S ept ember 1912
LABORATORIUM VOOR
SCHEEPSBOUWKUNDE
TECHNISCHE HOGESCHOOL DELFT
RESISTANCE DATA OF HULL FORD" 115
by
Ir. J.J. v.d. Bosch
Report No. 356
o
Contents Nomenclature List of figures Introduction4,
Model data Test procedure Test results7, iscussion of the test results
8.
References94. Appendix 1 : Summary of measurements 10. Appendix 2 : Table of offsets of model
1. Nomenclature A A
[A] = E
v2/3 Bc AB
=-era L cmaxHorizontal projection .of the area bounded by chines. 4114
transom, excluding external spray strips
Breadth over chines at any cross section
Average breadth of area A
Maximum breadth over chines
Span of planing surface, i.e. actual breadth of planing surface measured at main spray point
Incremental resistance coefficient
Speed-displacement coefficient based on volume of displacement
at rest
Centre of gravity
Acceleration due to gravity
L Length of A
1c Wetted length of chiné, measured parallel to the keel
from transom to main spray point
1k Wetted length of keel measured from transom 1 *1
1-
c k Mean wetted lengthm 2 [M] . -2 1/3 Resistance RA Incremental resistance S Wetted surface
[s]
= S 42/3Weight density of water
V Ship or model speed
X Centre of area Ap
G Rise of centre of gravity
a Angle of incidence, i.e. angle between still water surface and keel
-1-rTh
initial trim atrafgae eee
at
illwialt4e0 7-Sitirorf
]earise angle
:Skip or ;Fade' weigtk
Kinematic viscosity
:Ms density of Waarter
Distancke Of X
front traOSTorne`ekt
P'
g_)stance of G from:t'ir:ansom-at. Istera,
G alaeme 1Dase
-aqh1meof 0,e
aispioc
ement of 'Male
sia-
v.,(04- A
2. List of figures K_J
Figure 1. Lines and form characteristics of the hull
Figure 2. Resistance-weight ratio of the standard ship and angle
of attack
Figure 3. Wetted surface and mean wetted length ratio's
Figure 4. Wetted length ratio's and rise of centre of gravity Figure 5. Resistanceweight ratio as a function of A and
FnV
3. Introduction
The tested model was one of a series of three
.the numbers114, 115 and 116.
The aim of the test series was to compare the three hull forms with regard to the resistance in smooth water and the behaviour in irregular head seas
in the speed range betwee Fn7 = 2 and F1-17 = L. This was done in order to develop a hull form with a good overall performance at sea which could
function as a parent for a systematic series.
In this report the resistance data of hull form 1-5 in sea water are
given for displacements of up to 300 metric tons. For the information about the other test results the reader is,referred to the references [1]
[2] and [3] .
The tests, although being a part of the research program of-the Ship-building Laboratory of the University of Technology, were carried out at the Netherlands Ship Model Basin under the responsibility of the
Netherlands Ship Research Centre, TNO.
4 5 6 7 8
4.
Modeldata 9 oThe hullform is shown in figure 1.
2
The main particulars of the model 115 are given in the following table
3 4 5 6 7 A
.93312
m2 8 9 Bcmax0.54
00.432
2 cm 3 4 L2.16
5 6 4 7 /Bcmax 8 9 L/Bcm 5 3 :5 6 7 9 0.1 2 3 4 5 6 7 8 9 o 2 3 4 6 7 8 9 O 2 3 4 5 6 7 8 9 AX AG KG [A] Lml Test 1.04665
1.008
0.864
.18
7.2
6 m3 m m m4
Test 2.06133
1.008
0.864
.197
65.477
m3 m"ar
5. Test procedure
The model was tested at the loading conditions stated in the preceding section, over a speed range which correspOnded to the range of Froude
numbers from FnV = 1.6 to FnV = 4.0.
The model was attached to the towing carriage in its centre of gravity by an airlubricated support, which allowed the model to Ditch, heave
and roll freely.
The following parameters were measured
the modelspeed, which equalled the carriage speed the resistance, measured by a strain-gauge dynamometer
the rise of the centre of gravity, measured by a potentiometer the trim angle, measured by a gyroscope
the form and magnitude of the area wetted by'solid water were
determined from visual observation.
6.
Test results'The actual results are given in the appendix 1. The faired results are given in the figures 2 to 5. InlIgure 2 the resistance/weight ratio is given for a standard displacement of A = 16000 kg in seawater with a weight density of 1025 kg/m3 and a temperature of 15oC, using the I.T.T.C.
1957 extrapolator4without roughness allowance. When it is desired to take into account this additional resistance, use can be made of the curve in the lower part of the figure where the additional resistance/weight ratio RA is given forsan incremental resistance coefficient
_
0A = 0.0002.This curve holds for any value of the ship's displacement; for
12
CA.V
S= 0.0001.F 2. S
pgV ny
In figure 3 the wetted surface and the mean length of the wetted
surface are
given, reduced to nondimensional coefficients.In figure 4 the wetted length at the keel and at the chine are giyen and the
rise of the centre of gravity, also reduced to nondimensional coefficients.
In figure 5 the resistance/weight ratio is
given for displacements of
1to
250 metric tons. The resistance has been computed for seawater with w = 1025kg/m3 and t = 15o C. Use has been made of the I.T.T.C. 1957
e4.mtrapolator without
1
2 3
5
6
Discussion of test results
There are no exceptional things to report.
The resistance and trim curves are smooth without accessive humps. The resistance characteristics are good, considering the high deadrise
of the hull.
References
"Resistance data of hull form 114"
Shipbuilding Laboratory of the University of Technology, Delft.
Report no.
355.
"Resistance data of hull form 116"
Shipbuilding Laboratory of the University of Technology, Delft.
Report no. 357
[3)
"Comparative model tests of three planing hulls in calm water andirregular head waves"
Shipbuilding Laboratory of the University of Technology, Delft.
Report no.
358.
7 8
3 4 5 6 7 8 9 Appendix I o
2 Results of resistance test with model 115 in still water
3 4 5 Test 1 6 Displacement
46.65 am3
7 8 Temperature21.8
centigrade 9 o2 model rise of trim model wetted wetted wetted
3 speed centre of angle resistance length of length of surface
4 gravity keel chine
5 6 m/sec cm degrees kg cm cm m2 7 8 9
3.04
-
2.77
5.15
202 1941.070
o3.73
1.21
3.27
6.04
-
-
-.1 24.48
2.24
3.47
6.75
-
-
-34.41
2.19
3.45
6.76
-
-
-4 55.17
2.40
3.47
7.47
-
-
-65.21
2.60
3.43
7.50
-
-
-75.94
2.88
3.35
8.57
8 _ _ _ 95.84
2.88
3.23
8.44
_-
_ o 16.69
3.39
3.10
9.57
-
-
-27.52
4.14
2.78
11.00
-
-
-3 44.50
_-
-
194.0
170.0
.995
55.20
-
_-
191.5
172.0
.970
6 77.54
_ _-
186.0
157.5
.940
8 9 o 1 2 3 4 5 6 7 8 9 o 2 3 4 5 6 7 8 9 8-o2 3 4 5 6 7 8 9 o Test 2 1 Displacement
61.33 dm3
2 Temperature21.8
centigrade 3 4 5 6 rr 8 9 0 1 2Results of resistance test with model 115 in still water
3 4 5 7 8 9 o 1 2 3 4 5 o 1 2 3 4 5 D 7 8 9 D 1 2 3 4 5 5 1 id 9 o 1 2 3 J, 5 5 7 3 9
-9
3.11
.34
3.62
3.98
1.80
4.28
8.76
_ _ _4.67
3.20
4.17
9.17
-
-
-5.58
3.91
3.42
9.71
-
-
-6.22
4.43
3.30
10.29
190.5
143.0
.905
6.97
5.18
3.50
11.06
-
_ _7.82
5.35
2.82
12.02
-
-
-3.08
_-
-
204.5
198.5
1.125
3.92
-
-
-
199.5
177.5
2.085
4.64
-
-
-
195.0
163.0
.960
7.85
-
-
-
187.5
139.0
.900
model rise of trim model wetted wetted wetted
speed m /sec centre of gravity cm angle degrees resistance kg length of keel cm length of chine cm surface 2 m
4 5 6 7
-8 9 o Appendix IITable of offsets of model 115
4 ord 0 ord 2 ord 4 ord 6 ord 7 ord 8 ord 9 ord 10
5 6 mm MM M171 171M MM 1/1171 MM 111M 7 8 o
2.7
2.7
2.7
2.7
9 o 4 102.8 102.8 102.899.3
88.4
61.9
1 8 183.0 190.5 189.0 174.4 153.1 112.7 37.1 2 3 12 199.9236.9
261.0
236.5
206.7
156.171.0
4 16212.0
252.3
280.5
276.8
251.6
195.2 103.7 5 6 20 24221.9
264.1 231.1275.2
295.1307.8
295.7
311.8
274.9
294.6
225.9
135.0251.3
164.821.3
I 9 28239.6
285.2
319.9
326.1311.6
273.8
194.4 54.3 2 Deckline Chine 34 ord Beam Height ord Beam Height
5 6 7 o 240
300.0
o 18075.0
8 2 289315.6
2 225.1 97.1 9 o 4328.4
331.2
4260.3
119.0 6341.4
346.8
6267.3
142.3 2 3 7331.4
354.6
7249.0
155.8 8304.6
362.4
8206.3
171.8 5 6 9249.7
370.2
9 128.7 191.4lo
147.9378.0
102.7
216.0
9o Keel and 3tem
2 ord Beam Height
3 4 6
2.7
o 5 72.7
.1 6 7 82.7
3.7
8 92.7
41.6
9 olo
2.7
216.0
2 3 5 6 7 8 9-
10 o46.67 % L 0 8 st. 3-10 DETAIL SPRAYSTRIPS
SCALE 1 : 5 FOR A a 15 TON
Fig.1
Lines and formoharocteristies
of the hull of model 115.
A 120 100 80 60 .4,-;'''NI
di 60 50 40 90Illii4
-91-Ht. MEAN_...allim
BUTTOCK% 4..
40 20, %I
L/10A
116k
1
20 CENTE OF Ap PP-20 30 40 50 60 70 80 90 1'21E4R. etc
4
7
.2
o
FatVfig. 2 Resistance-weight ratio of the standard ship and angle of attack
Restsrafice toieRsersn
IN SEAlorret
ceE-FFILIEWMAO 48 : hioao lei
hIbiN4 7746 .17Tc., '357
lairmour
Re1aNNE46-Atom:vim.
6
14] .--.
--- ---
[Pi ---. 72
1.2
MaDEL. 1/5 % 4...
fig. 4 Wetted length ratio's and risë of centre of gravity
.10
741
'05
R.
lo
60
4
.pey,g7ONS
fig. 5 A Resistance-weight ratio as a function of A and F LA)
1.2
8
3
o
11111 FAV
fig. 3 Wetted surface and mean wetted length ratio's
-
. _
CS 7bvicg
ikTr.72
/*JD& #5
17* 2.2o
3o
4-0--m.4 PlErR le TOMS
fig. 5 B Resistance-weight ratio as a function of A and .F tAl= 6
nv