Strona 2_redak - Instytut Agrofizyki im. Bohdana DobrzaÅskiego ...
Strona 2_redak - Instytut Agrofizyki im. Bohdana DobrzaÅskiego ...
Strona 2_redak - Instytut Agrofizyki im. Bohdana DobrzaÅskiego ...
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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]