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        2 and the related  functions A, AR and A’  given by  Eqn. (3e) similarly need to be evaluated only once
        per Froude number.


        6  NUMERICAL RESULTS AND CONCLUSIONS
        The first design problem considered here is to determine the optimal hull arrangement for the original
        wave cancellation multihull  ship for the purpose of minimizing the wave drag of the ship. Figure  I
        depicts the experimental values of the residuary drag coefficient CR given in Wilson et. al. (1993) and
        the corresponding predictions of the wave-drag coefficient CW given by the present method for the four
        hull  arrangements.  These  hull  arrangements  correspond  to  a=-0.128,  -0.205,  -0.256,  -0.385  and
        b=O.136  for all four cases.  In this figure, the C, and the CW are nondimensionalized in terms of the
        surface area of the wetted hull, in the usual fashion. In the rest of the figures, the CW is defined by  Eq.
         la.  It  can  be  seen  that  the  CW predicted  by  the  present  method  is  in  fair  agreement  with  the
        experimental  CR.  In  particular, the  variation  of  CR with  respect  to the  Froude number  F is well
        captured by the theory.  The present method may therefore be used for the purpose of determining the
        optimal arrangements of the outer hulls.
             2.5
            ’
             2.0
            2  1.5
            8 1.0
            r
             0.5
                                                0.5
             0.0
               0.2   0.25   0.3   0.35   0.4   0.45   0.5   0.55   0.0 4
                       Fmude number (a=-0.128)   0.2   0.25   0.3   0.35   0.4   0.45   0.5   0.55
             2.5 7                              2.5  I




                                                               +* +
                                             ’
                                                0.5
             0.0 J                              0.0 J                          I
               0.2   0.25   0.3   0.35   0.4   0.45   0.5   0.55   0.2   0.25   0.3   0.35   0.4   0.45   0.5   0.55
                       Froude number (ai0.256)           Froude number (a-4.385)
                       Figure 1 : Calculated wave drag and experimental residuary drag
        The  hull  arrangements within  the range  of -0.75Ia10.75  and  0.11b10.3 with  Aa=O.O25and
         Ab = 0.01 are studied for 38 values of  Froude numbers  with0.2147 = F, IF, IF,, = 0.5426  .  For
        a=0.75, the stems of the outer hulls are aligned with the bow of the main center hull; similarly, the
        bows of the outer hulls are aligned with the stem of the center hull if r-0.75.   This study represents
        61  x 21 = 1281  hull  arrangements  and  61 x 21 x 38 = 48678  evaluations  of  CW. The optimal  hull
        arrangement for the speed range F, I F, 1 F3* approximately corresponds to n=0.55,  b=O. 11. Fig.  2
        depicts the  variations,  with  respect  to  the  Froude  number  F,  of  the  “no-interference  wave-drag
        coefficient”, C& + 2Ci and of the wave-drag coefficients CF and   associated with the best and
        worst hull arrangements found within the region.  Fig. 2 also shows the wave drag-coefficient curve
        CLp’”’(F) for  the  optimal  hull  arrangement  (a=0.55,  b=0.11).  The  wave-drag  coefficient curve
         C~!””’(F) corresponds to a hull arrangement that remains fixed over the entire speed range, while the
        curves CF(F)and Cy‘(F)are associated with hull  arrangements that vary with speed. The large
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