
542
5 Ankundinova(newmethodthatiswellverifiedin
realityandthatallowstocalculatethesquattingat
thebowandatthestern).
To calculate the final reserve for squatting ∆
8,
averagevaluesforsquattingwereappliedintheform
of:
5
1
88
5/
i
(3)
where:∆
i – values calculated through eachof the 5
modelsofsquatting.
The Huuska method overstates the value of
squatting as compared to other methods. According
to Briggs [13], the Huuska/Guliev squat method can
beusedforallthreechanneltypesanditisdefinedas:
2
2
2
1
nh
bs
pp
nh
F
D
SC K
L
F
(4)
– the squat constant, is typically used
as an average value, although Hooft (1974) had
originally used
(values from 1.9 to 2.03
wereusedattimes)
D–shipdisplacement
2.5 Modeloftheinfluenceofwavesonthebowmovement
In analysing a ship’s response (rolling) to waves, a
linear model of dynamics in 6 stages of free
movement is commonly applied, as well as the
stochastic nature of the process of waves, described
withthe function oftheso‐called spectraldensityof
thewaveenergy.
From the perspective of decreasing under keel
clearance, only 3 elementary movements are crucial:
one linear (vertical) movement and two angle
movements. These are, respectively: heave, roll and
pitch.Their
amplitudecharacteristics,calledresponse
amplitude operators (RAOs), present a ship’s
responsetotheharmonicwaveofagivenamplitude
andheight,i.e.amplitudeofavessel’srollingandits
shiftwithrespecttothewaveitself.Sixfunctionshave
beengivenascalardefinition,i.e.theamplitudeand
phasecharacteristics
foreachofthethreeenumerated
componentmovements.
Inorder todescribeaship’smovement,a mobile
(linked to the ship) clockwise system of coordinates
(Figure4)wasappliedandcriticalpointsresponsible
for UKC reduction were determined where
movements (vertical displacements) are finally
defined.Theyarethecornersofa
rectangleplacedon
the surface of the keel of the L (length between
perpendicular) and B (length all over) dimensions,
stretchedbetweenperpendicularandtheship’ssides.
Numbers and horizontal coordinates (xʹ
UKC,yʹUKC) of
criticalpointsarethefollowing:
portside starboardside
ʺ‐1ʺ‐bow
2
,
2
BL
ʺ+1ʺ‐bow
2
,
2
BL
ʺ‐2ʺ‐stern
2
,
2
BL
ʺ+2ʺ‐stern
2
,
2
BL
Amplitudecharacteristicsofelementaryrollingare
usually determined directly in the system linked to
theship’scentreofgravity–seethesystemGx
SKySKzSK
inFigure4.FortheneedsoftheUKCforecastsystem
created, condensed functions of 4 arguments were
used:waveamplitude,wavedirectionwithrespectto
theship(intheʺwheretoʺconvention),ship’sspeed,
depth of the basin determined based on the
commercial SEAWAY software [Journee, 2001;
Journee/Adegeest,2003].
TheverticalrollingofthecriticalpointzUKC,andtothe
sameextentthedecreasingUKC,foraregularwaveis
finallydefinedwiththefollowingequation:
UKC G UKC G UKC
z t z t t y' t x' x'
(5)
whereallthevaluesareexpressedinthemobileOxyz
inertial system temporarily stopped on the level of
calmwater,whereasʺprimedʺvaluesasstifflylinked
toOxyzareconstant:
z
UKC – vertical displacement (rolling) of the critical
pointintheOxyzsystem[m];
z
G– vertical displacement (rolling) of the centre of
gravityG[m];
– heelingangle(ofrolling)[rad];
– trimmingangle(ofpitch)[rad];
t – time[s],
xʹ
G – longitudinalcoordinateofthe positionofthe
ship’scentre of gravity intheOxyzsystem resulting
fromitsweightlayout[m];
xʹ
UKC,yʹUKC – longitudinal and crosswise
coordinateofthepositionofaselectedcriticalpointin
theOxyz[m]systemresultingfrom thedefinition as
above.
Theabovecalculations have to be carried out for
eachofthefourcriticalpoints.
Determining the basic parameter for defining
statistical parameters of rolling means
determining
theintegraloftherollingspectrewithrespecttothe
waveamplitudeasavariationofstochastic(random)
processofrollingortheso‐calledzeromomentofthe
spectre,markedasm
0zUKC.Oneofthembasedonthe
above‐mentioned Rayleigh’s layout is the amplitude
of rolling z
UKC0‐p%, which can be overstated with the
probabilityofp
%runbytheoperator/decision‐maker
(see [Dudziak, 1998], [Journee/Adegeest, 2003],
[PIANC,2014]amongothers):