Page 203 - Introduction to Naval Architecture
P. 203

RESISTANCE                         189

        relatively small, say 10 to 15 per cent of the hull resistance, and errors
        in their assessment are not likely to be critical.

        Wind resistance

        In conditions of no natural wind the air resistance is likely to be small
        in relation to the water resistance. When a wind is blowing the fore and
        aft resistance force will depend upon its direction and speed. If coming
        from directly ahead the relative velocity will be the sum of wind and
        ship speed. The resistance force will be proportional to the square of
                                                                        6
        this relative velocity. Work at the National Physical Laboratory
        introduced the concept of an ahead resistance coefficient (ARC) defined
        by:





        where V R is the relative velocity and A T is the transverse cross section
        area.
          For a tanker, the ARC values ranged from 0.7 in the light condition
        to 0.85 in the loaded condition and were sensibly steady for winds from
        ahead and up to 50° off the bow. For winds astern and up to 40° off the
        stern the values were -0.6 to -0.7. Between 50° off the bow and 40° off
        the stern the ARC values varied approximately linearly. Two cargo ships
        showed similar trends but the ARC values were about 0.1 less. The
        figures allowed for the wind's velocity gradient with height. Because of
        this ARC values for small ships would be relatively greater and if the
        velocity was only due to ship speed they would also be greater. Data is
                    7
        also available  for wind forces on moored ships.


        CALCULATION OF RESISTANCE

        Having discussed the general nature of the resistance forces a ship
        experiences and the various formulations for frictional resistance it is
        necessary to apply this knowledge to derive the resistance of a ship. The
        model, or data obtained from model experiments, is still the principal
        method used. The principle followed is that stated by Froude. That is,
        the ship resistance can be obtained from that of the model by:

           (1) measuring the total model resistance by running it at the
              corresponding Froude number;
           (2) calculating the frictional resistance of the model and subtracting
              this from the total leaving the residuary resistance;
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