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<strong>of</strong> size distributions and surface patterns <strong>of</strong> Shatter Zone clasts, so fractal theory<br />
will now be applied to these breccia characteristics.<br />
5.3. Quantitative Methods <strong>of</strong> Breccia Classification<br />
5.3.1. Clast Size Distribution<br />
Particle size distribution is a commonly applied method for determining<br />
brecciation mechanis<strong>ms</strong> from observed clast characteristics (e.g. Harris, 1966;<br />
Harris, 1968; Hartmann, 1969; Schoutens, 1979; Sammis et al., 1986; Turcotte,<br />
1986; Sammis & Biegel, 1987; Englman et al., 1988; Marone and Scholz, 1989;<br />
Blenkinsop, 1991; Shimamoto and Nagahama, 1992; Nagahama and Yoshii,<br />
1993; McCaffrey & Johnston, 1996; Jebrak, 1997; Tsutsumi, 1999; Perfect, 1997;<br />
Zhang, 1999; Higgins, 2000; Blott & Pye, 2001; Wilson et al., 2001; Elek and<br />
Jaramaz, 2002; Saotome et al., 2002; Clark & James, 2003; Spieler et al., 2003;<br />
Barnett, 2004; Zi-Long et al., 2006; Farris & Paterson, 2007; Bjork et al., 2009).<br />
The term “clast size distribution” (CSD) is preferred because <strong>of</strong> its relevance to<br />
breccias. Brittle materials have the general tendency to fracture in a self-similar<br />
pattern in which clast frequency increases exponentially with a decrease in clast<br />
size, and it has been proven possible to relate the size distribution <strong>of</strong> clasts to the<br />
mechanism <strong>of</strong> brecciation (Turcotte, 1986; Jebrak, 1997; Perfect, 1997). The<br />
relationship between clast size and cumulate frequency is defined by the power<br />
law equation (similar to equation 5.2)<br />
(5.3)<br />
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