Desiccation Cracking of Soils

Similar documents
Drying shrinkage of deformable porous media: mechanisms induced by the fluid removal

Constitutive modelling of the thermo-mechanical behaviour of soils

Computational Geomechanics COMGEO I

EXPERIMENTAL AND COMPUTATIONAL MODELING OF UNSATURATED SOIL RESPONSE UNDER TRUE TRIAXIAL STRESS STATES

Fundamentals of desiccation cracking of finegrained soils: experimental characterisation and mechanisms identification

STUDY OF THE BARCELONA BASIC MODEL. INFLUENCE OF SUCTION ON SHEAR STRENGTH

On the water retention behaviour of shales

Geotechnical Properties of Soil

Geology 229 Engineering Geology. Lecture 5. Engineering Properties of Rocks (West, Ch. 6)

Farimah MASROURI. Professor in Geotechnical Engineering. LAEGO : Research Center In Geomechanics & Geoenvironmental Engineering

Module 5: Failure Criteria of Rock and Rock masses. Contents Hydrostatic compression Deviatoric compression

Table of Contents Chapter 1 Introduction to Geotechnical Engineering 1.1 Geotechnical Engineering 1.2 The Unique Nature of Soil and Rock Materials

POSSIBILITY OF UNDRAINED FLOW IN SUCTION-DEVELOPED UNSATURATED SANDY SOILS IN TRIAXIAL TESTS

TIME-DEPENDENT BEHAVIOR OF PILE UNDER LATERAL LOAD USING THE BOUNDING SURFACE MODEL

Lecture #7: Basic Notions of Fracture Mechanics Ductile Fracture

GEO E1050 Finite Element Method Mohr-Coulomb and other constitutive models. Wojciech Sołowski

Ch 4a Stress, Strain and Shearing

Petroleum Geomechanics for Shale Gas

Numerical Simulation of Unsaturated Infilled Joints in Shear

Cyclic Triaxial Behavior of an Unsaturated Silty Soil Subjected to Suction Changes

Cubzac-les-Ponts Experimental Embankments on Soft Clay

Stress and Strains in Soil and Rock. Hsin-yu Shan Dept. of Civil Engineering National Chiao Tung University

Shear strength. Common cases of shearing In practice, the state of stress in the ground will be complex. Common cases of shearing Strength

NUMERICAL ANALYSIS OF DESICCATION, SHRINKAGE AND CRACKING IN LOW PLASTICITY CLAYEY SOILS

General method for simulating laboratory tests with constitutive models for geomechanics

PRINCIPLES OF GEOTECHNICAL ENGINEERING

Advanced model for soft soils. Modified Cam-Clay (MCC)

Shear Strength of Soils

MODELING OF GAS MIGRATION THROUGH LOW-PERMEABILITY CLAY USING INFORMATION ON PRESSURE AND DEFORMATION FROM FAST AIR INJECTION TESTS

Laboratory 4 Bending Test of Materials

GEOMECHANICAL MODELING OF THE STEINERNASE LANDSLIDE Alessio Ferrari, Lyesse Laloui and Christophe Bonnard

Interpretation of soil-water characteristic curves when volume change occurs as soil suction is changed

Soil strength. the strength depends on the applied stress. water pressures are required

Numerical model comparison on deformation behavior of a TSF embankment subjected to earthquake loading

Teaching Unsaturated Soil Mechanics as Part of the Undergraduate Civil Engineering Curriculum

Rock Mechanics Laboratory Tests for Petroleum Applications. Rob Marsden Reservoir Geomechanics Advisor Gatwick

Hypoplastic Cam-clay model

Experimental and theoretical characterization of Li 2 TiO 3 and Li 4 SiO 4 pebbles

A multi-cell extension to the Barcelona Basic Model

Finite element formulation and algorithms for unsaturated soils. Part II: Verification and application

SHEAR STRENGTH OF SOIL

An effective stress based model for the dependency of a water retention curve on void ratio

Unified Constitutive Model for Engineering- Pavement Materials and Computer Applications. University of Illinois 12 February 2009

Lateral Earth Pressure

1.8 Unconfined Compression Test

A Constitutive Framework for the Numerical Analysis of Organic Soils and Directionally Dependent Materials

Elastoplastic modelling of hydraulic and stress strain behaviour of unsaturated soils

Unsaturated Flow (brief lecture)

3D simulations of an injection test done into an unsaturated porous and fractured limestone

Prediction of torsion shear tests based on results from triaxial compression tests

Interpreting measurements of small strain elastic shear modulus under unsaturated conditions

1. Background. is usually significantly lower than it is in uniaxial tension

Intro to Soil Mechanics: the what, why & how. José E. Andrade, Caltech

Physical and mechanical properties of decomposed granite soils sampled in Cheongju, Korea

FCP Short Course. Ductile and Brittle Fracture. Stephen D. Downing. Mechanical Science and Engineering

A Thermo-Hydro-Mechanical Damage Model for Unsaturated Geomaterials

Rock Material. Chapter 3 ROCK MATERIAL HOMOGENEITY AND INHOMOGENEITY CLASSIFICATION OF ROCK MATERIAL

Plasticity R. Chandramouli Associate Dean-Research SASTRA University, Thanjavur

Table of Contents. Foreword... xiii Introduction... xv

Constitutive modelling of fabric anisotropy in sand

Pillar strength estimates for foliated and inclined pillars in schistose material

Hydro-mechanical response of collapsible soils under different infiltration events

20. Rheology & Linear Elasticity

A simple elastoplastic model for soils and soft rocks

Hardened Concrete. Lecture No. 16

Calculation of 1-D Consolidation Settlement

Experimental study of the hydromechanical coupling in argillaceous rocks: the example of Boom clay

Modelling of shear stiffness of unsaturated fine grained soils at very small strains

16 Rainfall on a Slope

Application of a transversely isotropic brittle rock mass model in roof support design

Micromechanics-based model for cement-treated clays

The CPT in unsaturated soils

INTERPRETATION OF UNDRAINED SHEAR STRENGTH OF UNSATURATED SOILS IN TERMS OF STRESS STATE VARIABLES

Volume Change Consideration in Determining Appropriate. Unsaturated Soil Properties for Geotechnical Applications.

Tectonics. Lecture 12 Earthquake Faulting GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD

The Effects of Different Surcharge Pressures on 3-D Consolidation of Soil

Modelling the excavation damaged zone in Callovo-Oxfordian claystone with strain localisation

Study of the behavior of Tunis soft clay

2.7 Shear Strength of Unsaturated Soils

Testing of an expansive clay in a centrifuge permeameter

SOIL MODELS: SAFETY FACTORS AND SETTLEMENTS

Chapter (12) Instructor : Dr. Jehad Hamad

Lecture #8: Ductile Fracture (Theory & Experiments)

Determination of Poisson s Ratio of Rock Material by Changing Axial Stress and Unloading Lateral Stress Test

Soil Mechanics for Unsaturated Soils

2017 Soil Mechanics II and Exercises Final Exam. 2017/7/26 (Wed) 10:00-12:00 Kyotsu 4 Lecture room

Anisotropy of Shale Properties: A Multi-Scale and Multi-Physics Characterization

Constitutive models for geotechnical practice

MEMORANDUM SUBJECT: CERTIFICATE IN ROCK MECHANICS PAPER 1 : THEORY SUBJECT CODE: COMRMC MODERATOR: H YILMAZ EXAMINATION DATE: OCTOBER 2017 TIME:

Homework Problems. ( σ 11 + σ 22 ) 2. cos (θ /2), ( σ θθ σ rr ) 2. ( σ 22 σ 11 ) 2

Chapter 1 - Soil Mechanics Review Part A

EOSC433: Geotechnical Engineering Practice & Design

Assessment of swelling deformation of unsaturated kaolinite clay

G1RT-CT D. EXAMPLES F. GUTIÉRREZ-SOLANA S. CICERO J.A. ALVAREZ R. LACALLE W P 6: TRAINING & EDUCATION

Advanced Numerical Study of the Effects of Road Foundations on Pavement Performance

PLASTICITY FOR CRUSHABLE GRANULAR MATERIALS VIA DEM

University of Sheffield The development of finite elements for 3D structural analysis in fire

Rapid Characterization of Unsaturated Soils using Simple Equipment. Xiong Zhang, Ph.D., P.E. August 12, 2016

Anisotropic behaviour of compacted clayey silt subjected to hydromechanical paths

The Influence of Contact Friction on the Breakage Behavior of Brittle Granular Materials using DEM

Transcription:

Desiccation Cracking of Soils Lyesse Laloui Hervé Péron, Tomasz Hueckel, Liangbo Hu Ecole Polytechnique Fédérale de Lausanne Switzerland Duke University, NC USA

The consequences of desiccation cracking Affects the stability of earthen structures Argiles.fr Dramatic increase of the permeability of engineered clay buffer for nuclear waste storage a major challenge in geotechnical engineering. Dramatic increase of the permeability of landfill clay liner

Scope of the presentation 1. To find out the hypothetical mechanisms (uncertain) and the controlling parameters of desiccation and desiccation cracking. 2. To formulate a mechanical constitutive model to predict the conditions for cracking initiation and to propose some tools for a correct modelling of desiccation crack extension.

Introduction Basic Processes Drying = loss of soil liquid evaporated to a drier environment. Loss (evaporation) of water / suction increase / effective stress increase mass shrinkage (free shrinkage) If shrinkage is constrained, reaction forces arise. tensile stresses are built up tensile strength is reached desiccation cracks can appear and propagate. Three main causes of shrinkage constraint: (1) Boundary restraint (2) Moisture gradients inside the body (3) Internal structure

-1- Experimental characterization and phenomenological study of desiccation cracking process

1. Exp. chara. and phenom. study Bioley silt La Frasse clay Rock powder Sion silt Presentation of materials (1/2) CM Clay = 25 % (with smectite) W L = 32 % / W P = 17 % CM Clay = 29 % (with smectite) W L = 31 % / W P = 20 % CL Almost no clay minerals W L = 30.7 % / W P = 20.3 % CL Clay = 8 % (with almost no smectite) W L = 25.4 % / W P = 16.7 % Preparation: saturated slurry Aim: air bubble removal + no structure

1. Exp. chara. and phenom. study WRC determined in pressure extractor (axis translation technique) with zero mechanical stress. Presentation of materials (2/2) Domain 1 Domain 2 Water retention properties Domain 1: deformation are mostly irreversible (large during the first drying). Threshold = shrinkage limit / air entry value Domain 2: deformation are reversible (very small). S r -s e - w Geotechnical Testing Journal, vol. 30, N 1, pp. 1-8, 2007 e - s w -s

1. Exp. chara. and phenom. study Free desiccation tests 5 cm30 cm Drying of Bioley silty clay cakes without any boundary constraint (Teflon support). Measurement of: total water content - weighing water content repartition - sampling strains - calipers Desiccation test procedures Constrained desiccation tests Drying is performed with controlled temperature and relative humidity Drying of Bioley silty clay cakes with axial bottom restraint (notches). Measurement of: cracking suction tensiometer, cracking water content - sampling and weighing, strains calipers, crack opening image analysis. Use of different liquids (water, ethanol solution or ethylene glycol) and different soils (Bioley silt, Sion silt and rock powder).

1. Exp. chara. and phenom. study α Free desiccation test results - NO CRACK - Bioley silt + water Water content repartition: only small moisture gradients. No large discrepancy between these tests and WRC with pressure extractor. Varying soils + liquids Shrinkage with Bioley silt is higher than with rock powder Water involves the largest amount of shrinkage, ethanol the lowest. Rock powder is less compressible than Bioley silt. Clay wetted with alcohol is much less compressible than when wetted with water. Surface tension plays a major role in the shrinkage process

1. Exp. chara. and phenom. study Constrained desiccation test results (1/2) General observations CRACKING Reproducible pattern of 6-8 parallel cracks perpendicular to the direction of constraint. Cracking occurs in a noticeably narrow w range.

1. Exp. chara. and phenom. study Constrained desiccation test results (2/2) Suction and saturation ratio at cracking Cracking occurs in Domain 1, close to the air entry value and the onset of desaturation. La Frasse clay Sion silt Cracking Cracking Flaws can be attributed to the formation of unsaturated zones between this irregularity and a potential crack [Scherer 1990]. analogy

-2- Experimental determination of tensile strength

Tensile strength determination Tests by the triaxial traction method Performing extension with an adapted sample shape: creation of a traction in the mid-section. [Bishop and Garga 1969] Principle Method : 1. Iso. consolidation OC. 2. Deconsolidation CD. 3. Cutting. 4. ( Suction imposition). 5. Extension DT 2. A σ,min 1 E C = σ A C radial Suction imposition technique: s 50 kpa: water sub-pressure s = 100 kpa: axis translation

Tensile strength determination Tests by the triaxial traction method σ = σ 3 t (compression) ( ) q = p σ 3 t Main points: 1. At s = 0 kpa, remoulded Bioley silt cannot sustain significant tensile stress cut-off 2. As suction increases, negative net stress can be experienced and brittle failure is promoted. At low stresses, tensile failure become apparent. 3. The criterion is shifted towards positive values of effective stress as suction increases.

-3- Constitutive modelling for soils subjected to desiccation

Constitutive modelling What we aim at modelling Key point 1: Domain 1: shrinkage mostly irrecoverable, follows NCL. Domain 2: residual shrinkage, recoverable. Elasto-plastic constitutive approach. Key point 2: Desiccation cracks in initially saturated remolded soil occur in Domain 1. Key point 3: Desiccation crack essentially mode I failure. Crack must be described with a tensile failure criterion. Key point 4: The tensile failure criterion should be expressed in effective stress. Key point 5: The tensile failure criterion depends on suction. Existing models: can fall in several categories (i) Do not use effective stress and elasto-plasticity. (ii) Model only Domain 1 (use of Terzaghi s effective stress) in simplified conditions. None of them features a tensile failure criterion (points 3, 4 and 5).

Constitutive modelling Constitutive modelling Uses the Bishop s generalized effective stress: σ = σ p I+ S ( p p ) I g r g l Effective Stress Concept in Unsaturated Soils: Clarification and Validation of a Unified Framework. International Journal of Numerical and Analytical Methods in Geomechanics, 2008. Uses the original Hujeux model: Strain hardening elasto-plastic constitutive model, based on the critical state concept Elastic part e dp e dq dε v = dε d = K p 3G( p ) ( ) Two plastic mechanisms: dε = dε δ + dε p p, iso p, dev ij ij ij Isotropic Deviatoric (non-associated) Hardening law: f = p' p r iso c iso p' fdev = q Mp'1 b log rdev = 0 p CR ( ) exp p p = p 0 βε c c v Remark: with the generalized effective stress concept, the CSL always meets the axis origin, whatever the suction is.

Constitutive modelling c0 p ( βε v ) p ( βεv ) p = p exp if s s c p = p exp 1+ if s> s c 0 γ s log s s c Constitutive modelling E E E Extension to unsaturated case Above air entry value, there is an increase of preconsolidation pressure due to suction: This makes possible simulation of Domains 1 and 2. Changes of saturation ratio with suction are managed with van Genuchten relation: S r 1 = n s 1 + ( αss) m s

Constitutive modelling Proposition of a tensile failure criterion (1/2) A tensile failure criterion is required to model desiccation cracks: 5 batches of tensile tests of the literature + present study are used to determine it Present study S r = 1 Sr < 1 Proposition of a law for tensile strength evolution with suction: sat ks 1 σ t = σ t + k2 1 exp k2 Significance of the parameters: S r = 1

Constitutive modelling Proposition of a tensile failure criterion (2/2) The following criterion is adopted: σ = σ 3 t Griffith criterion For compression state, it defines a line of slope 3 in the q-p plane. The form of the criterion in the circled zone is only inferred.

Constitutive modelling Free desiccation Activation of the isotropic mechanism through an increase of mean effective stress Model typical features Constrained desiccation: case of a soil column with lateral strain restriction, 2 1 3 One can manage constrained desiccation with a degree of shrinkage restraint X r r ( 1 ) dε = X dε s 3 imp 3 3 Influence of vertical load

Constitutive modelling Validation (1/3) Parameters determined with our consolidation, CTC, WRC, and traction tests on Bioley silt: Elastic K ref [MPa] / G ref [MPa] / n [-] 212.2 / 98 / 0.69 Plastic β sat [-] / φ [-] / C [ ] / φ E [ ] / d[-] / p CR0 [kpa] 24.5 / 31.5 / 25 / 2 / 5 Tensile failure σ t sat [kpa] / k 1 [-] / k 2 [kpa] -6 / 0.72 / 5x10 2 Unsat. mechanical and water retention behaviour s E [kpa] / γ s [-] 120 / 7 α s [-] / n s [-] / m s [-] 4x10-6 / 1.8 / 0.24 Desiccation tests (present study) Simulation of pressure plate tests (and free desiccation tests) : NO CRACK,

Constitutive modelling Validation (2/3) Desiccation tests (present study) Constrained desiccation: the loading of the simulation is the measured strain field (vertical / axial / transversal) during the constrained desiccation tests. [-] / CRACK The suction at which the first crack appears is fairly predicted (corresponds to the measured value). The corresponding saturation ratio is almost equal to 100%.,

Constitutive modelling Soil: mining waste (ML low plasticity silt) [-] / Validation (3/3) Tests of Rodriguez et al. (2007) Tests performed: WRC in K0 conditions, Uniaxial traction test at various suctions Air drying of thin slabs on grooved surface Back predictions: Simulation of constrained desiccation: WRC Tensile tests, Good correspondance with exp. cracking suction.

Conclusions (1/2) 1. Mechanisms of desiccation crack initiation: Existence of two domains of drying shrinkage with distinct behaviours. Cracking of initially remoulded saturated soil occurs when Sr is still close to unity. Tensile strength (expressed with effective stress) increases with suction and is shifted towards positive values. There must be a relationship between the tensile strength, the fluid pressures and the degree of saturation. In the test conditions, such variables are critical close to air entry value. Crack pattern geometry (such as crack spacing and interception) is the result of energy redistribution.

Conclusions & outlooks 2. Constitutive modelling: Conclusions (2/2) A tensile failure criterion depending on the suction level has been developed and validated. The Originality and strength of the model: to combine advanced concept of effective stress and constitutive approach for unsaturated soils with tensile failure. Shrinkage / suction / stress / strength and cracking are included in a unified framework. 3. Desiccation crack propagation: In progress XFEM and DEM 100 kpa 20 kpa

Thank you for your attention

1. Exp. chara. and phenom. study Constrained desiccation test results (4/4) First possibility: global considerations at the scale of the entire bar, considering a homogeneous stress field. Energy U stored during constrained deformation: How to explain it? Conservation of energy: equalling both terms: U = ELhl m ( ε ) 2 x 2 N C Energy W s required to form the pattern of N crack: E L = G c Crack pattern formation h ( ε ) 2 x 2 W = N a lg s c cf c Second possibility: Stress analysis: the first crack split the bar in two new bars, this process is resumed to create higher order crack, until total stress release.