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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 />

In the case of wear calculations the normal and friction forces on the front side and the wear flat can be interesting.<br />

According to Evans the normal and friction forces are the same on both sides, since this was the starting point of<br />

the derivation, this gives for the normal force Rn:<br />

1<br />

Rn<br />

T h w cos <br />

1<br />

sin 2 <br />

<br />

<br />

<br />

(8-69)<br />

<strong>The</strong> friction force Rf is now:<br />

1<br />

Rf<br />

T h w sin <br />

1<br />

sin 2 <br />

<br />

<br />

<br />

(8-70)<br />

8.3.4. Summary of the Evans <strong>The</strong>ory.<br />

Figure 8-23: <strong>The</strong> model of Evans used for a pick point.<br />

<strong>The</strong> Evans theory has been derived for 3 cases:<br />

1. <strong>The</strong> basic case with a horizontal moving chisel and the centerline of the chisel horizontal.<br />

2. A horizontal moving chisel with the centerline under an angle ε.<br />

3. A pick point with the centerline angle ε equal to half the top angle α, horizontally moving.<br />

Once again it should be noted that the angle α as used by Evans is half the top angle of the chisel and not the blade<br />

angle as α is used for in most equations in this book. In case 1 the blade angle would be α as used by Evans, in<br />

case 2 the blade angle is α+ε and in case 3 the blade angle is 2·α. In all cases it is assumed that the cutting velocity<br />

vc is horizontal.<br />

Copyright © Dr.ir. S.A. Miedema TOC Page 267 of 454

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