Page 310 - Marine Structural Design
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286                                                     Part II Ultimate Strength


                 14.2  Finite Element Formulation
                 14.2.1  Equations of Motion
                 The  striking and  the  affected structure are considered one structural system connected by
                 spring elements.
                 The  equations  of  motion  for  the  structural  system  are  established  under  the  following
                 assumptions:
                    The striking ship is treated as a rigid body without volume, and all the deformations in the
                    ship are assumed to take place in a zone around an impact point.
                    The deformations in the  ship and the  local  indentation in the  affected member of  the
                    offshore  structure  are  simulated  by  using  nonlinear  spring  elements  in  which  only
                    compression forces  act.  The  force  deformation curves  for  those  spring  elements are
                    functions of the strain-rate.
                    The  deformation of  the  affected structure, except  for  the  local  indentation in  the  hit
                    member, is taken into account by using a model of the structure, which is composed of
                    three-dimensional beam-column elements.
                    The hydrodynamic forces acting on the ship are accounted for, by introducing an added
                    mass  concept. Morison's Equation is  applied  with  the purpose of  including the  fluid-
                    structure interaction to the affected structure's analysis.
                 When considering the dynamic equilibrium of the structural system, the equations of motion
                 may be written in an incremental form as:

                      [Ml{d4+[Cl{4+ [fGlb>= {@dl                                     (14.1)
                 where  {du}, {dzi} , and  (dii} are  the  increments of  nodal  displacements, velocities,  and
                 accelerations, respectively. [MI is a structural mass matrix, [q is a structural damping matrix,
                 and [K,] denotes the structural tangent stiffness matrix. The external load vector (dF, ] is due
                 to the drag force term in Morison's equation, which is evaluated using an approach described
                 by Bai and Pederson (1991). The added mass term in Morison's equation is included in the
                 structural mass matrix [MI.
                 The equation of motion, Eq. (14.1) is solved by using the Newmark-p method.
                 14.2.2  Load-Displacement Relationship of the Hit Member

                 In  this section, a derivation of a nonlinear spring element will be used  to model the local
                 indentation in the hiffaffected member. The spring element will be used for steel platforms and
                 the hiffaffected members are therefore assumed circular thin-walled tubes.
                 The linear elastic displacement of the load point for a pinch loaded tubular member can be
                 determined by:


                                                                                     (14.2)

                 where P is the force and  6, denotes the elastic displacement, E is Young's modulus, and T is
                 the  thickness of the  tube wall.  D  denotes the  outer diameter of the  tube  while L,  is  the
                 characteristic length of the contact area along the axial direction of the tube.
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