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Cranfield University

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Experimental Methods<br />

Depth, mm<br />

0<br />

100<br />

200<br />

300<br />

400<br />

500<br />

600<br />

700<br />

Displacement, mm<br />

0 50 100 150 200<br />

Figure 9: Soil displacement vs. depth after a pass of an 800/10.5/2.5b: □<br />

800/10.5/2.5; - - 5% and - 30% increase in density; and▲ LSD<br />

When Eq. 1 is differentiated with respect to depth, the displacement change, i.e. the aver-<br />

age increase in soil density is derived:<br />

�d(<br />

z)<br />

� � �d<br />

�(<br />

z)<br />

� s<br />

�z<br />

Eq. 2<br />

Thus │s│ is a direct measure of the relative increase in soil density caused by vertical soil<br />

movement and will be used to compare the treatments.<br />

The method to determine density increase by measuring soil displacement with the draw-<br />

string transducer is much more accurate than the gravimetrical method as shown by detect-<br />

ing significant differences between individual treatments. The maximum error in measur-<br />

ing the depth of a layer is +/- 0.5 mm which would result in less than 1% error in soil den-<br />

sity increase in the worst case; i.e. if all points over the 500 mm depth range line up in such<br />

a way that the top has a larger displacement of + 0.5 mm than in reality and the bottom has<br />

0.5 mm less than in reality. This is unlikely due to the large amount of measurements and<br />

handling errors do not exist with the drawstring method.<br />

The curvature of the soil displacement graph raised the question whether a linear function<br />

was appropriate. Fitting different regression functions to the soil displacement data justi-<br />

fied the linear regression function approach described earlier for a depth range from 0 –<br />

500 mm depth. Each full regression model function included both a non linear and a linear<br />

Ph.D. Thesis Dirk Ansorge (2007)<br />

16

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