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Rock Mechanics.pdf - Mining and Blasting

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ROCK SUPPORT AND REINFORCEMENT<br />

If, for example, T = 10 tonne = 100 kN, = 25 kN m−3 <strong>and</strong> D = 4 m, equation<br />

11.8 gives s = 1.0 m.<br />

In this application, care must be taken to ensure that the bolt anchors have an<br />

adequate factor of safety against failure under the working load, T . This design<br />

method is conservative in that it does not allow for the shear or flexural strength of<br />

the strata above the abutments.<br />

Lang <strong>and</strong> Bischoff (1982) extended this elementary analysis to incorporate the<br />

shear strength developed by the rock mass on the vertical boundaries of the rock unit<br />

reinforced by a single rockbolt. The rock is assumed to be destressed to a depth, D,<br />

as in Figure 11.13, but variable vertical stresses, v, <strong>and</strong> horizontal stresses, k v, are<br />

assumed to be induced within the de-stressed zone. Typically, k may be taken as 0.5.<br />

The shear strength developed at any point on the perimeter of the reinforced rock<br />

unit is given by c + kv, where c is the cohesion <strong>and</strong> = tan is the coefficient of<br />

friction for the rock mass. Lang <strong>and</strong> Bischoff’s analysis leads to the result<br />

T <br />

=<br />

AR k<br />

<br />

1 − c<br />

R<br />

1 − exp(−kD/R)<br />

1 − exp(−kL/R)<br />

<br />

(11.9)<br />

where T = rockbolt tension, A = area of roof carrying one bolt (= s 2 for a s × s<br />

bolt spacing), R = shear radius of the reinforced rock unit, = A/P, where P is the<br />

shear perimeter (= 4s for a s × s bolt spacing), = a factor depending on the time<br />

of installation of the rockbolts ( = 0.5 for active support, <strong>and</strong> = 1.0 for passive<br />

reinforcement), <strong>and</strong> L = bolt length which will often be less than D, the height of<br />

the de-stressed zone of rock.<br />

Lang <strong>and</strong> Bischoff suggest that, for preliminary analyses, the cohesion, c, should<br />

be taken as zero. Design charts based on equation 11.9 show that, particularly for<br />

low values of , the required bolt tension, T , increases significantly as L/s decreases<br />

below about two, but that no significant reduction in T is produced when L/s is<br />

increased above two. This result provides some corroboration of Lang’s empirical<br />

rule that the bolt length should be at least twice the spacing. For a given set of data,<br />

equation 11.9 will give a lower required bolt tension than that given by equation<br />

11.8. Clearly, Lang <strong>and</strong> Bischoff’s theory applies more directly to the case of the<br />

development of a zone of reinforced, self-supporting rock, than to the simpler case<br />

of the support of the total gravity load produced by a loosened volume of rock or by<br />

a roof beam in laminated rock.<br />

Design to support a triangular or tetrahedral block. In Chapter 9, the identification<br />

of potential failure modes of triangular <strong>and</strong> tetrahedral blocks was discussed, <strong>and</strong><br />

analyses were proposed for the cases of symmetric <strong>and</strong> asymmetric triangular roof<br />

prisms. These analyses take account of induced elastic stresses <strong>and</strong> discontinuity<br />

deformability, as well as allowing for the self-weight of the block <strong>and</strong> for support<br />

forces. The complete analysis of a non-regular tetrahedral wedge is more complex.<br />

An otherwise complete solution for the tetrahedral wedge which does not allow for<br />

induced elastic stresses is given by Hoek <strong>and</strong> Brown (1980).<br />

The analyses presented in Chapter 9 may be incorporated into the design procedure.<br />

Consider the two-dimensional problem illustrated in Figure 11.14 to which the<br />

analysis for an asymmetric triangular prism may be applied. If it is assumed that the<br />

normal stiffnesses of both discontinuities are much greater than the shear stiffnesses,<br />

328

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