Page 136 - Rock Mechanics For Underground Mining
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ROCK STRENGTH AND DEFORMABILITY

              Figure 4.33  Variation of peak prin-
              cipal stress difference with the angle
              of inclination of the major principal
              stress to the plane of weakness, for the
              confining pressures indicated for (a) a
              phyllite (after Donath, 1972), (b–d) a
              slate and two shales (after McLamore
              and Gray, 1967).




































                                        measured variations in peak principal stress difference with the angle of inclination
                                        of the major principal stress to the plane of weakness.
                                          Jaeger (1960) introduced an instructive analysis of the case in which the rock
                                        contains well-defined, parallel planes of weakness whose normals are inclined at an
                                        angle   to the major principal stress direction as shown in Figure 4.34a. Each plane
                                        of weakness has a limiting shear strength defined by Coulomb’s criterion
                                                                                                      (4.29)
                                                                  s = c w +   n tan   w
                                        Slip on the plane of weakness (ab) will become incipient when the shear stress on
                                        the plane,  , becomes equal to, or greater than, the shear strength, s. The stress
              Figure 4.34  (a) Transversely iso-  transformation equations give the normal and shear stresses on ab as
              tropic specimen in triaxial compres-
                                                               1
                                                                          1
              sion; (b) variation of peak strength at        n = (  1 +   3 ) + (  1 −   3 ) cos 2
                                                               2          2
              constant confining pressure with the
              angle of inclination of the normal to  and
              the plane of weakness to the compres-
                                                                     1
              sion axis ( ).                                       = (  1 −   3 ) sin 2               (4.30)
                                                                     2
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