title of the thesis - Department of Geology - Queen's University
title of the thesis - Department of Geology - Queen's University
title of the thesis - Department of Geology - Queen's University
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clustering are indications <strong>of</strong> rock mass yielding and increased hazard (Vasak, n.d.). Progressive<br />
yielding and tensile failure will eventually render <strong>the</strong> rock mass aseismic, as <strong>the</strong> rock begins to<br />
behave in a plastic manner, transferring stress to <strong>the</strong> surrounding, more intact rock.<br />
Similar to <strong>the</strong> degradation process described by seismic event parameters in Chapter 3, <strong>the</strong><br />
distribution <strong>of</strong> stress around <strong>the</strong> excavation is suggestive <strong>of</strong> a progressive damage process. In <strong>the</strong><br />
yield zone, in situ strength reduction <strong>of</strong> <strong>the</strong> rock mass occurs as a result <strong>of</strong> unloading from a loss<br />
<strong>of</strong> confinement, stress rotation, crack-surface interaction and rock mass heterogeneity (Diederichs,<br />
2003). Rockmass failures caused by stress and marked by seismicity can occur along existing<br />
fractures or through <strong>the</strong> creation <strong>of</strong> new fractures in <strong>the</strong> damage zone beyond <strong>the</strong> yield zone. Both<br />
failure mechanisms are explored in <strong>the</strong> following sections by mapping slip conditions and rock<br />
mass degradation stress.<br />
4.6.1 Fracture Reactivation<br />
The reactivation <strong>of</strong> favourably oriented fractures is mechanically preferable to <strong>the</strong> creation <strong>of</strong> new<br />
fractures; when failure occurs, cohesion is lost. This lowers <strong>the</strong> Mohr-Coulomb failure envelope<br />
and field <strong>of</strong> stability, outlined in Figure 4.4, and allows rock to fail at lower shear and normal<br />
stress values. In Creighton, <strong>the</strong> rock mass in proximity to <strong>the</strong> excavation is assumed to be<br />
fractured, as inferred from both stress modelling and <strong>the</strong> distribution <strong>of</strong> seismicity. Fracture<br />
reactivation is thus a likely candidate for seismic emission. Zones subject to fracture reactivation<br />
can be mapped using Mohr-Coulomb failure conditions:<br />
<br />
n<br />
tan C<br />
(Equation 4.2)<br />
and <strong>the</strong> definitions <strong>of</strong> maximum normal and shear stresses,<br />
<br />
max<br />
1<br />
2<br />
<br />
and <br />
<br />
1<br />
3<br />
max<br />
1<br />
<br />
1 3<br />
. (Equations 4.3 and 4.4)<br />
2<br />
97