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Rock Mechanics.pdf - Mining and Blasting

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Figure 7.18 Contour plots of principal<br />

stress, <strong>and</strong> stress trajectories,<br />

around an ovaloidal opening in a biaxial<br />

stress field (after Eissa, 1980).<br />

EXCAVATION DESIGN IN MASSIVE ELASTIC ROCK<br />

the appropriate m <strong>and</strong> s values for the rock mass <strong>and</strong> replacing c by cd. For purposes<br />

of illustration of the method, defining the zone of failure involves examination of<br />

contour plots of the principal stresses, similar to the stress maps showns in Figure<br />

7.18. For more general shapes of openings, such stress contour maps are readily<br />

generated <strong>and</strong> displayed using computational techniques.<br />

Mapping of the zone of failure uses the rock mass failure criterion <strong>and</strong> the stress<br />

contour maps in the following way. Various values of 3(0.05p, 0.1p, etc.) are used to<br />

calculate corresponding, limiting values of (f)<br />

1 from the failure criterion. The contour<br />

plots of 1 <strong>and</strong> 3 are superimposed. Selecting a particular 3 isobar, the intersection<br />

is found with the 1 isobar which satisfies the failure criterion. Repetition of this<br />

process for the various values of 3 generates a set of points which together define<br />

the boundary of the failure domain.<br />

When dealing computationally with failure domain delineation, explicit generation<br />

of principal stress contour maps is not required. At any interior point, the computed<br />

state of stress is inserted directly into the failure criterion to determine local rock<br />

behaviour. The condition at a large number of locations throughout the rock mass can<br />

be displayed symbolically on a computer graphics terminal, for visual identification<br />

of the failure zone.<br />

216

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