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title of the thesis - Department of Geology - Queen's University

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quadrants <strong>of</strong> dilatation and compression, respectively) and are oriented orthogonal to each o<strong>the</strong>r<br />

and 45° to <strong>the</strong> nodal planes (Fig. 3.11; Stein and Wysession, 2003. P- and T-axes approximate<br />

maximum principal stresses, though <strong>the</strong>se can differ significantly if failure occurs along preexisting<br />

structure (Gephart and Forsyth, 1984).<br />

Figure 3.10: Block model <strong>of</strong> a shear-slip event and corresponding focal mechanism and waveforms,<br />

modified from Stein and Wysession, (2003).<br />

Solutions are limited to pure shear event mechanisms only, that is, mechanisms with doublecouple<br />

sources. Double couple (DC) sources have source radiation patterns that can be described<br />

by coupled forces with no net torque (Fig. 3.11; Stein and Wysession, 2003).<br />

Figure 3.11: (Left) coupled forces along fault and auxiliary planes; (middle) paired force couples (doublecouple);<br />

(right) resultant fault plane solution, where shaded quadrants are in compression. Modified from<br />

Stein and Wysession, (2003).<br />

Events involving interaction between more than one fracture, volume change and those having<br />

mixed mechanisms cannot be represented using <strong>the</strong> fault plane solution method (Miller et al.,<br />

1998; Stein and Wysession, 2003). Voids created by mining <strong>of</strong>ten cause extension and thus non-<br />

59

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