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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 />

<br />

<br />

<br />

2 kmax<br />

z 10<br />

0<br />

2 <br />

sin <br />

<br />

vc<br />

<br />

sin <br />

<br />

<br />

(6-109)<br />

<strong>The</strong> distance from the blade to the cavitation spot is considered to be constant over the blade. <strong>The</strong> magnitude of<br />

this distance is however unknown.<br />

Figure 6-49: <strong>The</strong> development of cavitation over the blade.<br />

<strong>The</strong> relation between the dimensions of the cavitation spot, and the water pressure profile on the blade.<br />

<strong>The</strong> progressive character of the cavitation spot development results from equation (6-109). If, at a certain cutting<br />

velocity, cavitation occurs locally in the cavitation zone, then the resulting cavitation spot will always expand<br />

immediately over a certain distance above the blade as a result of the fact that a certain time is needed to fill the<br />

volume flow rate of the vapor bubbles. <strong>The</strong> development of the water sub-pressures will, in general, be influenced<br />

by the ever in the pore water present dissolved air. As soon as water sub-pressures are developing as a result of the<br />

increase in volume in the shear zone, part of the dissolved air will form air bubbles. Since these air bubbles are<br />

compressible, a large part of the volume strain will be taken in by the expansion of the air bubbles, which results<br />

in a less fast increase of the water sub-pressures with an increasing cutting velocity. <strong>The</strong> maxima of the water subpressures<br />

will also be influenced by the present air bubbles. This can be illustrated with the following example:<br />

Assume the sand contains 3 volume percent air, which takes up the full volume strain in the dilatancy zone. With<br />

a volume strain of 16%, this implies that after expansion, the volume percentage air is 19%. Since it is a quick<br />

process, it may be assumed that the expansion is adiabatic, which amounts to maximum water sub-pressures of<br />

0.925 times the present hydrostatic pressure. In an isothermal process the maximum water sub-pressures are 0.842<br />

times the present hydrostatic pressure. From this simple example it can be concluded that the, in the pore water<br />

present (either dissolved or not) air, has to be taken into account. In the verification of the water sub-pressures,<br />

measured during the cutting tests in the 105 m sand, the possibility of a presence of dissolved air is recognized<br />

but it appeared to be impossible to quantify this influence. It is however possible that the maximum water subpressures<br />

reached (Appendix M the pore pressure graphs) are limited by the in the pore water present dissolved<br />

air.<br />

Page 178 of 454 TOC Copyright © Dr.ir. S.A. Miedema

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