This class defines a linear saturation rate dependent swelling stress model for the materials that swell strongly when water content increases.
Clay materials like bentonite have a high swelling capacity in dry state, and their swelling property can be described by this model.
The original model was proposed in [36] (equations (39) and (40) on pages 758–759). With a simplification of the parameters of the original formula and introducing a constraint to avoid shrinkage stress when saturation is below the initial saturation, the model takes the form
{\mathbf{\sigma}}^{\text{sw}} = {\alpha}_{\text{sw}} (S-S_0) \mathbf{I}, \, \forall S \in [S_0, S_\text{max}]
where {\alpha}_{\text{sw}} is a coefficient, and S_0 is the initial saturation, and S_{\text{max}} is the maximum saturation. The coefficient gives the swelling stress at full saturation, which can be computed as
{\alpha}_{\text{sw}} = \frac{{{\sigma}}^{\text{sw}}_{\text{max}}}{(S_{\text{max}}-S_0)}
where {{\sigma}}^{\text{sw}}_{\text{max}} represents the swelling stress at full saturation.
In the numerical analysis, the stress always takes the incremental form. Therefore the model becomes as
\Delta {\mathbf{\sigma}}^{\text{sw}} = {\alpha}_{\text{sw}} \Delta S \mathbf{I}, \, \forall S \in [S_0, S_\text{max}]
Note:
No additional info.
Used in no end-to-end test cases.