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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11<br />
Density ρ is strictly related to volumetric deformation and dependent on the major<br />
principal stress ρ(σ 1 ). The most <strong>im</strong>portant contribution in the development of the<br />
model of granular material with hardening and softening is that by Roscoe [143].<br />
In the model, for the particular values of density ρ we obtain, in the plane (τ,σ),<br />
yielding conditions separating the plastic states of the material from its elastic or<br />
rigid states. As higher density is related to higher strength, the yield condition is<br />
a monotonically increasing function of density. For a fixed density ρ the yield<br />
condition represents in the stress space an enclosed surface that, in the case of<br />
a cohesionless material, passes through the origin of the system of coordinates<br />
whose axis of symmetry is the axis of isotropic stress. In axial-symmetric state of<br />
stress the yielding condition can be written in the system of coordinates (p,q):<br />
where:<br />
(2.4)<br />
In figure 2.1 the critical line separates the area of compaction where plastic<br />
strain is accompanied by an increase in density ρ > ρ 1 and therefore expansion of<br />
the yield curve from the area of dilation in which strain is accompanied by<br />
volume increase of the material, decrease in density ρ < ρ 2 i.e. in effect shrinking<br />
of the yield curve. The change in density is defined by the law of mass<br />
conservation:<br />
where:<br />
1<br />
p = (σ1<br />
+ 2σ<br />
3<br />
q = σ − σ ,<br />
σ<br />
1<br />
1<br />
≠ σ<br />
2<br />
2<br />
= σ<br />
3<br />
.<br />
2<br />
),<br />
F( p,q, ρ)<br />
= 0,<br />
dρ = ρdε p<br />
,<br />
(2.5)<br />
dV<br />
dε<br />
p<br />
= = dε1<br />
+ 2dε<br />
2,<br />
V<br />
2<br />
dε<br />
q<br />
= ( dε1<br />
− dε<br />
2).<br />
3