Section 7 Guidance
7.1 Guidance Notes for Chapter 4
7.1.1
Guidance to detailed calculation of internal pressure for static design
purpose
- 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
given in Pt 11, Ch 4, 3.3 Functional loads 3.3.2.
P
gd is the associated maximum liquid pressure determined using
site-specific accelerations.
P
eq is to be calculated as follows:
P
eq= P
o + P
gd (MPa)
- 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 unit referred to in Pt 11, Ch 4, 3.4 Environmental loads 3.4.2. The value of internal liquid pressure
Pgd
resulting from combined effects of gravity and dynamic accelerations shall
be calculated as follows:
where
αβ
|
= |
dimensionless acceleration (i.e. relative to the
acceleration of gravity), resulting from gravitational and dynamic
loads, in an arbitrary direction β, (see
Pt 11, Ch 4, 6.2 Type B independent tanks 6.2.1)
Note for
large tanks an acceleration ellipsoid, taking account of transverse
vertical and longitudinal accelerations should be used
|
Z
|
= |
largest liquid height (in metres) above the point where
the pressure is to be determined measured from the tank shell in the β
direction (see
Pt 11, Ch 4, 7.1 Guidance Notes for Chapter 4 7.1.1) Tank domes considered to be
part of the accepted total tank volume shall be taken into account
when determining Z
β unless the total volume of tank domes Vd
does not exceed the following value: |
V
d
|
= |
|
where
V
t
|
= |
tank volume without any domes |
ρ |
= |
maximum cargo density (kg/m3) at the design
temperature |
The direction that gives the maximum value of P
gd shall be considered. Where acceleration components in three
directions need to be considered, the ellipsoid shown in Pt 11, Ch 4, 7.1 Guidance Notes for Chapter 4 7.1.1 shall be used instead of the ellipse
in Pt 11, Ch 4, 6.2 Type B independent tanks 6.2.1. The above formula applies only to
full tanks.
Figure 4.7.1 Determination of
internal pressure heads
See also
Pt 11, Ch 4, 7.1 Guidance Notes for Chapter 4 7.1.1.
Figure 4.7.2 Determination of
internal pressure heads
Accelerations in three dimensions are to be considered
for ship units with independent spherical Type B tanks for which the
ellipsoid as shown in Pt 11, Ch 4, 7.1 Guidance Notes for Chapter 4 7.1.1 is to be used. Where loading
conditions are proposed including one or more partially filled tanks, the
internal liquid pressure to be used will be specially considered. See
also
Pt 11, Ch 4, 3.4 Environmental loads 3.4.4.
Figure 4.7.3 Acceleration
ellipsoids
- Equivalent calculation procedures may be applied.
7.1.2
Guidance formulae for acceleration components
- The following formulae are given as guidance for the
determination of the maximum value of internal liquid pressure head P
gd, (see
Pt 11, Ch 4, 7.1 Guidance Notes for Chapter 4 7.1.1, internal pressure).
In
the transverse direction, as shown in Pt 11, Ch 4, 6.2 Type B independent tanks 6.2.1, the following apply:
The range of angle β is:
0
to βmax, with βmax = arc tan
For the longitudinal direction, βmax and
aβ
are to be determined with ax
substituted for ay.
7.1.3
Stress categories
- For the purpose of stress evaluation, stress categories are defined in this
Section.
-
Normal stress is the component of stress normal to the plane of
reference.
-
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.
-
Bending stress is the variable stress across the thickness of the
section under consideration, after the subtraction of the membrane stress.
-
Shear stress is the component of the stress acting in the plane of
reference.
-
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.
-
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.
-
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:
-
S
1 ≤ 0,5
and
-
S
2 ≥ 2,5
where:
S
1
|
= |
distance in the meridional direction over which the
equivalent stress exceeds 1,1f
|
S
2
|
= |
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 |
f
|
= |
allowable primary general membrane stress. |
-
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.
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