SOIL-WATER COUPLED BEHAVIOR OF HEAVILY OVERCONSOLIDATED CLAY NEAR/AT CRITICAL STATE

The time dependent elasto-plastic response of a heavily overconsolidated soil has been illustrated with simple yet typical examples that a heavily overconsolidated clay under loading exhibits either hardening or softening due to the migration of pore water. In the examples studied triaxial tests are numerically simulated, where the test is considered not as a test of a soil element but as a test of the soil mass with well defined boundary conditions. In order to describe the behavior of heavily overconsolidated soils, the subloading surface concept first developed by Hashiguchi and Ueno (1977) is newly applied to the original Cam-clay model. From this study, the following conclusions are obtained : (1) The subloading surface Cam-clay model describes the typical shear behavior of heavily overconsolidated soils such as the hardening procedure that occurs above the critical state line with a considerable volume expansion. (2) The hardening and softening of heavily overconsolidated soils due to the migration of pore water have non-local characteristics because of Darcy's law. Based on this gradient nature with positive permeability, plastic instability can be well simulated by the usual finite element computation. (3) As the results of coupling with Darcy's law, the total shear behavior of the triaxial soil specimens exhibits an apparent "time dependent" nature particularly for the "stress-dilatancy" characteristic. This can be observed equally under both undrained and drained conditions for triaxial experiments.

[1]  Takeshi Tamura,et al.  NUMERICAL ANALYSIS OF MULTI-DIMENSIONAL CONSOLIDATION ACCOMPANIED WITH ELASTO-PLASTIC CONSTITUTIVE EQUATION , 1978 .

[2]  A. Asaoka,et al.  Annealable behaviour of saturated clay : An experiment and simulation , 1995 .

[3]  K. Hashiguchi,et al.  Elasto-plastic constitutive laws of granular materials, Constitutive equations of soils , 1977 .

[4]  Toru Shibata,et al.  On the Volume Changes of Normally-Consolidated Clays , 1963 .

[5]  Toshihiro Noda,et al.  Imperfection-sensitive bifurcation of cam-clay under plane-strain compression with undrained boundaries , 1995 .

[6]  K. Hashiguchi,et al.  Plastic constitutive equations of granular materials , 1978 .

[7]  Toshihiro Noda,et al.  SOIL-WATER COUPLED BEHAVIOUR OF SATURATED CLAY NEAR/AT CRITICAL STATE , 1994 .

[8]  J. Dienes On the analysis of rotation and stress rate in deforming bodies , 1979 .

[9]  K. Hashiguchi,et al.  Subloading surface model in unconventional plasticity , 1989 .

[10]  Hideki Ohta,et al.  Analysis of deformations of soils based on the theory of plasticity and its application to settlement of embankments , 1971 .

[11]  Atsushi Yashima,et al.  GENERAL THEORY OF SHEAR BANDS FORMATION BY A NON-COAXIAL CAM-CLAY MODEL , 1989 .

[12]  Koichi Hashiguchi Constitutive Equations of Elastoplastic Materials With Elastic-Plastic Transition , 1980 .

[13]  J. Z. Zhu,et al.  The finite element method , 1977 .

[14]  A. Schofield,et al.  Critical State Soil Mechanics , 1968 .

[15]  Koichi Hashiguchi,et al.  Fundamental requirements and formulation of elastoplastic constitutive equations with tangential plasticity , 1993 .

[16]  John T. Christian,et al.  PLANE STRAIN CONSOLIDATION BY FINITE ELEMENTS , 1970 .

[17]  P. M. Naghdi,et al.  A general theory of an elastic-plastic continuum , 1965 .