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

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<strong>Rock</strong> <strong>Cutting</strong>: Atmospheric Conditions.<br />

140<br />

120<br />

100<br />

Shear Stress τ vs. Normal Stress σ<br />

Sigma Axis<br />

Tau Axis<br />

Shear Stress τ (MPa)<br />

80<br />

60<br />

40<br />

20<br />

0<br />

-20<br />

-40<br />

-60<br />

-80<br />

-100<br />

-120<br />

-140<br />

-50 -30 -10 10 30 50 70 90 110 130 150 170 190 210 230 250 270 290 310 330 350<br />

© S.A.M.<br />

For a given radius a this gives:<br />

Normal Stress σ (MPa)<br />

Figure 8-15 <strong>The</strong> Parabolic and Ellipsoid failure envelopes, with a=100·UCS.<br />

Mohr Circle<br />

UCS Test<br />

Mohr Circle<br />

UTS Test<br />

Mohr Circle<br />

BTS Test<br />

Parabole<br />

Mogi Criterion<br />

Brittle Ductile<br />

Failure Criterion<br />

Pseudo-Ductile<br />

Ellipse<br />

Mogi Criterion<br />

Brittle Ductile<br />

Failure Criterion<br />

Pseudo-Ductile<br />

b<br />

2<br />

<br />

<br />

<br />

1 <br />

<br />

<br />

<br />

p<br />

<br />

<br />

2<br />

p<br />

a<br />

UTS<br />

a<br />

2<br />

<br />

<br />

2<br />

<br />

<br />

<br />

<br />

(8-33)<br />

Figure 8-14 shows both the parabolic and the ellipsoid failure envelopes. <strong>The</strong> ellipsoid failure envelope is<br />

determined for a=1.75·UCS. <strong>The</strong> Mohr circles for UTS, BTS and UCS are determined for UCS=100 MPa,<br />

UTS=BTS=15 MPa. At low normal stresses the parabolic and ellipsoid failure envelopes behave almost identical.<br />

Also the Mogi brittle-ductile transition points are very close. Chosing a>10·UCS gives about identical envelopes<br />

in the normal stress range considered.<br />

Copyright © Dr.ir. S.A. Miedema TOC Page 257 of 454

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