FOOD AND 'AGRICULTURE ORGANIZATION OF THE UNITED NATIONS ; ROME ;ITALY . 510 April 1959. To be discussed ong THURSDAY MORNING 9 April
/A7
Sessiong SEAKINDLINESSTESTS WITH A TRAWLER MODEL IN WAVES
Essais d'un modele de chalutier dans les vagues Ensayos con un modelo de arrastrero en olas
by
J.D. van MANEN
UnderDirector, Netherlands Ship Model Basin
G. VOSSERS
Head, Seakeeping Laboratory, Netherlands Ship Model Basin H. RIJKEN
Naval Architect, Netherlands Ship Model Basin Wageningen, Netherlands Contents Abstract Page 3 Résumé 3 Resumen 3
tkerti,
ex_evvy,ZA..cxj--Introduction 3Particulars of ship and model test conditions 3
Results when trawling 4
Results in the free running condition 5
Conclusions 6
References 6
* * * * * * * * *
Paper No. 29
WORLD -FISHING' BOAT CitINGRESS
FAO/59/3/2044
-2
Nate
To be recorded in the final proceedings, written discussions should be submitted, in three copies, before 1 May
1959.
It would, of course, beadvantageous if they were received in advance of the session so that they could be duly presented and discussed.
Those wishing to participate in verbal discussion should notify the Secretary one day in advance. Reprints, summaries and abstracts may be published by the technical press, if it is clearly stated that the papers are a contribution to this Congress.
Note
Les textes des commentaires doivent etre soumis en trois exemplaires avant le ler mai
1959,
de faconpouvoir etre inclus dans le compte rendu final. Toutefois, 11 serait preferable que ces textes parviennent au Secretariat avant la reunion pour
etre dament presents et discutes.
Les participants desireux d'intervenir dans les discussions doivent en avertir le Secretariat le jour precedent.
Les tires a part, resumes et abreges peuvent etre publies dans la presse teohnique s'il est indique clairement que les articles originaux sont des contributions a cc Congres.
Note
Las discusiones escritas que hayan de figurar en las actas finales deberdn presentarse, por triplicado, antes del 1 de mayo de
1959.
Convendria mucho recibirlas antes de comenzar el Congreso para que se Duedan presentar y discutir en la forma debida. Los que deseen participar en el debate deberdn avisar en la Secretarfa un die antes.La Drensa tdcnica e2td n:atorizada a publicar reimpresio-nes, restimenes y extractos, mencionando claramente que el material
de
que se trate ha sido una contribuci6n a este Congreso.
Abstract
3
Tests with a trawler model with and without nozzle in still water and in waves are described. The model was tested in the free running condition (0 to 11 knots) and when towing (4 to 6 knots). It appears that the addition of a nozzle for trawler propulsion when towing in still water can be recommended. This also applies to towing in waves, except in head seas, where unfavourable tendencies were found.
Résumé
L'auteur decrit des essais d'un modele de chalutier avec et sans tuyere, en eau calme et dans les vagues. Le modele a ete essaye en route libre (0
a
11 noeuds) et en peche (4a
6 noeuds). Ii apparaltque l'addition d'une tuyere pour la propulsion du chalutier en Oche
par mer calme peut etre recommandee. Cela s'applique aussi
a
la 'Ache par mer forte, sauf en cas de mer deboutoa
on a trouve des tendances defavorables.Resumen
Se describen los ensayos de un modelo de arrastrero con tobera y sin ella en agua tranquila y en olas. El modelo se ensay6 en ruta libre (0 a 11 nudos) y remolcando el arte
(4
a 6 nudos). Parece ser recomendable la adiciOn de una tobera al arrastrero cuando remolca el arte en agua tranquila. Lc mismo es verdad cuando se remolca en °las, excepto si vienen de proa, en cuyo caso se encontraron tendencias desfavorables.Introduction
Since the successful improvement of the towing capability of tugs with the Kort nozzle (nozzle propeller or shrouded propeller), a steadily
increasing number of fishing boats, particularly trawlers, are fitted with nozzle arrangements. The advantage when trawling in still water is well
known; charts on performance and methods of design have been published
(van tbanen,
1956,
van Manen and Superina,1959).
Sometimes reference is also made to the beneficial effects of a
nozzle propeller on the behaviour of a trawler in waves. The resistance increase in head seas is claimed to give the nozzle propeller an advantage furthermore, it is said to increase the damping, thus reducing pitch. In order to verify these claims, a typical trawler model was tested in the Seakeeping Laboratory of the Netherlands Ship Model Basin with and without a nozzle propeller in still water and in waves.
Particulars of ship and model test conditions
The lines of the trawler are based upon one of Gueroult's
(1955)
designs. A paraffin wax model, scale 1 8 13 with bilge keels, was used.
The propellers were designed for trawling at 5 knots, with
940
SHP (metric), and a propeller r.p.m. of 160. The Wageningen Bseries charts were used for the normal propeller with a diameter of 11 ft. (3.00 m.) which was acompromise for the trawling and freerunning conditions.
The diameter of the nozzle propeller was 93 per cent of that of the normal propeller. The dimensions and the profile of the nozzle were similar to No. 18, (the open-water test results of which were published by van Manen and Superina, 1959). The dimensions of the nozzle propeller
were chosen in accordance with the ideas presented in the same publication, and Kaplan-type blades were selected.
Particulars of the ship and propellers are given in Table I and Table Body plan, profile and nozzle arrangement are shown in Fig. 1 and 2. The still-water trawling tests revealed that the propeller did not absorb exactly 940 SHP at 5 knots and 160 r.p.m. The resulting r.p.m. for the normal propeller were 160.5, and for the nozzle propeller 157.3. These values were used in the subsequent analysis.
Because no friction correction can be applied to a model in waves, the assumption was made that the differences in torque and r.p.m. between still-water and wave tests could be calculated for full size according to Froude's law. These differences were added to the still-water torque and
r.p.m. for the ship. The still-water conversion from model to ship was made with the 1957 I.T.T.C. friction formula with an allowance of 0.0004
added for roughness.
The model was tested in 0 to 13 knots free running, and 4 to 6 knots trawling. Trawling was simulated by applying a resisting force to the
model. The wave conditions were
Directions: nearly head seas (cK 1700),
nearly following seas (cK 10°),
quartering seas (o< = 450).
Lengths: ratio wave length/ship length: >./L . 0.759 1.00, 1.25.
Heights: ratio wave height/ wave lengths h/X . 1/50 and 1/30. The recordings taken were
Pitch angle (through the centre of gravity) Heave (of the centre of gravity)
Angle of roll (through the centre of gravity) Maximum emergence and submergence of the bow
in relation to the waves (Fig. 3) Acceleration at bow and stern
(f Shaft torque
(g r.P.m.
(h Speed
Results when trawling
The results of the still-water and head-seas tests when trawling are given in Fig. 4 to 6. Quartering seas and following seas results differed very little from those in still water and are therefore omitted.
The tests when trawling in waves were analysed for three operating conditions:
Trawling with constant speed and constant power- the changes in pull, propeller torque and r.p.m. as a function of the wave length/
ship length ratio are given in Fig. 4.
Constant power and constant pull the resulting speed of the ship, propeller torque and r.p.m. as a function of the wave length/ship length ratio are given in Fig. 5.
Constant speed and constant pull the resulting SHP and r.p.m. are shown in Fig. 6.
1AO/59/3/204.4 =
(I
) . 1. 3.-5
In still water, at 5 knots, the nozzle propeller gave a pull of 12.04 ton,-while the normal propeller produced one of 10.83 ton. The
same values were found in following and quartering waves. Therefore it can be concluded that the nozzle propeller gives a considerably increased pull (11 per cent).
In head seas, however, an unexpected phenomenon was found. The
differences between the propellers became smaller; in several conditions it was even found that the nozzle propeller gave a lower pull (Fig. 4)/ or a lower speed (Fig.
5),
or required more SHP (Fig. 6). This wascontrary to expectations as it should give a better performance at higher
loads. One explanation might be the greater sensitivity of the nozzle
propeller to changes in the direction of intake velocity, which occur with heavy pitching and heaving. Another explanation might be the greater variation in efficiency of a nozzle propeller to rudder angles, although to keep the model on course in head seas, only small rudder angles of 4 to 10° were required. Further research is therefore needed.
Subsequent tests were carried out with two rudders, each placed a quarter of the nozzle's diameter from the centre line. Although very . good steering resulted, there was no improvement in the nozzle propeller's performance when trawling in head seas.
Results in the free-running condition
Fig. 7 to 10 show only the still-water and the head-sea results the other tests produced very small differences. In Fig. 7 the SHP and propeller r.p.m. are plotted against the ship's speed and the ratios of wave length/ship length and wave height/wave length. In still water the nozzle propeller required higher SHP, which was to be expected since the propellers were designed for heavy pulls; thus in the free-running
condition with a small load, the nozzle propeller would be at a disadvantage. In head seas, especially in high waves with a length equal to the ship's length or longer, where the resistance increase is high, the difference
between the propellers became smaller, and in some conditions the nozzle propeller required less SHP. There, the advantage of the nozzle propeller working with a heavy load was demonstrated.
In general, the speed of the nozzle propeller is less sensitive to changes in load, which is of advantage for some types of propulsion
machinery. When the design situation is at
160.5
r.p.m. for the normal,and
157.3
rap.m. for the nozzle propeller, a higher sailing speed can beobtained with the nozzle propeller, although it will require more SHP. However, there is sufficient SHP available in the free-running condition,
due to the trawling requirements, as shown in Table III, compiled from
Fig.
7.
In certain conditions such as short wave length, small wave height and high speed, even in head seas, the SHP in waves is less than in still water. This was found on many occasions with different models. A theoretical explanation has recently been offered.
The motions in head seas are given in Fig. 8 to 10. Heave and pitch are given in dimensionless form; the heave, by dividing the heave
amplitude by the wave amplitude (wave amplitude . half the wave height); the pitch by dividing the pitch amplitude (in radians) by the maximum wave slope,')
21-0
9 where h/X represents the wave height - wave lengthrnratio.
From Fig. 8, with the pitch and heave amplitudes, no general conclusion can be drawn about the influence of the nozzle. Sometimes higher,
occasionally smaller amplitudes were found. The same applies to Fig. 10, where the emergence and the submergence of the bow is given in relation to the wave height. The influence of the nozzle on motions and taking water over the bow are of a secondary nature, and no definite trends can be discerned.
,7A0/59/3/20:,4
--6
However, the measurements indicate that the nozzle reduces the vertical accelerations at the stern. The influence at the bow is negligible. It is therefore likely that the nozzle influences the phase angles between the motions by its damping effect, which, while not reducing pitch and heave, does decrease the vertical accelerations at the stern.
Conclusions
The following conclusions can be drawn from these tests8
For a ship trawling in still water the nozzle propeller increases pull considerably.
This remains true in following and Quartering waves.
When trawling in head seas, the nozzle propeller is unfavourable
compared with the normal propeller, because it causes either a decrease in speed, a weaker pull, or an increase in SHP.
In the freerunning condition in still water the nozzle propeller
requires a higher SHP, although at a lower number of revolutions, which is advantageous for certain types of propulsion machinery in attaining a higher free running speed.
The same applies to the freerunning conditions in following and
quartering seas.
In the freerunning condition in head seas the differences between
the propellers become smaller, and in high waves with a length equal to the ship's length the nozzle propeller is better.
The influence of the nozzle propeller on the amplitude of pitch and heave and the wetness of the foredeck is negligible.
The nozzle propeller, however, reduces the vertical accelerations at the stern.
References
GUEROULT, E.R. French motor trawlers. Fishing Boats of the World,
1955
Fishing News, (Arthur J. Heighway Publications Ltd.), London, pp.143-153.
MANEN, J.D. van Recent research on propellers in nozzles. New York
1956
Metropolitan Section S.N.A.M.E.EANEN, J.D. van and SUPERINA, A. Der Entwurf von DUsenschrauben.
1959
(The design of propellers for use in nozzles), Schiff und Hafen, February1959.
* * * * * * * * *
FA0/5V3/20:(4
1. 2. 4..Length between perpendiculars L.B.P. 42.00 m. 137.8 ft.
Length on the waterline L 43.99 m. 144.3 ft.
Breadth B 8.25 m. 27.06 ft.
Draught T 3.85 m. 12.63 ft.
Displacement
A
695.1 cu.m. 24543 cu.ft.Shaft horsepower propeller SHP 940 h.p. (metric) Shaft horsepower motor SHP 1000 h.p. (metric) Speed of the propeller r.p.m. 160
Longitudinal radius of gyration
(in percentage of L.B.P.) 25%
Metacentric height GM 0.80 m. 2.62 ft.
Rolling period Tcp 8 sec.
Bilge keelsLength in percentage
of L.B.P. 40%
Height 0.20 m. 0.66 ft.
Nozzle Diameter D 2.80 m. 9.18 ft.
Lengthdiameter ratio 1/D 0.425
Anee of the nozzle profile
relative to the shaft line i 8.5°
Thicknesslength ratio s/1 0.15
PAO/59/3/2044
7
-TABLET
....5TA0/59/4/2044 Propeller No. Propeller type Number of blades Diameter Pitch ratio P/D Blade area ratio Ad
,
Hub diameter ratio d/D Rake
8
TABLE II
Particulars of the propellers
Normal 'propeller
2655
Bseries
4 3.000 m.9.84
ft.0.680
0.502
0.167
10°
TABLE IIIFree running speeds and shaft horsepower for fixed r.p.m. Nozzle propeller
2656
Kseries
42,800 m. 9.18
ft.0.900
0.540
0.184
5o Normal propeller160.5
r.p.m. Nozzle propeller157.3
r.p.m. Speed SHP Speed SHP 31111 water11.09
363
11.12
580
A/L=
0.75; h/,),
= 1%50
10.88
35711.10
563
0.75; 111,A
= 130
11.09
422
10.67
551
= 1.00;
h/A
= 150
10.83
363
10.65
588
1.00; h/A = 1%30
9.73
533
10.23
586
/YL= 1.25; h/A
= 1%50
9.60
455
9.73
610
1.25; h7A = 1%30
7.50
755
7.75
825
I -D=
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1/2 2t.SUBMERGENCE
FIG. 3 HAXINUN EEPCENCE AND
SUBMER-GENCE OF 33" IN RELATION TO NAVES. 175 ISO A T 17s 1500 1000
TOW ROPE FORCE TESTS 411 STILL WATER AND INHEAD SEA
WITHOUT NOZZLE WAVE DIRECTION 170
---WITH NOZZLE
-S.Prntr
0, 1.0 .5
WARE LENGTHis., LENGTH
FIG. 4 TO' ROPE FORCE, PROPELLER
TOR:ILIE AND R.P.M. VERSUS RATIO "'AVE LENGTH/SHIP LENGTH FOR CONSTANT FO7E7 AND SPEED.
WAVE HEIGHT
WAVE LENGTH
510
TOW ROPE FORCE CONSTANT ION] TON (WITHOUT NOZZLE)
TOW ROPE FORCE CONSTANT 12. TON WITH NOZZLE/
SNIP'S SPEED CONSTANT S KNOTS
IL I., 125 1 a .... 0 g .9.
TOW ROPE FORCE
WITHOUT
TESTS IN STILL WATER At. IN HERO SEA
NOZZLE WAVE DIRECTION 170.
--- WITH NOZZLE 175
1
Lail I ro 1 ,-
i...,... 4 WAVE HEIGHT WAVE LENGTH 30 { ISTt
.1PROPELLER ToRouI g. -I A)72-,,,
,
.,,
.-.
L --
,. 9... 0 a a 23 :...1..
O 1 . -SHIP SPEED\
TOM ROPE FORCE
Toll 9017E FORCE MK' CONSTANT
CONSTANT 10.93 CONSTANT 12.04
940 SI...,
TON (WITHOUT NOZZLE>
T. (WITH NOZZLE/
1
OS 1
WAVE LENGTH /SNIP LENGTH
FIG. E SHP AND R.P.X. VERFLE
RATIO 'NAVE LENGTH/SHIP LENGTH FOR CONSTANT TON ROPE FORCE AND
SHIP'S SPEED.
CO
golm os" p
FIG. 5 SHIP'S SPEED. PROPELLER
TORUE AND R.P.M. VERSUS RATIO NAVE LENGTH/S4IF LENGTH FOR CONSTANT FOI'ER AND TON POPE FORCE.
POWER
SHIP'S
CONSTANT 940
SPEED CONSTANT S KNOTS
WAVE DIRECTION 170° TOW ROPE FORCE TESTS IN STILL WATER ANON HERO SEA
WITHOUT NOZZLE WITH NOZZLE ROPE roRCE WAVE HEIGHT WAVE LENGTH 1.0
---
r 0-500/ WITHOUT NOZZLE --- MIN NOZZLE ZOO It% WAvE ISHT !AIL LERSTH 30 o 11: 10 SNIPS IN 1111071
FIG.. 8 RELATIVE HEAVE AND PITCH
VERSUS SHIP'S SPEED IN
HEAD SEAS.
IS 10
S L L 01p1
SELF 1PROPULSION TESTS WI STILL WATER AND IN WOAD SEA iiyE DIRECTION 170
*WOE HEiGHT t
'.!!!AIE LENGTH 30, /,,
So ,7
PIPP'4 9 ACCELEPOTIONS tT F.P. AN1
A.P. VERSUS SHIP'S SPEED
IN HEAD SEAS. 500 *000 SOO !pit HE IL,HT WAVE LET007.
\
/F4114, Slif 'ND R.P.M. vEnsus SHIPS SPEED FOR IvAnAaut
:NUDE OF VAVE LENGTH/NIP LEv'GTH.
SHIPS SPEED 0KNOTS.
MERGENCE ANC, SUINNERSIENCE 01 0110 110W IN HEAO SEA
-
IIWITHOUT 000E1E NEIG"ThEAvE ENSWI
111711 NOZZLE - WAVE DINEC Tips 17
10 1$ 10
SNIP'S IN NAM SHIP'S SPEED III RIOTS
...457,1..,L WATER
11( 001 PAO
HIT KOUT
PITCH 413 HEA 0 SEA NOZZLE WAKE OINEETios ITO
-- w 1 TH NOZZLE , ,....-- - ...,4 1 / /--- ".'. WAVE LEW II
/
,/
SHIP LE HST N 1 125 / / / SO N/
/
i/
ii
/ / r 0.3/
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3.iiimftin
I. WEile 075 ACCE... WITHOU AT IIIPL // .N 41[11.0 S[IINOZZLE WARE DIRECTION,I,er
-__ IRMA NOZZLE IPI 11001LENGTH SHIP LENGTH 125 1.00 . .-0.
ID
I SNIPS 3 TO SPEED IN "i S, Immo.
I 0.S : P ACCELERATIONS WITHOUTATA.P. IN 0IE013 SEA NOZZLE WINE DIRECTION 170.
-- WITH NOZZLE IOW LEWti
...4411111ftla
SNIP LENGTH 1211 1A0priglaill.. 11111.11
USFIG,. B01 EMERGENCE AND
SUPPER-GENCE VEPSUS SHIP'S SPEED
IN HEAD SEAS.
5 10
SHIPS SPEED INIKNOTS SHIP'S SPEED AN KNOTS
7
/
/.00
f