3.1 Objective
3.1.1 These Guidelines provide specifications for direct stability assessment
procedures for the following stability failure modes:
-
.1 dead ship condition;
-
.2 excessive acceleration;
-
.3 pure loss of stability;
-
.4 parametric rolling; and
-
.5 surf-riding/broaching.
3.1.2 The criteria, procedures and standards recommended in these guidelines ensure a
safety level corresponding to the average stability failure rate not exceeding
2.6·10-3 per ship per year.
3.1.3 Direct stability assessment procedures are intended to employ latest technology
while being sufficiently practical to be uniformly accepted and applied using
currently available infrastructure.
3.1.4 The provisions given hereunder apply to all ships and all failure modes.
However, the provisions for both the dead ship condition and pure loss of stability
failure modes should not apply to ships with an extended low weather deck.
3.2 Requirements
3.2.1 The failure event is defined as:
-
.1 exceedance of roll angle, defined as: 40 degrees, angle of
vanishing stability in calm water or angle of submergence of unprotected
openings in calm water, whichever is less; or
-
.2 exceedance of lateral acceleration of 9.81 m/s2, at the
highest location along the length of the ship where passengers or crew may
be present.
The Administrations may define stricter requirements, if deemed necessary.
3.2.2 Active means of motion reduction, such as active anti-roll fins and anti-roll
tanks, can significantly reduce roll motions in seaway. However, the safety of the
ship should be ensured in cases of failure of such devices, therefore, the
vulnerability assessment according to these Interim Guidelines should be conducted
with such devices inactive or retracted, if they are retractable.
3.2.3 The procedure for direct stability assessment consists of two major components:
-
.1 a method that adequately replicates ship motions in waves (see 3.3); and
-
.2 a prescribed procedure that identifies the process by which input values
are obtained for the assessment, how the output values are processed, and
how the results are evaluated (see 3.5).
3.3 Requirements for a method that adequately predicts ship motions
3.3.1 General considerations
3.3.1.1 The motion of ships in waves can be predicted by means of numerical
simulations or model tests.
3.3.1.2 The choice between numerical simulations, model tests or their combination
should be agreed with the Administration on a case-by-case basis taking into account
these Interim Guidelines.
3.3.1.3 The procedures, calibrations and proper application of technology involved in
the conduct of model tests should follow "Recommended Procedures, Model Tests on
Intact Stability, 7.5-02-07-04.1" issued by the International Towing Tank Conference
(ITTC) in 2008. Users may follow recent amended versions of the Recommended
Procedures at the time of execution of tests, if deemed necessary.
3.3.1.4 Numerical simulation of ship motions may be defined as the numerical solution
of the motion equations of a ship sailing in waves including or excluding the effect
of wind (see 3.3.2).
3.3.2 General requirements
3.3.2.1 Modelling of waves
3.3.2.1.1 The mathematical model of waves should be consistent and appropriate for
the calculation of the forces.
3.3.2.1.2 Modelling of irregular waves should be statistically and hydrodynamically
valid. Caution should be exercised to avoid a self-repetition effect.
3.3.2.2 Modelling of roll damping: avoiding duplication
3.3.2.2.1 Roll damping forces should include wave, lift, vortex (i.e. eddy-making)
and skin friction components.
3.3.2.2.2 The data to be used for the calibration of roll damping may be defined
from:
-
.1 roll decay or forced roll test;
-
.2 CFD computations, if sufficient agreement with experimental results in
terms of roll damping is demonstrated;
-
.3 existing databases of measurements or CFD computations for similar ships,
if suitable range is available; or
-
.4 empirical formulae, applied within their applicability limits.
3.3.2.2.3 If the wave component of roll damping is already included in the
calculation of radiation forces, measures should be taken to avoid including these
effects more than once.
3.3.2.2.4 Similarly, if any components of roll damping (e.g. cross-flow drag) are
directly computed whereas others are taken from the calibration data, similar
measures should be taken to exclude these directly computed elements from the
calibration data used.
3.3.2.2.5 Consideration of the essential roll damping elements more than once can be
avoided through use of an iterative calibration procedure in which the roll decay or
forced roll tests are replicated in numerical simulations. The results should be
determined to be reasonably close to the original calibration model test data set.
3.3.2.3 Mathematical modelling of forces and moments
3.3.2.3.1 The Froude-Krylov forces should be calculated using body-exact formulations
at least for the dead ship condition, pure loss of stability and parametric rolling
failure modes, for instance using panel or strip-theory approaches.
3.3.2.3.2 Radiation and diffraction forces should be represented in one of three
ways: one is to use approximate coefficients and the other two involve either a body
linear formulation or a body-exact solution of the appropriate boundary-value
problem.
3.3.2.3.3 Resistance forces should include wave, vortex and skin friction components.
The preferred source for these data is a model test. The added resistance in waves
can be approximated, if this element is not already included in the calculation of
diffraction and radiation forces. If the radiation and diffraction forces are
calculated as a solution of the hull boundary-value problem, measures must be taken
to avoid including these effects more than once.
3.3.2.3.4 Hydrodynamic reaction sway forces, roll moment and yaw moments could be
approximated, based on:
-
.1 Coefficients derived from model tests in calm water with planar motion
mechanism (PMM) or in stationary circular tests, by means of a rotating arm
or an x-y carriage.footnote
-
.2 CFD computations, provided that sufficient agreement is demonstrated with
a model experiment in terms of values of sway force and yaw moment. If the
radiation and diffraction forces are calculated as a solution of the hull
boundary-value problem, measures must be taken to avoid including these
effects more than once.
-
.3 Empirical database or empirical formulae, used within their applicability
range.
3.3.2.3.5 Thrust may be obtained by use of a coefficient-based model with approximate
coefficients to account for propulsor-hull interactions.
3.3.3 Requirements for particular stability failure modes
3.3.3.1 For the dead ship condition failure mode:
-
.1 Ship motion simulations should include at least the following four degrees
of freedom: sway, heave, roll and pitch.
-
.2 Three-component aerodynamic forces and moments generated on topside
surfaces may be evaluated using model test results. CFD results may be
admitted upon demonstration of sufficient agreement with a model experiment
in terms of values of aerodynamic force and moments. Empirical data or
formulae could be applied within their applicability range.
3.3.3.2 For the excessive acceleration failure mode, the ship motion simulations
should include at least the following three degrees of freedom: heave, pitch and
roll. If sway motion is not modelled, consideration should be given to accurate
reproduction of lateral acceleration.
3.3.3.3 For the pure loss of stability failure mode, ship motion simulations should
include at least the following four degrees of freedom: surge, sway, roll and yaw.
For those degrees of freedom not included in the dynamic modelling, static
equilibrium should be assumed.
3.3.3.4 For the parametric rolling failure mode, ship motion simulations should
include at least the following three degrees of freedom: heave, roll and pitch.
3.3.3.5 For the surf-riding/broaching failure mode:
-
.1 Ship motion simulations should include at least the following four degrees
of freedom: surge, sway, roll and yaw. For those degrees of freedom not
included in the dynamic modelling, static equilibrium should be assumed.
-
.2 Hydrodynamic forces due to vortex shedding from a hull should be properly
modelled. This should include hydrodynamic lift forces and moments due to
the coexistence of wave particle velocity and ship forward velocity, other
than manoeuvring forces and moments in calm water.
3.3.3.6 For the pure loss of stability and surf-riding/broaching failure modes, an
appropriate autopilot should be used.
3.3.3.7 For the pure loss of stability and surf-riding/broaching failure modes, the
initial condition should be set with a sufficiently small forward speed in order to
avoid artificial surf-riding, which cannot occur for a self-propelled ship.
3.4 Requirements for validation of software for numerical simulation of ship
motions
3.4.1 Validation
3.4.1.1 Validation is the process of determining the degree to which a numerical
simulation is an accurate representation of the real physical world from the
perspective of each intended use of the model or simulation.
3.4.1.2 Different physical phenomena are responsible for different modes of stability
failure. Therefore, the validation of software for the numerical simulation of ship
motions is failure-mode specific.
3.4.1.3 The validation data should be compatible with the general characteristics of
the ship for which the direct stability assessment is intended to be carried out.
3.4.1.4 The process of validation should be performed in two phases: one qualitative
and the other quantitative. In the qualitative phase, the objective is to
demonstrate that the software is capable of reproducing the relevant physics of the
failure mode considered. The objective of the quantitative phase is to determine the
degree to which the software is capable of predicting the specific failure mode
considered.
3.4.2 Qualitative validation requirements
Table 3.4.2 – Requirements and acceptance criteria for qualitative
validation
Item
|
Required for
|
Objective
|
Acceptance criteria
|
Periodic properties of roll oscillator
|
Software where hydrostatic and Froude-Krylov forces are
calculated with body exact formulation
|
Demonstrate consistency between calculated roll backbone
curve (dependence of roll frequency in calm water on roll
amplitude) and GZ curve in calm water
|
Based on the shape of calculated backbone curve. The backbone
curve must follow a trend which is consistent with the righting
lever
|
Response curve of roll oscillator
|
Software where hydrostatic and Froude-Krylov forces are
calculated with body exact formulation
|
Demonstrate consistency between the calculated roll backbone
curve and the calculated roll response curve (dependence of
amplitude of excited roll motion on the frequency of
excitation)
|
Based on the shape of the roll response curve. The roll
response curve must "fold around" the backbone curve and may
show hysteresis when the magnitude of excitation is
increased
|
Change of stability in waves
|
Software where hydrostatic and Froude-Krylov forces are
calculated with body exact formulation. Additional capability to
track the instantaneous GZ curve in waves may be
required
|
Demonstrate capability to reproduce wave pass effect
|
Typically in head and following waves, the stability
decreases when the wave crest is located near the midship
section (within the quarter of length) and the stability
increases when the wave trough is located near the midship
section (within the quarter of length)
|
Principal parametric resonance
|
Software where hydrostatic and Froude-Krylov forces are
calculated with a body exact formulation
|
Demonstrate capability to reproduce principal parametric
resonance
|
Usually, observing an increase and stabilization of amplitude
of roll oscillation in exact following or head seas when
encounter frequency is about twice of natural roll
frequency
|
Surf-riding equilibrium
|
Software for numerical simulation of surf-riding/
broaching
|
Demonstrate capability to reproduce surf-riding, while yaw is
fixed.
|
Observing sailing with the speed equal to wave celerity when
the propeller RPM is set for the speed in calm water which is
less than the wave celerity. The horizontal position of centre
of gravity is expected to be located near a wave trough
|
Heel during turn
|
Software for numerical simulation of surf-riding/
broaching
|
Demonstrate capability to reproduce heel caused by
turn
|
Observing development of heel angle during the turn
|
Turn in calm water
|
Software for numerical simulation of surf-riding/
broaching
|
Demonstrate correct modelling of manoeuvring forces
|
Observing correct direction of turn with large rudder
angles
|
Straight captive run in stern quartering waves
|
Software for numerical simulation of surf-riding/
broaching
|
Demonstrate correct modelling of wave forces including effect
of wave particle velocity
|
Observing correct tendency of phase difference of wave force
to incident waves
|
Heel caused by drift and wind
|
Software for numerical simulation of ship motions in dead
ship condition
|
Demonstrate capability to reproduce heel caused by a moment
created by aerodynamic load and drag caused by drift
|
Observing slowly developed heel angle after applying
aerodynamic load
|
3.4.3 Quantitative validation requirements
3.4.3.1 There are two objectives of quantitative validation of numerical simulation.
The first is to find the degree to which the results of numerical simulation differ
from the model test results. The results of a model test carried out in accordance
with 3.3.1.3 should be recognized as reference values. The second objective is to
judge if the observed difference between simulations and model tests is sufficiently
small or conservative for direct stability assessment to be performed for the
considered failure modes.
Table 3.4.3 – Indicative requirements and acceptance criteria for quantitative
validation
Item
|
Required for
|
Objective
|
Acceptance criteria
|
Response curve for parametric rolling in regular
waves
|
Parametric rolling
|
Demonstrate agreement between numerical simulation and model
tests regarding amplitude of the roll response
|
Maximum (over encounter frequency) roll amplitude should not
be underpredicted by more than 10%, if the amplitude is below
the angle of maximum GZ or 20% otherwise. Underprediction less
than 2 degrees may be disregarded.
|
Response curve for synchronous roll in regular waves
|
All modes
|
Demonstrate agreement between numerical simulation and model
tests regarding amplitude of the roll response
|
Maximum (over encounter frequency) roll amplitude should not
be underpredicted for more than 10%, if the amplitude is below
the angle of maximum GZ or 20% otherwise. Under-prediction less
than 2 degrees may be disregarded.
|
Variance test for synchronous roll
|
Software for numerical simulation of dead ship condition and
excessive acceleration
|
Demonstrate correct (in terms of statistics) modelling of
roll response in irregular waves
|
Reproduction of experimental results either within 95%
confidence interval or conservative
|
Variance test for parametric rolling
|
Software for numerical simulation of parametric
rolling
|
Demonstrate correct (in terms of statistics) modelling of
roll response in irregular waves
|
Reproduction of experimental results either within 95%
confidence interval or conservative
|
Wave conditions for surf-riding and broaching
|
Software for numerical simulation of surf-riding/
broaching
|
Demonstrate correct modelling of surf-riding/ broaching
dynamics in regular waves
|
Wave steepness causing surf-riding and broaching at the
wavelength 0.75 – 1.5 of ship length is within 15% of difference
between model tests and numerical simulations. Speed settings
are also within 15% difference between model tests and numerical
simulations.
|
3.5 Procedures for direct stability assessment
3.5.1 General description
3.5.1.1 The procedures for direct stability assessment contain a description of the
necessary calculations of ship motions including the choice of input data, pre- and
post-processing.
3.5.1.2 The direct stability assessment procedure is aimed at the estimation of a
likelihood of a stability failure in an irregular wave environment and because the
stability failures may be rare, the direct stability assessment procedure may
require a solution of the problem of rarity. This arises when the mean time to
stability failure is very long in comparison with the natural roll period that
serves as a main timescale for the roll motion process. The solution of the problem
of rarity essentially requires a statistical extrapolation; for this reason, the
validation must be performed for all elements of the direct stability assessment
procedure.
3.5.1.3 These Guidelines provide two general approaches to circumvent the problem of
rarity, namely assessment in design situations and assessment using deterministic
criteria. Mathematical techniques are provided that reduce the required number of
simulations or simulation time and can be used to accelerate assessment for both,
the full assessment and the assessment performed in design situations.
3.5.2 Verification of failure modes
3.5.2.1 Once a failure is identified in a numerical simulation, it is necessary to
examine whether it can be regarded as a failure mode for which the numerical method
is validated and direct assessment is intended. The suggested judging criteria for
this purpose are provided below.
3.5.2.2 If the local period of the obtained roll motion in following waves or in
stern quartering waves is nearly equal to the local wave encounter period and the
maximum roll angle occurs nearly at the relative wave position in which the
metacentric height becomes the smallest, it can be regarded as pure loss of
stability failure.
3.5.2.3 If the local period of the obtained roll motion is nearly equal to twice the
local wave encounter period and is nearly equal to the ship natural roll period, it
can be regarded as the parametric rolling stability failure considered in the
vulnerability criteria, which is sometimes called as "principal parametric rolling".
Other types of parametric rolling may occur with much smaller probability, which are
not addressed by the second generation intact stability criteria.
3.5.2.4 The condition when the ship cannot keep a straight course despite the
application of maximum steering efforts is known as broaching. The second generation
intact stability criteria address broaching associated with surf-riding. Other types
of broaching may occur at slower speed but are not considered here because the
centrifugal force, due to such slow-speed broaching which could induce heel, is much
smaller. The broaching associated with surf-riding can be identified if both the yaw
angle and yaw angular velocity increase over time under the application of the
maximum opposite rudder deflection.
3.5.2.5 If the local period of the obtained roll motion in beam waves is nearly equal
to the local wave encounter period, it can be regarded as harmonic rolling, which is
relevant to the dead ship condition failure mode, as well as the excessive
acceleration failure mode.
3.5.3 Environmental and sailing conditions
3.5.3.1 General approaches for selection of environmental and sailing conditions
3.5.3.1.1 The sea states chosen for the direct stability assessment must be
representative for the intended service of the ship.
3.5.3.1.2 Sea states are defined by the type of wave spectrum and statistical data of
its integral characteristics, such as the significant wave height and the mean
zero-crossing wave period. For ships of unrestricted service, the environment should
be described by the wave scatter table shown in table 2.7.2.1.2. For ships of
restricted service, the wave scatter table accepted by the Administration should be
used.
3.5.3.1.3 It is recommended to use the Bretschneider wave energy spectrum (see
2.7.2.1.1) and cosine-squared wave energy spreading with respect to the mean wave
direction. If short-crested waves are considered impracticable in model tests or
numerical simulations, long-crested waves can be used.
3.5.3.1.4 For a given set of environmental conditions, the assessment can be
performed using any of the following equivalent alternatives:
-
.1 full probabilistic assessment according to 3.5.3.2;
-
.2 assessment in design situations using probabilistic criteria according to
3.5.3.3; or
-
.3 assessment in design situations using deterministic criteria according to
3.5.3.4.
3.5.3.2 Full probabilistic assessment
3.5.3.2.1 In this approach, the criterion used is the estimate of the mean long-term
rate of stability failures, which is calculated as a weighted average over all
relevant sea states, wave directions with respect to the ship heading and ship
forward speeds, for each addressed loading condition.
3.5.3.2.2 To satisfy the requirements of this assessment, this criterion should not
exceed the standard of 2.6⋅10-8 (1/s).
3.5.3.2.3 The probabilities of the sea states are defined according to the wave
scatter table (see 3.5.3.1). For the excessive accelerations, pure loss of
stability, parametric rolling and surf-riding/broaching failure modes, the mean wave
directions with respect to the ship heading are assumed uniformly distributed and
the ship forward speed should be regarded as uniformly distributed from zero to the
maximum service speed. For the dead ship condition failure mode, beam waves and wind
should be assumed and the ship forward speed should be taken as zero.
3.5.3.3 Assessment in design situations using probabilistic criteria
3.5.3.3.1 Compared to the full probabilistic assessment, this approach significantly
reduces the required simulation time and number of simulations since the assessment
is conducted in fewer design situations. These design situations are specified for
each stability failure mode as combinations of the ship forward speed, mean wave
direction with respect to the ship heading, significant wave height and mean
zero-crossing wave period for each addressed loading condition.
3.5.3.3.2 In this approach, the criterion is the maximum (over the design situations
corresponding to a particular stability failure mode) stability failure rate,
defined in each design situation as the upper boundary of its 95%-confidence
interval.
3.5.3.3.3 To satisfy the requirements of this assessment, this criterion
should not exceed the threshold corresponding to one stability failure every 2 hours
in full scale in design sea states with probability density 10-5
(m⋅s)-1.
3.5.3.3.4 Table 3.5.3.3.4 shows the design situations for particular stability
failure modes, including mean wave direction with respect to the ship heading, ship
forward speed and range of wave periods; and the step of the zero-crossing wave
period in the specified ranges should not exceed 1.0 s.
Table 3.5.3.3.4 – Design situations for each stability failure mode
Stability failure
mode
|
Wave directions
|
Forward speeds
|
Wave period
|
Dead ship condition
|
Beam wind and waves
|
Zero
|
Tz/Tr from 0.7 to 1.3
|
Excessive acceleration
|
Beam
|
Zero
|
Tz/Tr from 0.7 to
1.3
|
Pure loss of stability
|
Following
|
Maximum nominal service
speed
|
Tp corresponding to
wavelengths comparable to ship length
|
Parametric rolling
|
Head and following
|
Zero
|
All wave periods in the wave
scatter table
|
Surf-riding/broaching
|
Following
|
Maximum nominal service
speed
|
Tp corresponding to
wavelengths in the range from 1.0L to 1.5L
|
3.5.3.3.5 For each mean zero-crossing wave period, the significant wave height is
selected according to the probability density of the sea state, as specified in
3.5.3.3.3. For unrestricted service, the significant wave heights are shown in table
3.5.3.3.5 depending on the mean zero-crossing wave period.
Table 3.5.3.3.5 – Significant wave heights for design sea states with probability
density 10-5 (m⋅s)-1
for unrestricted service
Tz(s)
|
4.5
|
5.5
|
6.5
|
7.5
|
8.5
|
9.5
|
10.5
|
11.5
|
12.5
|
13.5
|
14.5
|
15.5
|
16.5
|
Hs (m)
|
2.8
|
5.5
|
8.2
|
10.6
|
12.5
|
13.8
|
14.6
|
15.1
|
15.1
|
14.8
|
14.1
|
12.9
|
10.9
|
3.5.3.4 Assessment in design situations using deterministic criteria
3.5.3.4.1 A probabilistic assessment may require a long simulation time even when
using design situations and this can make it difficult to use model tests rather
than numerical simulations. Applying deterministic criteria, such as the mean 3-hour
maximum roll amplitude, may reduce the required simulation time and this may make it
easier to use model tests with, or instead of, numerical simulations. However, the
inaccuracy of this approach needs to be balanced by additional conservativeness.
3.5.3.4.2 In this approach, the criteria are the greatest (with respect to all design
situations for a particular stability failure mode) mean 3-hour maximum roll
amplitude and lateral acceleration for each addressed loading condition.
3.5.3.4.3 To satisfy the requirements of this assessment, these criteria should not
exceed half of the values in the definition of stability failure in 3.2.1.
3.5.3.4.4 The simulations or model tests for each design situation should comprise at
least 15 hours in full scale. This duration can be divided into several parts. The
results should be post-processed to provide at least five values of the 3-hour
maximum amplitude of roll angle or lateral acceleration, which are averaged to
define the mean 3-hour maximum amplitudes.
3.5.3.4.5 This approach uses design situations with the same mean wave directions
with respect to the ship heading, the same ship forward speeds and the same ranges
of the mean zero-crossing wave periods as the assessment in design situations using
probabilistic criteria (see 3.5.3.3).
3.5.3.4.6 For each mean zero-crossing wave period, the significant wave height is
selected according to the probability density of the sea state equal to
7⋅10-5 (m⋅s)-1. Table 3.5.3.4.6 shows these significant
wave heights for unrestricted service depending on the mean zero-crossing wave
period.
Table 3.5.3.4.6 Significant wave heights, in metres, for design sea states with
probability density 7⋅10-5
(m⋅s)-1 for assessment using deterministic criteria
for unrestricted service
Tz(s)
|
4.5
|
5.5
|
6.5
|
7.5
|
8.5
|
9.5
|
10.5
|
11.5
|
12.5
|
13.5
|
14.5
|
15.5
|
Hs (m)
|
2.0
|
4.4
|
6.9
|
9.1
|
10.9
|
12.1
|
12.8
|
13.1
|
13.0
|
12.5
|
11.3
|
9.0
|
3.5.4 Direct counting procedure
3.5.4.1 The direct counting procedure uses ship motions resulting from multiple
independent realisations of an irregular seaway to estimate the rate of stability
failure, r.
3.5.4.2 The procedure used for direct counting should provide the upper boundary of
the 95% confidence interval of the estimated rate of stability failure. This upper
boundary is the one which is used in direct stability assessment and operational
measures.
3.5.4.3 The counting procedure should ensure independence of the counted stability
failure events.
3.5.4.4 The failure rate r and associated confidence interval can be
estimated:
-
.1 by carrying out a simulation for each realisation of an irregular seaway
only until the first stability failure; or
-
.2 on the basis of a set of independent simulations with fixed specified
exposure time texp (s), under the assumption that
the relation between the probability p of failure within
texp and the failure rate r is p
= 1 – exp (-r·texp).
3.5.4.5 Alternatively to direct counting, extrapolation procedures can be used as
specified in section 3.5.5.
3.5.5 Extrapolation procedures
3.5.5.1 The extrapolation procedures to be used with these Guidelines should only
include those procedures that have been successfully validated and applied and which
should also include a detailed description of their application.
3.5.5.2 Cautions
3.5.5.2.1 The extrapolation method may be applied as an alternative to the direct
counting procedure.
3.5.5.2.2 Caution should be exercised because uncertainty increases, as the
extrapolation is associated with additional assumptions used for describing ship
motions in waves.
3.5.5.2.3 The statistical uncertainty of the extrapolated values should be provided
in a form of boundaries of the confidence interval evaluated with a confidence level
of 95%.
3.5.5.2.4 To control the uncertainty caused by nonlinearity, the principle of
separation may be used. Extrapolation methods based on the principle of separation
consist of at least two numerical procedures addressing different aspects of the
problem: "non-rare" and "rare".
3.5.5.2.5 The "non-rare" procedure focuses on the estimation of ship motions or waves
of small-to-moderate level for which the stability failure events can be
characterized statistically with acceptable uncertainty.
3.5.5.2.6 The "rare" procedure focuses on ship motions of moderate-to-severe level
for which numerical simulation are rarely required. Large motions may be separated
from the rest of the time domain data to obtain practical estimates of these
motions.
3.5.5.2.7 Different extrapolation methods based on the separation principle may use
different assumptions on how the separation is introduced.
3.5.5.3 Extrapolation over wave height
3.5.5.3.1 Extrapolation of the mean time to stability failure or mean rate of
stability failures over significant wave height is a technique allowing the
reduction of the required simulation time by performing numerical simulations or
model tests at greater significant wave heights than those required in the
assessment and extrapolating the results to lower significant wave heights.
3.5.5.3.2 The extrapolation is based on the approximation lnT = A +
B/Hs2, where T (s) is the mean
time to stability failure; Hs (m) is the significant wave
height; and A, B are coefficients which do not depend on the
significant wave height but depend on the other parameters specifying the situation
(wave period, wave direction and ship forward speed).
3.5.5.3.3 The extrapolation can be performed when at least three values of the
stability failure rate are available. These values should be obtained by direct
counting for a range of significant wave heights of at least 2 m. Each of the values
used in the extrapolation should correspond to the upper boundary of the
95%-confidence interval of stability failure rate and not exceed 5% of the
reciprocal natural roll period of the ship. The results should be checked for the
presence of outliers and non-conservative extrapolation and corrected, when
necessary, by adding or removing points used for extrapolation.
3.5.5.4 Other extrapolation procedures
3.5.5.4.1 Other extrapolation procedures may be used, taking into account 3.5.5.1 and
3.5.5.2. Such procedures may include those listed below and others:
3.5.6. Validation of extrapolation procedures
3.5.6.1 Extrapolation procedures used for direct stability assessment should be
validated.
3.5.6.2 Validation of an extrapolation procedure is a demonstration that the
extrapolated value is in reasonable statistical agreement with the result of the
direct counting, if such volume of data would be available.
3.5.6.3 The data for validation of the extrapolation procedure may be produced by a
mathematical model of reduced complexity (e.g. a set of ordinary differential
equations instead of a numerical solution of a boundary value problem) or by running
the full mathematical model on significantly more severe environmental and/or more
onerous loading conditions. The objective is to decrease the computational cost by
which a large data set can be obtained (the validation data set). Physical
experiments can be used for the same purpose.
3.5.6.4 The direct counting procedure applied to the validation data set should
produce the "true value". The extrapolation procedure applied to a minimally
required fraction of the validation data set should re-produce the "true value"
within 95% confidence.
3.5.6.5 Validation of the extrapolation procedure should be performed for 50
statistically independent data sets and evaluated for a number of ship speeds,
relative wave headings and sea states.
3.5.6.6 A comparison should be made between the extrapolation and the "true value"
for each data set. The comparison should be considered successful if the
extrapolation confidence interval and the confidence interval of the "true value"
overlap.
3.5.6.7 The validation should be considered successful if at least 88% of individual
data set comparisons are successful.