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F.BASILE 307
            have been taken as 0.0 and 0.99 for the axial response of the shaft and the base,
            respectively, and 0.9 for the lateral response.
              For the axial response, the profile of soil modulus has been derived from the
            correlation  E =400C u  for  the  linear  analyses  and  from  E =1500C u  for  the
                                                              s
                       s
            nonlinear analysis. For the lateral response, the profile of soil modulus has been
            assumed  to  increase  linearly  with  depth  from  a  value  of  zero  at  the  top  of  the
            London Clay (conservatively) at a rate of 4.14 MPa/m for the linear analyses and
            6.15 MPa/m for the non-linear analysis. The soil Poisson’s ratio has been taken as
            0.5.
              The applied vertical loads (V) result from the combined effect of live and dead
            loads, whereas the horizontal loads (H) and moments (M) are generated by the
            high-speed  trains  braking  and  accelerating.  For  the  load  case  presented  herein,
            the loads acting on the cap have been estimated as V=14,200 kN, H=470 kN and
            M =3200 kNm.
              This  problem  has  been  analysed  using  the  computer  programs  MPILE,
            DEFPIG  and  PGROUPN  (both  the  linear  and  non-linear  versions).  Table  10.7
            summarises the main results obtained from the analyses. In the linear range, there
            is a reasonably good agreement between the group deformations and axial load
            distribution predicted by the different codes. However, it is important to note the
            significant differences between the predictions of the pile head lateral loads and
            bending  moments.  As  discussed  previously,  due  to  the  interaction  between  the
            axial and lateral responses of the piles, higher loads are expected to occur for the
            piles in the leading row than for the piles in the trailing row of the group. While
            this  load-deformation  coupling  effect  is  modelled  by  the  PGROUPN  analysis,
            MPILE  and  DEFPIG  disregard  the  interaction  between  the  axial  and  lateral
            responses and therefore predict the same lateral loads and bending moments for
            both  the  leading  and  trailing  rows  of  the  group.  This  results  in  a  significant
            underestimate of the maximum values of lateral load and bending moment and
            hence may lead to an unsafe design of the piles.
              If  the  effects  of  soil  non-linearity  are  accounted  for  by  means  of  the
            PGROUPN analysis, two main features of behaviour are observed:

             1 A prediction of lower (and more realistic) group deformations.
             2 A decrease of predicted loads on the most heavily loaded row of piles (i.e.
               the  leading  row)  and  hence  a  more  uniform  load  distribution  between  the
               piles.

            It  should  be  emphasised  that  in  this  case,  due  to  the  low  load  level,  the
            differences  between  the  linear  and  non-linear  PGROUPN  results  are  mainly  a
            consequence of the higher value of soil modulus adopted in the non-linear analysis
            (i.e. an initial value), rather than the effect of soil non-linearity.
              This  observation  confirms  the  view  already  expressed  by  other  authors
            (Randolph, 1994; Mandolini and Viggiani, 1997): at low load levels (and hence
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