nasa technical note 1 · 2013-08-31 · the static efficiency and propulsive efficiency computed...

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NASA TECHNICAL NOTE NASA TN D-3122 - L?-. 1 a_. .cI Ln w x "5 z E PERFORMANCE CHARACTERISTICS AT ZERO ANGLE OF ATTACK FOR SEVERAL FAN BLADE ANGLES OF A 4-FOOT-DIAMETER DUCTED FAN Ames Research Center Moffett Field, Calif. NATIONAL AERONAUTICS AND SPACE ADMINISTRATION - WASHINGTON, D. C. - DECEMBER 1965 https://ntrs.nasa.gov/search.jsp?R=19660002851 2020-04-08T16:16:44+00:00Z

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Page 1: NASA TECHNICAL NOTE 1 · 2013-08-31 · The static efficiency and propulsive efficiency computed from the faired curves of figure 4 are presented in figure 6. The static efficiency

NASA TECHNICAL NOTE NASA TN D - 3 1 2 2 - L?-. 1 a_. .cI

Ln w

x

"5 z E

PERFORMANCE CHARACTERISTICS

AT ZERO ANGLE OF ATTACK FOR SEVERAL FAN BLADE ANGLES

OF A 4-FOOT-DIAMETER DUCTED FAN

Ames Research Center Moffett Field, Calif .

N A T I O N A L A E R O N A U T I C S A N D S P A C E A D M I N I S T R A T I O N - W A S H I N G T O N , D . C . - D E C E M B E R 1 9 6 5

https://ntrs.nasa.gov/search.jsp?R=19660002851 2020-04-08T16:16:44+00:00Z

Page 2: NASA TECHNICAL NOTE 1 · 2013-08-31 · The static efficiency and propulsive efficiency computed from the faired curves of figure 4 are presented in figure 6. The static efficiency

TECH LIBRARY KAFB, NM

O L ~ O L X I NASA TN D-3122

PERFORMANCE CHARACTERISTICS OF A 4-FOOT-DIAMETER

DUCTEDFANATZEROANGLEOFATTACK

FOR SEVERAL FAN BLADE ANGLES

By Kenneth W. Mort

Ames Research Center Moffett Field, Calif.

N A T I O N A L AERONAUTICS AND SPACE ADMINISTRATION

For sale by the Clearinghouse for Federal Scientific and Technical Information Springfield, Virginia 22151 - Price $1.00

Page 3: NASA TECHNICAL NOTE 1 · 2013-08-31 · The static efficiency and propulsive efficiency computed from the faired curves of figure 4 are presented in figure 6. The static efficiency

PERFORMANCE CHARACTERISTICS OF A 4-FOOT-DIAMETER

DUCTED FAN AT ZERO ANGLE OF ATTACK

FOR SEVERAL FAN BLADE ANGLES

By Kenneth W. Mort Ames Research Center

The s t a t i c and propulsive performance charac te r i s t ics of t h e ducted fan were defined f o r a wide range of fan advance r a t i o s by varying t h e fan rota- t i o n a l speed from 1800 t o 4800 rpm and t h e free-stream veloci ty from 0 t o 140 %ots. These c h a r a c t e r i s t i c s were examined f o r fan blade angles from 1l0 t o 43 .

The s t a t i c e f f ic iency ( f igure of m e r i t ) a t blade angles from 11' t o 20' was e s s e n t i a l l y constant a t about 78 percent, but a t higher angles it decreased rapidly. achieved a t an advance r a t i o of 0.6 and a blade angle of 23'. For a more com- prehensive means of evaluating performance over t h e e n t i r e veloci ty range, t h e t h r u s t t o horsepower r a t i o w a s examined as a function of free-stream veloci ty . The r e s u l t s indicated t h a t t h e performance was reasonably good f o r free-stream ve loc i t ies from 0 t o 100 knots. A t higher ve loc i t ies , performance deterio- ra ted rapidly because t h e ducted fan w a s designed primarily f o r good s t a t i c performance. Evaluation of another ducted fan design indicated t h a t i f higher ve loc i t ies a r e s p e c i f i c a l l y considered i n the design, good high speed perfor- mance can be achieved.

A m a x i m u m propulsive eff ic iency of about 58 percent w a s

INTRODUCTION

A 4-foot-diameter ducted fan mounted on a wing t i p was t e s t e d previously t o obtain aerodynamic data f o r a wide range of operating conditions ( r e f s . 1 t o 3 ) . Most of those t e s t s were performed a t a s ingle blade angle; hence t h e e f f e c t of blade angle on propulsive performance w a s not determined. Data a r e presented here f o r t h e same model a t Oo angle of a t t a c k but f o r severa l blade angles. The objectives of t h i s report a r e t o present t h e t h r u s t and power r e s u l t s and t o evaluate t h e s t a t i c and propulsive performance.

NOTATION

Ae net e x i t area, (shroud exit area)-(centerbody area at e x i t ) , sq f t

b f a n blade chord, i n .

Page 4: NASA TECHNICAL NOTE 1 · 2013-08-31 · The static efficiency and propulsive efficiency computed from the faired curves of figure 4 are presented in figure 6. The static efficiency

c duct chord, f t

c blade-section design l i f t coef f ic ien t , sect ion design l i f t ai qb

c f

CP

CT

d

de

FM

h

J

n

r

R

SHP

T

TC

V

Ve

v,

P

f r i c t i o n drag (wetted a rea)q

f l a t - p l a t e f r i c t i o n drag coef f ic ien t ,

power coef f ic ien t , 5.50 SHP pn3d5

T t h r u s t coef f ic ien t , - p n2 d4

fan diameter, f t

duct e x i t diameter, f t

fan blade thickness, i n .

V fan advance r a t i o , - nd

fan r o t a t i o n a l speed, rps

free-stream dynamic pressure, psf

r a d i a l distance from duct center l i n e , f t

fan radius, f t

input power, hp

t h r u s t , lb m 'I' t h r u s t coef f ic ien t , -

qcde

free-stream veloci ty , fps

computed ve loc i ty a t duct e x i t , fps

free-stream velocity, knots

fan blade angle measured a t t i p (unless otherwise noted), deg

2

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q propulsive eff ic iency, J - CT 100, percent c?

p mass densi ty of a i r , slugs/cu f t

MODEL AND APPARATUS

Character is t ics

The ducted fan and t h e semispan wing panel upon which t h e fan was mounted The general arrangement f o r t e s t i n g i n were t h e same as those of reference 1.

t h e wind tunnel i s shown i n f igure 1, and t h e dimensions of t h e f a n and t h e wing a r e presented i n f igure 2 and t a b l e s I and 11. It should be noted t h a t t h e shroud and s t a t o r s were designed primarily f o r good s t a t i c performance r a t h e r than optimum cru ise performance. The fan blade form curves a r e shown i n f igure 3.

Instrumentation

Forces and moments on t h e ducted fan were measured independently of those on t h e wing and support s t ruc ture by s t r a i n gages which were mounted on t h e duct-trunnion support tube.

The power t o t h e motor f o r dr iving the fan was recorded on a polyphase wattmeter and t h e meter readings were corrected f o r motor eff ic iency. rect ions were made f o r gear box losses because they were estimated t o be much less than t h e indicated input power accuracy.

No cor-

TESTS

For t h e t e s t s t h e fan blade angle w a s s e t and t h e f a n advance r a t i o w a s varied from 0 t o 1.8 by combining fan r o t a t i o n a l speeds ranging from 1800 t o 4800 rpm with free-stream v e l o c i t i e s from 0 t o 140 knots.

REDUCTION OF DATA

Duct-Trunnion S t r a i n Gage Data

The t h r u s t gages were d i r e c t l y ca l ibra ted i n pounds of force and required no correct ions.

3

Page 6: NASA TECHNICAL NOTE 1 · 2013-08-31 · The static efficiency and propulsive efficiency computed from the faired curves of figure 4 are presented in figure 6. The static efficiency

Accuracy of Measuring Devices

The various measuring devices w e r e accurate within t h e following l i m i t s . The values include e r ro r s involved i n reading and reducing t h e data as w e l l as t h e accuracy of t h e device i t s e l f .

Thrust 510 l b

Fan r o t a t i o n a l speed kO.5 rps

Shaft horsepower k20 hp

Free-stream dynamic pressure 50.1 psf f o r values < 20 psf k1/2 percent f o r valLes - > 20 psf

Fan blade angle ko .5O

RESULTS AND DISCUSSION

Basic Thrust and Power Charac te r i s t ics

These cha rac t e r i s t i c s a r e shown i n f igures 4 and 5 f o r fan blade angles from 11' t o 43'. The P = 15' and 23' performance r e s u l t s of reference 1 have been added t o t h e s c a t t e r evident i n f igu re 4 i s due t o t h e r e s u l t s obtained at lower r o t a t i o n a l speeds where t h e measurement e r ro r of t h e t h r u s t and power i s a grea te r per- centage of t h e value measured. For t h e range of r o t a t i o n a l speeds and free- stream ve loc i t i e s t e s t ed , these coe f f i c i en t s were found t o be only a funct ion of fan advance r a t i o and blade angle. It i s apparent from t h e r e s u l t s pre- sented i n f igu re 4(a) t h a t t h e var ia t ions i n t h r u s t coef f ic ien t a r e regular f o r blade angles from 11' through 35O, but a t 43' t h e blades s t a l l e d at zero advance r a t i o and remained s t a l l e d u n t i l t he advance r a t i o exceeded about 1.0. So t h a t t he r e s u l t s of t h i s report can be used conveniently with those of ref- erence 1 i n predic t ing f l i g h t performance of t i l t i n g ducted fan vehicles, t h e t h r u s t coef f ic ien t curves of f i gu re 4(a) a r e presented i n f igu re 5 referenced t o free-stream dynamic pressure and duct projected area (chord times e x i t diameter).

P = 15' and 23' r e s u l t s of t h e subject tests. The

1

Efficiency

The s t a t i c e f f ic iency and propulsive e f f ic iency computed from t h e f a i r e d The s t a t i c e f f ic iency i s shown curves of f igu re 4 a r e presented i n f igu re 6.

i n f igure 6(a) by presenting t h e f igu re of merit (based on ne t e x i t a rea) as a function of blade angle. It i s apparent f rom these r e s u l t s t h a t t h e f igu re of merit i s near ly constant a t about 78 percent f o r blade angles from 11' t o 20'. A s blade angle i s increased beyond 200 t h e f igu re of merit decreases. The

- . -~ . - i . . . . - . . - . . . ~~ ~

%he t h r u s t coef f ic ien t i n f igu re 5 i s equal t o - C D ~ a t zero angle of a t t a c k i n reference 1.

4

Page 7: NASA TECHNICAL NOTE 1 · 2013-08-31 · The static efficiency and propulsive efficiency computed from the faired curves of figure 4 are presented in figure 6. The static efficiency

propulsive eff ic iency, which is ind ica t ive of t h e high speed performance, i s presented i n f igure 6 ( b ) . eff ic iency has a m a x i m u m value of 58 percent a t an advance r a t i o of 0.6 and a blade angle of 230. envelope so t h a t over ??-percent eff ic iency i s ava i lab le f o r a range of advance r a t i o s from about 0.4 t o 1.1.

It i s apparent from t h i s f igure t h a t t h e propulsive

However, t h e eff ic iency curves have a reasonably f la t

Evaluation of t h e Performance

Comparison with theory.- From t h e r e s u l t s of f igure 4, t h e T/SHP was determined as a function of free-stream veloci ty f o r an input power which was held constant a t t h e design value f o r zero free-stream veloci ty (420 hp) . blade angle and r o t a t i o n a l speed were adjusted as free-stream veloci ty was increased t o give t h e bes t t h r u s t . The r e s u l t s a r e presented i n f i g u r e 7. Along with these r e s u l t s t h e t h e o r e t i c a l performance is presented f o r compari- son. theory" and with t h e assumption t h a t 90 percent of t h e input power w a s deliv- ered t o the a i r stream f o r producing t h r u s t . I n addi t ion, a simple f l a t - p l 3 t e drag coef f ic ien t w a s used f o r estimating t h e reduction i n shroud f r i c t i o n drag, and t h e estimate was subtracted from t h e computed r e s u l t s . The r e s u l t i n g curve i s considered t o be representat ive of t h e p e r f o p mance possible with a very good ducted fan design with t h e same power loading and shroud dimensions. It i s apparent from f igure 7 t h a t t h e T/SHP of t h e present ducted fan was good f o r v e l o c i t i e s from 0 t o about 100 knots, but a t grea te r ve loc i t ies it deter iorated very rapidly from t h e t h e o r e t i c a l value.

The

This performance w a s computed by means of "simple momentum ducted fan

T/SHP due t o

If an estimated zero-power f a n drag i s subtraeted from t h e zero-power drag which can be obtained from f igure 4, t h e drag of the shroud, centerbody, vanes, etc. ,can be estimated. This estimate shows t h a t t h e reduction i n per- formance i s la rge ly due t o t h i s drag. A l s o , i f t h i s drag i s added t o t h e experimental T/SHP curve, the r e s u l t would indicate t h a t the fan e f f ic iency i s r e l a t i v e l y constant over a large range of free-stream ve loc i t ies (about 100 t o 300 or 400 knots) as i s usual ly the case f o r propel lers and ducted propel lers .

Since t h i s f a n was designed f o r s t a t i c performance r a t h e r than c ru ise performance, i t s shroud has a r e l a t i v e l y high thickness r a t i o and a la rge diffusion r a t i o , and i t s s t a t o r vanes a r e s e t f o r o p t i " s t a t i c performance. To determine t h e extent t o which T/SHP reduced and t o determine whether t h e t h e o r e t i c a l curve is reasonable, t h e next sect ion presents a comparison with the ducted fan of reference 4. This ducted fan had two shroud configurations: one d e s i s e d expressly for good high speed performance and t h e other f o r good s t a t i c performance.

might be increased i f t h e drag w e r e

Comparison with t h e ducted f a n of reference 4.- The ducted fan of reference 4 f o r the same exit area power loading (SHP/Ae = 28.2 hp/ft2) and best t h r u s t producing conditions is presented i n f igure 7. It i s apparent t h a t with t h e shroud designed f o r c ru ise , performance a t free-stream v e l o c i t i e s grea te r than 100 knots d i d not decrease from t h e t h e o r e t i c a l value as did t h a t of t h e ducted f a n reported herein. I n f a c t , t h e

T/SHP r a t i o f o r t h e

5

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performance is very close to the computed curve for this velocity range.2 Hence the reduction in performance of the ducted fan of reference 4 due to shroud drag is relatively small and indicates that high speed performance com- parable to that computed theoretically can be obtained.

For free-stream velocities less than 100 knots the performance of the cruise shroud of reference 4 is poor because the flow separates at the inlet lip. The static performance of the shroud configuration which had a large bell mouth is very good; however, it is only slightly better tNan that of the ducted fan of this report. Hence it can be concluded that the shroud design of this ducted fan was very good for static performance.

Ames Research Center National Aeronautics and Space Administration

Moffett Field, Calif., Sept. 14, 1965

mFERFNCES

1. Mort, Kenneth W.; and Yaggy, Paul F.: Aerodynamic Characteristics of a 4-Foot-Diameter Ducted Fan Mounted on the Tip of a Semispan Wing. NASA TN D-1301, 1962.

2. Yaggy, Paul F.; and Mort, Kenneth W.: A Wind-Tunnel Investigation of a 4-Foot-Diameter Ducted Fan Mounted on the Tip of a Semispan Wing. TN D-776, 1961.

NASA

3. Yaggy, Paul F.; and Goodson, Kenneth W.: Aerodynamics of a Tilting Ducted Fan Configuration. NASA TN 0-785, 1961.

4. Grose, Ronald M.: Wind-Tunnel Tests of Shrouded Propellers at Mach Num- bers From 0 to 0.60. WADC TR 58-604, United Aircraft Corp., 1958.

- _ _ - -

2The computed shroud drag increment for the shroud of reference 4 would be about 3/4 of that of the subject ducted fan shroud.

6

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TABLE I.- BASIC DIMENSIONS OF DUCTED FAN AND WING

. .

Duct Ins ide diameter . . . . . . . . . . . . . . . . . . . . . . . Outside diameter . . . . . . . . . . . . . . . . . . . . . . C h o r d . . . . . . . . . . . . . . . . . . . . . . . . . . . . E x i t diameter . . . . . . . . . . . . . . . . . . . . . . . . Diffuserangle . . . . . . . . . . . . . . . . . . . . . . . Exit a r e a . . . . . . . . . . . . . . . . . . . . . . . . . . C h o r d . . . . . . . . . . . . . . . . . . . . . . . . . . . . Number of vanes . . . . . . . . . . . . . . . . . . . . . . . A i r f o i l sec t ion . . . . . . . . . . . . . . . . . . . . . . . Posi t ion of vane c/4, percent of duct chord . . . . . . . . . T w i s t . . . . . . . . . . . . . . . . . . . . . . . . . . . .

plan-form curves . . . . . . . . . . . . . . . . . . . . . . Number of blades . . . . . . . . . . . . . . . . . . . . . .

I n l e t guide vanes

Fan

Hub t o t i p diameter r a t i o . . . . . . . . . . . . . . . . . . Posi t ion o f hub center l i n e , percent of duct chord . . . . . Design s t a t i c t h r u s t d i sc loading . . . . . . . . . . . . . . Blade angle cont ro l . . . . . . . . . . . . . . . . . . . . . Blade angle a t t i p . . . . . . . . . . . . . . . . . . . . . Approximate blade t i p clearance . . . . . . . . . . . . . . . Posi t ion of s t a t o r c/4, percent o f duct chord . . . . . . . . T w i s t , centerbody t o t i p . . . . . . . . . . . . . . . . . . 8 s t a t o r s with 6-inch chord

A i r f o i l . . . . . . . . . . . . . . . . . . . . . . . . . . Mean l i n e . . . . . . . . . . . . . . . . . . . . . . . . . A i r f o i l . . . . . . . . . . . . . . . . . . . . . . . . . . M e a n l i n e . . . . . . . . . . . . . . . . . . . . . . . . .

A i r f o i l sec t ion . . . . . . . . . . . . . . . . . . . . . . . Area . . . . . . . . . . . . . . . . . . . . . . . . . . . . Mean aerodynamic chord . . . . . . . . . . . . . . . . . . . Taper r a t i o . . . . . . . . . . . . . . . . . . . . . . . . .

Sta to r s

Additional 9-inch chord s ta tor which housed fan dr ive shaf t

Wing

Semispan . . . . . . . . . . . . . . . . . . . . . . . . . .

I 1111 1m.1.111.1111111 111111II I

. . . . 4 f t 4 f t 10.5 i n . . 2 f t 9 i n .

4 f t 6.3 i n . . . . . .11c . . 14.9 f t2

. . . . 3 i n . . . . . . . 7 NACA 65A010

14.5 percent . . . . . oo . see f i g . 3 . . . . . 8 . . * . 0.333 29.3 percent . . . 150 psf

f ixed p i t ch . . . . . U 0 . . 0.030 i n .

49.4 percent 15 O

NACA 0008.4 . . . a = 0.4

. . NACA 0017 . . . a = 0.4

. . . 48 f t 2 . . . . 8 f t . . 6.09 f t . . . . 0 675

. . . . .

- NACA 2418

7

I

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TABU 11.- SHROUD AND CENTERBODY COORDINATES

Shroud coordinates tabulated i n percent of shroud chord

(33.00 in . )

Chordwise length

0 -5 -75 1.25 2.5 5 00 7 -5 10.0 15 .o 20 .o 25 .o 30 .O

40 .O 45 .O

35 -0

50.0

60 .o 65 .o 70 .o 75 -0 80 .o 85 .o go .o 95.0

55 -0

100

Outside radius

81.5

83.8 83.4

84.4 83.4 86.4 87.1 87.6 88.2 88.6 88.6 88.6 88.6 88.6 88.6 88.6 88.6 88.6 88 .o 87.4 86.8 85 -9 85.2 84.3 83 03 82.2

~

Ins ide radius

81.5 79.6 79 -0 78.4 77 -2 75.8 74.9 74.2 73 -3 72 *9 72.7 72.7 72.7 72.7 72 -7 72 *7 73 02 74.1 75.1 76.1 77.1 78.1 79 -1 80.1 81.1 82 .o

-~

Cent erb o dy coordinates tabulated i n percent of centerbody

length (71.5 i n . ) .. ._

aShroud leading-edge pos i t ion.

Length

0 -5

1.25 2.50 5 * O 7 *5 10 15 20 25

30

40 50 60 70 72.05' 80 83.20 90 95 100

25 J375"

32 *57b

- .

Radius

0 2.07 3.20

6.17

8.31 9.68 10.34 11.01 11.06 11.19 11.19 11.19 11.19 11.19 10.49 10.14 7-97 6.77 4.03 2.01 0

4.46

7.40

b I n l e t guide vane c/4 l i n e pos i t ion .

'Shroud t ra i l ing-edge pos i t ion .

8

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A-25140.1

Figure 1.- Ducted fan model mounted i n the Ames 40- by 8 0 - ~ o o t Wind Tunnel.

9

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P 0

33" t--

Wing quarter- chord l i n e 1

\/Momen+ reference

Figure 2.- Basic model dimensions.

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n b.20- 4 L

0

cn tn Q, C

+ *I2

Y 0 E .08

.04

c 0

- k I

- n

t C

w3.332 .4 .5 .6 .? .8 .9 I .6 Radial station, r /R

1 1 I I I I 1 I I 7.2 8.0 9.6 12.0 14.4 16.8 19.2 21.6 24.0

Radial station, in.

Figure 3.- Fan blade-form curves with the design l i f t coefficient, blade chord, blade angle, and blade thickness t o chord r a t i o as functions of the r ad ia l distance from the duct center.

Page 14: NASA TECHNICAL NOTE 1 · 2013-08-31 · The static efficiency and propulsive efficiency computed from the faired curves of figure 4 are presented in figure 6. The static efficiency

n 3 5 -

J

(a) Thrust coefficient as a function of advance ratio.

Figure 4.- Performance characteristics for several blade angles.

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P w

.9

.8

7 . I

P I deg .6 O I I -

.5 0 2 3 -

.4 n 3 5 -

.3

.2

. I

0

-. I 0 .I .2 .3 .4 .5 .6 .7 .8 .9 1.0 1 . 1 1.2 1.3 1.4 1.5 1.6 1.7 1.8

J

(b ) Power coeff ic ient as a function of advance r a t i o .

Figure 4 .- Concluded.

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60 -

56 -

52 -

48 -

44 -

40 -

36 -

32 -

T c 28 -

0 .2 .4 .6 .8 1.0 1.2 1.4 1.6 1.8 J

Figure 5.- Thrust coefficient referred to free-stream dynamic pressure as a function of advance ratio.

14

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80

70

60

50

c c a, Y Q) 40 n

2- L L

30

20

IO

0 IO P , deg

(a) Figure of merit as a function of blade angle.

0

Figure 6.- Figure of merit and propulsive e f f ic iency computed from t h e curves of f igu re 4.

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0 .I .2 .3 .4 .5 .6 .7 .8 .9 1.0 1 . 1 1.2 1.3 1.4 1.5 1.6 1.7 1.8 J

( b ) Propulsive efficiency as a function of advance ratio for several blade angles.

Figure 6 .- Concluded.

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z % 7

2 Y I- (D m 01 6 ? [u 0 03 P

5

Q r P \ 4

a

- L

Estimated decrement due t o ( f la t - plate) shroud

+I% 3

2

I

0 40 80 I20 I60 200 240 280 320 360 400 V,, knots

Figure 7.- Thrust t o horsepower r a t i o as a function of free-stream velocity fo r an ex i t area power loading of 28.2 hp/ft2.

Page 20: NASA TECHNICAL NOTE 1 · 2013-08-31 · The static efficiency and propulsive efficiency computed from the faired curves of figure 4 are presented in figure 6. The static efficiency

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