Page 202 - Numerical Analysis and Modelling in Geomechanics
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BACK ANALYSIS OF GEOTECHNICAL PROBLEMS 183


























            Figure 6.6 Elastic moduli of the sand layers obtained by the in situ dilatometer tests and
            by the elastic back analyses of the displacement measurements.
              The τ–δ relationship can be schematically subdivided into three main parts. In
            the first, the average shear stress increases until its peak value is reached. This
            corresponds,  in  the  average  normal  stress-shear  stress  (σ–τ)  plane,  to  the  so-
            called peak failure envelope characterised by peak cohesion and friction angle.
            Relatively small additional increments of displacements produce a reduction of
            the  shear  resistance,  caused  by  an  almost  complete  loss  of  the  peak  cohesion.
            This  leads  to  a  second  (fully  softened)  failure  condition.  Finally,  further  large
            increments of the horizontal displacement bring the friction angle to its residual
            value, which represents the only non-vanishing parameter of the residual failure
            envelope.  During  this  process  also  a  reduction  of  the  instantaneous  elastic
            modulus could take place.
              In  order  to  account  for  this  material  behaviour  in  a  finite  element  stress
            analysis  it  is  necessary  to  define  a  law  governing  the  reduction  of  cohesion,
            friction angle and elastic moduli from peak to residual values. This was based on
            the relationship graphically depicted in Figure 6.9.
              It  is  assumed  that  shear  strength  and  stiffness  parameters  are  functions  of  a
            measure of the (irreversible) plastic deformation, represented by the square root
            of the second invariant J  of the deviatoric plastic strains.
                               2
              The friction angle keeps its peak value until J  reaches a “peak” limit J . Then
                                                                      2p
                                                  2
            a reduction occurs until a second limit J  is attained, which corresponds to the
                                             2r
            residual friction angle. Analogous relationships, with different limits on J , are
                                                                        2
            adopted also for the remaining mechanical parameters.
              In order to account for the effects of dilatancy, the plastic flow rule is related
            to  the  variation  of  the  friction  angle.  In  particular,  an  associated  flow  rule  is
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