2 JUU 1981
--
--
lab.
y. Scheepsbouwkun1e
ARCHIEF
Technische Hogeschoo!
OPEN WATER TEST SERIES OF M011ifIED
AU-TYPE-FIVE-BLADED PROPELLER MODELS
OF AREA RATIO 0.80
SERIES DE TESTES EM CANAL ABERTO DE MODELOS DE HELICES DE CINCO PAS DO
TIPO A U MODIFICADO, DE COEFICIENTE DE AREA E X P A N D I D A IGUAL A 0,80.
ATSL'O YAZAXIpor/by MICHIO TAKAHASHI (*)
JUNZO MINAKATA
()
RESUMO
Este trabalho apresenta resultados de testes ne Tanque de provas do Instituto de Pesquisas Navais de Tóquio realizados sôbre urna série sistemática de modelos de hélices de cinco pás do tipo A U, propositairnente modificado.
O coeficiente de área expandida da série de modelos ficou mantido no valor de 0,80 e os diagramas relativos aos coeficien-tes de velocidade J contra coeficiente de fôrça propulsora KT e as outras curvas, dando os outros valôres dos coeficiencoeficien-tes espe-cíficos, foram preestabelecidos através de diagramas para projetos de hélices preliminarmente determinados em outros testes.
Trata-se de um trabaiho que embora publicado em poucas páginas possui um valor de multo maier profundidade e pene-traçâo por se tratar de um tipo de hélice de caracteristicas bem modernas e de aplicaçâo s e m p r e major, principalmente nos supernavios.
I.
INTRODUCTIONThe authrs have reported the results of tank tests
on the AU-type-five-bladed propellers with the
expan-ded area ratio of 0.50 and 0.65
(1).
Further to the work, the authors conducted a
sys-tematic testing work with same type of propeller
mo-dels with the expanded area ratio of 0.80 in the Mejiro
n.° 2. Experiment Tank. In this paper, thi authors
pre-sent the results of the open water tests and the
ö design diagram.
II.
MODEL PROPELLERS AND OPEN WATER TEST
Model propellers used here are made of alminium
alloy and they have the diameter of 0.25 m. Their
principal particulars are given in Table 1, and the
model propellers are shown in Fig.l
-Open water tests were carried out in the n.° 2
Ex-periment Tank according to the ordinary practice.
To obtain the net thrust, the correction for the
re-sistance of the screw hub was made at various speed
of advance for the measured thrust.
The Reynolds number R0
of the tests are shown
in Table 1.
(')
Engineers and scientists of Ship Research Institute Tokyo,Japan.
VOL. I - N.° 3 - JULY/SEPTEMBER 1968
Table i
Particulars of Propeller Model,
Diameter (m)
Boss Ratio
Exp. Area Ratio
Max. Blade Width Ratio
Blade Thickness Ratio
Angle of Rake
Number of Blades
Reynolds Number (Rai = nD2/y)
III.
TESTS RESULTS AND DESIGN DIAGRAMS
The results of tests are shown in Fig. 2 in the form of
J-KT ,K0
, ,diagram. Values of KT
, K0 and 1 read
from the figure above are tabulated in Table 2.
Fig. 3 shows the
V'-
I type design diagram. In
this diagram, the metric units are used, and the
den-sity of sea water is assumed as 104.51 kgsec2/rn1.
IV. ACKNOWLEDGEMENTS
The authors wish to valuable cooperation and
as-sistance of Mr. Tadashi YAMAMOTO and the staff of
Ship Research Institute.
V. REFERENCE
(1)
K. Tsuchida, A. Yazaki and M. Takahashi;
Open Water Test Series with Modern Five-Bladed
Pro-peller Models, Journ. of Zosen Kiokai Vol. 102, 1958.
243 Modified AUS-SO 0.250 0.180 0.800 0.364 0.050 1000' 56.346.61 x 10
LOOR
--q 5.0d\r2.4Q..
3.60 Valuesof J - K
Table 2
k O.60R \-
_____
\..:
-j
' O.40R .-\
i . .I
L 0.20R...
_
DIMENSIONS ARE SI0WN
AS PERCENTAGE OF D.
Fig. i General plan of modified AU 5-80 propeller model.
'N. 0.4 0.6 0.8 1.0 1.2 K, lO K5 fl0 K, 10 K0 1), K, loK5 1) K, loK) 1k K, lo1E k 0 0.1590 0.1310 0 0.2690 0.2730 0 0.3870 0.4760 0 0.4970 0.7230 0 0.6020 1.0140 0 0.05 0.10 0.1310 0.1230 0.1693 0.2390 0.2500 0.1520 0.3540 0.4420 0.1274 0.4615 0.6810 0.1078 0.56S0 0.9610 0.0935 0.15 0.20 0.1000 0.1070 0.2972 0.2040 0.2220 0.2922 0.3180 0.4040 0.2502 0.4235 0.6360 0.2118 0.5270 0.9070 0.1848 0.25 0.0825 0.0980 0.3351 0.1855 0.2065 0.3575 O.2985 0.3840 0.3094 0.4045 0.6120 0.2630 0.5090 0.8'80 0.2301 0.30 0.0630 0.0870 0.3460 0.1660 0.1900 0.4176 0.2770 0.3620 0.3658 0.3840 0.5860 0.3132 0.4890 0.3490 0.2753 0.35 0.0430 0.0760 0.3151 0.1445 0.1735 0.4639 0.2545 0.3385 0.4187 0.3630 0.5590 0.3617 0.4695 0.8190 0.3193 0.40 0.0210 0.0630 0.2123 0.1220 0.1550 0.5014 0.2315 0.3140 0.4696 0.3410 0.5310 0.4091 0.4490 0.7880 0.3630 0.45 -0.0005 0.0495 0.0955 0.1370 0.5200 0.2080 0.2895 0.5144 0.3175 0.5010 0.4537 0.4270 0.7560 0.4044 0.50 0.0760 0.1180 0.5126 0.1840 0.2650 0.5528 0.2940 0.4710 0.4969 0.4040 0.7240 0,4440 0.55 0.0510 0.0975 0.4577 0.1600 0.2390 0.5858 0.2705 i4410 0.5367 0.3795 0.6895 0.4821 0.80 0.0240 0.0780 0.3016 0.1365 0.2130 0.6120 0.2460 0.4100 0.5730 0.3545 0.6550 0.5168 0.65 -0.0010 0.0515 0.1130 0.1880 0.6220 0.2220 0.3790 0.6063 0.3295 0.6195 0.5505 0.70 0.0890 0.1620 0.6120 0.1980 0.3470 0.8360 0.3050 0.5830 0.5828 0.75 0.0620 0.1330 0.5566 0.1735 0.3145 0.6587 0.2800 0.5450 0.6135 0.80 0.0350 0.1040 0.4288 0.1495 0.2820 0.6754 0.2545 0.5050 0.6420 0.85 0.0070 0.0720 0.1315 0.1245 0.2490 0.6765 0.2295 0.4660 0.6663 0.90 -0.0220 0.0380 0.0980 0.2130 0.6592 0.2040 0.4260 0.6863 0.95 0.0710 0.1760 0.6100 0.1790 0.38i' 0 7011 1.00 0.0430 0.1350 0.5072 0.1540 0.3450 0 7106 1.05 0.0140 0,0955 0.2449 0.1290 0.3030 0.7114 1.10 -0.0140 0.0550 0.1035 0.2610 0 6944 1.15 0.0760 0.2170 0.6410 1.20 0.0470 0.1710 0.5249 1.25 0.0190 0.1245 0.3035 1.30 -0.0110 0.0730 244 TECNOLOGIA NAVAL
.2 o 08 07 06 0 - 05 04 03 02 0. o DIAGRAM
TYPE. MODIFIED AU 5-BLADED PROPELLER, CONSTANT PITCH
o' 0.7 .6 .5 4ç-, .3 .2 MODIFIEDAUS -80 CONSTANT PITCH BOSS RATI0Q, 180 0.050 RAKE AP4GLE-iO'O Ka EXPA.R.Oeoo ,1n,j/23rK B.T R. tI,. T/95.5.
iuiIIuiIu.
I'IIIII.III.
I
III1UIiIII
iiuiuiui
Ì!iIIIII
uur4iiiIIIiI
iiiimiuii
IU(4iIIIIU
V1IIkII
!4IIII1ILIIIIL'
VOL. I - N.° 3 - JULY/SEPTEMBER 1968 245 O 01 02 03 04 0.5 06 07 08 09 0 Il 2 3 14Fig.2 J_KT,KQ,Ì?O Curves
Exp.A. R. 0.800 Boss Ratio 0.180 8.T.R. 0.050 flak.
Angie .Q'
\OO
'. 7
' n.., .'UL.UsS U5 Sa I4.ae ..%. IU.I4.IU .'ji,.'... :.
... ....
4US'
vea..m ii. ii ,i., i, ic ,.0 ,.ii, .1dUP. .r'*uI.. OV UI IUI'jI.I'
i
i.'.
w.YA .0 uII
l.il
i l..lp4 vii
. i
. CS 5.SUr k'.,e,'
aE
==I
.\ i
: :; ;'j
I I I... p
,. ò . , , , . . , F U .Us'-iI
eIPJ1'dl
1"pPP'4Pø'F1r 'r
B.
N M . ., w' P r 4 IO II 12 13 4 5Fig.3 f- Diagran (AU 5-80)
Lo N .9 08 7
r
o. .6NAVAL HYDRODYNAMIC
PROBLEMS SOLVED
BY RHEOELECTRIC ANALOGIES
PROBLEMAS DE HIDRODINÁMICA NAVAL RESOLVIDOS ATRAVES DE CRITERIOS DE ANALOGIA REO-ELETRICA
por/by
L. MALAVARD ()
APRESENTAÇAO
Durante dez anos o Centro de Cálculo Analógico do Conseiho Nacional da Pesquisa Científica de Paris, na França, con-tribuiu corn vários trabalhos para o estudo e a soluçâo de urn sem-núrnero de problemas de Hidrodinámica Naval. Tal contribui. cáo deve Ser considerada muito significativa, pela relevância dos estudos realizados e pela influência exerckia na soluçào de pro-blemas fundamentals da Arquitetura Naval.
Tal importante contrlbuiçäo se tornou possível, entretanto, graças apenas a urna p e q u e n a equipe de pesquisadores de grande valor que, utilizando equipamentos de cálculo e de experimentaçäo bem simples, deu ao mundo urna sobeja demonstra-cáo do pêso das qualidades humanas, incluindo nelas a perfeita aplicaçâo de correta metodologia e mentalidade científica, na con-duçâo de pesquisas teorético-aplicadas.
Corn éste trabalho, todavia, o Professor Malavard, Ilustre catedrático da Universidade de Paris e Diretor do referido Cen-tro de Cálculo Analógico, conseguiu, a nosso ver, produzir a tese de major importância para a Arquitetura Naval, do referido time daquela instituiçâo, tendo merecido um significativo sucesso noSÉTIMO SIMPÓSIO INTERNACIONAL DE HIDRODINÁMICA NAVAL, recentemente realizado em Roma, na ltália, de 25 a 30 de agôsto próximo passado.
TECNOLOGIA NAVAL esta apresentando, portanto, um trabalho de grande valor, prâticarnente inédito.
I. - INTRODUCTION
For ten years the Centre de Calcul Analogique
(C.C.A.) of the Centre National de la Recherche
Sci-entifique has contributed by various works to the study
and to the solution of quite a large number of naval
hydrodynamic problems. This contribution may be
considered very significant since it has been made
possible by a small team of research scientists using
very simple computing equipment. This
equipment
could seem inadequate for the work to be done in the
eyes of the non initiated or of the
staunch believers
in computing on large computers.
However, it is not possible to consider these studies
of naval hydrodynamics completely isolated from a
context where rheoelectric analogy is the means which
has enabled, and still enables, important developments
in the most varied fields of Mathematical Physics.
And, in this connection, it is convenient to recall that
the
first studies carried out in France using the
electrical analogy techniques concerning some
hydro-dynamic problems; flows around bodies with or without
circulation, Oseen flows (1) * (2), flows with jet stream
lines
(3),etc.;
premise
of a budding vocation;
a
vocation which became more decisive as from 1958
thanks to the experience acquired by the C.A.Ç. in
the treatment of problems in incompressible
aerodyna-mics, thin foils, lifting line, lifting surface, cascades,
simple helicoidal machines, etc.,
(4),(5).
(6), and
thanks to the introduction by Tulin and Burkart (7)
in 1955 of the linearised theory of cavitations.
One of the assets which has assured the success
of rheoelectric analogy since its early beginnings has
been its rapidity, as well as its ability in solving
La-placien field equations. This capacity for computing,
Professor of the University of Paris (Chair of Aviation), FrunceDiretor of the "Centre de Calcul Analogique" of the C.N.R.S., France
together with the experimental character of the
tech-nique employed, makes an ideal means for the practical
worker, engineer or physicist, who remains in contact
with a model on which his controlling action may
be
exercised without any restraint. Nevertheless, for an
intensive and complete use of the method, analog
simulation often requires turning to certain
methods
of theoretical formulation familiar to the
mathema-tician. It is in this way, for example, that the
know-ledge of elementary analytical solutions, the use
ofconformal mappind, the analysis of singularities,
etc.,
allow the solution of each problem in the most efficient
way
From these three given elements cited, experience
acquired in incompressible aerodynamics, the
ilneari-sed theory of cavitations and auxiliary analytical data,
naval hydrodynamic studies have been developed as
follows.
1.1. TWO-DIMENSIONAL PROBLEMS (fig. i;
In 1958, Luu carried out studies on the solution of
the direct problems of supercavitating hydrofoils (8),
(9). These studies were the continuation of important
research devoted to the problem of thin jet streams
in aerodynamics (8), (10), (11), (12) and came within
the framework of linearised free boundaries.
In
1960a: research programme was envisaged
concerning the effects of the free surface on slightly
immersed sub and supercavitating hydrofoils. In the
case of small Froude numbers, that is to say a
consi-derable influence of the gravity field effect, is was
possible to proceed easily to their design for imposed
pressure distribution (inverse problem) (13) (14). These
studies took into account the gravity effect on the
free surface and on the finite cavity, which, to our
knowledge, had not
yet been treated. The direct
246