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STABILITY OF UNSATURATED SOIL SLOPES 111


                                                                         (4.9)


            By  comparing  equations  (4.4)  and  (4.9),  it  can  be  deduced  that  S =γ m .  For
                                                                        w
                                                                   s
                                                                     w
            water flow in saturated soils, u =u , then equation (4.6) becomes:
                                    a
                                       w
                                                                        (4.10)
            where m  is equivalent to the coefficient of volumetric change m  which is common
                                                              v
                  a
            to saturated soil mechanics.
                         Theory of shear strength for unsaturated soils

            The  mechanical  behaviour  of  soils  is  governed  by  stress  state  variables  which
            control  the  equilibrium  of  the  soil  structure.  Physically  meaningful  stress  state
            variables  must  be  expressed  in  terms  of  measurable  quantities  such  as  the
            total stress σ, the pore water pressure u , and the pore air pressure, u . Matyas
                                                                     a
                                            w
            and  Radhakrishna  [16]  introduced  the  two  stress  state  parameters,  (σ–u )  and
                                                                        a
            (u –  u ),  to  describe  the  volumetric  behaviour  of  unsaturated  soil.  These  two
                 w
             a
            stress state parameters were subsequently adopted by Fredlund and Morgenstern [17
            ]  to  conduct  stress  analysis  of  unsaturated  soils  on  the  basis  of  multi-phase
            continuum mechanics.
              For  soil  located  above  the  main  water-table,  the  pore  water  pressure  is
            negative  with  respect  to  the  atmospheric  pressure.  This  negative  pore  water
            pressure is commonly referred to as the matrix suction of soil. To account for the
            influence of this negative pore water pressure on soil shear strength and hence
            the factor of safety, Fredlund et al. [18] developed a modified form of the Mohr-
            Coulomb failure criterion for unsaturated soils, as follows:
                                                                        (4.11)


            where  σ n  is  normal  stress  and  ф b  is  an  angle  defining  the  increase  in  shear
            strength  for  an  increase  in  matrix  suction.  Based  on  some  recent  triaxial  test
            results  on  completely  decomposed  granite  (CDG)  with  suction  measurements
            (Gan and Fredlund [19]), effective cohesion c'=10kPa, angle of friction ф'=38°
                 b
            and  ф =15°  were  adopted  in  the  limit  equilibrium  analyses.  It  should  be  noted
            that shear strength varies with matrix suction in a non-linear fashion (Gan et al. [
                            b
            20]). The value of ф  decreases with increasing suction. However, for simplicity
            and  the  small  suction  range  considered  in  the  stability  analyses,  a  constant  ф b
            value was assumed.
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