Page 264 - Introduction to Mineral Exploration
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10: EVALUATION TECHNIQUES  247


                                                                     τ
                                               Yield point
                                                                                        Failure criterion


                                                                                               θ




                   σ                  Granite
                   Stress σ             Marble

                                                                          σ 3'  σ 3''         σ 1'  σ 1''

                                                              FIG. 10.28 An example of a Mohr diagram.
                                         Shale


                                          Clay                tested rock specimen. A value for c can also be
                                                              determined from the diagram.
                                                                The expected confining pressures and axial
                                 Strain ε ε                   loads that might be encountered in a mine can
                                                              be calculated. Any sample whose test results
                 FIG. 10.27  A simplified stress–strain diagram  plot as a Mohr diagram that falls below the tan-
                 illustrating the idealized deformational behavior  gent should not fail. A sample which failed in a
                 of some rock types. That of granite represents an  test with lower confining stresses but similar
                 idealized perfectly elastic material. Clay is a typical  axial stresses, would give rise to a circle which
                 material that behaves as a plastic material which  would cut the tangent suggesting that the crit-
                 will not deform until a certain stress is achieved.  ical stresses have been exceeded and failure
                 Marble is an example of an elastoplastic material  might occur (Peters 1987). This does not take
                 and shale represents a ductile material where stress  into account failure that might take place along
                 is not proportional to strain. (Modified after Peters
                 1987.)                                       discontinuities, nor does it consider the effects
                                                              of anisotropic stress systems in the rock mass
                                                              or changes that will occur with time.
                                                                The effect of discontinuities is probably more
                 where τ = total shearing resistance, σ n = normal  important than being able to measure the rock
                 stress acting at right angles to the failure plane,  strength. The discontinuities may be weak and
                 c = cohesive strength, tan θ = coefficient of in-  could result in failure at strengths below that of
                 ternal friction where θ = angle between stress  the rock itself.
                 fracture induced and  σ 1 . The theory behind
                 this equation is explained by Farmer (1983) and
                 Brady and Brown (1985).                      In situ stress determination
                   Triaxial test results are used to construct  Most in situ stress determinations are made be-
                 a Mohr diagram (Fig. 10.28). The symbol σ 3  rep-  fore mining takes place usually from a borehole
                 resents lateral confining pressures in succes-  drilled from the surface or from an adit. Two

                 sive tests, while  σ 1 represents the axial load  common procedures are employed in the deter-
                 required to break the rock. Circles are drawn  mination of in situ stress. The first is based on
                 using the distances between the different    the measurement of deformation on the bore-
                 values of σ 3  and σ 1  as the diameter. The com-  hole wall induced by overcoring (Fig. 10.29) and
                 mon tangent to these circles is known as the  the second by measuring the component of
                 Coulomb strength envelope. The angle θ can   pressure in a borehole or slot needed to balance
                 be determined from the diagram, rather than  the  in situ stress. In the overcoring system,
                 having to measure the fracture angle on the  a strain gauge is fixed to the borehole wall
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