Page 247 - Practical Design Ships and Floating Structures
P. 247

222

             the  pressure distribution method  is applied to the  zero draft  assumption. The effectiveness of the
             shallow draft assumption is compared mainly on the elastic deformation and the steady wave  drift
             force. The steady wave drift force is calculated by the momentum theory.
             Several numerical procedures have been  proposed  and  developed  on  hydroelastic responses of  a
             pontoon type floating structure with  a finite draft. Those procedures may take much  computational
             time in the relatively high frequency range. Then zero draft assumption has been introduced in order to
             save computational time. (See, Maeda et al. (1996), Kashiwagi (1998), Ohmatsu (1998) and Kim et al.
             (1998) ) The zero draft assumption has been partially verified by model tank tests, while the model
             tests may have some uncertainty and may not correspond to the full scale wave frequency range. The
             application area of the zero draft assumption is still not clear yet. Kim et al. (2000) verified about this
             problem, however, there are a few examinations on the zero draft assumption related to an analysis of a
             very large floating structure. In addition, few researchers verify the effectiveness of the assumption on
             wave drifting forces.
             Figure 1. In addition, velocity potentials @,  pressures P ex
             2  THEORY

             It  is  assumed that  the  fluid  is  ideal  fluid.  The  hydrodynamic  forces are calculated by  the linear
             potential  theory.  However  the  second  order  wave
             excitations  are  considered  by  the  momentum  theory
             using  the  linear  velocity  potentials.  The  coordinate
             system  is  the  right  hand  Cartesian and  the  z-axis  is
             positive upward. The coordiiate system is illustrated in

             and  vertical  displacement  7  of  a  free  surface or  the
             structure are defined. Two  methods are applied  to the
             hydroelasticity analysis for the pontoon type very large
             floating structure. One is the three-dimensional  singular              I
             distribution method for the analysis of finite draft bodies.
             Another one is the pressure distribution method for the
             analysis of zero-draft bodies.                   Figure 1: Coordinate system
             2.1 Theoryfor afinite drap body

             The 3-D singularity distribution method (3-D SDM) is used in the calculation in which the effect of the
             body's  draft is  considered. It  is very  general  method  for an  analysis of  hydrodynamic  forces on
             offshore structure with arbitrary shapes. The authors modified our program code to calculate the elastic
             floating structure. The method for an analysis of the elastic motions is same as Nagata et al. (1997).
             A  theory to  analyze the wave  drifting force which  is called  as the  second-order wave excitation
             generally is explained here. The momentum theory (far field theory) is applied.
             The velocity potential 4 in the fluid field at an arbitrary point is expressed as follows:
                                    -
                                       a
                                 ah
                                             Y, X; X' ,v', z'b ,
                      &(.I  Y, 2) = - Jl(x h ~)G(x,                                 (1)
                               SH
             where G is Green's  function. When a distance between the source and observation points becomes
                               '
             infinity, Green's functions (in this study) are:
                                         _.
                      ti=-- i
                                    cosh k(z + h)cosh k(z'+h)
                           h+-
                              k2 - K2
                         i
                      G = - K exp k(z + z')                                         (3)
                         2
   242   243   244   245   246   247   248   249   250   251   252