samples........................ 146

5. Conclusions ............................................................................................................147

Acknowledgments ......................................................................................................147

References....................................................................................................................148

Chapter 12. On the use and abuse of N2 physisorption for thecharacterization of the pore structure of shales ....................................................151

by PIETER BERTIER, KEVIN SCHWEINAR, HELGE STANJEK, AMIN GHANIZADEH,

CHRISTOPHER R. CLARKSON, ANDREAS BUSCH, NIKO KAMPMAN, DIRK PRINZ,ALEXANDRA AMANN-HILDENBRAND, BERNHARD M. KROOSS, and VITALIY PIPICH

1. Introduction ............................................................................................................151

2. Principles of N2 physisorption ..............................................................................152

3. Data-processing methods and their applicability

to shale samples......................................................................................................153

4. The conundrum of low-pressure hysteresis ..........................................................155

5. Comparison of results from N2 physisorption with those

from other methods ................................................................................................157

5.1. Materials and methods ................................................................................ 157

6. Results ....................................................................................................................159

7. Summary and conclusions......................................................................................159

Acknowledgments ......................................................................................................160

References....................................................................................................................160

Chapter 13. Comparison of methods for the determination of the pore

system of a potential German gas shale..................................................................163by S. KAUFHOLD, G. GRATHOFF, M. HALISCH, M. PLOTZE, J. KUS, K. UFER,

R. DOHRMANN, S. LADAGE, and CH. OSTERTAG-HENNING

1. Introduction ............................................................................................................1642. Materials and methods............................................................................................167

3. Results ....................................................................................................................170

3.1. Characterization of the samples .................................................................. 170

3.2. Direct methods ............................................................................................ 173

3.2.1. m-CT ................................................................................................ 173

3.2.2. FIB .................................................................................................... 176

3.3. Indirect methods .......................................................................................... 179

4. Discussion ..............................................................................................................180

5. Summary and conclusions......................................................................................185

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Acknowledgments ......................................................................................................187

References....................................................................................................................187

Chapter 14. Microstructural insights into the petrophysical characteristicsof indurated clays ......................................................................................................191

by P. MARSCHALL, L. KELLER, S.B. GIGER, and J. BECKER

1. Introduction ............................................................................................................191

2. Geotechnical characteristics of the Opalinus Clay ................................................192

3. Results and discussion............................................................................................192

3.1. Porosity and pore-size distribution.............................................................. 195

3.2. Grain-size distribution and mineralogical composition.............................. 196

3.3. Deformation behavior.................................................................................. 196

4. Summary and conclusions......................................................................................197

Acknowledgments ......................................................................................................198

References....................................................................................................................198

Chapter 15. Hydration of Febex bentonite as observed by environmental

scanning electron microscopy (ESEM) ..................................................................199by FRANK FRIEDRICH, DIETER SCHILD, PETER G. WEIDLER,

and THORSTEN SCHAFER

1. Introduction ............................................................................................................199

2. Materials and methods............................................................................................200

2.1. Material ........................................................................................................ 200

2.2. Environmental scanning electron microscopy (ESEM).............................. 201

3. Results and discussion............................................................................................204

4. Summary and conclusions......................................................................................208

Acknowledgments ......................................................................................................209

References....................................................................................................................209

Chapter 16. Porosity evolution in the chalk: An example from thechalk-type source rocks of the Outer Carpathians (Poland)................................211

by KATARZYNA GORNIAK

1. Introduction ............................................................................................................211

2. Materials and methods............................................................................................212

3. Results and discussion............................................................................................213

3.1. Mineralogical analysis (XRD, optical microscopy,

FESEM/BSE) .............................................................................................. 213

3.2. Petrography (optical microscopy, FESEM/BSE/CCI) .............................. 214

3.3. Deposition and diagenesis .......................................................................... 215

3.4. Compaction.................................................................................................. 215

3.5. Porosity ........................................................................................................ 215

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4. Summary and conclusions......................................................................................216

Acknowledgments ......................................................................................................217

References....................................................................................................................217

Chapter 17. The internal architecture and permeability structures offaults in shale formations..........................................................................................219

by PIERRE DICK, CHARLES WITTEBROODT, CHRISTELLE COURBET, JUUSO

SAMMALJARVI, IMENE ESTEVE, JEAN-MICHEL MATRAY, MARJA SIITARI-KAUPPI,MIKO VOUTILAINEN, and ALEXANDRE DAUZERES

1. Introduction ............................................................................................................219

2. Materials and methods............................................................................................221

3. Results and discussion............................................................................................223

3.1. Fault architecture ........................................................................................ 223

3.2. Porosity ........................................................................................................ 224

3.3. Mineralogy .................................................................................................. 226

3.4. Hydraulic pulse-tests .................................................................................. 226

4. Summary and conclusions......................................................................................227

Acknowledgments ......................................................................................................228

References....................................................................................................................228

Chapter 18. Monitoring water-chemistry evolution in the bentonite

buffer using magnets: Effects of corrosion on buffer stability ............................231

by NICOLA RIGONAT, CHRISTIAN MAVRIS, SIMON HARLEY, and IAN B. BUTLER

1. Introduction ............................................................................................................231

2. Materials and methods............................................................................................232

3. Results and discussion............................................................................................233

4. Summary and conclusions......................................................................................238

Acknowledgments ......................................................................................................239

References....................................................................................................................239

Chapter 19. Clay-based modeling approach to diffusion and sorption in the

argillaceous rock from the Horonobe URL: Application to Ni(II), Am(III),and Se(IV) ..................................................................................................................241

by YUKIO TACHI, TADAHIRO SUYAMA, KENJI YOTSUJI, YASUO ISHII, and

HIROAKI TAKAHASHI

1. Introduction ............................................................................................................241

2. Experimental and results ........................................................................................242

3. Modeling and discussion ........................................................................................244

Acknowledgments ......................................................................................................249

References....................................................................................................................249

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Chapter 20. Diffusion model considering multiple pore structures incompacted bentonite..................................................................................................251

by KENJI YOTSUJI, YUKIO TACHI, and TAKAHIRO OHKUBO

1. Introduction ............................................................................................................251

2. Modeling approach ................................................................................................252

3. Results and discussion............................................................................................255

Acknowledgments ......................................................................................................256

References....................................................................................................................256

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