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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> General <strong>Cutting</strong> Process.<br />

<br />

2 2 2<br />

sin sin sin <br />

Fh<br />

r cos sin 2 sin sin sin <br />

<br />

<br />

<br />

<br />

2 2 2<br />

sin sin sin <br />

sin sin 2 sin sin cos <br />

<br />

<br />

(3-31)<br />

<br />

<br />

2 2 2<br />

sin sin <br />

sin<br />

<br />

sin sin 2 r sin sin cos <br />

<br />

In the special case where there is no adhesion, r 0, the shear angle is:<br />

<br />

0<br />

<br />

2 2<br />

sin sin <br />

Fh<br />

sin 2 sin cos <br />

<br />

<br />

0<br />

(3-32)<br />

So:<br />

<br />

sin 2 <br />

0 for 2 giving = (3-33)<br />

2 2<br />

<strong>The</strong> cohesion c can be determined from the UCS value and the angle of internal friction φ according to (as is shown<br />

in Figure 3-12):<br />

<br />

<br />

UCS 1<br />

sin <br />

c <br />

2 <br />

cos <br />

<br />

(3-34)<br />

According to the Mohr-Coulomb failure criterion, the following is valid for the shear stress on the shear plane, as<br />

is shown in Figure 3-13.<br />

S1<br />

N1<br />

<br />

c tan (3-35)<br />

Figure 3-12: <strong>The</strong> Mohr circle for UCS and cohesion.<br />

Copyright © Dr.ir. S.A. Miedema TOC Page 83 of 454

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