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ROCK STRENGTH AND DEFORMABILITY





              Figure 4.4  Influence of end restraint
              on stresses and displacements induced
              in a uniaxial compression test: (a)
              desired uniform deformation of the
              specimen; (b) deformation with com-
              plete radial restraint at the specimen–
              platen contact; (c) non-uniform nor-
              mal stress,   n and shear stress,   in-
              duced at the specimen end as a result
              of end restraint.

                                          Varying the standard conditions will influence the observed response of the spec-
                                        imen. Some of these effects will be discussed briefly in sections 4.3.3 to 4.3.7.
                                        More extensive discussions of these effects are given by Hawkes and Mellor (1970),
                                        Vutukuri et al. (1974) and Paterson (1978).

                                        4.3.3 End effects and the influence of height to diameter ratio
                                        The objective of the test arrangements should be to subject the specimen to uni-
                                        form boundary conditions with a uniform uniaxial stress and a uniform displacement
                                        field being produced throughout the specimen (Figure 4.4a). Due to friction between
                                        the specimen ends and the platens and differences between the elastic properties of
                                        rock and steel, the specimen will be restrained near its ends and prevented from de-
                                        forming uniformly. Figure 4.4b illustrates a case in which complete radial restraint
                                        occurs at the specimen ends. The result of such restraint is that shear stresses are
                                        set up at the specimen–platen contact (Figure 4.4c). This means that the axial stress
                                        is not a principal stress and that the stresses within the specimen are not always
                                        uniaxial.
                                          As a consequence of these end effects, the stress distribution varies throughout the
                                        specimen as a function of specimen geometry. As the height to diameter (H/D) ratio
                                        increases, a greater proportion of the sample volume is subjected to an approximately
                                        uniform state of uniaxial stress. It is for this essential reason that a H/D ratio of at least
                                        2.0 should be used in laboratory compression testing of rock. Figure 4.5 shows some
                                        experimental data which illustrate this effect. When 51 mm diameter specimens of
                                        Wombeyan Marble were loaded through 51 mm diameter steel platens, the measured
                                        uniaxial compressive strength increased as the H/D ratio was decreased and the shape
                                        of the post-peak stress–strain curve became flatter. When the tests were repeated with
                                        ‘brush’ platens (made from an assembly of 3.2 mm square high-tensile steel pins),
                                        lateral deformation of the specimens was not inhibited; similar stress–strain curves
                                        were obtained for H/D ratios in the range 0.5 to 3.0 However, ‘brush’ platens were
                                        found to be too difficult to prepare and maintain for their use in routine testing to be
                                        recommended.
                                          It is tempting to seek to eliminate end effects by treating the specimen–platen
                                        interface with a lubricant or by inserting a sheet of soft material between the specimen
                                        and the platen. Experience has shown that this can cause lateral tensile stresses to be
                                        applied to the specimen by extrusion of the inserts or by fluid pressures set up inside
                                        flaws on the specimen ends. For this reason, the ISRM Commission (1979) and other
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