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

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The ratio <strong>of</strong> maximum principal stresses can be expressed in terms <strong>of</strong> <strong>the</strong> angle <strong>of</strong> internal friction,<br />

<br />

<br />

3<br />

1<br />

1<br />

2<br />

2<br />

(tan 1)<br />

tan<br />

, (Equation 4.5)<br />

1<br />

2<br />

2<br />

(tan 1)<br />

tan<br />

when cohesion is zero (McKinnon, pers. comm., 2009; see Appendix F for derivation). This<br />

allows for zones <strong>of</strong> eligible fracture reactivation to be mapped regardless <strong>of</strong> fracture orientation.<br />

Minimum-to-maximum principal stress ratios computed for plastic and elastic models in UDEC<br />

are shown in Figure 4.22. Such figures allow fields <strong>of</strong> fault reactivation to be contoured as a<br />

function <strong>of</strong> <strong>the</strong> internal angle <strong>of</strong> friction (Fig. 4.23). This demonstrates that, based on <strong>the</strong><br />

minimum-to-maximum principal stress ratio, <strong>the</strong>re is a large area to <strong>the</strong> south <strong>of</strong> <strong>the</strong> excavation,<br />

extending to <strong>the</strong> Return Air Raise Shear Zone where cohesionless fractures in any orientation can<br />

be reactivated, even at high friction angles. This is modelled in both elastic and plastic models.<br />

Based on stress conditions, slip is possible even in <strong>the</strong> yield zone, though seismogenic slip is not<br />

expected.<br />

Figure 4.22: Ratio <strong>of</strong> minimum-to-maximum principal stress for (A) elastic model; (B) plastic model.<br />

98

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