Analysis of Total Ships Resistance with Variation of Hull Bow Types,
Ulstein X-Bow, Spherical and Tapering Bulbous Bow using CFD
Method
Kiryanto, Deddy Chrismianto and Ahmad Firdhaus
Department of Naval Architecture, Faculty of Engineering, Diponegoro University, Semarang, Indonesia
Keywords: The Total Resistance, Model X-Bow, Spherical Bulbous Bow, Tapered Bulbous Bow.
Abstract: Ships must have good performance and economic value. To achieve it, optimum speed is needed with minimal
engine power usage so it can increase the efficiency of fuel use. The use of engine power is closely related
to the total resistance on a ship. One alternative way to reduce ship resistance is to install bulbous bow. This
research aims to obtain the resistance of ships with variations in the type of bow shape of the ship. The analysis
on this research uses numerical method using CFD. Variations in the modelling of bow design are; X-Bow,
spherical and tapering bulbous bow. Based on the results of CFD calculations, each model is obtained, namely;
the lowest value of the total resistances coefficient and total resistances model X-Bow 0,006565 and 242,76
KN, while for the spherical bulbous bow model is 0,007211 and 267,22 KN and for the lowest form of tapering
bulbous bow the total drag coefficient and total resistance is 0,007368 and 273,40 KN. Referring to the results
of the analysis, resistances of the ship model using the X-Bow design is the best model that can be used as an
alternative if compared to spherical and tapering bulbous bow.
1 INTRODUCTION
Nowadays, various researches have been conducted
in the field of ship which aims to improve optimum
results both in terms of economy and performance.
Ships are expected to have good performance when
sailing, so the ship can sail in bad weather or extreme
sea conditions. Besides, the target of the design
optimizing efficiency is about the speed of the ship,
which is how to get the ship design that has optimum
speed but the minimum use of engine power so that it
can increase the efficiency of fuel use. The use of
engine power is closely related to the resistance
experienced by a ship. One alternative way to reduce
ship resistance is to install bulbous on the bow of the
ship. Ships with a good bow will provide the
efficiency of the resulting barriers so that ship
operations and ship movements become better
(Chrismianto, et.al, 2014) The hydrodynamic effect
of bulb bow placement is based on changes in the
distribution of flow around the bow, interfering with
the waves that occur due to the hull so as to reduce
the overall wave system (Francisco, et.al, 2007).
Currently the concept in shipbuilding design
especially in the bow of the ship to reduce fuel
consumption is the Ulstein X-Bow Bulbous bow
concept, which is a rounded structure in the bow of a
ship that is below the surface of the water which
functions to produce waves before the ship pushes
water. The waves produced by the bulbous bow are
opposite to the waves produced by the ship's body, so
that both waves will offset each other and make the
resulting waves smaller. The effect of using a bulbous
bow can reduce the total resistance of the ship by
30%. (Watson, 1998) Therefore, through this research
is expected to analyze the value of the total resistance
experienced by ships with the Ulstein X-Bow design
and the ship uses bulbous bow spherical and tapering.
The purpose of this research was to obtain the total
resistance of ships using Ulstein X-Bow and bulbous
bow (tapering bulb and spherical bulb) with the
calculation of CFD method.
2 LITERATURE REVIEW
2.1 Ulstein X-Bow Definition
Overall the shape of the Ulstein X-Bow is different
from conventional bow. The Ulstein X-Bow is
dominated by a high, rounded and expands slightly at
the top of bow (Lewis, 1998). Ships with Ulstein
60
Kiryanto, ., Chrismianto, D. and Firdhaus, A.
Analysis of Total Ships Resistance with Variation of Hull Bow Types, Ulstein X-Bow, Spherical and Tapering Bulbous Bow using CFD Method.
DOI: 10.5220/0008374400600064
In Proceedings of the 6th International Seminar on Ocean and Coastal Engineering, Environmental and Natural Disaster Management (ISOCEEN 2018), pages 60-64
ISBN: 978-989-758-455-8
Copyright
c
2020 by SCITEPRESS Science and Technology Publications, Lda. All rights reserved
X-Bow have great buoyancy because of increasing
volume of the bow shape. Ulstein X-Bow was first
introduced in 2005. Known as inverted bow because
of the bow shape with the top flipped towards the rear.
Ulstein X-Bow was originally designed for offshore
vessel. A vessel with a bow like this has better
seakeeping than a conventional bow. In addition to
seakeeping, this bow is also able to increase fuel
efficiency and makes waves more subtly.
Figure 1: Ulstein X-Bow model.
2.2 Tapering and Spherical Bulbous
Bow
Bulbous bow is a part of the ship located in the bow
section. This part is a part that is integrated with the
hull. The main function of this section is to reduce
ship resistance when the ship is operating. The
bulbous bow shape plays an important role in
determining the magnitude of the benefits. The
optimum shape depends on the size of the Froude
number (Harvald, 1983). Most resistances on the
ships are caused by the part of the ship that has direct
contact with the fluid. The fluid, which the ships
through, forms a wave pattern due to the movement
of the ship's body that eventually causes friction with
the hull, the working principle of the bulbous bow is
to generate waves or interfere the waves of the ship
coming from the bow, so that the incoming wave will
lose power due to wave interference from bulbous
bow and in the end the wave energy around the hull
will decrease, thus the resistance of the ship will be
decrease too.
Figure 2: Bulbous bow model.
2.3 Ship Resistance
Ship resistance is the most important factor that
determines the power of the ship needed (Rawson and
Tupper, 2001). Ship resistance is the study of fluid
reactions due to the movement of the ship through the
fluid. In order for a ship to move at a desired speed,
the ship's resistance must be overcome by other forces
that push the ship (Wartono, 1982) In terms of
hydrodynamics the ship is the amount of fluid force
acting on the ship in such a way that it opposes the
movement of the ship. The main and most significant
factor is the hull geometry and the wet surface of the
vessel (Bhattacharrya, 1978). The resistance is the
same as the force component that works parallel to
the axis of the ship's velocity. the total resistance of
the ship is calculated based on the mathematical
approach of the Holtrop Method in the Principles of
Naval Architecture Vol II, Second Revision (Lewis,
1988)
𝑅
0.5𝐶
𝜌𝑉
𝑆
(1)
Where:
C
t
=total resistance coefficient,
S =wet surface area on hull (m2),
ρ = density of sea water (kg/m3)
V
s
= service velocity (m/s)
2.4 Computational Fluid Dynamic
(CFD)
Computational Fluid Dynamics (CFD) is an analysis
system that includes fluid flow, heat transfer, and
related phenomena. As a chemical reaction by using
computer based simulation (numeric). This technique
is very useful and can be applied in industrial and
non-industrial fields. CFD codes are structured on
numerical logarithms, so they can be used to solve
problems in a fluid flow. Computational fluid
dynamics code here consists of three main elements,
namely:
a. Pre Processor.
b. Solver Manager.
c. Post Processor (Visualize).
One reason why CFDs are so successful and
popular is their ability to simulate currents that are
close to the original conditions, 3 dimensions,
irregular current geometry, and phenomena that have
complex physical. This is possible because it uses
numerical solutions from equations that regulate fluid
flow rather than using analytical solutions (Jayanti,
2004).
Analysis of Total Ships Resistance with Variation of Hull Bow Types, Ulstein X-Bow, Spherical and Tapering Bulbous Bow using CFD
Method
61
3 RESULTS AND DISCUSSION
On the table 1 is used ship principal dimension in the
research.
Table 1: Principal Dimension.
Principal Dimension
Length of Perpendicular (LPP)
Breadth (B)
99,20 m
18,94 m
Draft (T)
Height (H)
Displacement
Wetted Surface Area
4,00 m
6,00 m
4595,00 ton
1900,50 m²
Table 2: Dimension of model.
Model Dimension
Length of Perpendicular (LPP)
Breadth (B)
2,02 m
0,39 m
Draft (T)
Height (H)
Displacement
Wetted Surface Area
0,082 m
0,12 m
0,0384 ton
0,794 m²
Furthermore, the ship's resistance analyses with
the variation of the X-Bow form and bulbous bow
model.
3.1 Modelling with CAD Software
From the main dimension data of the ship model, the
ship body modelling was made with the help of CAD
Modeller.
Figure 3: Modelling with CAD Modeller.
3.2 Modelling with CAD Software
Ship model making also uses CAD 3D software so
that it can be opened in CFD software.
Figure 4: Modelling spherical bulbous bow with CAD 3D
software.
Figure 5: Modelling tapered bulbous bow with CAD 3D
software.
Figure 6: Modelling X bow with CAD 3D software.
3.3 Computational Fluid Dynamic
(CFD) Simulation
The process of numerical simulation on
Computational Fluid Dynamic starts from making a
hull model. Modelling using the CAD software, then
the file is exported in the form of a file igs. The model
used must be solid. After the model is finished, the
work continues using numerical simulations. The
numerical simulation software used is software based
on computational fluid dynamic. This simulation
steps are divided into several stages including:
geometry, mesh, setup, solution and result.
ISOCEEN 2018 - 6th International Seminar on Ocean and Coastal Engineering, Environmental and Natural Disaster Management
62
Figure 7: Geometry solid modelling.
After the running or simulation process is
complete, the results can be seen in the result stage.
The results obtained are the resistance value of the
ship, the model and visualization of the flow on the
free surface and station behind the hull.
Figure 8: Visualization of fluid flow.
3.4 Validation
In this research to validate the results of the test model
is using the results of towing tank test that has been
done in previous research. Validation is used to
determine the right boundary condition to be used in
the boundary condition when analyzing 3 ship models
using CFD software. The maximum error for
validation between numerical method and towing
tank test results is 10%.
Table 3: Validation Data.
Ship Model
Ct x 10
-3
Experiment
Ct x 10
-3
CFD
Difference
Model of spherical
bulbous bow
(1
st
model)
6.362 5.999
0.363
(5.71%)
Model of tapered
bulbous bow
(2
nd
model)
6.658 6.122
0.536
(8.05%)
The Ct results or the total drag coefficient
obtained on the CFD Software for the spherical
bulbous bow model is 0.005999, with the results still
in the error criteria below 10% of the towing tank test
results of 0.006362, so that there is a difference of
0.000363 or 5.71%. For the bow model of the bulbous
bow tapering model is 0.006122, the results are still
included in the error criteria below 10% from the
towing tank test result of 0.006658, so that there is a
difference of 0.000536 or 8.05%. And for the Ulstein
X-Bow bow model is 0.005699, the results are
included in the error criteria below 10% from the
towing tank test results of 0.006214, and the
difference of 0.000515 or 8.29%.
4 CALCULATION AND
DISCUSSION
The result of Ship resistance analysis using CFD
gathered, and then process it to get the final data. Ship
resistance value from each models with various speed
can be seen on the table below:
Table 4: Ct, Cf and Cr from each ship models.
Name
of
model
Fn Value Ct
x 10
3
Cf x 10
3
Cr x 10
3
1st
model
0.129
6.604
5.092
1.511
0.145
5.998
4.962
1.036
0.161
6.413
4.848
1.563
0.178
6.786
4.727
2.059
0.194
7.211
4.632
2.578
2nd
model
0.129
6.728
5.161
1.566
0.145
6.122
4.986
1.135
0.161
6.537
4.882
1.654
0.178
6.905
4.758
2.147
0.194
7.378
4.662
2.705
3rd
model
0.129
6.195
5.054
1.141
0.145
5.709
4.900
1.038
0.161
6.135
4.807
1.317
0.178
6.381
4.716
1.665
0.194
6.575
4.613
1.951
Analysis of Total Ships Resistance with Variation of Hull Bow Types, Ulstein X-Bow, Spherical and Tapering Bulbous Bow using CFD
Method
63
Table 5: Calculation of Rt value (Total Resistances) for
each 1: 1 scale model.
Name
of
model
Fn Value
Velocity
(m/s)
Ct
x 10
3
Rt (kN)
1st
model
0.129
4.112
6.604
108.77
0.145
4.626
5.998
125.04
0.161
5.140
6.413
165.03
0.178
6.564
6.786
211.31
0.194
6.168
7.211
267.22
2nd
model
0.129
4.112
6.728
110.96
0.145
4.626
6.122
127.79
0.161
5.140
6.537
168.45
0.178
6.564
6.905
215.32
0.194
6.168
7.378
273.40
3rd
model
0.129
4.112
6.195
101.82
0.145
4.626
5.709
118.54
0.161
5.140
6.135
157.28
0.178
6.564
6.381
198.26
0.194
6.168
6.575
242.76
Figure 9: Graphic of total ship resistance.
From the table presentation, the calculation results
and the graph image above show the difference in the
total coefficient value and the total resistance value of
each ship model according to the Froude number and
the speed of each ship model.
1. The lowest total coefficient value produced by the
three models when Froude number is 0.145 with a
ship speed of 9 knots. The Ct value of model 1
was 0.005999 with Rt of 125.04 kN. Ct value of
model 2 is 0.006122 with Rt of 127.79 kN. And
model 3 has a Ct value of 0.005699 with an Rt
value of 118.54 kN.
2. The highest total coefficient value is produced by
the three models when Froude number is 0.194
with a ship speed of 12 knots. Ct model 1 was
obtained at 0.007211 with Rt of 267.22 kN. Ct
value of model 2 is 0.007368 with Rt of 273.40
kN. And model 3 has a Ct value of 0.006565 with
an Rt value of 242.76 kN.
5 CONCLUSIONS
Based on the experiments and simulations that have
been done, it can be concluded that of the three
variations of the model, the lowest resistance value
occurs in model 3 with the design of the X-Bow
direction, namely the total coefficient of 0.006565
and the total resistance value of 242.76 kN. Whereas
for model 1 and model 2 produce a total coefficient
value of 0.007211 and 0.007368 respectively. With
the total resistance value of model 1 is 267.22 kN and
the total resistance value of model 2 is 273.40 kN.
REFERENCES
D. Chrismianto, A. Trimulyono, M. N. Hidayat, 2014.
J. Teknik Perkapalan, 11, 1, pp. 40–48.
D. G. M. Watson, 1998. Practical Ship Design, Elsevier,
Oxford.
E. V. Lewis, 1988. Principles of Naval Architecture Second
Revision Volume II, The SNAME, USA.
E. V. Lewis, 1998. Principles of Naval Architecture,
Vol. II, Resistance, Propulsion and Vibration, The
SNAME, Jersey City.
K. J. Rawson, E. C. Tupper, 2001. Basic Ship Teory,
Volume II, Butterworth-Heinemann, Inc., Oxford.
M. Wartono, 1982. Propulsi Kapal, Fakultas Teknik Perka-
palan, Institut Teknologi Sepuluh Nopember, Surabaya.
P. Francisco, J.A. Suarez, J.A. Clemente, A. Souto, 2007.
J. Mar Sci Technol, 12, 2, 83-94.
R. Bhattacharrya, 1978. Dynamics of Marine Vehicles,
John Wiley and Sons, New York.
S. A. Harvald, 1983. Resistance and Propulsion of Ship,
John Wiley and Sons, Toronto, Canada.
S. Jayanti, 2004. Computational Fluid Dynamics for
Engineers and Scientist, Springer, Dordrecht.
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