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Rock Mechanics.pdf - Mining and Blasting

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Figure 4.46 Influence of scale on<br />

the three components of discontinuity<br />

shear strength (after B<strong>and</strong>is et al.,<br />

1981).<br />

SHEAR BEHAVIOUR OF DISCONTINUITIES<br />

decreases, <strong>and</strong> so the nett apparent friction angle decreases. As the scale increases, the<br />

steeper asperities shear off <strong>and</strong> the inclination of the controlling roughness decreases.<br />

Similarly, the asperity failure component of roughness decreases with increasing<br />

scale because the material compressive strength, JCS, decreases with increasing size<br />

as discussed in section 4.3.5.<br />

4.7.5 Infilled discontinuities<br />

The previous discussion referred to ‘clean’ discontinuities or discontinuities containing<br />

no infilling materials. As noted in section 3.3, discontinuities may contain infilling<br />

materials such as gouge in faults, silt in bedding planes, low-friction materials such<br />

as chlorite, graphite <strong>and</strong> serpentine in joints, <strong>and</strong> stronger materials such as quartz or<br />

calcite in veins or healed joints. Clearly, the presence of these materials will influence<br />

the shear behaviour of discontinuities. The presence of gouge or clay seams can<br />

decrease both stiffness <strong>and</strong> shear strength. Low-friction materials such as chlorite,<br />

graphite <strong>and</strong> serpentine can markedly decrease friction angles, while vein materials<br />

such as quartz can serve to increase shear strengths.<br />

Of particular concern is the behaviour of major infilled discontinuities in which the<br />

infilling materials are soft <strong>and</strong> weak, having similar mechanical properties to clays<br />

<strong>and</strong> silts. The shear strengths of these materials are usually described by an effective<br />

stress Coulomb law. In a laboratory study of such filled discontinuities, Ladanyi <strong>and</strong><br />

Archambault (1977) reached the following conclusions:<br />

(a) For most filled discontinuities, the peak strength envelope is located between<br />

that for the filling <strong>and</strong> that for a similar clean discontinuity.<br />

(b) The stiffnesses <strong>and</strong> shear strength of a filled discontinuity decrease with increasing<br />

filling thickness, but always remain higher than those of the filling<br />

alone.<br />

(c) The shear stress–displacement curves of filled discontinuities often have two<br />

portions, the first reflecting the deformability of the filling materials before rock<br />

to rock contact is made, <strong>and</strong> the second reflecting the deformability <strong>and</strong> shear<br />

failure of rock asperities in contact.<br />

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