MEDDELANDEN FRAN
STATENS SKEPPSPROVNINGSANSTALT
(PUBLICATIONS OF THE SWEDISH STATE SHIPBUILDING EXPERIMENTAL TANK)
Nr 60 GOTEBORG 1967
THE SSPA STANDARD PROPELLER
FAMILY
OPEN WATER CHARACTERISTICS
BY
HANS LINDGREN AND E. BJARNE
SCANDINAVIAN UNIVERSITY BOOKS
SCANDINAVIAN UNIVERSITY BOOKS
Denmark: navNzsoAAzi,D, Copenhagen Norway: IINlyEBSITETSFORLAGET, Oslo, Bergen-Sweden: ASADEDILFORLAGET-GUIEPERTS, Goteborg SVENSKA BOICTSRLAGET/NOT8tedtS B011EllerS, Stockholm
PRINTED IN SWEDEN BY
ELANDERS BOICTILYCKERL AKTIEBOLAG, GUTEBORG 1967
Summary
A family of 3, 4, 5 and 6-bladed conventional merchant ship
propellers of simple geometrical shape is presented. Propeller
char-acteristics obtained from open water tests are given. The results
from each propeller group are presented on the base of J, KTIJ4 and ICQ/J5. The ranges covered by experiments correspond to:
1. Introduction
The SSPA standard propeller family has been developed primarily
to be used in connection with preliminary project studies and
systematic model tests. At present it consists of about 100 propeller models with different blade numbers Z, diameters D, pitch ratios PID and blade area ratios A D/A0. The dimensions have been chosen so
that for every normal merchant ship project, it is possible to find
at least one suitable propeller model. For the preliminary
deter-mination of wake and thrust deduction factors, studies of the optimum
propeller diameter and influence of the number of blades, this propeller
family is very useful.
All the propeller models have been tested in the towing tank as well as in the cavitation tunnel and the test program comprises:
Open water tests
Cavitation tests in homogeneous flow
Cavitation tests in different wake distributions
In the present report, the geometric characteristics of the propellers
as well as the results of the open water tests are presented.
Number of blades Pitch ratios Blade ratios 3 0.55-0.75 0.45 4 5 0.65-1.15 0.65-1.15 0.47, 0.53, 0.60 0.60 0.75 0.60
4
2. Symbols and Units
ir D2
di \
=
propeller disc area (.
VA = propeller speed of advance
Z = number of blades
a = profile angle of attack
no = propeller open efficiency
= mass density of water = kinematic viscosity
Dimensionless coefficients and ratios are used throughout.
5
4 i
A,
= developed blade areaCi, = drag coefficient
C Dm; = minimum drag coefficient
CL = lift coefficient
c = blade section chord length
D = propeller diameter DR = hub diameter
J
= advance number ( DT7 An ) KQ = torque coefficient Q pD5n2) T \KT = thrust coefficient pD4n2) n = rate of revolutionP
-= propeller pitch (mean value = 0.9794 P max)P max = maximal propeller pitch Q = propeller torque
R = propeller radius (=D/2)
= Reynolds number. For propellers lifi+ (0.75 TT Dn)2
= blade section radius -= blade section thickness T = propeller thrust
6
3. The Propeller Family
The geometry of the propellers is defined in Appendix I. The
outline of the propeller blades is illustrated in Fig. 3 and the profile
shape in Fig. 4. Dimensions and profile ordinates are given in Tables
1 and 2.
The radial thickness distribution is almoSt linear and the
thick-ness diameter ratio, silD is about 0.05.
The hub diameter was kept constant within a group of propellers with different diameters. This means that the hub-diameter ratio
DHID varies within the ranges 0.15<DH/D<0.20. This variation
does not significantly influence the test results.
4. Tests and Method for Fairing the Test Results The propellers were tested in the towing tank over the range
0-100 per cent slip. The rate of revolutions was kept constant, whilst the speed V, was varied.
05 003 PIO a769 0.856 a' 0950 1.052 da t.163 -- Faired Ponies (40.1 aqua,* method) .2 -6 -6
Profile angle of <Moak. Profile angle of-attack
7
The method for fairing the test results follows the scheme outlined
in ref. [1],). All the material was analysed in accordance with the principles published by Lerbs [2]. For each propeller, lift and drag coefficients for the equivalent profile were calculated. Within each group of propellers, common lift and drag curves were determined
by the aid of the least square method. In Fig. 2, the primary test
spots converted to lift and drag coefficients for the 4.47 propeller group are presented. The faired mean curves used for the further. calculations are also given. The pitch ratio seems not to have any
significant influence on the results within the range tested.
Starting from the lift and drag curves obtained as above, faired J, KT, KQ and 770-curves could be calculated for arbitrary pitch ratios. No corrections for Reynolds' number effects have been in-troduced. The minimum drag values and Reynolds' numbers for
the different propeller groups are given in the table below:
All the analysis and fairing of the test material has been carried out on an electronic computer of the type FACIT EDB 3. The
prin-ciples have also been discussed in ref. [3].
5. Presentation of the Test Results
All the test results, faired and partly extrapolated as outlined
above, are presented in the diagrams in Appendix 11. The presentation
is quite dimensionless and the same parameters are adopted as in
ref. [1].
1) The numbers within brackets refer to the list of references in Section 7.
Type of propeller ./?. CD 3.45 4.99 105 0.0074 4.47 3.93 10 0.0086 4.53 4.68 105 0.0076 4.60 5.41 10' 0.0078 5.60 4.00 10' 0.0088 6.60 3.63 10' 0.0103
8
For each group of 3, 4 and 5-bladed propellers three kinds of
diagranis are given. In these diagrams the curves have been based on
KT K
J --and
Q-J4 J5
respectively.
The well-known Taylor variables B. and Bp are related to the
abovementioned variables by the equations
B.----0.05541N ,V8=Ci
r
N 1
/jr4 = c 1lirQV A2 17,2 V v 2 J5
where N -= number of revolutions in r/min
P = power in HP (HP=76 kprci/sec), fresh water
S =- thrust in lbs, fresh water
VA = speed of advance in knots
The factors C, and C2 can be obtained from the table below.
For the time being only one 6-bladed propeller belonging to the family has been tested. Complete diagrams have therefore not been
worked out. Preliminary curves representing 6-bladed propellers with optimum diameters have, however, been determined with the method
described in Section 4. These curves are given in Fig. 20 together with the corresponding curves for 4 and 5-bladed propeller with
ADIA0=0.60.
6. Acknowledgement
The authors are indebted to Dr. HANS EDSTRAND, director general
oftheSwedish State Shipbuilding Experimental
Tank for having stimulated and granted the work with this survey.
Thanks are also due to Mr. EDGAR FREIMANIS, who designed the
parent propeller form and worked out the preliminary plans for the
propeller family, to Mr. ARNE HANSSON who assisted in most of the
analysis work and to other members of the staff for their assistance
in various stages of the work.
Cl C2
Fresh water (p=102.0 kp see2/m4)
Salt water ( p = 104.5 kp see2/m4)
13.19 13.36
33.08 33.48
9
7. References
LINDGREN, Hs "Model Tests with a Family of Three and Five Bladed
Pro-pellers", The Swedish State Shipbuilding Experimental Tank, Publication No.
47, 1961.
LERBS, H. W.: "On the Effect of Scale and Roughness on Free Running Propellers", Journal Am. Soc. Nay. Eng. No. 1, 1951.
LINDGREN, laws and KILBORN, JAN: "Datamaskinverksamheten vid statens skeppsprovningsanstalt", The Swedish State Shipbuilding Experimental Tank, Allman rapport nr 10, 1965.
Appendix I
TABLE 1 SSPA 3.45 rIR , 0.3 0.4 0.5 0.6 0.7 ' 0.8 I 0.9 1.0
Total blade width
Multiplied by: 1.936 2.109 2.225 2.271 2.229 2:038 1.591
Leading edge to generator line
Z 1.195 1.265 L301 1.279 1.175 0:972 0.617 -0.327
Trailing edge to generator line
D , AD/AO 0.741 0.844 0.924 0.992 1.054 1.066 0.974 0.327
Length of face lift (lead. edge)
0.143
0.081
0.025
Length of face lift (trail. edge)
Divided by:
0:276
0.131
0.014
Distance of the point of max.
c.
thickness from the leading edge
0.360 0.374 0.399 0.430 0.458 0.481 0.500 Divided by: . Blade thickness D 0.0344 0.0300 I 0.0256 0.0211 0.0168 0.0124 ' 0.0079 00035
Distance of the ordinates from the point of max. thickness (pan.t.)
Radius
From p.m.t. to trailing edge
From p.m.t. to leading edge
Divided by: s Table of Trailing Leading back ordinates rIR 1.00 ' 0.76 050 0.25 0.25 0.50 0.75 1:00 rIR edge edge Divided by: s 0.3 0.159 0.488 . 0.740 0.932 0.945 0:819 0.603 0.219 0.3 0:041 0.104 0.4 0.110 0.469 0736 0925 0950 0.818 .0.582 0.148 0.4 0.035 0.082 0.5 0.063 0.456 0.728 0.919 0.949 , 0.816 0.566 0.074 0.6 0.026 0052 . 0.6 0.031 0.464 0.732 0.920 0.955 0.817 0563 0.031 0.6 0.031 0.031 0.7 0039 0.472 0742 0.921 0.955 0.815 0.562 0.039 07 0.039 0.039 0.8 0.053 0.521 0.763 , 0.931 0.954 0.817 0.573 0053 08 0053 0.053 0.9 0.083 0.607 0.821 0.952 0,952 0.821 0.607 0.083 0.9 0.083 0.083
TABLE 2
SSPA 4-, 5- and 6-bladed propellers
rIR 0.3 0.4 0.5 0.6 0.7 0.8. 0.9 1.0
Total blade width
Multiplied by: 1.777 1.976 2.123 2.197 2.177 2.003 1.581
Leading edge to generator line
Z 1.079 1.172 1.215 1.199 1.115 0.925 0.578--0.323
Trailing edge to generator line
D AD/A0 0:698 0.804 0.908 0.998 1.062 1.078 1.003 0.323
Lengtli'of face lift (lead. edge)
0:115
0:066
0025
Length of face lift (trail. edge)
Divided by:
0.180
0.112
0:058
0.013
Distance of the point of max.
c
thickness from the leading edge
0.360 0.377 0.401 0.430 0.466 0:494 0:500 Divided by: Blade thickness D 0.0332 0.0282 0.0235 0.0190 0:0148 0:0107 0.0068 0.0029
Distance of the ordinates from the point of max. thickness (p.m.t.)
Radius
From p.m.t. to trailing edge
From p.m.t. to leading edge
,
Divided by: 8
Table of back ordinates
rIR 1.00 0.75 0.50 0.25 0.25 050 0.75 1.00 rIR Trailing Leading edge edge Divided by:. 8 0.3 0.208 0.538 0.795 0.949 0958 0.833 0.624 0.208 0.3 0:031 0.130 0.4 0128 0497 0.777 ' 0.944 0.954 0.832 0.582 0.128 0.1 0.022 0:071 0.5 0.065 ' 0.463 0.761 0:940 0.949 0.797 0.544 0:065 0.5 0.019. 0:035 0.6 0025 0.441 0.752 0.938 0.946 0.784 0:513 0.025 0.6 0.021 0:025 0.7 0.027 0.436 0.749 0.937 0.943 0.774 0A91 0.027 0.7 0027 0027 0.8 0.038 0.446 0.754 0938 0.943 0:771 0.484 0.038 0.8 0:038 0:038 0.9 0:061 0.493 0.775 0.944 0.945 . 0.779 0.502 0.061 0:9 0:061 0:061
14
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Appendix II Open Water Diagrams
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