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CLOSED-FORM SOLUTIONS FOR SIMPLE EXCAVATION SHAPES

                                        plane can be readily established from an orthogonal Cartesian system in the   plane
                                        through the transformation

                                                         z = x + iy = c cosh   = c cosh(  + i )

                                        so that

                                                          x = c cosh   cos  ,  y = c sinh   sin       (6.17)

                                        Equations 6.17 are also the parametric equations for an ellipse of major and minor axes
                                        c cosh  , c sinh  . The analysis of the stress distribution around the opening proceeds
                                        by expressing boundary conditions, source analytic functions and stress components
                                        in terms of the elliptic co-ordinates. The detail of the method then matches that
                                        described for a circular opening.
                                          The conformal mapping method involves finding a transformation which will map
                                        a chosen geometric shape in the z plane into a circle of unit radius in the   plane. The
                                        problem boundary conditions are simultaneously transformed to an appropriate form
                                        for the   plane. The problem is solved in the   plane and the resulting expressions
                                        for stress and displacement distributions then inverted to obtain those for the real
                                        problem in the z plane. Problem geometries which have been analysed with this
                                        method include a square with rounded corners, an equilateral triangle and a circular
                                        hole with a concentric annular inclusion.



                                        6.3 Closed-form solutions for simple excavation shapes

                                        Theprecedingdiscussionhasestablishedtheanalyticalbasisfordeterminingthestress
                                        and displacement distributions around openings with two-dimensional geometry. In
                                        rock mechanics practice, there is no need for an engineer to undertake the analysis
                                        for particular problem configurations. It has been noted already that comprehensive
                                        collections of solutions exist for the analytically tractable problems. The collection
                                        by Poulos and Davis (1974) is the most thorough. The practical requirement is to be
                                        able to verify any published solution which is to be applied to a design problem. This
                                        is achieved by systematic checking to determine if the solution satisfies the governing
                                        equations and the specified far-field and boundary conditions. The verification tests to
                                        be undertaken therefore match the sets of conditions employed in the development of
                                        the solution to a problem, as defined in section 6.1, i.e. imposed boundary conditions,
                                        differential equations of equilibrium, strain compatibility equations and constitutive
                                        equations. The method of verification can be best demonstrated by the following
                                        example which considers particular features of the stress distribution around a circular
                                        opening.

                                        6.3.1 Circular excavation
                                        Figure6.3ashowsthecircularcrosssectionofalongexcavationinamediumsubjectto
                                        biaxial stress, defined by p yy = p, and p xx = Kp. The stress distribution around the
                                        opening may be readily obtained from equations 6.6, by superimposing the induced
                                        stresses associated with each of the field stresses p and Kp. The complete solutions
                                        for stress and displacement distributions around the circular opening, originally due
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