!VASA ct-/05)',1
Transcript of !VASA ct-/05)',1
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3 1176 00161 4974
F~ EARLY DOMESTIC DISSEMINATION ~'. ~
Beca'i:1se of its significant early commercial p6tential. this informat"ion. which has been developed unei'er a U.S. Government p;Bgram. is being disseminated within the United
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States in advance of general publication. This information may be duplicate~a,rd used p{the recipient with the express limitation that'rhnot.<be published. Release of this information to other dom~;~ parties by the recipient shall be made subject to th(se limifations.
. // "'-Foreign relea;\vmay be made only"wilh prior NASA ap-proval and appropriate export Iicenses~'This legend shall -,," ;J\ be markedbn any reproduction of this info;ma ion in whole or in RzfI. ",~
/ _ ~7"lew for general release
ENERGY EFFICIENT ENGINE HIGH-PRESSURE TURBINE UNCOOLED
RIG TECHNOLOGY REPORT
prepared by
W. B. Gardner, Program Manager Energy Efficient Engine Component
Development and Integration Program
UNITED TECHNOLOGIES CORPORATION Pratt & Whitney Aircraft Group
Commercial Products Division
!VASA ct-/05)',1 NASA CR-16514Q ~ PWA-5594-92
NASA-CR-165149 19820024507
.NOV 1 O,9aO
Because of their possible significant early connnercial value, these data developed under a U.S. Government contract are being disseminated within the U.S. in advance of general pUblication. These data may be duplicated and used by the recipient with the expressed limitations that the data will not be published nor will they be released to foreign parties without permission of Pratt & Whitney Aircraft Group and appropriate export licenses. Release of these data to other domestic parties by the recipient shall only be made subject to the limitations contained in NASA Contract NAS3-20646. These limitations shall be considered void after two (2) years after date of such data. This legend shall be marked on any reproduction of these data in whole or in part.
Prepared for NATIONAL AERONAUTICS AND SPACE ADMINISTRATION
NASA-Lewis Research Center Contract NAS3-20646
111111111111111111111111111111111111111111111 NF02430
BEST
AVAILABLE \
COpy
1 Report No 2 Government Accession No
NASA-CR-165149 4 Title and Subtitle
Energy Efficient Engine - High-Pressure Turbine Uncooled Rig Technology Report
7 Author(s)
W.B.Gardner, et al
3 RecIpient's Catalog No
5 Report Date
October 1979 6 Performing Organization Code
8 Performing Organization Report No
PWA-5594 -92
1---------------------------1 10 Work Untt No 9 Performing Organization Name and Address
United Technol ogi es Corporati on Pratt & Whitney A ircraft Group - CPO
11 Contract or Grant No
NAS3-20646 E as t H artf ord, C onnec ti cut 06108 13 T f R P Co t--------...;.--------------------I ype 0 eport and ertod vered
12 SponsOrlnll Ajlency Name and Address National Aeronautics and Space Administration
Technology Report
Lewi s Research Center 14 Sponsoring Agency Code
21000 Brookpark Road, Rocky River, OH 44135 15 Supplementary Notes
NASA Project Manager, Mr. N. T. Saunders, NASA-Lewi s Research Center
16 Abstract
Results obtained from testing five perfonnance builds (three vane cascades and two rotating rigs of the Energy Efficient Engine uncooled rig have established the uncooled aerodynamic efficiency of the high-pressure turbine at 91.1 percent. This efficiency level was attained by increasing the rim speed and annulus area (AN2), and by increasing the turbine reaction level. The increase in AN2 resulted in a performance improvement of 1.15 percent. At the design point pressure ratio, the increased reaction level rig demonstrated an efficiency of 91.1 percent. The results of this program have verified the aerodynamic design assumptions established for the Energy Efficient Engine high-pressure turbine component.
17 Key Words (Suggested by Author(s))
U nco 01 ed Rig Reacti on Level Annul ar Cascade
Annulus area Stress Testing Rotating Rig
18 Distribution Statement
19 SecUrity Classlf (of this report) 20 Securtty Classlf (of this page) 21 No of Pages
242
• For sale by the NatIOnal Technical Information Service, Springfield, Virginia 22161
NASA-C-168 (Rev 10-75)
22 Price·
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FOREOORD
The Energy Efficient Engine Component Development and Integration Program is being conducted under parallel National Aeronautics and Space Administration contracts to Pratt & Whitney Aircraft Group and General Electric Company. The overall project is under the direction of Mr. Neal T. Saunders. Mr. John W. Schaefer is the NASA Assistant Project Manager for the Pratt & Whitney Aircraft effort under NASA Contract NAS3-20646, and Mr. Michael Vanco is the NASA Project Engineer responsible for the portion of the project described in this report. Mr. William B. Gardner is manager of the Energy Efficient Engine project at Pratt & Whitney Aircraft Group.
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TABLE OF CONTENTS
Section
1.0 SUMMARY
2.0 INTRODUCTION
3.0 ANALYSIS AND DESIGN
4.0
3.1 Aerodynamic Design 3.2 Mechanical Design
3.2.1 Design of Rig Subsystems 3.2.2 Design of Test Rig
FABRICATION AND ASSEMBLY 4.1 Fabrication
4.1.1 Blades 4.1. 2 Vanes 4.1.3 Disks and Sideplates 4.1. 4 Cases 4.1.5 Shaft and Main Bearings
4.2 Assembly 4.2.1 Vanes 4.2.2 Rotor 4.2.3 Cases 4.2.4 Shaft and Main Bearings 4.2.5 Stand Instrumentation
5.0 TESTING 5.1 General Description
5.1.1 Test Facility 5.1.2 Test Rigs
5.2 Instrumentation 5.2.1 Annular Cascade Instrumentation 5.2.2 Rotating Rig Instrumentation
5.3 Test Procedures 5.3.1 Annular Cascade Test Conditions 5.3.2 Rotating Rig Test Conditions 5.3.3 Data Acquisition 5.3.4 Data Recording 5.3.5 Data Reduction 5.3.6 Shakedown Testing 5.3.7 Rotating Rig Stress Testing
6.0 RESULTS 6.1 Annular Cascades
6.1.1 Performance Discussion 6.1.2 Analysis Discussion
6.2 Rotating Rig 6.2.1 Performance Discussion 6.2.2 Blade Analysis Discussion
6.3 Summary
v
1
2
5 5 21 21 23
29 29 29 29 30 30 30 30 30 31 33 33 33
35 35 35 35 35 35 38 39 39 41 42 42 42 42 42
49 49 49 56 59 59 68 73
TABLE OF CONTENTS (Cont' d)
Section Page
7.0 CONCLUSIONS 77
APPENDIX A Airfoil Coordinates 79 B Build 1 Cascade Data 97 C Build 2 Cascade Data 117 D Build 3 Cascade Data 145 E Build 1 Rotating Rig Data 171 F Build 2 Rotating Rig Data 199
MAILING LIST 229 ~
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Figure
1
2
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5
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8
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17
LIST OF ILLUSTRATIONS
Interaction of Uncooled Rig Supporting Technology Program with the High-pressure Turbine Component Effort
Reaction Level Versus Turbine Efficiency
Energy Efficient Engine Uncooled Rig Flowpath
Velocity Triangles for Low Reaction Design
Velocity Triangles for High Reaction Design
Energy Efficient Engine Uncooled Rig Build 1 Vane Root
Energy Efficient Engine Uncooled Rig Build 1 Vane Mean
Energy Efficient Engine Uncooled Rig Build 1 Vane Tip
Energy Efficient Engine Uncoo1ed Rig Build 1 Blade Root
Energy Efficient Engine Uncoo1ed Rig Build 1 Blade Mean
Energy Efficient Engine Uncoo1ed Rig Build 1 Blade Tip
Energy Efficient Engine Uncooled Rig Build 2 Vane Root
Energy Efficient Engine Uncoo1ed Rig Build 2 Vane Mean
Energy Efficient Engine Uncoo1ed Rig Build 2 Vane Tip
Energy Efficient Engine Uncoo1ed Rig Build 2 Blade Root
Energy Efficient Engine Uncooled Rig Build 2 Blade Mean
Energy Efficient Engine Uncoo1ed Rig Build 2 Blade Mean
vii
3
5
8
9
10
11
12
13
13
14
15
15
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17
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Figure
18
LIST OF ILLUSTRATIONS (Cont'd)
Energy Efficient Engine Uncooled Rig Build 3 Vane Root
19 Energy Efficient Engine Uncooled Rig Build 3 Vane Mean
20
21
22
23
24
25
26
27
28
29
30
31
32
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34
35
Energy Efficient Engine Uncooled Rig Build 3 Vane Tip
Uncooled Rig Resonance Diagram (Build 1 Low Reaction Blade)
Uncooled Rig Resonance Diagram (Build 2 High Reaction Blade)
Energy Efficient Engine High Pressure Turbine Uncooled Rig
Circumferentially Traversing Exit Instrumentation Ring
Uncooled Rig Modifications Required for Annular Cascade Testing
Uncooled Rig Critical Speed Characteristics
Energy Efficient Engine High-Pressure Turbine Uncooled Rig Vane Assembly
Energy Efficient Engine High-Pressure Turbine Uncooled Rig Rotor Assembly
Annular Cascade Rig
Rotating Rig
Energy Efficient Engine High-Pressure Turbine Uncooled Rig primary Performance Instrumentation
Typical Run For Rotating Rig Testing
Rig Wire Seal and Damper Locations
Strain Gage Location
Strain Gage Location
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19
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24
25
26
27
31
32
36
37
38
41
43
44
46
LIST OF ILLUSTRATIONS (Cont'd)
Figure
36 Holographs From Blade Bench Tests
37 Stress Ratios From Blade Bench Tests
38 Rig Blade Resonance Diagram
39 Annular Cascade Pressure Loss vs Mach Number
40 Annular Cascade Pressure Loss vs Mach Number
41 Typical Vane Loss Contours at Design For Build 1
42 Typical Vane Loss Contours at Design For Build 2
43 Typical Vane Loss Contours at Design For Build 3
44 Vane Loss vs Percent Span
45 Vane Exit Angle Distribution
46 Deviation vs Mach Number
47 Flow Parameter vs Mach Number
48 Vane Surface Statics (50 percent span)
49 AN2 Increase
50 Efficiency vs Pressure Ratio
51 Outer Diameter Kielhead Efficiency Change with Clearance
52 Reaction vs Pressure Ratio
53 Efficiency Contours, Build 1
54 Efficiency Contours, Build 2
55 Efficiency vs Percent Span
56 Blade Exit Angle
57 Mass Averaged Blade Total Loss vs Pressure Ratio
58 Mach Triangles
ix
45
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48
50
51
52
53
54
55
57
57
58
60
61
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63
64
65
66
67
67
69
70
Figure
59
60
61
62
63
LIST OF ILLUSTRATIONS (Cont'd)
Total Blade Deviation (air angle at the exit plane minus the gage plane air angle)
Blade Surface Statics
Effect of Leakage Flow on Efficiency
Uncooled Rig Efficiency vs Pressure Ratio
Uncooled Rig Efficiency vs Pressure Ratio
x
71
72
73
74
75
Table
1
2
3
4
5
6
7
8
9
10
11
12
LIST OF TABLES
EFFICIENCY GOALS OF THE UN(J)OLED RIG PROGRAM
MAJOR TEST CONFIGURATIONS OF THE HIGH-PRESSURE TURBINE UN(J)OLED RIG
PRELIMINARY TURBINE DESIGN PARAMETERS
AERODYNAMIC PROPERl'IES
VANE THROAT AREA
BLADE THROAT AREA
ANNULAR CASCADE TEST INSTRUMENTATION
ROTATING RIG TEST INSTRUMENTATION
TYPICAL RUN FOR ANNULAR CASCADE TESTING
FLOW COMPARISCN
DESIGN POINT PERFORMANCE
COMPARISCN OF DESIGN AND EXPERIMENTAL MACH NUMBERS
xi
4
4
6
7
31
32
39
40
41
59
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A annulus area, in2 bx axial chord, in cx axial flow velocity, fps
LIST OF SYMBOLS
g force-mass conversion constant, 32.174 f/s2 h specific enthalpy, Btu/lb
J work equivalent,
M Mach number
ft-lbs Btu
N mechanical speed, RPM P pressure, in of mercury T temperature, OF or ~ U tangential wheel speed, fps W mass flow, lbs/sec x axial distance, in. y tangential distance, in. a absolute angle, degree P relative angle, degrees
Subscripts
a air AA area-averaged m metal MA mass-averaged S static condition T total state
xiii
1.0 SUMMARY
To achieve the goal efficiency for the Energy Efficient Engine high-pressure turbine component, a single stage turbine was designed to produce a high ratio of wheel speed to specific work, velocity ratio, and a low ratio of through flow to wheel speed (Cx/U). This aerodynamic concept was limited structurally by allowable blade stress, typified by parameter AN2 (product of annulus area and wheel speed squared). This design reduced turbine Mach numbers at the expense of airfoil turning, and was predicted to increase high-pressure turbine performance by 1.1 percent. The actual performance improvement, 1.15 percent, is in excellent agreement with the predicted value.
In addition to high velocity ratio and low Cx/U feature, design trade studies indicated that a 0.5 percent increase in turbine efficiency could be attained by increasing the turbine reaction level from a balanced Mach number design to a design with a subsonic vane. At the design point pressure ratio, the increased reaction level rig demonstrated an efficiency of 91.1 percent, 0.8 percent higher than the lower reaction rig.
The results obtained by canting the vane 13 degrees in the direction of rotation showned that the canted vane configuration had the lowest mass averaged total loss of all of the airfoils tested.
These results have established the uncooled aerodynamic efficiency of the high-pressure turbine at 91.1 percent and have verified the feasibility of the Energy Efficient Engine high-pressure turbine aerodynamic design concepts.
2.0 INTRODUCTION
The objective of the NASA Energy Efficient Engine Development and Integration program is to develop, evaluate, and demonstrate the technology for achieving lower installed fuel consumption and lower operating costs in future commercial turbofan engines. NASA has set minimum goals of 12 percent reduction in thrust specific fuel consumption (TSFC), 5 percent reduction in direct operating cost (DOC), and 50 percent reduction in performance degradation for the Energy Efficient Engine (flight engine) relative to the JT9D-7A reference engine. In addition, environmental goals on emissions (meet the proposed EPA 1981 regulation) and noise (meet ~R 36-1978 standards) have been established.
The Pratt & Whitney Aircraft Energy Efficient Engine high-pressure turbine is a single-stage design. A single-stage design has certain advantages when compared to its multi-stage counterpart. Single stage turbines require no interstage seals, require fewer cooled airfoils, and contain fewer leakage paths. The inherent design simplicity of the single stage reduces engine initial cost, maintenance material cost, and overall engine weight.
The purpose of the Energy Efficient Engine high-pressure turbine uncooled rig program was to (1) establish the uncooled aerodynamic efficiency base for the high-pressure turbine component and (2) verify the aerodynamic design assumptions for this component. The program was conducted to ensure timely interaction with the high-pressure turbine component effort, as summarized in Figure 1. The efficiency goals are presented in Table 1, and the major test configurations are summarized in Table 2.
Five performance builds (three vane cascades and two rotating rigs) of the uncooled turbine rig were tested to establish the Energy Efficient Engine turbine efficiency base and to verify the advanced aerodynamic design concepts of the program. The first rotating rig (Build 1) and its companion cascade had a design reaction level of 35 percent and examined the effects of high AN2 (low Cx/U and high velocity ratio) on turbine efficiency. The second rotating rig (Build 2) and its companion cascade examined the effects of stage reaction on stage efficiency. This build of the rotating rig was also used to evaluate blade vibratory stress levels. The tests with the third annular cascade rig investigated the effects of a l3-degree vane tangential cant on cascade losses.
Thiq report describes the design of the two transonic single stage turbines and the test results obtained in the annular cascade and rotating rig test programs.
2
HIGH-PRESSURE TURBINE COMPONENT DESIGN AND FABR ICATION
UNCOOLED RIG PROGRAM
1.1 2
V
9
*0 Program critical decisIon point
1978
I 3 r 4
PDR 1 2
V 1]-
3 ,-
1979 1980
1 I 2 I 3 I 4 1 I :1 1 3 I *0
-9 ,.
l' 4 I
f-l 9
2
3
Component prellm1nary des1gn effort completed, prel1m1nary des1gn review (PDR) held.
Componpnt detailed design pffort inItIated on non-aerodynamic act1vlties.
Build 1 rotating stage tests completed. Results establish feasiblilty of advanced aerodynamic concepts
'I
4 BU11d 2 rotat1ng stagp t~sts completed Results enable decision to be made on b~st vane and blade aerodynam1c conf1gurat10n. Component deta11ed des1gn effort cont1nues, incorporating aerodynam1c activltles
Figure 1 Interaction of Uncooled Rig Supporting Technology Program with the High-Pressure Turbine Component Effort - The un- cooled rig program was conducted to ensure timely interac- tion with the high-pressure turbine component effort.
3
AN2 (in.-rpm) 2
TABLE 1
EFFICIENCY GOALS OF THE UNCOOLED RIG PROGRAM
Build 1 Build 2 Rotating Stage Rotating Stage
49 x 109 49 x 109
Rim Speed, Redline (ft/sec)
Reaction (percent)
Uncooled Efficiency (percent)
Vane Cascades
Build 1
Build 2
Build 3
Rotating Stages
Build I
Build 2
4
1730 1730
35 43
90.3 90.8
TABLE 2
MAJOR TEST CONFIGURATIONS OF THE HIGH-PRESSURE TURBINE UN<XlOLED RIG
35-Percent Reaction, "Zero" Vane Cant Angle
43-Percent Reaction, "Zero" Vane Cant Angle
43-Percent Reaction, 13-Degree Vane Cant Angle
35-Percent Reaction (vane and blade), "Zero" Vane Cant Angle
43-Percent Reaction (vane and blade), "Zero" Vane Cant Angle
Blade Vibratory Stress Level Testing of the 43-Percent Reaction (vane and blade), "Zero" Vane Cant Angle
3.0 ANALYSIS AND DESIGN
3.1 Aerodynamic Design
Turbine design studies indicated that to meet the goal efficiency, advanced aerodynamic concepts which achieve a high ratio of wheel speed to specific work (velocity ratio) and a low ratio of through-flow velocity to wheel speed (Cx/U) are required. These aerodynamic design concepts are limited by structural considerations typified by the parameter AN2 (product of annulus area to wheel speed squared). By designing the Energy Efficient Engine high-pressure turbine to an AN2 level of 49 x 109, an increase of 1.1 percent in turbine efficiency was predicted relative to state-of-the-art single-stage turbines. Design trade studies also indicated that turbine efficiency could be improved by increasing the reaction level from a balanced Mach number design to a design featuring a subsonic vane. However, as turbine stage reaction increases, rearward thrust across the turbine is increased and, therefore, bearing thrust balance can become a limiting factor. In the Energy Efficient Engine design, this limit was reached at about 43 percent reaction (see Figure 2).
PREDICTED DELTA
EFFICIENCY
STAGE REACTION
Figure 2 Reaction Level Versus Turbine Efficiency - Maximum turbine reaction was limited by the engine rotor thrust balance.
As a result of these studies, two high AN2 turbines with reaction levels of 35 and 43 percent were designed for uncooled rig performance evaluation. The turbine parameters for these two designs are listed in Table 3.
In addition to the two full stage designs, a third set of vanes was designed, incorporating a 13-degree cant angle in the direction of rotation. This design imparts radial body loads to the gas flow and, according to published literature, has been shown to reduce the inner diameter endwall losses. The aerodynamics for the three vane designs are summarized in Table 4.
5
TABLE 3 PRELIMINARY TURBINE DESIGN PARAMETERS
No. of Stages Pressure Ratio Mean Velocity Ratio, U
-~v;:;:;2:='gJ;=~'77h-
Work Factor, (Jgf h)
AN2 (SLTO), (cm-rps)2«in-rpm)2) AN2(Redline),(cm-rps)2«in-rpm)2) Rim Speed (SLTO), m/sec (ft/sec) Rim Speed (Redline), m/sec (ft/sec) Inlet Speed Parameter, N/ v'T Inlet Flow Parameter, W .J'T/p Specific Work, ~ hiT Blade Tip Clearance, cm (in.) Mean Reaction Level Mean Blade Turning Goal Cooled Turbine Efficiency, %
Build 1
1 4.0 0.56
1. 59 8. 24xl07 (46xl09) 8. 79xl07 (49xl09)
511. 0 (1677) 527.0 (1730)
252.1 17.69
0.0729 0.051 (0.020)
0.35 1250
88.2
Build 2
1 4.0 0.56
1.59 8. 24xl07 (46xl09) 8. 79xlO 7 (49xl09)
511.0 (1677) 527.0 (1730)
252.1 17.69
0.0729 0.051 (0.020)
0.43 117.80
88.2
Specific procedures followed in the turbine aerodynamic design included a meanline analysis, streamline analysis, airfoil design, airfoil pressure distribution, and boundary layer analysis. Meanline analysis was performed to determine flowpath areas. primary considerations during the streamline analysis were inlet and exit Mach triangles and gas turning angles. This analysis generated radial profiles using both two- and three-dimensional analytical procedures to produce suitable airfoil pressure distributions. This analysis also determined the radial distribution of aerodynamic properties. Boundary layer calculations were then used to verify the low loss characteristics of the airfoils. Through this approach, a comprehensive turbine design study was conducted, and criteria were established for the design of both the vane and blade.
The vane airfoil sections were designed so that the flow was accelerated past the gage point (throat) with low, smooth backend diffusion. Durability constraints set the minimum thickness for the airfoil. The uncovered turning and exit wedge angle were optimized to minimize the two-dimensional loss. Based on previous single-stage turbine design correlations, an existing exit angle deviation system and a radial work distribution were applied to the design of the Energy Efficient Engine. The blade airfoil sections were designed to the same pressure distribution criteria as the vane. The blade uncovered turning and exit wedge angle were further optimized to reduce trailing edge shock losses. The blade leading edge diameter was set by durability considerations. The uncooled rig was scaled to match the engine Mach number triangles and vane exit Reynolds number. This aerodynamic scaling, coupled with the constraints of using existing uncooled rig hardware, resulted in a scale factor of 0.7325 between rig and engine turbines.
6
Vane
a Exit (degrees) MExl.t Gap/Chord
Blade Mean
Reaction Turning (degrees) Load Coefficient ~xit Cx/u Gap/Chord
Blade Root
Reaction Turning (degrees) Load Coefficient Gap/Chord
Blade Tip
Reaction Turning (degrees) Load Coefficient Gap/Chord
TABLE 4 AERODYNAMIC PROPERTIES
Build 1
10.4 1.01 0.90
0.35 125
0.92 1.15
0.328 0.90
0.29 133.3
0.78 0.88
0.42 111.3
1.13 0.92
Build 2
10.4 0.93 0.90
0.43 117.8
0.95 1. 23
0.320 0.96
0.36 133.9
0.81 1.01
0.49 87.5 1.16 0.91
Build 3
10.4 0.93 0.90
Reaction = Static Pressure drop across the rotor ratioed to the static pressure drop across the stage.
pS2 - psI. 5
pS2 - pSI
Load Coefficient = 2 :x Sin 2 a 2 [~~; ctn a 1 + ctn a 2]
7
The flight engine flowpath was scaled to rig size (see Figure 3). Mach numbers and velocity triangles were made to correspond to those required in actual operating conditions (see Figures 4 and 5). The uncooled flowpath dimensions were reduced to maintain design reactions without cooling air.
10.211 R
~LED FROM ENGINE UPI SCALE FACTOR = 0.7325
10.174 R SCALED ENGINE FLOWPAT~
__ ~L-__ ~ ________ ~--;
24 AIRFOILS p4 AIRFOIL
11.9 6R -.L ~
;"'I\':='\ ~\ ~\=r\=T\=\t!-.:;~;:::t~--fr-
0.01465 12.028 R 12.342 R
Figure 3 Uncooled Rig Flowpath
An iterative procedure uS1ng a computer interactive airfoil design system was used to design the external contours of the airfoils, and to establish the desired airfoil static pressure distribution. Figures 6 through 20 show the resultant airfoil shapes and surface pressure distributions of the three vane cascades and the two blade designs. Figures 6 through B show the Build 1 vane; 9 through 11, the Build 1 blade; 12 through 14, the Build 2 vane; 15 through 17, the Build 2 blade; and IB through 20, the Build 3 vane. A set of coordinates for these airfoils is presented in Appendix A.
8
VANE EXIT ROOT
BLADE EXIT
MEAN
~o MREL=~ 0298
Mil = 0 7582 Mil = 0 8441
!3 = 37 95° Cl = 10 43° Cl = 55 19°
TIP
Mil = 09124
Figure 4 Build 1 Velocity Triangles
9
VANE EXIT
ROOT
03513
MIL = 06986
(3 = 31 5540 a = 104320
MEAN
0233
MIL = 0 7482
(3 = 46 1180 a = 10 4320
MREL=
01608
Figure 5
10
TIP
MIL = 07992
Build 2 Velocity Triangles
BLADE EXIT
MIL = 0 7809
(3=16175 0 a=41746°
= 0 4893
MIL = 0 8486
(3 = 17 0750 a = 47 7270
0 0 10
09
04 1 0 l- 08 c.. 07 ...... en
08 20 c.. 06
05 Ci)
1 2 30 04 w ::I: 0 02 04 06 08 1 0 U Z 16 :2: x/bx - ~ >
20 1 50
24 RADIUS 2594 em (10211 In )
# FOILS 24
28 AXIAL CHORD 324 em (1 275 In )
LE DIA 1 02 em (0 400 In )
80 TE DIA 010 em (0040 In ) 0 1 0 20 30 UNCOVERED TURNING 8°
(CM) EXIT WEDGE ANGLE 4° FOIL INLET!3 90°
I I FOIL EXIT!3 11 68° 0 04 08 12 Max Mn s s 1 257
X (INCHES)
Figure 6 Build 1 Vane Root Section
11
0 0
04 1 0
08 20
Ci) 1 2 30 w J: :2: 40 U 1 6 2 ~
MEAN SECTION
> 20 50
24 60
28 70
32 80
o 10 20 30
(CM)
I I
o 04 08 12
X (INCHES)
VANE STACKING
Figure 7 Mean section Build 1 Vane
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MEAN SECTION CHARACTERISTICS
10
09
I-08
c.. 07 ...... en
c.. 06
05
04 00 02
PRESSURE DISTRIBUTION
RADIUS # FOILS AXIAL CHORD LE DIA TE DIA UNCOVERED TURNING EXIT WEDGE ANGLE FOIL INLET 13 FOIL EXIT 13
Max Mn s s
04 -
06 08 10
x/bx
2818 em (11 094 In )
24 324 em (1 275 In )
1 02 em (0 400 In )
010 em (0040 In )
o
04 10
08 20
1 2
en w 1 6 :I: :2: u 2 ~
20
>-24
28 70
32 80
36 90 0 10 20 30
(CM)
I I I I 0 04 08 1 2
x (INCHES)
10
I-08
c.. ...... en c.. 06
04
RADIUS tI FOILS AXIAL CHORD LE DIA TE DIA
0 02
UNCOVERED TURNING EXIT WEDGE ANGLE FOIL INLET iJ FOIL EXIT iJ Max Mn 55
04 06 08
x/bx
31 35 em (12 342 In )
24 324 em (1 275 In )
1 02 em (1 275 In )
010 em (0040 In )
10° 4° 90° 869°
1 136
Figure 8 Build 1 Vane Tip Section
14
12
1 0 en w
08 :I: U 2 06 ->-
04
02
0
30
20
1 0
09
I-~ 07 en c..
05
00 02 04 06 08 10
x/bx
RADIUS tI FOILS AXIAL CHORD LE DIA
2584em (10174 In)
54
O'-__ ......... __ ........II--_~ TE DIA UNCOVERED TURNING EXIT WEDGE ANGLE FOIL INLET iJ
3015 em (1 187 In )
o 30 em (0 117 In )
010 em (0040 In )
10° o
o
1 0 20 30
(CM)
0204 06 08 10 12
X (INCHES)
2° 2957°
FOIL EXIT iJ 1712°
Max Mn 55 1 359
Figure 9 Build 1 Blade Root Section
13
en w J: U Z
>
Figure 10
14
16 40
1 4
1 2 30
1 0
::2E 08 20 ~ MEAN SECTION
06
04 10
02
o o~ ______ ~ ____ ~~~~~ o 10 20 30
o
(CM)
04 08
X (INCHES)
BLADE STACKING
Build 1 Blade Mean Section
12 le. -rfl
RADIUS # FOILS
MEAN SECTION CHARACTERISTICS
05
PRESSURE DISTRIBUTION
28 17 em (11 093 In )
54 AXIAL CHORD 258 em (1 015 In )
o 30 em (0 117 In )
010 em (0040 In )
LE DIA TE DIA UNCOVERED TURNING 8° EXIT WEDGE ANGEL 2° FOILINLET/3 3203° FOILEXIT/3 1802°
Max Mn s s 1 461
1 6 40
14
12 30
-en 1 0 w ::t: U 08 Z
>- 06
04 10
02
0
10 20 (CM)
I I " I
o 02 04 06 08 10
X (INCHES)
10rr-----.....
I- 08 c.. -~ 06
04
o 02 04 06 08 10
x/bx
RADIUS II FOILS AXIAL CHORD LE DIA TE DIA UNCOVERED TURNING EXIT WEDGE ANGLE FOIL INLET i3 FOIL EXIT i3 Max Mn 55
3051 em (1201210 ) 54 2 14 em (084210 ) 030 em (0 117 10 ) 010 em (004010) 4° 2° 4474° 1892° 1442
Figure 11 Build 1 Blade Tip Section
o o
04 10
08
en ~ 12 U Z
16 >-
20
30
40
20 50
24 60
28 70
o 10 20 30
(CM)
o 04 08 12
X (INCHES)
Figure 12 Build 2 Vane Root Section
1 0
I- 08 c.. -en c.. 06
04 L..._-'-_...J.._---' __ .L-_...I
00 02
RADIUS II FOILS AXIAL CHORD LE DIA TE DIA
04 06
x/bx
UNCOVERED TURNING EXIT WEDGE ANGLE FOIL INLET i3 FOIL EXIT i3 Max Mn 55
08 10
2594em (1021110) 24 324 em (1 275 In ) 1 02 em (0400 In ) 010 em (004010 ) 8° 4° 90° 1043°
1 131
15
0 0
04 10
08 20
Cii' 1 2 30 w :z:: -(.) 1 6 ::: 40 :2 ~
> 20 50
24 60
28
32 80
VANE STACKING
0
I 0
10 20 30
(CM)
I 04 08
x (INCHES)
TIP MEAN ROOT
1 2
Figure 13 Build 2 Vane Mean section
16
MEAN SECTION CHARACTERISTICS
10
09
I- 08 11. en 07 11.
06
05
04L----L----~--~~---L--~ o 02
PRESSURE DISTRIBUTION
RADIUS tI FOILS AXIAL CHORD LE DIA TE DIA UNCOVERED TURNING EXIT WEDGE ANGLE FOIL INLET iJ FOIL EXIT iJ Max Mn s s
04 06 08 1 0
x/ox
28 18 em (11 094 In )
24 324 em (1 275 In )
1 02 em (0 400 In )
010 em (0040 In )
10° 4° 90° 1043° 1074
0
04
08
1 2 en w J: 0 1 6 2
>- 20
24
28
32
Figure 14
14
1 2
1 0
en w 08 J: 0 2
06 >-
02
o
Figure 15
:2 ~
o 10 20 30
(CM)
o 04 08 12
X (INCHES)
Build 2 Vane Tip Section
o~ ______ ~ ______ ~ o 1 0
(CM)
20
10
09 I- 08 c.. -en 07 c..
06 05
0
RADIUS # FOILS AXIAL CHORD LE DIA TE DIA
02
UNCOVERED TURNING EXIT WEDGE ANGLE FOIL INLET (J
FOIL EXIT (J Max Mn 5 5
04 06 08 1 0
x/bx
31 35 em (12342 In )
24 324 em (1 275 In )
1 02 em (0 400 In )
o 10 em (0040 In )
12° 4° 90° 1043° 0979
1 0 """_----_
04
03~--~--~--~~~--~ o 02 04 06 08 10
RADIUS # FOILS
x/bx
AXIAL CHORD LE DIA TE DIA UNCOVERED TURNING EXIT WEDGE ANGLE FOIL INLET(J FOIL EXIT (J
Max Mn 55
2584 em (10 174 In )
54 258 em (1 018 In )
o 30 em (0 117 In )
010 em (0040 In )
8° 2° 2498° 1618°
1484
o 02 04 06 08 10
X (INCHES)
Build 2 Blade Root Section
17
1 4
1 2
10
en w 08 :r: U Z
> 06 ~ ~
04
02
o
Figure 16
18
30
20
0
0
I 0
10
(CM)
I 02 04 06
X (INCHES)
BLADE STACKING
MEAN SECTION
20
I 08
ROOT
MEAN
TIP
Build 2 Blade Mean Section
MEAN SECTION CHARACTERISTICS
le:. rf' 06
04
02L-__ -L __ ~~ __ ~~~ __ ~ o 02 04 06 08 10
x/bx
PRESSURE DISTRIBUTION
RADIUS # FOILS AXIAL CHORD LE DIA TE DIA UNCOVERED TURNING EXIT WEDGE ANGLE FOIL INLET {3
FOIL EXIT {3
Max Mn s s
2818em (11 093 In )
54 2 22 em (0 875 In )
o 30 em (0 117 In )
o 10 em (0040 In )
6° 2° 4015° 1708°
1577
1 6
14
1 2
10 en w ::I: U Z
08
>- 061
04
02
0
Figure 17
0
04
08
en w 1 2 ::I: U Z - 16 >-
20
24
28
Figure 18
401
:;!: ~
10
0
0 10 20
(CM)
o 02 04 06 08
X (INCHES)
Build 2 Blade Tip Section
0
10
20
30
I-CL.
06 -en CL.
05
04
03 02
00 02
RADIUS # FOILS AXIAL CHORD LE DIA
TE DIA UNCOVERED TURNING EXIT WEDGE ANGLE FOIL INLET {J
FOIL EXIT {J
Max Mn s s
10
09
08
k" 07 -,fl 06
05
04 06 08 10
x/bx
3051 em (12012 In )
54 1 86 em (0 732 In )
o 30 em (0 117 In )
o 10 em (0040 In )
4° 2° 6953° 17 98°
1568
:;!: 04L-__ ~ __ ~ __ -L __ ~ __ ~
~ 40
50
60
70
0 1 0 20 30
X (INCHES)
I I 0 04 08 1 2
(CM)
o 02 04 06 08 10
RADIUS # FOILS AXIAL CHORD LE DIA TE DIA UNCOVERED TURNING EXIT WEDGE ANGLE FOIL INLET {J FOIL EXIT (J
Max Mn s s
1 6
x/bx
2594 em (10211 In )
24 324 em (1 275 In )
1 02 em (0 400 In )
o 10em (0040 In)
8° 4° 90° 1043°
1257
Build 3 Vane Root Section
19
0 0
04 1 0
08 20
en 1 2 30 w ::I: 2 ~ 16 ~
40
> 20 50
24 60
28 70
32 80
0 10 20 30
(CM)
I I 0 04 08 12
x (INCHES)
TIP
MEAN
."--ROOT
VANE STACKING
MEAN SECTION CHARACTERISTICS
10
I- 08 c.. -c..VJ
06
I I
04 '--_....J.. __ ..I...-_--I __ ...J..._---' o 02
PRESSURE DISTRIBUTION
RADIUS # FOILS AXIAL CHORD LE DIA TE DIA UNCOVERED TURNING EXIT WEDGE ANGLE FOIL INLET i3 FOIL EXIT i3 Max Mn s s
04 06 08 10 x/bx
2818 em (11 094 In )
24 3 24 em (1 275 In )
1 02 em (0 400 In )
o 10em (0040 In)
10° 4° 90° 1043°
1 196
Figure 19 Build 3 Vane Mean Section
20
I-08 c..
"-en c..
12
en w
1 6 ::I: U :2E z ~
> 20
24
28
32 80
o 10 20 30 (CM)
o 04 08 12
X (INCHES)
Figure 20 Build 3 Vane Tip Section
3.2 Mechanical Design
3.2.1 Design of Rig Subsystems
Disk
10
09
08
07
06 05
0 02 04 06
x/bx
RADIUS "# FOILS AXIAL CHORD LE DIA TE DIA UNCOVERED TURNING EXIT WEDGE ANGLE FOIL INLET J3 FOIL EXIT(j Max Mn s s
08 10
3135 em (12 342 In )
24 3 24 em (1 275 In )
1 02 em (0 400 In )
010 em (0040 In )
12° 4° 90° 1043° 1 136
The rotor disk was conservatively designed for a nominal 30-percent burst margin above maximum anticipated operating speed. Computer analysis ensured that the stress levels in this disk were consistent with structural design criteria.
Blade and Disk Attachments
Blade and disk attachments were designed to keep stresses well within design margins. Potential vibratory stress problems were avoided by "tuning" the disk design to provide a frequency margin at 24E vane passing exitation for both the low and high reaction blades at maximum speed and to keep the occurrence of low order resonances well above maximum speed (see Figures 21 and 22). Fixed inlet rakes were aerodynamically configured and located sufficiently upstream to minimize any potential exitation from this source. Blade and
21
disk-coupled vibration characteristics were analyzed by a conventional beam analysis and a more rigorous NASTRAN finite element vibration analysis. Blade dampers controlled the levels of buffeting and resonant response.
Cl Z Cl 10
w t:) w w W 0.. Ui 0.. en w
Cl en 40E w Cl X
...J w t:) w ~ Cl 0.. :::;; BLADE ALONE a: en 36E
8 DAMPER DEFLECTION RATIO = 9 9%
32E
N 28E
J: 6 26E ~
>" 24E
U 22E Z 20E w :::> 18E 0 4 w 16E a: 14E LL
12E
10E 2
OL-______ ~ ______ ~~ ____ ~ ____ ~~------~------~------~~----~. 6
Figure 21
7 8 9
ROTOR SPEED, KRPM
Uncooled Rig Resonance Diagram (Build 1 Low Reaction Blade) -Results of an initial beam deck analysis with disk rim and blade root changes made to avoid first or second mode resonances with the number of nozzle vanes (24) in the rig operating range.
Bearing Arrangements
Bearing arrangements were established on the basis of rotor stiffness, weight, and speed. The optimized bearing arrangement ensured that the operating range was free of vibrational modes that could otherwise cause premature hardware failure.
22
10
8
N ~ ~ 6
> U Z w ~ a w ~ ~
6
Figure 22
0 z 0 w ~ w w ~ w ~ w ~ ~ 0 ~ w 0 w ~ ~ w X 0 ~ ~
BLADE ALONE ~ ~ ~ 40E
36E
32E
28E 26E
BLADE ALONE ~E
22E 20E 18E 16E 14E 12E
10E
ROTOR SPEED. KRPM
Uncooled Rig Resonance Diagram (Build 2 High Reaction Blade) -This diagram is based on the same calculation procedure and requirements as the Build 1 design (see Figure 21).
3.2.2 Design of Test Rig
The test rig, illustrated in Figure 23, was used both for the vane annular cascade testlng and full-stage (rotating rig) testing. A unique feature of the rig was the circumferentially traversing instrumentation ring, which permitted pressure, temperature, and six angle measurements both radially and circumferentially in the flowpath. The total range of circumferential travel for a given sensor mounted on the ring was 30 degrees (corresponding to two vane pitches). This flowpath scanning capability is illustrated in Figure 24.
23
Figure 23
BLADE OUTER AIR SEAL
CIRCUMFERENTIALLY TRAVERSING INSTRUMENTATION RING
~ NEW HARDWARE
Energy Efficient Engine High-Pressure Turbine Uncooled Rig - A unlque feature of the rig is the circumferentially traversing instrumentation ring which permits pressure, temperature, and air angle measurements both radially and circumferentially in the flowpath. '
The test rig was adapted to annular cascade testing as shown in Figure 25. Filler pieces were installed in the rig flowpath to cover the steps in the flowpath that originally contributed to endwall losses. In addition, the rotor and blade outer air seal assemblies were removed, and the inner and outer diameter exit flowpath ducts and instrumentation ring were moved forward to the exit instrumentation plane.
24
Figure 24
--
0.300
(LOOKING UPSTREAM)
Circumferentially Traversing Exit Instrumentation Ring - The total range of circumferential travel for a given sensor mounted on the ring is 30 degrees (corresponding to two vane pitches).
Structural design criteria and mechanical constraints consistent with experimental hardware were used to establish the design configuration of the test rig. Computer programs helped determine airfoil stresses and deflections caused by centrifugal force, gas bending loads, and foil-to-platform transitions. Computer analysis also established the proper running clearance in order to simUlate the tight clearances required by the full scale component.
25
Figure 25
)=:'
FLOW DIRECTION
•
IDWAll
)
FlllER PIECES IN STEP lOCATIONS
ODWAll
Uncoo1ed Rig Modifications Required for Annular Cascade Testing - For vane annular cascade testing, the rotor and blade outer air seal assembles were removed and the inner and outer diameter exit flow path ducts and instrumentation ring moved forward to the exit instrumentation plane of the vane annular cascade.
A rotor dynamics analytical model of the rig was constructed and the critical speed analysis was run to predict system resonances and mode shapes. The analysis of rig critical speed characteristics (Figure 26) demonstrated that the inherent stiff bearing margin of 100 percent was sufficient to compensate for any potential high strain energy modes that might occur in the rig running range. Trim balance capability was incorporated into the rig to provide additional margin. In addition, the rig speed control system was set to allow a 2000 rpm margin of safety between maximum overspeed and burst speed in case of a water brake failure.
In order to reduce cost, the rig utilized many parts from an existing Pratt & Whitney Aircraft single-stage rig. Hardware designed and fabricated to adapt
26
that rig for testing is shown in the shaded areas of Figure 23. The major items designed for this program were:
o inlet cases o vane airfoil and inner and outer shrouds o the rotor (including disk, blade airfoils, sideplates, dampers, and speed
pickup ring) o the blade outer air seal o the circumferentially traversing instrumentation ring o exit outer cases interfacing with the rotor rim seals o instrumentation.
30
25
20
:;§: c.. e: ~
c:l w w c.. 15 til -I « u l-e: U
10
5
RSE - ROTOR STRAIN ENERGY
MAX SPEED
14% RSE I
I I I I I
97% RSE
100% RSE
o~ __________ ~ ____________ ~ ____________ ~~ __________ ~~ __ __
105 106 107 108 109
BEARING AND SUPPORT SPRING RATES, LB/IN
Figure 26 Critical Speed Characteristics - A stiff bearing critical speed margin of 100 percent is sufficient to guarantee no modes with high levels of rotor strain energy in the engine operating range.
27
This Page Intentionally Left Blank
4.0 FABRICATION AND ASSEMBLY
4.1 Fabrication
In this task, hardware was procured and fabricated based on the specifications established in the analysis and design task. AMS 5613 material was used in all of the major parts.
The fabrication procedures used for each of the rig sub-assemblies (blades, vanes, disks and sidep1ates, cases, and shaft and main bearings) were structured to maximize the use of existing hardware and established machining procedures. Fabrication procedures are discussed in sections 4.1.1 through 4.1.5.
4.1.1 Blades
Two sets of blades (one set for each of the builds of the rotating stages) were fabricated. Each set incorporated the different aerodynamic configurations defined in Table 2 (see page 4). As the blades were fabricated, provisions were made for the necessary instrumentation.
The blade airfoil sections for Build 1 testing were electrochemically machined; the blade platform, trailing edge, and fillet radii were conventionally machined. The electrochemical machining process used in Build 1 blade fabrication was judged too costly and too time consuming for Build 2 blade fabrication; therefore, the Build 2 blades were conventionally machined.
To ensure that blade contours were within established tolerances, each blade was shadowgraphed at the mean section, and every sixth blade was shadowgraphed at the root, mean, and tip sections. Seventy-two shadowgraphs were made for each build.
4.1.2 Vanes
Three sets of vanes were fabricated (each set fabricated for use in the vane cascades was later reused in the rotating stage tests). Each set incorporated the different aerodynamic configurations defined in Table 2 (see page 4). Provisions were made for the necessary instrumentation as the vanes were fabricated.
The vane airfoil sections for Build 1 testing were electrochemically machined and the endwalls were finished by a computer controlled milling machine operation. The vanes were difficult to secure during machining because of their longer chord geometry. The conventional techniques were modified to provide the rigid support needed to hold the vanes in place during the machining process.
The electrochemical machining process used in Build 1 vane fabrication was judged too time consuming for Build 2 and Build 3 vane fabrication; therefore, the Build 2 and Build 3 vanes were conventionally machined. The l3-degree canted vane did not cause any unusual machining problems. Each vane was shadow-
29
graphed at the root, mean, and tip sections to ensure that vane contours were within established tolerances. Two hundred and sixteen shadowgraphs were taken for the three builds.
4.1.3 Disks and Sideplates
Disks and sideplates were fabricated from raw material using standard machining practices.
4.1.4 Cases
Inlet and exhaust cases were made available from an existing in-house rig. The cases required only minor modifications to accommodate the dimensional standards of the rig flowpath. Inner and outer diameter rings for the vane assembly were fabricated from raw material by standard machining practices.
4.1.5 Shaft and Main Bearings
The main shaft, stub shaft, bearing housings, and oil jets were made available from in-house hardware. Vendors, following Pratt & Whitney Aircraft specifications, fabricated the No.4 and No.5 bearings and the No.4 and No.5 carbon seals.
4.2 Assembly
Following fabrication, the hardware was assembled into the required configurations using normal bench assembly procedures. These procedures, as applied to each of the rig subassemblies, are discussed in sections 4.2.1 through 4.2.5.
4.2.1 Vanes
A typical vane assembly is illustrated in Figure 27. Each assembly contained 24 vanes. Six vanes were instrumented with surface static pressure taps and with mid-gap chordwise and trailing edge gapwise wall static pressure taps. Each vane was secured at the outer diameter by two pins and at the inner dia~ eter by one pin. The two vanes equipped with surface static instrumentation at the tip section were held in place without the bolt. The seal lands in the vane inner diameter shrouds were machined rough while the vanes were being finished machined. Following this procedure, the seal lands were built up with epoxy to ensure that they were dimensionally concentric.
Gaging dimensions were measured at three locations along the gaging plane. Actual gaging areas were calculated from these dimensions and compared with the design areas. Agreement between design gaging areas and actual areas is shown in Table 5. Trailing edge mid-span angles and flowpath diameters were also measured.
30
Figure 27 Uncoo1ed Rig Vane Assembly
TABLE 5
VANE THROAT AREA
Design (cm sq. (in. sq.» Actual em Sq. (in. Sq.»
Build 1 138.19 (21. 418) 137.14 (21.256)
Build 2 143.20 (22.194) 141.16 (21.878)
Build 3 143.20 (22.194) 145.94 (22. 619)
4.2.2 Rotor
A typical rotor assem~ly is illustrated in Figure 28. Each assembly contained 54 blades. Nine blades were instrumented with surface static pressure taps and immersion thermocouples. Strain gages were placed on four blades of the first build of the rig and on three blades of the second build. To ensure dimensional concentricity, the blade tips, seal lands, and knife edge seals were machined to their final diameters while assembled in the disk. The blade outer air seal was also machined during assembly so that it would be concentric with the inside diameter of the rear main bearing housing. Wire seals were axially positioned in grooves at the edge of the blade platform to control radial leakage. Blade dampers were also included.
31
Figure 28 Uncooled Rig Rotor Assembly
Blade instrumentation was led out through rivet holes and through openings created by drilling into the rear sideplate. The leads were then routed along the rear face of the disk and out to the base of the driveshaft.
Gaging dimensions were measured at three radial locations of 42 blades (instrumented blades were not included in this measurement). Actual gaging areas were then calculated from these dimensions and compared to the design gaging areas. Agreement between design values and actual values is shown in Table 6. Flowpath dimensions and blade tip diameters were also measured.
Build 1
Build 2
32
TABLE 6 BIADE THROAT AREA
Design (cm sq (in. sq.» Actual (cm sq. (in. sq.»
239.92 (37.185) 240.53 (37.280)
223.79 (34.685) 225.68 (34.979)
4.2.3 Cases
Many of the inlet and exhaust cases used in this program were made available from in-house hardware supplies. These cases required only the following modifications to conform to program requirements: (1) the case flanges had to be modified to accommodate required dimensions of the rig flowpath and (2) the radial step of the exhaust case had to be leveled by adding filler rings. This same exhaust case was used in both the cascade and the rotating rig tests (the filler rings were removed before the rotating rig tests).
The rig exit plane instrumentation caSe was adapted to program requirements from readily available parts. To permit circumferential traversing, the case was axially positioned on a Teflon-coated surface with eight bearings. Four additional bearings radially supported the case. Two "pusher" type traverse cans were used to circumferentially rotate the case. Flat-faced, spring-loaded Teflon seals prevented leakage.
4.2.4 Shaft and Main Bearings
The main shaft, stub shaft, bearing housings, and oil jets were also made available from in-house hardware supplies. The No. 4 and No. 5 carbon seals and the No. 4 and No.5. bearings were new parts.
Bearing compartments were assembled in accordance with established procedures. The duplex bearing was assembled in a tandem arrangement to increase bearing life. Critical measurements verified that the assembly met design specifications. The oil jets were examined to ensure that they provided the desired oil flow patterns. No additional modifications were required for incorporating thrust balance air.
4.2.5 Stand Instrumentation
Provisions were made for specialized instrumentation (in addition to the previously discussed instrumentation). This instrumentation included accelerometers, vibration pickups, thermocouples, and optical proximity probes. Accelerometers were positioned vertically and horizontally on the front and rear bearing housings. Vibration pickups were located vertically and horizontally on the outer inlet and exit cases. Thermocouples were placed at the No. 4 and No.5 bearings and at the No.4 and No. 5 carbon seal locations. The three optical proximity probes, positioned in the blade outer air seal, recorded blade tip clearances at each performance condition. These probes were backed up by three rub buttons, also built into the blade outer air seal. The blade surface static pressure instrumentation was recorded by the data system via a rotating scanivalve system.
33
5.0 TESTING
5.1 General Description
A test program was established and conducted to substantiate the program objectives described in section 3.1. This included (1) use of a test facility designed to simulate an engine operational testing environment over the range of test parameters evaluated, (2) test rigs designed for low cost but retaining the capability to accurately duplicate the full-size high-pressure turbine design definition, (3) instrumentation specifically selected or designed to maximize data acquisition capability without unduly perturbating the flow characteristics of the rig, (4) time tested procedures and equipment for data acquisition and recording plus "real-time" data reduction capability, permitting rapid and accurate assessment of test results, and (5) test conditions and parameters chosen to provide the most effective range of data with which to accurately determine rig performance. Specific details of this test program are described in the following sections.
5.1.1 Test Facility
All testing was conducted at the Pratt & Whitney Aircraft X-2l2 test stand. The test turbine was mounted on an open bedplate and connected to the inlet air collector and exhaust duct. Air was supplied by laboratory compressors. The power generated by the turbine was absorbed by a waterbrake, and exit conditions were varied using flow exhausters. All controls and instrumentation required to operate and monitor the testing were located in a room adjacent to the test cell.
For emergency purposes, an explosive-actuated burst disk was located in the inlet duct to enable the rapid discharge of high-pressure air. If an emergency had arisen, the explosive would have been detonated within 50 milliseconds after receiving a signal from the overspeed limiter.
5.1.2 Test Rigs
Each of the hardware subassemblies described in section 4.2 was incorporated into the completed test rig and mounted in the test stand. Figure 29 shows a vane cascade test rig; Figure 30 shows a rotating test rig mounted for testing. The exhaust cases have been pulled back to expose details of the flowpath hardware.
Figure 31 identifies the locations of the primary instrumentation used in the rigs. A detailed description of the instrumentation used in the test program is presented in section 5.2.
5.2 Instrumentation
5.2.1 Annular Cascade Instrumentation
The primary performance instrumentation for the rig consisted of inlet total temperature and inlet and exit total pressure rakes (see Table 7). Additional instrumentation was used to measure primary and secondary flow rates, exit flow angle, static pressures (airfoil, flowpath, and cavity), cavity air temperatures, and metal temperatures.
35
Figure 29 Annular Cascade Rig
36
Figure 30 Rotating Rig
37
CAVITY STATICS (Ta, Ps) LOCATED RADIALLY ALONG WINDAGE PLATE
CAVITY STATICS (Ta, Ps) LOCATED IN REAR DISK CAVITY
= CAVITY STATICS (Ta, Ps) LOCATED IN FISHMOUTH SEAL
INLET INSTRUMENTATION PLANE PT & TT
CIRCUMFERENTIALLY TRAVERSING INSTRUMENTATION RING PT, TT, AIR ANGLE
Figure 31 Uncooled Rig Primary Performance Instrumentation
Exit instrumentation was mounted on a circumferentially traversing instrumentation ring supported on the outer diameter. The instrumentation ring contained 4 radially fixed total pressure rakes and 4 radially traversing air angle probes. The traversing ring rotated through 30 degrees; therefore, the four probes mapped 120 degrees of the exit circumference.
5.2.2 Rotating Rig Instrumentation
For the rotating rig test, the ring contained 4 radially fixed total pressure rakes, 4 radially fixed total temperature rakes, 1 radially traversing concentric temperature/pressure probe, and 3 radially traversing air angle probes. The total range of circumferential travel for a given sensor mounted on a ring was 30 degrees (corresponding to two vane pitches). The instrumentation used in the rotating rig tests is summarized in Table 8.
38
Location ~
Inlet Pt, Tt
Inlet Ps
Vane Sur face Ps
Vane Endwalls Ps
Exit
TABLE 7
ANNULAR CASCADE TEST INSTRUMENTATION
Quantity
4 Pt Rakes, 8 Tt Rakes (10 Sensors per Rake)
12 Total, 6 Each on the Inner and Outer Flowpath Walls
51 Total, on the Pressure and Suction Surfaces at Three Radial Locations
42 Total, on the OD and ID Vane Channels
4 Rakes (10 Sensors per Rake) Mounted on the Outer Diameter Supported Circumferentially Traversing Instrumention Ring
Exit Air Angle, Pt 4 Radially Traversing Probes Mounted on the Circumferentially Traversing Instrumentation Ring
Exit Ps
Exit
Exit
12 total, 6 each in the inner and outer vane cavi ties
20 Total, 12 on the Inner Diameter Flowpath and 8 on the Outer Diameter Flowpath
10 Total Along the Inner Diameter Flowpath Inner Liner to Exhaust Dump
The primary performance instrumentation for the rig consisted of inlet and exit total temperature and total pressure rakes (see Table 8). Additional instrumentation was used to measure primary and secondary flow rates, speed, exit flow angle, static pressures (airfoil, flowpath, and cavity), cavity air temperatures, metal temperatures, and blade tip clearance.
5.3 Test Procedures
5.3.1 Annular Cascade Test Conditions
The annular cascade test consisted of operating points covering a range of vane pressure ratios (exit Mach numbers). Inlet conditions were held constant and the cascade exit static pressure was varied using exhausters. The annular cascade test program is summarized in Table 9.
39
Location
Inlet
Inlet
Vane Surface
Vane Endwalls
Vane Exit
Blade Surface
Exit
Exit
Exit
Exit
Exit
various Cavities
Disk Blade
Rotor Casing
Rotor Casing
40
TABLE 8
ROTATING RIG TEST INSTRUMENTATION
Ps
Air Angle, Pt
Concentric, Pt, Tt
Ps
Proximity Probe
Quantity
4 Pt Rakes, 8 Tt Rakes (10 Sensors per Rake)
12 Total, 6 Each on the Inner and Outer Flow path Walls
54 Total, on the Pressure and Suction Surfaces at Three Radial Locations
42 Total, on the OD and ID Vane Channels
12 Total, 6 Each in the Inner and Outer Vane Cavities
35 Total, on the Pressure and Suction Surface at Three Radial Locations
4 Pt Rakes, 4 Tt (12 Sensors per Rake) Mounted on the Outer Diameter Supported Circumferentially Traversing Instrumention Ring
3 Radially Traversing Probes Mounted on the Circumferentially Traversing Instrumentation Ring
1 Radially Traversing Probe Mounted on the Circumferentially Traversing Instrumentation Ring
12 total, 6 each in the inner and outer blade cavities
20 Total, 12 on the Inner Diameter Flow path and 8 on the Outer Diameter Flow path
48 Ps , 48 Ta for Diagnosis
12 Tm at 4 Radial Locations for Tip Clearance Analysis and Rotating Static Corrections
9 Tm for Tip Clearance Analyses
3 Laser Probes for Tip Clearance Measurement
TABLE 9
TYPICAL RUN FOR ANNUIAR CASCADE TESTING
Operating Exit PT inlet TT inlet Point Mach No. PSIA Degrees R Ps exit/PT inlet
1 0.70 57.42 775 0.70 2 0.80 57.42 775 0.64 3 0.92 57.42 775 0.56 4 1.01 57.42 775 0.49 5 1.13 57.42 775 0.41
5.3.2 Rotating Rig Test Conditions
The rotating rig test covered approximately 12 operating conditions, consisting of a range of turbine speed parameters, pressure ratios, and front disk flow rates. The values that were determined included the sensitivity of the blade-to-incidence angle, Mach number, and the injection of the front disk leakage flow. Inlet conditions were held constant, and the turbine conditions were varied by exit flow exhausters and a power absorbing waterbrake. Flow was injected into the primary flow stream at varying rates. This flow was directed through the front disk cavity at the pressure ratio and speed parameter of the design point. The rotating rig test program is summarized in Figure 32 •
Figure 32
• DESIGN POINT
0 DATA TAKEN
390 0 0 0 PLANNED, BUT NOT TAKEN DUE TO STRESS
375 0 0 0 0 PROBLEMS
3501 0 • 0 0 0
315
2801
o o
o
3.5 4.0
o
o
4.5
PRESSURE RATIO
o
5.0 5.5
Typical Run For Rotating Rig Testing - Additional testing was conducted to determine the effect of leakage by injecting air into the front disk cavity at the design point conditions.
41
5.3.3 Data Acquisition
Annular cascade and rotating rig data were acquired in a planned sequence for all of the test conditions.
5.3.4 Data Recording
All test data were automatically recorded by a time sharing computer (Sigma 8) via a remote batch terminal located at the test stand. Pressure data were acquired by scaniva1ves using high precision transducers with negligible hysteresis. Thermocouples were "hooked into" Universal Temperature Reference boxes with unbroken leads to copper buses before the signal went to the digital voltmeter. Pressure and temperature data proceeded through a high accuracy digital voltmeter to the remote batch terminal. The data were then processed through the Sigma 8 computer, converted into engineering units, and either displayed at the test stand or printed.
5.3.5 Data Reduction
Data from the annular cascade test were reduced to row total pressure loss, which was calculated from the measured spanwise and circumferential inlet and exit total pressure traverses. Measured vane exit air angle profiles, airfoil static pressure distributions, and endwa11 static pressures were also determined from the data.
Rotating rig efficiency was calculated using the measured inlet and exit total temperatures and pressures. Stage exit air angle profiles, vane and blade static pressure distributions, endwa11 static pressures, cavity static pressures and air temperature, flows, mechanical speeds, clearances, and metal temperatures were measured, recorded, and presented. Data was then analyzed and compared with the predictions.
5.3.6 Shakedown Testing
During assembly, instrumentation was first installed and connected and was later checked for identification and leakage. The shakedown procedure consisted of obtaining a complete data point to substantiate the mechanical integrity of the test rig and to verify the performance of the instrumentation and data acquisition systems. The testing resumed after it was ascertained that all instrumentation and systems were operating properly.
5.3.7 Rotating Rig Stress Testing
Four blades of the Build 1 rotating rig were eac' instrumented with one strain gage (see Figure 33) to monitor vibratory stresses during performance testing. During the initial attempt to acc(.erate to design speed (nominal 9800 rpm), a first mode 24E resonance was encountered at 8900 rpm with blade stresses reaching 18 ksi. These stresses were higher than normal test limits, so a review of the running program was instituted. To reduce these stresses, thereby allowing accelerations to design speed, rig inlet pressure was
42
decreased and the rig was rapidly accelerated through the 24E resonance. The combination of increased rate of acceleration and reduced inlet pressure resulted in acceptable airfoil stress levels which allowed performance testing at the higher speeds.
Figure 33
TIP
A
LE
GAGE ORIENTATION
CONCAVE SURFACE
A
0.864 em (0.34 in.)
-1. __ ..1-_ A
TE
Strain Gage Location (Build I)-Installed to monitor vibratory stresses during performance testing.
43
The experience gained in Build 1 with the low reaction blading and the Slmllarity of resonant characteristics between low and high reaction blading indicated that the Build 2 high reaction blading should be equipped with strain gages. Three blades of the Build 2 rig were instrumented with 4 gages on each blade to better define the dynamic stress distribution in the modes of response. During Build 2 testing, high stresses again occurred in the first mode 24E resonance at approximately 8800 rpm, reaching a maximum of 34 ksi. Again, rig inlet pressure was reduced and the rig rapidly accelerated through the 24E resonance so that performance data could be acquired at higher speeds.
The high 24E first mode stresses of Builds I and 2 were thought to be associated with a higher than predicted resonant speed coupled with inadequate mechanical damping. The rig incorporated a wire seal, positioned between the platforms of adjacent blades for sealing, plus a damper, located under the platforms for minimizing resonant response (see Figure 34). The indications from both Builds I and 2 were that either the wire seal, the damper, or both, were "locked up." This condition would produce higher frequences and minimal mechanical damping. Since the wire seal and damper were parts unique to the rig, an abbreviated test plan was formulated to evaluate the frequency and stress response of the Build 2 high reaction blades. For this test, a lighter weight design was created by removing the wire seal and reducing the damper thickness.
Figure 34
44
lHRE SEAL
DAMPER
WIRE SEAL
Rig Wire Seal and Damper-Wire seals were used to prevent leakages between adjacent platforms and dampers were used to minimize resonant response.
5.3.7.1 Test Program
The primary objectives of this program were to (1) determine how the removal of the wire seal and the reduction of the size of the damper seal would affect the resonant frequencies and (2) determine how effective a platform damper is in minimizing dynamic response.
Bench Testing
Four low reaction blades were tested in the holography laboratory to define mode shapes and frequencies. Each blade was held in a broach block that was uniformly squeezed from the sides. The broach block loading was sufficient to prevent attachment slippage and maintained at a constant level for each blade. Typical holograms are shown for the first five modes in Figure 35 where significant chordwise bending motion can be noted even in the first flap mode. These mode shapes required the use of additional strain gages in the rotating rig test to adequately define actual airfoil stress distribution in the various modes of response.
1st FLAP 1st STIFF
1st TORSION 2 nd FLAP TIP CHORDWISE
Figure 35 Vibrational Holographic Analysis of the Energy Efficient Engine Cold Flow Rig Turbine Blade
45
The three high reaction blades previously instrumented in Build 2 were reinstrumented with eight strain gages per blade (see Figure 36).These gages were located at expected areas of high stress for the 5 modes previously identified. Bench testing was then performed at room temperature to define the vibratory stress distribution in each of these first five modes. Figure 37 shows the level of stress for each gage location in terms of a percentage of maximum for the first two modes •
• EIGHT 40.64 em (1/16 IN.) DYNAMIC STRAIN GAGES PER BLADE • THREE BLADES (SN 43,49 & 56)
CONCAVE SURFACE
10° TIP
C - -- +--...,--- --_-~---r"~ #4 ,
B---~I--""'--~ r-B #3 r
4.414 em (1.738 in.1
LE 3.703 em (1.458 in.)
A---f--Ir-91
CONVEX SURFACE
TIP
TE
AT FILLET RUNOUT
C-- _"#S-----t---C
TE
-'_#7---"""1""--+--- B
#6
3.703 em (1.458 in.) LE
-11l1li---.... --+--- A
t B
#7
1.194 = '0.47 ;0.(' ~ ) -VSECTION B-B
t C
1.676 em (~.66 i~
Y SECTION C-C
Figure 36 Strain Gage Location (Stress Test and Bench Test)
46
l r-~-+----....,
97-100%
1 .194 em -+ ___ ~ 4.414 em (1.738 in.)
3.70 em (0.47 in.)
0.254 em (0.1 in.)
(1.458 in.) 1.943 em
r(0.765 in.) l @]
SUCTION SIDE
((; 92-99%
<2> 84-92%
~
-----1ST MODE
97-100%0
95-99% <§>
051-53% OJ 96% 86-
,-J
PRESSURE SIDE
-
\ 86-91%81
\ 100%<9 \
\~ NODE
" " "- ........ ......
@]<10% @]<10% ill 22-27% ~----~~------~~
2ND MODE
Figure 37 Stress Ratios From Blade Bench Tests
47
Rig Testing
A slow acceleration was run to 11,000 rpm followed by a slow deceleration. Stress levels for all three blades were recorded during this running for all 24 strain gages. The previously recorded 24E first mode resonance from Build 2 was noted to be approximately 1000 rpm lower and responded at about 25 percent of the stress level. These two facts met the primary objectives of the test by showing that removing the wire seal and reducing the size of the damper did lower the first mode frequency as well as show that this mode could be effectively damped at the under platform location.
5.3.7.2 Results and Conclusions
Test results confirmed that lower stresses were obtained when the rig-unique wire seal and damper design were replaced with a modified lighter weight damper. This type will be used in the engine. Also, the frequency information gathered from the bench and rotating rig testing was used to adjust the NASTRAN analysis for the component design (see Figure 38).
en c.. (,)
(Y) o
Figure 38
.... C >() :2 w ::J o w ex: u..
10
2
Rig Blade effect of frequency
4 6
W -1 o
Z <.:J Vl w o
ROTOR SPEED (X103 RPM)
10
w z
12
Resonance Diagram - 24E first mode response wire seal removal and damper size reduction and stress.
14
shows the on
As a result of this test program, the component rotor design effort will include evaluation of lighter weight design concepts for the damper located under the blade platforms.
48
6.0 RESULTS
6.1 Annular Cascades
6.1.1 Performance Discussion
6.1.1.1 Loss Comparison
Vane losses, which include span mass averaged total loss, endwall loss, and profile loss from the three annular cascade tests, are shown in Figures 39 and 40 for the wedge probes and the exit rakes. On each figure, all losses are plotted against mass averaged Mach number; the endwall loss (or secondary loss) is derived by subtracting the profile loss from the total vane loss. The wedge probes were in the axial plane of the blade leading edge (about 0.46 in. axially from the vane trailing edge). The exit rake kiel heads were further downstream (about 0.84 in. axially). Therefore, increased mixing losses cause the losses measured by the rakes to be higher than losses measured by the probes.
The testing of three different vanes in annular cascades has substantiated the low loss predictions established for the uncooled rig. The trends with profile loss are in excellent agreement with predicted values. A comparison of the data at the blade leading edge location shows the canted vane to have the lowest mass averaged total losses. The Build 1 vane had the next lowest losses, and the Build 2 vane had the highest losses.
6.1.1.1.1 Data Presentation
The contour plots for the three builds of the annular cascade show a clean low loss core flow and higher loss endwall and wake regions (see Figures 41 through Figure 43). These data were acquired from the radial circumferential traversing of the exit probes.
The low loss core region is also shown by circumferentially area averaging the vane loss contours and plotting the results spanwise (see Figure 44). The comparison between the data from the probes and rakes shows the additional mixing loss at the rake station to be predominately at the inner diameter. A spanwise comparison of the probe data shows the Build 1 vane to have higher loss at the inner diameter and lower loss at the outer diameter than the Build 2 vane. The figure also shows additional reduction in loss at the inner diameter and increased loss at the outer diameter caused by canting the Build 2 vane 13 degrees in Build 3.
The comparison of total losses, generated by mass averaging the spanwise losses with the results from the air angle traverse, showed the lower loss at the outer diameter for Build 1 outweighs the higher loss at the inner diameter, thereby giving the Build 1 vane a lower mass averaged total loss than the Build 2 vane at the same Mach number (see Figure 39). The results of the canted vane tests showed the reduced loss at the inner diameter outweighed the increased loss at the outer diameter to give the canted vane the lowest mass averaged total loss of the three airfoils tested.
49
0.13 TOTAL LOSS
0.11
0.09
0.04 « 2! 0 Cl. --.
Cl. <J
0 0.02
8 Ch 6 6
0
0.05 MIDSPAN LOSS 0
Cl. --. 0.03 Cl. <J
0.01
0.7 0.8 0.9
MNMA
Figure 39 Annular Cascade Pressure Loss vs Mach Number
50
013 TOTAL LOSS
011
009
« :2: 007 c.. --c..
<l
005
CO VANE
OBLD 1 003
OBLD2
6 6 6BLD3
001 __ PREDICTED
006 ENDWALL LOSS
004 0 « 0 :2 0 c.. ~ --c..
<l 002
6
0
005 MIDSPAN LOSS
c.. -- 003 c.. <l
001
07 08 09 10 11 1 2 13
MNMA
Figure 40 Annular Cascade Pressure Loss vs Mach Number
51
:- f- - r L L ....... Jj-~ i t--t---t-... Curve Label Curve Value d PIP
Figure 41
52
2 3 4 5 6 7 8 9
10 11 12 13 14 15 16 17
0.0 0.01000 0.02000 0.03000 0.04000 0.05000 0.06000 0.07000 0.08000 0.09000 O. 10000 0.11000 0.12000 0.13000 O. 14000 O. 15000
BUlld 1 Mnma = 0.997
Typical Vane Loss Contours at Design - This plot represents circumferential traverse data over two vane gaps at 8 radial p:>s i ti ons •
Figure 42
Curve Label Curve Value
2 0.0 3 0.01000 4 0.02000 5 0.03000 6 0.04000 7 0.05000 8 0.06000 9 0.07000
10 0.08000 11 0.09000 12 O. 10000 13 0.11000 14 O. 12000 15 O. 13000 16 O. 14000 17 O. 15000 18 O. 16000 19 0.17000 20 O. 18000 21 0.19000 22 0.20000 23 0.21000 24 0.22000 25 0.23000 26 0.24000 27 0.25000
BUlld 2 Mnma = 0.932
Typical Vane Loss Contours at Design - This plot represen~s circumferential traverse data over two vane gaps at 10 radial positions.
53
~ PIP
Figure 43
54
Curve Label Curve Value
2 0.0 3 0.01000 4 0.02000 5 0.03000 6 0.04000 7 0.05000 8 0.06000 9 0.07000
10 0.08000 11 0.09000 12 O. 10000 13 O. 11000 14 O. 12000 15 O. 13000 16 O. 14000 17 0.15000 18 O. 16000 19 0.17000 20 0.18000 21 0.19000
BUlld 3 Mnma = 0.951
Typical Vane Loss Contours at Design - This plot represents circumferential traverse data over two vane gaps at 9 radial positions.
AP/P
RAKE PROBE MASS AVG MASS AVG MACH # MACH #
BUILD 1 0 0971 • 0997
BUILD 2 0 0909 • 0932
024 BUILD 3 6 0945 • 0951
020
016
c.. 0: 012 <J
008
004
OL-____ ~ ____ _L ____ ~ ______ L_ ____ ~ ____ _L ____ ~ ____ ~L_ ____ ~ ____ ~
o
Figure 44
10 20 30 40 50 60 70 80 90
% SPAN
Vane Loss vs Percent Span - The low loss core region is indicated by circumferentia11y averaging the vane loss and plotting the results spanwise.
100
55
The mass-averaged total losses for Builds 1, 2 and 3 were .0376, .0369 and 0.0245, respectively, at the design conditions as measured by the exit probe.
Vane gas exit angle is important for good performance, because blade inlet conditions, incidence distribution, and flow distribution are functions of vane exit angle and wheel speed. Design point vane exit angle spanwise data are shown in Figure 45. The level of the measured data, acquired with a radial traverse at mid-gap, was adjusted to match continuity. The data shows the angle skews, with higher angles near the inner diameter and lower angles near the outer diameter. Build 3 has the largest skew, Build 1, the next largest, and Build 2, the least. Although_the angle skew was not predicted, good overall rotating rig performance for Build 1 and Build 2 suggests that the incidence and flow distribution shown in the annular cascade were not the same in the rotating rig because of a redistribution of flow caused by the rotor. The Build 3 vane was not tested in a rotating rig, therefore, it is not known if its larger angle skew would cause a performance penalty. For this reason, the Build 3 vane will not be used in the engine design without additional rig work. Therefore, the Build 1 vane, having proven air angle distribution and lower loss than the Build 2 vane at comparable Mach numbers, will be used for the engine design. Additional data for the annular cascade tests for Builds 1, 2 and 3 are presented in Appendices B, C, and D, respectively.
6.1.2 Analysis Discussion
6.1.2.1 Deviation
Airfoil deviation is defined as the difference between the exit air angle and the gage plane (throat) air angle. The calculation of the deviation becomes important because it is a factor in setting the flow through the cascade. The average deviation for the three builds of the annular cascade was calculated based on continuity and measured geometry and is compared to the design system used for each build. Figure 46 shows this comparison. At the cascade design point, the Build 1 results indicate an approximate 0.3-degree difference; the Build 2 results, an approximate 0.S5-degree difference, and the Build 3 results, an approximate O.SO-degree difference. Therefore, the Build 1 design system was in better agreement with the experimental deviation than the system used for Builds 2 and 3.
The measured and predicted flow parameters are shown as a function of exit Mach number in Figure 47. The flow parameter measurements used here were calculated with rig inlet flows measured with choked venturis. The predicted flow parameters were based on an analysis that was performed with averaged data using the measured throat areas and a deviation system similar to that used for the Build 1 design. Table 10 compares the predicted and measured flow for the high Mach numbers where the flow is choked. Build 1 shows the best agreement with the design system. This may be caused by the margin of error in measuring the airflow or throat area, the deviation system, and possible leakage between the rig and the sonic venturi.
56
18
16
14
w ...J C!) 2 12 <C l-X w w 10 2 <C >
8
6
4
0
Figure 45
------
O MEASURED DATA ADJ TO CONTINUITY o BUILD1}
BUILD 2
6 BUILD 3
10
3D DESIGN
STREAMLINE DESIGN
20 30 40 50 60
% SPAN
70 80 90 100
Vane Exit Angle Distribution - Higher angles near the inner diameter and lower angles near the outer diameter were measured.
o
o
O~ __________ L-________ ~~ ________ ~ __________ ~ __________ ~
07
Figure 46
08 09 1 0 1 1 12
MACH NO
Deviation vs Mach Number - The deviation prediction system used for the Build I design gave better agreement than the system used for Build 2 or Build 3.
57
124
120
116
0.. 11 2 --~108 ~
104
100
---------------~BU~l
MEASURED
o BUILD 1
o BUILD 2
6 BUILD 3
PREDICTED
9~L6----------0L7----------0L8--------~0~9--------~1~0--------~1~1--------~12
Figure 47
58
MN
Flow Parameters Mach Number - At high Mach numbers, the rig exhibits a higher flow parameter than predicted.
TABLE 10
FLOW CDMPARISON
Measured Predicted w "TIP w" TIP
Build 1 11.39 11.04 Build 2 11.95 11.32 Build 3 12.22 11.68
6.1.2.2 Pressure Distribution Discussion
Percent Difference
3.1 5.6 4.6
Low loss vane performance is attained by maintaining a desirable airfoil surface pressure distribution. Effects of adverse pressure gradients and shock losses are minimized by appropriate loading distributions. Mean section vane surface static pressures at design are compared for all three builds in Figure 48. This figure shows the airfoil static pressure, non-dimensionalized by the average inlet total pressure, plotted against percent of axial chord. Loading distributions from front to rear are similar, yet vary from build to build. Predicted distributions qualitatively match the data, which verify design procedures. Predictions accurately follow the changes from build to build. The prediction, a two-dimensional calculation at a given radius, uses a streamtube radial height ratio between the airfoil leading edge and trailing edge to model the flow over the airfoil sections. Consequently, the Build 3 canted vane configuration, which has identical sections to Build 2, can have different pressure distributions from Build 2 only because of radial forces caused by the vane cant, and other 3-dimensional flow effects. Airfoil surface pressure distributions for both the cascade and stage tests are presented in Appendices B through F at various radial sections.
6.2 Rotating Rig
6.2.1 Performance Discussion
6.2.1.1 Efficiency Comparison
An efficiency gain of 1.1 percent was predicted at the design point by increasing AN2 from 34 x 109 to 49 x 109 (in-RPM) 2. This increase in AN2 allowed the Energy Efficient Engine high-pressure turbines to run at a lower Cx/U ratio and a higher velocity ratio. The experimental gain in efficiency is shown in Figure 49 where the area averaged efficiency of Build 1 of the uncooled rig is compared to the state-of-the-art AN2 level at the Build 1 reaction level. At the design point, the efficiency gain was 1.15 percent, which agrees with the predicted value of 1.1 percent.
59
Figure 48
60
1000
0900
0800
0700
0600
0500
0400
OBUILD 1
OBUILD 2
6BUILD 3
____ BLD 1 - PREDICTED
___ BLD2-PREDICTED
_____ BLD 3 - PREDICTED
0300 L-____ ~ _____ ~ _____ ~ ________ ~ ________ ~
o 20 40 60 80 100
%x/bx
Vane Surface Statics (50 percent span) - Low loss vane performance is achieved by maintaining a desirable pressure distribution.
~T/ = 1 15%
7JAR 86
Fl.gure 49
84
82
80L-____ ~ ______ ~ ______ ~ ______ ~ ______ _L ______ _L ______ ~------~
20 25
PRESSURE RATIO
AN2 Increase - A net area-averaged efficiency gain of 1.15 percent was achieved by increasing the AN2 parameter.
A comparison of low reaction and high reaction rig performance is shown in Figure 50. The high reaction turbine demonstrates a 0.8-percent higher efficiency than the low reaction turbine at the design point. This exceeds the predicted efficiency gain of 0.5 percent. This benefit for high reaction decreased as the turbine was run off-design (see Figure 50). The Build 1 test data agree with predicted values at lower pressure ratios, but at the higher pressure ratio points efficiency is overpredicted. For Build 2, the measured efficiency exceeded the prediction at the design point, but at the higher pressure ratio points, efficiency is overpredicted. The lower corrected speed (280) data are overpredicted, and the high corrected speed (375) data are underpredicted. The design point data are summarized in Table 11 and in Figure 50.
Build
1
2
'mBLE 11
DESIGN POINT PERFORMANCE (Corrected to 0.0145 in. tip clearance)
Reaction (percent) Predicted Test
36 33
43 37
Mass Averaged Efficiency (percent) Predicted Test
90.3 90.3
90.8 91.1
61
92
90
88
~~~375 I~ ••
% /w ~ 0 350 BLD BLD ........
_'_2--1t-N_1....;VTT_T_T--+ ____ 2__ .. .... ........ ..... ?80 • 0
86 o. 350 o. 280 ~ • 375
84
82
0 350 0386 II 6. II 350 0770 0733 JI
~~ 350 , '89 '254 iJ.7 DESIGN PRESSURE
---- BLD' PREDICTED I RATIO
II BLD 2 PREDICTED II
II II
80L-___ L_ ___ L_ ___ ~ ___ ~L_ __ ~ ___ ~---~~--~
20 25 30 35 40 45
Figure 50
PRESSURE RATIO
Mass-Averaged Efficiency vs Pressure Ratio - The high reaction level rotating rig perfooned better than the low reaction rig at the design pressure ratio.
Efficiency of the uncooled rigs was calculated using inlet and exit measurements of pressure, temperature, and air angle. Fixed temperature and pressure rakes were used to measure inlet conditions. Temperature and pressure rakes that traversed through the same IS-degree arc (1 vane gap) were used to measure ~onditions at the exit plane. The efficiency values over the IS-degree arc were circumferentially area averaged and radially mass averaged with the results from the radial air angle traverse.
The measured efficiency data were adjusted for variations in tip clearance caused by speed changes and temperature changes of the disk due to front disk leakage flows. The sensitivity of the change in efficiency to tip clearance was arrived at by correlation of running clearances from three sources. These included readings made by the laser optical probes located at two circumferential locations, measurement of mechanical rub buttons installed at three circumferential locations, and from analytical calculations based on disk, outer air seal, and case metal temperatures. Once the tip clearance was established, the change in local efficiency at the outer diameter was determined as a function of clearance (Figure 51). To adjust the stage
62
efficiency to the design clearance, these data were applied to the spanwise efficiency. study of the spanwise efficiency profiles showed that the loss caused by tip clearance m~grated to 65 percent of the span, resulting in a spanwise average adjustment of 0.079 percent in efficiency for 0.0025 em (0.001 in.) in tip clearance.
Figure 51
4 KIELHEAD CIRCUMFERENTIAL
~ LOCATION >-U 3 0 -850
2 w 0 U u.
-1750
-2650
LEAST SQUARES DATA FIT
0 u. 2 ~ 3550 w
<l ...J
<31 0 ...J
O~ __ ...J-____ ~ __ ~ __ ~ __ ~ ____ ~ __ ~ __ ~
o 0002 0004 0006 0008 0010 0012 0014 0016
(em)
o 0001 o 002 0 003 0 004 0 005 0 006 0 007
Ll CLEARANCE, INCHES
Outer Diameter Kielhead Efficiency Change - study of the spanwise efficiency profiles showed that the loss caused by tip clearance migrated to 65 percent of the span, resulting in a spanwise average adjustment of 0.079 percent in efficiency for 0.0025 cm (0.001 in.) in tip clearance.
Reaction for the rotating rigs was defined as a ratio of the static pressure drop across the rotor to the static pressure drop across the stage. The results of the tests on the two rotating rigs are shown in Figure 52, where reaction is plotted against pressure ratio. The cooling flow points are not presented because the inner diameter cavity static pressure taps were affected by the disk leakage flow and did not read the correct flowpath pressure. The measured reaction was lower than predicted as shown in Table 11. This was caused by three factors: (1) fabrication tolerances on the airfoil throat areas, (2) the differences between the measured and predicted deviations for the vane and blade, and (3) the predicted versus measured losses for the vane and blade.
63
:2 o
044
042
040
038
i= 036 (J
<! w a:
034
032
030
• • • • 0
§
• • • • 0
0 0
0
BLD
1 2 N/VTI
o. 350 o. 280
• 375
028~ ______ ~ ____ ~~ ____ ~ ______ ~ ______ ~ ______ ~ ______ ~ ____ ~
20 25 30 40 45 50 55 60
PRESSURE RATIO
Figure 52 Reaction vs Pressure Ratio - The measured reaction for both builds was lower than design values.
6.2.1.1.1 Data Presentation
During the design efforts, attempts were made to maintain high efficiency in core regions and to minimize endwall losses. In practice, endwall flow regions and wake regions generally have lower efficiency than core flow regions, as shown by the contour plots at design in Figure 53 and Figure 54. This plot shows the efficiency contour lines over one vane gap for Builds 1 and 2. The data were then circumferentially area averaged as shown in Figure 55. The shapes of the efficiency curves for the low and high reaction Builds are similar, with the high reaction turbine showing greater midspan efficiency.
Blade exit absolute air angle, which was used to mass average the efficiency data, is shown in Figure 56. The level of the measured data was adjusted to match continuity. For Build 1, original design point data (350) and repeat design point data (344) are shown. Build 2 angles are lower than Build 1 angles, as predicted by the streamline design. Additional stage performance data for both the lower reaction Build 1 and higher reaction Build 2 are presented in Appendices E and F.
64
r~I"'l:l- I' I I
I +- H- 4" I' - H-"t-r 1 , -I- t - t I ,
~/!!> , r 1 ~t:b I- i- I i - -j
" I I I -1..-
1 +1- ' __ L - -- ~W - R:IT I - - - -I , I
:r--r I + -~- L 1 ~I i- I ' 1"'- t:::;",. - - I "'il! , ~I-:: --l-H- -f 1- -~- -f-l- , , , , :.- 1- I-y- 4-, , , I
I -+ w.- f+ -~ ~ _L 1-1- 1->1- -G ,,- -- -l - - - -I , ,
~ -f- j;;.!-=,v i H-,
f--+- V:-- ~ _1_ -'- - 1" , I
.;" I I-t-- H--R=- 1--' - I- t-l-. +-1- -I- -- r-.. 1 1-1" , ' ,
?-~ "+ ir ~ , -1+ 1-'
, .;. -~- -'-- - - -t - T -+-
J
t.. - - -- +, - - 81 --i-r+ -+- -I-f --I- -1-1 , I
-~ ~~ H- --+ I L ,
I-L H--;- 1- - - - T I
-~ r+- +-1- -II I _L ri-- , ;- - -,
I -y ~ I - T-.~ -
, I 1i' I;!-Id'" ~ ,
-1- -t-1kt --'- -+- T -I-- I I
H- '-t-V!'-IJ ~-~+~ I H-::<-1--- -; -r -1--
I ,<.."
l -t:t -I- 1- ~+ ,
f-r t-!- -i I - ~-:! .J\ , T-
~- ~ , , I
J--f:- - - I I--i- -f-rl- 1-- I
f-r,-I- L -r f-J: R KI-- u- -~ I ~ I
N:: , bi: ...., l+...: -,
~, , t-;..... , --+ -r-- , - I -- - - I ,- -r-, , Ih'r
:~h ! T' 11,,- 1-Ff-Fl~ I
~' ~';-~ I
61u"'Ll, I 0 -I ,;, h I, , , ;;;. I I ~
Figure 53 Efficiency Contour
, r _'_ I
~~ }-- 1
-- ~- ~1"- J , t--- -i- -H- I-,
, + ---Fl- -I I I ,
Rt -0-~\L: I ,
I'::" -T - , I '~ , _ .J
iF=T I r- --
I_ ---8- 0-
1-0 1\-- .L I
_J_ H-r-! - , -t" T-I
~I -f- 11:-- , I 1--~ v,- I -- - , --'-e I
+" --+-,
- - -,-, ,
4:. - .. - - !~ -l-I ..:;. -l -- I r-
:-
:::::::: f--l--
----,
i== § I
t"7' I ,
1 rF*:::::ti;~t;~ -n
Curve Label
6 7 8 9
10 11 12 13 14 15 16 17 18
0.81000 0.82000 0.83000 0.84000 0.85000 0.86000 0.87000 0.88000 0.89000 0.90000 0.91000 0.92000 0.93000
BUlld 1 N/sq. rt. TT = 351.4 PR ma = 4.088
65
'I ~ W- I " -- J i , . ! -'p.:: , II r , ~
..j.
T~ T: V),j Il' - , ;--:;::; I I I.,
~I-V: - --K ~ [7y f1~ 1-,
r-L-i u-l-t- I t::- V; -I f\ . - I , t- l,-, -J ~ VI 1-,;" ~ - -r ,... I , ,
..! - ~+~ -t- -:-r-h~ H- I\T !I 7~ I\f-/1 - pM- I f-_L 1- ~I : ,j" Iii j:' ~
.1 1 I I-I-L - i - -~ J_ Y J: c;r vt-"+ ,
I , k-L Ii.. + --;: l/V !j -; ~ --
I 1\-
" f"+ -JiQ i' -+. f-r 1- -- -I~ ,-- -\ '7~- _L I-+-p+- !l ± .1;; hi V I
~IJ :-TIS i--';'" k_ + I;'~ , , r+-VV k'1_ ' H-t - -+-i-u~ I I~ - - /~- ~y --1- 1--_' I -t-t-j --
" ~l'l ! - l--V- - - -~ _L __ - - - -- t- -I ,"r , , I
~rt Vr ' , . I- -- - - - - -;- ,- - -- --I ,
" ,
'1P~~' I i la-v t:f _. - - -I'r ,) , ~? T 1 t:r: 1 , I
, c.c: ~ c -r: I ,e I
i~f$. 8- _-C ~ ~ :x: -~ ;::t 1111 , -,....
"f-f- ' __ R-:- f-+::: ~1 i· -; I- i-- -t-1'1 ! t=P I -1
~~I ~l- ±: H I fiT" [-i- '::", ,--:,1 tti
Figure 54 Efficiency Contour
66
~ r '}: f-l..
M-: I
-i- i ~- 1 , t-
~ -1 ---1 - ~
-F= :::r , :..:.:::: ,
1+ +-.:::
1 1-1-
1-+' H-Ii -I-~+ -1-~I-'
,
~ ,
1-....-....-r ~ ~/
:.-r: V Il- r
, I-t r,
- ::L I t-l I
, (2 I ~t-... ----
iT - - -I--- I I , ,
IH Ii --~ ~ r-- -~ K --, - -1--~R i-,
f.:-..... 1 " -v
r- I.=-___ L - -
1 - r-. 1
f"K , r -1-~ 1--1--- - ~-
l ........ H-I i
+ ~ k - -~ I
~- +--I-- - -1-~ I T -~
~ fx.. ,
-1-- -~ :::--: ~ ,
"-): ~ ~ - t
, ~ 1--1 ~
I ---'--K- '-]
---. I'N ~II f'I
Curve Label
5 6 7 8 9
10 11 12 13 14 15 16 17 18 19 20
0.80000 0.81000 0.82000 0.83000 0.84000 0.85000 0.86000 0.87000 0.88000 0.89000 0.90000 0.91000 0.92000 0.93000 0.94000 0.95000
BUlld 2 N/sq. rt. TT = 350.8 PRma = 4. 149
94
92
90
I=:" 88
86
84 o o
o o
o o
o o
o
o
o
o o o
o o o o
o BUILD 1
o BUILD 2
o o
82L-____ ~ ____ _L ____ ~ ______ L_ ____ ~ ____ _L ____ ~ ______ L_ ____ ~ ____ ~
o
Figure 55
80
70
w ...J 60 <!l 2 ~ (f)
w I- w X a: 50 w <.:J w w C C ~ ...J 40 al
30
20 0
Figure 56
10 20 30 40 50 60 70 80 90 100
% SPAN
Efficiency vs Percent Span - The shapes of the efficiency curves for the low and high reaction builds are similar, with the high reaction turbine showing greater midspan efficiency.
10 20 30 40 50
o o
~ H __ -8 __ ..... -------
o BUILD 1 (344) } MEASURED DATA o BUILD 1 (350)
f::l BUILD 2 (350)
ADJ TO CONTINUITY
___ BUILD 1 - STREAMLINE
___ BUILD 2- STREAMLINE
60 70 80 90 100
% SPAN
Blade Exit Angle - The predicted angles have the trend of l~ier inner diameter angles and higher outer diameter angles shown by the data.
67
6.2.2 Blade Analysis Discussion
6.2.2.1 Blade Pressure Loss
The high reaction Build 2 rig demonstrated lower losses at design pressure ratio and design speed (see Figure 57). The blade total loss was calculated with a meanline analysis using the mass average vane loss and efficiency (the calculation did not consider losses caused by blade tip clearance as being separate from the foil). Off design, Build 1 and Build 2 losses were generally comparable. Large losses were associated with low speed (positive incidence) , but there were no increased losses for the higher speed (negative incidence) Build 2 design. Low speed losses were underpredicted, and high speed losses were overpredicted. Build 1 predicted loss values matched the test data at design, but were too low for off-design conditions. Generally, the test data for Build 2 were lower than the predicted values, except at the high-pressure ratio.
The meanline analysis used for the blade losses was also used to calculate the actual Mach triangles for Build 1 and Build 2 of the rotating rig. The Mach triangles presented in Figure 58 are compared with the design Mach triangles (see Figure 4 and Figure 5) in Table 12. The Build 1 and Build 2 vane Mach numbers are higher than the design intent, and Build 1 and Build 2 blade Mach numbers are lower than the design intent. The reason for this difference is that the reaction level of the rigs was lower than the design reaction level.
TABLE 12
CDMPARISCN OF DESIGN AND EXPERIMENTAL MACH NUMBERS
Design Experimental Design Experimental Build 1 Build 1 Build 2 Build 2
Vane Mn 1. 017 1.061 0.932 0.999
Blade Mn 1.150 1.127 1. 232 1.193
6.2.2.2 Deviation
The blade deviation for Build 1 and Build 2 1S shown in Figure 59 for the design corrected speed of 350. The experimental deviation (air angle at the exit plane minus the gage plane air angle) was calculated from continuity and the exit plane measured conditions. The predicted deviation was calculated using the design system updated for the measured areas and test conditions. The prediction follows the trend of the data~ however, the level is low.
6.2.2.3 Pressure Distribution
Due to instrumentation system malfunctions, no valid blade surface pressure distributions were measured for Build 1.
68
• 020
0
0175
015
Q. 0125 --Q.
<l
010
0075
BLD
1 2
o. o. • 0 6. ~ ..
.0
BUILD 2 (350)
BUILD 1 (350)
% WC/W
BLD
N/VTT 2
350
280
375
350
350
350
0386
0770 0733
1 183 1 254
~-:. __ } PREDICTED
005 L-L-________ ~ __________ ~ __________ ~ ________ ~ __________ ~
35
Figure 57
40 45 50 55 60
PRESSURE RATIO
Mass-Averaged Blade Total Loss vs Pressure Ratio - The high reaction Build 2 rig demonstrated lower losses at design pressure ratio and design speed.
Build 2 blade pressure distributions are shown in Figure 60 for all spans at design. The blade relative inlet total pressure was approximated by using the measured 30-percent axial chord, pressure side static pressure in calculating the PS/pT ratio. Good performance was maintained because the adverse pressure gradients at all spans occured well back on the foil. Also, the pressure increases caused by shock waves were relatively small. The design prediction qualitatively matches 50-percent span data, but is not a good match at other spans.
69
BUILD 1
~FLOW BUILD 2
l FLOW
MR'03~ MR = 0 29
Figure 58
70
360 106 400 108
J.l.
~'0424 ~-047 192 608 186 539
Mach Triangles - Experimental Design Point Mach Triangles for Build 1 and Build 2.
7
'"
6
(I.) 5 w w a: C,!l W C 4
2 0 i= « 3 :; w C
2
0 08
Figure 59
o o
0
0
0 o BLD 1 DATA
o BLD 2 DATA
0 _ BLD 1 PREDICTION
_ __ BLD 2 PREDICTION
1 3 14 15 16
Total Blade Deviation (Air angle at the exit plane minus the gage plane air angle) -
71
1000 - ~
~\ 0900 ~
~\ \\
0800
~\ , \ " ~\
A .
0700 \\ \\ I- \' c.. \t .....
\\ en c..
0600 \' 0\ \\ \
0500 ~\ \ \' 6 \ ,\0
~ \\ 6 0400
o 12% SPAN
~~ r- '" o 50% SPAN
~ 88% SPAN \ ~--.~ 0300 12% S-PRED ~/61/ e
___ 50%S-PRED \01
__ 88% S-PRED 'J 0200
0 20 40 60 80 100
%x/bx
Figure 60 Blade Surface Statics - All distributions successfully delay the start of adverse pressure gradients until well back on the foil.
72
6.2.2.4 Disk Cooling Flow Penalty
The presence of leakage and cooling air in the engine environment will create a performance penalty relative to the uncooled rig environment. In the uncooled rig, leakage flowed outward along the front of the blade disk, where mixing with gas path flow caused an efficiency reduction. The performance penalty caused by blade disk leakage flow is summarized in Figure 61. The figure, showing span mass averaged efficiency corrected to design clearance, shows the change in efficiency caused by the mixing of the cooling flow. The data agree reasonably with predicted values.
6.3 Summary
The results of the Energy Efficient Engine high-pressure turbine uncooled rig program have established the uncooled aerodynamic efficiency of the highpressure turbine at 91.1 percent and have verified the feasibility of the Energy Efficient Engine high-pressure turbine aerodynamic design concepts.
91
90
1] AA(%)
89
88
87 o
Figure 61
0 2
0
0
o BUILD 1
o BUILD 2
__ PREDICTED
02 04 06 08 10 12 14 1 6
% WCOOL
WMAIN
Effect of Leakage Flow on Efficiency - The change in efficiency because of mixing compares reasonably to predicted values.
The measured benefit of higher AN2 is shown in Figure 62. This figure compares the area averaged efficiency of the current state-of-the-art single stage turbine with the area averaged Build 1 results and shows an improvement of 1.15 percent at the Energy Efficient Engine design point.
73
92
90
88
71AR 86
84
82
80 20
Figure 62
o ~
BUILD 1 PREDICTION
AREA - AVERAGED 077 = 1 15%
STATE OF THE ART
PRESSURE RATIO
Area-Averaged Efficiency vs Pressure Ratio (Effect of AN2 Increase) - An increase in AN2 resulted in an increase in turbine efficiency.
The Build 2 rotating rig demonstrated a mass averaged efficiency of 91.1 percent, 0.8 percent higher than the lower reaction Build 1 rig. Build 1 was tested with a reaction level of 33 percent, and Build 2 was tested with a reaction level of 37 percent. Figure 63 shows the comparison of efficiency vs pressure ratio for these two builds.
Results also showed that the 13-degree canted vane configuration had the lowest mass averaged total loss of the three airfoils tested. The massaveraged probe measurements indicated an overall pressure loss of 0.0245 as compared to 0.0369 for the radial Build 2 vane at the design point.
74
811 = 0 8% 92
90
* 88 I >-U 2: o BUILD 1 N/VTI = 350 w U
86 o BUILD 2 N/VTI = 350 u.. u.. w
84
82
80L-______ L-____ ~~ ____ _J ______ ~ ______ _L ______ ~ ______ ~ ____ __J
20
Figure 63
25 30 35 40 45 50 55 60
PRESSURE RATIO
Mass-Averaged Efficiency vs Pressure Ratio (Effect of Reaction Level Increase) - An increase in reaction level resulted in an increase in turbine efficiency.
75
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7.0 CONCLUSIONS
o The second build of the Energy Efficient Engine uncoo1ed rig has verified that increased AN2 and higher turbine reaction level lead to increased efficiency. The demonstrated uncoo1ed efficiency was 91.1 percent.
o The Build 1 vane demonstrated the best compromise between low loss and a proven air angle distribution.
o The 13-degree canted vane configuration had the lowest performance loss of all the vanes tested.
o The Build 2 high reaction blade demonstrated lower losses than the Build 1 blade at the design point ••
77
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APPENDIX A - AIRFOIL COORDINATES
F1gure T1tle
A-I BU1ld Vane Root Sect10n
A-2 BU1ld Vane Mean Sect10n
A-3 BU1ld Vane T1P Sect10n
A-4 BU1ld Blade Root Sect10n
A-5 Bu 11d Blade 1/4 Root Section
A-6 BU1ld Blade Mean Sect10n
A-7 BU1ld Blade 1/4 T1P Sect10n
A-8 BU1ld Blade T1P Sect lon
A-9 BU1ld 2 Vane Root Sect lOn
A-1O Bu 11d 2 Vane Mean Sect10n
A-ll BU1ld 2 Vane T1 P Sect lOn
A-12 BU1ld 2 Blade Root Sect10n
A-13 Bu 11 d 2 Blade 1/4 Root Sect10n
A-14 BU1ld 2 Blade Mean Sect10n
A-15 BU1ld 2 Blade 1/4 T1P Sect10n
A-16 BU1ld 2 Blade T1P Sect10n
79
This Page Intentionally Left Blank
A-l Build 1 Vane Root Section
SUCTION SIDE PRESSURE SIDE PERCENT X/bx X Y TOP Y BOT
o.u 0.00136 2.766lt1 2.582SU
0.u10 O.Ol"ulS 2.7bl'1o 2.~b219
0.020 'O.026t1U 2.7'1679 2.~76S1
o. (UOo U.OJ'lI!ll ".blu'I1 2.~0778
O.UltU 0.USl24 2.tiZltJS 2. 5561sl
O.U!>O 0.06490 2.~.H 11 2.544l0 O.ObO 0.0716tt 2.1S"'I21t 2.~3030
0.U70 0.0'l1l1t0 ".bou71 2.51536 0.1180 O.10.HZ 2.bU)1 2."9'i~2
0.0.,,0 O.US&4 ".bblu1 2.4b2'11
0.100 O.lltl5b 2.8'114) 2.46S63
0.125 0.160Jb 2.'Ill'lS 2 ... 2000
0.IS0 0.19116 2.'I~uIj6 2.~114~
0.175 0.22,j'l6 2.'I45i4 2.31051 O.2UI)- 0.25510 2.'I5b13 2.267b2 0.225 O.i&I)S ,.'16354 2.l1199
0.2SO- 0.3193) 2.9t~146 2.1507'1 0.215 0 • .;)115 l.'I61t1' 2.09919
0.300 0.3bl'l) 2.'Ib'tbU 2.040.;)::' O.~25 O.4141~ 2.9~/b2 1.'itlUL6 0.3)0 0.44655 2.'14072 1.'11'100
0.315 0.47&35 2. 'l/3J.10 1.&5b18
O~4"\J O.Slul) 2.91lZ9 1.1'134'1
0 ... 2S 0.541'1) 2.bbbll 1.12'111
O."SO O.~1,j14 ".tI)U6'1 1.bbJHY 0.lt15 u.60554 2.U2.H9 1.59164 o.soo 0.b3131t 2.lb135 1.53045
U. 52 5 0.6691 .. ".13135 1.46227 0.55U CI.1UO'l" 2.0715'1 1 • .:l'l.:llb 0.5"/5 O.13i74 i. )'1'111 1.32304 0.000 o. ·'blt54 2.)(JU85 1.25195 0.015 0.7"bj4 ". ,j'i711 1. 17'1UO 0.b50 0.82bl .. 2.21112 1.10b60 0.67) O.b5'1'13 2.1.HJ5 1.Cl3a5 U.700- o .U'I17,j 1.'l/'ib50 O. 'J56 73 0.725 0.92~5j l.b5l1llt O.Ul'iU'I 0.150 O.'I5)~;S 1.b'l'l54 0.110169 0.175 0.9ulll 1.) .. 4bJ 0.711'J1
O.HOO 1.011l.,3 I.Jbb5't 0.b4042 O.b2S 1.05UH 1 • .l£ .. uo 0.~!>b9l
0.U50 1.0tl2),j 1.0~'1'i~ 0.47101 O.tl7!! 1.1l .. ~~ 0.U'Il1b 0 • .)bl31 0.900 1.14b12 O.120~3 0.28963 0.'110 1.15b&4 0.b5l11 0.25146 o. '1~CJ 1.171~b u.!>tll17 0.21218
O • .,.~O 1.161t.l6 O.!>J.(.b'l 0.17171 U.'140 1.1'1700 O.ltJ'Ibb 0.12'iul O.'1)U 1.lCl'l12 0.,jbbU6 O.UtloOl O.'1bO 1.1..2i44 0.Z'i!>9l 0.03'1b5 0.'170 1.l3!»16 0.223 J.5o -0.01069 0.'16U 1.247t18 U. H'I72 -O.CJ5'l/16 0.'1'110 1.20000 0.01)0. -0.10121 1.UOO 1.",7332 0.00101 -0.15040
81
A-2 BUlld 1 Vane Mean Sectlon
tilT RALJIUS & 11.09400
SUCTION SIDE PRESSURE SIDE PERCENT X/bx X Y TOP Y BOT
0.1.1 0.00110'1 2.1i/S313 2.70'l~S
0.010 U.014~1 l.U'I71b 2.10.22, ~
0.1.121.1 O.UlU'lj 2.'1U'I1 2.09321i 0.0301 U.O..i'lb4 2.'12)00 2.Ob2'l1 0.0 .. 0 0.0~2..ib 2.'Hd8l 2.07132 O.O~u O.Ob)Od 2.'I!)1!)1 2.b51ioH
:' 0.000 O. u171'1 2.'Io.)/j,j 2.04~O'l
0.U10 0.0'l0~1 2.'0)02 2.b.)0b4 0.080 O.lO.:ll.j 2.91:10'13 2.01543 o.v'lO 0.1l!>'I" 2. '1'1 17 b 2. !)'1950 0.100 0.1"bob 3.U(;IJU'I 2.!)1:I2'12 0.125 0.100'" 3.0.)110 2.~u/j94
0.150 0.19L2) j.0'~l9 2.4'111't 0.175 0.22 .. 0 .. 3.00'1)'1 2.44175 0.20U 0.2!)5b.:l .:l.0/s.j!>1 2.38931 v .l2!) o .2tOt>2 3.0'1 .. J.l 2 • .).)40,j 0.2!)0 0.31'141 3.1u10'l "./.718'1 0.21) 0 • .)!)121 3.11.14.:14 2.l192) 0.300 0.38300 3.10.)10 2.15880 O.3lS 0.4147'1 3.0'1"'13 2.0'1070 0 • .)51.1 0."40~b 3.Uu'l1'1 l.O.:l30 .. 0.,j75 O.471U1 l.U'!)"'I 1.'10110 0.4UO 0.)lu11 J"u51l1 1.'tOU'l9 0 ... .2) 0.541'10 3.U3lb'l 1."3272 0.45(.1 0.57375 3.00':0" 1.7b303 (/ ... 75 0.(05)4 2.90)75 1.o'Hao 0.500 0.oj7j3 2.9L14.) 1.b19L8 U.!Jl) 0.bb'l13 2.l:IblS)0 1. ~452.j 0.5!)O 0.10092 l.8u)''1 1.40915 0.;]) 0.1.).:11 2.1.Hll 1.3'1210 O.bUO 0.7b450 2.b4173 1.31427 0.025 0.196l,9 2.5.) .. l,8 1.L3 .. 18 0.b5U O.l'Jldu'l 2."10'11 1.15250 u.(1) 0.85'1Ub l.LI .. lil. 1.00'107 0.100 0.8'1101 2. 121S.:l2 0. 'I/s.)1i1 O.llS 0.'Il.j40 1.91LHb 0.8'166'1 0.75(.1 0.'155l)- 1.bU'Ib4 0.&1.1741 (/.715 0.9810) 1.oj'l .. b 0.11!>9l O.bOO 1.Q1b84 1 ... t>.)0'l 0.b211'J5 v.&l5 1.0500,) 1.2bO'l.) O.!Jl'tU8 O.b!>O 1.lIbi ... 2 1.0't.)!)1 0 ... 2460 O.b1S 1.114,l1 0.'IOI0b 0.3l031 u. '1U(J' 1.1"001 O.lu.)'1J. O.ll113 v.'11v 1.15812 O.6Z.)tsl 0.lb515 O.'I.lO 1.111 .. 4 0.~4.:108 0.11'122 U. '130 1.1b"10 0 ... 01!>& o. (,11;;8 1.1.9 .. 0 1.19b81 0.,j1,,"1 0.021 'to o • .,~o 1.20'l~'1 O.,l'tb!>b -0.(/2'133 U.'160 1.li,l,j1 O.L1305 -O.OIi2'1" 0 • .,,(/ 1.l3!>U2 O.lZ81'J'i -0.1l951 O.'1dO 1.2417" 0.0 .... 10 -0.20011 0.'1'.10 1.lb04b -0.U413~ -0.26101 1.000 1.27311 -0.121 .. 1 -o • ..;448b
82
PERCENT X/bx 0.0 0.010 U.OlU (I.U;'V U.040 0.050 O.vbU 0.1170 U.080 11.1190 0.100 0.125 0.150 0.175 O.lOO 0.ll5 u.l~O
O.ll' u • .jOO 0.325 0.":'0 (J.37S 0 ... 0<1 0.4l5 0.4~O
0 ... 75 0.;00 0.,25 u.,50 O.~15 U.bOO 0.b25 0.b50 u.b7; 0.100 0.U.5 0.750 u.n; O.bOO U.fll5 o.u!>o lI.ln; 0.900 0.'110 0.'120 (J.'1JU U.'140 0."'50 0.'160 0.970 0.'180 0.'190 1.000
A-3 Build 1 Vane Tip Sectlon
hOT RAOIU~ • 12.34200
x 0.00156 0.01 .. 28 0.Olb"'9 (;.03'110 0.0'''4l O.065J.3 0.077115 0.0'10,6 0.10J£7 0.11)99 0.12b70 O.lbO .. y 0.19l27 0.22406 0.l!»;U4 0.,,&lb3 0.31'1 .. 1 0 • .,5120 0.3&,,'10 0.41471 0.446!»5 0.41&34 0.51U1J 0.541'11 O.!»7.HO 0.6054& 0.b~U.7 O.06'i1J, 0.70vu .. o .1.,lb2 0.70 .... 1 0.7'101'1 0.tlZ7'1U 0.8).,-/0 0.8Yl!>5 0.'I2J.U 0.9,512 O.'IUb'lO 1.01db9 1.05("47 1.0Ul26 1.114U4 1.14)d3 1.1,u54 1.1112b 1.18.)97 1.1Y6blt 1. ,,0'140 1.22211 l.l34U;' 1.24754 1."bO.£o 1.27l'l1
SUCTION SIDE Y TOP
l.Y4J,l 2.951147 l.'I7ib!» 2.Ybbb1 2.'1'1'1'1';) 3.01L7IJ 3.0L4YJ J.0.,666 3.047'H J.0!>b66 ).OuO'l4 3.0'1"03 3.113)1 3.1,,166 ".14111 3.1)98'1 3.11uOO 3.17743 3.1ltlll 3.1U .. uu l.IU2'1B 3.11b'll 3.171b5 3.16l1'1" J.14b41i ~.11192 ';;.111470 3.U7(;27 J.O .. l~1J l.'1YU"''1 2.'14b40 2.blY14 l.71J'H8 2.06.,Ob 2.,lIb5'1 2 • .,"b61 2.1.j't0'l 1.'1261'1 1.70/,,6 1 ... 71J'7o 1.24lU1 o. 'I"'b(J1 0.7 .. 148 0.04!»51S 0.5 .. 215 0.4J'IOs 0.,,;;44'1 O.""'Ilb 0.12298 ".OlbO~
-<I.091b" -O.~"'(')Ol -o.~0916
PRESSURE SIDE Y BOT
2.772Jl 2.1642) 2.1'''81 2.74419 2.1.,2)0 2.719ti!) 2.10b.H 2.69194 2.b7682 2.bb0911 2.b444ti 2.b005.j 2.!»;313 2.s0l62 2.449J4 2.~93)0
2.33S..!4 2.l7474 2.21212 2.14146 2.uaOb2 2.01211 I.Y'tltl& 1.tl6CJ63 1.7'1';)''1 1. n'l7Z 1.b4207 1.!»6~56 1.481.!4 1.';;9799 1.31111) l.l25bb 1.13641 I.CJ44Y5 0.,}5119 O.IS'4'11 0.7,59b 0.b)404 0.!>488b O ... 3 'I '1b 0.~267b 0.101i42 0.UU.j18 0.03176
-0.OlI75 -0.07b93 -O.IJIt11 -0.1'1~b5 -O • .l)b01 -O.~2220 -0.39330 -0.-.1175 -0.;6264
83
PERCENT Xjbx
84
"'."1 1'."11' ". ""2"1 ... ' ." ~ ( • "4 .... ".05" '."E,'" ,"I .... 7(\
t'. 18 ~
". 09~ ,.. • ! '"I '" n.125 ".1St"! 1""'. 1" c=
~.21"\" ~ • Z",r ,.. • 2· ~
".2'('" ''',.3''''('' ".n.s \.35 " ".375 r _ 4' "'; ........ .,1:, f). /,-'::: ....
,...~...,..:.
f"'\. I ~. ~ . "' -". r; ...
"1.' 7~ "'I • .t"'" "'. ~ ..... r:: r~.lc",
,. • f -. r: 1"\.-,0-.."
('. 7'" It
'" ... .::1""\
('\. ,. "", r,. u' t)
.... "'1 " <~~
,... • t ... "\
r,.O/."
r.. I , "
,. • COIl, ....
"\.97'" ".980 0.<"19"1 1 ..... '1 ...
A-4
x '.0 ".()l'~?
1"\.'" "'"17 "t
".""'1~tl
", ....... -, • '1 i"'."IC:;~~
- .1"\-'1 .,., n."\n-"'I~
"."Q/. }! '"\. J -'f':~. " • 1 ' ,. .... r· n.!4 C''''-·
l).l7t"rr,
"'\1"\-7""
..... " ft .... ,
" • "'1.,(, ... ? I) • -:. ' f, 1 () r".-·"U·'7 "'\ • ' 1 ' ... ' r,
'" .1.:' f ., '")
r ."."7 .,... "" 1'1.'" "'" ... -' ..... ,.~1/·1 ... "'.rI-1~?
r ;'''' "
7
rJ. ',"". ? r'.71""1-r. ').7 't 1 ('17 t""."'7'r"S - .~ .... ~~.,
-.8~"Ir",
'"'I .. ' 1,(, r"1
r • f't(J') .... -:
".(""1 .... "'.., 1"'\ .0/4 - 1',,,"\
,.. • ,,-,.;;. ')7
1 • f',.., co I r; 1 .r . ...,'" f,") '.r·O~ln
1 • " .... ""\ 1 7 1 .r""""I. ...... ., I' ,
.... ' " , .... 1 • 1"" , I r,
1 • 1 ., 'I t" "! 1.'"1-''' 1.1h ...... {, '.!7 r l-1.l Q 7-('>
BUlld Blade Root Sectlon
SUCTION SIDE Y TOP
r.7 w 161 -."77~<;5
[."("1'-1)')
".' -'.71) 1'\." ( ., J 1
• .,. Q "'1. '" r. '1''''''' (,.c-'.96 :'.(')"1,' ... "."' .... I"",qJ •• '" - 1 34 ! • ('" t.!) 1.1,
1. ," «'3 "
'.1(,-," 1.1:-"'1'>7 1 • ?' I. t.,-:'
:.--:h"1'?, 1 • ~, .: ;, () ' ..... j ..... n7 , • ., r 1 (')r1
]. :9-1") I&G"l"~
1 • -: '/ ,1 <) 1.-"141
! ." ~"t> i')4 1.::'(,1<)4 1.17' ~o 1.1/."'",) J .: \ 17 'I." r '" l? ( • ("' ... "J r4 C'. ') r "4<> ,... r., 16-' ... \. "'7 "''10 ,.. .f"7·.~o ". t' 5" .. I.Q
;:'1 ...... "")7 ..
:-. ;'J~/-,
"'.-'(,l~ti
~.""?"'71
,.. • .., r '77 ,. • ., .... ~. 4 C'
( • -; [II. ,)r, ".1'",04 .... 1 ,:. (10,.., ....... 01.49
PRESSURE SIDE Y BOT
O.4 P " ... f\r-,
"."1<;(10 (1. ';4 ViQ
". 5T~".O C. (-.J';;"3 (\. ()? 't '::. 0.6',,.,(1) f't./)h3!..O I). t,0100 ("'.f,"?)!) ':'. on"".;. n.7~"C:'f 1).7l\..,tjr
".7",,:;oQ
1).77.,.")" f.7n'"'9 -.7,,\r" ".-"S:1.Gl O. 777-;~ ().77?5~
"'. 7fJ - !,7 '). 7(A,~Q ..... ..,.4I-fl t". '73/ .. 6~ O.7?11)? fl. 71"'<;01 'l.t-t"'q'")o
'"\.1"7 11') '"' • I," 1 r 9 ".A31"l4Q r..6roP(-' fl. C;"~f.'3 "'~.~~)7C"'1Q
,.. • .- '0;'" I.?
I"'.~""'ll?
(\.4 7 nr,6 0 ... ""16<)2 ".4f'1r:.t
". ":!n°'7~ ~ • ., ",1 ')
"'.""7,"''' C.''"'14"3 0.1 7071 1'\.1''';'11 ".1,1"2 "'.lr,(,", "."-r o t.7 fl. ()I,n ;'j 1).'l195~
-".'"'l"'''J - ..... ('.';7 / 3
-0.10'1"" -".1F'9f'fl
A-5 Build 1 Blade 1/4 Root Sectlon
HOT RADIUS ~ 10.63400
SUCTION SIDE PRESSURE SIDE PERCENT X/bx X y TOP Y BOT
(I. f) 0.04300 0.9497 5 0.65504
('."10 C.('l'5401 O.9C?ab 0.(,1439
C. .,.)20 O.(J6~02 1.01740 0.13598
( •• 030 0.07"(13 I.G393? 0.77636
0.)'.0 o .I)n04 1. (63e6 O.!?07CJ
C.J~O O.O<Jr.O~ 1.t/'lc46 0.03191
0.060 0.10900 1.1 11137 O.P5760
(.(,7r. 0.12007 1.12680 G.e7ne {'.()~J 0.13108 1.1',:.91 0.1'8579
( .0<;'') 0.14709 J.1LIP.3 0.e9939
0.100 0.1'5310 1.1776<; 0.'10975
0.125 0.1"002 1.<-}300 0.93214
f'. 1 "G 0.201\1<; 1.743(,9 f).n4769
C.17e; O.235f7 1.:>6e64 0.957£'9
0.;:0'>0 .1.?6370 J.~o('\15 0.Q6369
~.7?5 0.79077 1.:O[:!/j0 0.96574
C.~50 0.318<'5 1.3'744 C.96453
0.'75 0.34571 1."3369 C.9~041
C.300 0.37330 J.:V.J8'i O.9~364
n • ...,~'5 0.400",2 1.34713 0.94446
I"j.250 0.47P35 1.:49 .. 7 0.93301
('.37'5 0.45597 1.34095 0.<)1943
C.I.C~ I) .4 ':! 3-',0 1.34555 O.9;):se?
O.42!l 0.51092 1. :3922 0.08628
O.4~O 0.~3A45 1.3]990 0.86635
0.470; O.!"65Q1 1.31146 O.P4559
r.5')1) O.593~O 1.10112 O.C22~3
C.5?5 ').6711)2 1.2!:.U,6 0.79770
C.~50 O.('4q~5 1.25936 C.171C9
".o;7~ Ci.676f)1 1.2~19d 0.14770
(\.600 O.703t>0 1.1 "<)73 0.11 ?57
O.t.2e; 0.73112 1.1t,175 0.68051
(\.65(1 C' .75 P('S 1.111.74 0.64664
C.(7" 0.71'617 1.01.761 O.lo1004
('.700 0.8137(, 0.9'11\('8 c. ~7?o04 ('."1' 5 0.'l41?2 C.'i?910 0.53213
0.7'50 0.U6'l7!. 0.e~~24 0.490'19
('.775 O.'lQf,"7 0.77'130 0.446 .. 6
0."00 O.923!'O 0.c.9PP1 C'.39Q35
(.'1"" 0.q'I"'2 0.',17:33 0.349::;'9
o. 8~ 0 0.97'385 C.S34f'6 0.£9625
Ct. :'7''# 1.00'>:'7 Ci.449uf 0.2::949
C'. ~(j0 1.013'10 O.3(,inO O.17P49
r.910 1.044<;1 0.32754 0.15212
'\.720 1.0'55i:? 0.:'9237 0.1i1607
C.4I;", 1.01>6'13 (,.7'>697 0.09644
(".q4() 1."7794 0.72127 0.C6975
(1.""0 1.0!l8Q5 O.ll'S~q 0.03983
r.Ql,O 1.OQ<JQ6 O.14'J31 0.00856
0.<"70 1.11097 0.11303 -0.07429
C.9"'0 1.1<'1Q'3 C.076~? -0.05696
(,.t)<)O 1.13299 O.O;9Pl -0.09588
1.<'00 1.144fO 0.007<10 -0.13551
85
PERCENT X/bx
86
r. "',-., fl.r:. ... f'\. ",r ")
".("\f" '''"'. n"." n. ",,~ .... 1"\. ""~"\
,).'~'1
l;~
('\ •• t""'\
".'''''' r ..... " .. r.-"')~
r,. "r, "'\ ().":.7 r
" .... "''' (\.-.,c.
-.-'7 C
... I." ,... ,. • ' ., C
r". It r" r, '). -,~
f"'.~"(,,\
,... L .., t'
r.rno n.(~c
r. {.r:...,..,
n.. 1-,7 r ~~,
r.-,.?('
" ... , .. ,.. "".'7 r
..... "'(,"
"'.01:' ..,
" ........ ...,. rJ'-, ~
(" • r1 ~.
,... ,. ~ .. . ~. ~~ ""I
,~ • ( I #'
"'. oC' r n. C f," f'I.C"'7 r "i-. " I" ,.
". r ()r, 1.'l)r
A-6
x n .r." .. .,o " • ""; c:; I) 1 5
".'''''''',) '" • 1 1 f,' 5 1.1 ') I , "
"".!4~"(')
".1 C::7 "'I)
" .1(1~~C '.17i- r
'.1~7r')
"'.'1; .., ".-,"'o~5
"'\. "0" .. ?
" • ""t +'),),... ("
,. • ;. 1 '. "'l -,
"".'l,'1?7,)
" . - "'. l ') " • .., r"lr" '" " • '.1 ' ~ 7
.,f'i.' ').L ," ')~
".~l7-7
1."4''7~
"'.'"1,<"1' "'. 0"# r (t
.1."" "7 ..... ' '. t.. .... C"
.. • f, t.,'J f,?
j ./)()~"'t'
n. """) --,
".7"1':' "" • -' .. ~ I ~,.
., • t'" 1 .. '7
". n:~7?': " • ("~ 7"'> '"2 ... f')f"> ''1
t"\ .', .... .,-7 ,. • ~ ' ..... -'t" (\ ...... 7 •• ., ., "'\ .rJr, , fie
.""'0 ~ , • r-, 1 "'I" ..,
1 ....... ~ ,~
1 • "'4r ! f\
l.nr() ..... ~ '.')",)40 1.1'\7n<;<; 1 • r.. cr-, "'\
'.f"'..-,"''''t'' 1.11"\1'10
Build Blade Mean Sectlon
HOT RADIUS:: Jl.09300
SUCTION SIDE Y TOP
!.l1;bl 1 .11, r,3 I. 1.!7"'3'~ 1 • 1 '-1' "0 1 • '! () 7 (,
~.''''44 1. "07el. 1.'''1<:'4 1.?r;'·~~
].~")1)6~
, • "'I'"":', l .. ~~?O' 1 .: l')t')":1
! . I. r." -, 1 !.:·')1')4 1.- n .)(,r,
!.ln~!(,
1.' f"lr,/:,:", 1. 1 7f,4-'
1. -; F, ~ 41 1.J471.Q 1 • -, ~ I,' 1 • ~ '1 r " ~
, .... n .... " 1 ! • ~(f ~-: ...
~.":/ .. 5n 1.17~?l 1.11",(\1 1.f"f';l.r)
1. :)1) 4
•• -:"',,"~7f, "'\.7C"{"\~')
('. ~ il, -.: ..... ' " rIo S ", • r "ll. -. "
r .' ~/.77
"'.4f}°lt;o "'.-?"73 ,...--~~7')
• -; fJ # '" (")
,.. .... "";'Q ,. .1 \.f'4c,!i
r'.'!.h7:6 (':.1\(.7: '1.1"11'1C; ,.. ." ",nQ rI .... ?(,lfl r.f'O--Qq
PRESSURE SIDE Y BOT
:1.9"Of,7 0.91""1 ~. Q4~ ~o
f'.Q,t.<bn '1.on')~"~
l.OO"'7" 1.01""2 I.()?'16 1 • "'tl. 't~ l.n<~"'2 1. , ... b511 1.1°41,7 1."97o ? :.1~·An6
1.lOCJF'2 1.1"o6~
1.1 r'''''3 1. )'ie-,,> 1.f\:;~16"
1 .""';'76 ! .I)f.n,o 1.n4~1' 1."'2103 "l.QQ"94 fl. q-':::!:l' f)."4 ';,f,4 ",,\.c"17"'~
o.[)('rq9
"'."'5~r;o
n.?!717 °.770 -'1. ,).7/,0:'1 1).t.Qn "7 r'I.( <;<;_\9
'.6,))0., ".r(\.,.,,, n. <;1 ?51 C.' /,f) J.)"
0.'. nt,·' r ". "4'"l~~: ,.?Q("\C,':;
(I. ?2 0 ;?9 1"\.1(,',')0 n.l1°46 ~. 111 '.7 ".0°-;'-"'" "". '" I' r--4..,n
0.n;;7/·5 -D.OO] t.? -0."'125 -').(\(,11,3
-".('C)?31 -l'I.l:'31Q
A-7 BUlld 1 Blade 1/4 T1P Sectlon
HOT RADIUS = 11.55200
SUCTION SIDE PRESSURE SIDE PERCENT X/bx X y TOP Y BOT
o.c 0.17'113 1.?41~1 1.0(,966
O.:I)() ('1.138 .. 2 1.:6764 1.{)9942
f". \.~? '. ('.14771 1.78950 1.10171
0.0:0 O.156 QQ 1.:!,)fl38 1.11175 0.('\40 C.IM:'9 1.324Q 6 1.12350
C.Cco O.17'i51 1.33'171 1.135103 l.(\60 (I .1 Q4116 1.:5291 1.14684
n.o7r. 0.1'1414 1. 2 f ... !l 0 1.15751 e.l'C") ('.?C)"3 1.37553 1.16730
C.ooO 0.71277 1.J~525 1.17f-12
v.ll)n C.;!;>;>()1 1.:N40:? 1.18195
C. 12 t o .74S?? 1.101747 1.19937
0.15t' 0.7/''',44 1.47641 1.2C927
0.17' O.?91t6 1.43661 1.21414
G.21"11) 0.314fla 1.44341 1.214313
C,. '" 5 o. BP 10 1.',470'1 1.2103Q
o. :50 0.36132 1.44737 1.?C746
O.27!:· ('\.3'3453 1.44~B4 1.1c;.091
0.300 0.40775 J.44110 1. l7t-CO
().'75 0.43097 1.43365 1.15794
c.:SC 0.4541'1 1.47348 1.13"95
0.:75 0.477 .. 1 1.1.1052 1.11219
0.400 O.5C'()('3 I.Z<J46Z 1.Of6!!4
(,.42'; (I.523'i4 1.37564 1.05801 O.45 r, 0.5 .. 7')6 1.3!>324 1.02686
C.47' O.<·702tl 1.37699 0. 0 9347 (l.~ro 0.5 0 3<;0 1.2 4 676 0.95794
'l.~25 0.(01677 1.?59 C r 0.Q7037
r. ':~ ..J o .fJ9C,4 1.71325 C. C80C1
C.~75 O.(,t.31~ 1.171.,0 o. e3935
0.600 0.6f16:'7 1.1202«1 0.79603
('. t-7 5 O.709~9 1.06221 0.750QO r. ~.c r", O.732'H (l.o9642 0.70401 0.l.7,) 0.7'5603 O.97P29 (\.6!:537
1. 7': ~ ('.7-,Q"5 0.€(,O49 0.1-,1)503
u. 7? ~ 0.1'0"1.6 C.74714 (,.<;5307 0.?')(" O.e756B 0.72303 0.49935
0.775 0.C41190 O.bC,317 0.44406 O.~O(l o.r72]~ O.'ii:'73 0.38714 o.ne:; o.e9~J4 0.5117{J 0.32P65 :) or("l 0.0Ie~6 ,) .44:')1 Ii 0.ll-86? . - , i).!l75 ".94173 c.. 3f-R n 0.20709 O.O/JO O.Q64o q O.79~'''6 0.14418 (1.41" 0.'174:>8 0.26683 0.11864 (,. <:'7 (' J.9"3~7 (,.::'3770 0.0'12"'2 ('\.'-'3(' 0.Jn':6 O.20!!55 0.06704
C.<'4C' 1.C0214 C .1743<; ('.04098 G.("'5'1 1.rH1 4 3 C.15007 0.01480
o.o .... C 1.02077 0.11077 -0.01150
CI.S70 1.030"0 0.('9131' -0.0378Q
C.9n~ 1.C39"'9 0.C6700 -0.06443 O.oc,:) 1.041l~3 10.0:256 -0.09174 1.(,00 1.057P7 0.00306 -o.11Q71
87
PERCENT X/bx
88
('. - r ,"'
('. -.-1'\ I". "l7r
.-.r "'. , c, ....
".1 7 ' n. -. l' "'. -~~ 1."r'lf"!
"' ... .,r ,..-.." ...
., ..... 'i • .:. "r ... 4?~ r.,r"\ ".'-,r ..... ' if'" ,. • t' -. C
'. C" c
r.r-.r
".,')') ". ' -. ~
•• , "'I r
ro. ~r j
". --..,.. '1.(''''''
"."'",r
..... ("I"' ....
"'. I 1 r.
..... I I.'" r • r 'I ('
" • t' ,_ f\
....... 71' ('.C;~
(',o<)n t • nr·r,
A-8
x ", • 1"7'" r r
I'I.'''I'\')?
".1':)~t.
"'.'7'-". ,.. • .... r L, .. t")
'1 • "'1 (, r "' 'I.:'?"' "'2 ".",1 /.(, ,,)."''''-;''"6 r..~ ... Q~tJ n .... C t, ... ,...,
~.;>-'7-,r;
" .;--~Qf'r
~.:"! I'J'" r:: f'\. '14""0 "I • ., I, , &I r
"'. -'"1 (' ,.., • IT 1"11 ."" ~ ~.Jf?cln
f'\ • It I. I) 1 r
("" .'.f.. 7"" n f't. t f" ()..., '"
"'l ..... ...,~.,""" """.r""l.)",r
..... r~t/~
".r-,., .... r:
r • c '1"".1. r ')
-•• I J .' <;
".'''. ',(' \ • ,.e:" r.{.~
'"'.,.. .... 7-,n ".IQ'l .... c:
".71f)"'"
.... -''''''' r:
r'\. '1 '"'4 t'. 0 r • f"")~"". "."l.lln I'll. '" (7" ,. ""'i. "''''''''''1
("\.~~., ... "7?
I) • (J' .. 71 , "".,?rr~·(
("I. ,,.,.'" "'I?
..... nQ'4 r. • 'I ,-, I h
1 .(If • .'."' '1 1."1', ri)
BUlld Blade T1P Sectlon
H')T ~AOIUS - l~.~}?OO
SUCTION SIDE Y TOP 1.:,')77 !.'<;111 1 • '''', ') 1 ~.""'77q;)
! .', '/4't
1.4"'~('t1
1.1,"'19'3 /, 1.4lf75 1. i , :t,:" ~.';431
1 •• 41r .... 1 • ·9 r r.; 1 ") !.G.h~,5~
'.4??6'i 1.' 7!,',', 1. _nc7 1.'7'''''' 1 .';"11 "'" 1. 1,'.:'.4 1 .4~ ,,\"e; 1.,~1")19
1.'.:-?2' ! .J·~'17'3 :.177:>r'.~l.P?1'\
:.:1~67 , • .., 7? 1 Q
1."''''1~'' , • 1 !) - ':" '2 ~.1"\3?
:. "? q ~ f, r."7''')?
,"'."lIn: ,... n .() 7':; ..... "7 r .-,?n . .' "'.·'!7hh 0.(52°l. "'. I .., ~ l't r.r:"'?7 r'.I.'~15 ..... .., ';''':l L. ') r"."l. .... .)4?
..... -'6:'4"1 O.?:-..,."'tq
"'.~~1:7
.... 1 r r: "l" "' .. 1 ",q "'i'")
-.l"!"~"
r.· '')77''1
"".1"1 ?'j
• r~"l t ..... r,'(~l;1
n.fl'\"'I14
PRESSURE SIDE Y BOT
1.1""'4 1.1"['<')1 ].1'74:;" 1.7"7?('I 1.?1e<n{t !.22?4,! 1. '3917 1.7'.779 1.2~r4<"2
1.?n??2 l.~f-"O? 1.2":>47 l.?(l'31Q 1.??:?"5 1. 7 1'1-(9
!."f,7Q 2 1.''5''7'' 1.23')65
1.1'10."7 1.1(,n·Q I.IZ'l'5Q 1. 'l9f>O? l.nnon? 1.07?0' n.<;91<)9 ('. Qt,"" 17 "."Of?l n.''''>l?t. n.p""S40 C.7577Q n. -H1Q"o (1.""9}9 "".ln~-i<>
". ~)~666 "'.rn(,11 ('.4~,(n'l
". -:"(,74 "'."4?03 n. ?Po7J ". 2J"\~,~ '1.1741Q .... 11"4., ,).Of' .. +r~
"".'171(·0 n.,,1."';6 ()."'~C;I.r;
1"\.1",(\., ")7
-f\.07091 -n.('I447? -'i."',?f,4 -f\.09107 -0.114')5
PERCENT X/bx 0.0 0.010 0.020 0.030 0.040 0.05U 0.060 0.070 0.080 0.090 0.100 0.125 0.150 0.175 0.200 0.225 0.2">0 0.215 0.300 0.325 0.350 0.:315 0.400 0.425 0.450 0.415 0.5JO O. ~-7 5 0.550 0.575 0.6JO 0.625 0.050 0.0(5 0.100 0.725 0.750 0.115 0.800 0.825 0./j';0 0.1l7S 0.900 0.910 0.920 0.430 0.<,140 0.9')0 0.960 0.(110 0.980 0.'J90 1.000
A-9 Build 2 Vane Root Section
HOT RADIUS. 10.21100
x 0.0 C462 0.0 l127 0.02991 0.04256 0.05520 0.Ob1d~ 0.Ob050 0.09314 0.10579 0.11£43 0.1310b O.162b9 001 "431 0.225'13 0.25754 0.2 B916 0.32011 0.3523'1 0.38400 0.41562 0.4472:'1 o ... 11185 0.51046 O.5420tl O.513{)·' O. () O'dl 0.63692 0.6N<:>4 0.10015 0.73177 0.7t.338 v.7'1~OO O. 6 ~661 O.B ~1)23 O.B fj"8'+ 0.'>'2146 0.95307 0.98469 1.0163U 1.(-4192 1.07'1!>3 1.1U15 1.14216 1.15541 1.16805 1.11,010 1. 1 ',fB5 1.205Q Q
1.21664 1.23129 1.24343 1.2~~5e
1.26QZ2
SUCTION SIDE Y TOP
2.71029 2.18472 2.7'1871 2.81223 2.82531 2.831'f4 2.85011 2.86185 2.67312 2.311393 2.8'1430 2.91821 2.9 :)922 2.~H29 2.9723"+ 2.98428 2.99302 2.99844 3.00038 2.q9864 2.99;:'03 2.9!l327 2.96904 2.94993 2.'12547 2.89501 2.85774 2.01257 2.751302 2.691A3 2.61085 2.50816 2.311S16 2.~5010 Z.lOh51 1.95671 1.8018<) 1.64254 1.410 10 1.311 h3 1.1 .. 0l5 0.96,,+75 0.78477 0.7113t! 0.63721 0.56205 O.435'l1 O.401:l70 0.33028 0.25035 0.16814 0.08520
-0.00093
PRESSURE SIDE Y BOT
2.60028 2.59138 2.56134 2.57032 2.55843 2.54516 2.53237 2.51R34 2.50312 2.46855 2.47286 2.43163 2.38180 2.34110 2.29356 2.24356 2.19182 2.1:)8 .. 6 2.08361 2.02729 1.96958 1.91050 1.&5012 1.78844 1.72550 1.66126 1.59516 1.!l289b 1.460u1 1.3'1143 1.32065 1.2,,+840 1.17471 1.0'1941 1.02248 0.94313 0.66306 0.16019 0.694<)3 0.60686 0.51553 0.42019 0.31919 0.27781 0.23456 0.18980 0.14319 0.09426 0.04228
-0.01408 ~0.07774 -0.15559 -0.22302
89
A-10 BUlld 2 Vane Mean Sectlon
HOT RADIUS :0: 11.09400
SUCTION SIDE PRESSURE SIDE PERCENT X/bx X y TOP Y BOT
:
0.0 0.00483 2.82634 2.65481
0.010 0.01747 2.84050 2.64625
0.020 0.03011 2.85428 2.63648
0.030 0.04275 2.66767 2.62565
0.0 .. 0 0.05539 2.80069 2.61385
0.050 0.Oo1lO3 2.8'1.BO 2.60120
0.060 0.Ob067 2.90551 2.58175
0.010 0.09331 2.91132 2.57358
0.080 0.105'14 2.'12870 2.55814
0.090 0.11&~8 2.93961 2.54329
0.100 0.13122 2.95021 2.52126
0.1~5 0.16282 2.97464 2 .4b4 &5
0.150 0.1'1442 2.99622 2.43950
0.115 0.2l601 3.01484 2.39151
0.200 0.25761 3.02)032 2.34111
0.:>25 0.2&921 3.04251 2.28861
0.2!JO 0.3201:'1 3.05123 2.23414
0.215 0.35':'40 3.05621 Z. .11115
O.JOO o .3t .. CO 3.05139 2.11959
0.325 0.41560 3.05433 2.05973
0.350 0.44120 3.046113 1.99623 0.315 0.47H19 3.03438 1.93514
O. ',00 0.510;:''1 3.01675 1.87054 0.4<:5 0.5 .. 199 2.99339 1.80439 0 ... 50 O. 5 13~8 2.96374 1.13616 0.415 0.60;16 2.92713 1.66166 0.500 0.63618 2. B8?73 1.59101 0.5,6 0.6bH38 2.829'+8 1.52496 0.;;0 0.6 '199 1 2.76613 1.45135 0.575 0.13151 2.6'1095 1.37611 O.bOO 0.16317 2.60164 1.29944 0.625 0.79471 2.49664 1.22102 0.650 0.82636 2.31178 1.14093 0.675 0.857'16 2.24711 1.05902 0.100 0.81:1956 2.10611 0.97523
o. 7~5 0.'12115 1.95608 0.1:<8938 0.750 0.95215 1.79180 0.80135 --0.715 0.90435 1.63196 0.71088 0.800 1.01595 1.45<122 0.61117
0.1125 1.04154 1.27996 0.52159 0.850 1.07'114 1.09461 0.42191
0.875 1.11014 0.90351 O.31H9 0.900 1.142.H 0.10104 0."0694 0.910 1.1!1491 0.62693 0.16353
0.920 1.16761 0.54600 0.11691 0.930 1.lti025 0.46424 O.068R9
0.940 1.1'1269 0.38167 0.01924 0.950 1.2e553 0.29831 -0.03235-
0.960 1.21tll1 0.21,+16 -0.086~4
0.970 1.23081 0.12924 -0.14341 0.9130 1.24345 0.04352 -0.20465 0.990 1.25609 -0.04294 -0.21213 1.0UO 1.2oti12 -0.13016 -0.35014
90
A-ll BUlld 2 Vane T1P Sectlon
HOT RADIUS = 12.34200
SUCTION SIDE PRESSURE SIDE PERCENT X/bx X y TOP Y BOT
0.0 0.00504 2.87973 2.70205
0.010 0.01767 2.89441 2.69689
0.020 0.03030 2.90&57 2.68930
0.030 0.042-}3 2.922.!1 2.67973
0.040 0.05556 2.93534 2.66852
O.O~O 0.06819 2.947Q7 2.6~592
0.060 0.0 1l0e2 2.90009 2.64211
0.070 0.0'f345 2.97171 2.62724
0.0!<0 0.IOo0B 2.9~281 2.61141
0.0'10 O. 1111 71 2.99340 2.59472
o .ICO 0.13134 3.0034'1 2.57724
0.125 O.lbi92 3.02651 2.53054
0.1'>0 0.1 '144'1 3.04633 2.48010
0.115 0.22606 3.06292 2.42647
0.200 0.25764 3.01622 2.l7007
0.175 O.2ll'l21 3.06616 2.31118
O."SO 0.32079 3.0'1263 2.25001
o.ns o. ~!:.i.)6 3.09551 2.18674
0.300 0 • .3 b3'14 3.0'1463 2.12157
0.325 0.41551 3.(.R981 2.05456
0.350 11.44709 3.080t'1 1.98579
0.375 0.47l66 3.06733 1.91536
o ... JO o.~ 1023 3.0 .. 9C2 1.84332
0 ... 25 O.541tH 3.02544 1.76970
O.4~0 0.573:>8 2.99bOO 1.69456
0.475 0.6(4'16 2.95995 1.61788
0.500 0.~j,...53 2.Q1634 1.53970
0.525 O.66H 11 2.80379 1.45998
0.5!J0 0.6'14 68 2.80039 1.37877
0.575 0.73121:> 2. 72~ 11 1.29598
0.600 0.76283 2.62841 1.21164
0.625 0.79 .. 40 2.51581 1.12565
O.r-50 o .1l2598 2.3t'667 1.03801
0.675 0.85755 2.2 .. 261 0.94859
0.700 0.8 to9l3 2.0(;561 0.&0;733
0.125 0.92070 1.91743 0.76408
0.750 O. '15228 1.73991 0.66874
0.775 0.Qt385 1.55447 0.57107
0.8..10 1.01542 1.36249 0.,+1088
Ci.825 1.047UO 1.16497 0.36779
0.850 1.01£<57 0.96292 0.76146
0.b75 1.11015 0.75b95 0.1:;1 20
0 • .,,00 1.14172 0.54780 0.03627
o. 'ill 0 1.1 ~35 0.46332 -0.01l2Q
0.920 1.1t>69d 0.37844 -0.05993
0.930 1.11'161 0.29317 -0.10980
0.<140 1.14224 0.20753 -0.16105
0.950 1.20481 0.12156 -0.21394
0.900 1.21750 0.03527 -0.26882
0.970 1./30l3 -0.05134 -0.32617
0.980 1.2 .. 27b -u.ll822 -0.3866~
0.'1'10 l,.!~,,"q -O.ZZ53d -0.45152
1.000 1.2"h(.2 -0.312 7 9 -0.52292
91
PERCENT X/bx
92
c. U (,.(,10 , • ;:~C o. C~1) 0.040 C. (,50 0.060 C.070 C.fJ30 C.OQ:) c. lOO 0.125 0.1';0 (".175 O.7ne t.:':!: O.2':>C ':'.275 V.J{)~
C" ??5 t. )~lC C. "7~ 0.1.0e. (.4<'5 C ... 'iO C. 475 c. ~OG :.525 0.5')0 C.575 O. (,00 ().625 (.l50 C'. 675 ('.700 C.725 c. -'50 (. n5 o. PCI) 0.825 C.SliO C.875 c. QQO C.910 o. "70 0.910 r.940 0.'150 O.QbO C.970 0.9CO C.990 1.000
A-12 BUlld 2 Blade Root Sectlon
HOT RADIUS. 10.11400
x 0.0 0.01018 O.C2036 o .G30 54 0.04072 0.050 QO 0.06 lra 0.07126 0.0314 .. 0.09162 O.IOleO 0.12725 O.l">27C 0.118;"5 0.7031.0 0.22QL5 0.25450 0.77<195 0.JC540 0.33065 0.35630 o .3r115 0.40720 0.43765 0.'.5810 0. 108355 0.50Q(0 0.51445 0.55990 0.58535 0.61080 0.63675 0.66110 O.bA715 0.71260 0.73805 0.76350 0.78895 0.81440 0.83905 0.86530 0.89075 0.91620 0.92638 0.93656 0.94674 o .956n 0.96710 0.91773 0.98746 0.99764 1.00782 1.01800
SUCTION SIDE Y TOP
0.70967 0.16221 o. CC548 0.&'.236 c.. b1604 0.90599 0.93336 0.95(>57 O.9t195 1.C':'374 1.(;2411 1.06919 1.1(,914 1.14324 1.1 n-'9 1.]ge29 1.22u10 1.23849 1.;'~J64 1.26568 1.?7411 1.7e076 1.2c~e3 1.78389 1.28C88 1.174(:.5 1.26505 1.25H2 1.23462 1.71299 1.13627 1.1~34? 1.11315 1. Cb271 0.99952 0.92883 0.85423 0.77687 0.69132 ~.(,1600
0.53306 t.44855 0.36264 0.32763 0.29779 I). 2574fl 0.22197 0.18615 1).15006 0.11367 0.07103 r 1)40 CO 0.O,.;26~
PRESSURE SIDE Y BOT
0.48962 0.51336 0.53533 0.55574 0.57474 0.59241 O.609C2 0.624~O (1.63£>98 O.6~253 O.66~21
Ci.69343 0.71719 0.73698 0.75319 O.7M14 O.770()5 0.76313 0.78754 0.78939 C.78881 0.78587 0.7(1064 0.77317 n.16350 0.75166 0.73165 0.72148 0.70314 f..68l60 0.65983 0.63477 0.60738 1).57755 0.54520 0.51020 0.1,7238 O.4~157 0.38753 0.33996 0.28849 0.23265 0.17180 0.14587 0.11893 0.09091 0.06171 (i.03121
-0.00071 -0.03422 -0.06951 -0.10684 -0.14653
PERCENT X/bx
0.0 C.OlO 0.C70 C.030 (.040 C.Cr,O 0.C60
c.cso O. ;:'90 O. 100 J. 125 C.150 C.17~ (). "::0 O. ??5 0.250 C.275 (\.300 (I. 2125 C'. :-''i0 t.375 (\.4()0 C.425 0.4')0 (,.1,75 r'. ~,co ~. <;25 o.~~O 0.575 C.bOO C.625 ('.650 r.615 C.7CO Ci.725 (.150 C'. ;-75 D.POO ,~. P?5 0.850 c.a15 (,.QOO C.910 C.920 c. '130 o. <;40 0.950 c .... {;O O. c<10 0.980 o. Q<OO 1.0'lO
A-13 Build 2 Blade 1/4 Root Section
HUT RAUIU~ • lO.63~OO
x 0.02723 0.<)3670 0.04617 0.O~564 0.(.6511 0.07458 0.00'.<"5 O.OS3~7 0.10299 0.11246 0.12193 0.14560 o .1!>928 0.19295 o .?l663 0.24030 0.26398 0.28165 0.:n133 0.3350:> 0.35863 o .3P2 35 0.40603 0.42970 0.45338 0.417(,5 0 .... 0073 0.52440 0.54806 0.57175 0.595"'3 0.61910 0.64278 0.666~5 0.69013 0.71380 0.73148 0.76115 0.18483 O.808~O 0.83218 0.1\5585 0.81953 O.P1.'900 0.e9841 0.'10194 0.91741 0.92688 0.93635 0.945ez 0.95529 0.96416 0.97423
SUCTION SIDE Y TOP
0.89211 C.92342 Ci.'t5185 0.9Tl93 1.00704 1.'2445 1.04538 1.(;6498 1.08340 1.10u7'-1.11108 1.15406 1.18614 1.71395 1.23192 1.25rI3~
1.27548 1.28945 1. 30~'39 1.3CB35 1.31335 1.31537 1.31436 1.31021 1.30278 1.29183 1.27707 1.25"01' 1.23426 1.20476 1.16828 1.12263 1. (;6471 0.9,,931 0.'i3053 0.85969 0.18121 0.71345 0.63R5R (;.56270 C.485B5 0.40806 0.32928 0.29749 O.Z6559 !I. 23346 0.20ll4 0.16863 0.13591 0.10304 C,.C69d7 0.03642 0.00273
PRESSURE SIDE Y BOT
0.69667 0.71601 0 .. 73392 0.75053 0.76593 C.78022 0.79J47 0.80576 0.81715 0.82766 0.83140 o.e58~4 0.81523 0.88819 0.39766 0.90390 0.90714 0.90756 0.90530 O. 'i0049 0.£9324 0.8e362 0.81170 0.85755 0.84120 0.en69 0.P0203 0.77925 G.75433 0.72728 0.69807 0.66669 0.63308 0.59720 0.55900 0.51838 0.47526 0.42952 O.3et02 0.32960 (i.27506 0.21714 0.15555 0.12980 0.10337 0.07614 O.Q4836 0.01970
-0.00979 -(;.04015 -c..01l4!» -{j.l0314 ~.13709
93
A-14 BUlld 2 Blade Mean Sectlon
HUT RADIUS • 11.0'1300
SUCTION SIDE PRESSURE SIDE PERCENT X/bx X Y TOP Y BOT ':'
c.o 0.05314 1.07601 0.87672
0.00 0.06lL9 I.L94e2 G.l'9931
C.(20 0.07064 1.11244 0.91902
C.030 0.07939 1.12900 0.9363-4
0.C40 0.08814 1.141.59 0.95161
C.050 0.096139 1.1593(; G.96510
C.CI).) 0.1\1564 1.11319 0.91103
c. :::70 0.11439 1.1[1&:>2 0.98755
c. ('PO 0.123]4 1.1'187" 0.99681
c.cqo 0.13189 1.11048 1.004"4
O.lCO 0.14064 1.22160 1.01200
C.l?5 0.16251 1.24679 1.02559
0.150 0.13439 1.26860 1.03411
C.175 0.20676 1.28728 1.03828
C.20;) 0.22814 1.3e304 I.C3864
C'. :.>Z 5 0.25001 1.31602 1.03560
o. ~50 0.271 89 1.32631 1.02948
C.275 0.29376 1.33396 1.(,2054
0.300 0.31564 1.33899 1.00e99
C.::25 0.337 "1 1.34137 O.9c;4Ci9
(\.:S() 0.359~9 1.34104 ().97870
C..37~ 0.38176 1.3.H90 0.96021
0.400 0.40314 1.33179 0.93964
0.425 0.42501 1.32251 0.91706
0.4<;0 0.44629 1.30975 (\.89254
0.1. 75 0.46376 l.z'nC8 0.86612
C.5:» 0.49064 1.27192 0.83786
c. !.2!> 0.51251 1.24~36 0.80779
(,.550 0.53439 1.212"0 0.77592
(.575 0.556"6 1.16940 0.74228
c.w::. 0.57314 1.11411 0.70687
0.625 0.60~O1 1.C!>230 ".66969
o. 6~O 0.621139 0.S8805 0.63074
0.675 0.64376 CI. 92241 O.~O999
o. 7C~ 0.665(4 O.85!>65 0.54743
C.725 0.68751 £I. 7rao 5 (j.50301
C.7'i0 0.70939 0.71975 0.45670
C.775 0.731l6 CI.b!>089 0.40844
('.1'00 0.7!>314 0.53137 0.35816
C.fl25 0.775ul O.!.1l29 0.30578
o. P')O 0.7Q689 0.44066 0.25120
c. e75 0.81876 0.36953 0.19431
c.<,o:) 0.B4::>64 0.79769 C.13495
o.'no 0.84939 (,.26881 0.11048
0.920 0.85814 0.23981 0.08558
o. Q)O 0.86619 0.21070 0.06023
0.940 0.P7564 0.11'147 O.034r.1
C.950 0.eS439 0.15211 0.00813
0.960 0.89314 (,.12261 -<l.OI867
o. Q70 O.90Ul9 O.O929!> -C.04!.97
0.980 0.91064 0.063C13 -o.onez
0.'1'10 O.~1939 0. C33C 0 -o.10ZZ2
1. tOO 0.92614 0.00262 -(1.13122
94
A-15 BUlld 2 Blade 1/4 T1P Sectlon
HOT RADIUS· 11.55200
SUCTION SIDE PRESSURE SIDE PERCENT X/bx X Y TOP Y BOT
c. c 0.083')9 1.25737 1.(i1672
C.CIO 0.09163 1.26350 I.C6302
C.C20 0.09967 1.71404 1.(,9122
C. DO 0.10171 L. ?B400 1.11282 '. C.C40 0.11515 I. ~9342 1.12902
C.050 0.12379 1.30232 1.14212
C.ObO 0.1313) }'~lO13 1.15282
(.en 0.139r? 1.31P05 10 1t.155
0.C80 0.141'11 1.32611 1.16912
c. G90 o .1,>,>QS 1.33311 1.11484
C.100 0.16399 1.33969 1.17901
C.I?,) 0.18409 1.35421 1.18388
C. 1 'i0 0.20419 1.36632 1.18244
(1.175 O.n4?9 1.375'73 1.17601 0.;;(,0 0.24439 1.::e315 1.16561
C.125 0.'26449 !.3e8C;I 1.15185
<.'.250 0.£'8459 1.39049 1.13507
c.ns 0.30469 1.29051 1.11568
C.3Q() 0.32419 1.38816 1.09394
C.375 0.3441'9 1.:'P)15 1.07007
r • ~r)o 0.30499 1.37~38 1.044210
0.:;15 0.38509 1.36462 1.01659
C.400 0.40519 1.35fJ57 Q.98723
('.425 0.42'>29 1.33280 0.95676
('.4'i0 0.44539 1.31066 0.92376
(.i.75 0.46549 1.7P32P 0.P'979
C.'CO G.49559 1.74910 0.85441
C.~25 O.!-O569 1.;:0543 0.81767
o. ~,50 0.52579 1.15014 0.77960
C. !>75 0.54569 1.09238 0.74024
(.600 0.56599 1.03249 0.69960
C'.625 0.5El609 0.97151 ~.65771
~. £,0;0 0.60619 0.90982 0.61458
c. b15 0.62679 C.84754 0.57021
(1.700 0.64639 0.711480 0.52461
(,.725 0.66649 0.72162 0.47117
C.750 O.6!!659 0.65807 0.42969
0.175 0.70669 0.591.,16 0.31'035
(I. eGO 0.12679 0.52992 0.32973
(\.825 0.14669 0.46533 0.27781
O.P'>O 0.16699 0.40042 0.21456
0.815 0.18109 0.33516 0.16993
O.CO') 0.r0119 0.76951' 0.11367
C.910 0.81573 0.24326 0.09104
C. <;20 0.823?? 0.21660 C.C6197
0.930 0.63131 0.1'1035 0.04465
C.940 0.83935 0.16316 0.02107
c. Q50 0.64139 0.13717 -0.00275
(1.960 0.1'5543 0.11051 -0.02683
(,. <,,70 0.86347 C.08369 -0.05119 C" qQo 0.fl7l51 0.05686 -0.01581
(.9QO 0.87955 0.07994 -0.10012
1.(00 0.(18159 0.00269 -0.12591
95
A-16 Build 2 Blade Tip Sectlon
hLJT RADIUS· 12.01200
SUCTION SIDE PRESSURE SIDE PERCENT X/bx X Y TOP Y BOT
~ 1.27932 (\.0 0.1111:8 1.40015
C.ol0 0.125;>0 1.4071(: 1.28672 ('.020 0.13253 1.41339 1.29267 C.030 0.13985 1.41909 1.298&2 c. :)40 0.14111' 1.47423 1.30312
C.050 0.15450 1.42885 1.3C72Z C.060 0.16183 1.43297 1.31092
C'.070 C .16915 1.43664 J.31342 (.C,flO 0.11648 1.43~36 1.31492 O.G90 0.IU3no 1.L.42b!> 1.31521
C.IOO 0.19113 1.44504 1.31472 c.125 0.20944 1.41,931 1.30791
(".1"0 0.22775 1.45126 1.29499 (.175 0.24607 1.45J.OO 1.27746 G.700 o .?6438 1.44860 1.25631 C.22!) 0.2821.9 1.44/.04 1.23215 Ci. <''50 0.30lUO 1.43732 1.20546 C.275 0.31932 1.42e35 1.11658 c. :00 0.33163 1.1,170., 1.14519 o. ~25 0.35594 1.4C3(17 1.11328 o.?<c 0.314;>5 1.3&628 1.07925 (.:75 0.39257 1.36620 1.04331 C.40j 0.41088 1.34214 1.0')710 C.425 0.42919 1.31301 0.96921 0.450 0.44150 1.£7673 Q.930n C.475 0.46532 l.n9!>3 0.89021 c. !)OO 0.48413 1.11~81 0.81,923 (:.525 0.50244 1.12025 0.80734 r.5')0 0.52075 1.06373 0.76459 o. ~75 0.539(,7 1.0':'661 0.72102 ('.60,) 0.55138 0.94905 0.67666 (.1>25 0.51569 0.89111 G.63155 0.650 O.5Q4(i0 0.1l3~04 0.5R512 o. () 15 0.blZ3? 0.77463 0.53920
"(,.100 0.63063 0.11603 0.49200 C.125 0.64894 C.6513C C.44415 G.750 0.66125 0.59837 0.39567 C.715 0.68557 O.~J930 0.34657 c. FCO 0.70338 0.408015 0.Z9688 o. e25 0.12219 0.42(,82 (\.24659 C.850 0.74050 0.36140 0.19573 0.875 0.75882 0.30~67 0.14431 0.900 0.71713 0.;>4227 0.09233 0.910 0.18445 0.21842 0.07139 C.9?Q O.7911P 0.19451 0.05036 0.930 0.19910 0.17063 0·.02925 c .... 40 0.80643 ... 14669 ('.00804 (1.<:50 0.81375 0.12219 -!I.CI325 G.Q60 0.021US 0.u9883 -0.03462 0.970 0.92840 0.074 9(1 -().O5607 e'.990 0.S3573 C.C!"U91 -ti.07762 ('. (1'10 0.84305 0.<..2695 -0.09924 I.COO 0.e50~3 O.OO2'H -G.12095
96
Flgure
B-1
B-2
B-3
B-4
B-5
B-6
B-7
B-8
B-9
B-10
B-11
B-12
B-13
B-14
B-15
B-16
B-17
B-18
APPENDIX B - BUILD 1 ANNULAR CASCADE DATA
Tltle
EEE Uncooled Rlg 36% Reactlon Annular Cascade Loss vs. Mach Number (Area Averaged)
EEE Uncooled Rlg 36% Reactlon Annular Cascade Loss vs. % Span EXlt Rake Data (Area Averaged)
EEE Uncooled Rlg 36% Reactlon Annular Cascade Loss vs. % Span (Area Averaged)
EEE Uncooled Rlg 36% Reactlon Annular Cascade Loss vs. % Span (Area Averaged)
EEE Uncooled Rlg 36% Reactlon Annular Cascade Loss vs. % Span (Area Averaged)
EEE Uncooled Rlg 36% Reactlon Annular Cascade Mach Number vs. % Span (Area Averaged)
EEE Uncooled Rlg 36% Reactlon Annular Cascade Exit Ps vs. % Span (Area Averaged)
EEE Uncooled Rlg 36% Reaction Annular Cascade EXlt Pt vs. % Span (Area Averaged)
EEE Uncooled Rlg 36% Reactlon Annular Cascade Deslgn POlnt (Area Averaged)
EEE Uncooled Rlg 36% Reactlon Annular Cascade Inlet Pt vs. % Span
EEE Uncooled Rlg 36% Reactlon Annular Cascade Inlet Tt vs. % Span
EEE Uncooled Rlg 36% Reactlon Annular Cascade Alr Angle vs. % Span (Area Averaged)
EEE Uncooled Rlg 36% Reactlon Annular Cascade Mld-Channel Statlcs vs. Predlctlon (Area Averaged)
EEE Uncooled Rlg 36% Reactlon Annular Cascade T.E. Platform Statlcs vs. Predlction (Area Averaged)
EEE Uncooled Rlg 36% Reactlon Alrfoll Surface Statlcs 11% Span (Area Averaged)
EEE Uncooled Rlg 36% Reactlon Alrfol1 Surface Statlcs 50% Span (Area Averaged)
EEE Uncoo1ed Rlg 36% Reactlon Alrfol1 Surface Statlcs 89% Span (Area Averaged)
EEE Build 1 Annular Cascade Clrcumferentlal Instrumentatlon Locatlon
97
TARLE 8-1 DATA SU~'~MARY
UNCOOLED RIG - BLD #1 ANNULAR CASCADE DATA SUMMARY
RAKE PROBE AREA AREA HTD AREA AREA HTD ~lID-
OPERATING PT-IN TT -IN W-MAIN WTD TOTAL MID-SPAN ~~TD TOTAL SPAN POINT f. PSIA oR LBrVS '·lACH # PTjPT PT jPT r~ACH # PTjPT PTjPT
1 57.42 77"' 22.51) 0.779 0.0415 0.0131 0.787 0.0330 0.0125
2 57.42 775 23.09 0.899 0.530 0.0165
3* 57.42 775 23.31 0.967 0.0500 0.01 85 0.979 0.0459 0.0190
4 57.42 775 23.39 1.116 0.0625 0.0255
I) 57.42 775 23.49 1.194 O.07f)5 0.0405
*Des; gn POl nt
98
c.. -c.. <J
-n- , . 1 I I'!" ]f -'I' I:' '1 '!1-', "'1 '.+!' fi ':1 . 012 '! ,11"1:' ",'.'-, ".1':1""1. 1 :, 1': ,r ;'1" :1'I{i!i;H::'lHW1,,,,llt:r: '.'·1 .... 1l1tl!,lfH.r/:t."!tp 1"1 11"-' , I--t~"":r:-'I"'~' In... ',~j+ ' I - -+-.d!.'r::'T1" .,-...-;- ' '. 'P' Ij· T"' 'ffl" '1'1', I"!::r '," , 1-, : I ,":f. It: I'll f,:I, j : 1,1. WI" ': :" " :' .'; II J1:" I: " '" '1.~;' "lil!:!!"' r •• '" J ",x, , ,.... - - .... - • "I," ',1" l~t i"l'l/l .' - 'j,.,. "::t~'H ;ri~ .. ,' y' ~"l'~ ... , - I j (" • It • °t. ~1 I: 1 t • "UfO t" • j' I , ';~, , I ' •
r-- --r-""-I'- j'-fi +-- + -1 ,., 1'-- "~ .. i '-' -'1-" ,1- 'rr'.:.!:! ·t' , ~- "-r-- - " ' -- --I 'j'1 ' ' , " . I , ' , "
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EEE BUlld Locatlon
VIEW LOOKING UPSTREAM
o T E PLATFORM STATICS
o INLET PT
o INLETTT o EXIT PT RAKES
t6. EXIT WEDGE PROBE
\) SURFACE STATICS
o MID-CHANNEL STATICS
Annular Cascade Clrcumferentlal Instrumentatlon
APPENDIX C - BUILD 2 ANNULAR CASCADE DATA
Figure Tltle --C-l EEE Uncooled Rlg 43% Reactlon Annular Cascade Loss
vs. Mach Number (Area Averaged)
C-2 EEE Uncooled Rlg 43% Reactlon Annular Cascade Loss vs. % Span (Area Averaged)
C-3 EEE Uncooled Rlg 43% Reactlon Annular Cascade Loss vs. % Span (Area Averaged)
C-4 EEE Uncooled Rlg 43% Reactlon Annular Cascade Loss vs. % Span (Area Averaged)
C-S EEE Uncooled Rlg 43% Reactlon Annular Cascade Loss vs. % Span (Area Averaged)
C-6 EEE Uncooled Rlg 43% Reactlon Annular Cascade Loss vs. % Span (Area Averaged)
C-7 EEE Uncooled Rlg 43% Reactlon Annular Cascade Loss vs. % Span (Area Averaged)
C-8 EEE Uncooled Rlg 43% Reactlon Annular Cascade Mach Number vs. % Span (Area Averaged)
C-9 EEE Uncooled Rlg 43% Reactlon Annular Cascade EXlt Ps vs. % Span (Area Averaged)
C-1O EEE Uncooled Rlg 43% Reactlon Annular Cascade Exhaust Case I.D. Statlc Pressures (Area Averaged)
C-ll EEE Uncooled Rlg 43% Reactlon Annular Cascade EXlt Pt vs. % Span (Area Averaged)
C-12 EEE Uncooled Rig 43% Reactlon Annular Cascade Deslgn POlnt (Area Averaged)
C-13 EEE Uncooled Rlg 43% Reactlon Annular Cascade Deslgn POlnt Inlet Pressure
C-14 EEE Uncooled Rlg 43% Reactlon Annular Cascade Deslgn POlnt Inlet Temperature
C-1S EEE Uncooled Rlg 43% Reactlon Annular Cascade Average Alr Angle vs. % Span (Area Averaged)
117
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EEE Uncooled Rlg 43% Reactlon Annular Cascade Mid-Channel Statics - 1.0. (Area Averaged)
EEE Uncooled Rlg 43% Reactlon Annular Cascade Mld-Channel Statlcs - 0.0. (Area Averaged)
EEE Uncooled Rlg 43% Reactlon Annular Cascade T.E. Platform Statlcs - 1.0. (Area Averaged)
EEE Uncooled Rlg 43% Reactlon Annular Cascade T.E. Platform Statlcs - 0.0. (Area Averaged)
EEE Uncooled Rlg 43% Reactlon Annular Cascade Alrfoll Surface Statlcs 11% Span (Area Averaged)
EEE Uncooled Rlg 43% Reactlon Annular Cascade Alrfoll Surface Statlcs 50% Span (Area Averaged)
EEE Uncooled Rlg 43% Reactlon Annular Cascade Alrfoll Surface Statlcs 89% Span (Area Averaged)
EEE Uncooled Rlg 43% Reactlon Annular Cascade Clrcumferentlal Instrumentatlon Locatlon
TABLE C-1 DATA SU~lI'lJl.RY
EEE RIG-70709-2 ANtlULAR CASCADE DATA SUtv'r~ARY
*DESIGN POItJT
STEADY STEADY STEADY STATE STATE STEADY TRAVERSE
()PERATIr~G STEADY DATASET JULIAN STATE TRAVERSE DATASET PT-IN TT-Hl POINT # SCAN t NA~lE DAY TI~'E SCAN If NAi-1E PSIA oR --
11)70 HR:tHN 1 648 20074701 as 24 22:111 067-995 270747012R 57.32 778.6
2 798 ?00836410S 29 21:39 883-9]1 27083(i412R ,7.42 796.3
3* 1) 0 8 2009756]OS 211 17:07 600-627 ?70975612R 57.3? 779.7
4 366 20J 064910S 21) 10:47 398-4?6 ?7J 0649] 2R 57.37 7R7.11
5 10 201204110S 75 ?O :15 1?- 47 271204112R S7.32 788.3
RAKE PR08E AREA AREA WITED AREA AREA HITED
OplTG VJ-MAHl WTED TOTAL MID-SPAN \.JITED TOTAL ~lID-SPAN POINT LBM/S r"ACH # PT/PT PT/PT MACH # PT/PT PT/PT
1 22.n 0.703 0.0328 0.0100 0.7015 0.0281 0.OOCJ4
? ?3.13 O.7Sr:; 0.0432 0.01?8 0.791 0.0363 0.01?7
3* 74.10 0.896 0.0538 0.0151 0.911 0.0456 O.0~60
4 ?4.28 O.oSf O.066? 0.0200 0. 000 0.0571 0.0]79
5 2/f.37 1.105 0.09110 0.0357 1. ) 06 0.08h8 0.04?8
119
This Page Intentionally Left Blank
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AREA AVG LOSS
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60 EEE Uncooled Rig 43% Reaction Annular Cascade Exit Ps vs. % Span (Area Averaged)
l'::l 986 ~1.~~5 100
<t en :I:
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L
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% SPAN
EEE Uncooled Rlg 43% Reactlon Annular Cascade Deslgn POlnt (Area Averaged)
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t-:: --- -- ::.r 1 DEG 7 !"-- -- -- - -f-: t -I ,:- X 1400
- -- -.-113000 - 0 DEG r .- :=-~ - :=: c- --I -1- - i - I -[ 2175 -- - -.
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% SPAN
C-13 EEE Uncooled Rlg 43% Reactlon Annular Cascade Deslgn POlnt Inlet Pressure
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C-14 EEE Uncoo1ed Rlg 43% Reactlon Annular Cascade Deslgn POlnt Inlet Temperature
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VALUE
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90
MACH NO
703
786
896
100
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%x/bx
C-16 EEE Uncooled Rig 43% Reaction Annular Cascade Mid-Channel Statics - 1.0. (Area Averaged)
136
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- i
o 20 40 60 80 100
%X!BX
C-17 EEE Uncooled Rlg 43% Reactlon Annular Cascade Mld-Channe1 Statlcs - 0.0. (Area Averaged)
137
Ia.. -CI) a..
o PS
20 40
%GAP
60 80 SS
C-18 EEE Uncooled Rlg 43% Reactlon Annular Cascade T.E. Platform Statlcs - 1.0. (Area Averaged)
138
I-0. --(I) 0.
C-19
03
02
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,ilitti!: :ffEf: i:;~ 'Z', ~;l ±Hi '.rf m; "'::h'" -:n.:.+;... tn. ~t!~ljttt ~~l.t!~ "It +-fli::d .,.t.,. ~~.t! !t.+~ ! " .. ! :. .. ~! t~ 1" ~rit -"tit +
:itHm~ t-o~:!tht::J~t1~l !!1i ~'t::"~'1 ·L'"±liti • i ~~H-ti t~tf tl~± ~J! ~~!it t~ itt ~L;: ~~1;1 ff1"L;± t MACH NO
o PS
20
lh iff rrl 'tiHlihllit '
40
%GAP
60 80
o 703
o 786 o 896
~ 986
~1105
100 SS
EEE Uncooled Rig 43% Reactlon Annular Cascade T.E. Platform Statlcs - 0.0. (Area Averaged)
139
I~ (I)
c..
1--- -- -
o 20
MACH NO
o 703
o 786
o 896
6 986
~1105
C-20 EEE Uncooled Rig 43% Reaction Annular Cascade Airfoil Surface Statics 11% Span (Area Averaged)
140
lll. -en Q.
I---- ---I-- --
o 600 1--+---+--+---- f---f-. I __
o 20 40 60 dO 100
%x/bx
C-2l EEE Uncooled Rlg 43% Reaction Annular Cascade Airfoil Surface Statics 50% Span (Area Averaged)
141
le.. -en e..
•• - f..-.. ••
0800
1--'- .. -MACH NO
o 500 "I--+--1 o 703 '. 'I~' ,::~ o 786 o 896
6 986
~1105
f--+----- ." -_. r··· •... f-- ·-l~--J.--+----I----+--4---1~-l-,~ I r'
" ,. '" --~+-+-4·-+-4--~~+-4-~~-+-4~·'~"~' " ' , ~ I:,
" not:l: :j .. : 1;,~ 0400~1--I ....
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~' '1j!' .... ," lIP (M975) ;i' ., , :'1' :;:! ;r; !1:: h: 'I
, •• I
o 20 40 60 80 100
%x/bx
C-22 EEE Uncooled Rig 43% Reaction Annular Cascade Airfoll Surface Statics 89% Span (Area Averaged)
142
C-23
0 CAVITY STATICS
4\ CONCENTRIC PT, TT
0 T E PLATFORM STATICS
0 INLET PT
0 INLET TT
0 EXIT PT RAKES
~ EXIT WEDGE PROBE
0 SURFACE STATICS
0 MID-CHANNEL STATICS
VANE #'S
VIEW LOOKING UPSTREAM
143\ 140"
EEE Uncooled Rig 43% Reactlon Annular Cascade Clrcumferentlal Instrumentatlon Location
143
This Page Intentionally Left Blank
Flgure
0-1
0-2
0-3
0-4
0-5
0-6
0-7
0-8
0-9
0-10
0-11
0-12
0-13
0-14
0-15
APPENDIX 0 - BUILD 3 ANNULAR CASCADE DATA
Tltle
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Loss vs. Mach Number (Area Averaged)
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Loss vs. % Span (Area Averaged)
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Loss vs. % Span (Area Averaged)
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Loss vs. % Span (Area Averaged)
EEE Uncooled Rig BUlld 1 Canted Vane Annular Cascade Loss vs. % Span (Area Averaged)
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Mach Number vs. % Span (Area Averaged)
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade EXlt Ps vs. % Span (Area Averaged)
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Exhaust Case 1.0. Statlc Pressures (Area Averaged)
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Exit Pt vs. % Span (Area Averaged)
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Design POlnt (Area Averaged)
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Oeslgn POlnt Inlet Total Pressure
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Design POlnt Inlet Temperature
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Average Alr Angle vs. % Span (Area Averaged)
EEE Uncooled Rig BUlld 1 Canted Vane Annular Cascade Mld-Channel Statlcs - 1.0. (Area Averaged)
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Mld-Channel Statlcs - 0.0. (Area Averaged)
145
0-16
0-17
0-18
0-19
0-20
0-21
146
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade T.E. Platform Statlcs - 1.0. (Area Averaged)
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade T.E. Platform Statlcs - 0.0. (Area Averaged)
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Alrfoll Surface Statlcs 11% Span (Area Averaged)
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Alrfoll Surface Statlcs 50% Span (Area Averaged)
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Alrfoll Surface Statlcs 89% Span (Area Averaged)
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Clrcumferential Instrumentatlon Locatlon
TABLE 0-1 DATA SU~MARY
EEE RIG-70709-3 ANNULAR CASCADE DATA SUr·1MARY
*DESIGN POINT
STEADY STEADY STEADY STATE STATE STEADY TRAVERSE
OPERATING STEADY DATASET JULIAN STATE TRAVERSE DATASET PT-IN TT-IN POINT If SCAN # NAME DAY TIME SCAN # NA~lE PSIA oR
1979 HR: MIN 1 56f) 2007570l0V 65 07:46 568-596 2707'i7012V 57.51 777.4
2 967 200836410V 65 23:07 969-997 270836412V 57.47 784.3
3* 53 200985610V 59 07:07 3- 31 270985612V 57.37 773.2
4 121 201064910V 61 Ofi:04 123-151 2710611912V 57.47 787.2
5 gOO 201204110V 65 20:19 902-930 271204112V 57.42 792.3
RAKE PROBE AREA AREA ~JITED AREA AREA ~JlTED
OplTG \~-MAIN W'TED TOTAL MID-SPAN WITED TOTAL r~ID-SPAN POINT LBM/S MACH # PT/PT PT/PT ~~ACH # PT/PT PT/PT
1 23.29 0.7]0 0.0303 0.0135 0.712 0.0284 0.0127
2 24.08 0.793 0.0368 0.0167
*3 24.94 0.914 0.0487 0.0203 0.9]1 0.0496 0.0177
4 24.96 1.001 0.0623 0.0242 1.003 0.0588 0.02J3
5 24.q3 1.] 33 0.0744 0.0352
147
This Page Intentionally Left Blank
012
o nl'l
• 002
o 07
0-1
I -.,. ... -- -+-~--+--- t----+---.--+-i r I
08 10 1 1
MN
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Loss vs. Mach Number (Area Averaged)
-VI o
024 MACH NO
EXIT RAKES 0 710
J WEDGE PROBES 0 712
020
016 _____ .J_
--.., I
012 --- -- - --.... -~~i 1 ~
008 --<-----
004 , +--__ -1-_ . \ --- ..- .. __ .. _ -/--- ... --1_
i-1 I
J~ __ , , . --+--"'1 I I ' •
1 ----1-_ - -.
% SPAN
D-2 EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Loss vs.·% Span (Area Averaged)
VI ....
.e: c.. <I
r-~--r-~"--- -r- -,----~-
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---"1 - --1- - --r --- ----
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I - I
o 08 I-~_+_--t_~_r_---+'--~ '--. I
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1 --
t--..,--+--I--! -r-~"""t"i -~ ..l.---~ __ .. . .:. --.-... _-t-. I
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1 I. I • t -' --,---,. t r • • I
! ,-
10
, I I '- I , - .. ------._t_ . l : I
% SPAN
L
: MACH NO I
EXIT RAKES I 0 914
, WEDGE PROBES! 0 911
! i - f -I
90
I __ I • !
I I
D-3 EEE Uncooled Rig Build 1 Canted Vane Annular Cascade Loss vs. % Span (Area Averaged)
.e:. 0.. <I
024 I -+-------- .. ,
j
-'T- - -r ---.- -- f
o 20 t---I---.- -- _..1. --, -- --f
I I
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012
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... __ ----A-o.-________ _
t t L
i I I
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'-+-+-~~"';""~--r-;--' _---l.. I'! .- I :
I
20 30
---- !
40 50 60
% SPAN
- --- - ~---.~--_==:;n_-
---- -------.-'----R:t- . i -
I I
- __________ • __ ~ __ ~_._ I _~ __ ~ __ +
70
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---:..-+---..:.---+~ -: : - - 1.-._ i-. .l.- L , . I I . .
MACH NO
EXIT RAKES 0 1 001
WEDGE PROBES 0 1 003
0-4 EEE Uncooled Rig Build 1 Canted Vane Annular Cascade Loss vs. % Span (Area Averaged)
024 --j- .-.4-- -.... -----------t- --......... _-
-;-------
020 ---... -----..---, ,
I
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e: f I ~ U 12 t-~+_-+_-r---~-
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. -t- - ! "!; i : I ... , : I I o 04 -+-.-+---H.~--t"----- --.---... -- ---, - -+---T--~~-
I I , I -J __ I
10 20 30 40 50
% SPAN
- -+-- -- ... -- -
---- -- .... -- ----
60 70 80
MACH NO
o 710
o 793
-'---,-- o 914
~1 001
~1133
-- i -i-
I , j
, I
.' - j- -- - -1
+ "I
'-, -- l' , t ,.! -- - ;-1
! i I
90 100
D-5 EEE Uncooled Rig BUlld 1 Canted Vane Annular Cascade Loss vs. % Span (Area Averaged)
~. 1 I : I r-f-~ --.-- I j MACH NO
• J -t------!---....----------- _ --------~-- -----..,--- -,-----. _____ -- :""-"t--- 0 710 t i ! I i I 0
1;---+--1- Toft -. - "" • - t - + -, , I --. ,- 793 12 , , l.!:~! ~ ___ ~ 1 _______ ~ ___ ,_____ _. _ _ _ __ ----+--~:....i_-- 0 914
J ,I 1 .~ : /\ i-- --. -1- -Ii' , l' . " j ~ 1 001
~ ~ I +-+--,--.+--:..------ -----~-- --=f- ---- ~- .--t-~ -- ~ 1 133
:-.~ - -- --1- 1- - - I - ; 1 -t -- --]
llf + .'! ~ ~+---i-- ~ --- ----- -.-- -- .--'--------- - --- -.--~---~~--- ' I i-7-, f_-. rr- - - t -+i'!..:' - -, - . - - ---,
- ~- -+ "" __ :.. ___ ~ _______ L __ -.----- -- _..l-.. ____ 1 I -r--,--t----+--~+_I- ~ , 1 " : I : -~f--+-- - -'I -, .' : ~ ; 1 ,- \- i ~ -, -.. _- 11
1 • 1 ", , I I I' 1 0 r~ -~----.----------~___r_-- -~--- - ------, .-+--+- 1
r~'i-;~F-~-t- -<>1-- ~I ~; : . '~;'; :; LN -'--~--~ t- :-~ . r.-,;;.. : ' ' "" "'"""'- .. 'A" I I I -'.~, . , j
,H-h-~ t --~:-~-11 I IV: !--;:~-:----; 1'; -. ~-.. -:..-i·--i-.1-.. _f-~.J 1 til i I r- ~~, ;~, • I'
091 I: I' I --+- i I 'I J 1 i NL--: :, ..... "': I ':-+ -r-:. -. -j -::",1 i t - 4 ; i -, - : J !I ,- -~ -j i- " • -l - -;.. !........ A ....... ,1-+---I--""';'--i f t .p-:- -i.-I. ---1----L_-t ___ ~_--!-~_ ¥"'J I
:. • ~ ..... i-~ --~ - !"'"'It T 11t-J-
1' "~r":J. 1 J ~ - ' ; j -l.-- t : .. t-:~~ -+- -+- --~ -r i~::
l 1 - J I I ' I ,'l.:.1 ......r"'i 1 • I' i .~ ..... , -1 ' " o 8 I. ' ....... -..., ---;-~'f-'-L~1oo::~±:_-+_r_....;...."""7_t_f_1f_'_F--;....::Ioo.j(,...~_+__t_1r_:_f__i
lLL ~~~,- -- ; .. J I, 1,1 - - 1-, -1- ,- + '- l-~~ - - ~- 1. ,~- --- c-L_~--r-:'- -i~: f ,_ I ' I ~ t 0( J:J. ' I,.... ):' : ~~~, ' 1 .j -: 1 _~ I'. j • 1 1 'I I - ~ I.("'\. I ' ! I ,~, j '; . 'l~":-fE-l.........r--+--;--1--- -,'-'- 1 I i rv r- ~--~l -, --;-·----,--t- ;--1- +.~-~ .:,--;' ~.; r -::c I! i;, I~' l-........n ' I.ti-'" ,-..,L ! 1
% SPAN
0-6 EEE Uncooled Rig Build 1 Canted Vane Annular Cascade Mach Number vs. % Span (Area Averaged)
'J
80
70
<C CI
r-l ~ 60 l-X w
50
40
30 o 10
D-7
';f:m~ '. j '~lf:H 'l;,.:. '1' ',j IU 'r t: ~t: I,':~ f,', t, ~:. 'I· f~ ~::, i!ft;1 !!!H:: k~' ~::: 't~'!,Fl':' , .; F:[": jtI:':;: 1:;-.:.: r:, ,::,F:--:tu
t;: 1' •• ;" -.::;IJ: :;':\'1 '; --.::L:. m;:" ':::1:::\:,:..: ~:'i;'t ::: rot' I~.H :!' J' ';.,' ."'j::: ...i: ~~ [E.;:, ," :1,,~ :~j'::j ,;:~
:: ;l1F.r-t~i= ~ I;:;" ': - I 710
L.:." '; [Eo i,: -1 :;': r':: ''';: I=i '" I! :- ~t':: I':' I", "I:!.,h
:;!~~ 1'\ ' .. ';07931 " :~, I," .• '.,1' .::: ' ,H~!' I'" r~: .'!~ 'f:
20
~:f f:;? ':I~: t::: ''';" f-.:" ,'! l':, t'· .. ,'1 ':t.
,~~:J;'~:q'i':;'·f~':"~I~~F.::~ ~:·::0:,.,J ~
ft :::;r:I: IE ~E 'f;~~ ~~ ':~1 ~2.!4"~ ,.c,'
It ',it : :a,..%;: c::: 1 ",.:..i·: :;' :l:rt
f:;~:! ~:; &~: :;:""I:!~ 0~ • .:ihf " t' .:-:, ",:
,'" 1::: :~ it;; E:' :::j 1 001 ~ :.
,:1:~;r::·t!rrr.::" :::: :.:.r ~t F~ 1:':-,1:;;; Ii]. ;::: It;:.' ~ ~" .' :11 fmi 1:+:::::-
r; t' r.;:;l: f:I!, !~ .: ~ ,-:~ $ F lilt;~ H:
[Jnlf!;,.l·;, tr~:lf- [..!.:t'" ~~1 133
30
j •. t'.; rr:: t:- :: r;:- f,f- . .1: ::; 't; ~" ~r:'l .-;:::
t! ,I:: I I~: I,~t ::Eb :; ::: J; ~':. •.. .: r·: I' :.![:;:
40 50
% SPAN
60 70 80
EEE Uncooled Rig Build 1 Canted Vane Annular Cascade Exit Ps vs. % Span (Area Averaged)
90
MACH NO
o 710
o 793 o 914
61001
~ 1.133
100
<t CI
~ en
Q.
t: x w
90 . :H: I " 1: t ... '1"
_ _ ..... _ .... ~. --4-- '" t : ' ~~ 1 '"
''1,:'' f- .. -
~ at t:~ .. ,
80 ;; ~':! +1 "·t'
o ' ~
:.1
t---+-~--.-- .... --
.. "
-+- pt:=k' wi'
.,..... 70.~ -1 1· rrr~t i'
r'r ih.l.1;t ·tt ._tj-·tt-t.t-t,~-t·· ··t· I M
rJ E[ -tlEL:et.r!t-f--t--+.-~ .. -t I I' L' • ,':" t-t- -ok --- -.~~. -... --r·' .- ._ .. - "'r~ ,.: • -+,
60~ .1 ... -. r-~~~ . _.~-:::D~Y' ~p~~f'~-;~~r-~ I lI\ tv . ~~ .
_. _ .. "3 f\- L lir~~,,:~-v~ ~~ _ .. ' .... fA: ~~i'~-50~ ~!\ w . ~ , . t-- - r-' _.,- ~ t~r"\ ... :-- --,-- _. f- - •. t;... .- r- _.. '. ,: . ~ .... -,--
" p 1\ L_._ ... ~ .. +j _ _ .. \. .. ___ . ~ __ .. . _. . II I.L -~.\ N~ .-~Kfl.
4011
\ ~ \ r- . Ir-f- --..... f-- .-. i£(L -. _. - ~--\ --7 -~~, -~- ...
II " f-.. -- ..... - -- _.f-.. -f-- -- _ ... , f-••••• f-.•. -~ -. '-r--: '~I:-"'-~-30 l , f I ,
f-+.-+-+--'j--+-+ .. +-.t-.4 ~-.- t_. -+~+--:l-:"+--+ -l-~--+~HH7:-• 1 • ~ ,.",. t. I., ttt It', "t
20tt=t1-t--t-tG-j'-t1·-t·I I I :t7 t1-j tt-tf.} .. } ]n:i
. !t::Jil:ii
•• ,. II'. d.
Ii ..
. 'J . ~ I " ++t ,
;:t: .,: .. ~r.: , > tl'! t If :+' ~ 0' t; t +: t!:~ :!d t.., i::! ·:.i fl!ll :1 I +. • I.. ~. • +. • ~. I • f
:"', t t, fl.. : I I:. : : .' ,1 H1: r ;. t :11 OJ: !"f t • H! tr+ ~'~f :pf ;'ttl!±ll .! t j' . ~ .• . tI f f' • f t j , 1 !;.t' , • l tlU • t .. , H rtI. l:L Ii f1
10 H ",: .. :." l ., .~:' • :: ~~ ,: !t, ::'.:, to: t t"': t ...... :/. :- tt : , .'" 'to "II .:111;,1' ,t'" , .p.::, .. , d I e' ,HI .. ·, . ii' Iii ttl. t • h • ·t" , .• ::::.lI1t· I t 't' '~;! '.:. if. I:t ::i~ Tr: ft;t !ll, !'~ Ht! ttt It·: Plr Hi: lir; :Hi fjl, tJ;! i :iifilf '<1: li 1!n q Ii: :;~!!m:;pi iF H I" 1 t!
tl; I I' I it· It n' lIl' tt·tt rmrp1 t" .f." • Ph1; iHi tt ttl r~ 11 ~ !if! tr·u"! ~1i1~l;r .l~ttti 1 t •
o It !lit ~Httl :m . IUft iii!: ! ;t~fP Ii!: m T 023 4 5
AXIAL· VTE ON.)
0-8 EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Exhaust Case 1.0. Static Pressures (Area Averaged)
156
I-0.. l-X w
.... - ~ .... - ... .. ... - - ...
. i I
i ! 1 1 j
~~~~ •..• ::~:.:.. '; 1 1 . -~ -;;;':.::. --: b i ·1 . i
'. -:- tt:t:::~;;:: .~ .- 1 ·.f ~ :~ ::~ ;::.: '. J.- J
- . _ ~~:7~ ,:-. 1;:-~· r~ _' , " _ -~ _. '_-F!-::-Z:,. :--. - .;-.:.r -! i:::!:F-";F _ _;;, J;8,= £' L
'Hl -_. "! E=' :-:::n:: :J:, ~ -r . :;"!:f:~..:" ~: E=- - - _. -, . :-..!~;: ~-:1-" '~~fri: :: t·: :'1: -'-~i ~: :-. '::V'::: ._-
10 20 30 40 50 60
% SPAN
MACH NO
.j
i _ -I . \: .'.: -:-~ ;: ;: .~' ~
i·' f _ •• ~I·.'::: .:.=:i1. ::'. f! . ;-_ !.~: _-::E:::£~::+.-: . ~ . _:. ::. _f..: ~~ 3! :. ~ ..
.. .. .' ;:,-: :.:: ttl .t:=::1 t::.: .:
70 80 90 100
0-9 EEE Uncooled Rig Build 1 Canted Vane Annular Cascade Exit Pt vs. % Span (Area Averaged)
...... VI 00
% SPAN
D-10 EEE Uncoo1ed Rlg BU11d 1 Canted Vane Annular Cascade Deslgn POlnt (Area Averaged)
(I) w a: :::l (I) (I) w a: Q.
116 000
115 000
114 000
113 000
0-11
90 a DEG
140 a DEG
217 5 DEG
% SPAN
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Oeslgn Point Inlet Total Pressure
VALUE
116780
..... 0\ o
u:: C!:J w 9. CI) c.. 2 w I-
327000 -:-~ ~: If :.~ I~.' -'4 ._ '1" ~r~r rr ri I r- - 0 450DEG ,~SPAN VALUE
.~ _ .41;'~ : ~ .. ~ ~ ~' ~tl -- -b-~t+- -' -i~-t=~ +x 1237 DEG ~ ~ :~~ ~ :~~: ~:: ;~~ , r", -;I. ,'~h~ I I t 1690 DEG I I I I
323000 ,,',, :,;':' 'f , -I·-,-trt~-'~f--I-M, :--_--0 2002DEG -'-,r-.-l'-.. - -+-r--4-......... ...,...j
,~ ,1;~1 ~-~.'~ '-. '-Ir-, - t I I' 0 2437 DEG - - •• : :
• ~ I 1'" t - : 'n ~ .. f.1 - -, r -, :'-' L..l ..., I j.. . r - - "T
'n i " , I ,I .- • Ii- - - I A 2690 DEG - '71-- H---t-..f-.+--+- --c-
i'I'" ' , ,oJ, ' , ..... 3112 DEG ," 1 ' 319000 , 1.111~Ji: '," :,,' !i::, ", , -t ~f- i-. -q-: T 'j-4--tt:, M-+-+-+~!
. +~~ ii~ ;rr'-: 'r~· ;- ri'~;" '! ,r., ~'--, - l .,:~: ~ 3565 DEG + [. --. ~ ,' •• -~., ,1' r.,.' ,", I, , , •• f- •.• •• . .~ _1.....- f-- _' 'I'
315000
311 000
307000
. ," ' 'I, " 'i' ,II "--rft!t-: ",f] iif .... 1..._ ,j r" " ... t!- ~ - ~~ ,- "Ttl'
l'l'!!; 111 111;1.1 11 ,I j,', I "~ I I " """ :',:11
" " '" T --, 'I: 'I' ,~ '~r ~rr 'Iy-~:'.c 1 , ,,,. -~ I -r--,. ..... - ~~,'., ' , ,I; i ~ " : ..!:..~:- 'r -...: i ~ '1:"
" ",' ',": ,," , , ' , jl' I ~ , - T ;'n 1'1; ,II: ",' '-~ ~- ' _ •• rr'_ T --,- r r ,. I' -I~~ 'T~t\~::; -:%:T~
-: :;: ri; nil ,""" ,,:.t.!LW;11·'/ r:" -;, ~ ", - J:~ -', tt,'f: +",~li :11, .I:, :~, 1 jl+,,":~ :;r--~b. ~ :- !." 1, (, ! 111t','I;I, ,I o! Il:'1! I II!: II"! 11 "jt I I I III I ! I~ II
I !" J ,"""" , I ' , 1--- ,,, "" ,," "I ,,' " ,-,.,. .4 I, : ',I!rt' 1.1 m": ':', :',' ,I', : I'" I' 'I'" I' "iliff !ili' ~'!i ~I f' ", i" , '-'
-l,t ':~, -111T I 11,1 :,..J..l M T[ry.j.J- '''i f-I . -' t , -- r 'It r 1t1T! • I ., ". f- --'" ",' -., -- t.+" .... -~ "I , "" I,': " , ','1' Ii'! '1'1 ' 'I! I I" I" ", " " I I' " I' I II ,I"'" I I' I"'" "I ! I r il !l111 I I I I t.', I 'I I I I I -d ... --t l 1'1,1\' rt-",~I' I I
" I':, '~' 'II !,II!P: ":! B't 'II ! 4'~ TIil: ;!'j'!i, ,:I,I~',' 1 ,r "I, :!I, 'iij [I:i ; I , I! ,+'" ': 'i' I", i.l: I: _ ~'._' ~', f'j't! ,'t_1L • 1rM~ .~. 11 ~cU';';tt 'It''~1 ' .- In,'-m-mr" ·t ri·r---''''''- - I li;T'i:1 ','Ii!;1I1 :1"'1' 1,1 ,:',i!1 :,",, I "i,' ~~,: "i""":1 ;':[I'I,;liU: I"'" I" , !'II'! 'Ii': ',I"
,,1\: ::1\ !. Wilti jli, \]11 !ll; I,' :,jllP' ':' i!! !,'" ,'I"",' ':' ~ 1;1 m;ll' Ii" i""!. ',I', 'I 'II' 'I "" "I','" \ , 'II '\:, " t'l' r'-H tH "'I ill [, , .~ '1Itt, 't!if+i r, , F '-," ,-:-. ~ i-+i.p ,1+ ++I~;'.:..tt 111 '1 ~~i!':, ."',,,'! 'ttl I r I' I ~ (I II! I II i ! 1 I; Ii! i. 1 I,' I' : i III 11 I I II : Jill t I I 1 • ' I II, I I :: ! I II I 1.1 I!I ! 'I I I I I ' + tI I I I I I I , , II ,
303000 --+~~+~~~~~~~~~~~f--~~~~Mh'~~ I, ' Ii Ii "I 'J: tiP "IIJ!lli I, IIi' liG II' :; ! I ',;1 ,Ii' .' c '" :, !: I! jill, , 11" " i, ~ ",', I II,,'!, :';, " !! I ,: ,:: ,
I. ~. ·11i t 11' 1f+,· II" + -- In m ... ,'1 - • or. 'rtt '11 -- n'" " +.~ 'r - ,- _.j -. '-;-. r -rt' I';' • ..: '" " Iii' 'II Ii! Ii., iii It I!i I :,' ::' 1.1 ", 'I' '" 'I' ,Iii 'I ',II :: II !,' ': " " : I " il,!
I, "jill I"" ,t 11'1 ''I' II' :, ,',: ,ti' " 1 ' I I '! ,'\ , ,'I -~ ,'" -'-~~Ti' I -, 'J' ~T ,;1, ~1' II j' I I I I, I ,', .. 1 I" I, "" I 'j • ',,:" r:' t;11 ,-.~ ~ - --.., - -' ,.- ,,- ". -,. - .. - I
I " ,'I II: I ';' II! II : I' 'I I I, 1 I t I I I 1;' 299000 ----+ +. T-,:+' -,tt~';""'_"l ~:...- -••• ,.----1-
1---- --:-~~ - ..-- ' , - -1'
"I! • ""':f I,', ,:'1' , I', ' : t" I',,' •. J' l' H r - I' , " -- ',- I I " r I I - I ,
:' I ,i'", "" ," "', ' I 'j I I ~ , 'j' L I -,~-~Inr- -, -, " -i- -r .. ~-·t :-. -- 1-:-1-- _, ______ ,_L -I ,- -[ , t ,,' " ' I I \; I : t i ji,' I I I j I j
295000L-~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~--~~~~~~~~
00
0-12
'J
20000 40000 60000 80000
% SPAN
EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Deslgn POlnt Inlet Temperature
100000
0\
0-13
% SPAN
EEE Uncooled Rig Build 1 Canted Vane Annular Cascade Average Air Angle vs. % Span (Area Averaged)
162
10,
09'
08
07
01
t Itt
1 ~ .;. , $ I) -~ i-i ' ! _ 4 <0 ~ -, ,
t ,
a 20 40 60
%x/bx
I I
t ,-I I I - .. i
t j
, -
o Q
o
,-. l
. ,
80
MACH NO
o 710
o 793
o 914
D. 1001
~ 1133
- .1
j -l
,
o 00 1
0 8 ,0
100
0-14 EEE Uncoo1ed Rig Build 1 Canted Vane Annular Cascade Mld-Channe1 Statics - 1.0. (Area Averaged)
l.e:: CI) 0-
l CI) 0-...I W Z :2 <t ::I: U 6 :§
07
06
05
04
03
-l i I
I . i -r 1- -
1
I II
%x/bx
0-15 EEE Uncooled Rig BUlld 1 Canted Vane Annular Cascade Mid-Channel Statics - 0.0. (Area Averaged)
163
164
le.. -~
0-16
o PS
20 40
%GAP
60 80 100 SS
EEE Uncooled Rig Build 1 Canted Vane Annular Cascade T.E. Platform Statics - 1.0. (Area Averaged)
Ia. ---CI) a.
i - ~ .... - f--- .. ~----- ......... - +-- .. -- .-. ---+-+-+--if--ir--t-+-:.+-~" h-:- MACH NO
710 ! t
20 40 60
%GAP
..... p 0
80
793
914
1001
1 133
100 SS
0-17 EEE Uncooled Rlg Build 1 Canted Vane Annular Cascade T.E. Platform Statics - 0.0. (Area Averaged)
165
l.e:. en
c..
I MACH NO
1 ! !I 0 710
I 'Ir i ."~r-- . 100 793 Ir:~~-·~-·· . - - - .1 •• , r 'J ' ---! .,~ l 914
-,~.-- ~N~--r -- -.~- .- -t--- --~- - ~ e: ~~: ~ I 1 ~-DENTON
09001--__ ....... ; --~:_ __ Nl.l . ___ ~- _ .. _. +--.-t-,~-.. ~_. ----Ir--t--~....,;tH--t--r--I '\ 1 i :.4 \ .
1000
-- -t -..ll~·· ,-- --:" .- -: ~~-\J~-lil.-~- L--~-. tp. I I I t1 ' ' 'I L
06001-_-""';. ('-_ -+ __ --+-;-+--.+-1 t --+---~--t- •.. _: ____ -.-i _~ty+' JD ~~.f~ .. ~t}._ I I ! r\ ..J
%x/bx
D-18 EEE Uncooled Rig BUlld 1 Canted Vane Annular Cascade Alrfoll Surface Statlcs 11% Span (Area Averaged)
166
l.e:. CI)
c..
0800 1
'I
li1 Hi [1 HihU ti o .lUU ,,~= ill
o 20 40
\ ..... '0 :::: ,i'11:;;:;1; :11::' ~;l)U
"r~ I~ !h:';' ~ .. ~ li;lr\::{~;:!r. :i:!TI
It il 100
%x/bx
0-19 EEE Uncooled Rig Build 1 Canted Vane Annular Cascade Airfoil Surface Statics 50% Span (Area Averaged)
167
%x/bx
D-20 EEE Uncooled Rlg Build 1 Canted Vane Annular Cascade Airfoll Surface Statics 89% Span (Area Averaged)
168
o INLET PT RAKES
o INLET TT RAKES o EXIT PT RAKES
6. EXIT PT. AA WEDGE PROBES o T E PLATFORM STATICS o SURFACE STATICS
o MID-CHANNEL STATICS
o CAVITY STATICS
25°
/ 234°
14340
\.
~ 140°
0-21 EEE Uncooled Rlg BUlld 1 Canted Vane Annular Cascade Clrcumferentlal Instrumentatlon Locatlon
169
This Page Intentionally Left Blank
Figure
E-l
E-2
E-3
E-4
E-5
E-6
E-7
E-8
E-9
E-lO
E-11
E-12
E-13
E-14
E-15
APPENDIX E - BUILD 1 ROTATING RIG DATA
Title
EEE Uncooled Rlg 36% Reactlon Rotatlng Rlg Efficiency vs. Pressure Ratlo (Area Averaged)
EEE Uncooled Rlg 36% Reactlon Rotatlng Rlg Efflciency vs. Speed Parameter (Area Averaged)
EEE Uncooled Rlg 36% Reaction Rotatlng Rlg Efflclency vs. Mean Veloclty Ratlo (Area Averaged)
EEE Uncooled Rig 36% Reactlon Rotating Rlg Reaction vs. Pressure Ratlo
EEE Uncooled Rlg 36% Reactlon Rotatlng Rlg Inlet Temperature vs. Span
EEE Uncooled Rlg 36% Reactlon Rotating Rlg Inlet Pressure vs. Span
EEE Uncooled Rlg 36% Reactlon Rotatlng Rlg Inlet Temperture Contours
EEE Uncooled Rlg 36% Reactlon Rotating Rlg EXlt Temperture vs. Span
EEE Uncooled Rlg 36% Reactlon Rotatlng Rig EXlt Pressures vs. Span
EEE Uncooled Rlg 36% Reactlon Rotatlng Rlg Area Averaged Spanwlse Efflclency
EEE Uncooled Rlg 36% Reactlon Rotatlng Rlg EXlt Alr Angle vs. % Span at Circ. = 155.2 degrees
EEE Uncooled Rig 36% Reactlon Rotatlng Rlg EXlt Alr Angle vs. % Span at N sq. rt. T = 350
EEE Uncooled Rlg 36% Reactlon Rotatlng Rlg EXlt Air Angle vs. % Span at N sq. rt. T = 350
EEE Uncooled Rlg 36% Reactlon Rotatlng Rlg EXlt Air Angle vs. % Span at N sq. rt. T = 280
EEE Uncooled Rlg 36% Reactlon Rotatlng Rlg 11% Span Vane Surface Statlcs
171
E-16
E-17
E-18
E-19
E-20
E-21
E-22
E-23
172
EEE Uncoo1ed Rlg 36% Reactlon Rotatlng Rlg 50% Span Vane Surface Statics
EEE Uncoo1ed Rlg 36% Reactlon Rotating Rig 89% Span Vane Surface Statlcs
EEE Uncoo1ed Rlg 36% Reactlon Rotatlng Rlg Mld Gap 0.0. Statlcs vs. % x/bx
EEE Uncoo1ed Rlg 36% Reactlon Rotatlng Rlg Mld GaPO.D. Statlcs vs. % x/bx
EEE Uncooled Rlg 36% Reactlon Rotatlng Rlg 1.0. Platfo rm Ps vs. % Gap
EEE Uncoo1ed Rlg 36% Reactlon Rotatlng Rlg 0.0. P1atfo rm Ps vs. % Gap
EEE Uncooled Rlg 36% Reactlon Rotatlng Rlg Vane EXlt C av vs. % Span
EEE Uncoo1ed Rlg 36% Reactlon Rotatlng Rlg Vane Blade EXlt Cavlty Statlc vs. % Span
*DESIGN POINT
STEADY STEADY STATE STATE SCAN DATA SET N7 NAME
-"-'--"--
134
*101
276
419
562
* 24
774
330
165
746
888
316
352
388
603503520
603504120
603504620
603505020
603505520
603444120
603414120
603424120
603434120
602804120
602804620
603503020
603502320
607452920
STEADY
TA8LE E-1 DATA SUl~MARY
EEE RIG-70709-1 ROTATING RIG DATA SUNr1ARY
STATE STEADY JULIAN STATE
TRAVERSE TRAVERSE SCAN DATA SET
PT IN PSIA
TT IN oR
N RP~'
WMAIN LBM/ WCOOL
DAY TIME N2,s NAME .;..;;...;....::....-- SEC LBM/SEC
HR:mN: 1978 SEC
310 16.16'48 136 164 873503524N 57.43 769.93 9801. 23.45
293 12'40:16 313 341 873504124N 57.48 770.26 9737 23.45
299 22:54'25 279 307 873504624N 57.31 778.44 9814 23.26
300 6:41:45 421 449 873505024N 57.53 772.74 9709 23.43
300 17:37:36 564 592 873505524N 57.37 782.02 7818 23.25
307
307
307
307
306
306
311
311
311
8:09:49 26 54 873444124N 57.24 766.64 9819 23.40
17'50'04 278 306 873414174N 57.39 775.83 9733 23.31 0.090
20:15'45 335 363 873424124N 57.37 772.03 9754 23.37 0.180
13:19:34 182 210 873434124N 57.45 775.96 ~'8l? 23.34 0.277
14:21'45 748 776 872804124N 57.31 772.54 7880 23.37
20:28'48 890 918 872804624N 57.44 772.48 7779 23.42
0:28:43 318 346 873503074N 57.38 771.45 9804 23.38
1:49:03 3~4 382 873502524N 57.57 771.24 9750 23.38
3:59:39 390 418 872452920N 57.50 768.20 6873 23.50
% PRES-
COR-RECT
AVG. ED WCOOL REAC- VR N/ SURE AREA CLR AREA ~ TION MEAN !rIu RATIO WGT'D INCHES WGT'D
0.386
0.770
1.189
0.2845 0.5959 353.2 3.531 90.40 0.0136 90.31
0.3290 0.5631 350.8 4.184 90.19 0.0131 90.06
0.3606 0.5487 351.7 4.707 89.36 0.0131 89.23
0.3792 0.5371 349.3 5.179 88.17 0.0141 88.12
0.4000 0.5308 351.1 5.773 86.86 0.0141 86.81
0.3308 0.5656 354.6 4.178 90.15 0.0131 90.02
0.5623 349.4 4.208 89.77 0.0156 89.84
0.5642 351.1 4.209 89.60 0.0166 89.75
0.5675 352.2 2.239 88.93 0.0181 89.20
0.3412 0.4699 283.5 4.010 86.86 0.0191 87.21
0.3779 0.4530 279.9 4.514 85.24 0.191 85.59
0.2404 0.6317 352.9 2.959 91.20
0.2167 0.6783 351.1 2.574 87.87 0.0116 87.63
0.2472 0.4704 248.0 2.919 81.19 0.0206 81.66
This Page Intentionally Left Blank
92-"---""'--~-~--------- -- - ----- - -! I , ,
--,..------ ---- ----r--~-.-~-r----:l . --r-- -, - . . I--+-~-+---""""------------ -:-.----
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90~4_~_4----4_---
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I' I I ...... --..: . - ---t : ~ ...... ~-I • _ --t--l
86
386
770
1 189
-+-- -- ----1- ~- -~- - -- -l- -- --t- ~ --t---- t--- __ - L .--82~+_~~_+_4~:~}-~,~,~~+1_4'--~---il---, -t1~'--tr---i----r---1--~T
---1-- . -- ____ L _____ L __ J --.- i--- --1- -- L .--
E-l
t ( , iI' : I i I I i
PRESSURE RATIO
EEE Uncooled Rig 36% Reaction Rotatlng Rlg Efflciency vs. Pressure Ratlo (Area Averaged)
0 350
0 280
0 350
~ 350
~ 350
I
!
!
I
.:: '!~ 7!':,";+' .:' .. :, ,:f c' j.;... I.... -
88 i~·~ ~.'1;';.,~, .;;.~~ t: 'g r', IR~, r::, :: •
5:J:;.i '?';~' -,:~'i:~ , 86 .= , .. :-.j' ........ ' , ,
6·il .. , s':;~ ,," " ..... ... ~ ..
... • 0-........ ....
J I
1.. , I
~ ff' ;=-': !!: ' " .: :::- :' :'i- , tlr':: '=-, :!!..., -,' ',I:, "
, "; :::- ~.:~ ';~. ,-: : ~ .{
. j
: .. , rtF ~tg't! ,,;- .:: J~: t:: -,.' • :t 'I •• + .. ~.~::..~:~ ~E. :~ :,!
82
80 280 290 300 310
i
320
I , I f '. ,r',
f- ' ! !
.. __ ....... 4
.:" t..:' • .. t t ..
II"!' .r .~, ~I~ ';1' .: - ,':, I :f"'" _ '1~'::£~ ...........-~ .. , _'" ... .. ~ 0.- .. ......i-.j... ......
. i ,! ' 1 i f
'I 1 !, 'I 'j
l ' t
.. ~ I
I
1
t -
330 340
N/VT-r
1 r' T: '," ,1: ":::'.: ;h:fo!E e: 'I _ i 'i~":, ~~~.::, 'I1i J: :;,' ;;
. l. , I
i -
. - :::f~
,-,',:-jf';
350
%Wc/Wm
386
770
1 189
360
PR
0 35
0 41
0 46
~ 50
~ 55
D 41
0 41
0 41
PREDICTED
370
E-2 EEE Uncooled Rig 36% Reactlon Rotating Rig Efflclency vs. Speed Parameter (Area Averaged)
"
I ,1 I I' Iii I I I I I I 'I; ~ I" . 1·':' . t ~1
88 .i
.-.. I , t--' J~ ~ I r." I ll!S - -1 : _;- ~l I"--~~--+-----r--+---+--r----+---'- -.- ---L-l-+- ·-l-l·--+T---..--t.--1--+-......... -+---+---1-~-l-.-4-':....+--+-.:..;.-.;l. j _.': : ! _ - 1 1 :./" _;, I • I. ! -- t i· -. --;1
86 _-- - t T. -t • I _ ~ I l % W IW _ i'-, - -!. .', L If". Y" -+--f--,--+--+--r--j-";""+-__ +--;--+-+-+-Ti '+-+-i' _ 0 c m
~_-,~E~:~_~-1~;~:-~:·~!~--~1-4-+1-~~~V'-+-- t !!! 1 \'1
84 : .. _ '. i:. -. !l ~' :'. __ - _. , -!II _-t i
, , ,
80 ~ ~&::~-~.::::: ::$~: ':--. L:" t - <t:' '- J --o~..; .( o 40 0 42 0 44 0 46 0 48 0 50 052 054
VR MEAN
056
E-3 EEE Uncooled Rlg 36% Reaction Rotating Rig Efficlency vs. Mean Velocity Ratio (Area Averaged)
386
770
1 189
058
PR
O~ 041
046 650
~ 55
D 41
041
041
060
--...l 00
z o Ic.J <t w a::
..:
036! t _ ------t' -: --1.1 -- j.-~--~--' 1~' t IV ~r-~~E-+-' --~-; -i--~+---+-+-t--+l_-.+--~; I l I 'i !, I' I I,' I
032, J I ! .1', -- 1,--'-'_ '--J. I I : ,'j t, I II
.:1 -! ,--'- I -.- -----r·--- I I ! / ' ! i 1· "j: '"1-: .... -~.. .. I .. ~J._ .. _L._ L.L.J{~-t-+'-+-+-!4-4--t-~i +--It----:r-i-t-:-f" i-I-rt-:-~±l'='::!::::=-±:-;:::-i:::::;:;: ~:Hr::' . 1\ I I ' I: j 1 i! I r t L -' N/../f
o 30 ~ .. 1 I It.. . I' I _ Itt I I t 1. , .- 0 J.!:._~;-;1-4f._-"':I--+--+J--:+-+: -+--+-1 --t -.. _. II : Ii. til . 1 _ ." -: 350
::: . -.! i ! I t _:..J!_-+_f -+.~:r--t......J--i"-+---rt ---r-"~ :'j ... }. _ 0 280 028J.;a;;:'.:I-=·;~'~~~-.1J-_--+--~j-+-+-!f-1Ir--+; E -r 1 ',I _I 1. I I. I ::,1 -, i-L.f':':!tt:r:- ..
20 25 30 35 40 45 50 55 60
PRESSURE RATIO
E-4 EEE Uncooled Rlg 36% Reactlon Rotating Rig Reaction vs. Pressure Ratio
'.
u: d w C
CI) c.. ~ w I-I-w ...J 2
..,
10/23/78 21 06 35
AVERAGE - 310 523 DELETED POINTS
o 45 a DEG CIRC SPAN VALUE
+ 90 a DEG 200 2 67 09 367 160
X 1237 DEG I I I·; -! 0 169 a DEG I '- ~ -: ~ 1
,~:~~~:~ t-1::~~1 I .; : 1 ,,' ' J~2690DEG, i'-)~"t-:1
I I : X 356 5 DEG - 1 -I - -, 1 " I, 1---:"- l_;
1 :' ',: l-J I 1 " : I I I I I : .-~-=:-=-__ !-~--=--_-:~--""-~ I' --______ ~ I _I I ..- __ ·0 ~ _ --~-~-=:::::::= .. --_ ~ ----. I
_--------=--t<-===-~ .::=:--'--~.:::--~)~-~ I L-~~""~--=---=-. -= ~-.;- ---=:;=-~-:--~~=-=--- ,-I I, I I ,t I - -~ I " I I:' I
1 t--- I ---1 1 i I I I 1 :, I I 1- ,--- '--: -,
1- -; -.- I .- f --I 1 I I I ,I -I --,
-j -1- .. i--I
326 000
322 000
318 000
314 000
310 000
306 000
302 000
298 000
, .1
294 000 -I !. I .-+ ~I 290000L--L~~~~~~ __ ~ _____ L' __ LI~'~~~ __ L-___ -·Jl_-_·J·t_-_-~~· __ jL·_-J~
E-5
a a 20 001) 40 000 60 000 80 000 100 000
PERCENT SPAN
EEE Uncooled Rlg 36% Reactlon Rotatlng Rlg Inlet Temperature vs. Span
..... 00 o
w a: :J en en w a: c.. Iw ..J Z
116000
20000 60000
PERCENT SPAN
1400DEG "
2175DEG
3112DEG
80000
E-6 EEE Uncooled Rlg 36% Reactlon Rotatlng Rlg Inlet Pressure vs. Span
.-00 E-7
3565 DEG
",
DATA - 6035041200
STATION NUMBER 5
STATION 05 INLET
N/.JT = 350 6
PR = 4 096
CURVE CURVE
LABEL
12
13
14
15
16
17
900 DEG
1690 DEG
EEE Uncooled Rlg 36% Reactlon Rotatlng Rlg Inlet Temperture Contours
VALUE
30700000
30800000
30900000
31000000
311 00000
31200000
-00 N
N/.JT PR N/.JT PR
*NO 'S ARE % COOLING 0 353 353 39* D 349 421
115 ~=1'==-t"=tt='1===r==t========t====t==~ 0 351 4 18 77 * 0 351 4 21 =;=i :;:=:;:;:
f-- .-- .• -. [ - ' L. -! _.- 0 351 471 1.19* 0 352 424 -+- L.+.~. , ;!. I I .1 t ;
'i , 6 349 5 18 0 283 401 t 1 ' ! .. ~,t:) --~.. ~.- 1-- I . t -..... ~ 351 577. ___ • _0 279 4 51 1j~':- -I
105 r i ._ 'l ._. _ i-- ._. ! _ 11 __ I .i .... ~~__ J"J. .:"1 _ _ __. ~V7Jt' I:-+:~ . 1 'I ~ ~ 1'V ...... hI:\! ! -.wr-::;; j
% SPAN
E-8 EEE Uncooled Rig 36% Reaction Rotatlng Rig Exit Temperture vs. Span
« C'>
::c
I lX w I-0..
1 ~ , I 1 ....r'\. I *I\IO'S ARE % COOLING N/.jT . i ..rr~' "I
34 1---+_+, -+--+-+--t---"~Jf-";:--!!~-:I~-''---ti ~ , 1 : :! 0 353
1 .. 'l\ 1 • 1 " 0 351 33
---I-, 1
i '" f Y 0 1 • _ 1 ,~ 351 1 ' " 6349
L I
~-+, __ ~I--~I~--+~~~~~~'~--r'~_-+--~~'---Ir--f·--T,---r--~="-~,---32~~~_i~7~9~~I~-~~~~+-~~~~r-+-~~~1r-7!,'--rI' ~351
~ , .... --:- 1 , '. ! 'i Ii, , '. 39*D 349
~==±I==+=~t==~==~=~~==~==j~;'~~~=I~==~==r-==t==t:=+==t==~=~i'--1-1 t~:j~t=~~~-~·~'j:=t~~-~-~~'~~=+~~~=t~I==;~~ 77*() 351 31 ~, 1.1 ...1 i ! I -' ~~' ~--~~' ~-L~I~~---+"~/,'--~~-'~~--+--r'~r-i--+--r' 1 19*() 352
I : . I /. _ f\ \ I I I I 0 283 30~~I--~-+--+--+~+--4,-~~t--'~'~'~'~'~I~~~.~~I--r-~--:i~'~I--+-~ ~279
~~--4--";--~I--+,--+----~1f-r~t-~I--~,---r~~-+--~ ,---T-~ ~
27 .-----":'£f JOf// 1J +-..'.T--L~----- ~_ _:. __ /-::-7.A" ' .-./ I . \, : u
,/ - i k7"l' ! 0 ! ' ! ; --!-.... ,--+i-;~ 24~-J+-J+~1~L~~~,~·-i+-,-i4-~~--r----~,~---~+-~~-,~~-_-+--~I-T-Irl --r,--~,--"I---
u y., I'. , - I=-'" I
1- __ 1
, . fl>:. Lff I" • " --JI.. ~-+,-'--+ v'""7.~--+, --+-~--j/'. .... -:,r---rl--TI--'i--,I'- I '\. ! I ~--
23 ./1 I I .If' -I I I I' , " ---t-L--, ~~I---l _--'+-_ # . - '.L'::f. i 1 -;'\. . / •
22 i I - I, 'i 1 1 1 ' ,:LJ.'..!.~I, ~ - i-J-.+-L ~ - "\ -,I , 1 I j , ~-
I -f f _I - ~: - - t 21 ,.: _ A 1 t I .... I t 1 T -+----t---~ \. f !
. ,_IF; I ~_ -r=r+~~'/--,,---+I_'--jl:--:I_:' - _, _I ;.;., j _ f--r~ f ~ I I. I I ---,-- __ 1 " IT"-( ~-j - / - ,- - 1 1 • , --t- 1 1 ""'-.h.. V --..---,
20 -~I '.'- .1- _ f - -.. I i 1 .. , • i -J---j
8 -t :L 1ft _ . .r ~ v
f-tl t-:.l __ ~ - _ 1 I I - I
I I ,
r .,
I
- I , ~
- I '.i ~-+--+--+~-, J
F~--~~~~'-+'~~f-~'~--·~-~r--r~+-~---~-+--~I---r--~-T~' ~~-~-t.;-i 7 i I:{' t 1 - .1. ~ C I..L I' , a 10 20 30 40 50 60 70 80 90 100
%SPAN
PR
353
418
471
518
577
421
421
424
4 01
451
E-9 EEE Uncooled Rlg 36% Reactlon Rotatlng Rig EXlt Pressures vs. Span
183
.-00 ~
% SPAN
E-10 EEE Uncooled Rig 36% Reaction Rotatlng Rlg Area Averaged Spanwise Efficiency
J
N/.Jf PR
353
418
471
518
577
401
451
en w w a::
" w C ~
W ..J
" Z c:(
a:: :;:
-00 VI
,
80
70
100 ~ i - -r--- N/.JT PR %WclWm I_ I ,
! L-~ ___ ! f-!-.O 350 41 -i 1 I --- 0 350 46 - i i I
, t--'-O 350 50 - r----t-.-1-"'-,6 350 55 t .- : - ii, ,
B~ 350 35 - M-~~ 350 41 - ! : I
, () 280 41 -
to--~,C - . .. t':!l: 280 46
, ' . - I
~D 350 41 39 _ L~~ ! (. .-
~O 350 41 77 ,
I
~. - ! .. )- -r-70 350 41 1 19 ' 'I
90
60
1-' ;'-.~ -f-r--t - "- _ •. - K" ' L I e-'r- -" 1t ;-I~ l\I'h. I I "-..
, , ~l
---,.~ ik ,
50
J. ,I : f--~ ~St t .. :... ! • . i~ h;:::-: ,
t- :~ i
• 't t" f*
I :
• 1 1 i .~ ~~!Ca -" I'~ i' ,
Ei' ~-, ''7 1::"1' :11 "'Ii -
t ._]::. rj • I)t DCfl ,t· • .
~-+ . it •• ~ 'i- ! to--·
1 .' I,' I
kl- I. 1-1 ,,: ~ ! ; j. t .1 .j
40
:~~ t!::'! 30
o fu ~~ ~!~; fml
10 ." lit} !' j .1 20 30 40
')
! ! 1 T r, ! ! J J 1 ! hi. h..1. ,
J- ~~ ~ : 1 I \
1 - 1-- • 1 _ .. t " 1--I I ,
: 1 ,
! I -1' '-1'- ", r-- ~-.
1 ' - i'- -. , -'r-' ,
t-~ I'~- --~~ _. ~ +,_. f-t , ~ , i , , to;'
I I _ .. _ 1-- I
" t&i I
I . ._- - , • i 1 _, I
_ L_~ :--' .- -.. - _. ~ .. '. 'r- --I 'I i - ~=(Elt:.±- c- .:;
W·; ; - )' ~l, l~ ~::-1-] r .u-, T --=- .;:-.
ILt t If{ ill 'j ,. t Oi
I:.CJJ ,..-
'J~. - J fl ~ 1 ,.1,
1\-,"[1 -( lfp4''i:' ~
f f .1 ,'G~ Id '~ I.e;; •• 1 .~~ t!J :'"' ~ I'lli; l t:i~ ~ ,~
J...t: ~ , , ! -'---'-'
, t:: ;r .1 ~ r I
, 1- oGO·:l Q.it t'.
0- f· . ..:.. .. "r-,: " tit I : ! ~.': >
I_i . ' ....... -,- v . 1--
~ ! I' 1:-" I
..a. it; .' : 'r' ~ :'-j -- r-- t " ! " J. ..1 i-
,· .. ·-1 .. ~ I 1 ! . -i
',' 1 -J, I f 1 1 .
R i 1- .: f .' --. 50 60 70 80 90 100
% SPAN
E-ll EEE Uncooled Rig 36% Reaction Rotating Rig Exit Air Angle vs. % Span at eire. = 155.2 degrees
-(Xl
0"1
100
90
80
(I) 70 w w a: t!' w C
~ 60 w -I t!' Z <t a: <i: 50
40
30
~:-!fZ-:=: -- , 1 -1'·1 ~J_ r+ !k:' !-::- " - 1 c-:-::- ',L" , I fI 'I~ ~.
-:" -:" I , j
, i . til I~ .. -.--
~, , ; I : I~ I" -: I 1
~~-:, r' -. j : : : _I
T .,- "_. I
~~ ~--.-: I" I : I ! : -
:.-1--I 1 ; ! ~ If). t :" 'r~
:. -. '!::::: :';
~f2, : -. I : .. ~.
~j l1 i~ Uil ..... ~
~':~ -,: ~-:-I
~<: . . 1 . \1 ; 1'\1 i ,.' .
\I" _.-"-- 'r '0' .... 'Erl": " t._' 1-: f· I ~ j i Lr-
:t:Jr:-~_.;: -::-
,I tI T ! ! I ~ " '\ -~~ ~:t- ,~:
, . :.- , . I 1 ;. ~ ~ ! "
tfu};~ , ~- . ~ ,c:' . I , [J: t: f"r §~~. 1\1 A ~l 16 Q : ,-< l.,~ i-
I,', ,!' 14
~~'i "":, 10: ,. !<.... t ~ !l .~ 1-: [Q :~ 101' , ',' 1'" \-:-
~§: I.J·~ 181:1 ~~ -J
F \,i'; ;t. ,,' :r ,;+ T i ! l -':F", ~-
,
='-Ii ~~:;: 1:ICl -- . ';:: - :-:- . -' :-' 16 II. i. ••
. 1, , .' r! ~ riC it' 1'1 , 1
~~!~ r :- ... )I : , I~ t:f t:: I,,:, '0" :..,:.: :.' ~~. r!~r ~,::, --::
:;c , . : i·" ,i-.:: -!: .!= " i:.
bill :-:-: :;.-, : --:-::-'j,. "='
III r' ~i;' , .
" - , PR CIRC i%WcIWm
:, . ~ 35 r"MI .,...: i,t' " .1·::'
1552 1-':: - -
0 j I'::; tt~:. .- . ~ .
','! - r' .~ 35 3352 r', o 41 . : ~. r:, : " '. 'I :: [.-. ~'; ,' . F.::; t::l~ rft E:',; Fr' !_i: 1552
:::: ._' ); :. [;to! r; I,) - ":': I~ ti:l, I ':' D, ii' . X 41 3352
," :\::' hi'; [:-: i· ;: F::' I~l F H " fY: .... ~t [:~; Ie:, !.:'~;.~ Ri' :-" E.2 h' tit '-:t ~~ E': ttf .- I .. . I,·' :; . t.-:.; -: ,:i,r I", -!: E:~ h-:: 1:: ~ I.:
o 10 20 30 40 50 60 70 80 90 100
% SPAN
E-12 EEE Uncooled Rig 36% Reaction Rotatlng Rig EXlt Alr Angle vs. % Span at N sq. rt. T = 350
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197
This Page Intentionally Left Blank
Flgure
F-l
F-2
F-3
F-4
F-5
F-6
F-7
F-8
F-9
F-10
F-ll
F-12
F-13
F-14
F-15
APPENDIX F - BUILD 2 ROTATING RIG DATA
Title
EEE Uncooled Rlg 43% Reaction Rotating Rlg Efflciency vs. Pressure Ratlo (Area Averaged)
EEE Uncooled Rig 43% Reaction Rotating Rig Efflclency vs. Speed Parameter (Area Averaged)
EEE Uncooled Rlg 43% Reactlon Rotatlng Rig Efflclency vs. Mean Veloclty Ratio (Area Averaged)
EEE Uncooled Rig 43% Reaction Rotating Rlg Reaction vs. Pressure Ratlo (Area Averaged)
EEE Uncooled Rlg 43% Reaction Rotatlng Rig Inlet Temperature vs. Span (Area Averaged)
EEE Uncooled Rlg 43% Reaction Rotatlng Rig Inlet Pressure vs. Span (Area Averaged)
EEE Uncooled Rlg 43% Reactlon Rotating Rig Inlet Temperature Contours
EEE Uncooled Rlg 43% Reaction Rotating Rig EXlt Temperature vs. Span
EEE Uncooled Rlg 43% Reactlon Rotating Rig EXlt Temperature vs. Span
EEE Uncooled Rig 43% Reaction Rotating Rlg EXlt Pressure vs. Span
EEE Uncooled Rig 43% Reaction Rotating Rig Spanwise Efficiency (Area Averaged)
EEE Uncooled Rlg 43% Reaction Rotating Rlg Spanwlse Efficlency (Area Averaged)
EEE Uncooled Rig 43% Reaction Rotating Rig EXlt Air Angle vs. % Span at Circ. = 91.6 degrees
EEE Uncooled Rlg 43% Reaction Rotatlng Rlg EXlt Alr Angle vs. % Span at N/sq.rt. T = 350
EEE Uncooled Rlg 43% Reaction Rotatlng Rlg EXlt Alr Angle vs. % Span at N/sq.rt. T = 375
199
F-lb EEE Uncoole8 q1g 43% React10n Kotat 1 ng R1g Vane Surface Statlcs - 11% Span
F-17 EEE Uncooled ~lg 43% Reactlon Kotat1ng Rlg Vane Surface Statlcs - 50% Span
F-18 EEE Uncooled Rlg 43% React10n Kotatlng R1g Vane Surface Statlcs - 8~% Span
F- b EEE uncooled K1g 43% Reactlon Rotatlng Klg rvj10 Go.p 0.0. Stat1cs VS. % x/Of.. •
F-20 EEE Uncoo 1 ed t-<lg 43% React10n Rotat1ng R1g r~l d Gap 0.0. Stdt1CS VS. % x/tJx
F-2l EEE Uncoolea R1g 43% React10n Rotatlng K1g 1. D. Platform Ps VS. % Gap
F-22 EEE Uncooleo Klg 4310 Reactlon Rotat1ng K1g 0.0. Platform Ps vs. % Gap
F-23 EEE Uncooleo Klg 43% Reactlon Kotatlng Rlg Vane EXlt Cavlty vs. % Span
F-24 EEE Uncooled R1g ~3% Reactlon Rotat1ng R1g Blade EXlt CavHy vs. % Span
F-2~ EEE Uncooled K1g 43% Reactlon Rotat1ng Klg Clrcumter2nt1al Instrumentat10n Locatlon
200
TABLE F-1 EEE RIG-70709-7
ROTATING RIG DATA SUnr~ARY
*DE,)IGN POINT
STEADY STEADY STEADY STATE STATE STEAOY TRAVERSE
OPER'ITING 'iTfADY DATASET JULIAN STATE TRAVER'iE DATA,)ET PT-III TT -IN N POINT f SCAN F NAI'1E DAY TWE SCAN t NAI-lE PSIA oR RPn
78-7fJ HR MIN *<;5 473 60355il120Q 4 17.16 <;]1-519 8735<;4I2ilP 54.47 776.1 a7flQ
7 3'1 fi03'i04fi70Q 3'i5 04'40 36- fi5 87350ilfi2ilP 57.51 772.8 9703
3 177 601505020Q 355 12'02 179-206 87350502ilP 57.il7 7112.8 9798
4 376 fi03'i0'i<;20Q 31)5 70 54 328-35'i 87150r,r,7"Q 57.112 779.1 9796
5 410 603503520Q 11 13 51 il12-440 873'i03'i?4P 57A2 791.5 98iJ6
10 il35 6028141?OQ 356 07 07 437 -4(iil 117281ilI2tlQ 57.51 781 il 78il2
11 'i38 60?fJ04620Q 356 or; 78 <;40-568 8728045e11P 57.51 780 1 7110(j
13 514 6037511120Q 11 21 25 516-'iil3 8737'i1l]2ilP <;7 'i6 715.e 10003
'i7 za] 603574]70Q 10 OIt'ilZ 793-370 R73r,Zil]?4P 57.61 7"0.3 9807
53 635 60353il120Q 3<;6 11 31 637-fi611 R7353il1211Q 57 'il 779.3 01103
OV AVe; C(1RRECTEO OP'TG H-MI\IN H-COOL WCOOL VP N rRES AREA CLR. AREA POINT LBI1!S LBM/S ~n1I\IN REACTION I1EAN TT -IN RATIO WEIGHTED HlCHES WEIGHTED
(%) (%) (~ )
*55 21 94 o 3799 0.5672 3'i1.4 il ]2 qo fi2 0.0]45 90 60 2 C3% 0.11078 0.5517 351 '1 4 fi9 119 44 O.OH5 89 47 1 ?3 110 O.II??] o 'iill] 348 9 5 O'i 118.57 o 0135 88.43 4 23.81 0.4381 0.5354 35].0 5.65 86.80 0.0]1<; llfi.71 <; 23 fi7 0.342] 0.920 3<;0 0 1 5'i 00.32 o 013<; 90.23
10 23.90 0.38<;0 o 4640 280 'i il 03 Rn.fill 0.0705 87 14 11 73.9<; 0.4155 0.il507 279 4 4.(,0 lltl.49 0.Oe05 84.95 13 24. '13 0.3716 o fi039 374.1 4.08 00 87 0.0115 00 67 52 73.73 0.17il 0.733 0.5654 384 8 il .12 P'1.96 0.0165 90.10 <;3 ?1.8'i o 7ao 1. 7'iil 0.5fiCl 3 3<;] 7 il.12 pq (,4 o (JIgS 9lJ. 07
201
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N o IN
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PRESSURE RATIO
EEE Uncooled Rlg 43% Reaction Rotating Rlg Efficiency vs. Pressure Ratlo (Area Averaged)
60
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EEE Uncooled Rig 43% Reaction Rotating Rig Efflciency vs. Mean Velocity Ratlo (Area Averaged)
I' _.
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F-4 EEE Uncooled Rig 43% Reactlon Rotating Rlg Reactlon vs. Pressure Ratio (Area Averaged)
327 OOOr--.,----r---;I--I;--.I.---:-I--_,---:-'-,~I-r--1 .---r--,--- -:nl
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I " 0 --=-1----' --1--- '-_. 675 DEG :-- I '
CIRC SPAN VALUE
118000 __ , __ --t+-.~- .~_ ! ___ : __ ,_. 1 ;'( 1:~~~:~ 675 674,9 1171130 i
:-: -.:- I' .' 10 ~17 5 ~EG i ..' • , •• - I I! .1 .:. _ .J
117000 I ! .._ -,-' - .1,- _-. . I_r-_ ._I_~ ill i I I I I 1 , 1 1 I I I-~ ., 1'- -:. ._! i -; -; I i I' 'C \. !. 1 t -. - I I I
. \.-_. ! j _L --I- _J. - __ L.. .-1- . 1.. ~I:-- .. J~ -J!'-- - 'II - - - _L -! - . -.;. -' t ! j ! i I I I t 1 i "
116.000 +---+--+--+-....---l-:--+--+--:--~'--t--t--,-+-.;-.-1!-+-J--!--+-...!.--.J---<'--t.....:...-+--+-.!--I--,.-+-l.--t--l
t--"~-' +---:-' -+::: ...... ' :-t-~I' ! r- 1-'--'- -l-- _.1- -'TI- -:- -I·· -J--r-+. ~_ ._1- .. L_. --_.' I" t I : I I 1 1 I I I I I I
---- .. --1- I -1-' --I· I -I ·1 I I I I I· I I I ii' 1 115 000 ·t-:-t-t--+--t-+---I:-r-t--i--t--:--t-:~-+-+-t--i-+-~!-+-J--+--+--'--t-:-f-+-f--i
I ...L I I I -!- __ L -+-- _L -"IL '-1- __ L -.~. -i._ ...1_. . .. L _I. .... l' II! ! ! : I 1 I I" I ii'
: -1- j- +- -'i-- -I-"j I \.. -1-' 1 ' J tl-:+I --t-"+-I 1-+\ ~I I~I-t-+-II I 114000~!-+--+--t-+-~~-t-~-t-~~-t-+-t--i-+-~~-+~~-:--~:-f~-t--i-+-~~-+-+-~
----+-' -, +-~- -t- -1'-'+ -1-' -j -;.. -'1,.- -I· j. - ··1· 1-' . - +. -·1·· -I·· -.1' \., i I I :..L _L __ I- _ !- - -t-. -:1-~- --'-- -+- _ i --!-. _1_' -~.- - " ..: :
-- -, --, ·1 1 I I I i I 'I ' I I I,: , ': 113000t--'--t--+--t-+-~!-+-t--i--+-~~'--t---t--t-+-~~-+-i-~+-~~-+-t-~+-~~-+-t--r-
r-t- -+- + .-t- -+- -t- -+- -+ ---!~ -1- +. -+ ... \-- --1- .;. -- -.-~- --1-- .- -.. +.. . - .! ::;::':-:: ... -·1.: -:-L i '- '.-1,' :1:._. 1 j. - j, .1. I I --, : t I I : -:-'i.:. .:::.,-- y. '-J" I =-:::1: ":1:" ,I, I ' r I 1 I I ~'I'" I t I '
112000~~--~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
o 0 20 000 40 000 60 000 80 000 100 000
PERCENT SPAN
F-6 EEE Uncooled Rig 43% Reaction Rotating Rig Inlet Pressure vs. Span (Area Averaged)
"
N o \0
269DEG
3565 DEG DATA - 603554120a
STATION NUMBER 5
N/JiT = 351 4
PR
STATION 05 INLET
CURVE
LABEL
11
12
13
14
15
16
17
1690DEG
F-7 EEE Uncooled Rig 43% Reaction Rotating Rig Inlet Temperature Contours
= 412
CURVE
VALUE
31200000
31300000
31400000
31500000
31600000
317 00000
31800000
N -o
I PR ! I'" I ....
~..,..l ...'Rr ,i -,_. if~l : :-
.1 i '-Iii' ::ij i
IU: : : :. iA~·j ~- - lii,.r.. :1;:J
'\~ ,:!. I I tAr. 1
..... Ial'; . i .... -.l 1~!'" ~ Ji~::' '.": I"",! ~~ - . L ~~, - .3 ., ... , ~ir"'!"r'~: .:'.;:: .it
u.. 0
l !:: X If"I.7l: ! 1 I· t' ~~.:. I,: F.;; 1,'';'P
w l-I-
-::'; .. .- c,. ',. ! k~,". ltI-1'_.. .,. ~~ :-::' ;:: :,:. -" .... ~,....,.- ..0.; - ~ :..:;. - • I;.' ;:t r:;
"-:#.' . :' - l:- 1 --:: -ou: .; ;..~ ~.:.I·~.. ~~ ;.: .~ -:.-.: .• ":'=l..:n.·.J:::-"["'''
." ~~·I,~~~=:/:§;~~.!'~I-;.~r-.~~ ::. -:=-: to. ~~ :k:l:! ~IT ill: ~:i~ 1,::-c~"f~' ~~ ~ 1:::.1
40
30 a 2[) a to
% SPA-N
F-8 EEE Uncooled Rlg 43% Reactlon Rotating Rig EXlt Temperature vs. Span
t-J --
u. o
I !: X w lI-
...
130 :.:. :::::~'t-!I ~r-. ...,....:-_ ' .. -_~r-:: .,._~--r-, --r-__ -r~-iT .. -:r-.+'1I-.-,...~ _....,.~r-_'!.-.J'. __ ~_ ~._~ I:-:.. !--L.~ .... ~--1--f--~-:r-}-t-! I, J. i I ~L I 'T- 1 I' I' :
PR %Wc!W
355
412 733 I
412 1 254 '
403
460
60 14' 'J+':: "~~Ir::; E·:+: ~.::1' :::1·. ·l:'~: ::-i ., . f. .:'; ,··b.d:.: ,: ;!'.:= <; ::;"I:;;:~§.:::~:::T:f$lE~--tE: o 10 20 30 40 50 60 70 80 90
% SPAN
F-9 EEE Uncooled Rig 43% Reactlon Rotating Rig Exit Temperature vs. Span
212
« Cl J:
1 I-X W l-e..
34~41--~~-+~~+-~~1--r-~,r+~~~~~r,~~~--~;-r-~---+,-4~+-~~~~~--~~~~~kr!+-~-+--rT-t-
30 I I f-- ~_If---r' - __ --+~14__l~-+--t-,.~.A---:-+I-t--i~ ~ -----1
, 1 I I
29 -'--+-+-+-
28
27
ot'/ / ~/ I j _~' - +- /ii/' /,/1'1 ' I A ,.--r-" ::r.-- -
26
25
24
23
22
// I 00 ' !.1i ' _ E-~J / ' , J;::..q ~I ,I . fI. __ ~ / F.j' I'- 'I 'P A I I Y- I t to: .... ' f
21 'I I .- 1--+--:1-_ t-r--+-_--I'---.-"-""', <c;~ -
J;! 1.1 N/.JT PR N/.JT PR
19 ' I ~ 0 3514 412 D 3488 412
%Wc/W b 733 ~
~ ~--+---+--II-1r--+--'" 0 3519 469 0 351 2 412
18 -~ A I 0 348 9 5 05 0 280 5 4 03 -;-~f++ 6 3510 565 0 2794 460
l' f ~ 350 0 3 55 0 374 1 4 08 f 'f~T=f---Frr7"r-llr r I I I-I
Q ---", I
~ t-, , ,-17
1254
o 10 20 30 40 50 60 70 80 90 100
% SPAN
F-10 EEE Uncooled Rig 43% Reaction Rotatlng Rig Exit Pressure vs. Span
82
80 o 10
F-ll
tr.:
2U 30 40 50 60 70 80
% SPAN
EEE Uncooled Rig 43% Reaction Rotating Rig Spanwise Efficiency (Area Averaged)
469
355
408
90 100
N -~
F-12 EEE Uncooled Rig 43% Reaction Rotating Rlg Spanwise Efflciency (Area Averaged)
,\
80
70
(I) 60 w w a: t!' w c l w 50 ...J t!' :2 « a: « 40
30
20
N/.../f PR %Wc/W
I 0 3514 412 ~-- ~-,; _. I
~,-·i-·· , ; 1~'-1-+-' : '1
f-- -~ ;-- r-- ---- :,-0 3591 469
0 : ,
f-l· ' +- :--t ' I I
~ 3489 505 f--I-~- --, ,- - . I ~ 3510 565
,
, , ! ' ~ ~ 3500 355 ~
.~ ilia ~ D J t 3488 412 733 i !~ t.\ . , 1+-,
~l I l. :;:i 0 3512 412 1254 N, ~ ~ I'" --=rt ~j l~ li. - 1 i !/\ :
~r:: 0 2805 403 j 0 -{ { } ! wi Ie:: ... I \ ~ t,:p!
~~ C) f~ t r-- :e .,
~ T ~T: :& 1;;1 '~ ~ 2794 460 I" 4 t'.! 1"'1
0 3741 408 .. I't a1 ~ ~: t~ ;II l ~ ~' ' .. .! Ij.II ff;-j ',' I,l, --;:: ~f+' f-. ~I l: ~ l t$ ~I ;~ ~~.
I Jj " i .( -;,
"- ~ • ..t.-" ' 'III L-' I '~~ .~ ~~ I ~, j I . ~~ ~ , : 1
tt::f~j :::~ ':- .:' ·tii ' " IJS~ -C ~ ~ r\ 19! l~ " ... I .. , i [1:: , t-:
::;: :-1 kE ,'-18 ~ I" ,·I.:· ~ ~t) IVI :'\1 !i;.: : • .1 ,:;
," ~ P.§iF .:; Itf! -:: ~ .. ~ : :: I"'tt . 'V' :~ J; ~ ~;.
• .: ;r, : ; : :(,:~ ~ .,.,.
Jr:. .., '" I ',~ ':'
It..; I 1 . t . f: • .;- b : ~~i J;.:t !-
10. ,. j
I , I !(: ~~~l g::.:.~ I..-.. ! ,
, : . . j • ! .. I :'j h: ...: II.
I· . ! -.+ '; j •• '1 k ti; E..:l-; : .• :!
I'; iI, ~ - 1: t- "I :~. I': i" i,- ,:.f~ IS: ~:t .. :
I .: p. ',' ';' I;· I. !:' (':,-1=:- !,-: I- e ,: t:::: I;~ 1:;.' 1.:-" fI! ,:.:: .
, ;:!. :, tE; •. 8~: tr ~~ 1,':, I:' ' -: J'r ~ '.: '. F ,-::-
l!~: L~, t:E llt ::~ . .: ';' I. 1-
o 10 20 30 40 50 60 70 80 90
% SPAN
F-13 EEE Uncooled Rig 43% Reaction Rotating Rig Exit Air Angle vs. % Span at eire. = 91.6 degrees
rr-:~ ;~
f-··~
E!:? -, hi;~
~ <~ .:
~ ~ FrS; f.£ ,:0:
!OO If f.!
';
~ ~ ~S!
r!l ':.: tIn :-
r.~f: ~!;,
~.;-~ ~I'
::E 100
IV -0\
en w w a: e" w c l w ...J e" 2: ~ a: <t
~f:ili.:~';::'-r .1 _ .. i .. , ___ "_'\_" ! ... LJ .. , I 'li . __ ~ ... +.: -i I LJ_.~_....l~_ t t - • ~;:. :'jt' ~ '. '" I j',:, , I '1 ' "I I : :'
70 ~~ .. ; .•. ; '.;' :,1 - , I I '1 I 'I i ' ! 't I: ..h : " ,.... . . "T-I1-+-t, ,--r-, r- ',' . t· , '! .• - I .-~.' 1, .. ~ "1.1.·_· -1,-' :-. ': ·'I, .. ·:--t-i":"--1-~ t .. 1;..".... '; .. ~t:-~: '::::r . . T i j i\ ~ ""
:..: .:.: .. ~:. r :: I I',,!, I I 'i, , ! J '.... I J.:.J:""" -~F.-'lt-:=l-::-i--+--t--+-+---'+---r ., ...... - -, .. - t····· _. -. I . .~ i 'i I,' .',' i -, '+, '. "1-- "-;--j "-+-':"'c;.;;.'. Jt....;J , E:f.;:. :::; ~, , T' I, 'i, 4; rc ....,.. t': , .. :.;
60,.." .. " ., , !' I '~ t ; ...... -s: '.' '!.. •• ':: ... ,_.l.-h-r-.-+~ r'-' . ~,+ . Ir\l-\'" . -~. +&. 1---,-" -+ rr~.. l!:l:t.:l :;' -: "'.. ~. I i '\' !M' 1 l!l I 'A' ;-,... ~
% SPAN
F-14 EEE Uncooled Rlg 43% Reaction Rotating Rig Exit Air Angle vs. % Span at N/sq.rt. T = 350
'j
(I) w w 0::: Cl w c l w ...J Cl 2 « 0::
<i:
~~ :l!' "':t _. 1 - .:rl~f--~- -f !.! _ f- ~ ____ ~ I _.!_J _~-+--1_ '_!_L_I_J !' I J_' ~' :~: : __ I-P_R_~_CI_R_C "- ~ :', rTT I I I '1 I-r-r: . 0 4 1 91 6
80 Jr:::-;:;:.ct';::;.ct=.,..-+-+-+-+--4i- f--L ___ L f--~---L: ___ :._ ~ __ . -f ~ _____ ~_ L __ ....! __ ---L _+_ -l_~_."""'-.T0::..f~4...,1.......,~......,,1 ,.....6~ ::_ _~ . ~" I 'i i' 'i " I l i - ' '. ; _ :!: ;-f; :
70 It!.. t
E''"'"::
o 10
F-15
20 30 40 50 60 70 80 90
% SPAN
EEE Uncooled Rig 43% Reaction Rotating Rlg Exit Air Angle vs. % Span at N/sq.rt. T = 375
100
PR ~J j I ;. ·t .. ·· .. · .. ·t .. _.-. N/VT
o 350 41
1 0001+---+-~ --+--1-- --·~·i It-l---1-:-t--+-I
--± ll-:----t---t--H r\ ~ -'1 -i
1' :'<...vr~l ..... t\c1~" 41
I ~ ill.: I: 1- _ DESIGN (M975)
: :~~ 1· .. i I .. ·· - I .-~~
41 o 280
6. 375
PREDICTED
'\. I !!: I' 1 o 900 ~~ -- --t-~.~ ! .+--~! --+-·tf.-_-.. +-.-+l-.-+-,.-_ t-t.-.. -tt:I\--+--.. -+-_-.• t--T.-_.-t. -......:.+-"7:
I • ; \ ' Ij 1 : r-" ~
0800,r-::-~~ '~~ ~,.i-!+ --- ... \~"I·--·r-; t I I
-' . t : I ~ I I ·f --. ...11
- -1\-- ---.-~ 1 : ' ! I, ,
-.......... ~----
- ( i i ~ ~~"I -. 1·-- . -J.-.... --- _. -+-++-\-+---,-,+-"~~~ 0.7001+--+- -}---jf--+-, -+-+\-f\\-+-I !+-+--t--t-,-t--t--r-t-t-+-tr ,,--:-r-:-tj;i~
. I [ .... :.. ~ ,~ .. --. ---t- .. . -~~, '1~1 I\! ::~~
--j -.\ ... \. I .+ \ .... -- -+ ..... -.-- -- ·-.r--ft:---t-----t-'-.-:i::
o 600Jl-.~1-1-.-.-t-'i -+.-tl-t-+t,.-._+-_.-i'l~.k,\:-... +~-.. +._+.-+ _.-.. +. -._-t-T.-_t-it-,T, -:-, r~~.!t
- .!...-r .. j .. ··1 .. j .. , .. - .. _.Jt . ~~ ": 1~' ~:: i 1 1. ! /r (,~"""'-.l~ l ' .' It.' ! ••
0500! ! 1 I - ~-l~fJ .~ l~~.. rr.1-= ·tr; , t ,~ ~r ~t .. -... ~ ........ !.,.. -. t·· .- t·- I, (;. . ......... -'-r'- -.. . tJ' ~ ; it :i;f 1. ~ " 'u I 1 ( , rr: .": F
- ... - .. _+t'.· .. ·- '-1" .•.. "'-1---'-"- ~.- .- ·• .. f--------r-·- I. • ":
If. ,:t t ~ I ~ • j + ~
0400~~~-+-+-t-t-+-++-r-+~~r-r-+-;--r-r,-.~10.~:~.t,t.i~::~:1 ....... I ....
"-r:·+~-t-- --f--"l--~ .. #. ~,'. -, rl:tl7:nffi
H • t·· .t: :IU U
%x/bx
F-16 EEE Uncoo1ed Rig 43% Reaction Rotating Rig Vane Surface Statics - 11% Span
218
le.. ...... ~
N/.JT
o 350
o 280
6. 375
PR
41
41
41
'1"\ I "1 ,. i 1 tt !~~! t\ ~tL tl: t t! j I ,'lt oft;: t, .. l • ri': d~ ;;! +,t '-- _. ••• ••• •••• .~ ••• + •••••• "., ++.~ .++ "I~' ~-:-- .:: 'jLI ' .. ! I~:l' Ijlll:t rt I
I • ,!s.. ' . I + 1 " : I! It: t, tt it ~ PH l:tr ~
1t jl
, I
Itt t
, +
,
:t t , t +
•
Ii Itl
II P .. t
t
t
• •
~ 1 Ilt 1 ! ill li! iii !lW! 1; l t!!l ll411 t ~!ll4tt ~timlw HI 'lOO14mJ1 iummHummmfHffimfiOOiJ 0300 flU! II 1I HH tnt It! lililli!! lP 1 [iii! HifllllHIl tl
o 20 40 60 80 100
%x/bx
F-17 EEE Uncooled Rig 43% Reaction Rotating Rig Vane Surface Statics - 50% Span
219
'I" I : • ., . " " l .:< I" 1 000 '--+--+--+--+---+-....,IPIIoJf-,,· +-1f--t-f--:-,. +-rr .... !tIll" .. ·:.J.t :'I''":'t ::;..-1 +'"~r-, r.~--:-t .. -:;"T; ;-:-:1. ~ ;
"~~~··!lo.·~-'a"~----~-~~-+--+---4-~~---~~-~~~~-~~~--r-~~~"!7¥T~4~~~~'T.*01~"~'*"~" I j H, +1 I '1. • ~ ,. I' I,~, .. , tt"
f - "\ .. , .. r ,,' "" • :::; ".: • "1
.. : "~' ": ',:'t j .1 I Itt •• f
0900
-. I'--~~ -1-- K -.. -- .- -. -~ ... --- --_. ~ . -~ : ; [;;{I .. "'jf'
___ 1__ !\ --- -... -- -,- -.-- _l_~ •• '_._.. : :::~ 110- •
~-~~+--+-4--+-~-4--+-~~--r-~-+--r'~" ., : ' I: :-fl
c - --- -- - .. -- -.. -- - . ,_. .~ c--:--~ -- .~~tf::t11 ' I ...
0800L-__ ~.-.-_.+.-.-_~.-._~_-_-.+-_.-.~_-._~I\---+---~t~---.+--_~ __ 4-_~.~+.-._-r.-4-~-_t~-.--r.--i-~.r\,t~~.~~.~~,.~~:~l , ,:1 II ,,,.
t I ~ .... I • t t
.. _. f- .. - •
- - --. f--. •••.••.• -. - -- .•
r-'
F-18 EEE Uncooled Rig 43% Reaction Rotating Rig Vane Surface Statics - 89% Span
220
41
41
0800
0700
~. [E1:;t;I::.~~~ti .;~:Ir:hl~~; ttl nbli:' I~ flil/ffl<iTI r} m f'- it Harn+t!lnl
~ ;J! Ii mGI nUi iHUW: fI Ii th rEi Ki~ ~l 0300 [1 r. Ii fE :t If ~. ~Ht eJ
Il ~l~
u ft il f1 o 20 40 60 80 100
%x/bx
F-19 EEE Uncooled Rlg 43% Reaction Rotating Rig Mid Gap 0.0. Statics vs. % x/bx
221
Iw ..J :2
I~ ~
o 20 40 60 80 100
%x/bx
F-20 EEE Uncooled Rig 43% Reactlon Rotating Rig Mid Gap 0.0. Statlcs vs. % x/bx
222
N N W
06
I-w 04 ...J 2:
l-e.. -C ..: :!E a: 03
0 LL I-~ ...J e.. W ..,: w 2: ~ > en e..
20 40 60 80
%GAP
469
505
565
355
412
412
403
460
100 55
733
1254
F-2l EEE Uncooled Rlg 43% Reaction Rotating Rig 1.0. Platform Ps vs. % Gap
IW -J 2
o -1'5
20 40 60
%GAP
--!--.I---,
, ; ..
80
;
733
1254
100 55
F-22 EEE Uncooled Rig 43% Reaction Rotating Rig 0.0. Platform Ps vs. % Gap
224
CI) c..
68
64
> 60 I-
~ <.J
!::
~.~ = rug 'F ;;:.
ll.
~
t!;j
::.:
~ t..'":: r::-
X 56 w I ~ ~:j! w 2
~ ~
52 . ~
48
44 o
:r t:: I" i I 1 11 1 ... .- :.! F;H :: ._t . ...: :-~.-: : I j
, . r;~ -' "'.Y: i i
: I ! r .. •• ,0 j .+- ~-+- l
:- , t::- I·:: :;j ~ I , 1-,.
f--; ." 1-: b-i 1:': ; I g .l._ ~I, L I ~ ~ ~ ~ ~ ~ :r ~ ~ ~ :~ :::
"- ....... t-t-:: j...I'r' ~ -::.. l--'" 7"'; ~ t-::; I!· .:.~ -;~ :~ J : ,.t..-- I-'"
t1 I 1 i .J-r--r; ~ J.-. ~ ~ I'"" f.-....... :: ", ,I~ :;.1 I
1£1i 1!1 r'·h l-t-I-i ---....... Lrf: ~ l...-~ j. .. -: F p.. •. ,i !
,. ~ ~
I-~ r--r." :.-V:...r-~ .......... ~ I ~: 's ';;:i:
';:<',1. ....... f.-r .-r- J..-.-~ t::-t-" : .';j .:' :!;., :1. :i * .' L- ......
~~ r l • ~ f-H'" , .-:,...-- --t. :.....- : !~; CT',
j'::l1; ,. f'~ I.;...-~ :. lr-' ~;;...... ~ ~ : : . ..:; rtf' f.-f-. .jl ::-; ~ _rarr:.' ~ i--'!'" -~ ~ I :~ 'Ii f~'" m
,: r·· .' t...-~ f'" ~ fZP i 1 : ,.; :-=c,. ~::f F:,~ -:' i :! !;--' :rffi -:r.t'.: ~ .ii+!~ 1_
ft~:
b:~
10
F-23
t F=' r:t ~ ..... ~ ~ ~ r 1-, --', r~
k1~ I . ': "I : I"::; .. ;:: !~i~ i .. ::
2:1.; . . , i i j J : :' 1·,- i'ii;] [f~ fl" ;" ,,: . ':
! j" .J! ..; '~ ~i'! 1$:
'.:; ... ~:. " 1 : I ; tr;1 f.~: j ..
. Ii. : .;' ':, I . ; N/F PR -'
~- '! ..: .J:: t~:;: .' i : : . : :'!; g 3514 412 ,.", :':
fW-!j::;~ :,: 12:: I·· .. .'= .: r. i ,:1' I , I' 3488 412 ;'. ~. :;;-.;.c 2;- ~;-! ':' ': == t .' 1- ':h;:-- .?-: ,~~ 0 351 2 412
F:S hI. .~ :.: [;- : :: f..: r~ '" '':~ 0 • !1~::; ;.. : ·'t :: . , '- 2805 403 .-' &" :-.,; t:c:· ~.!' I:: ! . F: '~, .:~ .'!± o 3741 408
11:: Fi:...j h~ II ~ .. : t:: I.!. : iT, I,;;
20 30 40 50 60 70 80 90
% SPAN
EEE Uncooled Rig 43% Reaction Rotating Rig Vane Exit Cavity vs. % Span
: :1 (:'r: r::? ,~~ :."< E?£: ;E 1:,- r:::: :.::: S ~.
%WclW
733
1254
100
en 0-
>t: ~ U l-X w w c <C ...J CIl
% SPAN
N/F
3514
3519
3489
3510
3500
2805
2794
3741
PR
412
469
505
565
355
403
460
408
F-24 EEE Uncooled Rig 43% Reaction Rotating Rig Blade Exit Cavity vs. % Span
226
,
o EXIT TT RAKES
~ CONCENTRIC PT. TT
o T E PLATFORM STATICS - VANE
o INLETPT
o INLETTT o EXIT PT RAKES
~ EXIT WEDGE PROBES
o SURFACESTATICS-VANE
o MID-CHANNELSTATICS-VANE
VIEW LOOKING UPSTREAM
F-25 EEE Uncooled Rig 43% Reaction Rotatlng Rlg Clrcumferential Instrumentation Location
227
This Page Intentionally left Blank
NASA Headquarters 600 Independence Ave , S W
WashIngton, rx; 20546 Attn RTP-6 R S Colladay
NASA-Lew.lS Research Center 21000 Brookpark Road Cleveland, OH 44135 C C Clepluch, MS 301-4 (20 cop)
NASA-Lew.lS Research Center 21000 Brookpark Roacl Cleveland, OH 44135 LIbrary, MS 60-3 (2 copies)
NASA-Lew.ls Research Center 21000 Brookpark Roacl Cleveland, OH 44135 Attn M A Berel1ll, MS 86-1
NASA-Lew.lS Research Center 21000 Brookpark Road Cleveland, OH 44135 Tech UtIlIzatIon Off , MS 3-19
NASA-Lewis Research Center 21000 Brookpark Road Cleveland, OH 44135 Attn W M BraithwaIte, MS 60-6
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NASA SClen and Tech Inf Fac. POBox 33 College Park, Maryland 20740 AqUlsltlon Branch (10 Copies)
NASA Dryden FlIght Research Ctr POBox 273 Edwards, Cahfocnia 93523 Attn LIbrary
Department of Defense Washington, D C 20301 Attn R Standahar
3Dl089 Pentagon
WClght-Patterson Air Force Base Dayton, OH 45433 Attn E E BaIley (NASA Liaison)
AFAPL/DO
NASA Headquarters 600 Independence Ave , S W WashIngton, rx; 20546 Attn RJP-2 D J Pbferl (2 Cop)
NASA-LewlS Research Center 21000 Brookpark Road Cleveland, OH 44135 Attn D L Nored, MS 301-2
NASA-LewlS Research Center 21000 Brookpark Road Cleveland, OH 44135 Report Control OffIce MS 5-5
NASA-Lewis Research Center 21000 Brookpark Road Cl eve land, OH 4413 5
Attn R W. Schroeder, MS 500-207
NASA-Lewis Research Center 21000 Brookpark Road Cleveland, OH 44135 AFS; Llasion OffIce MS 501-3
NASA-Lewis Research Center 21000 Brookpark Road Cleveland, OH 44135 Attn A J Glassman, MS 77-2
NASA-Lewis Research Center 21000 Brookpark Road Cleveland, OH 44135 Attn L ReId, MS 5-9
NASA Ames Research Center Moffett Field, CA 94035 Attn 202-7/M H Waters
NASA Langley Research Center Langley Field, VA 23365 Attn LIbrary
Wright-Patterson AIr Force Base Dayton, OH 45433 Attn R P Carmichael
ASD/XRHI
WrIght-Patterson Air Force Base Dayton, OH 45433 Attn H J P VonOhain
AFAPL/CCN
NASA Headquarters 600 Independence Ave , S W WashIngton, rx; 20546 Attn RTM-6/L HarrIs
NASA-Lew.lS Research 21000 Brookpark Road Cleveland, OH 44135 Attn J W Schaefer, MS 301-4
NASA-Lewis Research Center 21000 Brookpark Road Cleveland, OH 44135 Attn M J Hartmann MS 5-3
NASA-Lew.lS Research Center 21000 Brookpark Road Cleveland, OH 44135 Attn N T Saunders
NASA-Lewis Research Center 21000 Brookpark Road Cleveland, OH 44135 Attn R J Weber MS 500-127
NASA-Lewis Research Center 21000 Brookpark Road Cleveland, OH 44135 Attn D C MIkkelson, MS 86-1
NASA-LewIS Research Center 21000 Brookpark Road Cleveland, OH 44135 Attn R W. Graham, MS 77-2
NASA Ames Research Center Moffett FIeld, CA 94035 Attn 202-7/L J WIllIams
NASA Langley Research Center Langley Field, VA 23365 Attn D Malden
Wr.lght-Patterson ~r Force Base Dayton, OH 45433 Attn R EllIS
ASD/YZN
WrIght-Patterson Alr Force Base Dayton, OH 45433 Attn E C Simpson
AFAPL/TB
NASA Headquarters 600 Independence Avenue I SW WashIngton, rx; 20546 Attn LIbrary
NASA-LewIS Research 21000 Brookpark Road Cleveland, OH 44135 Attn L E MaCIoce, MS 301-4
NASA-Lewis Research Center 21000 Brookpark Road Cleveland, OH 44135 Attn W L Stewart, MS 3-5
NASA-Lew.lS Research Center 21000 Brookpark Road Cleveland, OH 44135 Attn R A. Rudey, MS 60-4
NASA-Lew.lS Research Center 21000 Brookpark Road Cleveland, OH 44135 Attn T P. Moffitt, MS 77-2
NASA-Lewis Research Center 21000 Brookpark Road Clevelancl, OH 44135 Attn K E Skeels, MS 500-305
NASA-Lewis Research Center 21000 Brookpark Road Cleveland, OH 44135 Attn Army R&T Prop Lab, MS 106-2
NASA Dryden Plight Research Ctr POBox 273 Eawards, CA 93523 Attn J A Albers
NASA Langley Research Center Langley Field, VA 23365 Attn R Leonard
Wright-Patterson Alr Force Base Dayton, OH 45433 Attn Col. C. E Painter
ASD/EN
WrIght-Patterson Air Force Base Dayton, OH 45433 Attn H.I Bush
AFAPL/TB
BoeIng Aerospace Co POBox 3999 Seattle, Washlngton 98124 Attn H Hlgglns
Lockheed Callfornia Co Burbank, CA 91502 Attn R Tullis, Dept 75-21
Boeing Aerospace Co POBox 3999 Seattle, WA 98124 Attn H Hlgglns
Lockheed Georgla Co Harietta, GA 30060 Attn H S SWeet
General ElectrIc Co lAD:: One Jimson Road Evendale, OH 45215 Attn T F Donohue
Pan American World Airways, Inc JFK Internatlonal AIrport Jamlca, NY 11430 Attn J G Boeger
United Alr llnes san Franc~sco Int A~rport
Haint Operations Cntr San Franc lSCO, CA 94128
Attn J J Overton
BrunSWIck Corporation 2000 Brunswlck Lane Deland, FlorIda 32720 Attn A ErIckson
George Shev lln POBox 1925 Washlngton, DC 20013
BoeIng Aerospace Co POBox 3999 seattle, WA 98124 Attn D S Hlller HS 40-26
Lockheed California Co Burbank, CA 91502 Attn J I Benson
Gates Lear]et Corp P O. Box 7707 Wichlta, KS 67277 Attn E Schiller
Gruman Aerospace Corp South Oyster Bay Road Bethpage, NY ll7l4 Attn C Hoeltzer
Amer~can Airl~nes
HaInt & Engr Center Tulsa, OK 74151 Attn W R Neeley
Pan AmerIcan World Al.rways, Inc JFK International Airport Jamica, NY 11430 Attn A. HacLarty
General Electric Co I AIX;
One Jimson Road Evendale, OH 45215 Attn B L Koff
FluiDyne Engineering Corp 5900 Olson HelOOr ,al Hlghway Hlnneapolls, HN 55422 Attn J S Holdhusen
UnIversIty of Tennessee Space Instltute Tullahoma, TN 37388 Attn Fr V. Smith
Gas DynamICS LaboratorIes Aerospace Englneering Buildlng UniversIty of HIchigan Ann Arbor, HI 48109
Attn Dr C W Kaufmann
The Boeing Co , Wlchlta D,V WIchIta, KS 67210 Attn D Tarkelson
General DynamICS Covalr P. 0 Box 80847 san DI~O, CA 92138 Attn S Campbell, HZ 632-00
HcDonnell AIrcraft Co HcDonnel Douglas Corp POBox 516 St LoulS, HO 63166
Attn F C Claser Dept 243
Eastern Air lines International AIrport Hiami, FL 33148 Attn A E FIshbein
Delta AIr lines, Inc Hartsfield-Atlanta Int Airport Atlanta, GA 30320 Attn C. C. DaVIS
Hamilton Standard Bradley Field Windsor Locks, CT 06096 Attn P J DumaIS, HS l"A-3-l
ROM Corporation POBox 878 - Foot & H Street Chula Vista, CA 92012 Attn LIbrary
TIM Equipment Corp TIM Inc 23555 Euclid Ave Cleveland, OH 44117
Attn I Toth
Hassachusetts Inst of Tech Dept of Structural MechanIcs CambrIdge, HA 02139
Attn James Har
Lockheed CalifornIa Co Burbank, CA 91502 Attn J F Stroud, Dept 75-42
Boeing Aerospace Co POBox 3999 seattle, WA 98124 Attn D SHiller HS 40-26
Lockheed Georgia Co Harietta, GA 30060 WIchIta, KS 67277 Attn E Schiller
Rockwell International InternatIonal Al.rport Los Angeles Divlsion Los Angelos, CA 90009
Attn A W HartIn
Transworld AirlInes 60S ThIrd Avenue New York, NY 10016 Attn A E. Carrol
HamIl ton Standard Bradley FIeld Windsor Locks, CT 06096 Attn A T Reiff, HS 1-2-2
Solar Division International Harvester 2200 Pacific HIghway san DI~O, CA 92112 LIbrary
Iowa State UnIversIty Dept of Hechamcal Eng Ames, Iowa 50011 Attn Dr. P Kavanagh
Hassachusetts Inst of Tech Dept of AstronautIcs and Aero CambrIdge, HA 02139 Attn Jack Kerrebrock
Penn State UnIversIty Dept of Aerospace Eng. 233 Hammond BuIldIng UnIversIty Park, Penn 16802 Attn Dr B LakshmInarayana
USAVRAD Command ro rox 209 sr Louis, MO 63166 Attn R M TItus (AstIO)
Eust~s Dlrectorate U S Army MobIlity R&D Laboratory Fort Eustis, VA 23604 Attn J Lane, SAVDIr-W-Tapp
Federal Aviation Administration NOJ.Se Abatement Dlvlslon Washin9ton, DC 20590 Attn J Woodhall
U S Naval Air Test Center Code Sf-53 patuxent River, MS 20670 Attn E A Lyzrh
~Research Han Co III South 34th Street ro Box 5217 Phoenix, Arizona 85010
Attention C E CorrIgan (93-120/503-4F)
Teledyne CAE, Turbine En9ines V30 Laskey Road Toledo, OH 43612 Attn W 0 Wagner
Williams Research Co. 2280 Maple Road Walled Lake, HI 48088 Attn R Horn
AVCO/Lycomin9 550 SHain Street stratford, CT 06497 Attn H Moellmann
Douglas Aircraft Co McDonnell Douglas Corp 3655 Lakewood Boulevard Lon9 Beach, CA 90846
Attn R T Kawai, Code 36-41
Envlronmental Protectlon Agency 1835 K Street, NW Attn J Tyler
Pederal AVIatIon )1rminlstratlon 12 New F'nglanrt ExecutIve Parle' Rurllngton, NA 18083 Attn J A <;'aln, AN8-200
Naval Alr PropulSIon Test Center Trenton, NJ 08628 Attn J J Curry
Environmental Protection Agency 2565 Plymouth Road Ann Arbor, MI 48105 Attn R Hunt
Cummins En9lne Co Tech Center 500 S Poplar Columbus, IN 47201 Attn J R Drake
The Garrett Corporatlon AiResearch Manufacturin9 Co Torrance, CA 90509 Attn F E Faulkner
General Electric Co /AEC One Jimson Road Evandale, OH 45215 Attn T Hampton (3 Coples)
General Electrlc Co /AFG 1000 Western Ave Lynn, HA 01910 Attn R E Neitzel
The Garrett Corporation AIResearch Aviatlon Co 19201 Susana Road Compton, CA 90221 N J. Palmer
Douglas Aircraft Co McDonnell Douglas Corp. 3655 Lakewood Boulevard Lon9 Beach, CA 90846
Attn M Klotzsche
NAVY Department Naval AIr Systems Command WaShIn9ton, D C 20361 Attn E A Lichtman, AIR-330E
Navy Department Naval AIr Systems Command Washln9ton, DC 20361 Attn W Koven, AIR-03E
Naval Alr PropulSIon Test Center Trenton, NJ 08628 Attn A A Martlno
CurtISS WrIght Corporation Woodrzdge, NJ 07075 Attn S Lombardo
Detroit DIesel Alllson Dlv GMC POBox 894 Indianapolls, IN 46206 Attn W L HcIntIre
WIllIams Research Co 2280 W Maple Road Walled Lake, HI 48088 Attn R Van N11Tl<legen
Boein9 CommercIal AIrplane Co POBox 3707 Seattle, WA 98124 Attn D C Nordstrom
Pratt & Whitney AIrcraft Group Government ProdUcts DIVISIon POBox 2691 West Palm Beach, FL 33402
Attn B A Jones
Aerospace CorporatIon R&D Center Los Angeles, CA 90045 Attn Library
Pratt & r'lll1tnr>l/ AJrcraft Group 400 I.ll n ~t rpf"t
F1St lI~rt("rri. rT 06102 Attn rrlccfnt"'r (3 ('r)1') anrl '5('n5
NAVY Department Naval AIr Systems Command Washln9ton, D C 20361 Attn G Derderian, AIR-5362C
Navy Department Naval A~r Systems Command Washlngton, DC 20361 Attn J L Byers, AIR-53602
Env~ronmental Protect~on Agency 1835 K Street, NW Washlngton, DC 20460 Attn J Schettino
Curt~ss Wr~ght Corporat~on
WoodrIdge, N J 07075 Attn S Hoskowltz
Detrolt Dlesel Allison DlV GHC 333 West FIrst Street Dayton, OH 45402 Attn F Walters
The Garrett Corporat~on ~Research Manufactur~ng Co 402 S 36 Street Phoenlx, AZ 85304
Attn F B Wallace
Boelng Commercial Alrplane Co POBox 3707 Seattle, WA 98124 Attn P Johnson, MS 40-53
West~nghouse Electr~c Corp P. 0 Box 5837 Beulah Road Plttsburgh, PA 15236
Attn Library
End of Document