Date Author Address
September 2005 Kapsenberg, G.K.
Delft University of Technology Ship Hydromechanics Laboratory
Mekelweg 2, 26282 CD Deift
TUDe Ift
Deift University of Technology
Page lof 1/1
Finding the hull form for given seakeeping
characteristics
by
Kapsenberg, G.K
Report No. 1457-P
2005
Presented at the 12th International Congress of the
mt. Maritime Association of the Mediterranean, IMAM, Lisboa, Portugal, ISBN: 0 415 39036 2
pROCEEDINGSOF THE i2 INTERNATIONAL CONGRESS OF ThE INTERNATIONAL MARITIME ASSOCIATION OF THEMEDITITERRANEAN (IMAM 2005), USBOA,
POAITUGAL, 26-30 SEPTEMBER 2005
Maritime Transportation and
Exploitation of Ocean and
Coastal Resources
Volume 1: Vessels for Maritime Transportation
C. Guedes Soares, Y. Garbatov & N... Fonseca
Instituto Superior Técnico, Lisbon PortugalTaylor & Francis
BALKEMA Proceedings and Monographs
Copyright © 2005 Taylor & Francis Group pic, London, UK
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ISBN (Set): 0 415 39036 2
ISBN volume 1:0415393736
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Maritime TmnsportationandEj loitation of Ocean and
GOataiResources - Guedes Soares. (3arbatov & Fonseca (ads)
© 2005 Taylor& Francis Group, Londòn, ISBN 0415390362
Table of Contents
Preface
XVII
Volume i - Vessels for Maritime Transportation
1.1
Hydmdynamics
Investigations on standards fox ship rnanoeuvring performance at slow speed inconstrained space 3
T Abramawicz-Geì'igk
Numerical study of the effects of hull shape and launching condilions on the behaviours
ofa free-fall' lifeboat:duringwater entry 9
M. Arai, Y Tsukioka,S. Tozawa & K Yamane
Simulationof a spring line applicatiónto enhance berthmgfunberthing manoeuvres 17
A Anyszuk
Numerical' assessment of operational behaviour ofhigh-speed, POD-driven large ships 27
ZAyaz O. Tumn&D. Vasralos
Largeainplitude slow motions of mooring systems 37
MM Bernitsss&.J.RL Matsuura
-Cost effective fiill!scaleobservation and recordingof propeller blade cavitation 53
N Bobánac, M Sambolèk, S RadU & I Beatovk
Weakly non-linear wave induced loads in thnedomain for high-speed miiltihuil vessels 61
D Bruzzone & R Gancia
Staggered Catamarans: experimental! data and feasibility study for environment friendly service 69
F Caprio A' Migali & C Peina
Second-order diffraction by asui-facepiercing truncated compound cylinder 77
1K cJzajigeorgiou& SA. Mavrakos
CEli analysis on the flyingshapeofmodern yacht sails 87
GE C1a1th&WIIeLen
Multi-body systems in waves - impact of hydrodynamiccoupliuigoninotions 95
G.FClaucs &K Jacobsen
Hydrodynaniiccoeflicients and;forces on catamarans inshallow water 107
N Dahcsi M Chagdali &A Hémon
Nonlinear waveresistance computations:asa dèsign tool inhull form improvement stUdies 113
DB. Danisman & O Gären
Sorne parainetersinfluencingthe accuracyof the wave pattern resistance!deteimination 121
N Deglull A Weiner &T Stasic
Numerical calculatiànof:ship's propulsiónmechanismofWeis-Fogh-type byvortex method 129
KD Ro H K Kang TN Kong & MII Kang
Effect of heel angle on global hull girder loads and ship motions
L. Foire & 1 ¡accarino
Experimental and numerical hydrodynamic coefficients of a conlainershipin
large amplitude heaving and pitching N Fonseca C Guedes Soares & A Morón
Catamaran wave resistance and central wave cuts for CFD validation
A S. Iglesias, R Zamora D Fernández & CL Pavón
Parametric study on relative wave height of ships in the rough sea
Y ¡noue NM Golam Zakaria & R Nakai.
Time domain computation of the wave making resistance of ships
F Kara
Computer simulation of interaction of tanker and offloading device
arranged at platform or single point mooring SL Karlinsky, VO Mrykin & MA Kuteynikov
On the ship maneuverability of tandem arrangement CRP pod propulsion system i Kayano T Haraguchi, l Tsukada & T Kano
Experimental verification ofan advanced deck wetness prediction method
R Kishev V Rakitin. V Chalakov & A. Maron
Manoeuvring characteristics of full-bodied ships with POD propulsion
L K KobylM ski & .1 Nowicld
Numerical simulation of low speed flows past under water vehicles
EA Korany, E H Atta B YBayoumi & MA. Korb
Some aspects of seakeeping of the floating body with attached pendulum
S Malenica IM Orozco & X-B. Chen
Hydrodynamic characteristics of two concentric surface - piercing floating
SA Mavrakas
Energy saving and dynamic stability of planning hull due to hydrodynamic
MA. Mosaad, MM Gaafa,y&IA Amin
A coupled third order model of roll parametric resonance MA S Never & CA. Rodriguez
Motion predictions and sea trials of roll stabiised frigate S. Ribeiro e S'uva, N Fonseca, R Pascoal & C Guedes Soares
Full-scale resistance study and analysis of a patrol boat at three different
hull/propeller roughness conditions
CM? Sampaio, AA Russo, K Nishimoto & K Hirata
A practical power prediction of an asyrmnetric catamaran hull form
R. Sampson, M At1ar A Mantouvalos. B Danisman & O Goren
A general expression of the internal friction in the boundary layer
C Simeone
An object-oriented manoeuvering simulation code for surface displacement ships
S Sutulo & C Guedes Soares
Computation of the resistance of a Series-60,Cli 0 6 model under a measured free-surfuce
G Tzabiras & D Ga,vfallidir
vi
circular cylinders
control of trim angles
137 265 273 283 287 295 147 157 167 179 185 189 195 199 207 215 221 229 243 255
Vortex shedding from a circulai cylinder at high Reynolds number 301
(10. Unal& O Gören
A study of the effect of steady flow on the unsteady motion of high-speed craft 309
NXie&D. Vacsalos
CF]) calculations on the sail-like three dimensional airfoils 317
i Yoo, ¡R Park i Kim. H A/rn & SR Van
Ship load model on large amplitude waves 327
A. Zamarin
HydrodynamiC experiments on a catamaran hull with a central bulb,
considering its resistance and seakeeping performances 337 ¡ Zatts!
1.2
Structures
Fatigue assessment of block joints on passenger ships and a proposal for
innovative technical solutions 347
G Bacicchi M Blot M Maestro, A Marinò &A. Toschetti
The use of artificial neural networks to reduce welding distortion 357
G.iBruce&MFLighfoot
Optimum design of composite ship panels 365
J
hinca, I Gawi!escu D. Boazu & EF BezneaSome considerations on global ship vibration analysis . 373
J Chirica, V Giuglea O Durnitriu & PR Pencu
Some considerations on the structura] modelling technique of double wan structures 379
A. Dimache, D. Olaru M Modiga & L Stoicescu
Experimental snidy of failure in pm-notched beams under transveise impact 387
D. M Dimas & C Guedes Soarer
Modal behaviour of a fÙll-scale deck panel with anti-noise treatments 395
A Ferrari&E Rizzuto
Fatigue strength assessment of fillet welds predominantly subjected to throat bending 405
WFricke A Kahl&H Paetzold
Effect of truck induced load on welded structural joints subjected to fatigue
Y Garbatov, ¡M Santos & C Quedes Soares
Fatigue damage assessment of a newly built FPSO hull 423 Y Garbatov, S Tomasevic & C Guedes Soares
Effect of the shape of localized imperfections on the coilpase strength of plates 429
C Quedes Soares, A R Teixeira, kM Luis, T Quesnel. Pf Nikolov, E Steen
JA Khan,
C Toderan CD Qlaìu A Bollero & M Taczala
Evaluation of nonlinear behavior for a typical stiffened plate panel to lateral load in ship structures 439
L Gusha
Some finite element estimates of ship collision event J Kajarte-Rudnitskj, R Varst.a & J Matusiak
Structural response of intact and damaged stiffened plated structure for ship structures
IA. KhanRK Das &YZheng
vn
413
447
Qualitative design assessment of crashworthy structures 461 A Kianac S Ehlers K Tabri S' Rudan & i Broekhujj.sen
Strength tests of steel sandwich pane) 471
L Kazak
Critical assessment of ultimate hull girder capacity of ships from a
reliability analysis point of view 477
T Moan, HKK Amlashi & G Dong
-Idealization of the plating complex initial deflections 487
RI Nikolov & A K Andree
A comparative study on the collision resistance of single and double side skin bulk carnets 497
O Ozguc RK Das & M Samuelides
Comparison of the 31F and JBP drafts with other class suIes 507
C M Rizzo & E Rizzuto
Fatigue strength assessment of a weld connection misalignment in LPG bilobe cargo tanks 521
S Rudan & I Senjanovh
Reinforcement of inipesfect biobe cargo tanks in liquefied gas carriers 527 I Senjanovth, S Rudan &A.M Ljuftina
Impact on single-skin marine composites 535
L S Sutherland & C Guedes Soarer
Corrosion behavior of shipbuilding high strength steel welds employing electrochemical methods 543
D Tsiourva. L i Dimarato.s. Di PantelEr & Vi Papazoglou
Rationalizing the design of ice strengthened side structures 549
G Wang R Basu,D Chavda&SLiu
Numerical methods solving dynamic finite element equations 559
IT Xìng
Powes flow analysis and applicationsfoEship vibration and control 569
YR Xion J T Xìng & WG Price
Superstructure deck effectiveness ofthe generic ship types - a concept designmethodology 579
Y Zanic .1 Andric & P Prebeg
Environmental factors affecting the time dependent corrosion wastage of marine structures 589
A Zayed Y Garbatov. C Guedes Soares & G Wang
Effects of hull defOrmations on ship displacement 599
K Ziha S. Goles A Radico & S Maksimovic
1 .3
Machinery and propulsion systems
Low emission propulsion plants for urban and coastal transportation 609
F Balsamo & F Quaranta
Interaction between ship propulsion plant automation and simulation 617.
G Benvenuto, G Cairem. M Figari & U Campora
Effects of fiel quality on two strokes slow speed diesel engines 627
G Benvenuto M Figari & CM Rizzo
Investigation in WHR-boìlez soot fires 635
Flow characteristics of air-caps for tank ventilation ra ships
SErgin
Hydrodynamicsadapration of pre-swirlstators to propellersof high speedmarine cram
MMGaafaiy
Reliability of ship machineryplants and damage chains R Häk/dnen
contra-rotating podded propulsorandits ñulscale model tests
X Kawana,ni, T Kijdo.& N Kawoshinia
Permanentniagnet electric motorsbased shippropulsion system K Kòroman D Linarii, R Milos
& B Rufoji
Development of multi-staged axial flow fans for caigoholds of container ships
S Lee, KS KimH-S Kirn&SH hun
Operational factors triggering off hazards for operatörsof\ship pOwer plants A. Podsiàdlo
Developmentyossibilities.of modern coal-fired marinepropulsionpiata
A testan & Z Parat
Machineryfunction factors triggeringoff hazards for operators of shippower plants W Tare/ko
1.4
Controlsystem
Fuzzy logicand model referenceadaptivecontrol of ship ro11stabilization using finactuatór
FAlarçin
Floating vessels control - mathematical modeling of thewaves
S Manduka
Research environment for motion control algorithms testing of scale ship models on a läke L.. Morawski. i Pomirski &A. Rak
Analysis of recursive neutral networksperformance trainedwith noisy manoeuvring data
L Moreira & C Guedes Soarer
Design of robuststeeringautopilot for ships L. Moreira & C Gueder Soarer
Isolation of theslainming-induced local vibration using fèedback control
M Mosieh &HS El-Kilarn
Roll-Yaw regulationusing stabilizing finsand rudder ¡na disturbance
observer based compensator scheme
R Parcoal, B Rodrigues & C Guedes Soares
The marine systems simulator state-space model representation for dynamically positioned surfacevessels
0 N Smogel4 T Ferez, TI Fassen & AL Sørensen
1.5
Veseldesign
Analysis of cargo offloading operations
ATRALho&RL.L Jij
Seakeeping metarnodeloffast ro-ro ships: RSM or ANNiechnique? 4 D A/kan, G Trincar & R Nabeigoj
763 771 643 651 661 669. 677 685 69] 699 705 715 721 727 733 .745 755 783 789
Design of an AFRAMAX tanker Baltic ice class i A acc to new SwedishFinnish
rules 2002 and model testing results - basic hydrodynamics problems 799
D Bezinovk
First evaluation of the design data for fast ferries 807
T Coppola & C Pensa
On the problem ofthe machinery choice and hull weight assessment
for the design of high-speed vessels 815
T Coppola A Paciolla & E Quaranta
Development ofa Mono-column type unit for harsh environment 823
A R Costa ¡Q Masetli M Cueva, K Nishimoto, G Machado & A Corte Design of the modern cargo ships of restricted navigation area to
Mediterranean and Black Sea region 831
G. V Egorov
Study of the intact stability of a Portuguese Nau from theearly XVII century 841 N Fonseca. TA Santos & 1? Castro
Multi-attribute design optimization of Adriatic catamaran ferry 851
i Grubisic & ¡ Munic
Application of genetic algorithm to s ucural optimisation of high speed craft 859
T Jastrzebsld & Z SelwLsJd
Finding the hull form for given seakeeping characteristics 867
GK Kapsenberg
Optimization and robust investigations in ship design 875 RN Kolev, TR Darn yanhiev & RG Georgiev
Evolution of LNG carrier design 883
.1 Romero & I Mosquera
Multi-objective optimization of fast ferry watertight subdivision 893
TA Santos & C. Guedes Soares
FPSO - Box Shape: A proposed tankers layout 901
¡M Vasconcellos
1.6
Shipyard technology maintenance and repair
Using throughput in approaching shipyard production process design 909
N Fafandjel M Hadjina, T Matuija & V Simone
Simulation foi criteria evaluation in shipbuilding production processlayout optimisation 915 N Fafandjel, D Pavletk & M Hadjina
Some aspects of complex production systems modelling 923
R. Iwañkowicz, .8 Metschkow, T Graczyk & T .Jastrzebsid
Development of underwater technology for maintenance of off-shore objects 929
S' Kra!j ZKo2uh&I Garafré
Production technology peculiarities of ships' body components from sheetproducts 935
VF Kvasnytskyy, VV Kvacnyts/cyy. G V Egoivv, Zh. G. Goloborod ko & Iii V Solonkhenko
rhe CAD system and its integration into the shipyard's integral IT system 941
M Milanovic, R Bencic & E. Yitasovic
Mapping the iIÏk)nnation flow through shiprepaii activities, 951
A. Sinha. K Ward & G Bruce
Photogrammetry in the shipbuilding production process 959 T Zaplatlé. .1 Kodvanf & B Ljubenkov
Author Index 965
Volume 2- Exploitation of Ocean and Coastal Resources
2.1
Maîine environment
On the levels of uncertainty in the estimation of extreme values
G Barbaro &MC Martino
Propagation of water waves through shearing currents in general bathymetry
KA Belibassoiric
High resolution wind modelling Mediterranean extremes
j Cateura, A Sanchez-Arcilla & R Bolaflos
A parabolic equation based on a rational quadratic approximation for surfhce gravity wave propagation followed in curvilinear orthogonal coordinates
M Chagdali & S Mordane
Bispectra and time-frequency spectra of wind waves in the coastal zone
Z Cherneva & C Guedes Soarer
Tests of wave shoaling and surf models in a partially enclosed basin
D.C. Conley&E Rusu
Does linear wave theory support freak waves
S Cosme & P Mónica
Influence of the distribution of the random wave heights on the longshore current velocity 1029
R Gentile & L R Landò
GIS based system to assess sea conditions along specified ship routes 1037
C Guedes Soares & MB. Pacheco
Robust Pareto optimal routing of ships utilizing ensemble weather forecasts
L Hinnenthal & O Saetra
Application of marine radar for real-time ocean wave monitoring R Hosoda, T Kojima, H Susaki, Y Hiraoka & Y Iwasald
lime and spatial variability of parameters of individual waves in a coastal zone 3 Kuznetsov, ¡ V Sapiykina & YS Yuresanrkaya
Formation of extreme storm waves on black sea
S Kuzneuov, I Sapryidna, K Kosyan & O. Purhkarev
A wave forecasting system developed for the Spanish harbors
MG L.alwz&jCCAlbjacJz
Bindcasting and forecasting the probability of freakwave occurrence L Lopaioukhin, A Boukhanovsky & C Gueder Soares
Impact of the upwelling on the sediinentology of the continental shelf of the Agadir Zone - Tarfaya
A Makaouz A OrbL A Agouzoulç ML Bouaamnzni & M Talbi
Filling gaps in wave records with artificial neural networks
O. Makarynsky, D Maka,ynçka E Rucu & A Gavirilov
Modeling wave propagation over a barred beach with the FUNWAVE model
./ Mil-Homens A A Pires-Silva & C.J Fortes
xl
971 981 991 999 1005 1015 1023 1045 1051 1061 1065 1069 1075 1081 1085 1093Estimation of directional wave spectra from measured ship responses 1103
UD. Nielren
On the stopping criterion to apply the Hubert Huang Transform method to sea wave records 1113
R Pascoal A D. Veitcheva & C Quedes Soares
Wave modeling for \'irtual Environments
i ia
A A. Russo C MR Sampalo & D Taniguchi
Computational strategies and visualisation techniques for the wave modelling
in the Portuguese neaxshore 1129
E Rusu, C. Ventura Soarer & L Rusu
Reanalysis of the wave conditions on the approaches to the Portuguese port of Sines 1137
L Rusu, R Pila, & C Quedes Soares
SOPRO - a software package for wave characteristics in ports 1143
LA Santos, CJE M Fortes, L Pinheiro & M G P/eves
Analysis of wave parameters in extreme wave records 1153
W Suiisz & M Paprota
Reliability of SWAN model simulations for the Black Sea Romanian coast 1159
C VTrusca
Survey of techniques for real-time visualization of the ocean surface 1167
AM Varela & C Quedes Soares
Modelling of the effect of the continental shelf on the marine circulation 1175
M Zarn M Bouammrani M Gowvhane & M Chagdali
2.2
Fïsheies and aquaculture
Preference communication in multiattribute procedures for optirnised ship design 1181
M Bamne E Begovic, C Bertorello &.M Stella
Response from current and regnlar/iiregjilar waves on a typical polyethylene fish farm 1189
A.Berstad&HTronszad
.Safety of fishermen: risk factor analysis and the influence of vessel nautical properties ¡197 G Boccadwno & A Scamardella
A mathematical model for the dynamics of the towed depressor used in the trolling fishery 1205
K Ebata, S Fuwa H Sano T Hirai;hi &K Yamainoto
Flow characterization around a cod-end 1211
G Germain, 1-VFacq &D Fnou,
Improvement of the "Soft Door", a newly developed mouth opening device for trawls
considering hydraulic dynamics 1217
M Ishizaki, Y ¡noue A. Habano, K Ebata. T Hiraishi & T Kumazawa
Precautionary approach in Baltic herring trawl fishery: the effect of hauling techniques and
engine power on unaccounted mortality estimates 1223
A. íd, vik, T Raid, H Shpilev, L .Jöjv&A L.ankov
The influence of the Albanian sea winds on fishing-boat stability of PV 2KP-400 type 1231
KN Lzpa&KI Ibrahimi
Computation modeling of the moored flexible structures 1239
C W. Lee, HS Kim GH Lee. KY Koo, M 1 Choe, B .L Cha & S. J Jeong
Design and performance of a software based fishing simulator 1245
CWLee MWLeeGHLeKYKoo&MYChoe
A multi-criteria stern trawler selection model using the analytic hierarchy process 1251
HWLeJzeta
Numerical study of the flows incod-ends
D. Marichai&G Massart
New net cage designs to prevent tearing during handliñg 1265
H Moe A Fredhei,n& MA Heide
A source panel modeFof plànktonsarnplér hydrodynamics 1273
FG O'Neill
A quickcstimation ofseakeepiñgchaiacteristics on fishing vessels 1279
F Pérez-Arribas, R Zamora, L Pérez-Rojas &.L Freiria
FEM modeling offlexiblestructures mal eofçables1 barsandnets 1285
D. Pria ur
BendingstifThessof a clamps-connected 2-rings PE fish cage collar 1293 K Vi'kestad & E LIen
23 Maritime transportation and port operation
Benchurarking analysis öf European ports and terminaIs
.p:Ant5o, C GuedesSoare&A Gerretzen
Economic operational studyofthe stockyad andshipment of Ubu Port RC Botter.'Á S. Siquei,a L.R Castro Neto & WR A. Ceciliano On thedevelopment:of new mooring supportsystem
S Hara K Hoshino H Kawashuna T ¡Cano K Tanizawa M Nakamunz H Kaflwwu M Manabe H Saiki & K Ohnô
The Ba ceuroegionstzutegieson1eve1opment of'short seashipping
J Kubiki
An innovative dynamic tanker freight rate index D,k'.Lyridis, RG Zacharìoudakis.& D. Chalzovouio.s
A dynamicregional forastof tanker freight.rates withtheusageof ana1yticaltechniques
DV Lyridis RG Zachar.ioudakis & T Paviidis Sùnulation of container terminal's operations
J Marchai & Z Zhang
Theoretical grounds to evaluate quality of the transport system operation L. Mtdlewski&.M Wompay
An analysis of the European Union porispolicy
NPsarafiis
SustainabIedeveJopmeot of the Port of Lisbon
AC Reis Cunha
R.ole.ofL.NG in Mediterranean, region. New fleet required , 1385
.1 Romero
Model for selecting container yard equipment and stacking formation strategies in container terminals
G.S deSá Peixoto& .RC Botter
Navigation Chaiacteiisticsof the Danube and its influence on the
main dimensions of the river-seashi,s
VSldiljaica & T Baclralié
1259 1303 1311. 1319 1327 1333, 1343 1351 1361 1371 1377 1395 1401
2.4
Coastal and offihore development
Monitoring of the Bulgarian Black Sea beaches 1411
VZ Dachev E V7)fonova & MK S:ancheva
Expanding urban development using floating infrastructures 1417
PB González 4. Alvarez, A. Salamanca & B Alvarez
A study of the effect of an underwater mound on the hydrodynamic
performance of onshore wave-power device 1423
F Gouaud V Rey, R van ¿fooff L Piazzola & G. Tedeschi
Pipeline installed by free immersion in the Black Sea offshore areas 1431
IC Matulea,i Strat&E Rusu
Modelling the effect of wave-current interaction on the sediment transport 1439 L Mouakkir. S Mordane, M Chagdali & H Smaoui
On the feasibility of installing SCR's by the reel-lay method . 1447
TA Netto A Bollo MI Lourenço & R Quaranta
A particle-tracking model of spreading of fine sand sediments 1455
VPenchev, B Savov & Z Theocisaric
Wave energy for oil and gas offshore application 1463
E Ricane M M Pinheiro PR Costa & SF Esrefen
Leirosa sand dunes: a case study on coastal protection 1469
C Schreck Reis. H Freiras & .1 Antunes do Carino
A conceptual design and fünctional assessment of the foaling
container terminal with high activities 1475
T Shinoda N Fukuchi & H Kim
2.5
Safety and neliability
Reliability of port transportation systems related tO their operation processes A Blo!ws. K Kolowrocki & .1 Soszynska
Sensitivity analysis of search area determination mathematical model Z Bureiu
SAFEDOR - risk-based ship design, operation and regulation
¡f Christensen, W Hensel AR de Lucas, PC Saines, R Skjong, T Strang & D Vassales
Hazard identification & risk ranking of AFRAIvIAX tankers by expert judgement
S Delautre S A/au, C Tuzcu N Mikelis & A Papanikolaou
A safety assessment for marine accidents considering mental
stress based on measuring heart sate variability N Fukuchi & T Shinoda
Challenges of modern assessment of safety of ships in critical conditions Options for preliminary design
M Gerigk
Selected problems and methods of navigational risk assessment
L Gucma & Z Smalko
Specific features of the reliability maintenance of lashings of the deck heavy-weight cargoes and bulk cargoes in flexible containers
VV Kozlyakov, IR Davydov & A. V Stas.ytsky
1487 1497 1503 1511 1521 1529 1537 1547
The SIFBITP tools for the assessment of passenger's behaviour in emergency situations
4 López-Pineiìv. EPérezA IC. Diaz C & VGonzále.zS
Improving formal safety assessment in shipping transportation
E. Mennic IN Lagoudis N Nikitakas &A Platis
Systematic analysis and review of AFRA.MAX tankers incidents
4. Papanikolaou E Eliopoulou A. Alicrafaki, S Ak.su, S. Delautre & N Mi/cells Risk-based approach to the design of passenger ro-ro ships regarding damaged stability TA. Santos & C: Gued Soares
Risk evaluation of life rafts in operation conditions
L S,nolarek
Assessment of partial safety factors for the longitudinal strength of tankers 1601 4. P Teixeira & C. Guedes Soarer
Reliability based approach to determine the design loads for the remaining lifetime of ship hulls 1611 A.P Teixeira.. C Guedes Soares & G Wang
Energising safety management in ports 1621
VM Trbojevic
Risk ciiteria foi ports and ships 1629
VM 7}'bojevic
Fundamental concepts of risk-based ship design 1637 D Vas.ralos D Konoves.szs & L Guarin
The navigational width for a vessel going on the trajectory in shallow water under wind and wave 1645 YL. Vorobyov & M B Kosoy
Modification of the chart presented in ECDIS 1653
A. Weintrit
Presentation of safety contours on electronic navigational charts 1659 A Weintrit
Minimum reliability index of the weak points ofvariably curved beam elements under pure flexure 1667
X
WAn &H LiReliability analysis ofceniral compression of an imperfect strut with
initial geometrical deformations 1673
XWuWAn&ZLI
A benchmark study on response surface method 1679
X Zheng RK Das, L.. Mi & B. Leira
2 6 Deignfo the protection of the environment
Oil spills in coastal zones: environmental impacts and practical mitigating solutions
.15 Antunes de Carmo. IL Pinho & IR Vieira
Diesel oil degradation in sea water
C Bilgin&Eyonsel
SOS - integration of a seaway independent oil skimming system into an oil recovery vessel
G.E C/ausc MA Amro & S Kosleck
BaUasting with Fresh Water to be interchanged on the harbours RB. González A. Alvarez A Salamanca & B Alvarez
Evaluation of the emissions from the super eco-ship and the corresponding conventional ship X Minamj & T Kuno
xv
1555 1565 1573 1583 1593 1689 1697 1703 1713 1721System integration fo safety and effective operation of the superEco-Ship 1729
M Numano, T Kano, H Kin'arhinw & T Taidmoto
Black sea water pollution .1733
M Pana yotova Y Garbatov & C Quedes Soarer
Water and air pollution caused by maritime activities 1737
M Panayotova. Y Garbatov & C Guedes Soares
Life cycle assessment of ships 1751
MA. Shama
Design optimisation and test of TREBAWA system an onboard treatment of ballast water 1759
P Zhou T Leigh.. F Asian & K Hesse
MaritimeTransportatiöñ andExploitation of Ocean and
Coastal Resources - Guedes Soares,
Garbatov & Fonseca (ads) 2005 Taylor & Francis Group, London, ISBN 0415390362Preface
These two volumes present the proceedings from the 11th International Maritime Association of the
Meditesranean Congress held in Lisbon, Portugal, from 26 to 30 September 2005, under the theme Maritime Transportation and Exploitation ofOceanand Coastal Resources
The International Congress of International Maritime Association of the Mediterranean has nearly 27-year
history smce the first Congress of the International Mantune Association of East Mediterranean (IMAEM)
held in Istanbul in 1978 It isa voluntary organization that was initiallyestablishedin 1974 by institutions from six countries (Bulgaria, Egypt, Greece, italy, Yugoslavia and Turkey), and was progressively enlargedto other
countriesneighbouringthe Mediterranean
The IMAEM Congresses were held every 3 years:
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Finding the hull form for given seakeeping. characteristics
G.K. Kapsenberg
MARIN, Wageningen, the NetherlandÑ
ABSTRACT This paper presents a method to find a hull form that satisfies as good as possible a set of
seakeeping requirements. The method uses an initial hull form that is characterized by a set of polynomials
that define the beam on the waterline, the draft and the sectional area as a function of the length. The sectional
shape is then defined by a 2 parameter Lewis transform Limits can be supplied to the parameters describing
the hull form The hull form is changed by changing the driving parameters that define the polynomials The
seakeeping behaviour is calculated using a linear strip theory program. An optimization method is used to
find the hull' form that approaches the seakeeping requirements as good as possible.
The method is applied to the design of a frigate. The required seakeeping characteristics are vertical
accel-erations that are half those of the original design The intermediate steps are shown and' the final hull shape is
presented.
I
INTRODUCTION
Optimizing hull forms to achieve certain objectives
is now a well developed branch in science. In the
early days this. work was restricted to a number of
design variants that were tank-tested to have
mini-mum resistance or minimini-mum required power. Today
this type of optimization is usually carried out using
potential flow solvers; the geometry changes are
or-ganized by special software that controls the local
hull shape. An example of this work is the
optimiza-tion of the bulbous bow design (Hoekstra et al.
2003); in most cases the method is tuned to
optimi-zation in the advanced design stage where only
small changes are possible; nevertheless important
reductions of the wave making resistance are then
still possible. In the near future this type of
optimi-zation can be done using RANSE solvers instead of
potential flow solvers.
From the seakeeping point of view, these minor
modifications of the hull form are irrelevant the
seakeeping characteristics of the ship will hardly
change. Seakeeping behaviour is governed by the
overall hull form rather than local details. Apart of
this, relatively little is known about what makes a
ship a good sea keeper. Original work was carried
Out by Bales (1980); this was later extended 'by
Wal-den (1983). Bothauthors used aseries of strip theory
calculations and a choice of seakeeping
require-ments to develop a seakeeping index. This index was
then related to hull form parameters by regression
analysis. Systematic calculatiOns and experiments
were carried out (Blok et al. 1984); the good
quali-ties of the best hull form were allocated to the large
longitudinal separation between the centre of
buoy-ancy and the centre of floatatión of the waterline.
Lloyd (1988) presented results of calculations that
showed beneficial effects of wide beam 'and shallow
draft. The results from Blok et al. were later
ana-lyzed as resulting from maximizing the water plane'
area coefficient (Kapsenberg et al.
1998). Funny
enough this same publication came up with a design
with a very low water plane area coefficient as an
optimum fOr the given seakeeping requirements.
The method in this paper
iscomparable to
Lloyd's method (1988) The idea is to characterize
the hull in a limited number of parameters that fix
the seakeeping behaviour. Since 'good' seakeeping
characteristics are dependent on the tasks the ship
has to perform, general advice on what makes a
ships hull a good seakeeping one is replaced by
di-rect calculàtions with specific criteria. The
paramet-ric description of the hull form uses no a-priori
knowledge; the hull form generation process is
or-ganized such that also rather strange hull forms can
result. The idea behind this is to determine first what
is possible and then to restrict oneself to more 'ship
like shapes' and to détermine höw much of the good
seakeeping qualities are to be sacrificed. Such a
sec-ond stage is also the moment to realize that a linear
seakeeping prediction is quite limited and that also
considerations like emergence of the bow and
slam-ming on re-entry must be considered, This second
stage is not covered in this paper.
2 THE CONCEPT
The basis idea of this development was that
seakeep-ing characteristics. oía ship are determined by the
gross overall hull shape. This means that a rough
de-scription of the ship is sufficient, and that relatively
minor modifications can be made later (to improve
powering or manoeuvring characteristics) without
changing the seakeeping behaviour.. A second
start-ing point was the desire to know the required shape
regardless of all the other design constraints and
subjective criteria related to a 'good ship' or 'current
best practice'.
The choice was made to describe ship sections
with tWo parameter Lewis transform. This requires
only a description of the design waterline, the draft
and the sectional area as a function of the length to
have a full 3D description of the hull form. The
beam, draft an sectional area as a function of length
are each described by two 3.order polynomials; one
for the forward end and one for the aft end. These
polynomials are connected to a possible parallel mid
body.. This results in a set of 21. parameters for a
complete hull form definition and would thus result
in a 21 dimensional design space.
The original idea was that these 21 parameters
would be totally independent, but this proved to be
impossible. One of the additional constraints that
were put in, was to keep the displaced volume
con-stant. This results. in a strong interaction of the
pa-rameters describing the SAC. Next to this
it
ap-peared to be necessary to have some interaction
between the parameters controlling the polynomials
for the beam and draft to keep section shapes within
the limits imposed by the Lewis transforms. The
length between perpendiculars and the displaced
volume is kept constant throughoutthis optimization
process.
3 NOMENCLATURE
A [m2] B [m] [m]T
[m]
H0 [-1NAA [-j
NAF[-]
o.[]
V
[mi]
Sectional area
Sectional beam at the waterline
Length between perpendiculars
Sectional draft
Half beam to draft ratio, H0 = B/(2 T)
Station number aft where constant pail
of sectional area curve begins
Station number forward where constant
part of sectional areacurve ends
Sectional area coefficient, a = A/(BT)
Displaced volume
4 HULL FORM DEFINITION
The program uses a mathematical 'hull form
descrip-tion based on polynomials describing the secdescrip-tional
beam, draft and area. These polynomials are defined
by the values at the outer ends (at St O and' I or St 19
and 20 respectively) and at the location of their
maximum value with a zero longitudinal derivative
The hull form can either have or not a parallel mid
body. Initial testing of the software and the hull
forms it produced showed that better shapes' were
obtained using a description by polynomials of the
local beam to draft ratio HO and the sectional area
coefficient o- rather than the local beam and draft.
The polynomials define values for the beam, draft
and area for each of the 20 stations, the shape of the
sections :i5 defined by Lewis transforms and this hull
form is transferred to the seakeeping program.
The seakeeping calculations require some
addi-tional data: the' longitudinal position of the centre of
gravity LcG. and the pitch inertia Iyy. The
assump-tion is made that LcG is always the same as LcB and
the radius of gyration for pitch is assumed to be 0.25
Lpp; this results inI =(O25L) pV.
The method gives a good approximation of
nor-mal hull forms; this is illustrated in Figure 1 which
shows the body plan of a standard frigate hull form
and the form described by the software using the
polynomials and' the Lewis forms Certainly the
mo-tion characteristics of the hull form are well
charac-terized by this approximate method.
Figure 1 Actual hull shape of the frigate(top) and approxima-tion using Lewis forms;
5 LEWIS TRANSFORMS
The 'hull form is defined by a 2 parameter conformal
semi-circle. This so-called Lewis-transform is
de-fined by:
z
nO
This formula transforms a circle in the Ç -plane
with polar coordinates into a ship-like section in the
Z -plane with Cartesian coordinates. The formula
describes ship-like sections reasonably well, but at
extreme values of the parameters re-entry forms can
result. Therefore the following limits to the
coeffi-cients were used:
0.04 <HO <50.0
For HO 1,
c_up
=1.11735+0.0370/HO
tTLOW = 0.5843 5 - 0.2882*H0
(2)
Figure 3
YZ plot of possible section shapes using Lewis
transforms. B/(2.T) = 1, 0.30< c_< 1.10.Initiator
Other parameters that are changed; sign
is indicated in brackets
AO (+) AM (-) A19 (-) NAA (-) NAF (-)
Al (+) AM (-) A19 (-) NAA (-) NAF(-)
AM (+) Al (-)
A19 -)
NAA (+) NAF -)A19(+
5
AM (-)A20 +) AM (-)
NAA (+)
A19 +)
NAF (+)NAF (+)
Al -)
Al 9 -)
For HO> 1,
= 1.12435+0.0300*H0
with a maximum o,,, = 1.4
GLOW = 0.59565 - 0.2995/HO
(3)
This area where Lewis transforms of ship sections
is applicable is indicated in Figure 2; Figure 3
illus-trates that this allows a wide range of section shapes.
6 CHANGING THE HULL FORM
The basic idea was that the hull form could be
changed by changing any of the 21 parameters
inde-pendently. This proved to give undesirable hull
forms in the case that a value at one of the outer
ends was changed. Due to the choice of the 3rd order
polynomial this could resulted in extreme
'over-shoots' of the beam, draft or area curves. This
prob-lem was solved by creating a weak link between the
values of the parameters at the ends: if the value at
the ends is changed, the value of the same parameter
at the neighbouring section is also changed in the
same direction. The step size of this secondary
change is 60% of the step size of the primary
change. After including this, it appeared to be
possi-ble to change the hull form quite radically.
7 CONSTRAINTS
The constraints already listed are those imposed by
the
Lewis
transforms
and
those
imposed on
neighbouring sections
to
keep
reasonable
hull
shapes. Extreme values of the input parameters are
also supplied as a constraint on the design space.
Next to this it was decided to keep the length and
the displaced volume constant. This second
require-ment needs some attention because it is allowed to
change the Sectional Area Curve (SAC). If one of
the 7 parameters describing the SAC is changed, 4
other parameters are also changed according to
Ta-ble 2. The taTa-ble indicates (on the first line) that, if
the area at St O is increased, the area midships and at
St 19 is reduced, and that the parallel midbody is
shifted aft by reducing NAA and NAF. Changes are
made in an iterative procedure that converges to the
initial displaced volume.
0.01 0.1 10 100
H0 = BI(2.T)
Figure 2 Area (indicated in green) for Lewis transforms that
gives ship-like sections.
8 THE DESIGN SPACE
An initial investigation of the design space is
re-quired for the development of the optimization
tech-nique. Special care has to be taken if there are many
local extremes. Calculations were made changing
the beam-draft ratio and the sectional
area
coeffi-cient midships. The result is shown in Figure 4. The
colour indicates the error calculated on the actual
vertical acceleration level and the
required level.
The figure shows that the design
space
is very
smooth and that there are no local minima.
Figure 4 The design space illustrated by changing the beam drafi ratio and the area coefficient mid ships. The colour indi-cates the level of the error fijnction for the design objective (minimum acceleration).
9 THE ERROR FUNCTION
The error function to minimize in the first
example
is the vertical acceleration
on 3 locations: St 0, 10
and 20. The acceleration on the 3 locations is
mini-mized with equal weight; the actual error function is
calculated as the square root of the sum of the
squares of the error on each location.
As a second example the relative motion
at the
forward perpendicular is chosen as the error
func-tion.
10 THE OPTIMIZATION METHOD
The optimization method that is used
to minimize
the error function is based
on a successive local
search and steepest descend method.
The 'Local Search' routine changes each
of the
21 parameters individually, changes possible
de-pendent parameters, checks if the hull form is
feasi-ble (within constraints of Lewis forms)
and
calcu-lates the seakeeping characteristics. If
one of the
checks has a negative result, the variation is not
in-cluded. The parameter that gives the largest
reduc-tion of the error is then selected for the 'Descend'
step of the program.
The 'Descend' step finds the maximum
reduction
that can be achieved by changing just
one parameter.
Regardless of the success of the 'Descend' step, the
program continues with a new 'Local Search'.
If the 'Local Search' routine is unable
to find an
error that is smaller than the actual
error, the step
size is decreased and a new 'Local Search' is carried
out. The reduction of the step size results in
a
con-vergence criterion; in order to check for local
min-ima, a final check on the converged design is carried
out with an increasing step size.
This optimization method is not very advanced,
but it proved to be a robust method and suitable for
the present problem.
11
TI-lE SEAKEEPING PROGRAM
The seakeeping program embedded in the software
is a strip theory program with forward speed
correc-tions as developed by DeIft University of
Technol-ogy (Gerritsma et al. 1967). This method has been
used for many years and gives surprisingly good
re-suits for many hull forms, an application for very
fast ships is presented by Blok (Blok
et al. 1984).
Such a method is extremely fast
on present day
PC's, the performance is about 1000
calculations (1
speed, I wave direction, 15 frequencies) for
different
hull forms in 1 minute.
12 EXAMPLE MINIMUM VERTICAL
ACCELERATIONS
As an example an optimization is carried out for a
frigate. The starting point is
a hull form that has
been used in seakeeping optimization studies before
(Kapsenberg et al. 1998), see Figure 1 bottom. The
objective was to minimize the vertical
accelerations
on 3 locations: St 0, 10 and 20 to the minimum (the
target was set at 0). The ship is sailing at a speed of
18 kts in a head sea characterized by
a JONS WAP
spectrum with a peakedness parameter y = 3.3 and a
zero up-crossing period T2 = 7.5 s.
An optimum is achieved after 80 iteration
steps
which includes 2165 times a strip theory calculation.
The error reduces quite quickly in the first 15
steps;
Figure 9, the hull form changes and the
error
reduc-tions are quite small after this point. The initial
steps
to reduce the draft forward. This intermediate result
is shown in Figure 5. The vertical accelération is
mostly reduced at St 20
(37%relative to the value
for the starting point). For the locations St 10 and 0
this is 22% and
13%respectively.
After 15 iterations much more of the hull form is
changed, see Figure 6.. The Sectional area CUrve is
much flatter resulting in a very high prismatic
coef-ficient. The beam is increased over the full length
-5
50 CN E 50 E CD o 10 15 20and the draft is reduced. These dramatic changes iñ
the hull shape result in reductións of thé vertical
ac-öeleration that are 50%, 46% and 52% respectively
fOr st 0, 10 and 20.
If we consider the seakeeping characteristics in
more detail, it shows that the largest reduction is due
to a lower pitch motion. This is illustrated by the
plots of the RAO's, see Figure 10 and Figure ii.
O
i
0.5 0.5_5.
-15
-10
Bodyplan 50 E rD o iO 15 20 o E I-10 15 80 40 IterationFigure 6 Resulting hull form (in red) after 15 iterations for minimized vertical accelerations. Thebeam draft and SAC of the start-ing point is given in blue.
80 0. o O 10 CN
-5
IO 15 20 50 10 15 20 St 0 . o 0 5 iO 15 20 0 20 40 60 St IterationFigure5 Result after 7 iterations. The new hull form isindicated in red in the beam, draft and vertical acceleration plots; the hull... form of thestarting point is indicated in red. The body plan is that of the new hull form.
Bodyplan
E o E
I--5
50 CS' E o Figure 720/
E;
N E 50 O 50 O 10 15 20 10 15 20st
Final hull form for minimized vertical accelerations.
0.6
:::
Figure 9 Error as a fbnction of the iteration step.
Bodyplan
o
0 10 15
Iteration
13 EXAMPLE MINIMUM RELATIVE
MOTIONS
The same hull form as used in the previous
ex-ample has been chosen as a starting point. The
er-ror function chosen now is to minimize the relative
motions at the bow. In this case it appeared to be
possible to reduce the error with 39%. The final
hull form is shown in Figure 8. The hull form
shows a SAC (and Centre of Buoyancy) that is
shifted aft, while the beam of the waterline forward
is increased. This results in very hollow sections
forward and very wide sections aft. The resulting
-e
a
o 10 15 20 10 15 20 o w I a 10 15 20z 0.5
o
o 20 40 60 80 Iteration Bodyplan 20 25 10 15 20 15 20 o 5 10st
Figure 8 Final hull form for minimized relative motionsat the bow.
80 100 o 0 20 40 60 Iteration 1 0.5 w
RAU of the relative motion at the bow is compared
to the same for the starting hull form in Figure 12.
14 CONCLUSIONS
Whether or not the final result of the example
calculation is a practical hull form, is not the issue
of this paper. The idea is that the software shows in
rigorous and objective way the direction to
im-proved seakeeping of ships. Rather than very
gen-1.5
z
05
0
-540 0 0.5 115
0.10o
0.05 a. 0.00i MF I RAO e-- MF-fin RAO
4--MF-1 phase o--MF-fin phase
wave frequency (radis]
Figure 10 Heave RAO and phase angle of the hull form at the start of the optimization (MF-l) and at the end of the
procedure (MF-final).
i--- MF-1 RAO
e-- MF-fin RAO
.+--MF-1 phase e--MF-fin phase
180 o fin w -180 -270 o--360 180 90 OE -90 -18Oe
a--270 -360 -450 540Figure II Pitch RAO and' phase angle of the hull form at the start of the optimization (MF-1) and at the end of the pro-cedure (MF-final).
eral trends that are pointed out by studies using
systematic series, this method uses the existing
hull form and some - user defined - room in the
design parameters to find a better hull shape. Next
to this the actual seakeeping requirements are
di-rectly used'. The final
hull
form is dependent on the
requirement that is used in the optimization.
Ex-amples are given showing the minimization of the
vertical accelerations and the minimization of the
relative motions at the bow. Both requirements
re-suit in different hull forms as illustrated in graphs
and by the values of the main hull form parameters
as given in Table 1. This table shows that
minimiz-ing the vertical accelerations is achieved by
shift-ing both centre of floatatión and centre of
buoy-ancy forward (keeping the separation the same),
lowering block and vertical prismatic coefficients
and increasing prismatic and water plane
coeffi-cients. These results are mainly in line with those
from Lloyd (1988).
Optimizing the ship towards reduced relative
motions at the bow is achieved by shifting both
centre of floatation and centre of buoyancy aft
(also reducing the separation between the two),
lowering block and water plane coefficients and
increasing the vertical prismatic prismatic coeffi
cient. Noted is that the values of the coefficients
are dominated by the choice to base them on the
maximum values of the relevant parameters.
A warning is given to the user: never fully trust
the results from computer programs. Even if the
code has been written free of bugs, there are
as-sumptions made in the theory; it is a model of the
real world, not the real world itself in this case it
must be realized that the 'heart' of the software is a
linear seakeeping program. The results must be
used as an indication of the directión in which to
change a hull form. It is quite obvious that the final
- Sta rtingpoint
-
Final hullformFigure 12 Relative motion at the bow of the hull form at the start of the optimization and the result for the final hull
form.
0 0.5
i
1.5 O 0.5i
1.5hull forms that are presented in this paper with
their shallow draft will not be good seagoing ships;
for instance the hull will be prone to severe
slam-ming in rather low waves.
The main use of the method presented in this
paper is - as we see it - two fold: By doing an
op-timization with a large design space, one gets an
idea of the main features of a hull form that is
op-timized with respect to seakeeping only. These
re-sults can be used in an early design phase. The
second way of using the method is in the advanced
design phase when the freedom to changes the hull
form is limited. The method can then indicate the
most effective change in the hull form to further
improve seakeeping.
Table I Main hull form parameters of starting point and the two optimized hull forms. Coefficients are based on maxima for beam and-draft.