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design of bulbous bow for dtmb 5415

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CHAPTER 1
INTRODUCTION
1. The ability to perform numerical potential flow calculations using codes has
made it possible for naval architects to look into hull modifications prior to tank
testing. The actual flow fields and viscous effects are not accurately predicted
by the potential flow calculations, but they are sufficiently accurate in a relative
sense to optimise the hull form prior to model testing, even though tank testing
is still necessary at the end. Several scientists have successfully employed this
hull design optimisation method in recent years.
2. The first point of contact of the ship with the fluid is its bow, thus, making
changes to the bow geometry of the ship may lead to significant changes in
ship total resistance. The second chapter of this report talks about the literature
survey for this area of study.
3. This study was carried out with the objective to investigate the effect of
adding a bulbous bow to a fast-moving vessel with a finer hull form on the
resistance of the ship. The hull form selected was DTMB 5415 from David
Taylor Model Basin design. The bulbous bow was designed and faired to the
hull form as per Alfred M. Kratch’s “Design of Bulbous Bow” [1]. The design
parameters for the bulb have been discussed in the third chapter.
4. The fourth chapter consists of the modelling of bulbous bow using
SolidWorks and the consecutive chapter discusses the conditions for
conducting CFD over the model.
5. Chapter 5 talks about the results obtained from the simulations for
focussing on the variation of resistance for varying Froude number. The
consecutive chapter consists of conclusions drawn from the simulations and
the potential use of a bulbous bow in a final hull design of DTMB 5415.
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CHAPTER 2
LITERATURE REVIEW
1. Approximately ninety years ago, R. E. Froude explained that a torpedo
boat's reduced resistance following the installation of a torpedo tube was
caused by the thickening of the bow as a result of the torpedo tube. The bulbous
bow was first identified by D.W. Taylor as a simple tool for lowering the
resistance that creates waves. He added a bulbous bow to the battleship
Delaware in 1907 so that it could travel faster while maintaining consistent
power. Despite significant efforts in the experimental domain to investigate its
possibilities, it took seventy years for the bulb to emerge as a fundamental tool
in actual shipbuilding. Almost every aspect of a ship is impacted by a bulb that
is appropriately rated and designed.
2. The inclusion of a bulb permits a deviation from previously accepted design
rules for the purpose of a superior underwater form, particularly for rapid ships.
The only drawback is the greater building costs. The hydrodynamic fluctuation
of the velocity field near the bow, or in the vicinity of the rising ship waves, is
influenced by the projecting bulb form. The bow wave system is primarily
attenuated by the bulb, which typically results in a decrease in wave resistance.
3. The inclusion of a bulb permits a deviation from previously accepted design
rules for the purpose of a superior underwater form, particularly for rapid ships.
The only drawback is the greater building costs.
4. The hydrodynamic fluctuation of the velocity field near the bow, or in the
vicinity of the rising ship waves, is influenced by the projecting bulb form. The
bow wave system is primarily attenuated by the bulb, which typically results in
a decrease in wave resistance.
RT= RV + RWF + RWB = RF + RVR + RWF + RWB
where,
RT = Total Resistance
RV = Viscous Resistance
RWF = Wavemaking Resistance
RWB = Wavebreaking Resistance
RF = Frictional Resistance
RVR = Viscous Residual Resistance
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RWF and RWB are the components of wavemaking resistance. They vary from
ship to ship according to the respective block coefficients and speeds.
5. The frictional resistance (RF), which makes up the majority of the viscous
component (Rv), is always increased by the greater bulb surface. Since the
velocity field varies in the near bow region, it is still unclear if the bulb has an
impact on the viscous residual resistance (RV). Regarding the impact of the
bulbous bow on wavemaking resistance RW, there is no question. The main
contribution to the understanding of this issue has come from the linearized
theory of wave resistance. This idea states that the bulb problem is just an
interference between the ship's and the bulb's free wave systems. There may
be a complete mutual cancellation of the two interfering wave systems,
depending on the phase difference and amplitudes. The phase difference is
caused by the bulb's longitudinal position, whereas the amplitude is related to
its volume. Through examination of the free wave patterns obtained in model
experiments, the wave resistance is determined.
6. The wave-breaking resistance RWB is a function of the usual spray
phenomena and is directly influenced by the emergence and growth of local
and free waves in the area of the forebody. Comprehending the breaking
phenomenon of ship waves is crucial for designing bulbs for complete ships.
The entire energy loss resulting from the breaking of very steep bow waves is
included in the wave-breaking resistance. Wake measurements are useful for
detecting the majority of this energy.
7. The primary source of this resistance component is the local wave system.
The two back waves of the bow and stern, which are produced by the
momentum's deflection, make up the majority of this wave system. The
reduction of the wave-breaking resistance is limited to the extent that bow wave
breaking can be avoided. This can only be achieved, given the rationale behind
its design, by altering the momentum deflection or the bow's proximity to the
velocity field, respectively. This can generally be accomplished with both a
bulbous bow and the right hydrofoils.
8. The shape, speed, and loading conditions of the ship all affect how bulbous
bows affect the aforementioned components of resistance. It is crucial to
understand that a certain ship-bulb combination that performs well under
certain conditions may react badly under off-design conditions.
9. Given the significance of bulb form in lowering a ship's resistance, bulbs
must be categorised using a few geometrical factors. Kracht [1] classified bulbs
into three primary groups based on the cross-sectional form of the bulb
measured at the forward perpendicular.
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Δ – Type
Delta
Drop-Shaped Sectional
Area
Center of Area in the
lower half part
Concentration of bulb
volume near the base
O - Type
Oval
Oval-Shaped Sectional
Area
Center of Area in the
middle
Central Volumetric
Concentration
Table1: Types of Bulb
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∇ - Type
Nabla
Inverse Drop-Shaped
Sectional Area
Center of Area in the
upper half part
Volume concentration
near the free surface
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