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

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 />

6. A shear force C2 as a result of the mobilized cohesion between the soil and the wedge c. This force can be<br />

calculated by multiplying the cohesive shear strength c of the soil with the contact area between the soil and<br />

the wedge.<br />

<strong>The</strong> normal force N1 and the shear force S1 can be combined to a resulting grain force K1.<br />

2 2<br />

1 1 1<br />

K N S<br />

(14-1)<br />

<strong>The</strong> forces acting on the wedge front or pseudo blade A-C when cutting soil, can be distinguished as:<br />

7. A force normal to the blade N2, resulting from the effective grain stresses.<br />

8. A shear force S2 as a result of the soil/soil friction N2·tan(λ between the layer cut and the wedge pseudo<br />

blade. <strong>The</strong> friction angle λ does not have to be equal to the internal friction angle φ in the shear plane, since<br />

the soil has already been deformed.<br />

9. A shear force C2 as a result of the cohesion between the layer cut and the pseudo blade c. This force can be<br />

calculated by multiplying the cohesive shear strength c of the soil with the contact area between the soil and<br />

the pseudo blade.<br />

<strong>The</strong>se forces are shown in Figure 14-3. If the forces N2 and S2 are combined to a resulting force K2 and the adhesive<br />

force and the water under pressures are known, then the resulting force K2 is the unknown force on the blade. By<br />

taking the horizontal and vertical equilibrium of forces an expression for the force K2 on the blade can be derived.<br />

2 2<br />

2 2 2<br />

K N S<br />

(14-2)<br />

<strong>The</strong> forces acting on the wedge bottom A-D when cutting soil, can be distinguished as:<br />

10. A force N3, resulting from the effective grain stresses, between the wedge bottom and the undisturbed soil.<br />

11. A shear force S3 as a result of the soil/soil friction N3·tan(φ between the wedge bottom and the undisturbed<br />

soil.<br />

12. A shear force C3 as a result of the cohesion between the wedge bottom and the undisturbed soil c. This force<br />

can be calculated by multiplying the cohesive shear strength c of the soil with the contact area between the<br />

wedge bottom and the undisturbed soil.<br />

<strong>The</strong> normal force N3 and the shear force S3 can be combined to a resulting grain force K3.<br />

2 2<br />

3 3 3<br />

K N S<br />

(14-3)<br />

<strong>The</strong> forces acting on a straight blade C-D when cutting soil (see Figure 14-4), can be distinguished as:<br />

16. A force normal to the blade N4, resulting from the effective grain stresses.<br />

17. A shear force S4 as a result of the soil/steel friction N4·tan(.<br />

<strong>The</strong> normal force N4 and the shear force S4 can be combined to a resulting grain force K4.<br />

2 2<br />

4 4 4<br />

K N S<br />

(14-4)<br />

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

F h K 1 sin( ) C 1 cos( ) C 2 cos( ) K 2 sin( ) 0<br />

(14-5)<br />

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

F v K 1 cos( ) C 1 sin( ) C 2 sin( ) K 2 cos( ) 0<br />

(14-6)<br />

<strong>The</strong> force K1 on the shear plane is now:<br />

K<br />

1<br />

C1 cos( ) C2 cos( )<br />

<br />

sin( )<br />

(14-7)<br />

Page 386 of 454 TOC Copyright © Dr.ir. S.A. Miedema

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