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K. J. Spyrou 《Journal of Marine Science and Technology》1995,1(1):24-36
The behavior of a ship encountering large regular waves from astern at low frequency is the object of investigation, with a parallel study of surf-riding and periodic motion paterns. First, the theoretical analysis of surf-riding is extended from purely following to quartering seas. Steady-state continuation is used to identify all possible surf-riding states for one wavelength. Examination of stability indicates the existence of stable and unstable states and predicts a new type of oscillatory surf-riding. Global analysis is also applied to determine the areas of state space which lead to surf-riding for a given ship and wave conditions. In the case of overtaking waves, the large rudder-yaw-surge oscillations of the vessel are examined, showing the mechanism and conditions responsible for loss of controllability at certain vessel headings.List of symbols
c
wave celerity (m/s)
-
C(p)
roll damping moment (Ntm)
-
g
acceleration of gravity (m/s2)
-
GM
metacentric height (m)
-
H
wave height (m)
-
I
x
,I
z
roll and yaw ship moments of inertia (kg m2)
-
k
wave number (m–1)
-
K
H
,K
W
,K
R
hull reaction, wave, rudder, and propeller
-
K
p
forces in the roll direction (Ntm)
-
m
ship mass (kg)
-
n
propeller rate of rotation (rpm)
-
N
H
,N
W
,N
R
hull reaction, wave, rudder, and propeller
-
N
P
moments in the yaw direction (Ntm)
-
p
roll angular velocity (rad/s)
-
r
rate-of-turn (rad/s)
-
R(,x)
restoring moment (Ntm)
-
Res(u)
ship resistance (Nt)
-
t
time (s)
-
u
surge velocity (m/s)
-
U
vessel speed (m/s)
-
v
sway velocity (m/s)
-
W
ship weight (Nt)
-
x
longitudinal position of the ship measured from the wave system (m)
-
x
G
,z
G
longitudinal and vertical center of gravity (m)
-
x
S
longitudinal position of a ship section (S), in the ship-fixed system (m)
-
X
H
,X
W
,X
R
hull reaction, wave, rudder, and propeller
-
X
P
forces in the surge direction (Nt)
-
y
transverse position of the ship, measured from the wave system (m)
-
Y
H
,Y
W
,Y
R
hull reaction, wave, rudder, and propeller
-
Y
p
forces in the sway direction (Nt)
-
z
Y
vertical position of the point of action of the lateral reaction force during turn (m)
-
z
W
vertical position of the point of action of the lateral wave force (m)
Greek symbols
angle of drift (rad)
-
rudder angle (rad)
-
wavelength (m)
-
position of the ship in the earth-fixed system (m)
-
water density (kg/m3)
-
angle of heel (rad)
-
heading angle (rad)
-
e
frequency of encounter (rad/s)
Hydrodynamic coefficients
K
roll added mass
-
N
v
,N
r
yaw acceleration coefficients
-
N
v
N
r
N
rr
N
rrv
,N
vvr
yaw velocity coefficients K. Spyrou: Ship behavior in quartering waves
-
X
u
surge acceleration coefficient
-
X
u
X
vr
surge velocity coefficients
-
Y
v
,Y
r
sway acceleration coefficients
-
Y
v
,Y
r
,Y
vv
,Y
rr
,Y
vr
sway velocity coefficients
European Union-nominated Fellow of the Science and Technology Agency of Japan, Visiting Researcher, National Research Institute of Fisheries Engineering of Japan 相似文献
2.
Naoya Umeda 《Journal of Marine Science and Technology》1999,4(1):16-26
To provide a theoretical methodology to predict the critical condition for capsizing due to broaching, a nonlinear dynamical
system approach was applied to the surge–sway–yaw–roll motion of a ship running with an autopilot in following and quartering
seas. Fixed points of a mathematical model for the ship motion and unstable manifolds of the fixed point near the wave crest
were systematically investigated. As a result, the existence of heteroclinic bifurcation was identified. With numerical experiments,
it was confirmed that this heteroclinic bifurcation reasonably well represents the critical condition for capsizing due to
broaching. Thus the nonlinear dynamical approach can be substituted for tedious numerical experiments.
Received for publication on Nov. 20, 1998; accepted on March 16, 1999 相似文献
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唐哲 《船舶标准化工程师》2014,(6):9-12
介绍了骑浪/横甩的物理背景,以及骑浪/横甩第一层和第二层薄弱性衡准发展过程,并分析了骑浪横甩薄弱性衡准计算方法及初步衡准,掌握骑浪横甩薄弱性衡准技术的发展现状,有助于骑浪/横甩相关技术领域的研究,为船舶第二代完整稳性的技术发展奠定基础。 相似文献
6.
船舶骑浪运动的分叉研究 总被引:1,自引:0,他引:1
在纵荡运动模型的基础上,应用非线性动力学理论对骑浪产生的机理进行了研究,确认了骑浪运动是一个从周期运动到骑浪的过程,其中经历了两次分叉.给出了导致骑浪发生的危险临界参数值,以及周期运动和骑浪运动区域划分. 相似文献
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