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Some powder materials exhibit tendency to change volume during shear,<br />

known as dilatancy. Strength and resistance to slow deformation can be profoundly<br />

affected by dilation [1,2,4]. Sequences of compaction-dilation events were thought<br />

to be the most probable source of the shear stress oscillations. Oscillation can be<br />

considered as part of a sequence of compaction-dilation events occurring around<br />

the area of shear zones developing in the material. Compaction of the particulate<br />

material resulted in an increase in material strength and the ability to withstand<br />

higher shear loads. When the maximum strength of the particulate material is exceeded<br />

dilation in the shear zone occurs resulting in a sharp decrease in the shear<br />

load. This leads to limiting mechanisms of slow dilatant plastic shear deformation.<br />

Pitch of oscillation [mm]<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

σ n<br />

agglomerated milk<br />

fine milk<br />

potato starch<br />

0<br />

0 50 100 150 200 250 300<br />

Normal stress [kPa]<br />

Fig. 4. Pitch of the tangent stress oscillation as influenced by the normal stress.<br />

Based on the saw blades model of dilatancy proposed by Bolton [1] the two<br />

following strength components were determined from the tangent stress – shear<br />

displacement relationships: the physical friction strength and the extra component<br />

of strength related to dilation. It was assumed that the minimum value of tangent<br />

stress during oscillation corresponds to a critical state of the sample with zero dilation.<br />

Contribution of the stress oscillation to the total strength was approximately<br />

30% for the agglomerated milk, 35% for the fine milk and 45% for the potato<br />

starch.<br />

CONCLUSIONS<br />

The effective angle of internal friction δ of all tested materials was found to be<br />

in the range of 30-35 deg. There was no clear influence of the consolidation pressure.<br />

The angle of internal friction ϕ was smaller than the effective angle of friction<br />

δ of approximately 0.2-5 deg.<br />

61

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