Ship Waves in Shallow Water and Their Effects on Moored Small Vessel

Author(s):  
Katsuhiko Kurata ◽  
Kazuki Oda
1984 ◽  
Vol 1 (19) ◽  
pp. 218 ◽  
Author(s):  
Katsuhiko Kurata ◽  
Kazuki Oda

The characteristics of ship-generated waves in shallow water and the motions of moored small vessel induced by the ship waves were investigated in a wide range of water-depth and ship-length Froude Numbers. The maximum heights and periods of ship waves were obtained as functions of Froude Number. The relationships between maximum angular and translatory displacements of moored vessel and the maximum ship waves were determined.


2018 ◽  
Vol 3 (2) ◽  
pp. 109-126 ◽  
Author(s):  
Yi Zhu ◽  
Jaiyi He ◽  
Huiyu Wu ◽  
Wei Li ◽  
Francis Noblesse
Keyword(s):  

1997 ◽  
Vol 335 ◽  
pp. 305-321 ◽  
Author(s):  
XUE-NONG CHEN ◽  
SOM DEO SHARMA

This paper deals with the wave pattern and wave resistance of a slender ship moving steadily at supercritical speed in a shallow water channel. Using, successively, linear and nonlinear shallow-water wave theory it is demonstrated that, if the hull form is adapted to speed and channel geometry according to certain rules, the ship waves can be made to form a localized pattern around the ship that moves at the same speed as the ship and at the same time the associated wave resistance can be made to vanish. In the nonlinear case, the zero-wave-resistance ship hull is derived from a KP equation solution of the oblique interaction of two identical solitons. This astonishing phenomenon may be called shallow-channel superconductivity.


2000 ◽  
Vol 16 ◽  
pp. 375-380
Author(s):  
Katsutoshi TANIMOTO ◽  
Hidetaka KOBAYASHI ◽  
Katsuhiko KURATA ◽  
Hiroshi KONNO

2017 ◽  
Vol 29 (5) ◽  
pp. 817-824 ◽  
Author(s):  
Chen-liang Zhang ◽  
Jin-bao Wang ◽  
Yi Zhu ◽  
Francis Noblesse

1976 ◽  
Vol 77 (4) ◽  
pp. 737-751 ◽  
Author(s):  
Chiang C. Mei

Approximations for shallow-water ship waves are sought which are valid near the critical speed U = (gh)1/2. For sufficiently thin bodies (struts or ships) the governing equation is dispersive. Simple analytic solutions are given which are valid for all F2 ≤ O(1). As the thickness increases, nonlinearity also enters. A soliton solution is discussed which applies to a sharp-nosed half-body at slightly supercritical speed.


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