Page 106 - Numerical Analysis and Modelling in Geomechanics
P. 106

WAVE-SEABED-STRUCTURE INTERACTION 87
            approximation only considered the isotropic soil behaviour and a homogeneous
            seabed.  Recently,  the  general  finite  element  model  proposed  by  Jeng  et  al.
            (1998)  was  extended  to  the  wave-seabed-caisson  interaction  problem  by
            including the cross-anisotropic soil behaviour, and demonstrates the significant
            effects  of  cross-anisotropic  soil  behaviour  on  the  wave-induced  pore  pressure
            (Cha, 2000).


                                 Application of GFEM-WSSI
            In this section, we will demonstrate the application of the proposed general finite
            element  model  on  the  wave-seabed-caisson  interaction  problem.  The
            configuration of the problem is depicted in Figure 3.15. The boundary condition
            at the seabed surface, rubble mound foundation and caisson can be written as

                                                                        (3.23)

            and

                                                                        (3.24)


            for the part subjected to wave motion, and p=0 for the part subjected to no wave
            action.  It  is  noted  that  only  dynamic  wave  pressure  is  considered  in  the  study.
            The static wave pressure is not included here, since it remains a constant in the
            whole computing domain.
              To  give  a  basic  understanding  of  the  mechanism  of  the  wave-seabed
            interaction around a caisson, we examine several characteristics in this section.
            In  the  following  examples,  we  consider  the  rubble  mound  as  gravel,  and  the
            seabed to be coarse and fine sand. The wave crests are assumed to arrive fronting
            the  caisson.  The  detail  of  soil  properties,  wave  conditions,  caisson  and  rubble
            mound are given in Table 3.2.
              An example of a finite element mesh for the wave-seabed-caisson interaction
            is  given  in  Figure  3.16.  As  shown  in  the  figure,  a  finer  mesh  is  used  near  the
            rubble mound and caisson to enhance the accuracy near the interface of different
            materials.


                             Contours of pore pressure distribution
            Figure  3.17  illustrates  the  contour  of  the  wave-induced  pore  pressure  in  the
            vicinity of a caisson. In the figure, the result of the wave-induced pore pressure
            in  both  isotropic  seabed  (dashed  line)  and  cross-anisotropic  seabed  (solid  line)
            are included.
   101   102   103   104   105   106   107   108   109   110   111