Numerical optimisation to obtain elastic viscoplastic model parameters for soft clay

In this paper, a numerical optimisation procedure is presented to obtain non-linear elastic viscoplastic (EVP) model parameters adopting the available consolidation data. The Crank–Nicolson finite difference scheme is applied to solve the combination of coupled partial differential equations of the EVP model and the consolidation theory. Then, the model parameters are determined applying the trust-region reflective optimisation algorithm in conjunction with the finite difference solution. The proposed solution for the model parameter determination can utilise all available consolidation data during the dissipation of the excess pore water pressure to determine the required model parameters. Moreover, in order to include creep in the numerical predictions explicitly from the very first time steps, the reference time in the elastic viscoplastic model can readily be adopted as a unit of time. Results obtained from two sets of laboratory experiments adopting hydraulic consolidation (Rowe cells) on a soft soil are reported and discussed. The proposed numerical optimisation procedure is utilised to obtain the viscoplastic model parameters adopting the experimental results, while the settlement and pore water pressure predictions are compared with experimental results to evaluate the accuracy and reliability of the proposed numerical procedure. The predictions are in good agreement with the measurements, supporting the proposed numerical method as a practical tool to analyse the stress–strain behaviour of soft clay.

[1]  Ya-Xiang Yuan,et al.  Gradient Methods for Large Scale Convex Quadratic Functions , 2010 .

[2]  George Z. Voyiadjis,et al.  Finite element analysis of the piezocone test in cohesive soils using an elastoplastic–viscoplastic model and updated Lagrangian formulation , 2003 .

[3]  Abebe Geletu,et al.  Solving Optimization Problems using the Matlab Optimization Toolbox - a Tutorial , 2007 .

[4]  Fusahito Yoshida,et al.  Inverse approach to identification of material parameters of cyclic elasto-plasticity for component layers of a bimetallic sheet , 2003 .

[5]  T. Berre,et al.  OEDOMETER TESTS WITH DIFFERENT SPECIMEN HEIGHTS ON A CLAY EXHIBITING LARGE SECONDARY COMPRESSION , 1972 .

[6]  Dimitri Debruyne,et al.  Elasto-plastic material parameter identification by inverse methods: Calculation of the sensitivity matrix , 2007 .

[7]  L. Kestens,et al.  Effects of Holding Time on Thermomechanical Fatigue Properties of Compacted Graphite Iron Through Tests with Notched Specimens , 2013, Metallurgical and Materials Transactions A.

[8]  Lizhong Wang,et al.  Undrained behavior of natural marine clay under cyclic loading , 2011 .

[9]  Thu Minh Le,et al.  Soil creep effects on ground lateral deformation and pore water pressure under embankments , 2013 .

[10]  Daniel De Kee,et al.  Advanced Mathematics For Engineering And Science , 2003 .

[11]  Dallas N. Little,et al.  A thermodynamic framework for constitutive modeling of time- and rate-dependent materials. Part II: Numerical aspects and application to asphalt concrete , 2012 .

[12]  J. Shao,et al.  A unified elastic–plastic and viscoplastic damage model for quasi-brittle rocks , 2008 .

[13]  J. Qu,et al.  Parameter identification for improved viscoplastic model considering dynamic recrystallization , 2005 .

[14]  J. Yin,et al.  Non-linear creep of soils in oedometer tests , 1999 .

[15]  R. G. Robinson Consolidation analysis with pore water pressure measurements , 1999 .

[16]  James Graham,et al.  Viscous–elastic–plastic modelling of one-dimensional time-dependent behaviour of clays: Reply , 1989 .

[17]  Edward Kavazanjian,et al.  Prediction of the Performance of a Geogrid-Reinforced Slope Founded on Solid Waste , 2001 .

[18]  J. Crank,et al.  A practical method for numerical evaluation of solutions of partial differential equations of the heat-conduction type , 1947 .

[19]  Gun Jin Yun,et al.  A self-optimizing inverse analysis method for estimation of cyclic elasto-plasticity model parameters , 2011 .

[20]  Thu Minh Le,et al.  Viscous Behaviour of Soft Clay and Inducing Factors , 2012, Geotechnical and Geological Engineering.

[21]  L. Kestens,et al.  Measurement and characterization of Thermo-Mechanical Fatigue in Compacted Graphite Iron , 2013 .

[22]  Pieter A. Vermeer,et al.  A soft soil model that accounts for creep , 2019, Beyond 2000 in Computational Geotechnics.

[23]  Thomas F. Coleman,et al.  An Interior Trust Region Approach for Nonlinear Minimization Subject to Bounds , 1993, SIAM J. Optim..

[24]  J. Graham,et al.  Elastic visco-plastic modelling of one-dimensional consolidation , 1996 .

[25]  Katya Scheinberg,et al.  Introduction to derivative-free optimization , 2010, Math. Comput..

[26]  Linnan Zhu,et al.  Elastic visco-plastic analysis for earthquake response of tunnels in cold regions , 2000 .

[27]  R. H. Wagoner,et al.  A plastic constitutive equation incorporating strain, strain-rate, and temperature , 2010 .

[28]  P. W. Rowe,et al.  A New Consolidation Cell , 1966 .

[29]  Donald W. Taylor,et al.  Fundamentals of soil mechanics , 1948 .

[30]  J. Crank,et al.  A practical method for numerical evaluation of solutions of partial differential equations of the heat-conduction type , 1947, Mathematical Proceedings of the Cambridge Philosophical Society.

[31]  S. Leroueil,et al.  The permeability of natural soft clays. Part II: Permeability characteristics: Reply , 1983 .

[32]  Ayato Tsutsumi,et al.  Combined effects of strain rate and temperature on consolidation behavior of clayey soils , 2012 .

[33]  Sun-Myung Kim,et al.  Mechanistic-based constitutive modeling of oxidative aging in aging-susceptible materials and its effect on the damage potential of asphalt concrete , 2013 .

[34]  J. Shao,et al.  A micro–macro model for clayey rocks with a plastic compressible porous matrix , 2012 .

[35]  G Mesri,et al.  THE UNIQUENESS OF THE END-OF-PRIMARY (EOP) VOID RATIO-EFFECTIVE STRESS RELATIONSHIP. PROCEEDINGS OF THE ELEVENTH INTERNATIONAL CONFERENCE ON SOIL MECHANICS AND FOUNDATION ENGINEERING, SAN FRANCISCO, 12-16 AUGUST 1985 , 1985 .

[36]  Jian-Fu Shao,et al.  A micromechanical model for the elasto-viscoplastic and damage behavior of a cohesive geomaterial , 2008 .

[37]  Y. Watabe,et al.  Long-term consolidation behavior interpreted with isotache concept for worldwide clays , 2012 .

[38]  Panos M. Pardalos,et al.  Encyclopedia of Optimization , 2006 .

[39]  J. Strikwerda Finite Difference Schemes and Partial Differential Equations , 1989 .

[40]  T. Wright,et al.  A continuum framework for finite viscoplasticity , 2001 .

[41]  S. Leroueil,et al.  Permeability anisotropy of natural clays as a function of strain , 1990 .

[42]  K. G. Murty Optimization For Decision Making Linear And Quadratic Models , 2009 .

[43]  Carthigesu T. Gnanendran,et al.  Influence of using a creep, rate, or an elastoplastic model for predicting the behaviour of embankments on soft soils , 2006 .

[44]  David Nash,et al.  Modelling the Effects of Surcharge to Reduce Long Term Settlement of Reclamations over Soft Clays: A Numerical Case Study (IS-YOKOHAMA 2000「沿岸域の地盤工学における理論と実際」特集号〔英文〕) , 2001 .

[45]  Harry G. Poulos,et al.  Stress deformation and strength characteristics , 1977 .