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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 />

on the equilibrium of forces and the equilibrium of moments. So for now the mobilized adhesive force Am is used<br />

in the equations.<br />

<strong>The</strong> horizontal equilibrium of forces on the wedge:<br />

F h N 4 sin A m cos C 2 cos N 2 sin <br />

C 3 0<br />

(13-7)<br />

<strong>The</strong> vertical equilibrium of forces on the wedge:<br />

F v N 4 cos A m sin C 2 sin N 2 cos <br />

N 3 0<br />

(13-8)<br />

To derive N4:<br />

Multiply the horizontal equilibrium equation with sin(α).<br />

<br />

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

4 m 2<br />

<br />

N sin sin C sin 0<br />

2 3<br />

(13-9)<br />

Multiply the vertical equilibrium equation with cos(α).<br />

<br />

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

4 m 2<br />

<br />

N cos cos N cos 0<br />

2 3<br />

(13-10)<br />

Now add up the two resulting equations in order to get an expression for N4.<br />

<br />

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

(13-11)<br />

4 2 2 3 3<br />

<strong>The</strong> mobilized adhesive force Am can be derived according to:<br />

First multiply the horizontal equilibrium equation with cos(α).<br />

<br />

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

4 m 2<br />

<br />

N sin cos C cos 0<br />

2 3<br />

(13-12)<br />

Now multiply the vertical equilibrium equation with sin(α):<br />

<br />

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

4 m 2<br />

<br />

N cos sin N sin 0<br />

2 3<br />

(13-13)<br />

Subtracting the two resulting equations gives the equation for the mobilized adhesive force.<br />

<br />

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

(13-14)<br />

m 2 2 3 3<br />

This can also be rewritten as an equation for the normal force N3 on the bottom of the wedge.<br />

<br />

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

(13-15)<br />

3 4 m 2 2<br />

Copyright © Dr.ir. S.A. Miedema TOC Page 379 of 454

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