Abstract

We develop a non-associated flow rule (NAFR)-based elasto-viscoplastic (EVP) model for isotropic clays. For the model formulation, we introduce the critical state soil mechanics theory (CSSMT), the bounding surface theory and Perzyna’s overstress theory. The NAFR based EVP model comprises three surfaces: the potential surface, the reference surface and the loading surface. Additionally, in the model formulation, assuming the potential surface and the reference surface are identical, we obtain the associated flow rule-based EVP model. Both EVP models require seven parameters and five of them are identical to the Modified Cam Clay model. The other two parameters are the surface shape parameter and the secondary compression index. Moreover, we introduce the shape parameter in the model formulation to control the surface shape and to account for the overconsolidation state of clay. Additionally, we incorporate the secondary compression index to introduce the viscosity of clay. Also, we validate the EVP model performances for the Shanghai clay, the San Francisco Bay Mud (SFBM) clay and the Kaolin clay. Furthermore, we use the EVP models to predict the long-term field monitoring measurement of the Nerang Broadbeach roadway embankment in Australia. From the comparison of model predictions, we find that the non-associated flow rule EVP model captures well a wide range of experimental results and field monitoring embankment data. Furthermore, we also observe that the natural clay exhibits the flow rule effect more compared to the reconstituted clay.

Highlights

  • In a saturated clay medium, the liquid phase occupies the interparticle void spaces of the solid phase

  • We develop a non-associated flow rule-based elasto-viscoplastic (EVP) model considering the Modified Cam Clay (MCC) model [10] framework, Perzyna’s overstressed theory [16], the Borja and Kavazanjian [17] concept, the bounding surface theory and the mapping rule

  • We observe similar results for 200 kPa. Comparing both the flow rule EVP model and the Kutter and Sathialingam [27] model, we find that the non-associated flow rule model well captures the experimental results

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Summary

Introduction

In a saturated clay medium, the liquid phase occupies the interparticle void spaces of the solid phase. A similar situation may happen in any geotechnical structure founded on soft clay (see Brand and Brenner [2]) In this regard, the viscosity of clay most often contributes to the long-term time-dependent creep of clay, and subsequent damage to the structure, which requires billions of dollars in annual maintenance costs [5]. To avoid the mathematical formulation complexity, in most cases, the time-dependent constitutive models are limited to the associated flow rule (AFR). We develop a non-associated flow rule-based elasto-viscoplastic (EVP) model considering the Modified Cam Clay (MCC) model [10] framework, Perzyna’s overstressed theory [16], the Borja and Kavazanjian [17] concept, the bounding surface theory and the mapping rule After validation of the developed non-associated flow rule EVP model, we implement it in a coupled finite element solver named. For a field application of the developed EVP model, we compare the predicted response with the long-term monitoring measured response of the Nerang Broadbeach Roadway (NBR) embankment in Australia [20]

Importance of the Non-Associated Flow Rule
Numerical Modeling
Governing
Constitutive Assumptions
Strain Rate Tensor of the EVP Model
Bounding Surfaces of the EVP Model
Meridional section thepotential potential surface with ellipse
Relations
Image Parameters of the EVP Model
Couple Finite Element Formulation
Incremental Stress and Strain
Initial and Boundary Conditions
Model Parameters
Method of Determination λ κ ν
Shanghai Clay
San Francisco Bay Mud Clay
10. Comparison of observed and predicted stress triaxial test results of the San
Kaolin Clay
Application of the EVP Models
Conclusions
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