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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 />

A x B x C<br />

0<br />

2<br />

B B 4 A<br />

C<br />

a<br />

h<br />

hb,m<br />

x with: rm<br />

<br />

2<br />

A c<br />

h<br />

b,m<br />

i<br />

a cos<br />

<br />

sin<br />

2<br />

<br />

A <br />

sin<br />

(7-102)<br />

1<br />

a 2<br />

c<br />

B <br />

sin<br />

sin<br />

<br />

<br />

h<br />

i<br />

<br />

<br />

1<br />

c<br />

cos <br />

C hi<br />

h<br />

sin sin<br />

<strong>The</strong> following criteria are valid for the use of this method.<br />

i<br />

if h<br />

if h<br />

h then use h<br />

b,m b b,m<br />

h then use h<br />

b,m b b,m<br />

(7-103)<br />

To see which solution is valid, the terms of the equation have to be analyzed. For α+β0 and Cπ/2 the term A0 because of the minus sign. This will only result in a positive<br />

solution if the – sign is applied. So at small blade angles the plus sign gives the correct solution, while large blade<br />

angles require the minus sign solution.<br />

Figure 7-35, Figure 7-36 and Figure 7-37 show the shear angle and the horizontal cutting force coefficient and the<br />

vertical cutting force coefficient for the Curling Type. At large blade angles, both the horizontal and vertical<br />

forces become very large. In cases of large blade angles the Curling Type will hardly occur because the Flow<br />

Type results in smaller forces.<br />

<br />

<br />

<br />

sin<br />

<br />

<br />

<br />

sin<br />

<br />

<br />

<br />

<br />

<br />

<br />

sin sin<br />

rm<br />

<br />

sin sin<br />

F c h w c h w <br />

<br />

h s i s i HC<br />

cos cos<br />

rm<br />

<br />

sin sin<br />

F<br />

c h w c h w <br />

<br />

s i s i VC<br />

(7-104)<br />

(7-105)<br />

Page 226 of 454 TOC Copyright © Dr.ir. S.A. Miedema

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