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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 />

<br />

<br />

<br />

<br />

<br />

2 2<br />

<br />

N1<br />

cos sin sin 1 sin <br />

min<br />

c cos<br />

cos cos <br />

<br />

<br />

<br />

N1<br />

1<br />

sin <br />

<br />

c<br />

<br />

cos<br />

cos <br />

<br />

(3-42)<br />

Figure 3-13: <strong>The</strong> Mohr circles of the Tear Type.<br />

Now ductile failure will occur if the minimum principal stress σmin is bigger than then tensile strength σT, thus:<br />

(3-43)<br />

min<br />

T<br />

If equation (3-43) is true, ductile failure will occur. Keep in mind however, that the tensile strength σT is a negative<br />

number. Of course if the minimum normal stress min is positive, brittle tensile failure can never occur.<br />

Substituting equation (3-39) for the normal stress on the shear plane gives the following condition for the Tear<br />

Type:<br />

<br />

<br />

<br />

<br />

<br />

sin cos<br />

<br />

r cos sin <br />

<br />

sin 1 sin<br />

<br />

c <br />

<br />

<br />

<br />

sin <br />

cos<br />

<br />

<br />

<br />

<br />

<br />

<br />

T<br />

(3-44)<br />

In clay it is assumed that the internal and external friction angles are zero, while in rock it is assumed that the<br />

adhesion is zero. This will be explained in detail in the chapters on clay and rock cutting.<br />

<strong>The</strong> ratios between the pore pressures and the cohesive shear strength, in the case of hyperbaric rock cutting, can<br />

be found according to:<br />

Copyright © Dr.ir. S.A. Miedema TOC Page 85 of 454

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