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esolution images <strong>of</strong> each box were stitched to create the image mosaics (Figure<br />
6.9). Clasts were manually outlined from each mosaic in a drafting program to<br />
differentiate between clast and matrix, producing a black (clast) and white<br />
(matrix) image. Manual outlining was required because the grayscale separation<br />
between clasts and matrix was commonly too small to accurately distinguish<br />
them using image analysis s<strong>of</strong>tware (e.g. Sudhakar et al. 2005). The outlines<br />
were analyzed with NIH ImageJ for clast count, area, circularity, and boundary<br />
shape. CSD, CBS, and CCA data were calculated from these output data. The<br />
number <strong>of</strong> clasts used for CBS was limited compared to CSD because each<br />
randomly chosen outline had to be analyzed individually.<br />
For CSD <strong>of</strong> the Shatter Zone breccias, the equivalent radius was used to<br />
plot data on a logarithmic size cumulate frequency plot, with a clast radius<br />
interval <strong>of</strong> 10 0.02 cm. Only clasts greater than 1mm radius were plotted because<br />
<strong>of</strong> difficulty in distinguishing between smaller clasts and the granite matrix.<br />
Cumulate frequency was standardized to the total area covered for each outcrop<br />
location to allow better comparison between locations with greater or smaller<br />
outcrop representation. D s values were calculated from equation (5.3).<br />
CBS data were produced by 42 ribbon width and area measurements for<br />
428 clast outlines. Measurements were taken in NIH ImageJ. The log <strong>of</strong> ribbon<br />
width was plotted with respect to the log <strong>of</strong> ribbon area, and D r was calculated<br />
from the slope using equation (5.6).<br />
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