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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 />

Definitions:<br />

1. A: <strong>The</strong> wedge tip.<br />

2. B: End of the shear plane.<br />

3. C: <strong>The</strong> blade top.<br />

4. D: <strong>The</strong> blade tip.<br />

5. A-B: <strong>The</strong> shear plane.<br />

6. A-C: <strong>The</strong> wedge surface.<br />

7. A-D: <strong>The</strong> wedge bottom.<br />

8. D-C: <strong>The</strong> blade surface.<br />

9. hb: <strong>The</strong> height of the blade.<br />

10. hi: <strong>The</strong> thickness of the layer cut.<br />

11. vc: <strong>The</strong> cutting velocity.<br />

12. α: <strong>The</strong> blade angle.<br />

13. β: <strong>The</strong> shear angle.<br />

14. Fh: <strong>The</strong> horizontal force, the arrow gives the positive direction.<br />

15. Fv: <strong>The</strong> vertical force, the arrow gives the positive direction.<br />

For the weight of the layer cut G1, see chapter 5: Dry <strong>Sand</strong> <strong>Cutting</strong>.<br />

<strong>The</strong> weight of the wedge G2 is given by:<br />

2<br />

h <br />

b 1 1 <br />

G2 s<br />

g w<br />

2 <br />

<br />

tan tan<br />

<br />

<br />

<br />

(11-1)<br />

11.2. <strong>The</strong> Force Equilibrium.<br />

Figure 11-4 illustrates the forces on the layer of soil cut. <strong>The</strong> forces shown are valid in general for dry sand. <strong>The</strong><br />

forces acting on the layer A-B are:<br />

1. A normal force acting on the shear surface N1, resulting from the effective grain stresses.<br />

2. A shear force S1 as a result of internal friction N1·tan(φ.<br />

3. A gravity force G1 as a result of the weight of the layer cut.<br />

4. An inertial force I, resulting from acceleration of the soil.<br />

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

6. 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 />

<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 />

(11-2)<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 />

<strong>The</strong>se forces are shown in Figure 11-5. 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 />

(11-3)<br />

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

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

10. 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 />

Page 334 of 454 TOC Copyright © Dr.ir. S.A. Miedema

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