ARCHEF
HYDROMECHANICSo
AERODYNAMICSo
STRUC11JRAI MECHANICSo
APPLIED MATHEMA1IGS PRNC-THB-68 (Rev. 3-58)L
I L,i_4"e
'1 . e.Tedmche Hoschóo1
Dell
t!...-.-.-.-.-...-TMB 2-, 3-, AND 4-BLADED
SUPERCAVIT.ATING PROPELTFR SERIESby
E. B. Caster
HYDROMECILANIcS LABORATORY
RESEARCH AND DEVELOPMENT REPORT
'FMB 2-, 3-, AND 4-BLADED SUPERCAVITATING PROP SERIES by E. B. Caster January 1963 Report 1637 S-R009 01 01
METhOD OF APPROACH PRESENTATION OF DIAGRAMS USE OF DIAGRAMS CONCLUSION ACKNOWLEDGMENT REIERENCES TABLE OF CONTENTS Page ABSTRACT - 1 INTRODUCTION : - -- 1
APPENDIX A - CTJ DIAGRAMS F)R TMB SC PROPB1LER SERIES
APPENDIX B - C-J DIAGRA S FOR TMB SC PROPELLER SERIES 23
APPENDIX C BLADE THICKNESS FRACTIONS FOR TMB SC PROPELLER
SRES
33APPENDIX D - PITCH CORRECTION COEFFICIENTS FOR TMB SC
PRO-PEllER SERIES 43
APPENDIX E MxtM14 FACE ORDINATES AT 0.3, 0.5, 0.7, AND
0.9 RADIUS 'OR TMB SC PROPELLER SERIES 54
APPENDIX F MAXI}WM THICKNESS ORDINATES AT 0.2, 0.5, 0.7,
AND 0.9 RADIUS FOR TMB SC PROPELLER SERIES . 91
LIST OF TABLES
Page
Table 1 - RadiaJ. DistributiOn of Blade Chord for
Super-cavitating Propellers -
-4
Table 2 - CoefficientS for Obtaining Radial Distribution 9
of Pitch
Table 3 - Coefficients for Obtaining Face and Thickness
Distribution along Chord 10
2 3 7 11 11 12 13
BTF
cP
Blade thickness fraction
Power coefficient
Thrust coefficient
NOTATION
C Pitch correctiOn coefficient
D Propeller diameter
E A R cpanded area ratio
g Acceleration due to gravity
H Atmospheric pressure plus the submergence pressure at
0.7 section mTus the cavity pressure
J Speed coefficient
(_V
1 Chord length
10.7 Chord length at 0.7 radius
n Revolutions per unit time
Shaft horsepower
P/B Pitch ratio along the radius for finite cavitation numbers
R Maximum propeller radius
550 P8 U
D2V3)
8 a(
(p
- D2V
a iiiRe
Re)moids number07
vv
+
o.7TTflD2)(7
Xh Nondimensional radius at the hub
Kinematic viscosity
P Density of fluid
O.7
Cavitation nuiiber at 0.7 radius
iv
1)
r Radius of any prOpeller blade section
S0 Maximum compressive stress
T Thrust
t Section thickness
t Maximum section thickness along the radius
x
Va Speed of advance
0.7 Inflow velocity to section at 0.7 radius
x
Nondimensional radius - rx1 Fractional distance along the chord measured from the
leading edge
y PresSure face ordinate
Maximum pressure face ordinate along the radius
x
Z Number of blades
(P/D) Pitch correction coefficient
fl PropeUr efficiency
2gH 2gHJ2
r 0.7
ABSTRACT
This report presents theoretically derived series Of 2-bladed supercavitating propellers with expanded area ratios of 0.3, 0.4, and 0.5; 3-bladed propellers with expanded area ratios of 0.4, 0.5, and 0.6; and 4-bladéd propellers with expanded area ratios of 0.5, 0.6, and 0.7. These propellers have a specified radial distri-bution of' 'the section chord and a hub radius of 0.2 of
the propefler radius. The series data are plotted in
the form of nondimensional coefficients so that the performance of the propellers can be easily predicted and a complete design obtained if desired.
INTRODUCTION
Supercavitating (Sc) propellers, which have fully developed cavitation on the suction side (back) of their blades, are of interest to naval architects since conventional propellers experience an un-predictable performance breakdown, because of cavitation, when operated
at very high speeds.
This report presents series data which can be used to predict
the performance of SC propellers. Since an experimental series is /
costly and time-consuming, a theoretical series is of great value, if
only in a qualitative way. The series presented can be compared with
experimental resuits1'2' of propellers designed using this method. It
is apparent that there is some deviation from the experimental values, but this difference is not unreasonable compared to propellers design from experimentally derived subcavitating series.
A 3-bladed supercavitating propeller series with an expanded area ratio of 0.5 has already been derived at the Taylor Model Basin.4 Since the ultimate aim of a designer is to obtain the best propeller for a given craft, there is need for a method of predicting the performance of SC propellers due to variations in number of blades and expanded
ratio. The choice, of the number of blades and expanded area ratio is
important in designing propellers since the propeller stress is
d.ependent on these parameters. Because the propeller stress is directly
related to the loading of SC propellers, which have sectiOns that are usually thin and highly stressed, the choice of these parameters is invaluable.
In addition to stress considerations, the choice of number of blades and expanded area ratio is also important since it has been determined that any type of SC section operating at a given angle of attack has an optimum point, i.e , a minimum drag-lift ratio, which occurs at a specific lift coefficient.5 Thismeans that the blade chord becomes importaiit in deriving the most efficient propeller.
This report presents a series of 2-, 3-,, and 4-bladed SC propellers having various expanded area ratios. The results are plotted in a series of diagrams in the form of nondimensional
co-efficients which can be used to predict the performance and character-istics of SC propellers.
METHOD OF APPROACH
The series charts preSented here were derived by first designing
a ntniber of 2-, 3-, and 4-bladed sc propellers for zero cavitation
numbet operating in uniform flow. Each propeller had a hub radius of
0.2 of the propeller radius. The Reynolds numbers used for calculating
the section diag varied from 7.2 x io6 to
x
1O7 which corresponds topropellers having a diameter of 3 feet and operating at a speed of
ad-vance of 60 knots. It should be noted that these propellers were designed
for the same dIameter, speed of advance, speed coefficients, and non-viscous thrust coefficients as those propellers designed to derive the series presented in Reference 3, i.e., the speed coefficients covered a range from 0.3142 to 1.5708 and the nonviscous thrust coefficients covered a range from 0.15 to 4.0,
Like the series derived in Reference 4, the nonviscous thrust
and power coefficients, ideal efficiency, and hydrodynaxnic pitch
distribution for each of the series of 2-, 3-., and 4-bladed SC propellers were computed using Lerbs' mOderately loaded propeller theory.6 This
propeller theory has been programmed for the high-speed conuters at the
.7
Model Basin.
Once the above calculations were obtained, the next step was to determine the viscous corrections that must be applied to these nonviscous calculations, using the method given in Reference 1. In order to make these calculations, it was necessary to know the values of the section drag-lift ratio, which is dependent mainly on the section lift coefficient
and angle of attack. Table 1 gives the radial distribution of the section
chord for each series. From these values, the viscous thrust and power
coefficients and propeller efficiency were calculated for each propeller. The next step was to calculate the propeller pitch distribution for nonzero as well as zero cavitation numbers, using the method given
in Reference 1. Since the amount of cavitation changes the thrust and
power of a propeller, this effect must be compenated for by a corresponding
change in the propeller pitch. This was obtained by calculating the
pitch of each propeller at cavitation nthiibers ranging from 0 to 0.205 and comparing the results with the pitch calculated for zero cavitation number.
The section. ordinates of the "TMB Modified Tulin Section," used on these propellers, were calculated next. The camber line of this type section is the pressure side (face) of the foil, and the thickness is applied between the camber line and the free-stream line. The camber and thickness ordinates were calculated using the method presented in
Reference 1. The blade thicknesS fraction (BTF) was also calculated for
each propeller in order to compute the nominal stress at the blade root of these propellers by a siilified method derived from Reference 8.
PRESENTATION OF DIAGRAMS
Most of the diagrams presented here are designated by a number
and letter. The number indicates the propeller parameter and the letter
indicates the number of blades and the eanded area ratio (EAR) of the
propeller. The letters a, b, and c represent 2-bladed propellers having
expanded area ratios of 0.3, 0.4,. and 0.5, respectively; the letters d, e, and f represent 3-bladed propellers having expanded area ratios of
TABLE 1
Radial Distribution of Blade Chord for
Supercavitating Propellers 2-Biaded Series 3-Bladed Series 4-Bladed Series x
EAR0.3
1/flEAR0.4
1/I) EAR=0.5 1/flEAR0.4
1./I)EAR0.5
lIDEARO.6
1/flEARO.5
1/flEPRO.6
1/flEARO.7
1/fl 0.2 0.3438 0.4584 0.5730 0.3056 0.3820 0.4584 0.2865 0.3438 0.4011 0.3 0.3438 0.4584 0.5730 0.3056 0.3820 0.4584 0.2865 0.3438 0.4011 0.4 0.3438 0.4584 0.5730 0.3056 0.3820 0.4584 Q.28b5 0.3438 0.401.1 0.5 0.3429 0.4572 0.5715 0.3048 0.3810 0f4572 0.2858 0.3429 0.4001 0.6 0.3357 0.4476 0.5595 0.2984 0.3730 0.4476 0.2798 0.3357 0.3917 0.7 0.3159 0.4212 0.5265 0.2808 0.3510 0.421:2 0.2633 0.3159 0.3686 0.8 0.2754 0.3672 0.4590 0.2448 0.3060 0.3672 0.2295 0.2754 0.3213. 0.9 0.2070 0.27:60 0.3450 0á184O 0.2300 0'.2760 0.1725 0.2070 0.2415 0.95 0.1503 0.2004 0.2505 0.13,36 0.1670 0.2004 0.1253 0.].503 0.1754 1.0 0 0 0 0 0 0 0 00.4, 0.5, and 0.6, respectively; and the letters g, h, and i represent 4-bladed propellers having expanded area ratios of 0.5, 0.6, and 0.7,
respectively. it should be noted that the 3-bladed
series diagrams presented in Reference 4 are also presented here.
The propeller efficiency contours and the pitch ratio
calculated at 0.7 radius for zero cavitation number P/fl
are presented in Appendix A, Figures la through ii, as a function of the thrust
co-efficient /and the speed coco-efficient J and in Appendix B, Figures
2a
through 21, as a function of the power coefficient /çand J. The
solid efficiency contours in these diagrams indicate the region where the section-lift coefficient is between 0.0548 and 0.2 and the section
angle of attack is 2 degrees. The dashed portion below the solid
efficiency Contours represents the region where the section-lift co-efficient is less than 0.0548, resulting in flat-face sections having
angles of attack less than 2 degrees. This area should be avoided because
face cavitation is likely to occur on SC sections operating at these small
angles. The dashed portion above the solid efficient contours
re-presents the approximate area where the section-lift coefficient is greater than 0.2 and the angle of attack greater than 2 degrees. In this region, the cavities become thick and section loading high, and the.
theoretical results may be in.question. Also included in these diagrams
are maximum efficiency curves for obtaining the optimum rpm or diameter D.
The thrust coefficient CT, power coefficient C, speed
co-efficient J and propeller efficiency presented in Figures la through
2i were calculated using the following equations:
yT=
J T P 2 D 8 a 550P S V a nD 5 [1]where T is the propeller thrust, is the Shaft horsepower,
p is the density of the fluid,
D is the propeller diameter,
Va is the speed of advance, and
n is the revolutions per unit time.
CT cp
2gHJ2
0.7v (J2± 484)
and where H is the atmospheric pressure plus the submergence pressure at
0.7 section minus the cavity pressure, and is the acceleration due to
gravity. The other parameter 4 (PIP) derived for these propellers is also
presented in Appendix D, Figures 4a through 41, as a function of and J.
[4]
The propeller blade thic1iess fractions (BTF) derived for these propellers are presented next in Appendix C, Figtires 3a through 3i., as a
function of arid J so the propeller stress can be calculated. An
approximate method for calculating the maximum compressive stress at the blade root derived from Reference 8 is
l.95PC
Ta
V 2[5;]
z (BTF)2
ihere BTF is the blade thicithess fraction given In Appendix C..
As mentioned above, Appendices A and B give the pitch ratjo calculated at 0.7 radius for zero cavitation number P/Pd Since there is a change in thrust an power of a propeller due to cavitation, a corre-sponding change in this pitch must be iade to offset the variation in
thrust Or power. This change in P/P0 due to zero cavitation numbers
(A(P/D)C0) is presented in Appendix D, Figures 4 through 4i. The
paiwneter C is plotted in Figure 4 as a functicfriof the section cavitation number at the 0.7 radius (o7) Only, where
The final pitch ratio at .0.7 radius for propeflers operating at various cavitation numbers (P/D)07 can be obtained from the equation
(P/B)07 = P/B0
-[7]
where C is the pitch correction coefficient from Figure .4 of Appendix .D
and P/B is the pitch correction coefficient from Figures 4a through 41
of Appendix B. The radial distribution of (P/D)07 is presented in Table
2.
The section ordinates at various radii for the propellers are
presented in Appendices E and F. The maximum face ordinates are presented
in Appendix E, Figures 5a through 8i, and the maximum thickness ordinates
are presented in Appendix F, Figures 9a through 121, as a function o'
/çandJ.
A replot of the maximum efficiency curves given in Appendix A is
presented in Figiires 13 through 20 to show the.reiationship of number of
blades and expanded area ratio to optimum rpm and diameter. The
incon-.sistency in. these diagrams is undoubtedly due to the method of fairing
used as the curves were not cross-faired on the basis of number of blades
nor expanded area ratio. They do indicate, however, the trend with
varying number of blades and expanded area ratio.
USE OF DIAGRAMS
For a design based on thrust T, the propeller efficiency and
the Q.,7 radius pitch for zero cavitation number P/B
can be obtained from Appendix A, Figures la through li, depending on the number of blades and
expanded area ratio, once the thrust cOefficient and speed coefficient
J are obtained. Similarily, for a design based on shaft horsepower P5
values of and P/Il can be obtained from Appendix B, Figures 2a through
2i, once the power coefficient and J are obtained. Equations [1],
[2], and [3] can be used to calculate iç / and J, respectively.
Figures presented in Appendices A and B can also be used to obtain the optimum rpm or diameter D for a given thrust or power. The
optimum rpm for a given diameter is obtained by plotting iç or /?5 on
the maximuni efficiency line for a given CT or C,
in.
these figures. Thispoint represents the J that gives the optimum rpm fOr a given diameter,
and using this J value, the optimum rpm can be calculated using Equation [3]. The optimum diameter D for a given rpm is obtained by assuming a
diameter and plotting the calculated J and or iç on the figures
presented
in
Appendices A and B. The J obtained at the intersection ofa straight line drawn from the origin of the diagram through this point and the line of maximum efficiency for a given CT/J2 or C,/J2 represents the J that gives the optimum diameter for a given rpm. Using this J, the optimum diameter D can be calculated using Equation [3].
It should be noted at this point that. if the design being considered is based on shaft horsepower, the corresponding CT must be calculated since the remaining design diagrams are presented as a
function of
/5
an4 J. .This value of CT can be calculated using Equation[4] once and C are obtained from Appendix B for the propeller based
on power.
The approximate maximum compressive stress of the propeller can be calcUlated using Equation [5] where the blade thickness fraction
(BTF) is obtained from Appendix C, Figures 3a through 3' The final
pitch ratio for the propeller at the 0.7 radius for any cavitation number (P/D)07 is calculated using Equation [7] where P/B0 is obtained from
Appendix A or B. C(y is given
in
Appendix B, Figure 4, as a function ofO.7 which is calculated Using Equation [6]; 'and (P/D) is given
in
ppendix B, Figures 4a through 4i. The radial pitch distribution for th.is propeller is then obtained froi Table 2.
The section shape for these propellers can be obtained from
Appendix E which gives the maximum face ordinates (y/i and Appendix F
which gives the maximum thickness Ordinates (til)max atvarious radii. Once these ordinates are obtained, faired curves are then drawn to obtain
values for and (t/i)max at other radii where from, theory,
(y/)
is zero at the hub and tip. Table 1 gives the section chordlengths i chosen for these propellers. Thus, once y and t. are
max max
obtained, the chordwise distribution of the ordinates. y and t can be
obtained using the distribution given in Table 3. The method of
completing the, design of a SC propeller, using this series, is identical to the method presented in the Appendix of Reference 3.
TABLE 2
Coefficients for Obtaining Radial Distribution of Pitch
9 x (P/D)07 0.2 0.974 0.3 0.979 0.4 0.984 0.5 0.990 0.6 0.995 0.7 1.0 0.8 1.006 O.9 1.011 0.95 1.011 1.0 1.010
TABLE
3
Coefficients for Obtaining Face and Thickness Distribution along Chord
Y When i
t
Whent
When _____ t max t max max max0.051
O.05l<(-)
0.0753
0.O753(--)
max max max O O 0 0 0 0.0075 0.0189 0.0476 0.0343 0.0297 0.0125 0.0324 0.0705 0.0501 0.0429 0.05 0.1419 0.2053 O;.1326 0.1068 0.10 0.2915 0.3532 0.2124 0.1626 0.20 0.5669 0.5951 0.3421 0.2513 0.30 0.7846 0.7659 0.4453 0.3311 0.40 0.9319 0.8663 0.5285 0.4082 0.50 1.0000 0.9305 i 0.6075 0.4925 0.60 0.9834 0.9725 0.68.79 0.5866 0.70 0.87801.0100
0.7787 0.6963 0.80 0.6806 1..0215 0.86450,8064
0.90 0.3886 1.0236 0.9401 H0,9104
0.95 0.2065 1.0141 0.9719 0.95701.00
1.0
1.0
1.0
CONCLUSION
Theoretical results have been presented for 2-bladed SC
propellers having expanded area ratios of 0.3, 0.4, and O.5; for 3-bladed SC propellers having expanded: area ratios of 0.4, 0.5, and 0.6, and for 4-bladed SC propellers having expanded area ratios of 0.5, 0.6, and 0.7. This theoretical series should be of great value, if only in a qualitative way, in predicting the performance of SC propellers due to variations in number of blades and expanded area ratio.
Caution must be exercised in using these results in any but a
qualitative way. This is especially true for designs which deviate too
much from the optimum efficiency curves. Experimental results indicate
that, as would be expected, there is more of a variation from the theoretical
results than for subcavitating propellers. The theory used is the best
available for such propellers, but questions arise as to the validity of
the lifting surface corrections used as well as the lift and drag
characteristics available for SC sections. These questionable areas
should not detract from the usefulness of the series presented since the relative characteristics of different propellers would be expected to change little.
AC KNOWLEDGMENT
The author wishes tç thank Max. H. Morris, Inc. for their help in preparing the data for publication.
REFERENCES
1. Tachmindji, A. J. and Morgan, W. B., "The Design and Estimated Performance of a Series of Supercavitating Propellers," Presented at the Second Symposiwn on Naval Hydrodynamics (Aug 1958).
2, yenning, E. Jr. and Haberman, W. L., "Supercavitating Propeller Performance," Presented at the 1962 Annual Meeting of the Society of Naval Architects and Marine Engineers.
--/
3. Hecker, R., "Experimental Performance of TMB SC Propellers,"David Taylor Model Basin Report 1432 (in preparation).
Caster, E. B., "TMB 3-Bladed supercavitating Propeller Series," Dadd Taylor Model Basin Report 1245 (Aug 1959).
Morgan, W. B., "Optimum Supercavitating Sections," David Taylor Model Basin Report C-856 (Aug 1957).
Lerbs, H. W., "Moderately Loaded Propellers with a Finite Number of Blades and an Arbitrary DistributiOn of Circulation," Trans-actions, Society of Naval Architects and Marine Engineers (1952).
Hecker, R., "Manual for Preparing and Interpreting Data of Propeller Problems Which Are Programmed for High-Speed Computers at the David Taylor Model Basin," David Taylor Model Basin Report 1244 (Aug 1959).
MOrgan, W. B., "Centroid and Moment of Inertia of a
Supercavitating Section," David Taylor Model BasIn Report 1193 (Aug 1957).
APPENDIX A
Cri DIAGR AMS FOR TMB Sc PROPELLER SERIES
Maximum Efficiency for a given C1,ij2
-Maximum Efficiency for a given CT.
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10 U 1.2 13 1.4 1.5 1.6 17 Speed Coefficient JFigure ii
- CT-J
Diagram for TMB 4-Bladed SC Propeller Series, EAR = 0.7
%1.9.8°:i
II
I
I
0
II'I
I
04.*Ipii
1.8I
urnitir';
I
I__1III'IN. :°
ti
I__
iiiiir.
Q70IUO.5
:74
076 Efflciency 18 19ao
1.4 13 1.2 I.' 1.0 0.9 0.8 0.7 0.6 0.5 0.4 0.3APPENDIX B
Cp.i DIAGRAMS FOR 1MB SC PROPELLER SERIES
Mazurnum Efficiency for Constant C,/J°
...i...-.. MozumumEtfic'uency for Constant Cp I
L WD04.05 06O7
II iii
5"
11111
IkA
I1II'.
I;
P/Douuurniiiu'
U....
UUUUUUUUUUU 06
0.76UUUUUIUUU.
07-09 to
1111111111
1.3 4 P/Do 2.5 20 0,I 0.2 0.3 04 0.5 Ô6 0.7 08 09 Speed Coefficient JFigure 2a - C-J Diagram for TMB 2-Bladed SC Propeller Series, EAR =
0.3
1.0 I.' 20 1.9 I.e I? 1.6 '.5 14 13 1.2 9 9 0.7 0.6 0.5 0.4 0.2 0.I
1.6 '.5
"I'll"
...__
uguuiohiz
0.9 .1III
1.-I I I I I i... ..;.... ,. , 2 1.2 1.4 1.6 !I
r
I'
18. P/DOuIIuIiI I!1
IHIIILI
1.2 1.4 -2.0 .8 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0 1.1 1.2 1.3 1.4 1.5 1.6 1.7 1.8 1.9 2.0 Speed. Coefficient JFigure 2b - C-J Diagram for TMB 2-Bladed SC Propeller Series, EAR = 0.4
t
.25 Efficien cy-- _- 72
P/D0 2.2 2.1 2.0 1.9 1.8 1.7 I.0 0.9 0.8 0.7 0.6 0.5 0.4 0.3. 0.2 0.1, Maximum Efficiencyfora iven -A Q4 u6 0
,.
p,ruirUwii
'
IIUh1I11ro
iflhiIIlIHhllIflhIIIIHhIIHI
EuuIrnsiI
IIIMtWiii&1II1IIIUIIIIIIIIUIflhIIB
..III1fluhIUlLI.
-'.UlUNIU1iLS
UUUliU*1111L1IUi MU
U....
LIIUUUUU
UUUUUUII1I1W1
Efficlencuu
..UU.UUU&i&1Ui
Ui... *UUU
a65lU
0.72
U...
0.6 20 0.7 Q...U..UUUI
- . 16Maximum Efficiency for a given C/J21
I -1
0 0.1
02 03 04 Q5 06
0.7Q8 ü9
1.0 1.1 12131.4
15 16 1.7 1.8 l 2.0Speed
Coefficient J
Figure 2c - C-J Diagram for TMB 2'Bladed SC Propeller Serios, EAR = 0.5
26 2.0 '.9 18 17 1.6 '.5 '.4 '.3 .2 I.' I.0 09 0.8 0.7 0.6 0.5 0.4 0.3 02
2.3 2.2 2.1 2.0 1.9 1.8 '.7 1.6 1.5 1.4 1.3 12 Ia. LU LI l.0 0.9 0.8 0.7 0.6 0.4 0.3 02 27
Moximurn Efficiency for a given Cp,'1j2
Maximum Efficlenc for a Iven
C
-iu
-II1i1i:uIHIHhIH
1
I&iIiSflU ____________
!IiIUL1I1!iiIIUIIIH____________
-I11IUi9hIIHI
U
IIHII1%1
411
nu!LIii!!r
SUUEff
0.55 0.60 0.65 0 0.102 0.3
0.4 0.5 0.6 0.7 0.8 0.9 1.0 1.1 1.2 13 1.4 15 1.6 1.7 18 1.9 2.Ô Speed coefficnt JFigure 2d
- C,-J Diagram for TMB 3-Bladed SC Propeller Series, EAR = O4
0.1
UIIIIIHH1llN1Iil
1.9 -
1.40.4
0.3 0.2
,MoiimUm Efficiency for o given
Moilmum Efficiency for 0 given Cp
Op/p/ .___
lIWIl
i.o0 'I 'IiiiT ::
L
Ufll!flW
I*I__
__
2.5I__
UURNRUII
0.9 1.0 0.1Figure 2e C,-J Diagram for TMB 3-Bladed SC Propeller Series, EAR = 0.5
28 - os os 0.7 0.0 09 1.0 .2 Speed Coefficient J 2.0 1.9 i.e I.? I.e I.e 1.4 '.5 0.9 0.8 0.7 0.8 0.5
0.9 0.8 0.7 0.6 0.5 0.4 0.3
02
0.I P/EV
Effic y for a given
C1j2
1 1 14
0Max urn Efficiency for a given Cp
1 III
I2 14...
'.8
1
'.9
'!--.
1.0 1.60
0.102 0.3
0.405 0.6
0.7 0.8 0.9 1.0 1.1 1.2 1.3 1.4 1.5 1.6 1.7 1.8 1.9 2.0 Speed Coefficient JFigure 2f - C,-J Diagram for TMB 3-Bladed SC Propeller Series, EAR = 0.6
1i
I. \"
p,,11It1
Eff1:iII
0.60 0.65 0.70 0.72 0.74 0.76 29 1.2 1.4 2.1 2.0 1.9 1.8 1.7 1.6 15 1.4 132.3 2.2 2J 2.0 1.9 1.8 1.7 1.6 IS 1.4 1.3 1.2 I.' 1.0 0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 ' I
Maximum Efficienc for a iven Cp,ijt
UNUU.U.UUUUlUU
IlHPI!i1hiiIIiIHHHIHHIH1HH
uii..
'D0 0.9...U...UUUUUNUUNU
iUIEiUi
LOiiiiUI1!IIIIH1HhIHIIIIIIHIHhIII
....iiiiii,iri1iii.uuuUl.U.UUUUUUUUU
UUtIIIHh1UIUI L4
U1IUII1iIII11 UR....UUUUUUUUmU
NUUNiI1i1itSIUU r,
U..U..UUUUUUUUU
D0 ...u...a.
::::%iHflHIuI1flhIIHHH
Efficiency '.50 a70 0.55UU
0.60 0.650.70 UUU
8..
U
urn....
°
0.8uuuuuu
111111
I.g 0 0.10.2 03 04 05 0.6
0.7 0.8 0.9 1.0 1.1 12 13 1.4 1.5 1.6 1.7 1.8 1.9 2.0 Speed Coefficieni J I I I T. I .I I LFigure 2g - C-J Diagram fr TMB 4-Bladed SC
Propeller Series, EAR = 0.522 ai 20 '9 1.8 '.7 l.6 1.5 14 1.3 12 I0 a9 Q8 0.7 0.6 05 04 03 02 0.1 I I
Ill
IMaximum Efficiency far a Given C,/J2
II
III
Maximum Efficiency far a Given C
H
p/Doi.0liii
1 0.9i p,r,0.8
. DOAI
P/DnaI'hIflU
04Ii'
iiii
.iiiini1iI1!I
I
I.
-.,' ----2
2.0mr.uu
EffIciency...
i=_ 8:
[2 1.4 050 1631
0 0.1 0.2 0.3 4 0.5 0.6 0.7 02 0.9 1.0 1.1 1.2 1.3 1.4 1.5 1.6 I.? 1.8 1.9 2.0 SPEED COEFFICIENT, JMaximum Efficiency for a given CpjZ
Maximum Efficiency for a given Cp
I,
0Q
0:c1. 4UUii
'A1I1tl
__Ofl
t1III!iflU
rnviiiii'
__InhIiIw0p
2.51
____I1L1iii!1!tIiL
____
in
ui
I
____-
___
-uuuu
uuuluUUUI__
-09
-u
I1.2
14 1.6 0 0.1 0.20.3 04 0.5
0.6 0.7 0.8
0.9 1.0 1.1 1.2 13 1.4 1.5 1.6 1.7 1.8 1.9 2.0 Speed Coefficient JFigure 2i - C-J Diagram for TMB 4-Bladed SC Propeller Series, EAR = 0.7
32
i
-Ef-0.60
-070
0.76IILllliIiki 'IRkII*k'!
____
IIRIWiI
'/D0..
0.61nSV
2.2 2.1ao
19 1.8 1.7 1.6 1.5 .4 .3 1.2 1.0 0.9. 0.8 0.7 0.6 0.5 0.4 0.302
0.IAPPENDIX C
BLADE THICKNESS FRACTIONS FOR TMB SC PROPELLER SERIES
0.09
0.08
0.07
0.06
0.05
LI-0.04
0.03
0.02
0.01
JI 5
m1.2
__
_
H
I_
I
IqiAwAr4riu
Pd
ri
i, yr
0.20
0.40
0.60
0.80
1.00 1.20I40
160
0.07
0.06
0.05
0.04
LiI-0.03
0.02
0.01
J
I.ii.o
I/
0.8
4
06
05
FIV1A1
)7
4
0.3
0.20
040
0.60
0.80
L00
1.20140
1.60007
006.
0.05
0.04
ILI-0.03
0.02
0.01
8
.7.
AVA9. 0.6
0.5
I.0
J=I.5
0.20
0.40
0.60
0.80
1.00
1.20 1.40 I .60 'YCT0.07
0.06
0.05
0.04
LiI-0.03
0.02
0.01
4M
;3
- rrrr
I.'
1.00.9
J=I.5
1.48
0.7
0.6
0.5
04
0.3
0.20
0.40
0.60
0.80
1.00
1.201.40
1.60Figure 3d
0.07
0.06
0.05
0.04
003
0O2
!.ol
0
I.AAAA
-± !hVFIKAVA
A
1.0 0.9 0.8or
0.6
0.5
:0.4
0.3
0.20
0.40
060
0.80
1.00
.20
1.401.60
Figure 3e - Blade Thickness Fraction for TMB
3-Bladed SC Propeller Series:, EAR
0.07
0.06
0.05
0.04
LLI-
a)0.03
0.02
0.01KA
08
Ii
0
II
0.5
04
__AVAI
-_______I
I
Figure 3f - Blade Thickness Fraction for TMB 3-Bladed SC Propeller Series, EAR
= 0.6
0.20
0.40
0.60
0.80
1.00 1.20 1.40 1.600.07
0.06
0.05
0.04
0
0.02
0.01
JI.5
.4-
1.3A
05
0.4
i:ii
½'
0.20
0.40
0.60
0.80
I.00
1.20 1.40160
Figure 3g - Blade Thickness Fraction for TMB 4-Bladed SC
0.07 0.06
0.05
0.04
0.03
002
Q.0I/
0 4JI.5
1.4 244'.'
AVArV
V VO7
,03
r
r
r
0.3 0.20 0.400.60
080
1.29140
I.600.07
0.06
0.05
0.02
0.01
J:15
I.0.7
0.6
0.5
0
3
0.20
0.40
0.60
080
100
1.20140
1.60Figure3i - Blade Thickness Fraction for TMB 4-Bladed SC Propeller Series, EAR = 0.7
0:04
APPENDIX D
PITCH CORRECTOON COEFFICIENTS FOR TMB Sc PROPELLER SERIES
20
1.8
1.6
1.4
12
10
08
0.6
0.4
0.2
44
002
004
006
008
010
012
014
016
018
0'0
0.22
a07
Figure 4 - Pitch Correótion Coefficient (C
for Finite Cavitation.Numbers for
0.16 0.15 0.14 0.13 0.12 0.11 0.10 0.09
a
ooe (10? 0.06 0.05 004 003 0.0iJ.
1.5 1.4 '.3 1.2 1.1 1.0 0.9 0.8 0.7 0.6/
0.5 0.4 0.345
Figure 4a - Pitch Correction Coefficient A(P/D) for Finite Cavitation Numbers for TMB
2-Bladed SC Propeller Series, EAR = 0.3
0.16 0.15 0.14 0.13 0.12 0.11 0.10 0.09 a 0.08 0.07 0.06 005 0.04 0.03 0.02 0.01 0 0.1. 02 0.3 0.4 0.5 0.6 0.7 0.8 0.9 I.0 1.2 1.3 1.4 1.5 1.5 ''.3 1.2 1.0 0.9 0.8 0.7
/
JIlL
06 "IA'-0.5 0.4Figure 4b - Pitch Correction Coefficient
(P/D) for Finite Cavitation Numbers for TMB
2-Bladed SC Propeller Series, EAR = 0.4
46
0.10 0.09 a 0.08 0.07 0.06 0.05 0.04 0.03 0.02 0.01 l.0 0.9 0.5 0.6 0.4 0.3
47,
0.16 015 0.14 G13 0.12 Oil J: 1.6/
1.5 1.4 '3 2 I.' 0 aI 02 03 4 0.5 08 07 08 09 10 I.' '2 1.3 14Figure 4c
Pitch Correction Coefficient A(P/D) for Finite Cavitation Numbers for TMB
2-Bladed SC Propeller Series, EAR = 0 5
/
0.80.15 0.14 0.13 0.10 0.09 a 008 0.07 0.06 0.05 0.04 1.6 1.5 1.4 1.3 12 0.9 0.8 07 0.6 0.5 0.4 0.3 0 01 02 0.4 0.6 0.7 08 1.0 II 12 1.3 1.4 L5
0.16 0.15
0(4
0.13 0.12 0.11 0.100.09
0
0.010.06
0.050.04
0.030.02
0.010.8
uiuu
0.60l
0.2. 0.3 0.40.5
0.6
0.70.8
0.9
1. 1.1 u.i.
1.4 5Figure 4e - Pitch Correction Coefficient i (P4)) for Finite Cavitation Numbers for TMB
3-Bladed SC Propeller Series, EAR
0.5
cU6 0.15 0.14. 0.13 0.12 OH 0.10 0.09 0.06 0.05 0.04 003 002 0.01
I
I
H!JPJ:t
/
I41ii1iiL1
0.7/
0.6 0.5 0.4 0.3 50 oP 0.2 03 0.4 0.5 0.6 0.7 08 09 10 12 13 14 1.5Figure 4f - Pith Correction Coefficient A(P/D) for Finite Cavitation Numbers for TMB
3-Bladed SC Propeller Series, EAR = 0.6
0 0.15 0.14 0.13. 0.12 0.11 0.10 009 Q 0.08 0.07 0.06 0.05 1104 0.03 i 1.4 .3 1.2
I
jI.0 0.9 0.8 .0.7/
0.5 0.4 0.6 0.3 0.2 0.3 04 0.5 0.6 07 08 09 0 0I 1.0 1.2 1.3 .4 .5016 0.15 0.14 0.13 0.12 0.11 aI0-O.09 0.08
I
0.07 0.06 0.05 0.04 0.03 002 0.Q 52 0 a' 0.2 03 04 Q5 0.6 07 08 09 10 1.2 13 14 (.5Figure 4h - Pitch Co'rectionCoefficient A(P/D) for Finite Cavitation Numbers for TMB
4-Bladed SC Propeller Series,
AR = O6
1! 1.6 1.5 1.2 I.' 1.0 0.9 08 0.4
V
.4
0.3crrrpPv
pr
0.16 J. 1.5 0.15 '.4 a" I.0 010 0.9 0.14 1.3 0.13 .1.2 0.12 I.' 0 0.I 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0 1.1 1.2 13 1.4 15
Figure 41 - Pitch Correction Coefficient A (P/D) for Finite. Cavitatjon
Numbers for TMB4-Bladed SC Propeller Series, EAR
= O.753
/
0.8 07 0.07___M1VAW1iA
0.6 0.5Iffff4d
ill
I 0.09 0.08 0.06 005 0.04 0.03 00l ,0.4 0.3APPENDIXE
MAXIMUM FACE ORDINATES AT O.3 O5O.7, AND 0.9 RADIUS FOR
TMB .SC PROPELLER SERIES0.10 0.09 0.08 0.07 0.04 003 0.02 00I
A.
!
riiiiiiirnuiiuwm
iiiiiiuir
uI,iii,AiHiI
UViVAiPrUW4Nl__ A
iiuui___
AiiiiU
04 D 1.5. 11.4 1.3 1.2 0.5 0.3 0.1 0.2 0.3 0.4 0 5 0:6 0.7 0.8 0:9
I0
1:1 1:2'3
'4
Figure5a
Maximum Face Ordinate at .0 3 Radius for TMB 2-Bladed SC Propeller Series, EAR
= 0.3 1.1. I.0. 0.9 0.8 0.06 max 0.05
vu
= j'y
'8OUe .IeIIedOJclpepI- fflj,
J snpj rO
eUpJ eoj
wnwLxp
-qQ Oãfl!jj 131% ci i Fl 01 6080'LO
90 co o £0 I0 P.OillløØpV/
I41111/
90 10pr,'
80. 60 I.' ciucr
100 z0.0 £0.0t00
80.0 600 °lrO 0 coo In .xow 1/i 90.00.10 0.09 0.08 0.07 0.06
Y/.tmax
0.05 0L04 0.03 0.02 0.01
Iiviur_1__A__w_It
It,i,AVAVIr4ii,AIIr__I
va,iriIriIr1Iprd
,r
pPP -'0.3 1.5 1.4 1.3 1.2. 1
H
Ii
ill
if 11U4.
01 02 03 04 05 06 07 08Figure 5c
- Maximum Face Ordinate at .0.3 Radius fr TMB 2-Bladed SC Propeller Series, EAR = 0.5
09 10 II 12 13 14 15
0.10 0 09 008 0.07 0.06 1mox 06 0.5 J I 5 1.4 .1.3 1.2
Ii
lo
0.4 0.31
AiAAA
A
,iuiusii
Figure 5d - Maximum Face Ordinate at
.3 Radius for TMB 3-Bladed SC Propeller Series, EAR
= 0.4 13 0.05 0.04 0.02
,0l
0 0.030I
02 0.3I0
04 05 06 07 08 09OiIV '°ØS JOHOdOJd3S P°PIfl-2 WL JOJ SflIPll
OUUipJ0e3,J WflWIXU-91
121
1ri.
oi
60
80L0
90
90
O20
Oro
4iIUiU
Jl1iu1liLiLii44/4d1uuuII
Iiuu!ii!IHhIHH
IiHHfl1PIIIUIIHIH
iiiuiini:iiiiiuiuiiiuu
l'J!flJJ
1111111111
UII
4
A
1£1 bi 9il
I00
oo
200
U)900
900
£00
600
010
0J 0 0.09 0.08 0.07 0.06
o
0.05: 0.04 0.03 0.02 0.0l AV
A
j
1.4 1.3: 1:2,//
H4
14
0.9/
0.8 0.7 0.6 0.5 .3 0 0.I 0.2 0.3 0.4 0.5 0.6 07 0.8 0.9 l.0 1.2 13 14 '.50.10 o.oe 0O7 006 005 0.04 0.03 0.02 0.01
HIIIiUIH III
_______IIIIMII!iiiI__06
uuirirwirijiuriur
_______I1tVAVM1UUI4 r
_______r1,Aur4uruuruw
_______M7IUUr
-0.3 0.5 0.4 0 01 02 03 04 05 06 07 08 09 10 II 12'3
'4
15Figure 5g
0.10 0.09 0.08 0.07 0.06 y/A max 0.05; 0.04 0.03 0.02 0.01 J L4 1.3 1.0 I
JAA
A
III Iiiiiiii!I
HIIiiiNiiiiiflI
li&VAUJiUiNiU__
AiUiIUI
0.9 0.6 0 0.1 02 0.3 0.4 0.5 08 07 0.8 0.9 I 0 ! 1.2 3
'4
15Figure 5h - Maximum Face Ordinate at 0.8 Radius for TMB 4-Bladed SC Propeller Series, EAR
(.J 0.09 0.08 0.07 0.06 0.05 0.04 0.03 0.02 0.01 I.'
I
0.9 08/
0.6 0.4 0.5 Jn 1.5 1.4 1.3 1.2 0.(0 0.9 1.0 1.2 1.3 0 0.I 0.2 0.3 0.4 0.5 0.6 0.7 0.8Figure 5i - Maximum Face Ordinate at
0.3 Radius for TMB 4-Bladed SC Propeller Series, EAR = 0.7
1.4
0.06 0.0 I 1.51. 1.3 1.2 i. 10 9
11111 II! uIiii!1iiIII1II
04.aaa.aI,IAw1F1,iill.r4IlUIUlI
0.31
lIlWWIIlilIIU1lIIUl
II V
141 II .l.Uill U
I
2Figure 6a - Maximum Face Ordinate at 0.5 Radius
f
TMB 2-Bladed SC Propeller Series, EAR = 0.3
0.8
02
0 10 009 0'08 007 006 max c 0.05 th 0.04 0.03 0.02 0.01
IIuhiiIjIqIuuI
0.?II1IIiiiIiiHhIi1
I',wj,iiiu'uiuI
IDDuPJHUUIHt
0.5 04 0.3 0 01 0.2 03 0.4
05
06 0.7 0.909
1.0 I.' 1 2 13 I A Figure Ob- Maximum Face Ordinate at 0.5 Radius for TMB 2-Bladed SC Propeller Series, EAR
aio 0.09 008 0.07 0.06 0.05 0.04 0.03' 0.02 0.01
,
i1ii!
0.7
0.6
Ir1i1NVjVAiiVUr
I1MII1UUU411
1qv4riru!iuPJ-
ffiFAUUU
lip
0.4 03 01 02 03 04 05 06 '07 08 09 I0 'I F 12 3 I 4 I5Figure 6c - Maximum Face Ordinate at 0.5 Radius for TMB 2-Bladed SC Propeller Series, EAR
OLIO 0.09 0.08 0.07 0.06 max
-0.05 0.04 03 0.02 0.01Aii
d
MPJIII11___
NUViiIW1iiUi___
iiL!JUPUUP
WPIilP2U_
r
iuuu
J I. 1.4 1.3 r.2 1.1 0. 0.7 .8 1.0 0.6 00I
02 0.3 04 05 06 07 08 0.9 10 12'3
14'5
Figure 6d - Maximum Face Ordinate at 0.5 Radius for TMB 3-B laded SC Propeller Series, EAR
0.01
J:I.5 1.4
1.3 1.2I 1UP
-I
0.9 0.8P1!
0.7 0.6/IJA&A14i
0.5 0.4 0.3 0.10.2
0.3 0.4 0.5 0.6 0.708
0.9 1.0I.'
1.2 1.3Figure 6e
- Maximum Face Ordinate at 0.5 Radius for TMB 3-Bladed SC Propeller Series, EAR
= 0.5
0.10 0.09 0.08
007
0.06±
0.04
0.03 0.021.4
0.10 0.09 0.08 0.07 0.04 0.03 0.02 0.01
0.3
IIi iiI1IiiiiIi
II!AIIIHHHIH___
UFiii AU VAUuUi__
rir1rir4iIUU
/AUiUIPNUUUP'
1.5 1.4 1.3 0.6 0.5 0 0.1 0.2 0.3 04 0.5 0.6 0.7 0.8 09 1.0 I 2 3Figure of - Maximum Face Ordinate at
0.5 Radius for TMB 3-Bladed SC Propeller Series, EAR = 0.0
14
'5
0.10 0.06 0.04
03
0.02 0.0IJI.5
1.4 1.3 I.044
0.9IIIIIIIIIHAIUI
4,i.I.PIUI.
0.8 0.7 0.6 0.5 3 0 01 0.2 03 04 05 06 07 08 09 I0 12Figure 6g - Maximum Face Ordinate at 0.5
adius for TMB 4-1laded SC Propeller Series, 1AR
= 0.5 0.09 0.08 0.07 0.3 IS 0.4 14
0.7
____
J5 1.4
1.3 I214111
0.6UV1V1!1iiMVAUUVAi______
I VAM
U VIUUU V
VA!IVAVAVUIIrdUUPA
--.
i,AUUPi___
AU44UUIU_____0.'JUUU-
JiUUUiU
-0.9 -1 0 12'3
0.10 0.09 0.09 0.07 0.06. 0.05 0.04 003 002 0.01 '0 0J 02 0.3 0.4 0.5 ,0 6. 07 0.8Figure 6h
- Maximum Face Ordinate at0.5r-Radius for TMB 4-Bladed SC Propeller Series, EA
0.6
14
0.10 0.09 0.08 0.07 0.04 0.03
A______
urnrM1i!1VAi__
IiiIWU!1VAUVAU
I WA VA
WA__
iriiurirwiirnu
/IIu"
0.5 0.6 0.4 J -1.5 1.4 .3 1.2 l.1 1.0 0.9 .8 0.7Figure Gi - Maximum Face Ordinate at 0.5 Radius fcr TMB 4-B laded SC Propeller Series, EAR = a7
0.02 0.0I 0 0.1
02
03
04
05 06 0.7 08 09I0
2 13 '.4 '.50.10 0.09 0.08 0.07 0.06 y6 .'mox 0.05 0.04 0.03 0.02 0.01
I
A1HIii____
____WVAiPiilI
.4
____
__
AIdUIUI
0.3 J .15 1.4 13 1.2 1.1 1.0 0 0.8 0.7 0.6 0.5 0 0 I 0.2 0.3 0.4 0.5 0 60 7%/S 0 8
09
I0
12 13Figure 7a - Maximum Face Ordinate at 0.7 Radius for TMB 2-Bladed SC Propeller Series, EAR = 0.3
14
0.09 0.08 0.071 0.06 y mox 0.05 0.04 0.03 0.02 0.0I
4Ll1
"A'
JV1W
VU V
w
441(411
rr.,p-pp
1.0 0.51
0.3 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7,- 0.8
0.9 1.0 1.1 1.2 1.3i/c,
Figure 7b - Maximum Face Ordinate at 0.7 Radius for TMB 2-Bladed SC Propeller Series, EAR = 0.4
/
0.4 1.4 I.5 0.I0 J,.I. I4 1.3 12 LI:/
/ /
0.9as
0.7 1 0.60.10 0.09 0.08 0.07 04 0.03 0.02 0.01 0
I__l.5
1.4__U1UIIEU.I III
ilIøltWUVlo.9 N...
I__i11IAiiII1I!UU
I ItII1I1 VAN WINI
0.6
I IJiiAiiHhIiii_
IV1NAAIVIIVAN!4___
.r1'vA,iv....iiw
Y!ANIPIdIII___
0.4
0.3
0.5
Figure Ic - Maximum Face Ordinate at 0.7 Radius for TMB 2-Bladed SC Propeller Series, EAR = 0.5
2 13 14 15 0I 02 03 q.4 05 06 07 08 09 10 a06 Y/Im G05
0.10 0.O9 .
I.
0.9 08.111111141
0:5 0.4 0.3 J 1.5 4 1.3 1.2 1.1 0.6/
Figure Td - Maximum Face Ordinate at 0.7 Radius for TMB 3-Bladed SC Propeller Series,, EAR
ü4
0.06 mo 0.05 0.04 0.03 0.02, 00II 00I
02 03 0.4 05 06 08 09 I 0 I 2 1.3 14 5 0.08 0.070.10
0.04
0.03
0.02
0.01I
J.l5 1.4
1.3I.2_I.I
41
A
444
.0
a5
0.4 .3c.
Figure 7e - Maximum Face Ordinate at 0.7 Radius for TMB 3-Bladed SC Prc?eller Series, EAR = 0.5
0.9
1.0 1.1 1.2 I. 3 14 1.5 0. I 0.2 0.30.4
0.5
0.6 0.7.0.8
0.9 8 0.70.09
0.08
0.07 0.06 x 0 E0.10 0.09 0o8 0.07, 0.04 Q03 0.02 0.01 0 0.4 1.0 0.9 0.8
ItV1VAVAIIVAUVAUIW
rnr'ivAwi'.rA..r
,,i,,.T1r4Ii.
0.6 0.5 J 1.5 1.4 1.3 l2 0.1 0.2 0.3 04 05 0.6 07 0.8 0.9 10 I. I 12 13
Figure 7f
- Maximum Face Ordinate at 0.7 Radius for TMB 3-B laded SC Propeller Series, EAR = 0.6
1.4
1.5
0.06
Yb 'mox.
0.10 0.09 0.08 0.07 0. .3 0.05 002
___liliiiT1VAlA.
Al__
___lVAVi1AVAliiWAU_
___IIiDIiAWAlVlt
___ 11 VA
VA
VA
__IL
___IVMJVAIVA
VA___
___iiiAVAiUVAl
__
-.
__-I/aAlr1ur4l
__/ffFiUl___
iii
0.5 0.4j 0:3 1.5 .1.4 .13 1.2. 1.1; 09 0.8 0.7' 0.6 0.04 0:03 0.01 0.1 02 03 04 05 . 06
07
08
09 I0 12 13 14 15CE
0
0.10 0.09, 0.08 0.07 0.06 0.05 0.04 0.03 0.02 0.01 .5 1.4 .3 12 1.0 I.'/
0.9/
o.e 0.7 0.6 0.5 0.4 1.4 1.3 1.2 0.9 1.0 I.' 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8Figure 7h - Maximum Face Ordinate at 0.7 Radius for TMB 4-Bladed Sc
0.10 0.09 0.08 0.07 006 0.05 0.04 0.03 0.02 0.01 a.?
I Vi IA VA VAWA I!1Ii _____V
____4l
J 1.5 1.4 1.3 1:2 I'.G 0.4 0.5 0 0.1 02 03 04 05 0.6.07 _08
09 F 0 I F 12 13 14Figure 7i
Maximum Face Ordinate at 07 Radius for TMB 4-Bladed SC Propeller Series, EAR
0.10 0.09 0.08, 007 0.06, 0.o O.04 0.03 0.02 0.01
11111111
I1iiii11F Iflhllilil
P*IPIIFIIIIIII
0.3 0I 02 0.3 04 0.5 0.6 0.7 0.8 O9 1.0II
I2 13 1.4 1.50.3
J.I.5
1.4 0.7I
!
1.0 0.9 0.8 A4111
iiA__
__wirnmvirauruu__
ih11V11W1VAill
I1F1i4iWillU
0102
03 0.4 0 060.7 ,- 08
v'T
Figure 8b
- Maximum Face Ordinate at 0.9 Radius for TMB 2-Bladed SC
Propeller Series, EAR
= 0.4 0.6 09 I.0
II
1.2 13 1.3 1.2 14 150.10 J 14 i.3 1.2 1.I 1.0 0.9 o.e 0.3
/
0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0 12 1.3 14 15Figure 8c - Maximum Face Ordinate at 0.9 Radius for TMB 2-Bladed SC Propeller Series, EAR = 0.5
0.7
/
0.6 0.5 0.4 0.09 0.08 0.07 0.06 y,Ina* 0.05 a) 0.04 0.03 0.02 0.01 00.10 0.09 0.08 0.07 0.04 0.03 0.02 0.01 J 1.5 1.4 .3 1.2 1.1 1.0
4M1iiiii1
1IuiiiPAFl!
0.5I/IA
0.7 0.6 0 01 02 03 04 0.5 06 07 08 09 10II
1.2 3Figure 8d - Maximum Face Ordinate at 0.9 Radius for TMB 3-Bladed SC Propeller Series, EAR = 0.4
4
15
0.06
max
0.10
009
0.08 0.070.06
0.04
003
0.02 0.01I
I111'41I
IIOIllhiIAUhiUi!iIiHh1!
uuuuuuurnr1rurAui u.uuuau
urn
lIIlIiVMMAV
uaiiruuiuuu
UI
IHIHIUJIPPHPI!,i
PVØl
ill
ill
l.0
0.1 0.2a3
0.4 0.506
0.7 0.80.9
.0LI
1.2 1.3 1.4 1.5Figure 8e - Maximum Face Ordinate at 0.9. Radius for TMB 3-Bladed SC Propeller Series, EAR
0.5 J=I.5 '.4 .3 1.2
0.9
0.80.10 0:09 0.08 0.07 0.06 y1'Q "max. cri 0.05 0.04' 0.03 0.02 o:oi 0 1.5 1.4 1.3 1.2
7.
I.' I.0 '.9Aiii141___
0.5iiviwiuririir
NM1Y1VAW1iUPJi________
IrA
0.7 0.6 09 I0 12 13 0.1 0.2 03 04 05 06 0.7 0.8Figure 8f - Maximum Face Ordinate at 0.9 Radius for TMB 3-Bladed SC Propeller Series, EAR = 0.6
14
y'o
0.10 0.09 0.08 0.07 0.06 P0.05 0.04 0.03 0.o2 0 0.4 1.5. 1.4 1.3 1.2A
06iiiiviwiuw__
I1AVAVAIIUV
1iW1I!1V4UiN_______
4
IA VI VNAi!1UUUU
V
rwluurlur4ird_______
-.
p
0.1.'
02 0 04 0506
07 08 09 10 12'3
Figure 8g
Maximum Face Ordinate at 0.9 Radius for TMB 4-Bladed SC Propeller Series,
EAR = 0.5
'4
0I0 0.09 0.0e 0.07 0.06 0.05 0.04 0.03 0.02 0.01 5
H
II IIIII1H1
IV1IUUL____
____VA1Ji!iViWUWAl
____IAliV1UUiWA
____W?VMM1VAIiW1UUV
-,Ai,.iw1.--A
0.7 0.6 0 01 02 0.3 0.4 05 0.6 07 08 0.9 1.0 I., 1.2 3Figure 8h - Maximum Face Ordinate at 0.9 Radius for TMB 4..Bladed
SC Propeller Series, EAR
= 0.6
14
0.10 0.0 0.07 0.0
o
0.05 0.04 0.0 002 0.0I
IIiIiUVA .0111.
lriM1rnlVAUo. I
raiiirnuawuu
NI1W1W1IVUI
WW1NAIIMIAIW1__
ra-A,A-r1-.iIw
0.7 0 I 0 2 0.3 0 4 0 5 0.6 07 08
Figure Si - Maximum Face Ordinate at 0.9 Radius for TMB
4-Bladed SC Propeller Series, EAR = 0.7
0.6 oA 4 Is 0.9
I0
12 13APPENDIX F
MAXIMUM THICKNESS ORDINATES AT 0.2, 0.5, 0.7, AND 0.9 RADIUS FOR TMB SC PROPELLER SERIES
014
0.12
O.iO 0.0810.06
0.O4
0.02
0.5
I.0/
0.9
0;8
0.7
-j
IiMA I
_IMIJ4áAV
_1IhiiiAVMd
V
_V1I4d
/1 V'
0.6
0.4
0.3
0
0.20
040
0.60
0.80
1.001.20
1.40 I .601.80
2.00
Figure 9a - Maximum Thickness at 0.2 Radius for TMB 2-Bladed SC Propeller Series, EAR = 0.3
1.4 1.2
0.02
1110.8110.6
.IV4UUI
05
Figure 9b - Maximum Thickness at 0.2 Radius for TMB 2-Bladed SC Propeller Series, EAR = 0.4
02 04 06 08 1.0 12 14 16 I.e 2.0 2.2 2.4 2:6 2.8 30 0.20 0.18 0.16 0.14 0.12 max 0.10 0.08 0.06 0.04
.0.20 0.I8 0I6. 0.14 0.08 006 J 1.5 1.4 1.3 12 1.1 1.0. 0.9
AA4.4
d1dIIId1dIIId.
H H :0.8 0.3 0.5 0.4 37 Z 2 x 0.2 EAR. 0.5 I8 20 22 24 02 04 06 08 10 124 ,-
16Figure 9c - Maximum Thickness at 0.2 Radius
for TMB 2-Bladed SC Propeller Series, EAR = 0.5
2.6 0.12
L
0.10 0.04 0.02 2.8. 300.20 0.18 0.16 0.14 0.08 0.06 0.04 0.02
iinniuii
HhIiIiIiIo.7____
.vji,.r____
4MiIiiiII
iiiiiui
0.6 0.5 0.4 0.3 () 02 0.4 0.608
1.0 12 1.4 16Figure 9d - Maximum Thickness at 0.2 Radius for TMB 3-Bladed SC Propeller Series, EAR = 0.4
8 2.0 2.2
22
2628
3.00.12
Zmox
0.12
.0.I0
0.08 0 E i:30.O6 0.04 0.02JI.5
1.3 .1.1I.00.9
08
0.7 0.6 0 5FIWJW1UU4N
4-IIFAPA
1
WilA
1A
wi4
-0.304
0.20 0.40 0.600.80
1.00 1.20 1.40Figure 9e
Maximum Thickness at. 0.2 Radius for TMB 3B1aded SC Propeller Series., F
htR = 0.5 I .600.20 0.8 0.16 0.14 0.12 max 0.10 0.06 0.06 0.04 0.02
U...
IU .H
1111111.8
IIIrFjr,
0
0.4 05 0.3 0.7 06 1.8 20 2.2 2.4 26 28 30 0 02 0.4 06 08 1.0 12 160.20 0.18' 016 0I4 0.12 0.08 0.06 0.04 0.02 0 0 2 0 4 06 0.8 1.0 1.2 I 4 I 6 I 8 20 2 2 2 4 26 28 30
Figure 9g - Maximum Thickness at 0.2 Radius for TMB 4-Bladed SC Propeller Series:, EAR = 0.5
J 1.5 1.4 1.3 1.2 II I.' 0.9 0.8 0.7 0.6 0.5
0.4
0.3
0.20 0.18 0.16 0.14 0.08 0.06 0.04 0.02 0 7 J .4l.3 1.2 1 0.6 0.5 0.4 0.3 0.2 0.4 0.6 08 1.0 1.2 1.4 1.6
Figure 9h - Maximum Thickness at 0.2 Radius for TMB 4-Bladed SC Propeller Series, EAR = 0.6
0.18 0.I6 014 0.12 0.08 0.06 0.04 0.02 020 0.6 H H
AidliLi
/
H,/f
0.4 0.3Figure 9i - Maximum Thickness at 0.2 Radius for TMB 4-Bladed SC Propeller Series, EAR = 0.7
max 0.10 0.09 0.08 0.07 0.06 0.05 I 0.04 003 0.02 0.01
!!IPV
AM4ilil
, irliflhl
0.3 00l
02 0.3 0.4 0.5 0.6 0.7 0.8 o9 l.0 12 13 14 1 5Figure lOa - Maximum Thickness at 0.5 Radius for
TMB 2-Bladed SC Propeller Series, EAR
= 0.3t/D m 0.10 0.09 0.08 007 0.06 H 0.05: 0.04 0.03 0.02 0.01
1A
i
A
.UUIWWAJUV
uriwiraiirair
iiiidt!iuIi
0.3 0 0:1 0203
0.405
06
07 0.8 0L9I0
12 13'4
1.5Figure lOb - Maximum Thickness at 0.5 Radius for TMB 2-Bladed SC Propeller Series,
.'tR 0.40I0 0.09 0.08 0.07 0.06 ti61011 0.05 (J 0.04 0.03 0.02 0.01
iuwririiirir__________
IIIF!NIV1NWA
IU1ii11JJiVAlV_______
UIWffVAVAW
6'rir4r4iiIr_______
,1iiiiUiAiV
huM'
'
rr
/tIIIIAAA
A
A
4
1/II17ArA.pP
rr,,
U 1.5 1,4 3 12 1.1 1.0 0.9 0.8 0.7 0.5 0.4 0.3 01 02 03 05 06 07 0.8Figure lOc - Maximum Thiàkness at 0.5 Radius for TMB 2-Bladèd SC Propeller Series, EAR = 0.5
0.10 J-I 41.3 1.2 iI L.. 0 0.8 0.7 0.6 0.5 0.09 0.08 0.07 0.06 0.05
0
0.04 0.03 a02 0.0I 0UP7MAV
,r
li9ppii
i4liliiii
0.4 0.3 09 10I!
12 13 14 15 0.1 0.2 03 04 05 06 07 080
U' 0.10 0.09 0.08 0.07 0.06 a E 0.05±
0.04 0.03 0.02 0.01/
0.6 0.5A
0.4./r
0.3 1.3 1.4 1.50
0.102
0.3 0.4 0.5 0.6 0.70.8
0.9
1.0 1.2Figure lOe - Maximum Thickness at 0.5 Radius for TMB 3Bladed SC Propeller Series, EAR
0.5I I
0.10 0.09 0.08 0.07 0.06 ti3O 4mox 0.05 0.04 0.03 0.02 0.01
.JI.5I.
1.3 1.21.1 1.0 09 0.8 0.7 O.b 0.0uiiuum
ill..i
IW4UU4lU1UPgU aiii
v
Oi 02 0.3 04 05 0.6 0.7 08 09 10
II
12 1.3 4 1.50.10 0.09 0.08 0.07 0.06 0.05 0.04 0.03 0.02 0.01 0
uu:rjjririipju_________
iiuurniiiiwirii__
iiu!fviriiirivapuv
.IvrffA,.pi.rn____
II. rI1rrir4ui_________
II
PA
1UI________
riiirniu
iiuuiuiu
U2_I.I
10 0.9 08 0.706
05
0.4 0.30I
02 03 04 0506
0708
Figure lOg - Maximum Thickness at 0.5 Radius for TMB 4-Bladed SC Propeller Series, EAR = 0.5
a
90 = LV
'S9!JOS °I1°'°d 3S pepj-f ffltL °J 'Pl
0 BBOU)tOL4j. UIflUIiX
- 401 OflI
±2t
tO tO 01ri
31 SI L0 9O G0 O O 30 IO 0.i.i..Iii
UI...
Hi
!j
jp1pJiJJIJiJpp/iI'iiiH
::H
1.1 7.1 Li i c;i - pu--I''
P00 1000l0
L06'
600 coImoii 0.10 009 0.08. 0.07: 0.06 H 0.05
0
0.04 0.03. 0.02 0.0I J .5 1.4:13 12 1.1 1.0 0.9 . 0.8uuiiiiu
I1J1WiiiiHPJH___
iIIII VIA
IIFIIII1IIIIIOI
0.7 0.6 0.3 0:4/
05Figure lOi - Maximum Thickness at 0.5 ?.ad.ius for TMB .4-Bladed SC Propeller Series, EAR
0.7Z.4
0.5 E.A R 0.70.10 0 09 008! 0.07 0.06' max 005
0
004 0.03 0.02 0.01 0IIIflIILiI______
i:iiiiEiR1ii_
IIU1HiRI1
IRRRdl
RWiiP
Iuiip
p;pr
iir
0.3Figure ha - Maximum Thickness at 0.7 Radius for TMB 2-Bladed SC Propeller Series, EAR = 0.3
0.10 009 0.08 0.07 0.06 max. _i 0.05 0.04 0.03 0.02 0.01 J .5 I 1.3 1.2 1.1 1.0 08 0.7 0.: 0.5
IUIlJJ1TiUi4W1W1UI1UUU II
111111
..U.,rI.r4UI.uUUIr4IUIIU
4i'JXII!i1ii!iiiiili
.INI
IIIIPIUIUUIIUUI
!,PI1!PIPV
0 F 02 0.3 04 0.5 06 07 0.8 09 1.0II
I 2 13 14 IS0.10 0.09. 0.08 007 0.05 0.04 0.03 0.02 00 I 0
UUiU
i:. Ii 1.0U
08:uuin v i-i
0.4I____________
//ilM4WAiUIlIUU
liIUPIII
1rlHiiIIIIIII
IUIUIIIIUUIU
7N$DIVAWAIIIIU__
___AAU
UI
1.11
Ii
I__
01 0.2 03 04 05 0.6 07 0.8 09Figure lic - Maximum Thickness at 0.7 Radius for TMB 2-Bladed
10 2 13
SC Propeller Series, E.R
= 0.50.5
mo 0.10 0.09 0.08 0.07 0.06 005 0.04 0.03 0.02 0.01 0
uuiiiiiiuiumi'__H
Ill
VA VA VA VAU
uivivivwiariuuv
/AWAiHiIiiIiIl.
6 0.4 05 O3 0I02
03 04 05 06 07 08 09 I0 12 I 3Figure lid - Maximum Thickness at 0.7 Radius for TMB 3-Bladed SC Propeller Series, EAR
0.40.10 J=I.5 1,4 1.3 1.2' 1.1 1.0 0.9 0.8, 0.7 0.6, . . 0.5 0.09
0.08.
0.040.03'
--
--a - - - - I
VAllrdlll!iIIIIII
&
iiVUi Al Al All
I Ill
0.07
PiHh!IF 11111
0.06
A1diHhi!iI
PU!
IIIpriAflUiHiiflhiiiIIIII
002
llFdJIHdIHuIIIHIH11111I
.0 r 0.1 0.2 0.3 0.4 0.5 0.6 0.70.8
0.9 1.0 1.1 12 1.3 1.4 1.50.10 0.09 0.08 0.07 0.06 0.05 0.04 O3 0.02 0.01 J 1.5 1.4 1.3 1.2
Ii
LO 0.9 0.8 0.7 0.6RiiihAiUiIIUiiiIIUUii
uuuuauuuuii
p
v vr'p
0.1 0.2 0.3 04 0.5 06 0.7 0 8 09 1.0 12 1.3Figure hf - Maximum Thickness at 0.7 Radius for TMB 3-Bladed SC Propeller Series, EAR = 0.6
0J0 0.09 0.08 0.07 0.06 0.06 0.04 0.03 002 0.0I 0 0.9 0.8 0.7 0.6 05 0.4 0.3 0.1 0.2 0.3 0.4 05 0.6 0.7 0.8
Figure hg
- Maxiniuni Thickness at 0.7 Radius for TMB 4-fliadéd SC Propeller Series,
E.&R = 0.5