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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>Rock</strong> <strong>Cutting</strong>: Atmospheric Conditions.<br />

8.4. <strong>The</strong> Flow Type (Based on the Merchant <strong>Model</strong>).<br />

<strong>Rock</strong> is the collection of materials where the grains are bonded chemically from very stiff clay, sandstone to very<br />

hard basalt. It is difficult to give one definition of rock or stone and also the composition of the material can differ<br />

strongly. Still it is interesting to see if the model used for sand and clay, which is based on the Coulomb model,<br />

can be used for rock as well. Typical parameters for rock are the compressive strength UCS and the tensile strength<br />

BTS and specifically the ratio between those two, which is a measure for how fractured the rock is. <strong>Rock</strong> also has<br />

shear strength and because it consists of bonded grains it will have an internal friction angle and an external friction<br />

angle. It can be assumed that the permeability of the rock is very low, so initially the pore pressures do no play a<br />

role or cavitation will always occur under atmospheric conditions. But since the absolute hydrostatic pressure,<br />

which would result in a cavitation under pressure of the same magnitude can be neglected with respect to the<br />

compressive strength of the rock; the pore pressures are usually neglected. This results in a material where gravity,<br />

inertia, pore pressures and adhesion can be neglected.<br />

Merchant (1944), (1945A) and (1945B) derived a model for determining the cutting forces when machining steel.<br />

<strong>The</strong> model was based on plastic deformation and a continuous chip formation (ductile cutting). <strong>The</strong> model included<br />

internal and external friction and shear strength, but no adhesion, gravity, inertia and pore pressures. Later<br />

Miedema (1987 September) extended this model with adhesion, gravity, inertial forces and pore water pressures.<br />

Definitions:<br />

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

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

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

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

5. A-C: <strong>The</strong> blade surface.<br />

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

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

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

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

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

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

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

Figure 8-26 gives some definitions regarding the cutting process. <strong>The</strong> line A-B is considered to be the shear plane,<br />

while the line A-C is the contact area between the blade and the soil. <strong>The</strong> blade angle is named α and the shear<br />

angle β. <strong>The</strong> blade is moving from left to right with a cutting velocity vc. <strong>The</strong> thickness of the layer cut is hi and<br />

the vertical height of the blade hb. <strong>The</strong> horizontal force on the blade Fh is positive from right to left always opposite<br />

to the direction of the cutting velocity vc. <strong>The</strong> vertical force on the blade Fv is positive downwards. Since the<br />

vertical force is perpendicular to the cutting velocity, the vertical force does not contribute to the cutting power Pc,<br />

which is equal to:<br />

Pc Fh vc<br />

(8-96)<br />

Figure 8-26: <strong>The</strong> definitions of the cutting process.<br />

Copyright © Dr.ir. S.A. Miedema TOC Page 273 of 454

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