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sgr ms thesis - University of Maine

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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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