4.28
Guidance notes for chapter 4
4.28.1
Guidance to detailed calculation of internal pressure for static design
purpose
4.28.1.1 This section provides guidance for the
calculation of the associated dynamic liquid pressure for the purpose of static
design calculations. This pressure may be used for determining the internal pressure
referred to in 4.13.2.4, where:
-
.1 (Pgd
)max is the associated liquid pressure determined using the maximum
design accelerations.
-
.2 (Pgd
site)max is the associated liquid pressure determined using site
specific accelerations.
-
.3
Peq
should be the greater of Peq1
and Peq2
calculated as follows:
-
Peq1
|
= |
Po
+ (Pgd
)max (MPa), |
Peq2
|
= |
Ph
+ (Pgd
site)max (MPa), |
4.28.1.2 The internal liquid pressures are those
created by the resulting acceleration of the centre of gravity of the cargo due to
the motions of the ship referred to in 4.14.1. The value of internal liquid pressure
Pgd
resulting from combined effects of gravity and dynamic accelerations should be
calculated as follows:
![](svgobject/58C9-4856-8006-62040B01C0AB.xml_d9821332e188.png)
-
where:
-
αβ
|
= |
dimensionless acceleration (i.e. relative to
the acceleration of gravity), resulting from gravitational
and dynamic loads, in an arbitrary direction β (see
figure 4.1). |
- For large tanks, an acceleration ellipsoid taking account of transverse
vertical and longitudinal accelerations, should be used.
-
Zβ
|
= |
largest liquid height (m) above the point where
the pressure is to be determined measured from the tank
shell in the β direction (see figure 4.2). Tank domes
considered to be part of the accepted total tank volume
shall be taken into account when determining
Zβ
, unless the total volume of tank domes
Vd
does not exceed the following value: |
-
-
with:
-
Vt
|
= |
tank volume without any domes;
and |
FL
|
= |
filling limit according to chapter
15. |
-
ρ
|
= |
maximum cargo density (kg/m3) at the
design temperature. |
The direction that gives the maximum value (Pgd
)max or (Pgd
site)max should be considered. The above formula applies only to full tanks.
LR 4.28-01 For determining Zβ, see also Figure
4.3 and Fig. LR 4.3.
4.28.1.3 Equivalent calculation procedures may be
applied.
4.28.2
Guidance formulae for acceleration components
4.28.2.1 The following formulae are given as guidance
for the components of acceleration due to ship's motions corresponding to a
probability level of 10-8 in the North Atlantic and apply to ships with a
length exceeding 50 m and at or near their service speed:
-
- vertical acceleration, as defined in 4.14.1:
-
- transverse acceleration, as defined in 4.14.1:
-
- longitudinal acceleration, as defined in 4.14.1:
where:
L0
|
= |
length of the ship for determination of scantlings as defined in
recognized standards (m); |
B
|
= |
greatest moulded breadth of the ship (m); |
x
|
= |
longitudinal distance (m) from amidships to the centre of
gravity of the tank with contents; x is positive forward of amidships,
negative aft of amidships; |
y
|
= |
transverse distance (m) from centreline to the centre of
gravity of the tank with contents; |
z
|
= |
vertical distance (m) from the ship's actual waterline to the
centre of gravity of tank with contents; z is positive above and negative
below the waterline; |
K
|
= |
1 in general. For particular loading conditions and hull forms,
determination of K according to the following formula may be necessary: |
-
K
|
= |
13GM/B, where K ≥ 1 and GM =
metacentric height (m); |
- A =
; and
V
|
= |
service speed (knots); |
ax, ay, az
|
= |
maximum dimensionless accelerations (i.e. relative to the
acceleration of gravity) in the respective directions. They are considered
as acting separately for calculation purposes, and az
does not include the component due to the static weight,
ay
includes the component due to the static weight in the transverse
direction due to rolling and ax
includes the component due to the static weight in the longitudinal
direction due to pitching. The accelerations derived from the above formulae
are applicable only to ships at or near their service speed, not while at
anchor or otherwise near stationary in exposed locations. |
LR 4.28-02 For the purpose of calculating the acceleration
components in 4.28.2 the length of the ship for determination of scantlings shall be
taken as the Rule length (L) and amidships is to be taken as the middle of
the Rule length, L, measuring from the forward side of the stern. The breadth
and the Rule length are to be taken as defined in Pt 3, Ch 1,6 of the Rules for
Ships.
4.28.3
Stress categories
4.28.3.1 For the purpose of stress evaluation, stress
categories are defined in this section as follows.
4.28.3.2
Normal stress is the component of stress normal to the plane of reference.
4.28.3.3
Membrane stress is the component of normal stress that is uniformly
distributed and equal to the average value of the stress across the thickness of the
section under consideration.
4.28.3.4
Bending stress is the variable stress across the thickness of the section
under consideration, after the subtraction of the membrane stress.
4.28.3.5
Shear stress is the component of the stress acting in the plane of reference.
4.28.3.6
Primary stress is a stress produced by the imposed loading, which is
necessary to balance the external forces and moments. The basic characteristic of a
primary stress is that it is not self-limiting. Primary stresses that considerably
exceed the yield strength will result in failure or at least in gross deformations.
4.28.3.7
Primary general membrane stress is a primary membrane stress that is so
distributed in the structure that no redistribution of load occurs as a result of
yielding.
4.28.3.8
Primary local membrane stress arises where a membrane stress produced by
pressure or other mechanical loading and associated with a primary or a
discontinuity effect produces excessive distortion in the transfer of loads for
other portions of the structure. Such a stress is classified as a primary local
membrane stress, although it has some characteristics of a secondary stress. A
stress region may be considered as local, if:
-
and
-
,
where:
S1
|
= |
distance in the meridional direction over which the equivalent
stress exceeds 1.1f; |
S2
|
= |
distance in the meridional direction to another region where
the limits for primary general membrane stress are exceeded; |
R
|
= |
mean radius of the vessel; |
t
|
= |
wall thickness of the vessel at the location where the primary
general membrane stress limit is exceeded; and |
f
|
= |
allowable primary general membrane stress. |
4.28.3.9
Secondary stress is a normal stress or shear stress developed by constraints
of adjacent parts or by self-constraint of a structure. The basic characteristic of
a secondary stress is that it is self-limiting. Local yielding and minor distortions
can satisfy the conditions that cause the stress to occur.
Fig. LR 4.3 Determination of
internal pressure heads