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sgr ms thesis - University of Maine

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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 />

61

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