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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 />

Substituting the corrected shear angle gives for the mobilized shear strength:<br />

c m<br />

T<br />

<br />

/4 <br />

sin 2<br />

1<br />

sin<br />

<br />

<br />

<br />

1<br />

/4<br />

cos<br />

<br />

cos<br />

<br />

<br />

2<br />

<br />

<br />

<br />

(8-134)<br />

Now the cutting forces can be determined with:<br />

2c mhi wcos( )sin( )<br />

Fh HT Thi<br />

w<br />

cos( / 4) cos( )<br />

2c mhi wcos( )cos( )<br />

F<br />

VT T hi<br />

w<br />

cos( / 4) cos( )<br />

(8-135)<br />

(8-136)<br />

8.8. Specific Energy.<br />

For the cases as described above, cutting with a straight blade with the direction of the cutting velocity vc<br />

perpendicular to the blade (edge of the blade), the specific cutting energy Esp is:<br />

E<br />

sp<br />

Fh<br />

vc Fh<br />

<br />

h w v h w<br />

i c i<br />

(8-137)<br />

<strong>The</strong> specific energy of the Flow Type or Crushed Type of cutting mechanism can be written as:<br />

E<br />

sp HF<br />

c<br />

(8-138)<br />

<strong>The</strong> specific energy of the Tear Type or Chip Type of cutting mechanism can be written as:<br />

Esp HT T<br />

(8-139)<br />

Since the specific energy equations are based on the maximum horizontal cutting forces, where the cutting process<br />

is most probably either brittle shear or brittle tensile, the average cutting forces will be smaller. How much smaller<br />

depends on the type of rock, but literature mentions reductions by 30% to 70%. Since the specific energy is based<br />

on the average cutting forces, the values found with the above equations should be multiplied by a factor of 0.3-<br />

0.7.<br />

Copyright © Dr.ir. S.A. Miedema TOC Page 289 of 454

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