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ROOF STABILITY ANALYSIS FOR A TETRAHEDRAL BLOCK

                                        where
                                          M = [(k s /k n ) cos 2  cos i + sin(  − i) sin  ] sin(  −  )/D cos i
                                          D = cos   cos   k s /k n + sin   sin(  − i)/ cos i
                                                 2
                                          W =   R C w
                                                  2
                                          C w = cos 
(tan 
 + cot  ) −  /2 +
                                        The Factor of Safety against wedge failure is given by
                                                                     (S + P 0 )  S
                                                              FoS =         =    + q                  (9.33)
                                                                       W       W
                                        In a further development of this analysis, Nomikos et al. (2002) considered a sym-
                                        metric roof wedge in an inclined, deviatoric stress field. Expressions more complex
                                        than those above define the Factor of Safety against roof failure, and a reasonable
                                        correspondence was shown between the analytical solution and some solutions using
                                        UDEC.


                                        9.4 Roof stability analysis for a tetrahedral block

                                        A comprehensive relaxation analysis for a non-regular tetrahedral wedge in the crown
                                        ofanexcavationpresents someconceptual difficulties. These arisefromtheextranum-
                                        ber of degrees of freedom to be accommodated in the analysis. For example, on any
                                        face of the tetrahedron it is necessary to consider two components of mutually orthog-
                                        onal shear displacement as well as a normal displacement component. Maintenance
                                        of statical determinacy during the relaxation process would require that the wedge
                                        be almost isotropically deformable internally. For this reason, a thorough analysis of
                                        the stability of a tetrahedral wedge in the crown is not handled conveniently by the
                                        relaxation method presented earlier. A computational method which takes explicit
                                        account of the deformation properties of the rock mass, and particular joints and joint
                                        systems, presents the most opportune basis for a mechanically appropriate analysis.
                                          In some circumstances, it may be necessary to assess the stability of a roof wedge
                                        in the absence of adequate computational tools. In this case, it is possible to make
                                        a first estimate of wedge stability from an elastic analysis of the problem and the
                                        frictional properties of the joints. Suppose the orientation of the dip vector OA of a
                                        joint surface, which is also a face of a tetrahedral wedge, is defined by the dip angle  ,
                                        and dip direction  , measured relative to the global (x, y, z) reference axes, illustrated
                                        in Figure 9.17a. The direction cosines of the outward normal to the plane are given
                                        by

                                                     n = (n x , n y , n z ) = (sin   cos  , sin   sin  , − cos  )

                                        The normal component of traction at any point on the joint surface can be estimated
                                        from the elastic stress components and the direction cosines by substitution in the
                                        equation
                                                                   2
                                                            2
                                                     2
                                                t n = n   xx + n   yy + n   zz + 2(n x n y   xy + n y n z   yz + n z n x   zx )
                                                     x      y      z
                                        If the normal traction t n is determined at a sufficient number of points on the joint
                                        surface, its average value and the area of the surface can be used to estimate the total
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