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outline <strong>of</strong> the clast, with a dark backbone directly over the border that brightens<br />
up with distance from the outline. The brightness <strong>of</strong> the pixel is directly<br />
proportional to the distance to the clast border, and an outline <strong>of</strong> known width is<br />
made by setting a threshold to that value <strong>of</strong> brightness. D r can be calculated by<br />
plotting the log <strong>of</strong> ribbon area A versus the grayscale number W and is obtained<br />
by<br />
(5.6)<br />
with S as the slope subtracted from the Euclidean dimension <strong>of</strong> 2 to yield D r . The<br />
Euclidean dimension 2 signifies that the clast exists on a two-dimensional<br />
surface (Berube and Jebrak 1999, Lorilleux et al. 2002).<br />
5.3.4. The Fractal Dimension-Brecciation Mechanism Link for Clast<br />
Boundary Shape (CBS)<br />
The most complex boundary shapes come from chemical breccias (D r<br />
≥1.25), while the simplest are found in hydraulic or magmatic breccias (D r ≤ 1.1)<br />
(Jebrak, 1997; Barnett, 2004). Explosive and abrasive breccias initially produce<br />
angular clasts that may show relative complexity, but D r would still be relatively<br />
low (≤ 1.25). CBS would tend to be low in a physically brecciated material<br />
because fractures tend to align the<strong>ms</strong>elves with the direction <strong>of</strong> the maximum<br />
principal stress. Because the direction <strong>of</strong> fracture would tend not to change, the<br />
surface pattern <strong>of</strong> the fracture is defined by the paths <strong>of</strong> relatively straight cracks<br />
(Berube and Jebrak, 1999). Modification processes that involve clast rounding<br />
and corner break-<strong>of</strong>f would also effectively reduce D r . It is unlikely that chemical<br />
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