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

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

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A Wedge in Dry <strong>Sand</strong> <strong>Cutting</strong>.<br />

Chapter 11:<br />

A Wedge in Dry <strong>Sand</strong> <strong>Cutting</strong>.<br />

11.1. Introduction.<br />

<strong>The</strong> cutting theories until now works well for small blade angles, however when the blade angle and the other<br />

angles involved increase, a problem with the model may occur. <strong>The</strong> basic equations contain a denominator with<br />

the sine of the sum of the blade angle, the shear angle, the internal friction angle and the external friction angle.<br />

So if the sum of these angles equals 180 degrees, the denominator is zero, meaning a division by zero giving<br />

infinity. Even worse, if the sum of these angles is greater than 180 degrees the sine gives a negative result, meaning<br />

the cutting forces become negative. But already if the sum of these angles approach 180 degrees the sine becomes<br />

very small and since it is in the denominator, the cutting forces would become very high. Now nature will normally<br />

choose the road of least resistance, nature will try to find another mechanism for the cutting process and this<br />

mechanism might be the occurrence of a wedge in front of the blade. This wedge will form a pseudo cutting blade<br />

A-C with a blade angle much smaller than the angle of the real blade. <strong>The</strong> probability of the occurrence of a wedge<br />

is large for sand and rock since all 4 angles mentioned play a role there. For clay the probability is much smaller,<br />

since in clay cutting normally the internal and external friction angles do not play a role.<br />

Now nature may choose another mechanism which will result in even smaller cutting forces, like the model of<br />

Hettiaratchi & Reece (1975), but their model is more complicated. <strong>The</strong> philosophy here is that if a mechanism can<br />

be found resulting in smaller cutting forces than the model used for small blade angles, this model will give a better<br />

prediction than the model for small blade angles. <strong>The</strong> wedge mechanism is such a mechanism, with the advantage<br />

that it is relatively simple to use and the cutting forces predicted with this model match the cutting forces from the<br />

experiments of Hatamura & Chijiiwa (1977B) pretty close. So from a pragmatic point of view this mechanism will<br />

be discussed for large blade angles.<br />

Figure 11-1: Definitions.<br />

Figure 11-2: Alternative geometry of<br />

the layer cut.<br />

Figure 11-3: <strong>The</strong> cutting mechanism.<br />

Copyright © Dr.ir. S.A. Miedema TOC Page 333 of 454

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