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8/6/2019 Testing of Ships
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TUMSTShip Manoeuvrability- Theory and Assessment- 1
Ship Manoeuvrability- Theory and Assessment -
Toshio Iseki
Tokyo University of Marine
Science and Technology
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TUMST Ship Manoeuvrability- Theory and Assessment- 2
IMO (International Maritime Organization)
MSC (Maritime Safety Committee)
Interim Standards for Ship Manoeuvrability
(IMO Resolution A.751(18), 1993)
Standards for ship manoeuvrability
(IMO Resolution MSC.137(76), 2002)
Exclusion of the ships that were built with very
poor manoeuvring qualities.(causes of marine casualties & pollution)
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TUMST Ship Manoeuvrability- Theory and Assessment- 3
Contents
Basic theory of ship manoeuvrability
Manoeuvring equation of motion
Directional stability
Manoeuvrability indices
Assessment of ship manoeuvrability
Graphical analysis of Zig-zag test
Real-time identification of shipmanoeuvrability (IIR filter)
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TUMST Ship Manoeuvrability- Theory and Assessment- 4
Co-ordinate systems
O Y
X
x
GUT
u
v
rT jviu
TTT!
torlocity vecAngulerve:
angleHeading:
dt
d
r
U
U
!
T
axesyandxthealongorsUnit vect:, ji
TT
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TUMST Ship Manoeuvrability- Theory and Assessment- 5
Time derivative of a rotating co-ordinate system
productVector:
,
rotationfororUnit vect:
v
!v!v ijkjik
kTTTTTT
T
jdt
dik
dt
dir
dt
id TTTTTT
UU!v!v!
idtdjk
dtdjr
dtjd
TTTTTT
UU !v!v!
jdt
du
dt
dvi
dt
dv
dt
dudt
jdvj
dt
dv
dt
idui
dt
du
dt
Ud
TT
TT
TT
T
!
!
UU
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TUMST Ship Manoeuvrability- Theory and Assessment- 6
Equations of motion
!
!
!
NrI
Yurvm
Xvrum
zz
)(
)(
momentandforcesExternal:,,
inartiaofMoment:
shiptheofMass:
NYX
I
m
zz
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TUMST Ship Manoeuvrability- Theory and Assessment- 7
Definition of external forces
External forces
Acting on the upper part from the water line
Wind force, etc.
Acting on the lower part from the water line
Hydrodynamic forces based on manoeuvre,
Current force
Another forcesTowing force of tug boat
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TUMST Ship Manoeuvrability- Theory and Assessment- 8
Hydrodynamic forces
_ a)(),(),(),(),(),(),()( ttrtvtutrtvtuYtY H!
Manoeuvring hydrodynamic derivative
H
H
H
!
YrYvYuYrYvYuY
YrvurvuY
rvurvu
0,,,,,,
_ a0,0,0,0,0,0,0 UYY !
vv
vv
YY
!x
x!
Taylor expansion
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TUMST Ship Manoeuvrability- Theory and Assessment- 9
Manoeuvring equations of motion
!
!
!
H
H
H
H
NrNrNvNvNN
YrYrYvYvYY
uu
rrvv
rrvv
uu
!
!
!
NrI
YmUrvm
Xum
zz
uUu p)(,,
)1(
Iorvu
oU
!
!
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TUMST Ship Manoeuvrability- Theory and Assessment- 10
Linear manoeuvring equations of motion
!
!
!
H
H
H
H
NrNvNvNrNI
YrYrmUYvYvYm
uXuXm
rvvrzz
rrvv
uu
)(
)()(
)(
!
!
!
rzz
vy
ux
Nj
Ym
Xm
!
!
!
H
H
H
H
NrNvNvNrjI
YrYrmUYvYvmm
uXumm
rvvzzzz
rrvy
ux
)(
)()(
)(
Added mass, Added inertia moment
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TUMST Ship Manoeuvrability- Theory and Assessment- 11
Non-dimensional expression
),(
speedshipofcomponentConstant:
draft:length,Ship:
salt waterofdensityMass:
vuUU
U
dL
!T
V
dL
mm
!2
2
1':ass
V 22
1':Force
UdL
XX
!
V
tL
Ut !d:Time
dt
d
U
L
td
d!
d:derivativeTime
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TUMSTShip Manoeuvrability
- Theory and Assessment- 12
Non-dimensional manoeuvring equations
ddddddd!ddd
dddddddd!ddd
dd!ddd
H
H
H
H
NrNvNvNrjI
YrYrmYvYvmm
uXumm
rvvzzzz
rrvy
ux
)(
)()(
)(
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TUMSTShip Manoeuvrability
- Theory and Assessment- 13
Mathematical models
Hydrodynamic force model
Abkowitz
MMG model (SNAJ, JTTC)
Response model
Nomoto model
System
(Ship)
Input output
Rudder Yaw rate
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TUMSTShip Manoeuvrability
- Theory and Assessment- 14
Response model
dddddd!dddd
dddddd!ddddd
H
H
H
H
NrjIrNvNvN
YrYrmYvYvmm
zzzzrvv
rrvy
)(
)()(
0ssuming !du
vv dd andliminate
HH d!ddd 54321 qqrqrqrq
ddddd!
dddd!
ddddd!
ddddddddddd!
dddddd!
HH
HH
YNNmmq
YNYNq
mYNNYq
mYNmmNjIYYNq
YNjImmq
vy
vv
rvrv
rvyrzzzzvrv
rvzzzzy
)(
)(
)()()(
))((
5
4
3
2
1
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TUMSTShip Manoeuvrability
- Theory and Assessment- 15
Nomoto model (2nd-order & 1storder)
HH dddd!ddddddd 32121 )( TKKrrTTrTT
4
5
3
3
4
3
2
21
3
121 ,,,
q
qT
q
qK
q
qTT
q
qTT !d!d!dd!dd
Manoeuvrability indices
KT model
HKrrT d!ddd 321 TTTT ddd!d
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TUMSTShip Manoeuvrability
- Theory and Assessment- 16
Directional stability analysis
0)( 2121 !ddddddd rrTTrTT
Course stability without any steering function
Characteristic equation
terr P0ubstitute !d
01)( 21
2
21!dddd
PP TTTTVite's formulas (relation between the roots of a quadratic equation )
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TUMSTShip Manoeuvrability
- Theory and Assessment- 17
Directional stability criterion
01
0
2121
21
2121
"dd
!
dd
dd!
TT
TT
TT
PP
PP
Vite's formulas (relation between the roots of a quadratic equation )
v
v
r
r
YN
mYN
dd"
ddd
Neutral point:
The center of pressure in
pure sway.
The center of pressure in pure yaw.
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TUMSTShip Manoeuvrability
- Theory and Assessment- 18
Solution of KT model
Turning test
HKrrT d!ddd
u!
)0()
0(
0)(
0ttt
HH
0H
T
K
T
r
dt
rd
d
d!
d
d
d)(
10
HKrTdt
rddd
d!
d
T
dt
Kr
rd
d!
dd
d
0H
CT
tKr
d!dd )log(
0H T
t
CeKtr d
d!d0
)( H
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TUMSTShip Manoeuvrability
- Theory and Assessment- 19
Solution of KT model
Initial condition: 00 !d! rt .
0HKd!
)1()( 0T
t
eKtrd
d!d H)(trd
t
0HKd
063.0 HKd
Td0
0
10
63.0)1( HH KeKrTt !d!dd! .
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TUMST
Ship Manoeuvrability- Theory and Assessment- 20
Assessment of
manoeuvring performance
Standards for ship manoeuvrability(IMO Resolution MSC.137(76), 2002)
Turning tests
Zig-zag testsStopping tests
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TUMSTShip Manoeuvrability
- Theory and Assessment- 21
10r/10rZig-zag manoeuvre (stb.)
1. The ship is brought to a steady course and speedaccording to the specific approach condition.
2. The rudder is ordered to 10rto starboard.
3. When the heading has changed by 10roff the basecourse, the rudder is shifted to 10rto port. The shipsyaw will be checked and a turn in the oppositedirection will begin.
4. When the heading is 10r port off the base course, the
rudder is reversed as before.5. The procedure is repeated until the ship heading has
passed the base course no less than two times.
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TUMSTShip Manoeuvrability
- Theory and Assessment- 22
Requirements of the standards for
ship manoeuvrability
The 10r/10rand 20r/20rzig-zag tests
(Essential information)
The overshoot angles
Initial turning time to second execute
The time to check yaw
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TUMSTShip Manoeuvrability
- Theory and Assessment- 23
-20
-10
0
10
20
0 20 40 60 80 100 120
Graphical estimation of T, K indices
te
te
te
!eee ttt
dttKdtdt
tddt
dt
tdT
0002
2
)()()(
HUU
)0()()0()()0()(
0
!
brt
mee tKdttKt
dt
d
dt
tdT
e
HHUUUU
er
t
me tKdttKte
HHU !0
)()(
Ae
(te)
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TUMSTShip Manoeuvrability
- Theory and Assessment- 24
Graphical analysis of Zig-zag test
eree tKKA HU !
''' eree tKKA HU !
'''''' eree tKKA HU !
rK H,23
2
123 KKK
!
_
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TUMSTShip Manoeuvrability
- Theory and Assessment- 25
-20
-10
0
10
20
0 20 40 60 80 100 120
Graphical analysis of Zig-zag test
to to to
!ooo ttt
dttKdtdt
tddt
dt
tdT
0002
2
)()()(
HUU
)0()()0()()0()(
0
!
ort
moo tKdttKt
dt
d
dt
tdT
o
HHUUUU
or
t
m tKdttKTo
HHE !0
)(tan
Ao
Ao or
t
mo tKdttK
dt
tdT
o
HHU
!0
)()(
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TUMSTShip Manoeuvrability
- Theory and Assessment- 26
Graphical analysis of Zig-zag test
oro tKKAT HE !tan
'''tanorotKKAT H!
''''''tan oro tKKAT H!
2
2/)( 876 TTTT !
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TUMST
Ship Manoeuvrability- Theory and Assessment- 27
On-line Identification of Ship Manoeuvrability
Indices by Using IIR Filters( IIR: Infinite Impulse Response)
HKrrT !
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TUMSTShip Manoeuvrability
- Theory and Assessment- 28
Real-time identification
RLS: RecursiveLeast Square
Direct method: IIR filter
Indirect method: Pulse response function
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TUMSTShip Manoeuvrability
- Theory and Assessment- 29
Response function
)/1(
/
)(
)()( Tss
TK
s
s
sG !! HU
Laplace transform
)(/)()/1(
)()()(
)}({)}()({
2
sTKsTss
sKssTs
tKLttTL
HU
HU
HUU
!
!
!
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TUMST
Ship Manoeuvrability
- Theory and Assessment- 30
G zb z b
z a z a( ) !
1 2
2
1 2
a p a p p e
b KTh
T p b KT p
h
T
h
T1 2
1 2
1
1 1 1
! ! !
!
!
( ), ,
,
Pulse response function
Z-Transformation
)1()(
timesam lin
1
1
!
!
kkz
hezhs
UU
! )(
1)1()( 11 sG
s
LZzzG
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TUMST
Ship Manoeuvrability
- Theory and Assessment- 31
ARX model
)()2()1(
)2()1()(
21
21
kekbkb
kakak
!
HH
UUU
)(
)()(
212
21
k
k
azaz
bzbzG
H
U!
!
( )t kh!
e k white noise( ) :
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TUMST
Ship Manoeuvrability
- Theory and Assessment- 33
RLS (Recursive Least Square) Method
J k e k we k
w e w ek k
( ) ( ) ( )
( ) ( )
!
2 2
4 2 3 2
1
4 3
.
.IH v! ck)(
wkkkDT
/)1()()1(1 ! H
wDkkkG /)1()()1( ! H
)()1()1( kkk T !U
_ a)1()1()1()()1( ! kkkGkk UU
_ a wkkkGk T /)()1()1()1( HIH !
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TUMST
Ship Manoeuvrability
- Theory and Assessment- 34
Integrated Form ofthe Linear Response Model
)()()( 210 kkk FHEUU !
E F! !1T
KT
,
!
!
!
kh
hk
kh
hk
kh
hk
ddkk
dkk
khk
)1( )1(1122
)1(
11
0
)()1()(
,)()1()(
)()(
XXXHHH
XXUUU
UU
! dtdttKdtdtttT )())()(( HUU
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TUMST
Ship Manoeuvrability
- Theory and Assessment- 35
Impulse response of
FIR filter and IIR filter
1
t0(! Lt
)(tg
1
t0(! Lt
)(tg
s
esH
sL(!
1)( P
!s
sH1
)(
)()()( (! Ltututgtetg P!)(
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TUMST
Ship Manoeuvrability
- Theory and Assessment- 36
IIR Filter
G ss
( ) !
1
P
n
z
z
hs
n
n
z
z
hssGzP
!
!
!!
P
P 11
1
12 1
12
)(
1)()(
1
1
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TUMST
Ship Manoeuvrability
- Theory and Assessment- 37
_ a
_ a
_ a)2()(2)(2
)2()(2)(
)2()(2
)2()(2)(
)2()(2)(
)2()(2)(
2
22
22
2
02
00
!
!
!
kkkBh
kAkAk
kkBh
kAkAk
kkkB
kAkAk
HHH
HHH
UU
UUU
UUU
UUU
IIR Filter
A
h
hB
h!
!
12
12
12
2P
PP,
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TUMST
Ship Manoeuvrability
- Theory and Assessment- 38
Measurement conditions and T-K value
Table 1 Measurement conditions and T-K valueNO. S eed Wave T(sec) K(1/sec)
11.5kt Head 7.57 0.138 9.9kt Head 7.83 0.116
7.6kt Head 9.63 0.094
12.3kt Follow 7.74 0.153
9.5kt Follow 8.55 0.132
7.4kt Follow 12.41 0.089
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TUMST
Ship Manoeuvrability
- Theory and Assessment- 39
Measured time histories
7 LP HVH F