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ROCK STRENGTH AND DEFORMABILITY

                                        4.4.2  Biaxial compression (  1     2 ,   3 = 0)
                                        Biaxial compression tests are carried out by applying different normal stresses to
                                        two pairs of faces of a cube, plate or rectangular prism of rock. The great difficulty
                                        with such tests is that the end effects described in section 4.3.3 exert an even greater
                                        influence on the stress distribution within the specimen than in the case of uniaxial
                                        compression. For this reason, fluid rather than solid medium loading is preferred. An
                                        alternative approach is to generate a biaxial state of stress at the inner surface of a
                                        hollow cylinder by loading it axially with a fluid pressure applied to its outer surface
                                        (Hoskins, 1969, Jaeger and Cook, 1979) in a triaxial cell (section 4.4.3). However, in
                                        this case, the stresses at ‘failure’ cannot be measured, but must be calculated using the
                                        theory of elasticity which may not be applicable at peak stress. The inner boundary of
                                        the hollow cylinder is a zone of high stress gradient which could influence the result.
                                        For these reasons, it is recommended that the use of hollow cylinder tests be restricted
                                        to the simulation of particular rock mechanics problems such as the behaviour of rock
                                        around a shaft, bored raise or borehole.
                                          Brown (1974) carried out a series of biaxial compression tests on 76 mm square by
                                        25 mm thick plates of Wombeyan Marble which were loaded on their smaller faces
                                        through (a) 76 mm × 25 mm solid steel platens, and (b) brush platens made from
                                        3.2 mm square steel pins. Figure 4.15 shows the peak strength envelopes obtained
                                        in tests carried out at constant   2 /  1 ratios. The data are normalised with respect to
                                        the uniaxial compressive strength of the plates,   c = 66 MPa. The increase in peak
                                        strength over   c , associated with a given value of   2 , was greater for the solid platens
                                        than for the brush platens. This was attributed to the influence of end effects. When
                                        the brush platens were used, the maximum measured increase in peak strength over


              Figure 4.15  Biaxial compression
              test results for Wombeyan Marble (af-
              ter Brown, 1974).





























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