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SHEAR BEHAVIOUR OF DISCONTINUITIES

                                        are applied successively. The triaxial cell is well suited to testing discontinuities in the
                                        presence of water. Tests may be either drained or undrained, preferably with a known
                                        level of joint water pressure being imposed and maintained throughout the test.
                                          It is assumed that slip on the discontinuity will occur according to the theory set
                                        out in section 4.6. Mohr circle plots are made of the total or effective stresses at slip
                                        at a number of values of   3 , and the points on these circles giving the stresses on the
                                        plane of the discontinuity are identified. The required shear strength envelope is then
                                        drawn through these points. This requires that a number of tests be carried out on
                                        similar discontinuities.
                                          In an attempt to overcome the need to obtain, prepare and set up several specimens
                                        containing similar discontinuities, a stage testing procedure is sometimes used. A
                                        specimen is tested at a low confining pressure as outlined above. When it appears that
                                        slip on the discontinuity has just been initiated (represented by a flattening of the axial
                                        load–axial displacement curve that must be continuously recorded throughout each
                                        test), loading is stopped, the cell pressure is increased to a new value, and loading
                                        is recommenced. By repeating this process several times, a number of points on the
                                        peak strength envelope of the discontinuity can be obtained from the one specimen.
                                        However, this approach exacerbates the major difficulty involved in using the triaxial
                                        test to determine discontinuity shear strengths, namely the progressive change in the
                                        geometry of the cell–specimen system that accompanies shear displacement on the
                                        discontinuity.
                                          The problem is illustrated by Figure 4.36. It is clear from Figure 4.36a that, if
                                        relative shear displacement of the two parts of the specimen is to occur, there must be
                                        lateral as well as axial relative translation. If, as is often the case, one spherical seat
                                        is used in the system, axial displacement causes the configuration to change to that
                                        of Figure 4.36b, which is clearly unsatisfactory. As shown in Figure 4.36c, the use
                                        of two spherical seats allows full contact to be maintained over the sliding surfaces,
                                        but the area of contact changes and frictional and lateral forces are introduced at the
                                        seats. Figure 4.36d illustrates the most satisfactory method of ensuring that the lateral
                                        componentoftranslationcanoccurfreelyandthatcontactofthediscontinuitysurfaces
                                        is maintained. Pairs of hardened steel discs are inserted between the platens and either
                                        end of the specimen. No spherical seats are used. The surfaces forming the interfaces
                                        between the discs are polished and lubricated with a molybdenum disulphide grease.


              Figure 4.36  Discontinuity shear
              testing in a triaxial cell (after Jaeger
              and Rosengren, 1969).

















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