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ENRICO PRIOLO 275
            realistic.  This  supports  the  need  for  methods  that  accurately  model  realistic
            geologic structures.
              In addition to the earthquake data, environment microtremors were recorded at
            the  same  site  of  the  Catania  station  (Priolo  et  al.,  2001).  The  aim  of  this  data
            acquisition was to improve our prediction of the seismic ground motion locally.
            To this end, Nakamura’s approach was followed which, as proven, provides the
            main  features  of  the  dynamic  ground  response  through  the  calculation  of  the
            spectral ratio between the horizontal and vertical components (i.e., H/V ratio) of
            background  microtremors  (Nakamura,  1989).  In  Figure  9.8,  the  H/V  spectral
            ratios  obtained  from  (i)  the  environment  seismic  noise,  (ii)  the  seismograms
            recorded  by  the  accelerometric  station  during  the  December  13,  1990  M=5.8
            Eastern  Sicily  earthquake,  and  (iii)  the  seismograms  computed  by  the  2-D
            spectral  element  method  for  the  same  earthquake,  are  compared.  The  ratios
            obtained from the seismic noise measurements well detect the fundamental mode
            of vibration at about 1.5 Hz, but they miss the peak at the higher frequency of 4–
            5 Hz. This fact may either confirm that Nakamura’s method is only reliable for
            identifying the fundamental mode of vibration, or that the peak at 4–5 Hz in the
            earthquake  records  is  a  feature  of  the  earthquake  source.  The  H/V  ratios
            determined from the synthetic seismograms are generally noisier, but they well
            reproduce the behaviour of the spectral ratios determined from the full ENEA-
            ENEL  recordings  for  frequencies  larger  than  1  Hz.  The  origin  of  the  two
            additional peaks at 0.4–0.8 Hz is currently under investigation.


                    Influence of a massive structure on the free surface ground
                                         motion
            In this study, the 2-D SPEM was used to investigate how seismic ground motion
            is affected by the presence of a massive structure. The analysis of soil-structure
            interaction in seismic hazard studies is usually concerned with its influence on
            the response of and damage to the structure itself. One should expect, however,
            that  large  massive  loads  perturb  the  free-field  ground  motion  in  their
            surroundings.  Recent  numerical  investigations  indicate,  in  fact,  that  long-range
            soil-structure interaction for large buildings may have had a role in determining
            the abnormal amount of damage on the Mexico City clay basin during the 1985
            Michoacan  earthquake  (Wirgin  and  Bard,  1996).  The  aim  of  this  work  was  to
            investigate how much, and over what distance range, surface loads alter the free-
            field ground motion.
              Two-dimensional models were considered where a linear elastic structure with
            a  quadrangular  cross-section,  resting  on  an  elastic  homogeneous  half-space,  is
            impinged upon by the surface waves generated by a vertical and impulsive point
            source  located  on  the  ground  surface  at  some  distance  (Figure  9.9).  The
            scattering  of  Rayleigh  waves  and  the  response  of  the  structure  are  extensively
            analysed in a parametric way: by varying the size, mechanical parameters, and
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