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STABILITY OF UNSATURATED SOIL SLOPES 105
                                       Introduction
            Slope  instability  in  unsaturated  residual  soils  and  loose  fills  is  attracting
            increasing  attention  in  many  countries  around  the  world  such  as  Brazil,  Italy,
            South Africa, Japan and in the Far East. The causes of landslides in these slopes
            are  attributed  to  a  number  of  factors.  Rain-  induced  failures  are  the  most
            common  ones  around  the  world  (Brand  [1],  Fukuoka  [2],  Premchitt  et  al.  [3],
            Wolle and Hachich [4], Fourie [5], Lim et al. [6]). For instance, the annual number
            of landslides caused by rainfall in Japan is in excess of 10,000 and could be as
            high as 100,000 (Fukuoka [2]). Pore water pressure (u ) in the shallow depth of
                                                        w
            these residual soil and loose fill slopes is generally negative with respect to the
            atmospheric pressure (u ). The presence and the magnitude of matrix suction (u a
                               a
            −u ) have been found to be absolutely crucial to the stability of unsaturated soil
              w
            slopes (Fredlund and Rahardjo [7]).
              Infiltration of rain-water or ingress of a wetting front (Lumb [8]) leads to the
            development of a perched water table, rising in the main groundwater level and
            washing  out  (soil  erosion  due  to  concentrated  water  flow),  resulting  in  an
            increase  in  pore  water  pressure  or  a  reduction  in  soil  matrix  suction.  This,  in
            turn, results in a decrease in shear strength on the potential failure surface to a point
            where  equilibrium  can  no  longer  be  sustained  in  the  slope  and  then  failures
            occur.  Slope  failure  mechanisms  found  in  these  landslides  generally  consist  of
            both shallow and deep-seated slips, depending mainly on the thickness of these
            residual  soils  and  loose  fills.  Deep-seated  static  soil  liquefaction  occurred  in
            some loose fill slopes under intense rainfall (Brand [1]).
              The  physical  processes  of  infiltration  of  rainwater  into  the  ground  and  its
            seepage  through  the  soil  stratum  have  been  studied  by  hydrogeologists,  soil
            scientists and geotechnical engineers. Equations and numerical models have been
            derived and developed for use (Lumb [9], Leach and Herbert [10], Anderson and
            Pope [11], Lam et al. [12], Pradel and Raad [13]). However, several important
            limitations  on  the  use  of  these  equations  and  models  are  discussed  in  the
            following paragraphs.
              Lumb [9] derived an expression for the advance of the “wetting front”, with
            the assumption that diffusion is negligible at the end of an intensive rainfall:

                                                                         (4.1)


            where n is porosity, k  is saturated water permeability, t is time, and S  and S  are
                                                                    o
                             s
                                                                         f
            the initial and final degree of saturation respectively. The soil will only be fully
            saturated  near  the  surface,  but  will  be  wet  (degree  of  saturation,  S=0.8  to  0.9)
            down to a depth h (see Figure 4.1). The method was frequently used in the 1970s
            and 1980s to design the water table for slopes by superimposition of the depth of
            wetting  front  onto  the  main  groundwater  table  at  the  end  of  a  wet  season.
            However,  this  equation  does  not  take  account  of  sloping  ground  conditions,
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