FULL SCALE MEASUREMENT OF A LARGE CONTAINER
CARRIER ON THE FAR EAST
-
EUROPE ROUTE
H. C. Yu (AM), J. W. Choi (V), C. I. Park (V), S. Y. Han (V), S. C. Taj (V)
SMTC-074-2008
There is limited long term service experience with the modern generation of large container carriers and hence there is great interest in improving our understanding of the performance of these vessels. In an effort to assess the actual structural service performance of a large container carrier, a comprehensive full-scale measurement system was
developed to measure the wave environment, ship motions and structural response. The system was installed on an 8063 TEU container carrier built in 2006, and t he first year measurement campaign has successfully been completed
This paper presents a summary of noteworthy observations during the first year 's voyage records which includes ship motion, wind and wave conditions, and hull girder strains and derived hull girder bending and torsional moments.
The observed vibratory responses of the hull girder are also presented.
KEY WORDS: Full scale measurement, container carrier,
hull stress monitoring, onboard wave measurement
INTRODUCTION
The benefits of the full-scale measurement are once again
relevant as the recent growth in size of modern container
carriers has been very rapid. This has created challenges for the container shipping industry including the operators,
designers, builders and classification societies. The recent
trend in design and construction of large container carriers and
technical approaches taken by ABS has been presented in
recent publications [1] [2] [3].
The limitations of the
traditional classification rules criteria and linear seakeeping analysis were addressed, such as sag-hog wave moments, wave-induced shear force and torsional moment, and load
combination. These papers also presented the way in which the
nonlinear seakeeping program may be applied to overcome
these limitations.
Yu
The operators of modern large container carriers are also
concerned about the safety and performance of these vessels since they do not have a lot of experience with these ships.
The hull stress monitoring system is gaining popularity among
ship operators in order to provide assistance to the crew for better handling of difficult situations. For example, Orient Overseas Container Lines (00CL) has equipped all vessels of
Samsung Heavy Industries (SHI) built
8063 TEU class
container carriers with the hull stress monitoring system
(HSMS). The HSMS system has primarily been used by the ship's crew to monitor the hull girder bending moment and
bow acceleration to assure that the vessel operates within safe operational limits. ABS considers the monitoring of hull
condition important and has published the ABS Guide for Hull Condition Monitoring Systems (1995, 2003) [4].
The ship designers and builders are also interested in providing more value-added features to ships in order to enhance safety and operational efficiency to make their ships more attractive to potential owners. SHI has developed the HSMS system as a valued optional feature to be offered to interested owners.
1
Another desired feature to assist the ship's crew is the onboard wave measurement system. Although the ship's crew are well
trained to safely operate the ship in varying environmental
conditions, accurate wave information can assist them in
making correct decisions in potentially dangerous situations.
For example, fine hull form container carriers are susceptible
to very large roll angle due to parametric roll resonance at
certain speeds and wave conditions, such as relative heading to
the wave, wave height and period [5]. 1f such a condition
arises
in the dark, the assistance from the onboard wave
measurement system would be most valuable. SHI developed
the onboard wave measurement system, called WaveFinder,
based on the X-band navigational radar system.
00CL, SHI and ABS have been working together
in thedesign, classification review, construction, and commissioning
of the 00CL 8063 lEU class vessels.
These three partiesrecognized the opportunity for carrying out full-scale measurement in actual operating conditions. The objectives of
the full-scale measurement project are to validate the HSMS
and WaveFinder against analytical
results and
availableweather data and to investigate the long-term statistics of sea loads.
TEST VESSEL
MV 00CL Europe was one of a series of container carriers
built by SHl and delivered to 00CL on 29 July 2006. The first
of this series vessel was delivered in 2002, and principal
particulars are given in Table 1. The vessel was recognized as the largest container carrier at the time of delivery. The vessel
design was reviewed using full-ship finite element analysis
using ABS Dynamic Loading Approach. The profile and plan view of the vessel is shown in Figure 1.
Table I. Principal Particulars of the Test Vessel
Figure 1 Profile and plan view and of MV 00CL Europe 8063 TEU Container Carrier
HULL STRESS MONITORING SYSTEM
The full-scale measurement system consists of two main
component systems; the hull stress monitoring system (HSMS)
and the onboard wave monitoring system (WaveFinder). In
general, HSMS installed on commercial ships have been used
to monitor global hull girder stresses and related vertical
bending moment by using long base strain gauges (LBSG)
from a section near the midship. Existing guidelines for the
HSMS system require monitoring of the measured stress and moments to demonstrate the soundness of hull structures.
There are numerous studies
indicatingthat the
torsional moment, in addition to the vertical and horizontal bendingmoments, is one of the most important design parameters for a container ship having a channel-type cargo hold structure. The
detailed method of deriving external moments from the
measured strains, therefore, is to be developed by the HSMS designers.
Kenichiro et al [6] has proposed an approach to derive external
moments based on strain signals from a midship section and
correlation parameters that are
derived by applying FE
analysis. This is quite a useful suggestion but the limitation is
that the torsional component is derived from one transverse
section of the ship rather than from two adjacent sections. lt is
believed that the derivation of the torsional moment from the
strain measurements at two adjacent sections may yield more accurate results.
Choi and Kang [7] have proposed a method based on two
sections which conform to the theoretical formulation.
The derived bimoments using the strain decomposition method from two sections, which have four long base strain gauges at
each section, are used in the formulation. This systematic
approach is selected in this full-scale measurement project. Figure 2 illustrates the arrangement of long base strain gauges
for the hull girder stresses at three transverse sections: at two
sections in the midship region (Fr. 183, Fr. 207) and at the fore part (Fr. 320). The sensors in the midship region are four long base strain gauges at each section, and two LBSG are installed
at the forward part of the upper deck. All sensors have been
calibrated by the strain values using calculated levels in a calm sea condition. An accelerometer is installed at the forward bosun store to monitor the bow acceleration as well as the
effects of impact loads due to slamming.
Lengtho.A. 3230m
Length B.P. 3080m
Breadth (MId.) 428m
Depth (MId.) 246m
Draught (Scant.) 145m
Speed (Design) 26.0 knots
Container Capacity 8063 TEU
Cb 0.68
1,2.3
Figure 3 Sample Replay Screen of the Hull Stress Monitoring
System
ONBOARD WAVE MONITORING SYSTEM
The ship's crew typically receives weather information througha weather services company during ocean voyages. The
forecast is typically updated every 12 hours. The crew of the ship also use visually observed wave height and period in
making operational decisions, such as
slowing down or
changing course. It is not practical, however, to observe the
weather conditions in the dark or in severe weather conditions.
Wave measurement using marine X-band radar has been
introduced to overcome this drawback and has been installed
on some offshore structures. The radar images by near range
setting have suitable wave information of direction, period, and height [8]. The wave parameters can be estimated by applying Fourier analysis with a unique filtering procedure to
accommodate radar dynamics and to reduce certain undesirable
signals such as those from ships. The feasibility study for the
shipboard application has also been carried out by considering
the speed effects of the ship. However, the validation was
difficult due to the lack of true information on waves.
Recently, Park et al [9] have completed the development of the
system, using marine X-band radar, named WaveFinder, and
have performed several sea trial tests comparing this data with
buoy data. Their results illustrate the system's validity.
Hence, the system
has been included in this full-scale measurement such that the measured hull stresses may becorrelated with respect to the
related wave and wind
conditions.
The marine X-band radar at the fore mast is selected as the
scanner, and a scan converter is added to obtain radar images from the existing radar. Interfaced radar images are connected to the WaveFinder system. The system can separate the swell
and wind-generated wave components, which is quite useful information for estimating ship motion and sea loads in the waves.
DERIVATION OF HULL GIRDER LOADS
FROM STRA[N MEASUREMENT
A ship in a seaway is subject to irregular wave excitation that would produce the vertical, horizontal and torsional moments
on the hull girder. The strains measured from the full-scale
measurement are the combined effects of these external
moments. Therefore, it is necessary to develop a formulation such that allows the measured strains to be directly related to
the bending and torsional moments. Choi and Kang have
proposed a procedure [7]. The decomposition method can
derive the independent strain components due to the individual
moments from the combined measured strains. Figures 4
through 8 are sketches which define the arrangement of strain
gauges and the derived strain components due to different
external moments [12]. BBC') 4C'ABEGAI) 6 )IOGBB) 6 c,c6) 4 L2.3.5 S (ON 0100K) S 106R 6 .C'106 5 (ON 0100<) 6 (oN OBI j 6 (101010K) 6 LOSCO) 6 (co 010.0< 6(ooroo( 5(00CG) SMTC-074-2008 Yu 3
Figure 2 Arrangement of long base strain gauges for Hull
Stress Monitoring System installed on the test vessel A motion sensor is also installed at the accommodation area to
record the
roll and pitch motions.
The motion data
isaccessible to HSMS by serial connection for this ship.
All sensor signals of the HSMS are digitized at 20 samples per second. The sensor signals are processed to generate statistics
for each 5-minute time history, and then are recorded on the
hard disk of the processing computer. The statistics include the maximum, mean, minimum, peak-to-peak, standard deviation,
root mean square (RMS) and mean crossing period.
In addition to the statistics, the raw time histories of the 1-ISMSsensors are also recorded for 5 minutes on every hour during the first round trip voyage between the Far East and Europe.
The system software was modified to record all measurements
continuously then write a data file on every hour from the
second voyage.
The HSMS provides an interactive user interface to display the
bending moments, torsional moment, statistics, bottom slam occurrence, cumulative fatigue cycle count and the real-time sensor signal display. The HSMS also provides an option to
replay the recorded data.
Figure 3 illustrates a sample replay screen of the HSMS, which
shows the option to display the measured strain, the derived
bending and torsional moments, and the navigation route from the recorded data. Hence, hull structural conditions are easily
measured and analyzed using this hull
stress monitoring system. S1
6) I LGOGEN 0601*0 10<01 2 SIGNAL C14IOI000SINO *01 7 4 1 ZENOI 004010k 004 N JLOACflGN *0* 6 LONG 00000 01440< GAUGE 00001.04000000Long hase strain gauge
Figure 4 Arrangement of long base strain gauges for
two-section measurement
Cl
y
Yry
Figure 5 Arrangement of gauges at the
midship of a
container vessel
Figure 6 Graphical illustration
horizontal bending moment
y
YB.
z4
-_-,<__ y,
rs
-1_---í.>-Figure 7 Graphical illustration of strains
in the case of
vertical bending moment
Strain due to horizontal moment: =
of strains
inthe case of
Strain due to vertical moment: e. = e2Warping strain due to torsional moment: e, = St. Venant strain due to torsional moment: e. =
V
Figure 8 Graphical
illustration of warping strains due to
torsional moment
The strain from the long base strain gauge measures the
combined quantity of vertical, horizontal, warping and St.
Venant strains. Therefore, one can write the strain components at one midship section as follows.
. 6,,
Here, the measured strain components are counter-clock-wise and the symbol stands for the strain vector consisting of strain components of horizontal, vertical, warping, and pure torsion
at the Ist sensor, and stands for the warping function that can be obtained by the finite element modelling: Fujitani(1990)
[10]
for complex geometry, Kim et
al.[Il]
for simple geometry.The decomposed strain component vector, therefore, is defined as the following, with respect to the strain at the Ist sensor.
Similar results can be obtained at an adjacent plane with
subscript a and the distance d of in-between sections, and
then the subtraction of the two equations can be expressed as
=
Here,
Mm =
[,0
E3 S3 e4
M=
-
e e-
e-
aT-The transformation matrix A will be the same because the
two planes will be located at the plane having the same cross-sectional properties. Finally, the torsional component due to
warping can easily be obtained by the following:
= dz2 6aw -U1d
--i
I i I-1
A=
YB/
ZB/
U3/
(r3/
/Yr
/ZT
/U
yB/
z/
U3/
(r3,./
YT/Z
/U1/
SMTC-074-2008 Yu 4 rn = A where, em= [1 e2 e3 64fr-Fiere, f' is the torsional constant and multiplication of Young's modulus and the second moment of cross section at shear center. w is the slope of twisting angle. The warping strain ¿', at an adjacent cross section is required to obtain the
torsional moment.
ONBOARD
SYSTEM
TESTING
DURING
MAIDEN VOYAGE
The test ship MV 00CL Europe was commissioned to the trading route between the Far East and Europe, which would
take about 60 days for the round trip. lt was determined that
the installed hull stress monitoring system and the onboard
wave measurement system should be tested during the maiden voyage [12]. The onboard system was tested during the voyage from Busan to Port Suez, as shown in Figure 9.
HULL STRESS MONITORING SYSTEM TESTING:
Figure 10 is the selected records of the hull stress monitoring system taken during the voyage from Busan to Port Suez. Each data point in this figure represents a processed statistic, such as mean, maximum, etc., over a five- minute period.
Figure lO(a) shows the vessel
speed during the voyage
annotated with the names of the ports at which the ship had called.
Figure 9: The route of the onboard testing of the measurement
system
Figure 10(b) shows the ship's heading with key leeway points annotated. The annotated route segments are also shown in
Figure 12. The ship maintained 20 to 25 knots in the open ocean segment while reduced to lower speed in short coastal
segments. Figure 10(c) shows the mean wind speed measured by the onboard anemometer. The wind direction relative to the ship and ship's heading are also recorded. The true wind speed and direction may be determined for comparison to the weather forecast or hindcast data.
Figure 10(d) shows the average still water bending moment measured in the midship region (Fr. 183, Fr. 203) and at the
forward location (Fr. 320). It is noteworthy that the mean
bending moments show very little change over the long open
ocean segments compared to those during the short segments. It was observed that the transfer of ballast water or fuel oil was the main reason for the changes. This ship is equipped with an
automatic heel control system that maintains the ship in an
SMTC-074-2008 Yu
upright position during the loading and unloading operation in the terminal. The system automatically transfers ballast water between port and starboard ballast tanks located in the midship region. The ship typically intakes ballast water for heel control before entering a port and discharges in open waters. The fuel oil is also transferred before entering port for bunkering. There
exist many other causes that may change the mean bending
moment, such as trim, speed, temperature, etc.
Figure lO(e) shows the measured wave bending moment and the standard deviation of vertical acceleration measured at bow. The vertical scales are determined to produce the two
records aligned on top of each other as much as possible. This can be considered as simple ways of checking correlation. It is observed that
the wave bending moment and the bow
acceleration
indicate consistent correlation except for the
period between 8/24/06 20:00 and 8/26/06 12:00, which is annotated as the segment between leeway points A and B in Figure 9.
Figure 10(f) is the mean, maximum and minimum of the hull
girder stress measured by LBSG located at Fr. 183 on the
starboard side of the upper deck. The mean stress time history follows very closely with those of the mean bending moment. ONBOARD WAVE MONITORING SYSTEM Testing:
The WaveFinder system was tested during the open ocean
voyage from Port Kelang to Jeddah. The measured significant
wave height
from WaveFinder was compared with
theforecasted wave patterns from the weather service data in
Figure 11. The measured significant wave height is plotted
using a square symbol. The measurement results
of
WaveFinder are the average value of one-hour measurement. The discontinuity of the measurement is due to the rain or too
low level of radar echo signal.
Since the wave forecastprovides the anticipated wave conditions for the following five
days, the forecasted wave heights are overlapped in the plot. Hence, one can use the WaveFinder as a real-time onboard
wave measurement system.
4
Q4 Q5.3ß 082? 0878 0829 O83O O&31
ooc as.x 000o
oo
o000 oOE 00110 00:00Measured 6y Was54rder1Hrsausrage) Førecs1ed on 24th
r)recasted on 270, Farecaslerl on -. Forecasted on 3116 Hdcast
Fgure 11 Wave heights during the voyage from Port Kelang
3 .E +01 2.E01 Q) 1.E+01 (J.) 8.E+05 - E+05 4.E+05 j 2.E+05 0E+0D 8.EO1 6.E+U1 4EU1 2. E+ 01 ° 0.E+00 () Ship Speed n (h) Headiii ngI
aE.0i (c) Wind Speed
Shanghai
0.E±00 '
'--'
'I
''i'''
''''
8/13 8/14 8/15 8/16 8117
0113 0/14 8115 9/16 0/17
(d) Vertical Still Water Bending moment
2.E+05I(e) Wave Vertical Bending moment
f) Strain Mid-Starlioard-Upper SMTC-074-2008 Yu Forward(Er.320) 8/17 8118 8/19 8120 8/21 8)22 8/23 8,24 8125 8,2 8.27 8128 8/29 8/30 8131 9/1 9/2 9/3 0/13 8/14 8/15 8/16 8/17 8/18 8/19 8i20 8/21 /22 8123 0/24 825 8/26 8/27 8/20 828 8130 8131 9/1 912 9/3 Bow acceleration
Wave Bending moment
O E+OCI 000
8113 0114 0/15 0/16 8/17 8118 0/19 0/20 0121 0i22 0123 0/24 025 0.26 0127 8/28 0129 9130 0131 9/1 9/2 9/3
B,13 8/14 8/15 8/16 8/17 8/18 8/19 8.20 8/21 8122 8123 8124 8/25 8/26 0/27 0128 8/29 8/30 8/31 9/1 92 9/3
Figure 10 Selected records of measurements taken during the onboard test period
0.04
8/18 8/19 8/20 8/21 8/22 0123 8124 8/25 0/26 8/27 8i28 8/29 8130 8131 9/1 9/2 9/3
;:
I I_____________________
0/10 8/19 0/20 9121 9/22 0123 0i24 8/25 8i26 0,2/ 0120 9i29 0/30 0/31 9/1 9i2 9/3
Nirigho Singapore Port Kelaroq Jeddah
Q) a) a ci] 3.E.01 i.E 01 2.E.01 I.E .01 5.E.00 0.E.00 8/13 8114 9/15 flh1 Bow Acceleration E 1.EU5 5EÛ4 (13 4.E+02 3.E+02 2 E+02 i E02
Figure 12 Trading Route of the Test Vessel
VESSEL TRADING ROUTE AND ONSHORE
DATA PROCESSING
After the onboard system testing, the test vessel continued
service between the Far East and Europe. Figure 12 is the
trading route of the vessel. The round trip voyage takes about
60 days. The vessel completed three round trip voyages on this
route, and then was placed on a slightly different route. This
paper presents the findings from the first three voyages.
The project team engineer visited the vessel in Busan after completion of the round trip voyages where he recovered the recorded data, conducted system check and cleared hard disk
space ready for the following voyage. Onshore data processing
was carried out with the recovered data. There are three types
of data available for onshore processing. The first group of data consists of strains from LBSG, bow acceleration, roll and pitch
motion.
The second group consists of navigational data
including the Global Positioning System (GPS) position, ship's heading, engine RPM and speed. The third group consists of
derived hull girder loads at midship - vertical bending moment
(VBM), horizontal bending moment (HBM), and torsional
moment (TM). Statistics (maximum, minimum, mean, and
standard deviation, etc.) of the first group of data are processed
onboard and recorded every 5 minutes. Statistics of derived
channels are calculated during onshore data processing using the time histories of LBSG recording.
Selected statistics of all measured and derived channels were
plotted to evaluate the quality of recording and to screen out any erroneous data. The recorded data was found to be of high
quality without electronic noises or instrument drift, etc.
Occasional gaps were found in the recording, which were
caused by the crew turning off the computer system. The
measurement system is designed to start the software by itself
after the power to the computer has been restored, hence the loss of data recording can be minimized. Each record of data, i.e., S minute statistics, is further tagged with a flag indicating whether
the vessel was in port or at sea, since the allowable VBM ¡s
different for these two conditions.
After reviewing all three voyage records, it was found that the vessel encountered most severe weather conditions during the
westbound voyage number 3 in winter months.
lt was
determined to examine the recorded data in detail for the voyage segments in the Mediterranean Sea, along the coast of Spain in the Atlantic Ocean up to the entrance to the English Channel.
2
Figure 13 Selected Recordings, Westbound Voyage Number 3 Figure 13 shows measured mean wind speed, mm/max/mean of hull girder loads - VBM, HBM and TM - from 12January 2007
to 29January2007. It is shown that the vessel encountered two
storms, one in the Mediterranean Sea and another between
Gibraltar and Rotterdam.
STORM AND VESSEL RESPONSES IN THE
MEDITERRANEAN SEA
The vessel encountered a short and intense storm soon after
entering the Mediterranean Sea from Port Suez. Figure 14
shows the location of the vessel, vessel speed, wind direction, wave direction and heights along the vessel path during the
storm. lt is shown that the vessel passed through the storm area
within24hours. The wave record shows a very rapid growth of
wave height up to 5 meters in the first six hours then a gradual decrease in the following 18 hours as the vessel passes through the storm area. The true wind direction is fairly constant during the storm. Relative wave heading changes from bow seas to
stern quartering seas during the same time. It is also observed that the vessel reduced speed from23 knots to20knots near the peak of the storm.
L
UIIU$ UIMIUU:
IIi
UhIflhI' IUEIIIU0111
rtt
R9.W Iodng thnge
from mati sea. toS*ern quartering
Figure 14 Vessel Location and Weather Conditions During the
Storm in the Mediterranean Sea
SMTC-074-2008 Yu 7
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Figure 15 shows the engine RPM, min/maxlmean of bow
acceleration, VBM and HBM. It is
also shown that the
voluntary reduction of the ship speed occurred when the
maximum bow acceleration became greater than 02g while the
vessel's course was kept unchanged. The reduction of the
maximum VBM is observed when the speed was reduced.
These records show typical practice of the crew in heavy
weather to keep the vessel in safe condition. The ship's crew does not have the option to change the ship heading to avoid
large storms in the Mediterranean Sea because leeway points for
navigation cannot be changed in such a restricted area. The
speed reduction is the most frequently used method to reduce
large ship motions and hull girder loads. If the vessel were on a
route through the ocean then the crew would have a choice of
change of heading and/or reduction of speed. These practices
will affect the long term extreme values of ship motion or hull
girder loads that the vessel may encounter in its lifetime.
01
-3.!
Maximum Acceleration
A B C D F
Figure 15: RPM. Bow Acceleration, VBM and HBM in the
Mediterranean Sea
VBM during the storm was further analyzed to investigate the
frequency component which reveals some interesting features. First the time histories of VBM were created by combinìng the
recorded time series of four strain gauges.
Then spectralanalysis was carried out on the generated time histories of
VBM.
Spectrums of VBM are produced by Fast Fourier
Transform (FFT) method analyzing one hour time histories.One hour time series were divided to six 10 minute records, and
the spectra from each time series were averaged to generate a representative spectrum over one hour. Figure 16 shows the hourly spectra of VBM plotted along the time axis where the
vessel location is marked as A to F in Figure 14.
S1,ortìncoutit« waves (6-7 s&
frombow producedlarge2-node vibratory responses
Encounterwvepanodbecomes ong (15 sec.) towrd stern quarteringseas
':
-.
-.. SMTC-074-2008 Yu 8 A I C O A C O pFigure
16 Changes of Spectra of VBM in Time in
theMediterranean Sea
First, the peaks of VBM spectra shift from high frequency
(around 0.15 Hz) to low frequency (around 0.05 Hz) from
location B to C. This is mainly due to the change of relative
wave heading from bow seas to stern quartering seas that result
in
longer encounter wave period towards the
location B.Secondly, the 2-node hull girder vibration component is visible
around 0.5 Hz which is the natural frequency of the 2-node
vibration of hull girder. The peak of the 2-node vibration
component diminishes as the wave heading changes to stern
quartering seas as well as the wave height becomes small. The
third observation is the spectral peaks around 0.15 Hz that
persist throughout the storm from location B to C. This appears
to be the VBM responses to the wind-generated waves in
developing seas.
Figure 17 shows the spectra of VBM and corresponding time histories at two instances, one at 14:00 1-IR and 18:00 1-IR. Relative wave directions are bow quartering seas and stern
quartering seas from starboard. The spectrum of VBM at 14:00 HR shows two distinctive peaks, one around0.1 Hzrepresenting the VBM due wave frequency component and the other around 0.5 Hz representing the 2-node hull girder vibration component.
The spectrum of VBM at 18:00 HR shows three distinctive
peaks, one around 0.05 Hz, the second around 0.15 Hz and the
third around 0.5 Hz.
The peak around 0.5 Hz is a 2-node
vibration component of VBM of which the magnitude
isreduced compared to the 14:00 HR spectrum. The reduction is
due to the change in wave direction and wave height. Bow flare
impact is the main cause of 2-node vibration of hull girder for
fine hull form vessels. The vessel in stern quartering seas would
produce less bow flare impacts than bow quartering seas that would contribute to the reduction of 2-node vibration of hull girder. The other cause of reduction is due to decreased wave
height. Two spectral peaks, around 0.5 Hz and 0.15 Hz, can be explained that the sea conditions in the storm area may consist
of swell and locally generated wind waves. The encounter
frequency of swell becomes lower in stem quartering seas
compared to those in bow quartering seas while those of locally
generated wind waves would remain the same over the storm
area. lt is believed that the encounter frequencies of swell and
locally generated wind waves are close at 14:00 1-IR showing
one spectral peak, while these are separated
at 18:00 HR showing two spectral peaks when the relative wave headingchanges to astern.
VSM Spectrum 1-140714:00
Figure 17 Spectra of VBM and Corresponding Time Histories
of VBM in the Mediterranean Sea
STORM AND VESSEL RESPONSES IN THE
ATLANTIC OCEAN
The next storm event occurred where the vessel sailed along the
coast of Spain towards the English Channel. Figure 10 shows the position of the vessel and wave direction along the route
with selected channels. lt is shown that the wave environment changes abruptly from calm to heavy when the vesse! enters into
the Atlantic Ocean passing Gibraltar. It
is noted that the
predominant waves in the ocean are from the west while relative wave heading changed from head seas to following seas.
i
F aoe1-14.0? 14:00
VBM Spectrum 1-14-0? 18:00
peaks of spectra of VMB show the change of encounter
frequency from high to low as the wave heading changes from head seas to following seas. It is noteworthy to compare spectra
of VBM in the Mediterranean Sea to those in the Atlantic
Ocean. The VBM spectra in the Atlantic Ocean show very
small 2-node hull girder vibratory responses compared to those in the Mediterranean Sea. The plausible explanation is that the Atlantic waves are dominantly swells that have been propagated from far away hence there is very little wind wave component.
The wave conditions in the Mediterranean Sea appear to be
developing seas which is a
mixture of swell and locally
generated wind waves.
-J u VM Spectrum 1.19-07 12:00 f VBM Spectrum 1-19-07 00:00, VBM Spectrum 1-18.07 00:00 VBM Spectrum 1.17-4)7 13:001 t'lì
Figure 19 Spectra of VBM in the Atlantic Ocean
SMTC-074-2008 Yu 9
Figure 18 Vessel Location, Wave Direction, Vessel Heading
and Hull Girder Loads during a Storm in the Atlantic
Ocean
Figures 19 and 20 show the spectra of VBM and corresponding
VBM Time Historyl.19.07 12:00 700000 100400 300000 24.1 000400 050000 040000 040000 7x034 $50007 004040 400 3 70000000x00 -504000 700400 100400 006407 000000 4040 '10 070 740 700 440 7. 1)40 %0 4040 VBM lime Histolyl -19.07 00:00 VBMTineHistotyl -18-07 12:00 430 4*4 400 VBM Tine Hoiy1 -18.07 00:00 7120 420 040 VBMThu,e Historyl.17-07 13:00
Figure 20 Time Histories of VBM in the Atlantic Ocean
DIURNAL THERMAL EFFECTS ON HULL GIRDER
LOADS
Another interesting observation is the effect of the sun on hull girder bending moments. Figure 21 is mm/max/mean of VBM
and HBM during the westbound voyage number 2. It shows
large daily
fluctuation of mean HBM in
the circled areacompared to those of VBM. The mean HBM fluctuation also shows a sharp decrease of HBM (increase of tension on port side) over a short duration of a day. Figure 22 is a similar plot
of VBM and HBM during the eastbound voyage number 3. It
shows similar hull girder responses that the fluctuation of mean
HBM is greater than those of VBM. What is interesting in this figure is that the pattern of daily fluctuation of mean HBM is
opposite of those observed on the westbound voyage. It shows a sharp increase of I-IBM (increase of tension on starboard side).
The circled portion of the voyages were both in the Indian
Ocean where the vessel maintained steady heading either to the
west or to the east. It can be explained that these fluctuations are due the temperature difference between port and starboard
side of hull structures, since HBM is
proportional to the difference of strains of port and starboard side of the hull. Onthe other hand VBM is proportional to the difference of strains between deck and bottom structures.
It should be noted that the on-deck LBSG is housed in a
protective cover and positioned inboard side of the deck passage
towards the hatch coaming. Furthermore there is overhead
platform to store the most outboard stack of containers that
keeps the LBSG in shade all the time.
For other types ofvessels, such as oil tankers, the on-deck LBSG is more directly
exposed to direct sun which shows far greater fluctuation of
VBM than those of container carriers.
Figure 23 shows the fluctuation of strains at four parts of the
hull structure measured by LBSG. lt is clear that the deck strain on the starboard shows largest fluctuation due to position of the sun. The magnitude of daily fluctuation of the hull girder loads
is also affected by the atmospheric conditions, such as fog,
ovecast of cloud, etc.
>2 104.40 -.... 5x0.A4 47437040 - 040*44$1.---44*-44 600E_04 0U043* 8420,074 00.644.40 0.4660. .'7.),J,06 .8,44.740 0Oct.00
Figure 21 MinlmaxlMean of VBM and HBM during Westbound Voyage Number 2
----Vòyage-3 Eatb
Voyage -2 Westbound
44447.00 0.504440 !41E70 142101.20, 7*1.5.0.40
S.4..04 244,fl_7 7.4.6.20 42.0.807 42.044.47 72.141.-07 27.0 0.07
Figure 22 Mm/max/Mean of VBM and HBM during Eastbound Voyage Number 3 00*00... ¿... -. 01.400, ....t.&', -ee-05 DEbO .. ... 00.00 -I
.4...._.__.._...
...-SMTC-074-2008 Yu 10 0400 420 4440 7.0.1.07 12.0.1.07 '7.0-w 040.6.04 27.0.600CONCLUSIONS
A comprehensive full-scale measurement system has been
successfully designed and installed on a large container carrier.
The system consists of the hull stress monitoring system, the
onboard wave monitoring system, and the voyage optimization
system. The HSMS and WaveFinder systems were tested
during the maiden voyage, and three round trip voyage data has been analyzed.
It was found that the system was fully functional throughout
the test period and al! recorded data could be recovered in
good quality
The recording of operational data, such as ship's heading,
position, speed, etc., was found very usefu! in
understanding the recorded data and vesse! operational practices.
The onboard wave monitoring system can further provide important wave parameters that would assist in validating
the analytical results of ship motion and sea loads.
Hull girder responses of the vessel in the Mediterranean wave environment showed higher hull girder vibratory
responses than those observed in the Atlantic Ocean waves under similar significant wave heights.
Horizontal bending moment and torsional moment are more affected by the diurnal thermal effect than vertical bending
moment.
The recorded time histories of the sensors will also be
valuable in validating the phase relationship between the
ship motion and sea loads.
Long term distribution of the measured data has not been
studied due to short measurement duration. lt is planned to
carry out the comparison of measurements against analytical
methods in the future.
ACKNOWLEDGMENTS
The authors wish to express their appreciation to Captain K. H. Lee and all crews of MV 00CL Europe for their support during the onboard testing of the system. We would Ìke to give special
astbound
theindian Ocean
Figure 23 Fluctuation of LBSG Strains at four Location
thanks to Y. T. Kang of SHI who provided the data processing software for HSMS.
REFERENCES
I. American Bureau of Shipping, "Guidance Notes on
SafeHull-Dynamic Loading Approach for Container Carriers (2005)"
Bill Shi, Donald Liu, Christopher Wiernicki, "Dynamic
Loading Approach for Structural Evaluation of Ultra Large Container Carriers", SNAME Marine Technology
Conference & Expo, 2005
Sungeun (Peter) Kim, Yung-Sup Shin, Donald Liu, "Advance
'Dynamic Loading Approach' for Ultra Large Container
Carrier
Based on Nonlinear Time-Domain Seakeeping
Analysis", ISOPE Conference, San Francisco, May 2006
American Bureau of Shipping, "Guide for Hull Condition
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American Bureau of Shipping, "Guide for the Assessment of
Parametric Roll Resonance in
the Design of Container
Carriers (2004)"
Kenichiro Miyahara, Ryuju Miyake, Norikazu Abe, Atsushi Kumano, Masanobu Toyota and Yoshiyuki Nakajima,
"Full-scale measurements on hull response of a large-container ship in service", Proceedings of OMAE2006, 25th
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Choi J.W and Kang Y.T., "Two-plane hull girder stress
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Park G.l et al, "The Application of Marine X-band Radar to
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17-20, 2006
Park G.l et al., "Introduction of Optimum Navigation Route Assessment System Based on Weather Forecasting and Seakeeping Prediction, Journal of Korean Navigation and Port Research", Vol.28, No.10. pp833-841, 2004. (in
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Fujitani, Y. 1990 Thin-walled Beam Structural Analysis,
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(Original book: Yamamoto, Y., Ohira, H., Sumi, Y. and Hujino, M. 1997 Mechanics of Ship Structures, Seizando
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0f
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