05.03.2014 Views

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

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

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

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

16<br />

In turn, the model of Lade, also applied by Zhang et al. [175] for the description<br />

of wheat grain during loading, assumes that the plastic strain increment dε p ij is the<br />

sum of two independent components: the plastic strain increment related with the<br />

compaction of the material dε c ij and the plastic strain increment related with the<br />

dilation of the material dε d ij:<br />

dε = dε + dε<br />

p<br />

ij<br />

c<br />

ij<br />

(2.19)<br />

The division of the plastic strain increment into two independent components entails<br />

the necessity of adopting also two independent yield functions and two flow rules.<br />

For the description of the behaviour of wheat Zhang et al. [175] adopted the<br />

following yield functions F c and F d , and plastic potentials G c and G d :<br />

d<br />

ij<br />

.<br />

F<br />

c<br />

= I<br />

2<br />

1<br />

+ 2⋅<br />

I<br />

2<br />

− P ⋅(<br />

W<br />

a<br />

c<br />

/ C ⋅ P )<br />

a<br />

1<br />

q<br />

,<br />

(2.20)<br />

F<br />

d<br />

= ( I<br />

3<br />

1<br />

/ I<br />

3<br />

− 27) ⋅(<br />

I / P )<br />

1<br />

a<br />

m<br />

− ae<br />

d<br />

−bW<br />

⋅(<br />

W<br />

d<br />

/ P )<br />

a<br />

1<br />

q<br />

,<br />

(2.21)<br />

G c<br />

2<br />

= I 1<br />

+ 2 ⋅ I 2<br />

,<br />

(2.22)<br />

3<br />

m<br />

G<br />

(2.23)<br />

d<br />

= I1 − ( 27 + η ⋅(<br />

Pa<br />

/ I1)<br />

) ⋅ I3,<br />

where:<br />

a, b, c, m, q, η – material constants,<br />

I 1 , I 2 , I 3 – first, second and third invariant of stress tensor,<br />

P a – atmospheric pressure,<br />

W c , W d – collapse and expansive plastic work.<br />

The yield functions F c , responsible for irreversible compaction of material,<br />

represents in the space of principal stresses a concave surface with axis of<br />

symmetry lined with the axis of isotropic stresses. This condition confirms the<br />

known rule that a granular material compacts the easiest under the isotropic stress.<br />

In the plastic potential G d , responsible for material expansion, the material<br />

constant η represents the slope of the plastic potential surface, and the exponent m<br />

represents the curvature of the meridian of the surface.<br />

Figure 2.3 presents examples of the application of the models of Ghaboussi<br />

and Momen and of Lade for the approx<strong>im</strong>ation of the exper<strong>im</strong>ental stress-strain<br />

relations obtained during tests of monotonic loading of wheat grain samples in triaxial<br />

compression apparatus. The presented comparison shows that the model of Lade more<br />

accurately approx<strong>im</strong>ates the course of the stress-strain relation during monotonic

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!