Page 51 - Marine Structural Design
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28                                                Part IStructural Design Principles


                 speed corrections and the lack of viscous effects. All these methods assume the ship to be rigid
                 beam.  Bishop and  Price  (1979) developed  a  flexible beam  strip theory that  accounts for
                 bending and shear stiffness of the hull when  solving for compatibility between strips. This
                 kind of theory can estimate the distortional higher frequency responses of a hull to slamming
                 and whipping excitation. However, it is still linear analysis and extreme response is not well
                 modeled.
                 2.3.2  Wave-Induced Forces
                 Jensen and Pedersen (1979) proposed a second order strip theory for hydro-elastic analysis in
                 fiequency-domain. Their theory is based on a perturbational expression of the hydrodynamic
                 and the hydrostatic coefficients around the still water line and includes the incident pressure
                 field from second order Stokes’ waves. The equation used to evaluate the forces acting on a
                 ship in such an analysis is similar to:
                      F(X,t)=  FH(X>t)+FB(X,t)                                       (2.23)
                 The procedure for actually working out the above equation is rather complicated due to the
                 non-linear nature of some of the parameters. The following explanation is only to give a basic
                 understanding of the parameters present in Eq. (2.23).
                 The right hand side of Eq. (2.23) consists of two parts. The second part is the buoyancy force
                 known as the Froude-Krylov buoyancy force:

                                                                                     (2.24)

                 where,
                       B     = Breadth of the ship
                       Y     = Distance along an  axis starting from  the bottom of the  hull  and moving
                             vertically upwards
                       v     = Instantaneous vertical displacement of the hull

                       rl    = Distance from the calm water surface to the local elevation of the ocean wave
                       X     = Distance along an axis starting fiom the aft of the ship and travelling forward
                             along a horizontal axis
                       t     = Time
                       T     = Still-water draught
                       P     = Pressure given by Bernoulli’s equation:

                                                                                   (2.25)

                 where,
                       p     = Fluid density
                       4     = Velocity potential which is made up of first- and second- order terms. The
                             derivation of 4 is well described by Jensen and Pedersen (1979)
                       g     = Acceleration due to gravity
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