Section
3 Motion response
3.1 Relative vertical motion
3.1.1 The relative
vertical motion is to be taken as:
where
k
r
|
= |
see
Table 2.3.1 Hull form wave pressure
factor
|
C
w,min
|
= |
|
k
m
|
= |
|
x
m
|
= |
0,45 – 0,6F
n but not less than
0,2
|
C
w
|
= |
wave head, in metres |
= |
|
x
wI
|
= |
distance from aft end of L
WL, in metres, see
Pt 5, Ch 2, 2.2 Symbols 2.2.1
|
L
WL
|
= |
waterline length, in metres, see
Pt 5, Ch 2, 2.1 Parameters to be used for the determination of load and design criteria 2.1.19
|
C
b
|
= |
block coefficient, see
Pt 5, Ch 2, 2.2 Symbols
|
F
n
|
= |
Froude Number, see
Pt 5, Ch 2, 2.1 Parameters to be used for the determination of load and design criteria 2.1.7, where V
m = 2/3V
|
V
|
= |
as
defined in Pt 5, Ch 2, 2.1 Parameters to be used for the determination of load and design criteria 2.1.2.
|
Table 2.3.1 Hull form wave pressure
factor
Craft type
|
k
r
|
Mono-hull craft in the
non-displacement mode
|
2,25
|
Mono-hull craft in the displacement
mode
|
1,95
|
Catamarans and multi-hull craft with
partially submerged hulls
|
2,55
|
Swaths and multi-hull craft with fully
submerged hulls
|
2,10
|
Craft supported by hydrodynamic lift
provided by foils or other lifting devices
|
1,50
|
Note Where multiple craft types apply, the higher value of
k
r is to be used.
|
3.2 Vertical acceleration
3.2.1 The instantaneous accelerations determined in accordance with the formulae
in this Section are to be used to estimate the relationship between allowable speed,
V, in knots, wave height, H
1/3, in metres, and displacement, Δ, in tonnes, and they will form the
operational envelope.
3.2.2 Where the
Taylor Quotient, Γ, is greater than 10,8, the motion response
criteria are to be specially considered.
3.2.3 The vertical
acceleration at the LCG (longitudinal centre of gravity), a
v, is defined as the average of the 1/100 highest accelerations
at the LCG.
3.2.4 The vertical
acceleration in the non-displacement mode for mono-hull craft is to
be taken as:
where
|
= |
a
v is the vertical acceleration at the
LCG in terms of g
|
Γ |
= |
Taylor Quotient, see
Pt 5, Ch 2, 2.1 Parameters to be used for the determination of load and design criteria 2.1.17
|
g
|
= |
acceleration
due to gravity (9,81 m/sec2)
|
L
1
|
= |
, but is not to be taken as less than 3
|
H
1
|
= |
, but is not to be taken as less than 0,2
|
B
c
|
= |
breadth of hull between the chines or bilge tangential points
at LCG, as appropriate, in metres |
B
W
|
= |
breadth of hull at the LCG measured at the waterline, in metres |
Δ |
= |
displacement,
in tonnes, as defined in Pt 5, Ch 2, 2.2 Symbols 2.2.2
|
H
1/3
|
= |
design significant wave height in metres |
θD
|
= |
deadrise
angle at the LCG, in degrees, but is not to be taken as greater than
30o
|
θB
|
= |
running
trim angle in degrees, but is not to be taken as less than 3o
|
L
WL
|
= |
waterline length, in metres, see
Pt 5, Ch 2, 2.1 Parameters to be used for the determination of load and design criteria 2.1.19
|
3.2.5 The vertical
acceleration in the non-displacement mode for multi-hull craft is
to be taken as:
where
|
= |
a
v is the vertical acceleration at the
LCG in terms of g.
|
Γ |
= |
Taylor Quotient, see
Pt 5, Ch 2, 2.1 Parameters to be used for the determination of load and design criteria 2.1.17
|
fa
|
= |
hull
form acceleration factor |
|
= |
2,7 for craft supported
mainly by hydrodynamic lift provided by foils or other lifting devices |
|
= |
3,6 for Swaths
and multi-hull craft with fully submerged hulls |
|
= |
4,5 for catamarans
and multi-hull craft with partially submerged hulls |
B
M
|
= |
total breadth of hulls or struts at LCG at the waterline, in
metres, excluding tunnels |
Δ |
= |
displacement,
in tonnes. |
H
1/3
|
= |
design significant wave height, in metres |
θD
|
= |
deadrise
angle at the LCG, in degrees, but is not to be taken as greater than
30o, see
Pt 5, Ch 2, 2.1 Parameters to be used for the determination of load and design criteria 2.1.5
|
L
WL
|
= |
waterline length, in metres, see
Pt 5, Ch 2, 2.1 Parameters to be used for the determination of load and design criteria 2.1.19
|
3.2.6 The vertical
acceleration in the displacement mode for all craft is to be taken
as:
3.2.7 The vertical
acceleration, a
x, at any given location distance x
a from the AP along the hull may be taken as:
where
a
v
|
= |
vertical acceleration at LCG in terms of g, as
appropriate.
|
a
x
|
= |
is the vertical acceleration at distance x
a from
AP on the static load waterline, in terms of g
|
x
a
|
= |
distance from aft end of the static load waterline, in metres,
to the point at which the vertical acceleration is calculated |
x
LCG
|
= |
distance from aft end of the static load waterline, in metres,
to the LCG |
L
WL
|
= |
waterline length, in metres, see
Pt 5, Ch 2, 2.1 Parameters to be used for the determination of load and design criteria 2.1.19
|
ξa
|
= |
.
|
|