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             from the figure,  the wave angle is about 35’.  We can see both transverse and divergent wave systems.
             But the divergent wave systems are dominant. For Fig 10, 4 is equal to 1.2. The wave angle is about
             SO’ measured from the figure. We can only see the divergent wave systems. The wave angles are in
             good agreement with the results in Fig 1. Wash has a close relationship with the corresponding wave
             resistance. We can therefore get some information on how to minimize wash from Figs 4 and 5. The
             shallow  water  wave  resistance ratio  r  is about  1.5  for  Fh = 0.9 , HIL = 0.1  and  is  about 4  for
              Fh = 1.2, HI L = 0.1. This means that the wash at  Fh = 0.9 is favorable. By  using Figs 4 and 5 we
             could minimize wash by  changing 6. For  Fh = 1.2, we  should actually increase 6. If we  increase
             the  speed  by  -lo%,  r  will  decrease from  -4  to  -2.  But  for Fh = 0.9,  the change of 6 will  not
             improve the wash problem. Both increase and decrease of 4 will increase the value of r  if the change
             of 4 is confined to It 10%. We should note that a large value of shallow water wave resistance ratio
              r  is not  necessarily corresponding to  large value of wave resistance if there is a  large difference
             between  F, . It should also be noted that r can be less than 1 which means that shallow water can have
             a positive effect on wash.


             4  CONCLUSIONS
              Steady forward ship motions in finite water depth are numerically investigated by thin ship theory and
             steady Green’s function satisfying classical linear free surface condition in finite water depth. Both the
              wave part and the local disturbance of the Green’s function are studied carefully. The local disturbance
              is numerically difficult to handle. The longitudinal  force 4, vertical force 4, pitch moment 4 and
              wash are calculated.  The local disturbance part of the Green’s function is important in calculating 4
              and 4. The present methods have been tested for a Wigley hull, and the results are compared with
              experiments and Tuck’s  shallow water  slender body theory. The shallow water theory is limited  to
              small  water  depth  while  the  present  theory  applies  to  any  water  depth.  Wash  is  discussed by
              systematically presenting results for the wave resistance.


              References

              Abramowitz,  M.  and  Stegun,  I.  A.(1964),  Handbook  of Mathematical  Functions  with  Formulas,
                   Graphs, and Mathematical Tables, Dover Publications, New York.
              Chen, X.-N.  and Shanna, S.D.(1995), A Slender Ship Moving at a Near-critical Speed in a Shallow
                   Channel, J. Fluid Mech., .291, pp. 263-285.
              Dahlquist, G., Bjiirck,A. and Anderson, N.( 1974). Numerical Method, Prentice-hall, Inc. Englewood
                   Cliffs, New Jersey.
              Everest, J.  T. and Hogben,  N.(1970).  An  Experimental Study of the Effect of Beam  Variation and
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              Hofman, M. and Kozarski, V.(2000). Shallow Water Resistance Charts For Preliminary Vessel Design.
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              Kostyukov,A.A.( 1968),Theory of  Ship Wave and Wave Resistance, Effective Communications Inc.
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              Lea,  G. K.  and  Feldrnan,  J.  P.(1972).  Transcritical  Flow  Past  Slender  Ships.  qh S’mp.  Naval
                   Hydro@namics,  Paris,  1527-1539.
              Lunde, J.K.(1951).  On the Linearized Theory of Wave Resistance for Displacement Ships in Steady
                   and Accelerated Motion. Trans SNAME 25-85.
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