Products: ABAQUS/Standard ABAQUS/CAE
The clay plasticity model provided in ABAQUS/Standard:
is an extension of the critical state models originally developed by Roscoe and his coworkers at Cambridge;
describes the inelastic behavior of the material by a yield function that depends on the three stress invariants, an associated flow assumption to define the plastic strain rate, and a strain hardening theory that changes the size of the yield surface according to the inelastic volumetric strain;
requires that the elastic part of the deformation be defined by using the linear elastic material model (Linear elastic behavior, Section 17.2.1) or the porous elastic material model (Elastic behavior of porous materials, Section 17.3.1) within the same material definition; and
allows for the hardening law to be defined by a piecewise linear form or by an exponential form.
The model is based on the yield surface
is the equivalent pressure stress;
is a deviatoric stress measure;
is the Mises equivalent stress;
is the third stress invariant;
is a constant that defines the slope of the critical state line;
is a constant that is equal to 1.0 on the “dry” side of the critical state line () but may be different from 1.0 on the “wet” side of the critical state line ( introduces a different ellipse on the wet side of the critical state line; i.e., a tighter “cap” is obtained if as shown in Figure 18.3.41);
is the size of the yield surface (Figure 18.3.41); and
is the ratio of the flow stress in triaxial tension to the flow stress in triaxial compression and determines the shape of the yield surface in the plane of principal deviatoric stresses (the “-plane”: see Figure 18.3.42); ABAQUS/Standard requires that to ensure that the yield surface remains convex.
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Property module: material editor: MechanicalPlasticityClay Plasticity
The hardening law can have an exponential form or a piecewise linear form.
The exponential form of the hardening law is written in terms of some of the porous elasticity parameters and, therefore, can be used only in conjunction with the porous elastic material model. The size of the yield surface at any time is determined by the initial value of the hardening parameter, , and the amount of inelastic volume change that occurs according to the equation
is the inelastic volume change (that part of J, the ratio of current volume to initial volume, attributable to inelastic deformation);
is the logarithmic bulk modulus of the material defined for the porous elastic material behavior;
is the logarithmic hardening constant defined for the clay plasticity material behavior; and
is the user-defined initial void ratio (Defining initial void ratios in a porous medium” in “Initial conditions, Section 27.2.1).
The initial size of the yield surface is defined for clay plasticity by specifying the hardening parameter, , as a tabular function or by defining it analytically.
can be defined along with , M, , and K, as a tabular function of temperature and other predefined field variables. However, is a function only of the initial conditions; it will not change if temperatures and field variables change during the analysis.
Property module: material editor:
Initial void ratios are not supported in ABAQUS/CAE.
Alternatively, can be defined indirectly by specifying , which is the intercept of the virgin consolidation line with the void ratio axis in the plot of void ratio, e, versus the logarithm of the effective pressure stress, (Figure 18.3.43).
Property module: material editor:
Initial void ratios and initial pore pressures are not supported in ABAQUS/CAE.
If the piecewise linear form of the hardening rule is used, the user-defined relationship relates the yield stress in hydrostatic compression, , to the corresponding volumetric plastic strain, (Figure 18.3.44):
This form of the hardening law can be used in conjunction with either the linear elastic or the porous elastic material models.
Property module: material editor: MechanicalPlasticityClay Plasticity: Hardening: Tabular, SuboptionsClay Hardening
At least two experiments are required to calibrate the simplest version of the Cam-clay model: a hydrostatic compression test (an oedometer test is also acceptable) and a triaxial compression test (more than one triaxial test is useful for a more accurate calibration).
The hydrostatic compression test is performed by pressurizing the sample equally in all directions. The applied pressure and the volume change are recorded.
The onset of yielding in the hydrostatic compression test immediately provides the initial position of the yield surface, . The logarithmic bulk moduli, and , are determined from the hydrostatic compression experimental data by plotting the logarithm of pressure versus void ratio. The void ratio, e, is related to the measured volume change as
Triaxial compression experiments are performed using a standard triaxial machine where a fixed confining pressure is maintained while the differential stress is applied. Several tests covering the range of confining pressures of interest are usually performed. Again, the stress and strain in the direction of loading are recorded, together with the lateral strain so that the correct volume changes can be calibrated.
The triaxial compression tests allow the calibration of the yield parameters M and . M is the ratio of the shear stress, q, to the pressure stress, p, at critical state and can be obtained from the stress values when the material has become perfectly plastic (critical state). represents the curvature of the cap part of the yield surface and can be calibrated from a number of triaxial tests at high confining pressures (on the “wet” side of critical state). must be between 0.0 and 1.0.
To calibrate the parameter K, which controls the yield dependence on the third stress invariant, experimental results obtained from a true triaxial (cubical) test are necessary. These results are generally not available, and you may have to guess (the value of K is generally between 0.8 and 1.0) or ignore this effect.
Unloading measurements in hydrostatic and triaxial compression tests are useful to calibrate the elasticity, particularly in cases where the initial elastic region is not well defined. From these we can identify whether a constant shear modulus or a constant Poisson's ratio should be used and what their values are.
If an initial stress at a point is given (see Defining initial stresses” in “Initial conditions, Section 27.2.1) such that the stress point lies outside the initially defined yield surface, ABAQUS/Standard will try to adjust the initial position of the surface to make the stress point lie on it and issue a warning. However, if the stress point is such that the equivalent pressure stress, p, is negative, an error message will be issued and execution will be terminated.
The clay plasticity model can be used with plane strain, generalized plane strain, axisymmetric, and three-dimensional solid (continuum) elements in ABAQUS/Standard. This model cannot be used with elements for which the assumed stress state is plane stress (plane stress, shell, and membrane elements).
In addition to the standard output identifiers available in ABAQUS/Standard (ABAQUS/Standard output variable identifiers, Section 4.2.1), the following variable has special meaning for material points in the clay plasticity model:
Center of the yield surface, a.