Page 107 - Theory and Design of Air Cushion Craft
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Air  cushion wave-making drag  91






                                 .  a'/a=0.90
                              2.0



                              1.5




                              1.0

                                              1
                                              1  2a'  1
                                              1       1
                              0.5









          Fig.  3.6  Cushion wave-making drag  ratio  as a function  of equivalent  Froude Number. [22]
            In  addition,  Tatinclaux calculated two further  pressure distribution combinations,
          i.e.  linear  distribution  at  bow/stern  and  sudden  change  at  two  sides  (similar  to  an
          SES),  as  well  as distribution at  two  sides  and  sudden  change  at  bow/stern  (Figs  3.6
          and  3.7).  It  is  shown  that  the  first  condition  influenced  the  wave-making  drag
          dramatically,  but  the  latter  did  not.  For  this  reason  it  is clear  that  wave-making is
          mainly generated  from  the  bow and  stern  (this is similar in principle to  the  bow  and
          stern wave patterns generated by a normal  ship's hull).
            With respect to shallow water drag, theoretical calculation demonstrated  that wave-
          making  drag  in shallow  water  would  be larger  than that in water with infinite depth,
          particularly  at  hump  speed.  As  water  depth  reduces,  so  the  drag  increases  so  as  to
          increase the drag hump. When  the  effect  of  the water depth  on  the practical  limit for
          the  height of  generated  waves  is taken  into  account,  this  limits the  maximum wave
          drag, which is the reason operators  can use shallow water to  go through hump  speed
          on a marginal craft.
            If  the  progression  through craft  hump  speed was not  steady, but  accelerating,  Tat-
          inclaux  showed that  the wave-making drag peaks caused  by an  air  cushion with  the
          hyperbolic  tangent  pressure  distribution  at  the  bow/stern  running  over  both  deep
          and  shallow water at constant  accelerated motion  were flattened by the  acceleration.
            This effect  will be strengthened  while craft  are travelling  over  shallow  water  rather
          than  deep water  (Figs 3.8 and  3.9). These figures show that  the craft  peak  resistance
          will  decrease in shallow water by accelerated motion,  in  a similar manner  to  that  on
          deep  water at  approximately Fr  =  0.5.  This  is another  reason  why an  ACV  or  SES,
          particularly with flexible skirts, can pass through  the hump  speed  over shallow water
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