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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76<br />
1+ sinϕ<br />
k = . 1 − sinϕ<br />
(10.3)<br />
where 3 is the angle of internal friction.<br />
The commonly used assumption that the lateral stress is constant along the<br />
slice results in location of Mohr’s circle for stresses at the wall outside the yield<br />
locus [45]. This assumption does not adequately represent pressure distribution in<br />
granular material in a silo.<br />
$FWLYHFDVH<br />
3DVVLYHFDVH<br />
a)<br />
b)<br />
c)<br />
d)<br />
Fig. 10.1. Mohr’s circles for active (a), (c) and passive (b), (d) stress cases, (a), (b) – yielding at<br />
the centre, (c), (d) – yielding at the wall [67]<br />
10.2. Yielding at the silo wall<br />
Considering the assumption that yielding occurs at the silo wall, the stress<br />
ratio k can be determined from the Mohr’s circle construction as the function of<br />
the angle of internal friction and the angle of wall friction 3 w :