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Chapter 3
                A general finite element model for wave-

                         seabed-structure interaction
                                        D.S.Jeng










                                       Introduction
            The mechanism of wave-seabed-structure interaction is an important concern for
            designing  offshore  facilities,  such  as  pipelines,  anchors,  marine  platforms  and
            breakwaters.  In  the  field,  concrete  armour  blocks  at  the  toes  of  many  marine
            structures have been found to subside into the seabed; wave-induced liquefaction
            has  been  identified  as  the  reason  for  this  problem  (Silvester  and  Hsu,  1989).
            Moreover, it has been reported that some such structures have possibly failed due
            to seabed instability (Lundgren et al., 1989; Silvester and Hsu, 1989).
              Waves propagating in shallow water create a significant dynamic pressure on
            the sea floor. This pressure field induces a stress field and associated pore water
            pressure  fluctuations  within  the  seabed.  With  excess  pore-pressure  and
            diminishing vertical effective stresses, part of the seabed may become unstable
            or even liquefied. This causes a quicksand effect in which external loads cannot
            be supported. Furthermore, when liquefaction occurs, the soil particles are likely
            to be carried away as a fluid by any prevailing bottom current or by mass transport
            due to the wave action.
              Two  mechanisms  of  wave-induced  soil  response  have  been  observed  in
            laboratory experiments and field measurements (Zen and Yamazaki, 1990; Nago
            et al., 1993). The first is caused by the progressive development of excess pore
            pressure  that  occurs  after  a  certain  number  of  wave  cycles.  This  type  of  soil
            response is similar to that induced by an earthquake. The second is generated by
            the  oscillatory  nature  of  the  excess  pore  pressure,  which  appears  periodically
            many  times  during  a  storm  sequence.  In  most  cases,  the  wave-induced  soil
            response is oscillatory in nature except for some special cases of non-cohesive
            sediments with loose to medium density (Seed and Rahman, 1978). In this study,
            we will focus on the wave-induced oscillatory soil response.
              Many variables influence the wave-induced soil response in a porous seabed;
            anisotropy in soil behaviour is an important issue that must be considered in the
            wave-seabed interaction problem. In the field, most marine sediments display a
            certain  degree  of  anisotropy,  with  different  elastic  properties  in  different
            directions,  owing  to  the  manner  of  their  deposition,  particle  shape  and  stress
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