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

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

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Which <strong>Cutting</strong> Mechanism for Which Kind of Soil?<br />

<strong>The</strong> forces K1 and K2 on the blade, chisel or pick point are now:<br />

K<br />

K<br />

1<br />

2<br />

W2<br />

sin( ) W1<br />

sin( ) G sin( )<br />

<br />

sin( )<br />

Icos( ) Ccos( ) A cos( )<br />

<br />

sin( )<br />

W2<br />

sin( ) W1<br />

sin( ) G sin( )<br />

<br />

sin( )<br />

Icos( ) Ccos( )<br />

Acos( )<br />

<br />

sin( )<br />

(4-13)<br />

(4-14)<br />

<strong>The</strong> normal forces N1 on the shear plane and N2 on the blade are:<br />

<br />

<br />

N 1 K1<br />

cos<br />

and N 2 K2<br />

cos<br />

(4-15)<br />

<strong>The</strong> horizontal and vertical forces on the blade, chisel or pick point are:<br />

F h W2<br />

sin( ) K2<br />

sin( ) Acos(<br />

)<br />

(4-16)<br />

F W cos( ) K cos( ) Asin(<br />

)<br />

(4-17)<br />

v 2<br />

2<br />

<strong>The</strong> equilibrium of moments around the blade tip is:<br />

N<br />

W <br />

R G R N<br />

W <br />

1 1 1 3 2 2 2<br />

R<br />

(4-18)<br />

Analyzing these equations results in the following conclusions:<br />

At normal cutting angles in dredging, the argument of the cosine in the cohesive term of K1 is greater than 90<br />

degrees, resulting in a small positive term as a whole. Together with the adhesive term, this gives a positive<br />

normal stress on the shear plane. <strong>The</strong> minimum normal stress however equals the normal stress on the shear<br />

plane, minus the radius of the Mohr circle, which is the cohesion. <strong>The</strong> result may be a negative minimum<br />

normal stress. If this negative minimum normal stress is smaller than the negative tensile strength, the Tear<br />

Type will occur. This occurrence depends on the ratio between the adhesive force to the cohesive force. A<br />

large ratio will suppress the Tear Type.<br />

<strong>The</strong> adhesive force on the blade is proportional to the (mobilized) length of the blade, so the Curling Type<br />

may occur. <strong>The</strong> cohesive force on the shear plane is proportional to the (mobilized) cohesion, so the Tear<br />

Type may occur. <strong>The</strong> occurrence of the Curling Type or Tear Type depends on the ratio of the adhesive<br />

force to the cohesive force. A large ratio results in the Curling Type, a small ratio in the Tear Type.<br />

When the argument of the sine in the denominator gets close to 180 degrees, the forces become very large. If<br />

the argument is greater than 180 degrees, the forces would become negative. Since both conditions will not<br />

happen in nature, nature will find another cutting mechanism, the wedge mechanism. In clay this is not likely<br />

to occur, since there are only two angles in the argument of the sine in the denominator. It would require very<br />

large blade angles to occur.<br />

4.4. <strong>Cutting</strong> <strong>Rock</strong> Atmospheric.<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 under atmospheric conditions. Since the absolute hydrostatic pressure, which would result in a cavitation<br />

under pressure of the same magnitude can be neglected with respect to the compressive strength of the rock; the<br />

pore pressures are usually neglected. This results in a material where gravity, inertia, pore pressures and adhesion<br />

can be neglected.<br />

Copyright © Dr.ir. S.A. Miedema TOC Page 99 of 454

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