A KINEMATIC HARDENING MODEL WITH DEGRADATION OF STRUCTURE – APPLICATION TO SOFT NATURAL CLAYS Béatrice A Baudet University College London.

Slides:



Advertisements
Similar presentations
1 MAJOR FINDINGS OF THE PROJECT AND THEIR POSSIBLE INCLUSION IN EUROPEAN STANDARD -Major findings -Major findings suitable for inclusion in European Standard.
Advertisements

A. Mellal & Ph. Bellwald Implementation of a constitutive law in Z_Soil Z_Soil Day, 27 August 2007, Lausanne, Switzerland Aïssa Mellal, GeoMod.
6. Settlement of Shallow Footings
Investigation of Consolidation Promoting Effect by Field and Model Test for Vacuum Consolidation Method Nagasaki University H.Mihara Y.Tanabasi Y.Jiang.
4.3 STONE OR SAND COLUMNS IN SOFT CLAYEY MATERIALS :
Course : S0705 – Soil Mechanic
An Experimental Study and Fatigue Damage Model for Fretting Fatigue
TensiNet Symposium SOFIA 2010 – Tensile Architecture: Connecting Past and Future September 2010, Sofia, Bulgaria Biaxial testing of architectural.
Non-Linear Hyperbolic Model & Parameter Selection Short Course on Computational Geotechnics + Dynamics Boulder, Colorado January 5-8, 2004 Stein Sture.
Pore Pressure Coefficients
Impacts of Seismic Stress on Pore Water Pressure in Clayey Soil By: Qazi Umar Farooq Lecturer Civil Engineering Dept Univ of Engg & Tech Taxila.
Shear Strength of Soils
In Tai Kim & Erol Tutumluer University of Illinois, Urbana-Champaign
OUTLINE SPATIAL VARIABILITY FRAGILITY CURVES MONTE CARLO SIMULATIONS CONCLUSIONS EFFECTS DESIGN RECOMMEND BEARING CAPACITY OF HETEROGENEOUS SOILS APPENDIXOUTLINE.
Determination of Soil Stiffness Parameters
Lecture 8 Elements of Soil Mechanics
Modeling of CNT based composites: Numerical Issues
MICROSCOPIC STUDY ON SHANGHAI SATURATED SOFT CLAY’S DYNAMIC BEHAVIOR By Tang Yi-qun, Zhang Xi, Zhao Shu-kai Tongji University, China.
1 Asia Managing Geotechnical Risk Learning from the Failures “Issues related to the use of Numerical Modelling in Design of Deep Excavations in Soft Clay”
Paper: OSP-17 V.S. Pillai & B. Muhunthan THE FAILURE OF TETON DAM – A NEW THEORY BASED ON "STATE BASED SOIL MECHANICS"
Soil mechanics – a short introduction
Shear Strength of Soil τf = c + σ’ tan φ τf = shear strength
Characterization of 1mm lead-free joints. Test results (DIC 2D)
Shear Strength of Cohesive (Clay) Soil
Session 17 – 18 PILE FOUNDATIONS
What is compaction? A simple ground improvement technique, where the soil is densified through external compactive effort. + water = Compactive effort.
Lecture-8 Shear Strength of Soils
GEO-MECHANICS (CE2204) Shear Strength of Soils
Martin Fahey The University of Western Australia
Shear Strength of Soil By Kamal Tawfiq Fall 2007.
CEP Soil Engineering Laboratory
Ömer O. Erbay & Ahmet Çıtıpıtıoğlu 25 April 2008
Engineering Doctorate – Nuclear Materials Development of Advanced Defect Assessment Methods Involving Weld Residual Stresses If using an image in the.
CE 317 Geotechnical Engineering Dr. Tae-Hyuk Kwon
Predicting non-linear ground movements Malcolm Bolton Cambridge University, UK.
Department of Civil and Environmental Engineering, The University of Melbourne Finite Element Modelling – Element Types and Boundary Conditions (Notes.
Msc. eng. Magdalena German Faculty of Civil Engineering Cracow University of Technology Budapest, Simulation of damage due to corrosion in RC.
Amit Prashant Associate Professor Dept. of Civil Engineering Indian Institute of Technology Gadhinagar, India 5th Tongji-UBC Symposium on Earthquake Engineering,
14th Crisp user meeting at UCL1 Numerical analysis of a piled foundation in granular material using slip element Yongjoo Lee Soil Mechanics Group Department.
CHE 333 Class 14 True Stress True Strain Crystalline Processes During Deformation.
In Situ Stabilization of Pavement Base Courses Roads Pavement Forum Thursday, May 17, 2001.
Dynamic Behaviour of Unsaturated CH soil under Cyclic Loading in Unconsolidated Undrained Conditions 5th Tongji-UBC Symposium on Earthquake Engineering,
Elastic-Plastic Deformation. Simple Constitutive Relations.
Comparison of strength behavior of unidirectional HMC and HSC composite subjected to biaxial loading J. Krystek, R. Kottner, L. Bek 19 th Conference on.
Shear Strength of Soils
Unconfined Compression Test ASTM D-2166 /02
Giant landslide in Tibet 2000 Shear strength 5.1 General Shear strength 5.1 General.
Constant stress experiment ductile elastic Constant stress (strain varies) Constant strain (stress varies)
Numerical analysis of Concrete Face Rockfill Dams based on Lade’s model and gradient plasticity P. Dakoulas, E. Stavrotheodorou, A. Giannakopoulos University.
Consolidation I (CH11). Consolidation Process by which an in  ’ causes a deformation of a soil mass by reducing its e (water seeps out of the voids).
School of Civil Engineering University of Nottingham Predicting the Repeated Load Behaviour of Pavement Subgrades Using the Three- surface Kinematic Hardening.
Topic 3: Constitutive Properties of Tissues
Lecture 8 Elements of Soil Mechanics
Soil Mechanics Topic – Triaxial shear test(CD, CU, UU tests)
Critical state soil mechanics in prediction of strains
Elasto-plastic Behaviour of Soft Clays Tuesday, 5 th December– 1b.
Lecturer: Dr. Frederick Owusu-Nimo
Shear Strength of Soil.
Nanocomposite Materials Laboratory
Stress-strain behaviour
Slope stability of the “Corniche Ouest” of the Dakar
True Stress True Strain Crystalline Processes During Deformation.
( BDA 3033 ) CHAPTER 6 Theories of Elastic Failures
Bituminous-faced Rockfill Dam Seismic Performance Prediction of stress-strain behaviour and potential damages Proposal for the 15th International Benchmark.
Continuous and discrete models for simulating granular assemblies
Visco-plastic self-consistent modeling of high strain rate and
Determination of Soil Stiffness Parameters
Elastic & Plastic behavior of Materials
Instability of Geological Materials under Three-Dimensional Stress Conditions Poul V. Lade The goal of this project is to study the conditions for instability.
lectures Notes on: Soil Mechanics
Presentation transcript:

A KINEMATIC HARDENING MODEL WITH DEGRADATION OF STRUCTURE – APPLICATION TO SOFT NATURAL CLAYS Béatrice A Baudet University College London

INTRODUCTION  Natural clays have a different microstructure or structure to that of clays reconstituted in the laboratory.  In most clays, particularly soft clays, this structure breaks with plastic strain; this is termed destructuration.  A simple model including structure is proposed, with only three new parameters which can be derived from a single set of test data.

Cracking of roads due to settlement of soft soil foundation Failure of the Carsington dam during construction due to poor estimation of strength of the foundation clay TYPICAL PROBLEMS ASSOCIATED WITH CONSTRUCTION ON SOFT NATURAL CLAYS

stress displacement destructuration EFFECTS OF STRUCTURE ON THE BEHAVIOUR OF SOFT CLAYS soil element undisturbed disturbed Schematic behaviour

SOFT NATURAL CLAYS  Shear strength < 50kPa  Structure: combination of - fabric (stable elements) - bonding (unstable elements)

THE S3-SKH MODEL  Based on an existing model, the 3-SKH model, developed for stiff clays with a stable structure (Stallebrass & Taylor, 1997)  All effects of structure described by the size of the state boundary surface

NCL (S t = 1) SCL 2 p 0 2 s. p 0 ln p specific volume current sensitivity, s sensitivity at yield compression of intact clay  s: exponential function decreasing with  Three new parameters: s 0, s f, k that can be derived from a single isotropic compression test s s0s0 sfsf pp

CSL Experimental data (from Allman, 1992) Predicted data  Stiffness successfully simulated at small strain  Undrained shear strength correctly predicted  Post-peak, comparison of predicted and test data complicated

v lnp′p′p′p* ie  Reversal in normalised stress path direction: definition of a limit surface  Rate of destructuration with plastic strain consistent with experimental results iso-NCL*

CONCLUSIONS  A simple model including structure in the size of the state boundary surface is sufficient to describe the behaviour of natural soils in triaxial space  The new model (S3-SKH model) requires only three additional parameters to the base model which can be derived from a single isotropic test  Need to investigate how soil structure degrades in general stress space and whether the features of behaviour found in general stress space can be generated by simply extrapolating the model from axisymmetric to general space