Page 192 - Numerical Analysis and Modelling in Geomechanics
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BACK ANALYSIS OF GEOTECHNICAL PROBLEMS 173
            errors  on  the  computed  mechanical  parameters.  Among  them,  two  will  be
            mentioned here.
              A  first  approach,  is  based  on  the  so-called  Monte  Carlo,  or  simulation,
            technique. Following this method, the influence of the measurement error, and of
            the  number  of  input  data,  is  evaluated  through  a  series  of  numerical  tests  [9].
            Each of them consists of a set of back analyses based on suitable generated input
            measurements (e.g. displacements).
              The  input  data  are  obtained  by  adding  to  the  “exact”  measurements  a
            disturbance that represents the experimental “errors”. Independent generators of
            random numbers, with chosen probability distributions and zero mean value, are
            used to work out these errors. The number of generators coincides with that of
            the  input  measurements.  Their  probability  distributions  depend  on  the
            characteristics of the measuring devices and of the measured quantities.
              The “exact” displacements either can be evaluated on the basis of actual field
            measurements or could be simulated through a preliminary stress analysis of the
            problem  at  hand,  in  which  reference  values  of  the  material  parameters  are
            introduced [9].
              This  procedure  permits  establishing  a  probabilistic  correlation  between  the
            resolution  of  the  measuring  device,  the  number  of  measurements  and  the
            accuracy of the computed parameters characterising the soil/rock mass.
              The  simulation  technique  offers  the  advantage  of  an  extremely  simple
            implementation, but requires a computational effort rapidly increasing with the
            number of free variables of the numerical model and with the number of unknown
            parameters.
              This  drawback  could  be  limited  by  making  recourse  to  probabilistic
            approaches  [10–13].  Among  them,  the  so-called  Bayesian  approach  will
            discussed here, which was adopted in [14] and [15] for a rock mechanics problem
            and  for  the  back  analysis  of  the  field  measurements  performed  during  the
            construction of a railroad embankment.
              A typical feature of the Bayes approach is that “a priori” information on the
            unknown  parameters  can  be  introduced  in  the  back  analysis,  together  with  the
            data deriving from in situ measurements. In most cases, the a priori information
            consists  of  an  estimation  of  the  unknown  parameters  based  on  the  engineer’s
            judgement  or  on  available  general  information.  This  leads  to  a  numerical
            calibration  procedure  that  combines  the  knowledge  deriving  from  previous,
            similar  problems  with  the  results  of  the  in  situ  investigation.  For  the  sake  of
            briefness, only the bases of the approach are outlined here.
              Consider  the  experimental  measurements,  collected  in  vector  u*,  and  the
            corresponding  errors,  seen  as  random  variables,  grouped  in  vector  ≥ u.  Let  us
            assume  that  the  expected  average  value  of  the  error  vector,  expressed  by  the
            “expectation” operator E , vanishes,
                                x
                                                                        (6.12)
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