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

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

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A Wedge in <strong>Clay</strong> <strong>Cutting</strong>.<br />

L3 L7<br />

<br />

N3 cos N2 cos <br />

L4 2<br />

L4<br />

<br />

L5<br />

<br />

C2 sin C3 sin <br />

2<br />

L4<br />

<br />

<br />

(13-27)<br />

Now N3 can be expressed in a number of known variables according to:<br />

N<br />

3<br />

L7<br />

L5<br />

<br />

N2 cos C2 sin <br />

2<br />

L4 2<br />

L4<br />

<br />

<br />

L3<br />

<br />

cos<br />

L4<br />

<br />

C3<br />

sin <br />

<br />

L3<br />

<br />

cos<br />

<br />

L4<br />

<br />

<br />

<br />

(13-28)<br />

Substituting equation (13-28) in equation (13-11) gives a solution for the normal force N4.<br />

<br />

N C sin N cos C sin N cos<br />

(13-29)<br />

4 2 2 3 3<br />

Substituting equation (13-28) in equation (13-14) gives a solution for the mobilized adhesion Am.<br />

<br />

A C cos N sin C cos N sin<br />

(13-30)<br />

m 2 2 3 3<br />

This results in a horizontal force of:<br />

<br />

<br />

(13-31)<br />

F N sin A cos<br />

h 4 m<br />

And in a vertical force of:<br />

<br />

<br />

(13-32)<br />

F N cos A sin<br />

v 4 m<br />

Based on the experience with sand cutting it is assumed that the wedge angle θ can be determined by assuming<br />

that the horizontal force should be at a minimum for the angle chosen. It is very well possible that the mobilized<br />

adhesion is negative for large blade angles.<br />

Copyright © Dr.ir. S.A. Miedema TOC Page 383 of 454

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