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therefore it is possible to relate a breccia to its mechanism <strong>of</strong> formation by<br />
analyzing these self-similar characteristics.<br />
5.2. Fractal Theory<br />
When an object shows self-similar properties, it is described as fractal.<br />
Fractal theory sprouted from the desire to quantitatively describe geometries<br />
observed in nature. Unlike Euclidean geometry, fractals refer to complex shapes<br />
defined by a fractional, or fractal, dimension (D) (Mandelbrot, 1967, 1983; Urtson,<br />
2005). Founded by Benoit Mandelbrot in 1967, fractal theory has since been<br />
applied to many scientific proble<strong>ms</strong>. The self-similarity <strong>of</strong> fractals implies that<br />
patterns tend to repeat the<strong>ms</strong>elves at all scales, and for a true fractal, the<br />
number <strong>of</strong> scales <strong>of</strong> natural patterns is infinite. For the initial purposes <strong>of</strong> this<br />
<strong>thesis</strong>, it is best to consider the fractal dimension in ter<strong>ms</strong> <strong>of</strong> a repeated pattern<br />
<strong>of</strong> size distribution. Consider the repeated pattern in Figure 5.2 (Sammis et al.,<br />
1987). Sections <strong>of</strong> a cube are repeatedly split into smaller and smaller<br />
components, producing a distribution <strong>of</strong> various sizes. This pattern is quantified<br />
by<br />
(5.2)<br />
Assuming that the pattern <strong>of</strong> size distribution produced by breaking the cube is<br />
fractal, the fractal dimension is a function <strong>of</strong> the number <strong>of</strong> cubes with side<br />
length . For the broken cube, the pattern <strong>of</strong> size distribution is fractal, and =<br />
2.58. This value is unique to this size distribution and any change from this<br />
pattern would produce a different<br />
. Interest lies in the self-similar characteristics<br />
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