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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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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

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