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Rock Mechanics.pdf - Mining and Blasting

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Figure 15.2 Shear stress drop in the<br />

transition from static to dynamic conditions<br />

on a fault (after Ryder, 1987).<br />

Figure 15.3 Retrospective analysis<br />

of a large seismic event in terms of excess<br />

shear stress (after Ryder, 1987).<br />

LONGWALL AND CAVING MINING METHODS<br />

rockburst than in a pillar burst due to the larger volume of rock involved. However,<br />

in an operating stope, a local pillar or face burst may be as destructive as a large<br />

slip on an adjacent fault. Techniques are required to identify mining layouts which<br />

may be subject to each type of burst, <strong>and</strong> to develop preferred extraction layouts <strong>and</strong><br />

sequences to restrict burst frequency.<br />

15.2.2 <strong>Rock</strong>burst controls<br />

The concept of the ‘stress drop’ on a fault subject to frictional sliding was introduced<br />

in Chapter 10. It is defined by (s − d), the difference between the limiting static <strong>and</strong><br />

dynamic shear strengths at the prevailing normal stress, in the transition from static<br />

to dynamic conditions on the fault. The average stress drop, e, illustrated in Figure<br />

15.2, has been suggested to be in the range 0.1–10 MPa (Spottiswoode <strong>and</strong> McGarr,<br />

1975). Stress drops of 5–10% of the static shear strength of a fault have been observed<br />

in the laboratory.<br />

Application of notions of stress drop in rockburst mechanics has been discussed by<br />

Ryder (1987). It was proposed that the excess shear stress (ESS) on a fault, defined<br />

by the stress drop (e = s − d), may be used as an indicator of the potential for<br />

unstable slip on a fault, as it is the forcing function for the motion.<br />

In an analysis of rock mass deformation associated with a major seismic event at<br />

a deep gold mine, Ryder (1987) calculated the state of stress on the affected fault<br />

using a boundary element method. ESS contours were mapped on to the plane of<br />

the fault, <strong>and</strong> compared with the shear displacements on the fault which attended the<br />

event. The plots of ESS <strong>and</strong> shear displacements shown in Figure 15.3 indicate that<br />

the region of maximum fault ride is concentrated in the zone of relatively high ESS.<br />

The good correlation between ESS <strong>and</strong> observed fault slip suggests the prospect of<br />

predicting conditions under which seismic events may occur from the ESS parameter.<br />

However, it may be noted that stress analysis for this purpose should take account<br />

of progressive displacement on planes of weakness liable to slip, <strong>and</strong> not be based<br />

432

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