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The Delft Sand, Clay & Rock Cutting Model, 2019a

The Delft Sand, Clay & Rock Cutting Model, 2019a

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<strong>The</strong> <strong>Delft</strong> <strong>Sand</strong>, <strong>Clay</strong> & <strong>Rock</strong> <strong>Cutting</strong> <strong>Model</strong>.<br />

2<br />

<br />

2<br />

<br />

<br />

<br />

m m 4 1<br />

min UCS <br />

2<br />

2 1<br />

<br />

<br />

m m 4 1<br />

max UCS <br />

2<br />

2 1<br />

<br />

2<br />

<br />

2<br />

(8-10)<br />

This gives for the center of the Mohr circle:<br />

UCS m m 4 1<br />

center 1<br />

<br />

2<br />

2<br />

2 1<br />

2<br />

<br />

2<br />

<br />

<br />

<br />

<br />

<br />

UCS m m 4 1<br />

max 1<br />

<br />

2<br />

2<br />

2 1<br />

<br />

2<br />

<br />

2<br />

(8-11)<br />

Figure 8-8: Brittle, semi brittle and ductile failure.<br />

Figure 8-17 shows the Mogi criterion both for the top of the Mohr circle curve and the failure curve. Left of the<br />

Mogi criterion point there will be brittle failure, on the right there will be pseudo-ductile failure. When the<br />

coefficient α increases, the Mogi points move to the left.<br />

In the case of a straight failure plane this gives for the normal and shear stress:<br />

c 1 <br />

sin <br />

cos<br />

<br />

1<br />

<br />

<br />

and c tan <br />

tan<br />

1 <br />

1 sin<br />

cos<br />

<br />

1<br />

<br />

<br />

<br />

<br />

(8-12)<br />

Which is also shown in Figure 8-17. If the angle of internal friction is to high, the brittle-ductile transition will<br />

never be reached. <strong>The</strong> criterion for this is:<br />

1 sin <br />

1<br />

<br />

(8-13)<br />

Page 248 of 454 TOC Copyright © Dr.ir. S.A. Miedema

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