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HYDROSTATICS:
Hull Geometric Calculations
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Fundamental Hull Geometric
a cu a ons
fundamental geometric properties of the hull
The trapezoidal rule and Simpson's Rule are two
methods of numerical calculation frequently used.
Numerical Calculations involved such as Waterplane, , , ,
and VCB
Moreover, all hydrostatic particulars will be calculated
using this approach.
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Trapezoidal Method
e curve s assume to
be represented by a set
.
The area under the curve
is the area of total tra ezoid ABCDEF
Area=
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Simpson Rule
the most popular and common method being used innaval architecture calculations
It is flexible, easy to use, its mathematical basis is easilyunderstood reater accurac and the result reliable.
Its rule states that ship waterlines or sectional area
curves can be represented by polynomials, , ,
moments can be calculated from these polynomials
With Simpson rules, the calculus has been simplified by
us ng mu t p y ng actors or mu t p ers. There are 3 Simpson rules, depending on the number
and location of the offsets.
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1. Simpson 1st Rule
se w en ere s an o
number of offset
three offsets are 1, 4, 1
The multi lier must be in
and end with 1
For more stations (odd
num ers , e mu p ersbecome 1,4,2,4,24,1
This can be roved as
follows:
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where y is a offset distance
h is a common interval
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Area= )(3
1 offsetmultiplierh
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2. Simpson 2nd Rule
Only can be used when number of offsets = 3N+1
s num er o o se
The basic multiplier for set of four offsets are 1, 3, 3, 1
For more stations , the multipliers become
1,3,3,2,3,3,2,3,3,1
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Also the area is preferable to be written as:
8
o setmu t p er
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3. Simpson 3rd Rule
Commonly known as the 5,8-1 rule.
This is to be used when the area between any twoadjacent ordinates is required, three consecutive
.
The multipliers are 5,8,-1.
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Area is the first important geometry that need to be
calculated.
common ypes o area, a erp ane area, an
Sectional Area, AS (or sometimes known as Station Area). Waterplane area, WPA has its centroid called longitudinal
centre floatation (LCF)
LCF need to be determined for various waterplane areas,WPA at various waterlines
Waterplane area, WPA Sectional Area, AS
, ,comfortable making a tables in solving the calculation
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A B C D E F G H
tat on or nate ro uct
Area
ever ro uct
1st mmt
ever ro uct
2nd mmt
Product
Area
Product
1st mmt
Product
2nd mmt
Waterplane area, WPA= 1/3 x product area x h
1st moment = 1/3 x product 1st mmt x h x h
LCF =hproduct
pro uct
area
mmtst
3/1
1
e.g. for 1st
Simpson Rulehroduct
=
2nd moment I = 1/3 x roduct nd x h x h2 x 2
area
mmtproduct
1
*h = common interval (in this case, station spacing)
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(datum point). It can be set either zero at aft,
amidship or forward of the ship.If reference point is set at
Aft
For example;Station ordinate SM Product Option1 Option 2 Option 3 Product 2nd mmt
Amidship
Forward
Lever (Product Area x Lever)
AP 1.1 1 1.1 0 -3 6
1 2.7 4 10.8 1 -2 5. . -
3 5.1 4 20.4 3 0 3
4 6.1 2 12.2 4 1 2
5 6.9 4 27.6 5 2 1
FP 7.7 1 7.7 6 3 0
Product
Area
Product 2nd mmt
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Exercise 1
For a su ertanker her full loaded water lane
has the following ordinates spaced 45ma art:
0, 9.0, 18.1, 23.6, 25.9, 26.2, 22.5, 15.7 and 7.2
metres res ectivel .
Calculate the waterplane area, WPA and
water lane area coefficient Cw .
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Exercise 2
A water plane of length 270m and breadth 35.5m
has the following equally spaced breadth 0.3, 13.5,27.0, 34.2, 35.5, 35.5, 32.0, 23.1 and 7.4 m
respec ve y.
Calculate;1.Waterplane area, WPA, and its coefficient, Cwp
2.Longitudinal Centre of Floatation, LCF about the
am s ps.3.Second moment of area about the amidships
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Obtaining Volume
Volumes, hence
displacement of the ship at
an drau ht can be
calculated if we know either;i) Waterplane areas at WL 2
WL 3
var ous water nes up to
required draught, OR Waterplane areas at various waterlinesWL 1
required draught at various
stations
Volume has its centroid,called longitudinal centre of
buo anc LCB and vertical
centre of buoyancy (VCB)
Sectional areas at various stations
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A B C D E F
Station Station
Area
SM Product
Volume
Lever Product 1st mmt
Product
Volume
Product 1st mmt
Volume Displacement, (m )= 1/3 x product volume x h
Displacement, (tonne)= Volume Displacement x
1st moment = 1/3 x product 1st
mmt x h x h
= hroduct
e.g. for
1st Simpson
Rule
volume
mmtproduct
*h = common interval
(in this case, waterline spacing)
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ec ona areas o a m s p up o m
draught at constant interval along the length are as
.
from amidships.
Area 5 118 233 291 303 304 304 302 283 171 0
m
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Example
A shi len th of 150m breadth 22m has the
following waterplane areas at various draught.Find the volume, dis lacement volume and
vertical centre of buoyancy, VCB at draught
10mDraught (m) 2 4 6 8 10
Waterplanearea, WPA (m2)
1800 2000 2130 2250 2370
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HYDROSTATICS (part II):
H drostatics Particulars and
Curves
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Displacement ()
This is the weight of the water displaced by the ship for a
given draft assuming the ship is in salt water with a density of
1025kg/m3.
LCB
This is the lon itudinal center of buo anc . It is the distancein feet from the longitudinal reference position to the center of
buoyancy. The reference position could be the AP, FP or
.
midships are negative.
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VCB
.
meter from the baseline to the center of buoyancy.Sometimes this distance is labeled KB.
WPA or Aw
WPA or Aw stands for the waterplane area. The units of.
LCF
LCF is the longitudinal center of flotation. It is the distancein from the longitudinal reference to the center of flotation.The reference position could be the AP, FP or amidships. If
s m s ps remem er a s ances a o am s ps arenegative.
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TPC stands for tonnes per centre meter or sometimes justcalled immersion.
TPC is defined as the tonnes required to obtain one centre
meter of parallel sinkage in salt water.ara e s n age s w en e s p c anges s orwar an
after drafts by the same amount so that no change in trim
occurs.
SWWATPC
100
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MCTC
.
would be moment to change trim one centre meter.Trim is the difference between draught forward and aft. The
excess draught aft is called trim by the stern, while at
forward is called trim by the bow
LMCTC L
100
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This stands for the distance from the keel to thelongitudinal metacenter. For now just assume theme acen er s a conven en re erence po n ver ca y a ovethe keel.
KML= KB + BML
LCFL
IBM
)( midshipmidshipLCF LCFWPAII
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KMT
metacenter. Typically, Naval Architects do not botherputting the subscript T for any property in the transverse
rec on.
=
A B C D E
Station ordinate ( 3 SM Productnd
TI Product
T
2nd mmt
2211 mmtroducthI nd
e.g. is applicable for 1st Simpson Rule
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y ros a c urves All the geometric properties of a ship as a function of
graph for convenience. This graph is called the curves of form or Hydrostatic
.
Each ship has unique curves of form. There are also
tables with the same information which are called the, .
It is difficult to fit all the different properties on a singlesheet because they vary so greatly in magnitude.
even keel (i.e. zero list and zero trim). If the ship has alist or trim then the ships mean draft should be use
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y ros a c urves cn ..
curves are functions of mean draft and geometry. When weight is added, removed, or shifted, the
operating waterplane and submerged volume change
form so that all the geometric properties also change.
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0.9
1
MTc
0.8
KML
TPc
0.6
0.7
KB
KMt
raftm
0.4
0.5
LCB
LCF
0.2
0.3
Disp.
Wet. Area
WPA
0.10 2000 4000 6000 8000 10000 12000
0 3 6 9 12 15 18 21 24 27
-1.4 -1.2 -1 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8
Displacement kg
Area m^2
LCB/LCF KB m
0.4 0.6 0.8 1 1.2 1.4 1.6 1.8
5 10 15 20 25 30 35 40 45 50 55
0 0.1 0.2
0 0.02 0.04 0.06 0.08 0.1 0.12
KMt m
KML m
Immersion Tonne/cm
Moment to Trim Tonne.m
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0.9
1
0.7
0.8
Midship Area
0.5
0.6
Block
Draftm
0.3
0.4
Prismatic
0.1
0.2
0.3 0.4 0.5 0.6 0.7 0.8 0.9Coefficients
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Tutorial 2
vesse o engt 5 m, eam m as t e o ow ng
waterplane areas at the stated draughts.
Draught (m) 2 4 6 8 10
WPA (m2) 1800 2000 2130 2250 2370
If the lower appendage has a displacement of 2600
tonnes in water of density 1,025 t/m3 and centre ofbuoyancy 1.20m above keel, calculate at a draught of
' , b
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Other T es of Curvesi. Sectional Area Curve
The calculated sectional areas (at each stations) also can berepresented in curve view.
After all the sectional areas are calculated at particular
draught, they are plotted in graph.
e grap s nown as ec ona rea urve, s ow ng e
curve of sectional areas at each station, particularly at Design
draught or design waterline (DWL).
Sectional Area Curve represents the longitudinal distributionof cross sectional areas at (DWL)
The ordinates of sectional area curve are plotted in distance-
squared units
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Example: Sectional Area Curve at Waterline 5m
From the curve example, it is clear that the area under
the curve represents the volume displacement at
water ne m Also, displacement and LCB at DWL then can be
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Sectional areas of a 180m LBP ship up to 5m
as follows. Base on the values, create a sectional
area curve.
Station 0 1 2 3 4 5 6 7 8 9 10
Area
(m2)
5 118 233 291 303 304 304 302 283 171 0
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ii. Bonjean Curves
The curves of cross sectional area for all stations are
collectively called Bonjean Curves.
It showing a set of fair curves formed by plotting of the
At each station along the ships length, a curve of the
transverse sha e of the hull is drawn. The areas of these transverse sections up to each
successive waterline are calculated, and value is plotted
on a grap .
By convention, the Bonjean curves are superimposed
onto the shi s rofile.
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Any predicted waterline required can be drawn on the
comp e e on ean curve pro e
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displacement of ship and its LCB at any draught level, atany trimmed condition
A standard method used is by integrating transverse
areas, as learned before.
,
particularly useful.
In the case of trimmed waterline, the trim line maybe
drawn on the profile of the ship.
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Then, drafts are read at which the Bonjean Curve are to
be entered.
By drawing a straight line across the contracted profile,
directly at each station.
From there, the values of sectional areas are takenindividually at the intersection of the line of drafts drawn
and area curves.
integrated (eg: Simpson Method) in order to determine
the volume of displacement.