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Strona 2_redak - Instytut Agrofizyki im. Bohdana Dobrzańskiego ...

Strona 2_redak - Instytut Agrofizyki im. Bohdana Dobrzańskiego ...

Strona 2_redak - Instytut Agrofizyki im. Bohdana Dobrzańskiego ...

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15<br />

Ghaboussi and Momen adopted the Drucker-Prager yield condition for a noncohesive<br />

material (fig. 2.2):<br />

2<br />

F(σ<br />

) = I − Y I<br />

2<br />

ij 2 1<br />

=<br />

0,<br />

(2.17)<br />

where Y is the yield constant, and the plastic potential of the same shape as the<br />

yield condition additionally including isotropic and kinematic hardening:<br />

G(<br />

σij , αij,<br />

κ)<br />

= 0,<br />

(2.18)<br />

where:<br />

α ij – kinematic hardening tensor,<br />

κ – parameter of isotropic hardening.<br />

The eight-parameter model of Ghaboussi and Momen contains 3 parameters descrybing<br />

elasticity, 3 parameters of kinematic hardening, and 2 parameters of<br />

isotropic hardening. The model describes correctly all phenomena typical for<br />

isotropic as well as kinematic hardening, and it describes especially well the<br />

anisotropy of the material, hysteresis in the load-unload cycle, and the evolution<br />

of the hysteresis loop in the course of multiple loadings.<br />

Fig. 2.2. A schematic of yield and plastic potential surfaces in the principal stresses space [175]

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