Sand Plasticity Model Accounting for Inherent Fabric Anisotropy

A sand plasticity constitutive model is presented herein, which accounts for the effect of inherent fabric anisotropy on the mechanical response. The anisotropy associated with particles’ orientation distribution, is represented by a second-order symmetric fabric tensor, and its effect is quantified via a scalar-valued anisotropic state variable, \iA. \iA is defined as the first joint isotropic invariant of the fabric tensor and a properly defined loading direction tensor, scaled by a function of a corresponding Lode angle. The hardening plastic modulus and the location of the critical state line in the void ratio—mean effective stress space, on which the dilatancy depends, are made functions of \iA. The incorporation of this dependence on \iA in a pre-existing stress-ratio driven, bounding surface plasticity constitutive model, achieves successful simulations of test results on sand for a wide variation of densities, pressures, loading manners, and directions. In particular, the drastic difference in material response observed experimentally for different directions of the principal stress axes with respect to the anisotropy axes, is well simulated by the model. The proposed definition and use of \iA has generic value, and can be incorporated in a large number of other constitutive models in order to account for inherent fabric anisotropy effects.

[1]  K. Kanatani Stereological determination of structural anisotropy , 1984 .

[2]  Majid T. Manzari,et al.  A critical state two-surface plasticity model for sands , 1997 .

[3]  Zhi-Liang Wang,et al.  Bounding Surface Hypoplasticity Model for Sand , 1990 .

[4]  J. Thomas,et al.  Liquefaction and Postliquefaction Behavior of Sand , 1995 .

[5]  Yoginder P. Vaid,et al.  Static and cyclic liquefaction potential of Fraser Delta sand in simple shear and triaxial tests , 1996 .

[6]  Majid T. Manzari,et al.  SIMPLE PLASTICITY SAND MODEL ACCOUNTING FOR FABRIC CHANGE EFFECTS , 2004 .

[7]  S. Pietruszczak On inelastic behaviour of anisotropic frictional materials , 1999 .

[8]  Kanatani Ken-Ichi DISTRIBUTION OF DIRECTIONAL DATA AND FABRIC TENSORS , 1984 .

[9]  Yannis F. Dafalias,et al.  Dilatancy for cohesionless soils , 2000 .

[10]  Yukio Nakata,et al.  FLOW DEFORMATION OF SANDS SUBJECTED TO PRINCIPAL STRESS ROTATION , 1998 .

[11]  P. Guo,et al.  Effect of microstructure on undrained behaviour of sands , 2001 .

[12]  B. Muhunthan,et al.  Void Fabric Tensor and Ultimate State Surface of Soils , 1997 .

[13]  Ken Been,et al.  A STATE PARAMETER FOR SANDS , 1985 .

[14]  Yannis F. Dafalias,et al.  CONSTITUTIVE MODELING OF INHERENTLY ANISOTROPIC SAND BEHAVIOR , 2002 .

[15]  Masanobu Oda,et al.  STRESS-INDUCED ANISOTROPY IN GRANULAR MASSES , 1985 .

[16]  Michael A. Mooney,et al.  A Unique Critical State for Sand , 1998 .

[17]  M. Oda,et al.  Introduction of Inherent Anisotropy of Soils in the Yield Function , 1988 .

[18]  Gioacchino Viggiani,et al.  Undrained Shear Band Deformation in Granular Media , 1997 .

[19]  Raymond B. Seed,et al.  Factors Affecting Apparent Position of Steady-State Line , 1997 .

[20]  Kenji Ishihara,et al.  FLOW POTENTIAL OF SAND DURING LIQUEFACTION , 1998 .

[21]  Yoginder P. Vaid,et al.  Cyclic and monotonic undrained response of saturated sands , 1985 .

[22]  X. S. Li,et al.  Linear representation of steady-state line for sand , 1998 .

[23]  Yasuo Yamada,et al.  Undrained Deformation Characteristics of Loose Sand Under Three-Dimensional Stress Conditions , 1981 .

[24]  Yannis F. Dafalias,et al.  A constitutive framework for anisotropic sand including non-proportional loading , 2004 .

[25]  Kenji Ishihara,et al.  Effects of principal stress direction and intermediate principal stress on undrained shear behavior of sand. , 1998 .

[26]  Yannis F. Dafalias,et al.  An anisotropic critical state soil plasticity model , 1986 .