Page 190 - Practical Ship Design
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156                                                             Chapter 6


                        6.2 RESISTANCE AND SHIP MODEL CORRELATION

             6.2. I  The classical treatment of  resistance

             Resistance is the force that the ship overcomes as it moves through the water. The
             classical treatment of resistance is outlined in this section and is followed in the
             next section by an outline of the present day treatment of resistance.
               In the classical  treatment of resistance, this is divided  into two components,
             which are governed by different laws, so that they can be separately extrapolated
             from model to full-scale ship size:
               (i)   the skin frictional resistance, which is governed by the Reynolds’ number,
                    and
               (ii)  the  residuary  resistance,  taken  mainly  to  be  wavemaking,  which  is
                    governed by the Froude number.
               In the following paragraphs use will be made of the resistance coefficient  C.
             This is related to the wetted surface S, the speed V, and the mass density p by the
             following equation:

               R = 1/2. C. p. S. V2                                            (6.1)
             The coefficient C is given two types of subscripts. The first of these refers to the
             subdivision of resistance with t = total; f  = frictional; r = residuary; w = wave-
             making. The second subscript distinguishes between model resistance  = m; and
             ship resistance = s.
                In the classical treatment, the skin frictional resistance coefficient of the model
             is calculated based on the coefficient of friction applicable to a plank (flat plane) of
             model length and having the same wetted area as the model. This is then deducted
             from the total model resistance coefficient to establish the model residuary resist-
             ance coefficient.



             At a constant Froude number the residuary resistance coefficient remains the same
             for the ship as it is for the model, so there is no need for a suffix to indicate “model”
             or “ship” in this case.
                The  ship  frictional  resistance  coefficient  C,,  is  again  calculated  using  the
             coefficient of friction applicable to a plank, this time one of the same wetted area
             and the  same length as the  ship. This is then  added to  C, to arrive at the total
             resistance coefficient Ct, of the ship.

                ct, = Cfs + cr                                                 (6.3)
             It should be noted that the use of friction coefficients based on a plank for both model
             and ship implies that the skin friction is independent of the shape of the lines.
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