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

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

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25<br />

and therefore the angle of inclination of the normal directions to the slip plane is<br />

described by the equations presented in figure 3.6c.<br />

Figure 3.7 presents the stress condition realized in the direct shear apparatus.<br />

Point P in the Mohr graph illustrates the values of normal stress σ and max<strong>im</strong>um<br />

tangential (shear) stress τ measured in a horizontal shear plane. Point P is not<br />

identical with point T – the point of tangency of the Coulomb-Mohr yield criterion<br />

of strength with the Mohr circle [150]. Therefore, the plane in which the Coulomb-<br />

Mohr yield criterion is fulfilled does not coincide with the horizontally enforced<br />

shear plane, but is inclined to it at the angle δ/2. The angle of long granule axis<br />

preferred inclination γ 2 was referred not to the plane in which the Coulomb-Mohr<br />

yield criterion is fulfilled, but to the horizontal shear plane.<br />

a) b)<br />

failure surface<br />

slip surface<br />

horizontal surface P<br />

T<br />

c)<br />

Fig. 3.7. Sample of granular material in direct shear test: a) diagram of Mohr for state of stress in the<br />

sample, b) orientation of preferred direction of long axis of grains against theoretical slip plane γ 2 ,<br />

c) <strong>im</strong>age of deformation of the sample<br />

The results of the measurements are presented in figure 3.8 as graphs of the<br />

relation of the angle of internal friction φ to the angle of slip plane inclination to the<br />

direction of grain long axes or to the normal direction of the normals at contact points.<br />

The closest agreement of the relations φ(γ 1 ) and φ(γ 2 ) was obtained in the case of<br />

rapeseed. In both the tests performed on rapeseed the max<strong>im</strong>um of the angle of internal<br />

friction, φ = 29 o , occurred at s<strong>im</strong>ilar values of the angles γ 1 ≈ γ 2 ≈ 35 o . Considering the<br />

fact that the plane of the higher main stress σ 1 is inclined to the slip plane at an angle<br />

α = π/4+φ/2 it is easy to note the agreement of the obtained max<strong>im</strong>um of the angle of<br />

internal friction with the results obtained by Oda [126-128]. The author found that in<br />

the course of non-dilatational hardening of granular material the normal directions to<br />

the points of contact concentrate around the direction of the major principal stress, and<br />

that the direction gradually rotates with increasing tangential (shear) stress. The main

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