
Figure 1
Sand sample preparation for testing with gauges installed (photo by W. Świdziński).

Figure 2
The stress plane p′ − q with a grey zone in which the definitions of deviatoric loading and unloading are unclear.

Figure 3
The meaning of the variable η and the sign of dη.

Figure 4
Stress paths η = const used for the calibration of the incremental model.

Figure 5
Experimental results and an approximation curve for volumetric strain that develops during anisotropic consolidation of contractive sand.

Figure 6
Experimental results and an approximation curve for volumetric strain that develops in contractive sand for various stress paths η = const when dp′ < 0.
Table 1
List of experiments performed on contractive sand samples and the corresponding results for a single spherical loading–unloading loop.
| Test | η = const | dp′ > 0 | dp′ < 0 | ||
|---|---|---|---|---|---|
| LH75d | η = 0.64 | 0.077 | 10.75 | 0.239 | 5.10 |
| LH77d | η = 0.97 | 0.146 | 8.82 | 0.280 | 4.15 |
| LH79d | η = 0.44 | 0.23 | 8.69 | 0.356 | 5.07 |
| LH80d | η = 1.12 | 0.113 | 9.02 | 0.248 | 4.17 |
| LH81d | η = 1.27 | 0.082 | 10.26 | 0.204 | 4.49 |
| LH81dd | η = 1.22 | 0.057 | 10.42 | 0.201 | 4.45 |
| LH82d | η = 0.23 | 0.094 | 8.3 | 0.181 | 4.54 |
| LH84d | η = 0 | 0.056 | 8.4 | 0.178 | 4.72 |

Figure 7
Experimental results and an approximation of deviatoric strain that develops in contractive sand for stress paths η = const when dp′ > 0.
Table 2
Series of experiments performed to calibrate the model for contractive sand.
| Test | η = const | First phase: dp′ > 0 | |
|---|---|---|---|
| Aq | |||
| LH75d | η = 0.64 | 0.077 | 2.94 |
| LH77d | η = 0.97 | 0.146 | 6 |
| LH79d | η = 0.44 | 0.23 | 1.3 |
| LH80d | η = 1.12 | 0.113 | 9.76 |
| LH81d | η = 1.27 | 0.082 | 28.3 |
| LH81dd | η = 1.22 | 0.057 | 20.2 |
| LH82d | η = 0.23 | 0.094 | 0.21 |
| LH84d | η = 0 | 0.056 | −2.63 |

Figure 8
Relationship Aq (η): experimental results and their analytical approximation for deviatoric strain that develops in contractive sand for stress paths η = const when dp′ > 0.

Figure 9
Experimental results for deviatoric strain that develops in contractive for stress paths η = const when dp′ < 0.
Table 3
List of experiments performed on contractive sand samples and the corresponding results for a single spherical loading–unloading loop.
| Test | η = const | First phase: | Second phase: dp′ < 0 | |||
|---|---|---|---|---|---|---|
| Av | Aq | |||||
| SH73d | η = 0.96 | 0.702 | 3.3 | 1 | 0.749 | 2.59 |
| SH75d | η = 1.23 | 0.701 | 3.28 | 2.22 | 0.749 | 3.04 |
| SH76d | η = 0.64 | 0.669 | 3.72 | 0.52 | 0.722 | 3.04 |
| SH77d | η = 0.34 | 0.703 | 3.52 | 0.62 | 0.753 | 2.9 |
| SH78d | η = 0 | 0.701 | 3.45 | 0 | 0.750 | 2.96 |
| SH80d | η = 1.35 | 0.632 | 3.27 | 6.5 | 0.678 | 3.35 |

Figure 10
Relationship Aq (η): experimental results and their analytical approximation for deviatoric strain that develops in dilative sand for stress paths η = const when dp′ > 0.

Figure 11
Experimental results for pure shearing of dilative sand presented in the form of a single ‘common’ curve.
Table 4
Functions needed to build the incremental model.
| Function | Average values of coeflcients | |||
|---|---|---|---|---|
| Contractive | Dilative | Contractive | Dilative | |
| Ml | Av = 9.33 | Av = 3.48 | ||
| Pl | a = −0.68 | a = 0 | ||
| b = 9.74 | b = 1.62 | |||
| Nl | c1 = 2.97 | a1 = −0.74 * 10−4 | ||
| a2 = 6.39 | ||||
| a3 = 0.848 | ||||
| Ql | b1 = 0.023 | b1 = 3.5 × 10−4 | ||
| b2 = 6.245 | b2 = 6.648 | |||
| Mu | ||||
| Pu | 0 | - | - | |
| Nu | av = −0.87 | av = −0.39 | ||
| Qu | bq = 0.76 | bq = 0.4 | ||

Figure 12
Diagram illustrating the application of subsequent incremental equations.

Figure 13
Spherical unloading for different initial deviator stress levels.

Figure 14
Volumetric strains corresponding to different stress paths.

Figure 15
Static liquefaction: experimental and numerical results.

Figure 16
The behaviour of dilative sand under undrained conditions: experimental and numerical results.