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VAN NUV$ @A_IIOINIA
CLASS Z ENGINE INFORMATION
A STUDY OF
ADVANCED
COMPOSITE PROPULSION SYSTEMS
FOR
LAUNCH VEHICLE APPLICATIONS I._.
VOLUME SEVEN
Report 25,194
C ontract NAS7- 377
The Marquardt Corporation
Van Nuys, California
September 1966
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FOREWORD
This report constitutes a portion of the final report documentation
under National Aeronautics and Space Administration Contract NAS7-377.
This and two companion reports (Refs. 1 & 2) present general engine
data derived from the study which are organized to facilitate their
incorporation into concurrent and subsequent advanced systems studies.
Covered here are the Class 2 Engines (_o in number) studied in the
program's concluding phase. More complete study results relating to these
engine concepts, including such areas as subsystem design trade-off
studies and overall vehicle/mission analyses, are given in the main body
of the project report (Reference 3).
The present Volume is one of seven in the total published study documen-
tation. Its orientation in the report sequence is shown below:
Volume i Summary Report
Volume 2 Main Technical Report, Part i
Volume 3 Main Technical Report, Part 2
Volume 4 Class 0 Fact Sheets, Part i
Volume 5 Class 0 Fact Sheets, Part 2
Volume 6 Class I Engine Information
Volume 7 Class 2 Engine Information
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This report results from the contributions of the following
Marquardt Science and Technology Group personnel under
National Aeronautics and Space Administration Contract
NAS7-377:
W, J. D. Escher
B. J. Flornes
W. R. Hammill
J. J. Kuhlmeler
C. R. Orr
B. A. Otsap
A. F. Truitt
Acknowledgement is extended to C. H. Carlson and R. E. Brewster
of Marqumrdt's Product Operations Group who generated the super-
sonic combustion ramjet (SCRAMJET) performance data incorporated
in this report. Appreciation is also expressed to A. Malek and
A. J. Hayek of the same organization for assistance in defining
approaches for engine structural design and cooling.
The Contributions of Rocketdyne, a Division of North American,
Incorporated in the area of the primary rocket subsystems design
effort is noted. Lockheed California Company provided vehicle
integration support which permitted engine sizing and configura-
tion selection for the vehicle model considered here. The assis-
tance of Rocketdyne and Lockheed was received via Marquardt sub-
contracts under Contract NAS7-377.
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TABLE OF CONTENTS
PREFACE
INTRODUCTION
General
Background
Selected Class 2 Engines
Scope and Content of the Report
General Reference Data
SUPERCHARGED EJECTOR RAMJET (ENGINE NO. ll)
Technical Description
Schematic and Operation Mode Block Diagrams
Engine Drawing
Engine Weight Statement
Operation Mode Schematics
Engine Basic Propellant Circuits
Operating Mode Control System
Vehicle Design
Inlet Contour, Pressure Recovery, Capture Area Schedule
Ejector Mode Specific Impulse and Thrust Maps
Ejector Mode Air Flow Map and Capture Area Schedule
Ejector Mode Tabulated Performance Data
Fan Ramjet Mode Specific Impulse and Thrust Maps
Ramjet Mode Specific Impulse and Thrust Maps
Fan Operation Mode Specific Impulse and Thrust Maps
SENSITIVITY ANALYSIS (E_INE NO. ll)
Summary - Bases
Reference Trajectories
Baseline Specific Impulse and Thrust
Sensitivity Parameter Ranges
Summary - Results
Inlet Pressure Recovery Effect, Ejector Mode
Fan Pressure Ratio Effect, Ejector Mode
Primary Rocket Equivalence Ratio Effect, Ejector Mode
Primary Rocket Combustion Efficiency Effect, Ejector Mode
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VaN NUV|. C&teFOIINI4
TABU OF C0 nS (conn mD)
Primary Rocket Nozzle Efficiency Effect, Ejector Mode
Mixing Efficiency Effect, Ejector Mode
Afterburner Equivalence Ratio Effect, Ejector Mode
Afterburner Combustion Efficiency Effect, Ejector Mode
Exit Nozzle Efficiency Effect, Ejector Mode
Exit Nozzle Area Ratio Effect, Ejector Mode
Inlet Pressure Recovery Effect, Fan Ramjet Mode
Fan Pressure Ratio Effect, Fan RsmJet Mode
Afterburner Equivalence Ratio Effect, Fan Ramjet Mode
Afterburner Combustion Efficiency Effect, Fan Ramjet Mode
Exit Nozzle Efficiency Effect, Fan Ramjet Mode
Exit Nozzle Area Ratio Effect, Fan Ramjet Mode
Inlet Pressure Recovery Effect, Ramjet Mode
Combustor Equivalence Ratio Effect, Ramjet Mode
Combustor Combustion Efficiency Effect, Ramjet Mode
Exit Nozzle Efficiency Effect, Ramjet Mode
Exit Nozzle Area Ratio Effect, Ramjet Mode
Inlet Pressure Recovery Effect, Fan Operation
(¢ = O, 0.20)
Inlet Pressure Recovery Effect, Fan Operation
(_ : 0.50, 1.00)
Fan Pressure Ratio Effect, Fan Operation (_ = O, 0.20)
Fan Pressure Ratio Effect, Fan Operatien' (_ = 0.50, 1.00)
Afterburner Combustion Efficiency Effect, Fan Operation(_ = O, 0.20)
Afterburner Combustion Efficiency Effect, Fan Operation(_ : 0.50, l.O0)
Exit Nozzle Efficiency Effect, Fan Operation (_ = O, 0.20)
Exit Nozzle Efficiency Effect, Fan Operation (_ = 0.50, 1.OO)
Effect of + 10% Subsystem Weight Variation on Engine
Th ru st/We ight
Effect of + 50% Subsystem Weight Variation on Engine
Thrus_/We ight
78
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TABLE OF CO.ZEroeS (com_rmmw)
SCe ACE 22)
Technical Description
Schematic and Operation Mode Block Diagrams
Engine Drawing
Engine Weight Statement
Operation Mode Schematics
Engine Basic Propellant Circuits
Operating Mode Control System
Vehicle Design
Inlet Contour, Pressure Recovery, Capture Area Schedule
Ejector Mode Specific Impulse and Thrust Maps
Ejector Mode Air Flow Map and Capture Area Schedule
Ejector Mode Tabulated Performance Data
Ram0et Mode Specific Impulse and Thrust Maps
SCRP_MJET Mode Specific Impulse and Thrust Characteristics
and Reference Trajectories
SENSITIVITY ANALYSIS (ENGINE NO. 22)
Summary - Bases
Reference Trajectories
Baseline Specific Impulse and Thrust
Sensitivity Parameter Ranges
Summary - Results
Inlet Pressure Recovery Effect, Ejector Mode
Primary Rocket Equivalence Ratio Effect, Ejector Mode
Primary Rocket Combustion Efficiency Effect, Ejector Mode
Primary Rocket Nozzle Efficiency Effect, Ejector Mode
Mixing Efficiency Effect, Ejector Mode
Heat Exchanger Equivalence Ratio Effect, Ejector Mode
Afterburner Combustion Efficiency Effect, Ejector Mode
Exit Nozzle Efficiency Effect, Ejector Mode
Exit Nozzle Area Ratio Effect, Ejector Mode
Inlet Pressure Recovery Effect, Ramjet Mode
Combustor Equivalence Ratio Effect, Ramjet Mode
Page
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lll
ll3
ll6
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TABLE OF CONTENTS (CONTINUED)
Combustor Combustion Efficiency Effect, Ramjet Mode
Exit Nozzle Efficiency Effect, Ramjet Mode
Exit Nozzle Area Ratio Effect, Ramjet Mode
Inlet Pressure Recovery Effect, ScramJet Mode
Combustor Equivalence Ratio Effect, Scram Jet Mode
Combustor Combustion Efficiency Effect, Scram jet Mode
Exit Nozzle Efficiency Effect, Scram Jet Mode
Exit Nozzle/Inlet Cowl Area Ratio Effect, ScramJet Mode
Effect of + 10% Subsystem Weight Variation on Engine
Thrust/We ight
Effect of + 50% Subsystem Weight Variation on Engine
s'_/weig_.t
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LIST OF MAIN REFERENCE ILLUSTRATIONS
Figure No.
1
2
A
B
C
D
E
F
G
H
I
J
K
L
Title
Flight Velocity -Mach Number
Installed Engine Station Nomenclature
Inlet Pressure Recovery Sensitivity Analysis
Range
Exit Nozzle Area Ratio Sensitivity Analysis
Range, Engine No. ll, Ejector Mode
Exit Nozzle Area Ratio Sensitivity Analysis
Range, Engine No. ll, Fan Ramjet Mode
Exit Nozzle Area Ratio Sensitivity Analysis
Range, Engine No. ll, Subsonic Combustion
Ramjet
Inlet Pressure Recovery Sensitivity Analysis
Heat Exchanger Equivalence Ratio Sensitivity
Analysis Range, Engine No. 22, Ejector Mode
Heat Exchanger Equivalence Ratio Sensitivity
Analysis Range, Engine No. 22, Ejector Mode
Afterburner Equivalence Ratio Sensitivity
Analysis Range, Engine No. 22, Ejector Mode
Afterburner Equivalence Ratio Sensitivity
Analysis Range, Engine No. 22, Ejector Mode
Exit Nozzle Area Ratio Sensitivity Analysis
Range, Engine No. 22_ Ejector Mode
Exit Nozzle Area Ratio Sensitivity Analysis
Range, Engine No. 22, Subsonic Combustion
Ramjet
Inlet Pressure Recove_F Sensitivity Analysis
Range, Engine No. 22, Supersonic Combustion
Ramje t
ii
12
69
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UNCLASSIFIED Report Z5,194Volume 7
Page 1
PREFACE
This report comprises a major portion of the technical results of the Class
2 study phase of National Aeronautics and Space Administration Contract
NAST-37V, "A Study of Composite Propulsion Systems for Advanced Launch Vehicle
Applications". This phase of the program was conducted under Task IV (of four)
of the contract work statement.
Composite cycle launch vehicle engines, as defined for this study, are single
integrated propulsion systems which are comprised of both rocket (liquid-
propellant) and airbreathing subsystems, e.g., primary bipropellant combustors,
inlets. To date this type of powerplant has received little systematic study
wherein common ground rules are employed to judge the possible merits of the
large number of candidate engines.
The potential advantages offered by the more attractive composite systems in
advanced (reusable) vehicles include the following points: high payload per-
formance (exceeds the advanced rocket, roughly equals the turbomachine-type
airbreather), high operational flexibility across the reusable-cycle mission
profile, ease of development in terms of the indicated major facility require-
ment for competing pure-airbreathing engines (composite engines can be seg-
mented to fit existing or planned ground test facilities which provide high
simulated Mach number airflow capability).
It is the objective of the study to (1) appraise this potential for advanced,
reusable launch vehicle applications, and (2) provide technical guidance for
initiating possible research and development efforts directed toward the
ultimate creation of these systems. The study included consideration of both
single and multistage vehicles, for earth-orbit payload delivery. The study
concentrated on launch vehicles in the 1,000,O00 pound gross weight class
which operate on hydrogen/oxygen propellants. In general, the study was
directed toward propulsion system first availability in the period 1975-1985
and full mission-cycle propulsion requirements from lift-off to landing was
considered. The principal performance criteria for engine ranking purposes
was payload-in-orbit to gross weight ratio. Other criteria were, however,
brought into play as appropriate.
Marquardt, prime contractor, Rocketdyne and Lockheed were associated in this
analytical ana design study effort. The study was extended over nine (9)
months with a final report (of which the present report is Volume 7 ofseven) submitted to distribution in February 1967.
UNCLASSIFIED
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UNCLASSIFIEDReport ZS, 194
Volume 7
Page 2
INTRODUCTION
GENERAL
This report is the third in a series of three, which specifically present
engine information derived from the NASA-contracted study, "A Study of
Composite Propulsion Systems for Advanced Launch Vehicle Applications"
(NAST-377). The three reports (the other two are Refs. 1 and 2) are associ-
ated with the three chronological phases of the study and comprise varying
numbers of engine concepts and various degrees of technical penetration asfollows :
Report Associated Number of Technical
Order Study Phase Engines Included Penetration
1 Class 0 36
(Ref. l)Overall System Analysis
only, performance on
three (3) reference tra-
Jectories based on
"ideal" inlet, important
parameters 'bracketed"
orly
2
(Ref. 2)Class 1 12 Included subsystem con-
sideratlons, performance
presented in map form,
based on realistic inlets,
conceptual designs made,
important engine variables
exercised parametrically
3
(This
Report)
Class 2 2 Effect of varying subsys-
tem and component efficien-
cies and operational points
assessed, performance maps
broadened and refined,
detailed conceptual designs
rendered based on vehicle-
stipulated sizing parameters_
approaches for structural
and thermal design and engine
control investigated.
To this end the present report presents detailed working information on two
(2) engine concepts taken from both the initial candidate listing of 36 con-
cepts reported in Ref. l, and the twelve (12) engine types further treated
in Ref. 2.
The next section will briefly review the two engine concepts. Also the scope
and content of this report will be summarized prior to the two major engine-oriented sections of the document.
'UNCLASSIFIED
.eport 25,194Volume 7
Page 3
BACE_ROUND
Of the thirty-six (36) engines originally ordered within the Class 0 phase
study (Ref. 1), twelve (12) were selected for further study as Class 1 sys-
tems. These twelve (12) systems can be viewed as variations about a single
"parent" multimode composite engine concept; the afterburaing cycle, air
augmented rocket/ramjet system:
SELECTED CLASS 1 ENGINES
(12 SELECTED FROM 36 CANDIDATES)
AFTERBURNING CYCLEAIR AUGMENTED ROCKET/-RAMJET PROPULSION
SYSTEMS
•--_NON AIR LIQUEFACTION SYSTEMS
(FOUR ENGINES)
•.--,_AIR LIQUEFACTION SYSTEMS
tEIGHT ENGINES)
The basic split shown is that of higher performance air liquefaction systems
versus the somewhat simpler non-air liquefaction systems which effects a
grouping of eight (8) and four (4), respectively. Both sub-families are
represented in previous engine types studied by The Marquardt Corporation in
the guise of lightweight, efficient acceleration and cruise aircraft power-
plants. These are the Ejector Ramjet systems (non-air liquefaction) and the
RamLACE systems (air liquefaction). These "parent" engines are further des-
cribed in Ref. 2. Design and performance data for the twelve (12) Class 1
Engines, in essence, comprise Ref. 2.
Report 25,194Volume 7
Page 4
SELECTED CLASS 2 ENGINES
The two engine concepts selected for the Class 2 studies were:
Supercharged Ejector Ramjet (SERJ - Engine No. ii)
SCRAMLACE (Engine No. 22)
With reference to the Class I Selection summary given above, it can be seen
that a continuation of the duality: non-liquefaction/liquefaction engines,
reflected in the Class 1 selection, was also carried forward into Class 2.
That is, both an air-liquefaction engine (No. 22) and a non-liquefaction
engine (No. ll) were further appraised. Each of these is clearly a better
performer in its category, where at the same time additional complexity,
e.g., recycled hydrogen, brought only modest gains in payload for the mission
model used. The significant advantage of the Supercharged Ejector Ramjet
over the basic Ejector Ramjet was notable. This caused it to be chosen as
a Class 2 system despite the additional hardware implication of the fan sub-
system. The Class 2 Engines are summarily characterized in this table:
SELECTED CLASS 2 ENGINES
Supercharged Ejector Ramjet (SERJ, Engine No. II)
Attractive Payload Potential with Minimum
Technology Uncertainties- Providing a
Nearer Term Availability
ScramLACE (Engine No. 22)
Maximum Payload Potential via the Combination
of Air Liquefaction and Supersonic Combustion
Ramjet Operating Modes, which are not fully
Developed Technologies
. _ort 25,194Voluxne 7
Page 5
As can be inferred from this listing, the concept of having two packages
of varying technical risk is apparent in the engines selected. Engine ll,
does represent a significant improvement in potential over the baseline
rocket in a concept that has little technical risk associated with it. On
the other hand, the Engine 22 represents a considerably higher payload gain.
However, two technological risk areas are apparent: (1) the air liquefaction
process and, (2) the SCRAMJET mode operation. These selected engines for the
Class 2 study are schematically shown and further discussed in the following
pages.
SUPERCHARGED EJECTOR RAMJET (SERJ - Engine No. 11)
The supercharged Ejector Ramjet schematically is shown here as a basic
Ejector Ramjet which has mounted before the mixing section a low to moderate
pressure ratio, thin profile low blockage fan subsystem. In concept, the
fan can be driven by either an airbreathing or a bipropellant gas generator.
The fan acts to supercharge the basic cycle in the initial acceleration mode
thereby improving its specific impulse while reducing the rocket subsystem
sizing. Perhaps most important, it provides a mode of operation for low
speed flyback-to-base via a ducted fan mode with or without plenum burning.
(This would be accomplished by relighting the afterburner at various degrees
of lean burning up to stoichiometric.)
SUPERCHARGED
EJECTOR RAMJET - ENGINE NO. 11
m--'-"----- IN LE T "_ '_- M IXER/DIFFU SER _ EXIT --'e'
F[F_- 0_-----.) -"'TURBOPIJMP ASSEMBLY
Report 25. 194Volu._e 7
Page 6
This engine is capable of operating in four discrete modes : (i) supercharged
ejector mode, (2) fan ramjet mode, (3) subsonic combustion ramjet and (4) fan
only operation. The later operating mode is a low-thrust capability applicable
to the flyback and loiter aspect of the mission profile. The engine consists
of a single stage low pressure ratio fan capable of being retracted from the
main engine flow stream. Accompanying the tip turbine fan is a fan drive sub-
system consisting of a remote airbreathing gas generator, or small turbojet
engine. Following the fan, a primary rocket subsystem, mixer, diffuser, after-
burner, and variable geometry exit nozzle are included as in the basic ejector
ramjet engine.
For a typical mission profile the engine is initially operated in the super-
charged ejector mode wherein the fan operates at design speed. The stoichio-
metric primary rockets are operated at full thrust condition and the after-
burner operates stoichiometrically. At a flight condition in the approximate
vicinity of Mach 1 the primary system can be phased off, the engine continuing
in the faro ramjet mode (technically a high bypass ratio, full plenum burning
turbofan cycle). In the vicinity of Mach 2 plus, fan operation is stopped and
the fan is hinged forward and retracted from the flow stream. The engine con-
tinues in the subsonic combustion ramjet mode to the staging condition. Follow-
ing entry and cruise-back in the subsonic combustion ramjet mode, subsonic loiter
and landing is accomplished with fan only operation with little if any plenum
burning.
SCRAMLACE (Engine No. 22)
The SCRAMLACE is schematically represented as having inlet and exit configura-
tions which are compatible with the SCRAMJET mode operation. The heat exchanger
subsystem shown here in the engine flow passage will from practical considera-
tions be located external to the throughput area of the powerplant as will be
noted in the conceptual design drawing provided herein.
SCRAMLACE - ENGINE NO. 22
11-
eport 25,194Volume 7
Page 7
This engine is capable of three operating modes*: (i) liquid air cycle ejector
mode, (2) subsonic combustion ramjet and (3) supersonic combustion ramjet. The
engine consists of a primary rocket subsystem which operates on liquid hydrogen
and liquid air, with the liquid air being supplied from the air liquefaction
unit, consisting of a precooler and condenser. The refrigerant is the liquid
hydrogen total flow supplied to the engine. Following the primary rocket sec-
tion is the mixer, diffuser, afterburner and variable geometry exit nozzle.
Initial engine operation is in the ejector mode with full thrust operation of
the primary rockets at a stoichiometric condition. Air flow, nominally con-
stant, is controlled by hydrogen flow into the engine and the specific flight
conditions, non primary fuel being burned in the afterburner st a significantly
fuel rich condition. At an appropriate flight Mach number the primary rocket
subsystem is shut down and the air liquefaction unit is closed off from the in-
let diffuser. The engine continues to operate with stoichiometric combustionin the afterburner as a subsonic combustion ramjet. At approximately Msch 6
the engine transists into supersonic combustion ramjet operation by simultaneous
shifting of combustion forward into the region of primary rockets (the rockets
are not reignited) and full opening of the aft end of the engine to permit the
normal shock system to pass from the engine. Upon entry, flyback is nominally
accomplished in the subsonic ramjet mode with loiter and landing being achieved
in the liquid air cycle ejector phase operation.
It might be noted here that the geometric criteria for efficient mixing of fuelin the SCRAMJET mode are approximately the same as those involved in the rocket/
air mixing phase for the ejector mode. This implies that the physical geometry
of the rocket structure might in fact be compatible with the SCRAMJET fuel in-
Jection requirement. The presence of the primary rocket subsystem end its
supports, as well as the afterburner fUel injection struts (if these are not
retracted), will affect the supersonic flow stream and these must therefore be
designed with minimum stream shock losses as an objective.
* An inlet closer rocket vacuum mode is feasible for ScramlACE provided
vehicle supplied oxidizer (liquid oxygen, liquid air) is available.
This mode is schematically indicated in the Scraml_CE section of the
present report.
Report Z5,194Volume 7
Page 8
SCOPE AND CONTENT OF THE REPORT
As stated, this report includes a separate section for each of the two (2)
engine concepts described above. The original numerical coding assigned to
these engines as candidates (Class 0 Phase, Ref. I) is retained for continuity,
the engine sections appearing here in numerical order.
The orientation of the engine data presented herein is toward direct user
processing for broad and diversified study activities. Performance, weight,
physical envelope characteristics, operating mode availability, and other in-
formation of this genre is arranged here in a manner intended to promote
effective assimilation of composite engine data by the reader. For this reason,
the documentation of interpretative results of the engine data, e.g. mission
application studies, is left in the main body of the report (Ref. 3). Similarly,
discussions bearing on the trade-off studies leading to selection of engine
design parameters, such as primary rocket chamber pressure, also remain in the
main report, since - per se - these may not be of immediate utility to a sys-
tems analyst striving to assess the applicability of composite engines to his
particular mission requirement.
Therefore, as appropriate, reference should also be made to the main body of
the Study's final report documentation (Ref. 3). There the bulk of the para-
metric analysis which, for example, explore the effect of the internal design
variables, is provided. Also the Study's vehicle integration and mission per-
formance work is represented in these volumes.
Each of the two engin e sections to follow is divided into two parts: (1)
Engine Description, Physical Characteristics, and Performance, and (2) Engine
Sensitivity Analysis - Bases and Results.
In further detail, the topics included, in the order presented, are:
Engine Description I Physical Characteristics and Performance
I. Descriptive Text, Schematic, Operating Mode Block Diagrams
2. Detailed Conceptual Drawing (Includes Numerical Statement of
DesignFeatures)
3. Weight Statement
4. Operating Mode Schematic Diagrams
5- Propellant Flow Circuit Description
6. Vehicle Installation Description
_port 25,194Volume 7
Page 9
T. Assumed Inlet Physical Characteristics and Pressure Recovery
Schedule
e Ejector mode (or supercharged ejector mode) specific impulse,
thrust and airflow maps reflecting the effect of vehicle flight
speed and altitude. These maps are backed up by computer-gener-ated tabular data.
9.* Fan-ramjet mode specific impulse and thrust maps.
i0. Ramjet (subsonic combustion) specific impulse and thrust maps,
including the effect of inlet air precompression (flow field).
II.*_SCRAMJET (supersonic combustion) specific impulse and thrust
data, including the effect of inlet air precompression (flow
field). This information is presented for three reference
trajectories which follow the performance curves.
12.* Fan (ducted) operation specific impulse and thrust maps, reflect-
ing the effect of varying degrees of plenum burning.
Sensitivity Analysis - Bases and Results
i. Reference Trajectories
2. Baseline Specific Impulse and Thrust (both net Jet) Performance
Values derived on the reference trajectories
S. Range and Limiting Values of Sensitivity Parameters, Performance
and WeightC
_. Perturbed Specific Impulse and Thrust - results for each sensitivity
parameter.
Preceding the individual engine sections, and immediately following this
section, a general reference section appears which includes:
i. Mach Number/Velocity Conversion Chart
2. Engine Station Nomenclature Diagram
B. General nomenclature and legends
4. List of references
* Engine No. ll only
**Engine No. 22 only
Report 25,194Volume 7
Page 1 0
SUMMARY - GENERAL REFERENCE DATA
The purpose of this section as noted in the introduction is to provide tech-
nical information and general background material applicable to the two (2)
specific engine sections to follow. Each of the items to be provided in
this general section will be briefly discussed below.
Msch Number versus Flisht Velocity Conversion Chart - Although the basic
engine performance information to be presented in this report is given gen-
erally on the basis of flight velocity (ft/sec, m/sec), much of the general
information as well as the intermediate data is most effectively and conven-
iently stated in terms of Mach number. A conversion plot is provided to
assist in approximate conversions of these two velocity terms. For more
precise computations the use of appropriate tables, however, is recommended.
Ensine Station Desi&nation and Nomenclature - An installed engine schematicis presented reflecting a typical composite engine of the Class 2 series.
The several aerothermodynamically significant geometric stations employed
in the engine general description, as well as in the performance computations,
are called out in this figure.
Standard Efficiencies - The following listed efficlencles have been used as
baseline values for all engine performance computations:
PrimaryRocket:
Combustion, _c* = 0.975
Nozzle, _n = 0.98
Mixer:
Mixing, _m -- O.80
Afterburner or Combustor:
Combustion, _c = 0.95
Exit :
Nozzle _ n m 0.98
Legends_ Nomenclature 2 and References - Within the engine sections certain
diagrammatic conventions have been adopted and these are reflected in both
schematic and tabular form in this section of the report. Also a nomencla-
ture sheet is provided for all symbolic characters employed either in the
presentation of the engine information, or in the computations supporting
the performance provided. Finally a list of references is given at the endof this section.
.U I.ASSIFIE
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Report Z5, 194Volume 7
Page 11
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r- .... :-: ;;
:.:: -: :: ::
s-
6
|!! ::::i
:,;: ;:;:
:::: t:::
.... t"
;T:: :°'_:
i:?:
.... i:_• ..? ;,,_
! ..... -
8
.... 1 I I
i?/:t ......
.... l#-,.i ....
I] .... !. ,1_ :l,l.ll,
.t-:: ;/::I:: :FI::#.- • I .... _1_.
! .:h:::l::;
........ _--.11 ....
:1:_ .... _/-",71:
:::; : :I:1::::..
....... l-t._ ....
e.., ........ =.,o .......... 1-1.,t-:..
::;! |::_:'1:
..... e.,, ....
:::: .... i_..i ....:::: ' :::1-1
iii !i!iii....T;::
;::: i!i!ll .
-.:. .... .:::;
:;:.. '. ,:::
::: ::'j::_:::
: i.li:i!i!_i:i
-._- •.,i:t....:.._
.-._ !_. ,_,..! ....
i:--_. "i!it%!ti:-:.!
___ liii!l_4i
10
VELOCITY, I000 ft/sec
::::lii'iJ i!_i L:!:::] ............::;:1 ::::1 ::."1 MI.... I ............
::::i:L2 iii:: !i::
..i "_ 1"Iii.........
..e ............
.e ......... , , ..
[:: :':: :::- ::,.
: ::: .'.:::::!I
". .:;: :::::;:I!
...... ::L: ....
:.:. .:. :::: -:
......... i;,.0!
:::s:2_!gigi;_il
::: :::: T;xr_:;_!
............ ,...
............ ;.... i
_:; i::i i-._!ii_i]
t:ii ::! :Yl
_::1!..:!..'_12 14
I0
I I I1.0 2.0 3.0
FLIGHT VELOCITY, 1000 m/sec
I4.0
_8
rquard! .,..o,,.o.,,,o,.,.
FIGURE 2 INSTALLED ENGINE STATION
Report 25 194Volume 7
Page 1 Z
NOMENCLA TU RE
Ac
FLOW FIELD i:"
INLET
SHOCK
A2 A31 A4 A6
A3 A5iICOMBUSTOR
_PRIMARY '_THRUST
CHAMBER ASSEMBLY
/FUEL INJECTOR
ASSEMBLY
A (PRIMARY EXIT AREA)P
FOR CONSTANT AREA MIXER A2+ Ap = A3
FOR CONSTANT AREA COMBUSTOR A3a= A 4
: ii!:i_!ii!iil
The basic flow processing situation in a representative composite engine
is schematized in this chart, which also provides the station nomenclature
used in the study. It will be note that both on the inlet and the exit
portions of the aerothermodynamic processes the favorable utilization
possibilities of the vehicle are assessed. _ae precompression of the in-
duced air by the vehicle body (vehicle bow shock system) is fundamentally
important in providing high engine thrust performance, particularly in the
ramjet modes. At the same time, the possibility of expanding the exhaust
flow on the vehicle aft body is of fundamental importance, critically sofor the SCRAMJET mode.
/J
rcluaraz .... _.,..,,,o..,.-- s,Jr:iHll_,U'm",
LEGEND- ENGINE SCHEMATIC
..=port 25. 194Volur_e 7
Page 13
Inlet I Exit: Subsonic Combustion
= INLET _
.--- EXIT---.a
Inlet I Exit: Supersonic Combustion(Including Sub/Super Conversion)
Precooler I
air
Condenser 36"R H 2l
i yH2 liquid air
Precooler I Condenser
air
25"R H?A
i VH2 liquid air
" la r(luard!
IJNCLASSIFIED Report 25 194Volume 7
Page 14
LEGEND- ENGINE OPERATING MODE BLOCK DIAGRAM
Letter Symbols (Within Blocks)
I Inlet SubsystemHE Heat ExchangerF Fan SubsystemR Rocket SubsystemMC Mixer/CombustorMD Mixer/DiffuserC CombustorE Exit
Mixer/CombustorlExit Subsystem
Letter Symbols (Fluids)
H Hydrogen0 OxygenA AirX Exhaust
Graphical Symbols
[ 1I
!
I It j
Functioning Unit
Non-functioning Unit
I i
I I
)
Fluid Flow Direction
Fluid Flow Through a Non-functioning Unit
Flow Mach Number > 1
Flow Mach Number <1
Flow Mach Number is both below and above 1at changing flight speed conditions
UNCLASSIFIED
UNCLASSIFIED
VAN _U_'|. CAI.;FOeNIA
_eport 25,194Volume 7
Page 15
NOMENCLATURE
Nomenclature used in this report is given below. The tabulated computer
printout inforumtion does not include subscripting as will be noted by the
repetition of certain parameter symbols. Refer to Figure 2 for engine flow
area station designations including the distinction n_de between A c_and Ao
where a vehicle flow field is involved (where there is no flow field these
are identical).
AB
A_/A 3
A5
A6
A6/A 5 -
A6/A c
AHX
AO
AOT
BL
CF, CF
H2
HTO
Isp , IS
Mo, M0
M2
NS
o/;P2
Pc
PRf
PT2 , PT2
PT2/PTo
PT0
Afterburner
Afterburner/Mixer Diffusion Ratio
Engine nozzle throat area, ft2
Engine nozzle exit area, ft 2
Exit Nozzle Expansion Area Ratio
Exit to Capture Area Ratio (SCRAMJET) ..
Inlet capture area for heat exchanger air flow, ft2
Inlet capture area for secondary air flow, ft 2
Inlet capture area for total air flow, ft2
Baseline
Thrust Coefficient based on inlet capture area
Secondary air static enthalpy at mixer entrance, Btu/lb
Ambient Total Enthalpy, Btu/lb
Specific Impulse, lbf/lbm/sec (Net Jet)*
Local Mach Number
Mixer entranceMach number
"Normal Shock"" inlet (Includes Normal Shock losses
plus an assumed 90_ diffuser efficiency.)
0xidizer/fuelmass flow ratio
Secondary air static pressure at mixer entrance, Btu/lb
Primary chamber pressure, psia
Fan pressure ratio
Inlet recovered total pressure, psia
Inlet total pressure recovery
Ambient total pressure, psia
UNCLASSIFIED
"'A_/#'I _J/
//imrquamr .,,,o,.,.
UNCLASSIFIED Report 25_ 194Volume 7
Page 16'
R i
Ref
SIS
SPC
T
V6
Vo, V0
WFT
WKX
Wp, WP
Ws/WP, WSWP-
WS, WS
WT
8 -
_C'N" .
_I_ -
Rocket Mode
Reference
Sea Level, Static Conditions
Specific Fuel or propellant consumption, lbm/hr-lb f
Thrust, ibf (Net Jet)*
Exit velocity, ft/sec
Local velocity, ft/sec
Total fuel or propellant flow rate, lbm/sec
Heat exchanger air flow rate, ibm/sec
Primary flow rate, lbm/sec
Secondary/primary flow ratio
Secondary (WS + WHX), lbm/sec
Total air flow
Two dimensional wedge half angle, deg
Combustion efficiency based on enthalpy rise
Characteristic velocity efficiency based on velocity, or thrust
Inlet kinetic energy process efficiency
_M
?IN
_p, PHP
_prec
_sec, PHS -
Mixing Efficiency based on static pressure rise
Nozzle efficiency based on stream thrust
Combustor equivalence ratio
Condenser equivalence ratio
Heat exchanger equivalence ratio
Primary rocket equivalence ratio
Precooler equivalence ratio
Secondary equivalence ratio
Net Jet thrust and specific impulse includes air induction inlet
momentum penalty, but does not include external drag such as cowl,
induced, friction, or spillage drag
bI ED
VdIH NUY$. CAIIFOIIN,a
R_,Jrt 25,194Volume 7
Page 17
LIST OF REFERENCES
la
_o
m
"Class 0 Engine Fact Sheets (Thirty-six Engines)", Contract NAS7-37V,
Marquardt Report 25,19h, Volumes 4 & 5, Sept.1966. CONFIDERTIAL -
Title Unclassified.
"Class 1 Engine Information (Twelve Engines)", Contract NAS7-377,
Marquardt Report 25,19_, Sept. 1966. CONFIDENTIAL - Title Unclassi-
fied.
"A Study of Composite Propulsion System for Advanced Launch Vehicle
A.vp!ications (Main Technical Report) ", Contract NAST-BTV, Marquardt
Report 25,192, Volumes 2 & 3, Sep_ 1966. CONFIDENTIAL - Title Unclassi-fied.
Hrquaror ....o.,=.,,,o..,.
I I.1/RPt /RATIf_
Report Z5,194Volume 7
Page 18
SUPERCHARGED
EJECTOR RAMJET, NO. 11The Supercharged Ejector Ramjet (Engine No. ll,
Class 2 Study Phase) is a 215,000 lbf thrust
(sea level, static) engine with Mach 8 flight
speed capability. The propellants are liquid
hydrogen and liquid oxygen and the engine
normally operates in four progressive modes:
(1) supercharged ejector mode, (2) fan ramjet
mode, (3) subsonic combustion ramjet mode and (k) fan operation mode.
As displayed in this section, the engine has an overall length of 371 in.
(9.4 meters), an overall diameter of 142.5 in. (3.62 meters) and a height maximum
of 165 in. (k.19 meters). The unlnstalled engine weight is ll,9i0 lbm, yielding
a sea level thrust-to-weight ratio of 18.0.
The basic design specifiers for the engine are as follows: Design mass flow ratio
3.0 to l, primary chamber pressure 1500 psia, fan pressure ratio 1o3, maximum
internal pressure 150 psia.
The engine features a single stage retractable tip-turbine fan powered by a twin
airbreathing gas generator installation. The fan bypass ratio is l0 to 1. The
primal, rocket is a regeneratively cooled annular bell configuration featuring
a single toroidal combustion chamber fed by separate hydrogen and oxygen pumps.
The turbopump drive operates on the gas generator cycle using self-pumped propel-
lants. A third hydrogen pump provides fuel to the afterburner, during the super-
charged ejector mode, and thereafter feeds the ramjet combustor during high speed
operations. The afterburner fuel pump is also powered by a hi-propellant gas
generator utilizing self-pumped fuel and pressurized liquid oxygen provided frcm
the vehicle.
The basic engine structural components (mixer, diffuser, afterburner and exit
nozzle) consist of regeneratively cooled assemblies employing a ring-stiffened
Rene' kl wire-wrapped, brazed regenerative Hastelloy X tube bundle construction.
Within the mixer is an _lOngated centerbody which structurally connects a fixed
aft plug with the forward thrust ring. The center body and plug assembly is sup-
ported by a multiplicity of radial low drag fuel injector struts commencing atthe afterburner station. Variable exit geometry is accomplished by means of a
translating ring operating continuously to provide two coaxial flow expansion
compartments between the outer exit bell and the fixed plug. This dual throat
design provides a minimum weight, single moving part design and provides high
nozzle performance.
The engine was sized for a 1 million lbm gross weight, horizontal takeoff, two-
stage launch vehicle. The engine was located in a complement of five (5) along the
bottom side of a high fineness ratio, low drag, lifting body boost stage. Air in-
duction considerations for this installation consisted of a moving ramp, two-
dimensional variable inlet with mixed external and internal compression. The inlet
capture plane was located to make full use of body flow-field affects at speeds in
excess of Mach 3- Exit gas expansion is considered to take place solely within the
exit bell of the engine.
_a//
rquaror ...._,,..,,,o..,.I IX )#I_ _VATh'_
Report 25,194Volume 7
Page 19
Eng. No. 11
Engine OperatingSchematic
l/ I _""_ PilMARY TH UST __
.... ] ,,_,,,_ CHAMBER ASSEMBLY--"
_TURBOPUMP ASSEMBLY
Engine Operating Mode Block Diagrams*
@ X
®
©
@
H
I R I HMD' C EL_._" .j L____ _
H
: : L_._JI. .... J ---
H
,,,,,,, , :---",,,o,,,,[---], , ,0 '----'_ i. .... j I. .... J --- L .... a_
H
xI.-_.- J ......
*Note: Mode numerical coding is given on Page 18, first paragraph,
"R" indicates optional all-rocket mode.
_P
I
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VAN NU1FI. CAiifOINldl
Report 25,194Vohu'ne 7
Page 21
Eng. No. IIWEIGHT STATEMENT - ENGINE NO. ii
Fan Subsystem
Fan AssemblyGas Generators
Frame and Trunnion Unit
Compartment StructureCover
Actuator
Transition Section
Miscellaneous (5_)
12581120
73O36o210
i15
3O67O
4169 ibm
(34.9%)
Primary Rocket Subsystem
Rocket Chamber AssemblySupport Structure
TurbopumpsGas Generator
Ducting and Valves
Starting System
927
316
12788
126
2028
(17.o_)
Mixer/Diffuser/AfterburnerMixerDiffuser
Fuel Injection UnitCombustor
Forward CenterbodyTurbopump and Miscellaneous
io575_o635
315
3OO145
2992(25.1"_)
Exit Nozzle SubsystemExit Bell
Translating Ring Assembly
Fixed PlugActuator UnitMiscellaneous
523
973734!ooll6
2446(2o.5_)
Controls, LinesControl AssembliesValves and Lines
8o225
305(2.5_)
Total Weight, Dry(Thrust = 215,000 ibf)
i1,9_0 ibm (5416 kg)
Thrust/Weight, Uninstalled 18.0
Report Z5Volume 7
Page ZZ
SUPERCHARGEDEJECTORRAMJET (ENGINE NO. 11|PROGRESSIVE OPERATING MODES
(PUMPINGe COOLING AND CONTROL CIRCUITS NOTSHOWN)
1943
SUPERCHARGED EJECTOR MODE
:-:.:-y..:,:.:.:,:-:.:.:.:-:-.":_..:.'..:.:-:.:.:-:-'.:-
H•"":':.'.:::.':::.'.'.i:i.'::::::::::-.'.::::::.
•.$!:i:i@:_-.:: :::::::::: :::::::::
.. $i:::::::::::>.:i:i$::{:!:]:!:]:]:_::.:]:_...'+:...:.:.:.:.:,:.:.:.:.:.:::::.:.:.-.:.:::.:._
:::::::::::::::::::::::::::::::::::::::::::::
-::::_:::_::::::::::::::::::::::::::::c".'-:.:::::.<::::::::::::::::::::::::::::::
•-.::_:!:_:_:_:_:_:_@_$_!:.• .:..:::::: ::: :::::::
============================
•..:.:_:_i?::_i_ii!_!_i_i_:....'_!_i_._i_gi_iii_ii-i_it.:_iiiii.:'.'ii_i.::...'__i_i_!_i_..".'9!!_.
S :i:i.'.:.']:i:.::i:_:i:i:.v....._....4_.....:..:...:..:..:.:...
.,.,.,.....-...........,.,,..,.... ............. "...........:':':!_i_ ii_ii..%."i. .::_..... .... . ......... .................:_:_:_:_$:@!::::.... '"':'. . :.:.5".':i:i:i:_:$::i.';.:!:!:i:.::_:!:_@_"
• :.'.";:'$i:':__$_:_:_::."::::_$:.:i:_:::::.:::
i
FAN RAMJET MODE
R-22, 137
VAN NUV|. CALIPOINIA
Report 25
Volume 7
Page 23
194
SUPERCHARGEDEJECTORRAMJET (ENGINE NO.PROGRESSIVE OPERATING MODES
(PUMPING, COOLING AND CONTROL CIRCUITS NOT
11)
SHOWN)
H 2
RAMJET MODE
H2
FAN
:.:.:;::
_ili!iiii_iiii!i!!i!!i!iiiiiiiii!i!iiiiili!iiii!!iiiiii!iiiiiii!iii!!!ii!i!Y
OPERA TION M 0 D E ...,....,_._..:.
R -22, L 38
.....,..,,,o..,.
__ ._ort 25 1943
Volume 7
Page 24
BASIC PROPELIANT CIRCUIT
SEPJ, ENGINE NO. ii
Eng. No. II
The propellant circuits for Engine No. ll including the pumping, cooling
and primary control elements are displayed on the facing figure. The
engine is supplied hydrogen and oxygen as shown. The airbreathlnggas
generator, which is aerodynmmically coupled to the tip turbine single
stage fan, receives fuel and is controlled for maximum specific horse-
power output.
The three pump units are directly shafted units requiring no gearing.
One gas generator, operating on tapped propellants, is utilized to drive
the primary rocket fuel and oxidizer pump (bottom of figure) to supply
the combustion chamber operating at 1500 psia. A second bipropellant
gasgenerator drives the afterburner fuel pump which provides hydrogen
at an output pressure of 1OOO psia. For the ramjet mode it is required
that auxiliary stored oxidizer be provided to the turbopump gas generator
since oxygen itself is not being pumped in this mode. The primary
rockets are fed through main propellant valves operating in either open
or closed positions. Starting of the primary rocket is accomplished by
turbine blow down from a separate high pressure gaseous hydrogen supply
(not shown). The turbopump exhaust products, being considerably fuel
rich, are conducted into the afterburner of the engine where the excess
fuel is combusted with the induced air. This minimizes the turbopump
drive penalty during the ejector mode. Likewise, the ramjet pump turbine
exhaust is injected into the ramjet combustor. The turbine is therefore
designed for back pressures commensurate with sonic exhaust flow at the
full combustor pressure of 150 psia to preclude back pressure coupling
effects.
The coolant passages consist of two parallel flow circuits to the outer
jacket and to the inner centerbody/plug/nozzle assembly. The outer
engine wall is cooled in two passes first forward and then aft in order
to cool the exit nozzle with warmed hydrogen. The inner cooling circuit
progressively cools the forward centerbody, translating ring and fixed
plug. All coolant flow is injected into the afterburner via the self-
cooled fuel injection struts. Also, the primary rocket external structure
is cooled by regenerative structure during the high speed ramjet mode.
During fan only operation, with little or no plenum burning the engine
is essentially uncooled. For full stoichiometric afterburning (fan ramjet
mode), regenerative cooling of the aft section of the engine is required.
rquardlI t .YAe/4'_4 Y//]W
VAN NUY$. CAUFOINIA
Report 25 194Volume 7
Page 25
Eng. No. ii
mlm
I--'-
61.1
-r.C.Iu,')
I-,-Z
--.I.--.I1.6,1
Q.0
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,,-,,I
dZ
ZI
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R-ZZ, 142
H
rquamr ......,.I I,,YJRICmAI'IfJW
Re .'t25,194Volume 7
Page Z6
Eng. No. 11
OPERATING MODE CONTROL SYSTEM
(BLOCK DIAGRAM)
EJECTOR MODE (NO. 1)
•_. m FAN RAMJET MODE (NO. 2)
.... RAMJET MODE (NO. 3)
.... FAN OPERATION MODE (NO. 4)
OPERATING
MODE
INPUT SIGNAL
CONTROL
LOOP
SELECTOR
FII
t!I
II
COMBUSTOR/
AFTERBURNER
_- CONTROL SYSTEM
I
I _PRLMARYROCKET II CONTROL SYSTEM
I
EXIT NOZZLE
C ONT ROL
SYSTEM
AIRBREATHING
GAS GENERATOR
CONTROL SYSTEM
Engine control is based on manual and/or aut_natic selection of mperating modesvia four active control loops as will be described. The fan subsystem is
controlled to operate at design rpm with protection of both the fan tip-
turbine and the basic gas generator from turbine over-temperature. Retraction
of the fan is effected at mode shift from the fan ramjet to subsonic combus-
tion ramjet mode. The primary rocket is scheduled (pre-orificed) to operate
at design chamber pressure and design oxldizer-to-fuel ratio (8.0 to 1).
The afterburner/combustor controller is designed for operation at an equiva-
lence ratio of l, providing maximum thrust consistent with good performance.
The variable exit nozzle is controlled initially to provide a maximization
of the product of fan pressure ratio and air mass flow (approximately).
Once supersonic flight is reached the variable exit is translated to locate
the inlet nozzle shock at the throat of the inlet. The exit also operates
in an override loop to limit combustor pressure or inlet diffuser pressure
to the maximum design condition of 150 psia.
Report Z5. 194volun_e 7
Page Z 7
Eng. No. 11
COMBUSTOR/AFTERBURNERFUEL CONTROL SYSTEM
I AIRFLOWSENSOR
INPUT
REQ'D
____ EQUIVALENCE FUEL FUELCOMPUTER _ CONTROLLER
AC TUAL
FUEL
FLOW
RATE
I FUELFLOW
SENS OR
The combustor/afterburner fuel control system is a closed loop control system which senses
the air flow rate through the engine and modulates the fuel flow rate to maintain a
required fuel air ratio (_). A signal proportional to air flow is applied at the
equivalence computer which generates a command for the required fuel flow rate. This
signal is compared against a fuel flow rate feedback signal generating an error signal
which is applied at the fuel controller. The fuel controller modulates the fuel flow tonull the error.
ROCKET FEED CONTROLSYSTEM
COMBUSTIONcHAMBER I THROAT
The rocket feed control system is a fixed point control system. A positive feedback
from the pump which is controlled by a metering orifice is supplied to the gas
generator to drive the turbine and pump assembly until the available power is equal to
the required power which is the design condition (full chamber pressure). An external
power source (gas blowdown) is introduced to start the operation of the system.
'A2/V# _H
//I mrquamz ......,,..,,,o..,.I t_Pt _ATIt_
Report 25. 194Volu/ne 7
Page 28I
Eng. No. ii
EXIT NOZZLE CONTROL SYSTEM
J AEROTHERMO-DYNAMIC
FEEDBACK
REF.SHOCK
POSITION
SENSOR &
COMPUTER
PEAK
HOLDING
CONFROLL ER
AC TUATIONSYSTEM
DUCT
FLOW I
RATE J FLOW
J SENSOR
T FANPRESSURE
RATIO
EXIT
NO Z ZLE
AEROTHER/VIO-DYNAMICS
The exit nozzle control system performs two functions, i.e., positions the inlet
shock at its optimum location and maximizes the combination of fan pressure ratio and
duct flow rate by modulating the throat area of the exit nozzle. A pressure signal
indicative of the position of the inlet normal shock is compared against an actual
feedback signal generating an error which is applied at the actuation system to null
the error. The actuation system receives another signal from the peak holding control-
ler to maximize the combination of duct flow and fan pressure ratio. The actuation
system will be designed with the capabilities of selecting the correct signal in theevent there is a conflict between the two commands.
JJrquam[ ....,,.,...,,,o,.,.
Report Z5,194Volume 7
Page Z9
Eng. No. II
AIRBREATHING GAS GENERATOR CONTROL SYSTEM
REF.
ITEMP.SENSOR F
P •
FUEL
SUPPLY
CONTROLLER __GAS GENERAT OR
RPM
The airbreathing gas generator control system which is a closed locp ccntro! zyztem,
maintains the fan speed (RPM) at a selected reference speed by throttling the fuel
rate to the airbreathing gas generator. The reference speed is compared agalnz=
the actual speed (feedback), generating an error which is fed to the fuel sul=l:
controller to modulate fuel flow to the gas generator. This, in turn, controls
the fan speed until the error is nulled. A temperature override loop is included
to limit the temperature of products of combustion from the gas generator and prc=ect
the fan tip-turbine.
_eport 25,194Volume 7
Page 30J
Eng. No. l l
VEHICLE DESIGN - SERJ, ENGINE NO. ll
This figure shows the final Class 2 vehicle design utilizing super-
charged Ejector Ramjet engines. This 1.0 million pound gross weight
lifting body vehicle was determined to be substantially superior in
performance to the other vehicle types considered.
The lifting body shown features high slenderness ratio, elimination of
the second stage base drag through submergence, and attainment of
stabilizing surface at low unit weight. For the BERJ installation the
aft vehicle extension contains no propellants but provides for
increased slenderness ratio. This SERJ Mach 8 vehicle has a complement
of five 215,000-1b SLS thrust engines (1.075 T/W), with a capture areg
of 350 ft 2, integrated beneath the fuselage. The second-stage gross
weight is &_5,05& pounds for Mach 8 first stage cut-off conditions.
The lifting-body configuration employs a modified conical fuselage
where the forebody is a blunted cone with a depth-to-wldth ratio of
0.& at any station. Maximum cross section of the fuselage is at 73
percent of the body length, as measured from the virtual nose (apex).
The fuselage nose radius is one foot, and the body planform area is13,612 ft 2.
The horizontal stabilizer has a leading edge sweep of 65 degrees,
and an area of 2612 ft 2. The airfoil section is double wedge, with
a two-inch leading edge radius. The movable horizontal control sur-
faces comprise 2000 ft2. The horizontal control surface rotates against
the vertical stabilizer with forward extending dorsal fins, to alleviate
the thermal problem associated with the sharp edges of the control sur-
face under high-speed deflected conditions.
.
The twin vertical stabilizers have a total exposed area of 1200 ft 2,
with a leading edge radius of two inches. No toe-ln is provided for
the verticals, rather, a concept of utilizing small outward rudder
deflections to load the surfaces during hypersonic operation where
the control surface lift curve slope is zero at zero deflection is
proposed, in order to maintain minimum vehicle drag. All panel surfaces
have a thickness ratio of 5 percent.
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Report 25,194Volume 7
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Report 25.194Volu_e 7
Page 33
Eng. No. Ii
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Page 34
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Report 25,194Voluyne 7
Page 35
Eng. No. II
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Eng. No. 11
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_eport 25,194Volume 7
Page 44
FAN RAMJET SPECIFIC IMPULSE
Eng. No, ii
4400
4000
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VELOCITY, 1000 ft/sec
I0.2
I I I
0.4 0.6 0.8
FLIGHT VELOCITY_ 1000 m/sec
VAN NUY|. CALIFORNIA
Report 25.194Volun%e 7
Page 45
Eng. No. ii
FAN RAMJET THRU ST
c-o
e-
o,im
E
I--I.u
I--IJjZ
1.4 --
1.2 --
1.0-
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280
240
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..=
o 200o0r-4
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80
40
0
I0
0.5 1.0 1.5
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2.0
ft,/sec
I I I0.2
FLIGHT
0.4 0.6
VELOCITY, I000 m/sec
I0.8
VAN NUV|. C&LIFOflN|A
"-port 25,194Vol_e ?
Page 46
Eng. No. 11
FAN RAMJET CAPTUR E AREA
E
r_<:
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p.r_
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6
5
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3
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FLIGHT MACH NUMBER
_a__//
rquar(/z ...._.,,..,,,o..,.It:f_/v_4TNJ'o
UNCLASSIFIED
This Page Intentionally Blank
. UNCLASSIFIED
VAN NU¥$, CA&IFO|NIA
Report 25. 194Volu_n e 7
Page 47
Eng. No. II
RAMJET SPECIFIC IMPULSE
SUBSONIC COMBUSTION
NO PRESSURE FIELD
4400
4000
¢3
:' 3600
m
m
. 3200L_J¢n.J
0.
-_ 2800
m
=ram
1.1.1" 2400
_ 2000
16000
I0
ALTITUDE,
1 2 3 4 5
FLIGHT VELOCITY, 1000 ft,/sec
I I I0.5 1.0 1.5
FLIGHT VELOCITY, 1000 m/sec
6
I2.0
7 8
J2.5
VAN NU_'S. CAi.fPO|NPA
RA M JET THRU ST
SUBSONIC COMBUSTION
NO PRESSURE FIELD
Report 25,194Volume 7
Page 48
Eng. No. ii
1.4 - 320
1.2
Ult-O
=1.0C0
m
E
_0.8
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'"0.6
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2 3 4 5FLIGHT VELOCITY, 1000 P,./'sec
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FLIGHT VELOCITY, I000 m/sec
6 7
:120
8
Z2.0
I2.5
3800 ........
3600 .......
i:': _'-+'
3,400 ::::::::.;i-: _i-i..... ?+1
fJ :::: ':;;
:::: ....,,, 3200 .... :!i'::T'; ::::
• 3000 i!!:.:'::
(J) :::; ::-:
2800 ........
• o,
eL 2600 .... i!i;(J") :::: ::::
:::: :!!:
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!!!: ;'-'
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.... ,o.,
2000 '-' '_0
VAN NUY|, C&LIPOQN|Ai
RAMJET SPECIFIC IMPULSESUBSONIC: COMBUSTION
EFFECT OF PRESSURE FIELD
port Z5,194Volume 7
Page 49
Eng. No. 11
................ ; ........ !
ii!i: Ni :":i:.'_i: F:.il .... i
'.:'i :-:: 2.--..: :;:: ;:-',c" :::;}
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++..-+__++;++.+_+*+++++++++
7 8
I I ! I I I0 0.5 1.O 1.5 2.0 2.5
FLIGHT VELOCITY, 1000 m/sec
VAN MUY$, ¢ALfFOIINIA
Report 25,194Volume 7
Page 50
Eng. No, 11
RAMJET
SUBSONIC
THRUST
COMBUSTION
EFFECT OF PRESSURE FIELD
3.0
2.5
In
_2;0
iI
_z.5
==
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_ALTITUDE, 1000 ft-:Iii |_!! : :! :: Ii:::i_:::::;::i_! I ii:!::i:I::: :i:;i::ir ' _' :_. f::- I ' ' i300 ,: i: :I. l:-:I ::I::":F:: !.:i: 50 " :: :: :i--: l::..::::_:::r:::!..l: !::I: .I:::: :::I::l::::l::
._ :: . ,:_ :l:_:l::_:li_:!li_:i:::.: I ::::::::::::::::: ::::::::::::::: : :::::::I : ::_:,.;_:" "' 2oo : =:: :I: I::i i:.::ili!!::lii!I;::i:I:i!!::_l i _:!?_ i_i =:i !:;:it.:_;;.i!:.ii_!i!..ii_i_!r:!'ii_:_:_iZ • • :::I: , ::J:.-- •
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100 __:"" ..............................
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O- 0 6 7 8
_:_i::I iil:iiliiilI:i:i}i_i!lii!:l._iiI!:Ii:_:::i_I:i:•
0 1 2 3 4 5
FLIGHT VELOCITY, lOOO ['t/sec
I I I I I I
0 0.5 1.0 1.5 2.0 2..
FLIGHT VELOCITY, I000 m/sec
VAN NUY|, C&L|PO(INI&
R=port 25,194Voltage 7
Page 51
Eng. No. 11
FAN OPERATION SPECIFIC IMPULSE
m
,,.;U3.J
Q.=E!
m
IJ.m
t.)uJG.u3
I--I.iJ
I,.-uJz
24,000
20,000
16,000
12,000
8,000
4,000
12,000
8,000
4,0000
FLIGHT MACH NUMBER
VAN NUTS. CAiiFOINIA
Report 35,194Volume 7
Page 5?
Eng. No. ii
FAN OPERATION THRUST
150 -
30 1 { !: I i:l i' 1 ! 1 i f ; [ . I ; :i t: _PLENUM BURNING (_P = O)t , ':
! '. :: :i i i : j,::: :::; :::: :,'. :::: I ! ": I I t
! t::,: :.::.J:.,: ,"_L2I::ALTITUDE, I000 Ft .
'_ _!,]hi_ii!:i:I:_4,oiri:,l,_i:i0,::i_;l_ii-iii_li:i:!:l:ii: l , I !
200 _ ,:::st:/:151!t;ii:.ii:!!::::;ilii_::i:: I]! _i::
= _iit331t:i:H_3.:t:.--3T.33iFr:_!t]3i:l3T_:!':::rr_!;-:3::i: 71_i :I: !3.5o 13t: 1_:::::3337!_ii:fi:i!t!::::it!!!:.t3i3-t:.:t:i; :433!:i i _ i I i
i:::Nj:l:;iil:iiiti_i;l;7:::tT?iit+:i:t::Li::i;i !I:;i-:::! I: : i :..... _ti3:3lTii::':ii{!iii':i::3!i::-ii :77i37":{:7_17......i_:- ,
i: i_i]_iii,o i l;iiil;Lli/l i;l io - o -_:_!-.--_ii_-_?_ri_i_.-_.-:::_i__
0 0.2 0.4 0.6 0.8 i.0
FLIGHT MACH NUMBER
VAil NUY|, CALIFORNIA
Report Z5,194Volume 7
Page 53
Eng. No. tl
FAN OPERATION SPECIFIC IMPULSE
0
5200
4800
4400
,2Lt),,.I:Da.
m
IJ.m
t_I,,1.1a.0'3
I--LU
I--LI.IZ
4000
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2800 :,:
2400
20000 0.2
.... , ::: ::; .... -_.........
.... ;_i ]_:!...........BURNING (4, =
:::::::::::::::::::::::::::::::::::
,.,a 4
0 20) ::" ::::::"..... ::_.:_
, I000 ft
_36.2
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0.4
,_ _i!!_:il
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:: ;..": ;,,_..::: :,,_ . ,-tr .....
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FLIGHT MACH NUMBER
Report 25,194Volume 7
Page 54
Eng. No. 11
FAN OPERATION THR UST
300 -
200 -
100 -
i
o 00 --0
400-l--I.U,--)
I--I.U
z 300-
200 -
I00 -
O-
60
00
= 0.20)
0.4 0.6 0.8
FLIGHT MACH NUMBER
40
VAN NUlrlI. CALIFORNIA
oft 25 194Volume ?
Page 55
Eng. No. Ii
FAN OPERATION S PECIFIC IMPULSE
¢,)
i
I
_I
¢%.
i
¢,3I
u.i
¢.)UJa.el')
I-.U,.I
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2600
1800
1400
2600
2200
1800
:.: l: : :::::::::::::::::::::: 1:::l::::1:. I: 71::. i..::l:;: ; :: .... :: :.I :;
! LENUM BU NING (_= 0.75)!:_ :t:.:l._::_:_z-:
:_::_!!_!!_ii_:_!_:i::::_::_::i_ii!i!_i_!'_i?:_::ii_::i:_::i:!_:.!_:_i_!i::_i:::,,ii__ _/i!_.!!..................................................... ' ...._......... _ihiii:-:_....... :.l_i::.l_iiili:::!li::iiiii:.ili:.iit:.ii!tiiiF_i:iiii!ii::!it!iii!_ii_i: i!::_tiiii::ii_:_:_:.i_tlilil::!::iF:ii!li_!!ti_iilii!iliiiitiiiliii_iti::!_tii:!'__fiti_:_::I _:::liiii:':I: :::::::::::::::::::::::::::::::::::::::::::::::::::::::::::_,::::_:.::,_:::_::::r:::_:_::_:::'::::'.:::":_": :_ _ _ i!ii.i!i._!i!if_i::!
2200i i Ji_:1iitiiiil_:-::::tiii::ti!iit::ii::r:_ili::ii:l:_ilitii?_ / ..,il_:i_i__i::iF:iii............
ALTITUDE_ 1,000 _ff t: ::!;::::_ =====================_!ii:: :.,,. :..:.:.::::t ::,:_:: :::_:_.,::::
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PLEN ,,L_,,BURNING .(_ = !.00) _::ij':_!::iiii:.-_
: : I! .:1 ' : ;:!i :": ::::::::::::::::::::::::: ::;:t',::; :::; :::: "::: ::::......._............................_........, ........_!!i]:,_:"_::..,_:.,_I:_.._I:_:_I_i_::_::::::::::::I:-:::,.....I:_:.I:::;_:::I_::__i:._.!h.i: :t : X.i_:::t::iiilii::iti::i::l::i!!L_i::_F:iiit!ilit:::::.itliiitil _it_:_.i:_i_ _i!,::i::___'ii_
_.,_r..,::h:: :',::::'.:::_':::
ii::il:/:i::l_i:::_::::M:::i'ii_!i::i::_i::i_iiii!::::;:ti::::t __i"_ _ _::ii:_i!ii!i.i_i_ ::F.ii_i::_:i::i::I::,,_:__t_._t_i!_::i!!_:_i,_i: _i _:::_::_" _i_ i::it:_-
': ..........t":"'*": .....i_i_!i_!iiii'::!:.it!i::!t!i_t::]!itii!::li_i:_!:::_: !_[i!_._-_!.....
i:_. ;:-."1::::_::::- ,_,.-:_._ :_::_::::::'.:!!i"_b'_i ::!i':_.........' ..................:.
.... _ ............... i::'-"_t:::_J:_: :_:::,I=:i:::_ii_ii!Jiiii _!ii ::.: _' ................ ::;: .::_::_', :.*i _:::l.'_:_ '+_ :::; ::::'.:--',::H ";_
!_'-:ih_.:::' _::_:'_. ............
0.2 0.4 0.6 0.8 1.0IO001SIt_ ""_ ::.,i:._..":i_i!_:_.,,HiTi'_'i:=,,_:E_ !!:: ::;
FLIGHT MACH NUMBER
V4N NUV|, CAIIPORNI&
Report 25,194Volume 7
Page 56
Eng. No. ii
FAN OPERATION THRUST
e-
.9,°
000
i--
re.-mI--
I--
-.j
I--
Z
600
4OO
2OO
0
800
600
400
2OO
0
120
8O
4O
i
o 0OOi--(
p-(n
= 200-r-I-
F-LU
160p.WZ
120
8O
40
00
_i_ii__......_ _
1.00) ,
FLIGHT MACH NUMBER
UNC_SSIFIE_D_,-
va_ NUV|. ¢&ilFOIl_ea
This Page Intentionally Blank
UNCLASSIFIE_
VAN NUY|° CAAtQOINIA
Report Z5 194Volume 7
Page 57
Eng. No. II
SUMMARY: SENSITIVITY ANALYSIS - BASES
The performance data shown in the present report, as well as in the
Class 0 and 1 engine documentation (References 1 and 2), was computed
on the basis of a singular set of internal component efflclencies, as
well as stated operating points (e.g., design mass flow ratio, Ws/Wp).Component sensitivity studies were conducted as a major effort withzn
the Class 2 study phase. The bases for the analysis are given here,
followed immediately by the results.
The approach used was to define baseline performance, specific impulse
and thrust (both net Jet), for a reference trajectory. This was
accomplished for each of the engine's operating modes over the normal
range of flight velocities for that mode. It is appropriate here, to
comment to the point that sensitivity studies of trajectory effects,
per se, are already intrinsic in the previously displayed performance
maps.
Proceeding from this basis of specific impulse and thrust discrete
trends, each of the important engine variables was perturbed from the
baseline value, e.g., afterburner combustion efficiency: Baseline
value - 0.95, sensitivity excursions - 0.85 and 1.OO. All of the remain-
ing variables were essentially held at the baseline, or nominal value.
Any exception to this resulted from the engine performance computer
program's automatic compensation characteristics which, in some instances
"retunes" some of the engine internal variables. The extent and impli-
cations of this situation are covered in the main technical report
(Reference 3).
This section presents the following base_.___sfor the sensitivity analysis
results to be given subsequently:
i. Reference trajectories
2. Baseline specific impulse (on reference trajectory)
3. Baseline thrust (on reference trajectory)
_. Ranges of sensitivity variables, with reference to the baseline
values (both curve and tabular presentation)
VAN NUI'|. CAlfllOaNIA
Report 25,194Volume 7
Page 58
Eng. No. Ii
REFER ENCE TRAJECTORYSENSITIVITY ANALYSIS
120
_ = I00
80 /
I--
/40
/20
0 1 2
I I0 0.5
//
3 4 5 6
FLIGHT VELOCITY, 1000 ft/sec! I I
1.0 1.5 2.0
FLIGHT VELOCITY, 1000 m/sec
7
/
8
I2.5
VAN NUF|, CAL|FOIIN|A
Report Z5 194Volume 7
Page 59
Eng. No. Ii
R EFERENCE TRAJECTORYSENSITIVITY ANALYSIS
FAN OPERATION ONLY
5O
f,/}
E
0
LI.I,,-,,
I--i
I--.-I
12
8
4
0
'..=_
=o
m
,3
I--
,-I
4O
3O
2O
10
00
I
0
J
0.2 0.4FLIGHT
I
0.I
FLIGHT
//
/
0.6 0.8VELOCITY, 1000 ftYsec
I0.2
VELOCITY, I000 m/sec
1.0
1
0.3
YAM NUYS. CALIFORNIA
_eport 25,194Volume 7
Page 60
Eng. No.. II
BASELINE SPECIFIC IMPULSEEJECTOR MODE
1000
900u_
E.o
,.o
-- 800
uJu3_J
¢1.:_ 700
tOIJ.m
tO
"' 600o.(/)
I--la.I
_- 500uJz
Jf
//
///
/
///
4000
L0
0.4 0.8 1.2 "I 1.6 2.0
FLIGHT VELOCITY, 1000 ft/sec
I I I0.2 0.4 0.6
FLIGHT VELOCITY, I000 m/sec
2.4
I
0.8
2.8
_T_rTF.rr;_::]FrT--_nrq
VAN _UY$. CALIFORNIA
Report 25, 194Volume 7
Page 61
Eng. No. 11
BASELINE THRUSTEJECTOR MODE
2.0
U1e-0
e-
: 1.50
E
m,,-i-I--
I--i,i": 0.5I-=i,iz
0
500
4OO..0
300
200
I-,LI.I
--I-'-
I00
- 00
I0
0.4
/
f/
f
0.8 1.2 1.6
FLIGHT VELOCITY t 1000
I I0.2 0.4
FLIGHT VELOCITYt I000
2.0 2.4
ft/sec
0.6
m/sec
I0.8
2,8
___/]rquarez ,,. _..,,,.,.,.
It,ltmR_A_i_
Report Z5,194Volume 7
Page 6Z
Eng. No. 11
BASELINE SPECIFIC IMP ULSEFAN RAMJET MODE
4OOO
t,,,}
3600
_. 3200
/i
I.u
.J
m
m
u.
uJ
u')
k-
p-wz
2800
2400 /
2000 /
1600
//
/
/
12000
I
0
0.4 0.8 1.2 1.6 2.0
FLIGHT VELOCITY, I000 ft/'sec
I I I0.2 0.4 0.6
FLIGHT VELOCITY, 1000 m/sec
2.4
I
0.8
2.8
VdN NUYS. CAtlFOIINIA
Report 75 194Volu_ne 7
Page 63
BASELINE THRUSTFAN RAMJET MODE
Eng. No. ii
1,4 --
1.2
O,mJ
1.0c-
o
E 0.8
U3
e,,-rI'-
0.6)--UJ
I-.-uJZ
0.4
0.2
0
28O
240
J
w.,
°o 2000,-4
B
_c0'3
160ew
-_ 120
M-WZ
80
- 40 ¸
|0
/
0.4
//
/
0.8
FLIGHT
I0.2
FLIGHT
//-
/
//
/
1.2 1.6 2.0
VELOCITY, 1000 ft/sec
! |
0.4 0.6
VELOCITY, 1000 m/sec
/
2.4 2.8
I0.8
VAN NUY$, CALIFORNIA
i
}_port 25, 194Volume ?
Page 64
Eng. No. II
BASELINE SPECIFIC IMPULSESUBSONIC COMBUSTION RAMJET
_000
3600
3200
2800
2400
200O
16000
LI
0
i/
f \/ \/ \
/
I0.5
\\\
2 3 4 5
FLIGHT VELOCITY, 1000 ft/sec
I I1.0 1.5
FLIGHT VELOCITY, 1000 m/see
\
6 7
I2.0
\
8
I2.5
VAN NuYS, CALI#O|NIA
Report 25 194
Volume 7
Page 65
Eng. No. 11
BASELINE THRUSTSUBSONIC COMBUSTION RAMJET
1.2
(nm-
:I.0c-oo_
E
I--'0.8or)
m,,-r-l--
l--uJO°6
Z
0.4
0.2
0
280!
"- 240,.Qm
-- 00(Dp4
200k-or)
..p
160W-W
i,lz 120
8O
4O
00
[0
// \
\\
\
1 2 3 4 5
FLIGHT VELOCITY, I000 ff./sec
I I I0.5 1.0 1.5
FLIGHT VELOCITY, 1000 m/sec
\\
\
6
\
7
I2.0
8
I2.5
25,000
SPECIFIC IMPULSEOPERATION
._eport 25,194Volume 7
Page 66
Eng. No. ii
20,000
15,000
U
u_
E
I0,000
--_ 9,000
... 8,000u_
7,000
__ 6,000
,'i" 5,000
I,u
o. 4,000
_ 3,000IIW"Z
2,000
1,500
1,0000
I0
0.2
I0.05
/
PLENUM BURNING, _ -
./
//
0.2
0.4 0.6 0.8 1.0
FLIGHT VELOCITY, 1000 ft./sec
I I I I I0.i0 0.15 0.20 0.25 0.30
FLIGHT VELOCITY, 1000 m/sec
VAN NUY$. I_ALIFOIINfA
Report 25,194Volume 7
Page 67
Eng. No° ii
BASELIN E THRU ST
FAN OPERATION
200
io
o 150c
ooo
ee
Or)-_ 100
I--
I--"' 50
0 00 0.2 0.4 0.6 0.8
FLIGHT VELOCITY, 1000 Pjsec
I I t I I I0 0.05 0.i0 0.15 0.20 0.25
1.0
I0.30
FLIGHT VELOCITY, I000 m/sec
H
rcluamr ....o,,.,.,,,o,.,.
f-k
._eport ZS. 194Volur_e 7
Page 68
SENSITIVITY ANALYSIS RANGES
Ejector Mode:
Inlet - Pressure recovery, Pt2/Pto
Fan - Pressure ratio, PRf
Primary
Equivalence ratio,
Combustion efficiency, _ c*
Nozzle efficiency, W N
Mixer - Mixing efficiency, _ M
Afterburner
Equivalence ratio, _AB
Combustion efficiency, _c
Exit
Nozzle efficiency, N
Exit area ratio, A6/A 5
Fan Ramjet Mode:
Inlet - Pressure recovery, Pt#Pto
Fan - Pressure ratio, PRf
Afterburner
Equivalence ratio, _AB
Combustion efficiency, _ c
Exit
Nozzle efficiency, S N
Exit area ratio, A6/A 5
Subsonic Combustion Ramjet:
Inlet - Pressure recovery, Pt#Pto
Combustor
Equivalence ratio,
Combustion efficiency, _ c
Exit
Nozzle efficiency, W N
Exit area ratio, A6/A 5
Fan Operation:
Inlet - Pressure recovery, Pt2/Pto
Fan - Pressure ratio, PRfAfterburner - Combustion efficiency, _ c
Exit - Nozzle Efficiency,
Eng. No. II
Base-Iline I Range
Figure A
1.30 1.50 i.i0
1.00 l.lO 0.90
0.975 1.O0 0.92
0.98 1.O0 0.95
0.80 1.00 0.50
1.O0 1.50 0.50
0.95 1.00 0.85
0.98 i.oo 0.95
Figure B
Figure A
1.30 1.50 i.i0
1.00 1.50 0.50
0.95 1.00 0.85
0.98 1.oo 0.95
Figure C
Figure A
1.O0 1.50 0.50
0.95 1.O0 0.85
0.98 i.oo 0.95
Figure D
1.oo 0.95 0.9o
1.30 1.50 1.100.95 i.oo 0.85
0.98 1.oo 0.95
VAN NUYS. ¢A&IFO4PIIA
Report 25 194Volume 7
Page 69
Eng. No. II
Figure A INLET PRESSURE RECOVERYSENSITIVITY ANALYSIS RANGE
I--
¢M
m
>-m,,u.i
Q¢Jhi
I,Im,"
O0O0I,Im,"
1.0
0.8
0.6
0.4
0.2
00
I0
RED I ICED \ _SUBSONIC- \ X
REGIME
RECOVERY -
BASELINE
\',,,
\
\NORMALSHOCK
ID
MIL-E-5OO8B%\ -\
7/KE = 0.9_" _"
1
]0.5
2 3 4 5
FLIGHT VELOCITY t lOOO ft/sec
I I1.0 1.5
FLIGHT VELOCITYt I000 m/sec
6 7 8
I2.0
rqu ,_ .c°/1#/m.At_r_
•port 25,194Volume 7
Page 70
Eng. No. Ii
Figure B EXIT NOZZLE AREA RATIOSENSITIVITY ANALYSIS RANGE
EJECTOR MODE
2.8
_D
2.00m
I.--.¢
<:1.6ILl
<
I-"
Xl.2hi
Ul.JNN
°008z
_ v
i
If
,a
.1.25 BL
i/ _ _ • BASELINE CBL)
• f
/ .._ ..L... -_" 0.75 BL/ I
/ /
ql, '"'
0 o
|
0
0.4 0.8
I
0.2
1.2 1.6 2.0FLIGHT VELOCITY, 1000 ft,/sec
I I
0.4 0.6
FLIGHT VELOCITY, 1000 m/sec
2.4 2.8
I
0.8
3.2
I
1.0
VAN NU_|. ¢AL#FOIN/A
Report 25 194Volume 7
Page 71
Eng. No. II
FIGURE C EXIT NOZZLE AREA RATIOSENSITIVITY ANALYSIS RANGE
FAN RAMJET MODE
2.8!
2,4
U3<:
,,o<:
,.2.00m
I--<:ev,
<:16IaJ "ev"<:
I'-
X,.,1.2
-JNNOz0.8
/
J
J
//
/¢
/ f
/ /
/i / // ./
J/
Jv
I
•1.25 BL
" BASELINE (BL)
• 0.75 BL
0.4
I
0
0.4 0.8FLIGHT
I0.2
FLIGHT
1.2 1.6 2.0
VELOCITY, 1000 ftv'seci I
0.4 0.6
VELOCITY, 1000 m/sec
2.4
I
0.8
2.8 3.2
Io0
,_._ .....,.,,.o..,.
,eport 25,194Volume 7
Page 72
Eng. No. Ii
Figure D EXIT NOZZLE AREA RATIOSENSITIVITY ANALYSIS RANGE
SUBSONIC COMBUSTION RAMJET
20U3
,<
,,D,<
,,16Om
I--,<==
< 12ILl
I"
X,,, 8
IJJ--INNOZ
4
00
I0
1
fIp
2 3 4 5
FLIGHT VELOCITY, 1000 ft,/sec
I I
6
12.0
7
0.5 1.0 1.5
FLIGHT VELOCITY, 1000 m/sec
8
I2.5
Report 25.194Volu__e 7
Page 73
SENSITIVITY ANALYSIS - RESULTS
For the reference conditions stated in the previous section, resulting
specific impulse and thrust perturbations are presented here. Performance
is normalized to the baseline trends given over the appropriate flight
velocity ranges.
The specific impulse and thrust data are both displayed on individual sheetsfor each sensitivity variable. On the same sheet, a miniature plot of the
absolute specific impulse and thrust baseline characteristic is shown for
nominal reference purposes. For precise readings, the full-sized curve
appearing previously (its page number is indicated) should be referred to.
The section concludes with a plot reflecting subsystem weight variations
on uninsta/_led engine thrust/weight ratio.
van wilY|, C4¢O#OINIA
INLET PRESSURE RECOVERY
EJECTOR MODE
Report 25,194Voluro e 7
Page 74
EFFECT
kq. If, U _I¢ii
Page 60,....,.,,,..,,.Eng. No. II
|JICl$I ImM
Page 61Og$|Lm! t_m$1tJt_O| moot
1.60
'-'1 i i i i ! i i _ I _ I" I
i__[: _, ! + I : _ I/ i lj-_Vi _ i I : ; i 11,,"] i i}i_l_ Li i I iYL [ i i Ii I J I [ i [IY' ! ] i i 1
i +, tfl i[ i i I tl1.._ i k VE i { ; i i [ i I| ;
'. , i.!. i!, I,+I :. _,!._,!.l,_It w_ll_,, NIl lml
++ ,_ ,_, ,.'+ .,',
I,i..i_ ._lll_ iml
Baseline
PT2/PT0:
Figure A(Page 69)
g" I
I ='+F a __
: r'llHi>-T, iiiii i ii '.'_-l._--+'T t I I I I + I ( I I" i_ I I t I I I I l.J,I l I I I l
..,_-,,,I 1 I I 1 I I ! i ) _ 1 1 I !i " I
i,_iI lll,ii_. _ml ,,.i
=m
1.40
1.2oa,.
_= 1.oo
_1_ 0.80
]°el) {,0
.
1.60
1.40
I,-1.20
==1.oo0 80
O3
0.60
0.400.5
L I
0 0.2
= 0.92
NS __
-- ,gKE = 0.92
1.0 1.5
FLIGHT VELOCITY_
I
0.4
1000
2.0
flVsec
0,6
2.5 3.0
0.8
FLIGHT VELOCITY m/_c
RATIO
MODE
EFFECT
Page ? 5
1.15
I.I0
1.05
1.00
0
0.90
.
1.15
_: I.I04;O_
M-u_ 1.05
= 1.00F-
F--u_ 0.95
O(
F- 0.90
Page 60
'"'"" """' '-'" EngIJ|=TOU _N No. 11
,m i II[ i: : i[Ik_l1_J _ } j _ ; _ I J i/I i I| I i : i i _ i [ ] [i/1 i [ Im...J I _ i i £ i [ /,'I I ] f It It : ii i il/i !I] II|,,,[ ; ; [ [ I L_'! i L I = I i, [i ; ! ! tfi t I I I L :1!.,1 ! i [ I Vi [ ! I [ I I i t:' ! i !_ I I i i i i I _ I_ [ I :_R'I i I I i I i ! ! I
Baseline
PRf = 1.30
!
J! so
I.I0I
1.50
0"850 0.5 1.0 1.5
FLIGHT VELOCITY, I000
I
0I I
0.2 0.4
Page 61
gASltlml rw_us!(JlcTom mo|t
li.ZI i.JP'_
' i""I "F?"
eL
Ii [I IIIll i ! ill
I ! L 1 ; i t L_I_ i J ! i
I I I 1_I_ ! I [ i ! t i i-_li i i I I ! i ! I l
ll!l!liil_i_!!LII!!I llli _ [iiI.!.I.LI!',!.,?._!._.!
mu_ _. ,m e#m
2.0 2.5
ft/sec
I
0.6I
0.8
3.0
FLIGHT VELOCITY, 1000 m/sec
lq
1.02
EQUIVALENCE RATIO
Report 25 194Volu_ne 7
Page 76
EFFECT
EJEC TOR MODE
iml. _ 11
Page 60_S|LII SP[¢IFI¢ l.gVL||
IJlCI_ m@M Eng. No IIPage 61
IASILIU! tUmSl[J[Ct@llmOllI
--l..J
¢._ C.)
r_ia.
1.01
1.00
0.99
llmO
i_
i-II"
i_il 'liILil
] I Y; i I _ i_i i I I i I I
i!iL!lllli ._,,'" . : i L ! ] i i I I
]iiil_ll!!l
# ._ ... L,' _,
Ih
V
Baseline
4,= 1.O0
I.I0
me , ,
"F ._
|_.r!..(I({((_ I , _ I I I|$ I I I ! IAII I I I I I I 1 i
I "t'|.-_-_--_ I I ! I ! I i I I ]. (_ |JlllJllJ JJjJlJ
'"!i"l ' I I I I I lLill t
.C ,t '.!. _.!.',_,I,!._!. I!. I,.
m_Dw ,e_mmw wu .,i,
0.98
O.
1
. ._ ..
__.._ .._ 0.901
,2
k-
l--
p-
k-
1.02
1.00
0.99
0.98
0.97
|0
_y
I.I0
.5
f
1.0 1.5
FLIGHT VELOCITY,
I i
0,2 0,4
1000
0.90
2.0
ft,/sec
I
0.6
2.5
I
0.8
3.0
FLIGHT 1000 m/see
uard! .. +, .,oo°_.' II,Y_/R4/'X_
PRIMARY ROCKET COMBUSTION
EJECTOR MODE
EFFIClENCY
Report 25,194Volume 7
Page 77
EFFECT
I.,i.I¢.¢1
_+n-,
1.06
_I.04LUU_
l.o2__ 1.00
,r 0.98
_ o.96_
0.941.06
_: 1.94el,
l--u'l 1.02 -=3m,.= 1.00l--
h-0.98
,w
:= 0.96
0.94
&0
Page 60
_SlAJN SPI¢IFtC _MA$|IJ|GTg|14111 Eng. No. 11
Baseline
7/. =0.9"/5C
_JI
JI
1.00
I
1.00
0.5
!F;'I!+If-:
&
Page 61
IAStLII! i_nsvll|ci@lm@D!
_ mmmmmm_ mmmmmmmm m
1.0 1.5 2.0
FLIGHT VELOCITY, 1000 ff/sec
I ! I0.2 0.4 0.6
FLIGHT m/sec
2.5
I0.8
3.0
PRIMARY ROCKET NOZZLE EFFICIENCY
EJECTOR MODE
keport Z5 194Volume 7
Page 78i i
EFFECT
Page 60
""'"''"""',.°--- Eng. No. 11
'--i t : i i i t t I I [ I I,_1_!IL!!!111_ IIj--I I i ; I ! ! i i I _ ] ! Il_l i ! t j i i ! iYl I t I I
;-I i i i [ lit i t I ] I J I!_l ; i i I VL [ ] I f ! i I I=--r; i i _ ; i i ! I _ I i t_lI: _ lliilili]li _F"T"_I i i i I J
.[ i.]._ .[,,_ ,[. ; _.r,!. I.!.
Baseline
?7N = 0.98
Page 61I_H&III t#mu, I
l!I. ' " Iz"z i 1 _'_
J• .,'! I "
D.
¢,JE
Ji.o2
__ 1.oo
E 0.98
0.96(/1
0.94
1.06
-- 1,04rs,
_n 1.02
= 1.00h-
0.98
:= 0.96I---
0.94
li_lia_m m _miil_m mmmmm_a
j_
_ m m _lmmmm _
_.,I
_.,,,,... _
|0
5 1.0
FLIGHT
I
0.2
FLIGHT
... 1.00
0.95
1.00
0.95
1.5
VELOCITY,
|0.4
i m
mu
1000
1000
i
2.0
ft/sec
i0.6
m/_ec
---- ...- ..__j--__J
2.5 3.0
I
0.8
VIN NUYS. CIIJFOIIN/A
MIXING EFFICIENCY
EJECTOR MODE
Ixl el, U
Page 60
"'"'""'<,,.,,,........ Eng. No. II
i:
i
I I Z [ J ] _ i i i,g ] ] Ili ! i i I _ i]/ !l ! lI]i i ] ! LIF] Jillri i i f i ;_,'1 l [ I I Ili;IIl/ll; Ill]_l _1 i i ; I I I I[,]" 7 [[[1 ]tll
!i.!.i,!,i,Sl,!.',l,!.I,}.
n.,e..m_ *m
Base Iine
7/a = 0.80
EFFECT
Report 25 194
Volume 7
Page 79
Iq. _ 11
Page 61
IASILIWl fMllSTIJICTO| mO0¢
=.i r
I i,"I*.+!.
"P :+.o!i.i IL w
o i
I l 1I I', I'G_,_'! _I
1'!11 _1111I_ _1o., I.i t._ :.+ ;l z.4 z|
• '- ,.+, ' ,'.= ,.iiqmlln% lm _
T(l) ¢/)-J-- 1.01
0._.
1.00 "
0.99
0.98
0.97
1.03
-- 1.02O:
k-oo 1.01
= 1 O0I--
I--0.99
-T- 0.9p-
I I
0.97 0.5
.I0
1.00
0.50
1.00il
0.50
1.0 1.5 2.0
FLIGHT VELOCI_, 1000 _c
I I, I0.2 0.4 0.6
FLJGHTVELOCi_ )00 _c
i
2.5
I
0.8
3.0
AFTERBURNER EQU IV ALENCE
EJECTOR MODE
RATIO
Report Z5,194Volu_e 7
Page 80i
EFFECT
f_ktl
Page 60 Page 61
""....'""'""' Enq No 11I)|¢141 lIM I_SCLIM IN_LST• • ¢JI¢TN IIO0!
1.15
_1.10
1.05
1.oo
i: Baseline . _llt _(_}
i i i I IFi I _ I i I1 lYl I I I lL ].Icq i I J ¢ 'I _¢_ , [.I II I I I I I LcI_i I I
_. j_ I I 1 1 n..¢'l I I I _ I I I II![ I [ Ii/,i! i ; I I L [1¥' _ i I I I I I i_ffl--_ I I 1 I I I I I i
i;-iltl i Illltilll; i ' l/_ i i i I l t IJ i I I I I 1 I I I I: ._, _ ii_ ..'_"ri-Illli )llli_lll• i I I I I
" ' ":L. '_._','_.,".L ...... ,_-",-,_'-- ',f- .....=:. I _ ,-'o ,L. .'-
0.70 .5 1.0 1.5 2.0 2.5 _.0
FLIGHT _LOCIW, 1000 _c
I I i I i0 0.2 0.4 0.6 0.8
¢1 IP.MT Vl:'l I'IPII"V_ l l_fI m/_u=e
AFTERBURNER COMBUSTION
EJECTOR
EFFICIENCY
MODE
Report 35,194Volume 7
Page 81
EFFECT
u'}u')--I...I
u'3_
1.03
1.02
1.01
1.00
Page 60I_$1LIM SP¢Ct;JC _ULU
EJlCT@ll alOM
, i l!_,ll I!/_[!• IL i T_ I]
i ! iili_/_ If!i r W'!L i]_
! *i i/! _II: /;iI_ J{{
S i ' i i/ ' [ ; { ',I i
iTLii ,i ] LI_i.* a.,
Eng. No.
Baseline
= 0.95C
11
1.00J
I--c¢}
l--
c_
I--
O.
O.
0.
1.03
-- 1.02
1.01
1.00
0.99
0.98
O.
",.,.w
0.85
Page 61_A$|L_mE 1_lusl
1.00
i
0
0.5
__ 0.85I
1.0 1.5
FLIGHT VELOCITY,
| 1 ,,
0.2 0.4
FLIGHT VELOCI
2.0
1000 ft./sec
0.6
)0 m/sec
_mm
2.5
!
0.8
:5.0
VAN Nsrr$. ¢AJlPOQMMi
EXIT NOZZLE EFFICIENCY
EJECTOR MODE
EFFECT
i---..
Report Z5 194)
Volume 7
Pa. ge 8Z
1.06
N
-_ 1.02Q.a.
_m z.oo '
0.941.06
_: 1.04
1_02
z.ooF-
0.98
= 0.96F-
0.94
"i, iU
Page 60
'"""'"''',.,,.,-., Eng. No. ii
l,,r:
!.i.!I"11
[
0
.5 1.0
FLIGHT
I III
0.2
FLIGHT
Page 61|_S|LOml _N|UST
I,I[¢tlle liOl) !
Base line
_/N = 0.98
. "II I I II
I [,,,,I I I I I I/ = I!I111
,_--_.1 ] I ! 1 I|' Illl_l
fll![[tl] I ] L,,,,_ I IIL_]]i]
,,"f"q I I I I _
iii tii,_,L_,_,._,I.,'_,!.
1.00
0.95I
1.00
0.95
I1.5
VELOCITY,
i
0.4
2.0
1000 ft/se¢
I0.6
O0 m/=ec
2.5
!
0.8
3.0
EXIT NOZZLE AREA RATIO EFFECT
Report 2,5 194Voluz'h e 7
Page 83
EJECTOR MODE
Ilq, m U
Page 60
|ISIL¢_ SP(¢Irr{ r_H,S|IJlCT@l m.N
Eng. No. II Page 61
|AStLIUl rwmusrEJlgIOi moll
1.06
I_ 1.04
:r:_ 1.02
Q,. l_.
1.00
c,,)(J,TIE 0.98
I_LIJ_._. 0.96
0.94
1.06
_: 1.04n,,
k-u_ 1.02
" 1.00p-
F- 0.98u'}
" 0.96p-
0 °94
"l ] , : : ! i i i [ ] l [ I I,dt ; i L + iI iv,'rll}-II _i i /li_II ] ] ] t i t !/1 I I I I
W--I C i i I _ i IF'I I I I i 1|..! i + ! t . ',,,t"l I I I I I ], |_, _ 1 I I /I _ [ t I I i I!,.Fh i / l _,"l i i I I I I I I
+-_Fi i!_ll_[ [ ! 1"t' ,.+ ..,' ,+ ,. ,]* ,., t,
m+.l_ ,,ll,l_, lul _,ii
euml, _qumw. imlO._
Baseline
A6/A5: I"[",.,kl.
(Page 701 i'" "i.| _Lw,
.l.
i
J
+ IlItrl i]
t i t t.Jr'l t t I + I _ ]-b.b.-,_ I I I I I i i I l]tllll_tttt ttllIlii I ttl k t ]
rli(E iII[ll]]IIt]! !l
0.5J
1.25 BL _,.,
r-
/
f
._ / _'_ _ Oj 75 BL
1.25 BL! _,
f
__ _?__ 0.75 BL
_-- ---._.
1.0 1.5 2.0
FLIGHT VELOCITY, 1000 ft,/sec
2.5
I I I | I
0 0.2 0.4 0.6 0.8
3.0
FLIGHT VELOCITY 1000 m/see
INLET PRESSURE RECOVERY EFFECT
Report 25,194Volume 7
Page 84i
Page 62|IsCLtm[ SPI¢OFOC JI_'ULSt
_,le nAmJt*l uol!
FAN RAMJET MODE_IL II
Eng. No. II
!
1
Baseline
PT2/PTo:
Figure A(Page 69)
1.60
_o_
_uem_,m_
mu__ 1.40
1.20_ 1.00
u. 0.80 m /__0
_'i [" /a. _. 0.60 f
0.40
1.60
Page 6.3I*S[tOmt I_IUS_PA_ 1,lJll lOlL
i n _ l i
"; '°,, 'o2, _,J ....
A ,I, ,'.. ,L, v.,
1.40
1.2o
1.oo
F- 0.80
= 0.60
0,40
/
.5
/
1.0 1.5 2.0
FLIGHT VELOCITY, 1000 ft./sec
2.5
1 I | I I
0 0.2 0.4 0.6 0.8
0.92
3.0
FLIGHT _/ELOClI_I_O m/see
VAN NUVS. CAL|_O|NJA
FAN PRESSURE RATIO EFFECT
Report: 25,194V 01 _Z.I%'3e {
Page 85
I
FAN RAMJET MODE
Page 62 _" "
..........,..,.-,,,'*..........=,," Eng. No. 11
, ,:,_-',..=--"-:-
Baseline
PRf = 1.30
L.i,
I
i i.o
_t
L
Page 63 .....IA$I_I_I twIi sir_AII llal, l_ll MOOI
i,i
,,q
1.60
1.40
"' _ 1.5o1.2o
'_ 1.00 ---- .....m
,;" 0.80
o6o /0.40
1.60
-- 1.40
_ 1 20_ •
_" 1.00F--
F.- 0.80--(n
= 0.60
0.400.5
/f_
/ 1.10
" I1.0 1.5
FLIGHT VELOCITY,
u_mi m
p j--------
2.0 2.5
1000 ft/sec
3.0
I0
I
0.2i
0.4I
0.6I
0.8
FLIGHT VELOCITY 1000 m/see
EQUIVALENCE RATIO
FAN RAMJET MODE
1.60
1.40
1.20
:_ 1.00
Page 62 _"= "
IASlLlUt SPI¢I_I¢ tmp_Ls!FIk I&mJll ao#!
Eng. No. II *";J
I i,
Baseline :°'_
(_AB = 1.00 _°4I
0.50
1.50
Report ?.5 194Volu/In e 7
Page 86
EFFECT
Page 63 .....I_$[LINI l_lUs?PA_ IA_J[T moo(
_Cl 40"
J,vI'--u_ 1.20
n,,-r-_. 1.00
0.80
,Y= 060I-"
0.40 0
i0
1.50
0.50_ _ / III|
0.5 1.0 1.5 2.0
FLIGHT VELOCITY, 1000 ft/sec! l I
0.2 0.4 0.6
FLIGHT VELOCITY, 1000 m/see
2.5
I
0.8
3.0
V4N NUI'S. CALIFOINfA
AFTERBURNER COMBUSTION EFFICIENCY
Report 25,194Volume 7
Page 87
EFFECT
I..1.,I
E..
f,.;
(,/3
1.15
I.I0
.j 1.0
O.
O
0.95
0.90
0.85
1.15
Page 62
|,slt_.! $PI¢_FI¢ ,IPULS!_Am mJm_(l mOH
FAN RAMJET MODE
Eng. No. II
I"- Ba se!ine _"
;'- _/ = 0.95,. C
v
Page 63 .....|As|_im¢ IwtuS!_i_q mAa*J[l" _oo(
M.o, u. _m
1.00___ BIB
0.85
,.24Jo_
p.oo
c¢
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p-u$
I.I0
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1.00
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0.90
0.85
I
0
1.00
0.85
0.5 1.0 1.5 2.0
FLIGHT VELOCITY, 1000 f't,/sec
I I I
0.2 0.4 0.6
FLIGH_ m/sec
2.5 3.0
I
0.8
VAN NVV$o CAUfOINIAi I
EXIT NOZZLE EFFICIENCY
FAN RAMJET MODE
Page 62 _"" "I_$[_INI SPICIFIC ,ImPUL$!
i,s, |AmJf_ tool)!
_an ,m,a_ry° _m
_ .e.lo_ Lea.
Eng. No. 11
Baseline
_N = 0.98
iI;.!
i
.L
1.06
J
0.9
0
O.!
1.06
.: 1.04
_-_ 1.02
1.00
_" 0.98
= 0.96
0.94
I0
S
I
0.2
1.0 1.5
FLIGHT VELOCITY,
I0.4
1000
Report 25,194Volume 7
Page 88l u l i
EFFECT
Page 63 _,_,,fill&Ill l_lUS1IAh IAmJ(1 mool
1.00
i
LI
0.95
F
1.00
0.95
112.0
i0.6
FLIGHT VELOCITY 1000 m/sec
2.5
!0.8
3.0
VAN MUV$. CAI.IFOilNM
EXIT NOZZLE AREA RATIO EFFECT
Report 25,194Volume 7
Page 89
W,
1.15
I.I0
no.
',JUJ
u_oO
1.00
0.95
0.90
0.85
1.15
_: I.I0
k-_n 1.05
"_ 1.00k--
_" 0.95O0
_" 0.90k-
0.85
Page 62I*$1Lum! SPiCb_l¢ aM*u_s(
_a_ mAIJ[t MOO[
FAN RAMJET MODE
b_ N,L II
Eng. No. III
Figure C(Page 71) I
1.25 BL,/
/
1.25 BL,_
//
0.5
I
Page 63 .....
F*m eAMJ!t mOO[
"__0.75
_ "'_'_ _ 0.75
BL
1.0 1.5 2.0 2.5
FLIGHT VELOCITY, 1000 ft/sec
BL
3.0
| I I I |
0 0.2 0.4 0.6 0.8
FLIGH_O m/sec
Report 25,194_tA_ Volume 7
/A""" __,.,.,,,o.., . .
INLET PRESSURE RECOVERY EFFECT
1.30
1.00
0.80
O.7O
1.30
,.:1.20
u_ I.I0
a
I"
i11.
_m
mw
1.oo-----
090== o.8oI-
f,q. _ II
RAMJET MODE
Page6b Eng. No. 11|A|I&INI SPICOWI(: ImPULI!
Sm|SOeI¢ ¢omluSllom |*mJcT
m m mmmmmmmm m
Baseline J,*
PT2/PTo:II
Figure A ...(Page 69) ._
_._ _.____.___--.__ _
_ _i _'"- I?KE = 0.92
i,..
Page 65 _" "|AStLll( twlU$t
IMllOml¢ ¢OlOIIIllOI |AMJI1
MIL-E-5OO8B
_...--
MIL-E-500
= 0.92
v
3 4 5
FLIGHT VELOCITY, 1000 ft/secI t
1.0 1.5
FLIGHT VELOCITY, 1000 m/sec
O. 70_ I 2
I0.5
I
0
P
_J
J
8Bi
==,--
_JV
_a
6 7 8
I2.0
I2,5
vJN NUY$. ¢ALJlQmN|4
Report Z5 194Volume 7
Page 91n, ,
AFTERBURNER EQUIVALENCE RATIO EFFECT
RAMJET MODE
-,- ,, Page 65 .....
Pag_6_. Eng No. 11 '"...........SU|SO_lC CBM|U$110N IIJ*iJ(Tla|tLim( SPfGI_C I_pULI! •su|somtc COmOUSl;ob tJmJ[T
) i
ll.m t _
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1.20 ----
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0.60
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\
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4)= 1.00
• _9_o_._
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J
1.40
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F- 0.80
F- 0.60
0.40
L
0
i i_ _ m
V
.0.50__
1
I
0.5
2 3 4 5
FLIGHT VELOCITY, 1000I I
['t/see
1.0 1.5
FLIGHT VELOCITY, 1000 m/sec
6 7 8
2.0I
2.5
-J
=__=I
u.
Q.U'}
.......,_,.AFTERBURNER COMBUSTION EFFICIENCY
RAMJET MO DE
Report 25_ 194Volu_e 7
page 92
EFFECT
tick I]
Page6_ Eng. No. IIIAIILI_I SPICIfI¢ IIIPU&$1$wIl_Ii{ G_I_STIO_ IMIJlt
Page 65
lJs[Llm[ 1#|uslIuoswli¢ ¢OIlUSTImI |Jllj[!
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' i [_111IINI I !
i_IL I I N.! 1
t[ ' " ' I ! I N.Iiii Ltill[... III11
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_c = 0,95
L.I,
11.*
Ii"I
i.i
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1.15
"_ I.I0
i.o.:
__ 1.00
-- 0.95
0.90
0.8.=
1.15
,.:I.I0q;
p._n 1.05
n.
= 1 00k- •
_" 0 95
n,= 090
m_
e_
y
m
m
1.00
0.85
1.00
0.85
J
h
I
0.850
I
0
i
I
0.5
2 5 4 5
FLIGHT VELOCITY, 1000 ft/secI i
1.0 1.5
FLIGHT VELOCITY, 1000 m/sec
6
I
2.0
7 8
I
2,5
VAN NUV j. ¢AiI/OIIINiA
Report 25 194Volun_e 7
Page 93
EXIT NOZ ZLE EFFI C IENCY
RAMJET MODE
EFFECT
Page 6hIAiELIm! |_(CIFIC ImPULS[$UlSOmac com|ust*oN |AmJ[T
[a_. ql il
Eng. No. II
I •
,,161:io0000 1 05.,Jlo
=_ 1.00
M_° 0.95 ----
,o,o,0.90a.o.0003
0.85
1.15
i l_U/ I! I I
i ] i /I [ i ] "_ t I_ I I/1 I I i i / N ], i/I ] E i i i i L_,I
| nil]lil/i l iI
illll[ILI ili
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II
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i:!,-m,.
_m
Page 65 .....IAS[LJn[ t.mUSV
m,_,m
0.95
I
1.00 __-
-: I.I0,v
_n 1.05 __
= 1.00p-
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= 0.90t--
0.850
|i
1
I
0
n
I
0.5
2 _ 4
FLIGHT VELOCITY,I
1.0
FLIGHT VELOCITY,
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0
5
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1.5
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1.00
.95 _---
6
ft/sec
I
2.0
m/see
7 8
I
2.5
van NUlrl, C4LWPO|NJA
EXIT NOZZLE AREA RATIO EFFECT
Report Z5_ 194Volur_ e 7
Page 94
RAMJET MODE
Page 62|ASttll| SPl_lfI¢ ImPULS[
SU|S_O( COmOUSIIO* mAm_tTEng, No. ii
Page 65O*$tLIO0! TStUST
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Figure D(Page 72)
1.25
i
I
i
i
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1.25 BL_". _.,.. _._ _ ...._ _
/0.75 BL
2 3 4 5 6 7 8
FLIGHT VELOCITY, 1000 ft/secI i I
2.01.0 1.5
FLIGHT VELOCITY, 1000 m/sec
I
2.5
INLET PRESSURE RECOVERY
Report 25,194Volume 7
Page 95
EFFECT
FANPage 66
_ :_ol .... _-_
1.60
OPERATION
Eng. No. II
Baseline
/ -1PT 2 PTO-
.00
Page 67 .....IA_LaNF r.qusr_AN 0PE_rl0_
ILl
.J
O.U3
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I
u.
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1.40
1.20
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0.
0.40
1.60
1.40
1.20
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0.60_m
0.400
I
0
0.2 0.4 0.6
FLIGHT VELOCITY, 1000I I
0.i 0.2
0.8
ft/sec
1.0
I
0.3
PT 2
PT 0
0.95
0.90
0.95
0.90
0.95
0.900.95
0.90
0.200.200
0
0.20
0.200
0
FLIGHT VELOCITY, 1000 m/sec
INLET PRESSURE RECOVERY
Report 25,194Volume 7
Page 96
EFFECT
Page 66IA$[tOh{ SPIC_FI¢ imPeLS! b,& NIL n
flm OPtaAVO0_
I
:5,_ i
' 4
,.'- I _ _-_'1
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FAN OPERATION
Eng. No. 11
Baseline
- 1.00PT2/PT O-
Page 67 '_" "UA$ILIml iwmu$1_Ah OP[lJIIOh
iI
RI.I.
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PT
1.oo
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Ug
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1.40
1.20
1.00
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0.60
0.400
I0
_ jr
0.95 0.50__ "-" &l.O0
"-- 0.90 0.50
& 1.00
i
0.2 0.4 0.6 0.8
FLIGHT VELOCITY, 1000 ft/se=I I
0.1 0.2
1.0
I
0._
FLIGHT VELOCITY, 1000 m/sec
VAN NUIL CAL|FOmNIA
Report Z5,194Volume 7
Page 97
FAN PRESSURE RATIO EFFECT
i.s,l*
_.o**
c.#') (J')_J_l=L
m u
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Page 66
_*. OPlmAr_O.
[F
=
...i_ } :. L, ,!, o:.......
1.60
OPERATION
Eng. No. II
Baseline
PRf = 1.30
1.40 ----
1.20
Page 67 .....IAS[_N¢ I._USr
PRf 4)AB
__ 1.50 0
-- 1.50
1.00
0.80
0.60
0.40
1.60
1.40__
1.20 ....
0.20
._ I.I0 0.20
I.I0 0
1.50 0
1.00
0.80
0.60
O.
_fI
_Y
I0
0.2 0.4 0.6 0.8
FLIGHT VELOCITY, 1000I I
0.I 0.2
_w/sec
1.50 0.20
I.I0 0.20
I.I0 0
1.0
I
0.3
FLIGHT VELOCITY, !000 m/sec
van I, IUSPS. CJ&IPOINIA
FAN PRESSURE RATIO EFFECT
Report 25,194Volume 7
Page 98
Page 66IAS[LI_t SPICtHC ImpULSt
F_ OP[IAVtak
ii
_ Iom_' _bw Ivwac. * _
|,.-
i.o_,d
o.z o.+ +_* =.l
' °.,% oi= +.h +._ 01,,+ o._+
,.,lJ'+r".jl
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1.60
1.40_-
1.20
1.00
0.80
0.60
0.40
1.60...._
1.40
ew_- 1.20u'l
.- 1.00F--
F- 0.80
" 0.60Zp-
0.400
I0
FAN OPERATION
Eng. No. II
Baseline
PRf = 1.30 l"f!
I"'!
i .L'
.L
Page 67 .....II$ltltl TNIUST
FII OlllAllOk
r,-i..! i i i ! i i _/ ! _ i _ ! + I
I _ ! i'b.l ; I'*._,I
I r'*.i I I i 2>._.- i[ : [ ,7['._11 ! ! }
i I I 11
0.2
FLIGHT
PRf _AB
1.50 0.50
1.50 1.00
_ I.I0 0.50
/ I.i0 1.00
1.50 0.50
1.50 1.00
I.I0 0.50/_'- I.i0 1.00
0.4 0.6 0.8 1.0
VELOCITY, 1000 ft,/secI I I
0.i 0.2 0._
FLIGHT VELOCITY m/sec
- Report Z5 194
Volur_ e 7._/J///
iarqua,,../u._ ....u,,.¢.,,,.,,.,. page99
AFTERBURNER COMBUSTION EFFICIENCY EFFECT
! L=,a_mI +,._m
i +,¢¢G
Page 66|A_tL_"[ _PEClf*¢ tMPULS[
_*N O_I|MTIOm
FAN OPERATION
---_____ ", .-.----T _"
• L. t
, Page 67 .....ii IA$1LIII| t _llu s/
Eng. No. ll ............
Baseline
= 0.95-c
a.es o.to o.xs +.,.i +.+s a.m
I(hen_J.._
uJu_
1.06
1.04
1.02
1.00
0.98
0.96
0.94
1.06
-----.
7_C
1.00
0.85
_AB
0.20
0.20
neI-
(#}
n_
"-rI-
1.04
1.02
1.00
0.98
0.96
0.940
I
0
__..
0.2 0.4 0.6 0.8
FLIGHT VELOCITY, 1000 ft/secI I
0.I 0.2
_---- 1.00
0.85
1.0
0.3
0.20
0.20
FLIGHT m/sec
AFTERBURNER COMBUSTION EFFICIENCY
Report 25,194Volume 7
Page 100
EFFECT '
FANPage 66
fA_ Op[|A11@m
1,1_ Dx = ii
,.h .I° o.h o._,
OPERATION
Eng. No. 11
Baseline
_/ =0.95C
Page 67 .....IA$[LI_I INIUST
_J_ OPlmArt_
"r_,_.,...[[ i !
i,._-',.I J i I'_i
I i°L _, .....,:.,-
._ ,:. ,._, ,!.
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i r-,,,,_l ol
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1.06
1.04
1.02
1.00
0.98
0.96
0.94
1.06
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1.00 0.50
1.00 1.00
0.85 0.50
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1.04
1.02
1.00
0.98
0.96
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I
0
JY
0.2 0.4 0.6 0.8
FLIGHT VELOCITY, 1000 ft/secI I
0.I 0.2
1.00 0.SO
1.00 1.00
0.85 1.00
0.85 0.LO
1.0
I
0.3
FLIGHT VELOCl .000 m/sec
EFFICIENCY EFFECT
Report 25,194Volume 7
Page 101
_109_J.J
ff
page ooIA_(_IM[ _plClF+C 'MPuLSl
rA. O_[IAIlO_
_iii'
1.15
1 .I0
1.05
-=_'_Iz.oo
c_ 0.95
_ 0.90,Jl,,,
0.85
1.15
_: Z .I0
F- 1.0509
"_ 1.00-r-
_- 0.9509
=: 0.90
O.
I
0
FAN OPERATION
Eng. No. Ii
Baseline
"qN -_'= 0.98 +
; .
/I
jl
Page 67 .....
la_t_+NI _weus_F_ oPllallO_
= +.o+ +.1+ +++s +.++ +.z+ +.m
// 1.oo
'F/N
-- 1.00
//
0.95
j_
/I
0.95 0
1.00 0
0
0.20
0.2
FLIGHT
0.20
.--- --- 1.00 0.20
_" '--- ---- 0.95 0.20
0.95 0
1.0
I
0.3
0.4 0.6 0.8
VELOCITY, I000 ff/secI I
0.i 0.2
FLIGHT _ )00 m/sec
EX IT NOZZLE EFFIC IENCY EFFECT
Report 25,194Voluro e 7
Page IOZ
FANPage 66
IA_i_lh! SPfCIIl¢ Im_LSl [_ _A LL
fan OPEmM fDi
a_,oao ; i
i ,.i
rLOT _V,, _ON _
OPERATION
Eng. No. 11
Baseline
_N = 0.98
Page 67 _"*"|A$[LII! TN_US_
I.I i'_! ! I I !_.,i
' ._ ! i i ! i i ,_1l _ _ 1,4 4.1 O,I 1.1
1.06
l_ 1"°4_oo 1.02 _'"_J.J
o.o. 1.00
o_ 0.98
uJ_ 0.96--
0.94
1.06
_N _AB
1.00 0.50
1.00 1.00
.... 0.95 1.000.95 0.50
,.,: 1.04¢l,t
_- 1.02 _
" 1.00:%:I-
_.. 0.98U'}
0= 0.96_-rI-
0.940
I0
1.00 0.50__-_'_ _ __----_" --- 1.00 I.O0
_ _._..._..___. =_. 0.95 !.00"----_--'" 0.95 0.50
0.2 0.4 0.6 0.8 1.0
FLIGHTVELOClW, IO00 _secI I I
0.I 0.2 ,0.3
FLIGHT VELOCITY, 1000 m/see
rquaruz ..._,,._.,,,o..,.
Report 25,194Volume 7
Page 103
Enq, No. 11
EFFECT OF SUBSYSTEM WEIGHT VARIATIONON ENGINE THRUST/WEIGHT
18.8
+ 10 PER CENT WEIGHT VARIATION
18.6
-- 18.4
_- _ OES,_NPO,NT
_" 18.0
LU-J-J
<
(11
zi
z
_z
zi11
SUBSYSTEM __-@,'CONTROLS, LINES _'_-
PRIMARY ROCKET SUBSYS EM I_-
_-(_-IEXIT NOZZLE I SUBSYSTEM " _ (_)-
I t J I k_®--,(_- MIXER/DIFFUSER/AFTERBURNER
i \®__-@- FAN SUBSYSTEM
17.8
17.6
17.4
17.20.90 1.00 I.I0
NORMALIZED SUBSYSTEM WEIGHT
_8.dport 25.194
volun_e 7
Page 104
EFFECT
23+m
I
Eng.
OF SUBSYSTEM WEIGHT VAR IATION
ON ENGINE THRU ST/WEIGHT
50 PER CENT WEIGHT VARIATIONI I I I I
No. 11
22
• \o
/o s,o.
1/! \_i._ I ! , 0
SUBSYSTEM •
17 "_)-CONTROLS, LINES _l _"_.'_' '
-- .r_-PRIMARY ROCKET SUBSYS"EM .
:- _1 i i i i i i i,,\-,,,_16 ---_) EXIT NOZZLE SUBSYSTEM _ _ (_).
_.1 I I I I I I I "_._,_- M IXER/DIFFU SER/ AFT ERBURNER --
15---@ FAN SUBSYSTEM-
140.50 1.00 1o50
NORMALIZED SUBSYSTEM WEIGHT
/V I __ J1/,4Jarquaral ....,,., .,,.o..,.
- iiXiRplkftAtll_
Report 25 194Volume 7
Page 105
SCRAMLACE, NO. 22
The ScramLACE powerplant (Engine No. 22, Class 2
Study Phase) is a 173,000 ibf thrust (sea level
static) engine with Mach 12 flight speed capabil-
ity. The fuel is liquid hydrogen, with an auxil-
iary supply of liquid oxygen required for gas
generator drive purposes. The engine normally
operates in three progressive modes: (i) liquid air cycle ejector mode, (2) sub-
sonic combustion ramjet mode and (3) supersonic combustion ramjet mode. Primarily
because of SCRAMJET considerations, the engine has been packaged in a two dimen-
sional configuration. The uninstalled engine weighs 10,457 lbm, providing a sea
level static thrust/weight ratio of 16.5.
The basic design specifiers are: Design mass flow ratio 1.5 to l, primary chamber
pressure 1000 psia, maximum internal pressure 100 psia, and an air liquefaction
heat exchanger equivalence ratio of 8 to 1. The overall length of the uninstalled
engine is 300 in. (7.65 meters), the width is 142 in. (3.6 meters). The overall
height is 102.5 in. (2.6 meters).
The engine comprises a light-weight air liquefaction heat exchanger assembly con-
sisting of a precooler and condenser unit ducted together in a low pressure shell
constructed of reinforced plastic. All pumps are driven by hi-propellant gas
generators. The heat exchanger assembly is capable of being closed during the
high speed modes.
The primary rocket assembly consists of eleven (ll) regeneratively cooled vertical
two-dimensional linear bell rocket strips. These units act, also_ as mechanical
supports for the supersonic combustion ramjet fuel injectors. Aft of the rectan_a-
lar mixing section and diffuser is another series of cooled vertical struts which
inject the afterburner and subsonic burning ramjet mode fuel.
Exit throat area control is effected by four vertically hinged cooled exit panels
which close from the engine walls and a center structure. This throat variability
is consistent with ramjet (subsonic combustion) and ejector mode performance cited
herein. For supersonic combustion the panels are faired in line providing minimum
drag losses.
All internal engine surfaces are regeneratively cooled during all modes of engine
operation. The basic panel structure of the engine consists of light weight com-
posite structure consisting of a thin-gage, multiple wall internal surface cooled
by double passed hydrogen, supported through a bonded compliant layer of elastro-
meric compound by an externally insulated berryliumhoneycomb structure.
The engine was sized for a 1 million lbm gross weight horizontal takeoff two-stage
launch vehicle. The engine was utilized in a complement of six (6) units mounted
along the bottom side of a high fineness ratio, low drag lifting body design. The
inlet comprised a two-dimensional moving ramp, variable geometry, mixed external
and internal compression unit. Exit gases are considered to be further expanded
during the high speed flight modes against the underside of the vehicle in order
to maximize supersonic combustion ramjet performance.
_a/I
rquanTr ...._.,.:.,,,o,.,.14,YMbM_ATA'3W
Report 25,194Volume 7
Page 106
En_ No, 22
Engine Operating SchematicHEAT MIXER/ COMBUSTOR
..... I EXCHANGER I LDIFFUSERI_ _ .....
= |NL_I 7= --I I-- -_- --IZ _..,A I i ,-.,""4n
F_'_)_.-._""---TU.O,,U.,,ASSEM.LY
Engine Operating Mode Block Diagrams *
®H
®
_HEIL....J
H
J I
IHE_L .... .J
®H
_-_!" 1
I I sII0 '---J
r----, F---'ILl---'l.F---l. xS Ri F: Mo:_--I c I-_ E I-,'_I.-------J JL .... J _ I...-.---.a
r----,r---7L_,_. _, _xI, R : _mO,'--"l C I'_ EL.__J IL .... J _ ,-----
, ,,---,,!.El ,MD, , C:__ _,j L- --J I.___J
--'1 XLom ,J
*Note: Mode numerical coding is given on Page 105,
"R" denotes optional all-rocket mode.
/,
+
F-i
-- IOb.O
i
-L- ....
_0_ 0
Ila.OC _'._S",'-)
f
I
,i
Jl_I
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,_V r_UF.L, fUj_CTOR5 (_Z)
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f
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\
iI
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+" '_,' +i-::-;=,+l_,I
tl I +11_I, +ili+ !!i +jl_,+; :+,
ili! i: :'_
, ++ i +:, lit :ili ' _++J#ii, +I11 it,I :il ,' ti;' JJ/ :iLl=: t
:42.0
io_Va_i Q_r_D m
Report Z5 194Volume 7
Page 108
Air
WEIGHT STATW_MENT - ENGINE NO. 22
Liquefaction SubsystemPrecooler Core
Condenser Core
Forward Shell
Center Shell
Aft Shell
Sump
Boost Pump, Ducting
Catalyst (para/ortho)
Closure and Transition
526
_65
25O284
130
100
307969
53o
3561 ibm
Eng. No. 22
Primary Rocket Subsystem
Rocket Chamber Assembly
Support Structure
TurbopumpsGas Generator Unit
Ducting and Valves
Starting System
Mixer/Diffuser/Afterburner Subsystem
Mixer
Diffuser
Fuel Injection Unit
Combustion Chamber
Miscellaneous
Exit Nozzle Subsystem
Moving Plate Exit Nozzle
Actuation AssemblyExit Nozzle
Miscellanous (5_)
Controls, Lines
Control Assemblies
Valves and Lines
Total Weight, Dry
(Thrust = 173,000 lbf)
Thrust/Weight, Uninstalled
588I089
284
149
76148
605
585460
_95
107
11852_
5_
8o185
233_
(22.3_)
2252
(21.5_)
2025
(19.6 )
265
m
lO, 457 ibm
16.5
(2743 kg)
rquamr __,. o.,,._.
Report 25 194Volume 7 '
Page 109
SCRAMLACE (ENGINENO. 22)
PROGRESSIVE OPERATING MODES
(PUMPING, COOLING AND CONTROL CIRCUITS NOT SHOWN)
H2 _ -.-L-AIR
ii lllliilll 1,- ,_,____-_w_, _.._]_ . all-l i "l" __,_-"_]
":. " " " l |__:_::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::: "::_:::':"_'::_$:':':':+:':':":"
...... •";"":.....:":"'"""".........:__i$_---" E .. ,.i___-:':::::::::,':::.':':-'.'-::-:',:::::::-::,':-:::::'::::-:::':-::-'.,','_; •,-z,:,':-:,:::,.',:':,':-:,:'_-:,:-,',:,:,:.-:,,',.',;,:.:-:,
: ===============================================================r
•. : :::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::]:-:::::::::::::_:_:::::--"-- - ---- --- - ---_'-':::::?::::?:_:::::,'::_:_,!:i$:::'-.:::::_,g_,_'_' ..-$'b:::::::;:::::::_::,:%:$::$i::'-::::::::::::::::::::::::::::::.::':::::
<_:_mili_-i;ili;iii!m_;m_-_.._.._:,::....... ::::::::::::::::::::::::
EJECTOR MODE
====================================
,-:,_, ::::::::::::::::::::::::::::::::::::::
_:,- ,_g.:,','.'::::::-'.'.:::_'-'.'::,:::-',:::,::-.•: _,:_. :_:,:-:'_:,:,:,:-:-:::.:-:,:-:-:,:-:-:,:,:,:-:,:
::,:::::'.::::::::::::::::::::::::::::::::::::::::::::::::
"-':::_iA':';::::::::::::::::::::::::::::::::::::::::::::...======================================================
H2
iiiiii!iiiiiiii!i ..t.
5
SUBSONIC COMBUSTION RAMJET MODE
R ">-' 1 3 c)
Report 25,194Volume 7
Page Ii0
SCRAMLACE (ENGINE NO. 22)
PROGRESSIVE OPERATING MODES
(PUMPING, COOLING AND CONTROL CIRCUITS NOT SHOWN)
H2
SUPERSONIC COMBUSTION RAMJET MODE
::.- OR L-.,-t,IR
i
J_ ':::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::: iiiiii!i!iiiiiiiii!iiiii!!iiiiiiiiiiiiiiii!iii!!
.,_ _,:_i::iiiiiiii_i:,iiiiiiiiiii!'
ROCKET VACUUM MODE
R-22 1 40!
J2
rcuarar ..,,,=.,.
t _ .
.,_port Z5,194Volu_e 7
Page 111
Eng. No. 22
BASIC PROFEI/ANT CIRCUIT
SCRAMIACE, ENGINE NO. 22
The propellant flow circuit including pumps and primary controls
is reflected in the adjoining figure. The circuits shown are
essentially for hydrogen fuel_ the exception being the llne from
the liquid air condenser through the liquid air pump and to the
primary rocket unit and the liquid oxygen auxiliary supply. The
several valve Junctures shown in the propellant circuitry are to
accomodate bypass of fuel a_ appropriate for the individual
operating modes.
Three turbopump assemblies are shown; one for liquid air, the
remaining two for liquid hydrogen. Each pump is directly con-
nected to its drive turbln_ These are driven by bipropellant gas
generators as shown. The lower set of pumps (figure) operates to
provide propellants to the primary rocket and are driven by a
common gas generator. The exhaust products of the gas generator are
injected into the afterburner for further combustion of the fuel
rich gases. A single gas generator is associated with the ramjet
fuel pump which operates during the high speed modes following
primary rocket shutdown. Fuel for the gas generators is self-
pumped, with an auxiliary supply providing the oxidizer as shown.
All hydrogen, once pumped to pressure, passes through the condenser
and the pre-cooler of the air liquefaction unit (in that order)
prior to any other routing. A high pressure circuit of the order
of 2000 psia conducts fuel through the heat exchanger and to the
primary rocket assembly. Liquid air taken from the condenser is
first pumped by an in-sump boost pump from which it goes to the
suction connection of the high pressure liquid air pu_p. The pumped
out liquid air is routed directly to the primary rocket chamber. A
significantly higher flow of hydrogen is applied to the lower pressure
circuit (1000 psla) which, after passing through the heat exchanger,
is used for regenerative cooling of the entire engine. For the lower
speed modes, the hydrogen coolant is collected and injected via the
vertical fuel injection strips in the afterburner region. For super-
sonic combustion ramjet mode operation, the fuel is routed forward to
the region of the primary rocket assembly where fuel injection takes
place in the supersonic air stream. This shift is effected in order to
accomplish combustion at the maximum contraction point in the engine.
/Jrquara[ ...._.,..,,,o..,.
• II,Y_q_I_ATIIgN
Report 25 194Volume 7
Page 112
Eng. No. 22
i
I--
w-1-
I.--Z
..,,.I_.1I.i.I
(D
0,.
m
I
dZ
Zm
ZL_
(
R -22, 141
UN_FIEDi,_-
VMN NUTS, C&tOOOeNIJ
This Page Intentionally Blank
UNCLASSIFIED.
rquardl, lf(.T_9,cf_l_W VAN NUV|, ¢_¢J;OiINIA
Report 25 194
Volume 7
Page 113i i,,
OPERATING MODE CONTROL SYSTEMEng. No. 22
(BLOCK DIAGRAM)
J LIQUID AIRLEVEL
--[ CONTROLSYSTEM
OPERATING_
MODE CONTROL
INPUT LOOP
SIGNAL SELECTOR
EJECTOR MODE (NO. I)
--------- RAMJET MODE (NO. Z)
"---------- SCRAMJET MODE (NO. 3)
r--I
I '
III
II
NORMAL
SHOCK
POSITION
C ON TROL
SYSTEM
ROC KE T
FEED
CONTROL
S YST EM
,,, i
EXIT I
NOZZLE
CONTROL
SYSTEM
FUEL
C ON TROL
SYSTEM
The engine is controlled by manual and/or automatic inputs for mode
selection with several active control loops being used. Primary rocket
control is based on a scheduled or pre-orificed system and has no active
control as such. It is set to operate the system at a chamber pressure
of 1000 psia and an air/fuel ratio of 34 to 1 (stoichiometric). An active
loop controls the liquid air sump level. This is accomplished by propor-
tional control of total hydrogen heat exchanger flow since this controls
the air liquefaction rate. During the ejector mode the afterburner handlesall of the excess hydrogen from the heat exchanger (fuel rich condition).
During subsonic and supersonic combustionj ramjet mode, an active control
establishes a nominal equivalence ratio of stoichiometric burning. This
is accomplished by air and fuel mass flow sensing and consequent fuel
control. The variable exit accomplishes normal shock location in the inlet
throat during supersonic flight speeds. The exit also operates in an over-
ride loop to limit combustor pressure to the maximum design pressure of
100 psia.
Report 25,194Volume 7
Fag e 114
Eng. No. 22
LIQUID AIR LEVEL CONTROLSYSTEM
REF.
_ ,VALVE__ RPMLEVEL
r__)---_ COMB. _-_ TU_mE = PUMPRATE HEAT
EXCH.
SYST.
L. AIR
LEVEL
The liquid air level control system maintains the required liquid air level in the heat
exchanger sump by controlling the flow of total liquid hydrogen through the heat
exchanger, hence to the engine. The error signal which is generated by the difference
between the required and actual level is employed to modulate the output of the gas
generator controlling the speed of the turbine and pump. This results in flow modu-
lation of liquid hydrogen through the heat exchanger to null the error, i.e., to adjust
the air liquefaction rate to that being fed to the primary rocket.
NORMAL SHOCK POSITION CONTROLSYSTEM(EXIT NOZZLE MODULATION)
REF. co poTI oH ACTUATIONINETWORK ASSEMB LY NO Z ZLE
I AEROTHERMODYNAMICS iFEEDBACK
The normal shock position control system modulates the exit nozzle to position the
normal shock in a predetermined optimum location, normally the inlet throat. Pressure
signals indicative of the actual position of the shock are compared against a reference
signal and the error is fed to a computing network which generates the required signal
to the actuation system to null the error. The loop is closed by the aerothermodynamic
feedback on the engine internal air flow.
rquard/ _ ..,,..,,,o,.,.' It,YHIPIIIt,4TIt_ '
ROCKET FEED
Report 25,194Volume 7
Page 115
CONTROL SYSTEM Eng. No. 22
EXIT NOZZLE CONTROL SYSTEM
AREA
_PEAK HHOLDING
CONTROLLER
FLOW RATE
ACTUATIONSYSTEMEXIT INO Z ZLE
I AEROTHERMODYNAMICS
The exit nozzle control system is designed to maximize the combination of exit nozzle
area and air flow rate by modulating the exit nozzle throat area. A signal proportional
to air flow rate ahd exit nozzle area is introduced at the peak holding controller which
signals the actuation system to modulate the exit nozzle actuator to maximizej or peak,
the product of throat area and air flow rate.
FUEL CONTROL SYSTEM
•- 4) INPUT
CONTROLLER I
ACTUAL
FUEL
FLOW
RATE
I FUEL
FLOW
SENSOR
The fuel control system is a closed loop control system which senses the air flow rate
through the engine and modulates the f_,el flow rate to maintain a required fuel air
ratio (_). A signal proportional to air flow is applied at the equivalence computer
which generates a command for the required fuel flow rate. This signal is compared
against a fuel flow rate feedback signal generating the error signal which is applied
at the fuel controller. The fuel controller will then modulate the fuel flow until the
error is nulled.
RePOrt Z5,194Volume 7
Page 116
Eng. No..22
VEHICLE DESIGN - SCRAMIACE, ENGINE NO. 22
This figure shows the final Class 2 vehicle design utilizing ScramLACE
engines. This lifting body vehicle was determined to be substantially
superior in performance to the other vehicle types considered.
The lifting body shown features high slenderness ratio, elimination
of the second stage base drag through submergence, and attainment of
stabilizing surface at low unit weight. The vehicle incorporates an
aft hydrogen tank and a propulsion package consisting of six enginemodules of 173,000-1b thrust each (1.038 T/W), with a 408-ft 2 total
capture area. A vehicle affixed nozzle contour is effected to
accommodate the supersonic combustion mode. The system second-stage
gross weight is 397,573 pounds for Mach l0 cut-off conditions (payload maximum).
The lifting-body configuration employs a modified conical fuselage
where the forebody is a blunted cone with a depth-to-width ratio of
0.h at any station. Maximum cross section of the fuselage is at 73
percent of the body length, as measured from the virtual nose (apex).
The fuselage nose radius is one foot, and the body planform area is
13,612 ft2.
The horizontal stabilizer has a leading edge sweep of 65 degrees, and
an area of 2612 ft 2. The airfoil section is double wedge, with a
two-inch leadingedge radius. The movable horizontal control surfaces
comprise 2000 ft2. The horizontal control surface rotates against the
vertical stabilizer with forward extending dorsal fins, to alleviate
the thermal problem associated with the sharp edges of the control
surface under high-speed deflection conditions.
The twin vertical stabilize_shave a total exposed area of 1200 ft 2,
with a leading edge radius of two inches. No toe-in is provided for
the verticals, rather, a concept of utilizing small outward rudder
deflections to load the surfaces during hypersonic operation where the
control surface lift curve slope is zero at zero deflection is pro-
posed, in order to maintain minimum vehicle drag. All panel surfaces
have a thickness ratio of 5 percent.
i
SECTZO_,A-- A
°
. k
s_c,_oNC- C - ,i ,<.: "
, _)_.• -?..,!_._
" 4,
/' \l i
I
I "sEcT,o.IB- B
-.: ,-
F_
. . -,.
4D_, . •
,5 TA S TA S T A
600 _8,s zo_ A
HYDRC, GEN TANK
'4
I
•_ "; ,'c..'_"_, _" "-'. . , .- . .... _ ," _ . ' " _,. " _, , _--" . _;-.;'_ ..._.:,--, .....-._%_. _"-,,'_R..,'-
• t.i L '_. _
J
¥
V,.] "J_-r_c T
BCDY PLANFORM AREA 136t2 FT _
MORIZ STAB. AREA 20CC FT '_
STU§ 'A/tNG AREA 612 FT _
TOTAL FLANFORM AREA 16;'24 FT _
VERTTCAL FIN AREA 1200 FT _
A¢ 4C}8._ FT ¢
.... °I • I_q_d_r _ _
o _.i _.iD,g_ _ _ _i_ _ _ _i_r_ I,
__..___ L
/
//
jJJ
__.7-- _._._, -_
i l i I,
'_ .L_, _,__ ...... _-----.--_-_- .... =_
- :-------r .... _-', - -r_i i
== ...u .... _;__ ___,../___
/;rI
------ ---_, _---'-"_ _''"" i _'-
i
\
31FT
"_.+._,_++,_",+_.+,_. ..... , .... + " t' , .,, ..-+,.+ ,,..+ + + :+ " • :-+' . '
/
rquara __,:,,,,o...
>..I=.-
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mm
!
:!::
I
Q
Z
O
I,=--Ld..=1Zm
i
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I
Report 25 194Volume 7
Eng.
%
/
%
I iIi <r" -
Page 118
No. 22
YAW NI/YS, ¢ALIFOINI&
Re_rt 25_194Volu_ne 7
Page 119
Eng. No. 22
INLET PRESS URE RECOVERY
i-e,l
!-.
t,i
o
i.ue_
u_u'}I.Ue_
1.0
0.8
0.6
0.4
0.2
00
_:t. "::l _:.':', ::,_ :_:; :::'. _-_,
...... *" .... _-t .....
"'r .... I "fC'?" ........... t .......
.................... i;!!] i_i........ _::: i;.÷_!.=.:-!:::;;::'. ;::! ..,, : :;11
.......................... ' ::! _!_i:;:: ::1; :::-; ::I" :':.: t:::i ....
......... r. i.-.1;.... :;:::C::I +.-
;_i: .... _R! .:_i!:::;:........
;:SU ERSONIC i!:: 2_i:'COMBUSTION _i!i'"'
........ "::: i!!i !_7!_::; ii'!_:=: _ W_.",.......
..... : F-1_,[I-., ............
8 10
L_ i!:i
i!:i ii_:.:_.':i :;:.
:::L':-:::
"::/t ::::
T::,: ,1""
• .2: ,:::-
:;.=.:-[-.-?i
12
INLET MACH NUMBER, M0
VAN NUV| CALIFORNIA
Report 2-5,194Volume 7
Page I;)- 0
Eng. No. 2Z
INLET CAPTURE AREA
6
5
E
"¢ 4I,,0
3t_
I-"W
z 2i
1
0
l
N
W
W
I--O.
I--
Z1
!i!!ii::i..-i_ii_,-_u:':_iiii! INLET ......, _" ,.. !;ii_i+:_i _i i!i':ii II::ICOMBUSTION:.I i::'_;_ '"; ;i_. "_ _ _' ;. ' :_. :;'; ,' ' : :ii : : :i ',:: :ii ::: !: _ :: :;:: :: ::::
, _,.,. f: - .-i, --- I-.SUBSONIC .........................d]; _: ..... ::::': : '!:: ...... _,,,r..... COMBUSTION ::: i:i : i':i i:'i i i;
i;:iii':::i:'i-:.ii"u::::,: e._:::.:t :: i:i il; 'i_i__ii iii !i_i i_i__i_i_:;i _t:i_ _'_ :
_;',;:_":::....""_ii_it'"l":'::'":i!::i.,;_i:._:_;:i;_i;_!.....;:::ii'#_::'::: ::::::::!::_ ' :' t:=: :. :::, ::. :::: :::::::::::::::::::::::: ............i!i..-::.!.__"::=, ::_'.:.:.:::::::::ilia!!ili:!!i!_-_:;:.:::::............._........._..................... :: _:
40 :_:; :,:..:.:.:::: ;::: i_RAMJET OPERATION ili:i!l::;i:.lifi::l!::i::l;_!it:t_;i1_:;I;_:_i_If-''"'.'_.......;_'-.;_:,::.-_I_":::*:::: ;- (A_ LIMIT) !li_i! .:-:-.-:'iI]!i_ii!::llill ;;ilF.i:.I:::.
_ : '::' --' "I'I: ....i " _......'*'.., _,,.,-_u.-_-, ;,: _.::iiM._'-:..-_-'i_l:_: i:::t:: I_:;1_:_:_'::_]'::: :";: :I!; :I!I!!_:
'°' '" '1 .... i" ;,
!ii_.,_ii_.::_.$:_d;_:::i;:_:--::_;i:._-_i_i_ii_i:i::_i_:_t_::i_;_i::t__f-i!i_::i_i:::.[; ::
..... "............................ _......._!i!!!:_!::!I':iiI':!!............... :_!............ ; ......... :.:., _.... {....liill!'_ ...........................................................
............. ii!_=: r::_*!i:.!.i!-:_!_:.ii_if-:.;'l_-::: _il :.
..... :::::::::::::::::::::::::: illi: ::.:::o 2 4 6 8 I0 12
INLET MACH NUMBER, M0
vJN NuVlI, CA&WOII_IA
Report 25,194Volume ?
p_g?Izl
Eng. No. 22
EJECTOR MODE SPECIFIC IMPULSE
4400
4000
o
3600
m 3200
J
-- 2800
W
m 2400
_ 2000Z
1600
12000.5 I.i
FLIGHT
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I I I I I0 0.2 0.4 0.6 0.8
YAW _UV$, CJLJPOIIf4I "L
Report 25,194Volume 7
Page 122
Eng. No. 22
EJECTOR MODE THRU ST
3
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I I I I0.2 0.4 0.6 0.8
FLIGHT VELOGITY_ 1000 m/sec
I
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VAN NI/'rL C&Lfl_NINIA
Report 25,194Volume ?
Page. 123
Eng. No. 22
EJECTOR MODE A IRFLOW
0
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VAN NUVS. CALIFOINI*
EJECTOR MODE CAPTURE AREA
Report 25,194Volm_ne 7
Page 124
Eng. No. 22
8
7
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VAN NUYi, CALIFORNIA
Re, .rt 25,194Volume 7
Page 125
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Page 130
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.port ZS. 194Volu_e 7
Page 131m
ENGINE 22
_ARY DATA
MO WS _ WT A0 AID( A0T
ALTITUDE O. FEET
o.5o 938. 52o. 1458. 2]..99 12.19 34.18
0.75 lllS. 520. 1635. 17.41 8.12 25-53
i .00 1348. 520. 1868. 15.77 6.08 21.85
ALTITUDE - i0000. FEET
0.60 714. 433. _47. 19.50 11.82 31.320.90 910. 520. 1430. 16.56 9.46 26.02
1.20 1231. 520. 1751. 16.79 7.09 23.88
1.4o 1468. 520. 1988. 17.14 6.07 23.21
1.60 1816. 520. 2336. 18.52 5.30 23.82
ALTITUDE - 20000. FEET
O.77 562. 335. 897. 17.24 10.28 27.521.00 693. 419. lll2. 16.41 9.92 26.331.20 852. 520. 1372. 16.78 10.24 27.021.50 ]-191. 520. 171.1. 18.75 8.19 26.94
1.80 16&6. 520. 2166. 21.55 6.81 28.36
ALTITUDE - 30000. FEET
1.17 553. 327. '880. 16.65 9.85 26.50
1.30 6&0. 392. 1032. 17.27 10.58 27.85
1.40 716. _d_0. 1156. 17.93 11.02 28.95
1.50 802. 520. 1322. 18.75 12.16 30.911.90 1297. 520. 1817. 23.88 9.57 33.452.40 2345. 520. 2865. 34.04 7.55 41.59
ALTITUDE - 36000. FEET
1.39 548. 322. 87o. 17.84 10.48 28.321.5o 622. 385. 1007. 18.75 11.61 30.361.6o 700. 426. 1126. 19.75 12.o2 31.77
1.70 789. 478. 1267. 20.9& 12.69 33.63
2.O0 i138. 520. 1658. 25.64 11.72 37.36
2.40 1842. 520. 2362. 34.49 9.74 44.232.80 3004. 520. 3524. 48.03 8.31 56.3_
YAN NUY|, f_AL|fOflN|A
Report 25 194Volume 7
Page 132
ENGINE 22 CONT'D.
SUP_ARY DATA
MO WS WHX WT AO AHX AOT
ALTITUDE - 40000. FEET
1.52 525. 317. 842. 18.92 11.42 30.34
1.65 614. 373. 987. 20.32 12.34 32.66
1.85 782. 478. 1260. 23.08 14.11 37.19
2.00 940. 520. 1460. 25.64 14o18 39.82
2.50 1738. 520. 2258. 37.76 11.30 49.06
3.00 3126. 520. 3646. 56.34 9.37 65.71
ALTITUDE - 50000, FEET
1.86 490. 292. 782. 23.22 13.84 37.06
2.00 583. 347. 930. 25.64 15.26 &0.90
2.10 659. 385. 1044. 27.61 16.13 43.74
2.20 746. 436. 1182. 29.80 17.42 47.22
2.50 1077. 520. 1597. 37.76 18.23 55.99
3.00 1937. 520. 2457. 56.34 15.12 71.46
ALTITUDE - 60000. FEET
2.19 457. 255. 712. 29.57 16.50 46.07
2.25 492. 281. 773. 30.98 17.69 48.67
2.35 556. 304. 860. 33.51 18.32 51.83
2.40 591. 329. 920. 34.87 19.41 54.28
2.70 848. 429. 1277. 44.33 22.43 66.76
3.00 1201. 520. 1721. 56.34 24.39 80.73
ALTITUDE - 70000. FEET
2.53 430. 203. 633. 38.79 18.31 57.10
2.6O 466. 225. 691. 40.91 19.75 60.66
2.70 525. 256. 781. 44.33 21.62 65.95
2.80 590. 294. 884. 48.04 23.94 71.98
2.90 663. 326. 989. 52.03 28.58 77.61
3.00 743. 347. 1090. 56.34 26.31 82.65
RAMJET SPECIFIC IMPULSE
_eport 25,194Volume 7
Page 133
Eng. No. 22
SUBSONIC COMBUSTION
NO PRESSURE FIELD
B
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4000
3600
3200
2800
2400
2000
16000
I0
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_ APPROPRIATE ALTITUDE- VELOCITY__i RANGE PER THRUST PLOT !!
0.5 1.0
FLIGHT VELOCITY,
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m/sec
I2.0
VAN NUV|. CALIFOINtA
Report 25,194Volume 7
Page 134
RAMJET THRUSTEng. No. 22
SUBSONIC COMBUSTION
NO PRESSURE FIELD
1,,4 --
1.2
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FLIGHT VELOCITY, 1000 ft,/sec
I I I0.5 1.0 1.5
FLIGHT VELOCITY, 1000 m/sec
6
f---,
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4000
3800
3600
2400
22000
!
RAMJET SPECIFIC IMPULS ESUBSONIC COMBUSTION
EFFECT OF PRESSURE FIELD
1
FLIGHT
I0
Report Z5_ 194Volu_ne 7
Page 135
Eng. No. 22
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I I !0.5
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YAN HUV|. CAL|FOItN|A
Report 25. 194V olubne 7
Page 136
Eng. No. 22
RAMJET THRUST
SUBSONIC COMBUSTION
EFFECT OF PRESSURE FIELD
3.0 --
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_ALTITUDE, 1000 ft _iP:;;il_i;_l:/:li:i;i_'T:i_:i_:_:: i
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2 3 4 5 6 7
FLIGHT VELOCITY, I000 ff/sec
i::i '::-:- :::F::: i::: :::: :::: '::: :::--:_ :i: ;:::l: :: ;, :._:3"_£.ii.3_:1_i'f_ ....... :-3::
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:::::::::::::::::::::
1
I I 1 1 lO 0.5 1.0 1.5 2.0
FLIGHT VELOCITY, I000 m/sec
VAM MUY|, CAL#@O|MIA
/.. -..,
Report Z5_ !94Volu_e 7
Page 137
Eng. No. 22
RAMJET SPECIFIC IMPULSE
SUPERSONIC COMBUSTION
NO PRESSURE FIELD
3000
2500
I
-- 2000
MJu__J
a.
1500
U.¢.)
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500
05
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'--:::: :::::::::::::::::::::::::: :::I ::::::<:: :::::::::::::::::::::::::::::::::::::::::::::: ! !i i:::: ::ii!i:i---:,::_,,-.::.-::_::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::....j............t ..... t....::-:l:i::.-.,::::.,-::::=_::,:._==============================================....!.._:-I [ I. f-, t...... t ii_:!!!i:::"i:* :
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:'::i":: _:::11=_-==:=":T--:=,--::,=:i:::i:i_'__=-:_':_.=i."_ii!!li_ "=tii i: :::: "::::': i"_' '_ " "=:" ::':::::::::_=, _i:_: _l:
.............. =' :==:= =_'_iii_.........t..._..-_.........,...,.t ..........i .........I.... !;_:I::: ii::_--i...-!t:-=:_..-=..-=-=::i_it!::!.:-L'.-=._.......,.. ................ :....:................ :.............. .";; .... ; _ ...... :".... ;-":=.:i" " ' ;'-':_I'+.............-t.-..1.--,-.-,..,t.,..__.,.,........._i..=.,-t• _ ' ........................." ":::::_÷..:_L:_'-""T_-_=.'_'--_Ti-_._:_:.+=::7=_I::::':=':_::':-:'=:::::"=:":=:::=:::::::!:_..iiiliiT:::_a;::.-.,....,.......:.-,....,..._...............:._.::::::::-:::.::=:::-.:=ii::::]_iiL_iii.::iii._:.:.......... i:=':: ;:'" .... ::: _:_-.
iT..=_f_i_i!.......- .................................... ..........!_i..._.L_i`ii_-_._T_._:._._."_-:!_..i_!_im.._-_.i_i_i.!.i_i_-_!_ii_-_f_7_+_.........,.............. _...... ,...._.................. ,...=::,:--.i:LS=-:5:'-i=_H=_ ::::::::::::::::::::::: ::::: ....... :.,-:.............................................. : .... _... ::
= ":="=':i':'='': ::: :'_-I"='=-':i':" ..... -"i ""i .... !......................[ ]il i ................. i l ]t:":C'Z :T'Ti:Z:. ;7_]'7 " -_;;.]Z;" . { "'i;! ;7_!I---.'_.L_!t?-___AN7_-=_-_f!!fSi-7_'-=!7_"_-__-t_".-'7_-.!i!7" !!_i!iT::I!iTii:_iiiif_::i!7ii;!g::i_t!!-."71!i-:!Iii !i__: _i:!::-_
:. :: =:=-'--,,=_,,-:...............:_-!Ti!ifi77ili_i_t!_::!]_:.=:l::-_:_.i_:.=.-l::_!_l_!::liT_il!ii::::?_i17:___i!_-.-::=#->f_-!:.i;.'__!_L:==gli!i_'_.-7i_'.:iii!_:i::i::i!ii!l::_!lli!_!;-i::_-!'::!::_':::iiii!ii'i!!i'i-_i'_::_ii::-':..ii:'i!i'iii:.li_ _::i!i_ii_=::,=:::=::=: _._"t!!_! "!:.=..u=._ i_iliiif:!i_;z_i-'!i!i .....::iii ii!ili::il!i::_l!iiii_.:-!'i!i::!i:.-!!-ii!-
_=_.:._._'_:_'2__=-"k_..l,.-:=::==:=;.==._::=.:..:.;.=='"__=::_==:'ii::i1::?:_li::-ii_::_:i_!_i:li::::ill!::il_i!_ii[::_=-'.'_-:._i:_li::::-i!iiii:.i:::-i_iii
6 7 8 9 10 11 12
FLIGHT VELOCITY_ 1000 ft/secI I I I I
1.5 2.0 2.5 3.0 3.5
FLIGHT VELOCITY, 1000 m/sec
13
I
4.0
VAN NU¥|. CALIPO|NIA
RAMJET
SUPERSONIC
THRUST
COMBUSTION
Report 25 194)
Volume 7
Page 138
Eng. No. 22
P
NO PRESSURE FIELD
1.2 -
1.0
- 0.8
_=o.6p.
l--hl--j
0.4,,iz
0.2
0
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-- l.IJZ
280
|
240 * :_i % ; : :
' *" ' l::: ! , :liiiii:i:it::ii!ii::ili:::I:iiil!::i_i::iiii:;:i:::i_li!ii!:.::iii
: i I " I J t:; :;;t. I :!_::::t:i ]: li_f::_;iti:::.;Y:,iii;;::it:!ii_l!_i::ii::i;::_;]:::i!fili;i:_;ii! / I ]: "_:t i:i:i:i t l t i ;1_;1:i::;::t?::it!;!t::i!ti:_!l:iil;i:t::!:i;:!':::1:L_
; _6° _ l _ __ :ii:iii::iit{::_:]\t:_:_t; l::_1::;_t_:::! i:l:i:::t:li!:t::!::::tt::i{liiitfiii::t::::::::t:iti!{::l_:iil:_i.... I::!:_i::!i:_
II _ II: t:i: i! i[:i]tti:il:]::I:i..,_ i:i::!: f [::i: :'i::Jiii:.L:iii!::ii:.F:i!l:::i I::[i:L:I/i: : l _ : _ : ' i : { _ : _ : :
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8O
40
[iii! :::+,'i_'::_:_:::_::_::::::::::::::::::::::::
5 6 7 8 9FLIGHT VELOCITY,
!ii::F:lili_li:;it:,:::,::iii_::tiiiit:::::::f!iiii:i]::t!:::!:_i_;;ili:_:::: ;::: =:t::::|:::: :::: :::::::::::::::::::::::::::::::::::::::::::::
0
i::!i;:i]i!ii_-_!ili.i:!!L::i_it::!i!I:::i!!:ii!F:::iil;::-t::!iii!iliti!!ii
_iiiii!!i:
i0 IIi000 ft/sec
::: ":::r::::t:::!i: :: ::::=;:: ::::::F::::::::F::!I::[F:;: ::::i:i::
_iii :iiiili:!!:i,iiii{::i_l::ii:i
12 13
I , I I I I I I
1.5 2.0 2.5 3.0 3.5 4.C
FLIGHT VELOCITY, I000 m/sec
VAN NUVS. CAI.tflOIINJ&
Report 25,194Volume 7
Page 139
Eng. No. 22
RAMJET SPECIFIC IMPULSE
SUPERSONIC COMBUSTION
EFFECT OF PRESSURE FIELD
TRAJECTORY b
3000 L-L:I;I[.I .....
'" , ::':1 .... i!_._ii::z) _: . :; :: !i: il_i} tl;il :I ; ! i: : ! !i:::;!i ii1 : il!l::ii:_t!i!!ii!!!tii::::i::ilhiiiliii_tli::ilii?igi!@-ti!i_
i = :i:i :_i:,::N_:i i:l: i !: : _ _li:ii:, l!:_?i_lili!tiiiilii::i;iiil,i::i::!;iiliiii_iiil::ii!lliliti:.-.:iti_.:.!!!ii2500 I:_.,::::1 I :. ,: ._:t ::I:! ,.::!::,:1::::i=================================================================================
I . 1 ..... ' .......... ; .. .; , ............. '. ..- ;.
,-_ !::i ::! I I:i:t:_ :i:_l::l _t_:_l:ii:it;:l_;it_;si!ii::l!il;l;iiii:;itli:-it_iiit::;i_tii:J;i;ii::ii_livl
-" 2000 =: -_ :: _::t_!!,;_.,_::,_:::J:I. :li_.,_ ............................... ' .............! . !_ !,:: -..,. , ,-i_: :l_:_il_;i!t_:_:li!:.ili:iii!_iiT:i:i!I_iiifi!i! "::.-:.il::::_::::_s_i:_-'ii!,,," _ i: :7i: ::i_i;t!::_il{:._ti!!::l:iiJ: _i::iii::_iF!:t : _ _:'if:"t::!::::t::i:._t::!#!'::i::i::i::il!?iitiiiit::::ifi::iiti!f!i{iliii!
' I !: :_:!i*,iil:i2:l!:_i! :::: : :: Ii:£"_'.._::i !!iii!!:.i! il;ij_ = 0 o AND 4°"
=_. t; ' I:::: "ii_!it_:::::lii?!l?I]I_::1!; :i.i::ili!il :!i: i:.i:,li!!i,..,y ::li:ii._.:_:i:ii _ i-t_i_i:..!TF:git!:.!]:.iii":ii:. • -,,,a.. -: ......... ;;I ...... ......
- 15oo i: _' I :I:::::t!:!l!:!l;i!:l_;!l:__:1::f:::_;t::_:;::;i!ii;i!i;::_:.ii:ii;!i_i;:l!i!:f;__ _:_::!::;;:4!:!' : I :;_I;;:t:::::;I;i_t i/t: _I::_t :l::i!lli_t .ij:::_!ii::i;i::;::i!i:_[ii-ii::li:::!ii: [!?::;-_:-__i_!ii;i :_;
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ad i ! i ! !-T_I!!iF_E[_!H:_'_IE÷__iiii!i i_i!-ii!':u:;ii;ii .....z ...."-" .... " ..... '""" ....... '"' ....... !ii!i!!-! !i!I I _ I | | I II: _:1_]i_i::t! ifi::::::liiiitii::iti_i::t!_if! :_t:i:il_i!:.t::i::.:i::i?it:::_i'::_'iii_,:::!_lSiitii.:-.T-.-::ii.::g_]ii::i 2:;:_i!!iiii:/i!i i:_-;!lig_g_==i
500 ::. iiiiiiiii.liiiii!ililiiiii_i:i';i!i:::.ii_!iilF!ili!iiii!!!ii':_:i!iiii!! t!i]! ::::_::;;::!lik_li_{_i_i_;.i]!iii[iii!!!i'iiii'ii]!!':i]l _IF.I:_÷i:ii;
0
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....._....:...:_I:_.................. ;:_il L_._ .................!....!...! ....t....,..._..... _,.....t,.-.':'::::: :.-:_ :_:..-.,_.=--._ !iiil ::i=,i!!_!i'_:_._i__ :--_"_;5 6 7 8 9 I0 11 12 13
FLIGHT VELOCITY, I000 ft,/secI I I I I I
1.5 2.0 2.5 3.0 3.5 4.0FLIGHT VELOCITY, I000 m/sec
VAN NUS'$. ¢AiWPOIINM
Report Z5,194Volu.m e 7
Page 140
Eng. No. 22
RAMJET THRUST
SUPERSONIC COMBUSTION
EFFECT OF PRESSURE FIELD
TRAJECTORY b
1.0
O'l
_0.8
{
_.0°4
I,,-w
I--wzO.2
0
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_i_i-:_..!L'.'._;_:l_l_:!_:_l_i_i_'_-.i_!_!_ ._:I _ l_:J::_ _ I_:: :, ........:,::-_................. i................... _.................. I _ _ , I _ ii_illl200 ::::!:::;....................... k'_'-:J'"'!' "'l ........... J I. , {ii:" ; , :: ;:;
...................... ;'rq'-1--'" ; .................. , ' : j: :: ..:-: ',!_,_:__'_:_'__:_'_iI:___i.........! _ Ii"ii! .] iiilii] - :; .... ' ...... i...... _'h.... [[i ] ...... ' : .....
':if_i_.-:.i:!_L::iLij::ii_;qiT:_=i#_:!i_#!iii!ii#i_!i::ii:: i::ii:.iit!:.!_ti!i ; :_ ._:::= -
x6o _i_.:i.!_i:iI_ii_!i;:iii_T_:!iiF:ii3!i!_iiiI!:i_i._ij!_!:.i_:i`!_:i:_i:_:_ii :, IL:ii!:.l:_ :i!ii_:lii:: ilii:i_ i_j_i..--_iI.i_j:_!_!_i_i_::_i!_:_i_ii_i!iji!_.:!_:!ii;_!i:::.!_i!;_iiii_i_j__ J !_:ililJi! _ _!!_i LL:!II:.IJiI:L_ii
120 ..:.....'-.':.-- ................... =,.=_,:_, .... :.: ._:,::::_::,:::::::..:_ ._:i:::.::_! . _:t ::_.:,::::-:: :_.
IT::: _ ..... i "i I' '_[..', ... ._...... L ... ............ -.. ....... " ._ .... : ..... _'_ ............... , ......."' _i:i:._:L_-_!_!_,_:_::!:_,_._,_i- z_o::_!_:._I_: _I_ I:_!._4, 'I _! , _::_;_ i !
: :i .....: !ii!:i;
5 6 7 8 9 10 1Z 12 15
FLIGHT VELOCITY, 1000 ft/sec
I l I I I ',
1.5 2.0 2.5 3.0 3.5 4.6
FLIGHT VELOCITY, 1000 m/sec
_a
rquardlVAN NUf|, ¢AIIPOItNIA
i
Report ZS, IVolume
Page I,
Eng. No. 2;
5O
4O
Ul
20m
I0
0
REFERENCE TRAJECTOR IES
SUPERSONIC COMBUSTION RAMJET
160•:.!...._-_;-_....-,1.... :!:.!-:-:!--..-F-;F...,!:,:,_.-..!:_:!.,.!.;:_:4DYNAMICPRESSURE, psf_ 250_
i................................. 5-............................................................ I. ,,L::............I...m.._.L-i ....,.........I..]-..] ........,,,:-..:,...f....I...I...t....L_ ......t I _.!....I..._....I ..;....I ...... ___ ....
;_ :i:1:I=I; .%==:..'" :; ;::: " :':.'I,:. _..:; : :: , . :: ::: : ', "" _' " _,i_: . ,, :::' : :: ::: :::: "" .;..,.,.: .,:",.._.,,,,F=-_..,L.t_,L__.,,_,_..,,: ,.,, ,:,,, ._......._ ...._,,_ .....!_ ....t....._ _i ........
120 '::'::i.=:=.-::- -:::_.:-:::..:r:: .................... _ " _-_
i__,_-'-_:._ii._._..:_ili_ __-_..::,_T:_ ..1............. _,_._, !_::'_;_)::T::.::i):/i 1500..........'......._'" _" _li!_::!!,i!!!,_;ii,ili:t_;_ _ _ _!l!i::_.........;;_;;;_ ::__ 2ooo.:4.
:_;..........a"_,'...... _ : " _' _;i: _ii;::.::ii ....... i "_ ,_ 100 iiii(!i_',_ :.'_itii_Yi)_il:;ii:_:i'_:'r':_ 'ml':: _!:_':".i _.'i!))! _ _ !) iii::-"i_tii:_:::_ '::..... ....... ;_,000_
............ I..... ' ........ _ ........ , ......... I"" _ ..... ::":'_: .... "_ :i: ::: ::::::i:::t::):::::: - ,:::_ .- I_:- :_T : "" '.:" ";::..:_'::.t_.'_::', " .... ':"1 :: : ::/'=1 T::: T._.' _L_ i::i L:_(;::. :: ".':':: i_, _ : . :T::_t:T:I::::L::..::::h:'_::
............................... ......................................i....I.................................................. I ....... _ ......... =-...... I.............................. ] ..................... l ......._...... _ ......L.. _,,,... _ ...... _ 4000 ............ L-.t........t....t....................!......._...........:::; :::- :.._.= =.:=::=:- :--r:::." . :"=: L_.. *:=: _:;';:-L:' ;:.I._i.":;::$ ' ='= .'.;; :::: :::: ;:: '::' :::; :=: ;::: :':, :.::':L;:_':-: :':" :?:" ::;:........ _.......... _ _,_.--: .... _................. _.= ............... I _.................... _...... J ............
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40 !::""::::':::":=:=_'=1 :'.;:::-=_-"-_'=_t 'T_''_]il]::iii'i:._T_::'_=_:'-'''_iii i_ii.... : _=_::=1i:.::!t_:;iitii_iK'.-!t:]_::!/_,:.i!:i!iliI:!::f._iit ii i]::ili::_K4._l::iiiI_::it_ill_iii
::":*:-::-_==:='-.iL_.ii_i=)_i=_:!i-t;i/-:=:,_;:,.:_m_=-_:-:r_;F:i)itihli-i)"_:::';i]!_i7!I!:.:iiii-)_,_:_t_.:;f::t_J_(ifil........................................... _,.,_._......... : :-ii:i;]!::!_::::::_!i::!iii:!_)::i!i!!]]i--:_i]i_i_::)::;i!
20 ':i::i:: :::::::::::::::: ::: ::_::=_:.-. T:":_:_::: h: _!l!iii;!_!i!i li"_iii_i_l!::!!l_!'i1::_i_!iii!i_ i!iii !!i!l_!i l!iiil:!i]: :iili_i_I!::i_!::_!i,iiili-i _i!I:::ili_! _.:_ !._i _!::.._,i_!i ;.:; _iiii,;!_._.._: -:.,; ..... :::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::-F.ii.:_;. :ii!!i-_ii
_.._ r+-_- r_'t'i * "T, -
- 0 _=:=:'_';';";"_:'--'l_="_'_i':'"_':l""=:';:_":':':_; ':.:;'::::;:- =:::_'_"_'_z-='_::=:"._ii_]t]i:.l ::i!il)_':]:#I;:::_:::_,.-,-.::,=:_;;:::::'=:'_:::.::::_,:::..:::,::::="=:':.:":_(:::_ii_}T_f_lii_i. ._.,..,._iii5 6 7 8 9 10 11 12 15
FLIGHT VELOCITY, 1000 ft/sec
I I I I I a J
1.5 2.0 2.5 3.0 5.5 4.C
FLIGHT VELOCITY, 1000 m/sec
rquarar .....,, ..,,,o..,.
Report 25,194Volume 7
Page 142
Eng. No. 22
SUMMARY : SENSITIVITY ANALYSIS - BASES
The performance data shown in the present report, as well as in the
Class 0 and 1 engine documentation (References 1 and 2), was computed
on the basis of a singular set of internal component efficiencies, as
well as stated operating points (e.g., design mass flow ratio, Ws/W_).
Component sensitivity studies were conducted as a major effort withln
the Class 2 study phase. The bases for the analysis are given here,
followed immediately by the results.
The approach used was to define baseline performance_ specific impulse
and thrust (both net Jet), for a reference tra_ector 2. This was
accomplished for each of the engine's operating modes over the normal
range of flight velocities for that mode. It is appropriate here, to
comment to the point that sensitivity studies of trajectory effects,
per se, are already intrinsic in the previously displayed performance
maps.
Proceeding from this basis of specific impulse and thrust discrete
trends, each of the important engine variables was perturbed from the
baseline value, e.g., afterburner combustion efficiency: Baseline
value - 0.95, sensitivity excursions - 0.90 and 1.O0. All of the remain-
ing variables were essentially held at the baseline, or nominal value.
Any exception to this resulted from the engine performance computer
program's automatic compensation characteristics which, in some instances
"retunes" some of the engine internal variables. The extent and impli-
cations of this situation are covered in the main technical report
(Reference 3)-
This section presents the following bases for the sensitivity analysis
results to be given subsequently:
i. Reference trajectories
2. Baseline specific impulse (on reference trajectory)
3. Baseline thrust (on reference trajectory)
4. Ranges of sensitivity variables, with reference to the baseline
values (both curve and tabular presentation)
VAN NUY$. CA|IPOIINIA
Report Z5 194Volume 7
Page 143
Eng. No. 22
REFERENCE TRAJECTORYSENS IT IV ITY ANALY S I S
SUBSONIC COMBUSTION MODES
E
oo
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2 3 4 5
FLIGHT VELOCITY, 1000 _sec
L I !0.5
FLIGHT
6
1.0 1.5
VELOCITY, 1000 m/sec
I2.0
VAN NUY|. CAAtPQIIN#_
Report 25,194Volume ?
Page 144
Eng. No. 22
REFERENCE TRAJECTOR YSENSITIVITY ANALYSIS
SUPERSONIC COMBUSTION RAMJET
140
4O
t_
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s 30
20
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B
120
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FLIGHT VELOCITY, I000
I
2.5 3.0
FLIGHT VELOCITY, 1000
//
/
I0 II 12 13
ff./sec
m/sec
I
3.5 4.0
rquamz....,, .,,,o,.,.I III, IRPI _ATll'_
Report 25,194Volun_e 7
Page 145
Eng. No. 22
BASELINE SPECIFIC IMPULSEEJECTOR MO DE
3600
Em
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2800
2400
2000
1600
12000
_i
0.4 0.8 1.2 1.6
FLIGHT VELOCITY,
/
2.0 2.4
I000 ft/sec
//
2.8 3.2
i0
I0.2
I I0.4 0.6
FLIGHT VELOCITY, 1000 m/sec
10.8
I1.0
VAN NUYS. CALtPOJNIA
Report Z5,194Volume 7
Page 146
Eng. No 22
BASELINE THRUSTEJECTOR MODE
1.6 - 360
,,,1.4c0
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FLIGHT VELOCITY, 1000 ft,/sec
/
2.4
//
2.8 3.2
I0
I I I0.2 0.4 0.6
FLIGHT VELOCITY, 1000 m/sec
I0.8
VAN NUY$. ¢ALIIIOINIA
Report 25 194Volume 7
Page 147
Eng. No. 22
BASELINE SPECIFIC IMPULSESUBSONIC COMBUSTION RAMJET
4400
B
m
=h
LUu3_1
n
u.¢Di.g¢3.¢.D
I-
F-LUZ
4000
3600
3200
2800
2400
2000
1600
//
/ \\\
\\
12000
I0
1 2FLIGHT
3 4 5VELOCITY, 1000 ft/sec
6
I I I I0.5 1.0 1.5 2.0
FLIGHT VELOCITY, 1000 m/sec
VAN NUYS. CALIFO|NIA
Report Z5 1942
Volurn e 7
Page 148
Eng. No. 22
BAS ELINE THRUSTSUBSONIC COMBUSTION RAMJET
240
i000 -
8OO
o4.J
Oo 600O,-4
u3
,,- 400
I-
I-,
F- 200Z
0
.oo /\16o J
F-
_-:=_,,_120 /-_ 80
/ul
4O
00 1 2 3 4
FLIGHT VELOCITY, I000
I I I0 0.5 1.0
FLIGHT VELOCITY, I000
\\
\\
5 6P,.,/sec
L1.5
m/seo
2.0
H
rquarar ... _. ,.,,,o..,.
Report Z5,194Volume 7
Page 149
Eng. No. 22
BASELINESUPERSONIC
SPECIFIC IMPULSECOMBUSTION RAMJET
2800,
O
E2400
w
2000
1600
w
w 1200
Wz
8OO5
\
6
\
7 8 9 10 11
FLIGHT VELOCITY, 1000 ft/_c
12 13
I1.5
!
2.0I I
2.5 3.0
FLIGHT VELOCITY, 1000 m/sec
|_.5
!4.0
VAN NUY|. CAAIPOIINIA
Report 25.194Volu/ne 7
Page 150
Eng. No. 22
BASELINE THRUSTSUPERSONIC COMBUSTION RAMJET
400 -U_
e"0
¢,-
o 300 --00,-I
"_ 200-"-I-l--
1--
100 -l'-LgZ
O-
I00
80
=--I
.60I,,-
Z1-
40k-
l--LIJ
z 20
\
\
0
t1.5
6
I2.0
FLIGHT VELOCITYe
I
2.5
FLIGHT VELOCITY,
#
IIl_=llllllll ila=,... -
1
I000 ft/se¢
i3.0
I000 m/_c
I
3.5
12 13
4°0
n
rCuamr ...,,..,,,o,.,,I r:tk_Pf_ArlfW
SENSITIVITY ANALYSIS RANGES
Ejector Mode:
Inlet - Pressure recovery, Pt#Pto
Heat Exchanger
Equivalence ratio, _HX
Equivalence ratio, _HX
Primary
Equivalence ratio,
Combustion efficiency, _ c*
Nozzle efficiency, _ N
Mixer - Mixing efficiency, _ M
Afterburner
Equivalence ratio, _AB
Equivalence ratio, _ AB
Combustion efficiency, W c
Exit
Nozzle efficiency, W N
Exit area ratio, A6/A 5
Subsonic Combustion BamJet:
Inlet - Pressure recovery, Pt#Pto
Combustor
Equivalence ratio,
Combustion efficiency, W c
Exit
Nozzle efficiency, W N
Exit area ratio, A6/A 5
SupersonicCombustion Ramjet:
Inlet - Pressure recovery, Pt#Pto
Combustor
Equivalence ratio,
Combustion efficiency, _ c
Exit
Nozzle efficiency, 9 N
Exit/Capture area ratio, A6/A c
Base- Iline Range
Figure E
Report 25.194Volu_ne 7
Page 151
Eng. No. 2z
Figure F
Figure G
1.00 i.i0 0.90
0.975 1.00 0.92
0.98 l.OO 0.95
0.8o l.OO 0.50
Figure H
Figure I
0.95 1.oo 0.85
0.98 1.oo 0.95
Figure J
Figure E
1.00 1.50 0.50
0.95 1.O0 0.85
0.98 1.OO o.95
Figure K
Figure L
l.OO o.75 0.5o
o.95 0.9o 0.85
0.98 1.00 0.96
1.50 4.0o 1.oo
Report 25,194Volume 7
Page 15Z
Eng. No. 22
Figure E INLET PRESSURE RECOVERYSENSITIVITY ANALYSIS
0
Q.
M-f:.
>.m_u.i>0(.1i,i
him_
U3U3l,Im,,rt
1.0
0.8
0.6
0.4
0.2
0
,NEI_" SE
I--REDUCED-
SUBSONIC--REGIME
RECOVERY
¢! _.
\\\
' \ _,_, MIL-E-5OO8B
NORMAL\ SHOCK _
\\ %.. "_k_._,: o._
\
0 1
I0
2 3 4 5
FLIGHT VELOCITY, 1000 ft/sec
t I ]0.5 1.0 1.5
FLIGHT VELOCITY, I000 m/sec
6
12.0
'VAN NUY|, CALIPOONIA
_port 25,194Volume 7
Page 1 53
Eng. No. 22
Figure F HEAT EXCHANGER EQUIVALENCE RATIO
SENSITIVITY ANALYSIS RANGE
EJECTOR MODE
X-.i-
m
I--,,¢n,,
LIJ(.,)=,,1.1.1,.,I,,¢_>
O'1.1.1
,vu4
z
0Xu4
U4
10
6
5 0
I0
_.. EL + "_'I.,)CHX
.4
___ BASELINE (BIJ
BL- .vZ.O CHX
1.2 1.6 2.0FLIGHT VELOCITY, lO00 ft,/sec
! I I I0.2 0.4 0.6 0.8
FLIGHT VELOClTYt 1000 m/sec
2.4 2.8 3.2
I1.0
Report 25,194Volume 7
Page 154
Eng. No 22
Figure G HEAT EXCHANGER EQUIVALENCE RATIOSENSITIVITY ANALYSIS RANGE
EJECTOR MODE
EFFECT OF INLET PRESSURE RECOVERY ON _(;OHXFOR CONSTANT LIQUEFIED AIRFLOW
X..p
"e-
c_m
I--<I:n,,.
IJJ
zI.iJ.._1<:_>g
O'ILl
e,,,LI.If,DZ<:.-r
XI.IJ
I.-.-<:I.U"-r"
10
9
7nmm_
//
/
_wmm _m_
//
0.92
•'_'=" F
BASELINE
6
50
I0
0.4 0.8 1.2 1.6 2.0
FLIGHT VELOCITY, 1000 ft/secl l l
0.2 04 0 6
FLIGHT VELOCITY, 1000 m/sec
2.4 2.8
I0.8
3.2
Ii0
VAN NUt'S. CALPFO|NIA
Report 25 lg4Volume 7
Page 155
Eng. No. 22
Figure H AFTERBURNER EQUIVALENCE RATIOSENSITIVITY ANALYSIS RANGE
EJECTOR MODE
6
BASELINE INLET PRESSURE RECOVERY
_5"-
m
Or_J
uJz
_n
Ld
L_.<C
_ _._ BL + " 1.0 CHX
3
.RASELINE @HX
2
1
. . _
00
I0
0.4 0.8 1.2 1.6 2.0 2.4 2.8FLIGHT VELOCIW, ZOO0 _sec
I I ! I0.2 0.4 0.6 0.8
FLIGHT VELOCI_, 1000 m/sec
'¢AN NUI_|o CALIPO|NIA
Report 25,194Voluxne 7
Page 156
Eng. No. 22
Figure I AFTERBURNER EQUIVALENCE RATIOSENSITIVITY ANALYSIS RANGE
EJECTOR MODE
rm<:6
0
m,,
_Q,,=
._ 4 \\
LLI
ILlZr_
rmm-LLII-Ll.<:
3
//
/
%>,, +.. I•_ 4 . _ " HX
' __ _
BASELINE _HX-_
1
00 0.4
I
0
0.8 1.2 1.6 2.0FLIGHT VELOCITY, 1000 ft/sec
i I I0.2 0.4 0.6
FLIGHT VELOCITYo 1000 m/sec
2.4
I
0.8
2.8 3.2
11.0
VAN NUY|° CALIFOa*NIA
_leport 25,194Volume 7
Page 157
Eng. No. 22
Figure J EX IT NOZZLE AREA RAT I0
SENSITIVITY ANALYSIS RANGE
EJECTOR MODE
6
,< 5,,D
'_ Ir
Om
F- 4e,,,,
I,,,I.i
"_ .3I--g
X
IJJ 2NNOz
i Ii il i i
1
/
/
/
mnmnW _ _ _ -- /
_I
O0 0°4 0,8
I I0 0,2
1.2 1.6FLIGHT VELOCITY,
I0.4
FLIGHT VELOCITYa
2.0 2.41000 ft/sec
I0.6
1000 m/sec
2.8 3.2
I !
0.8 1.0
VAN NUVS. CALIFORNIA
Report 25,194Volume 7
Page 158
Eng. No. 22
Figure K EXIT NOZZLE AREA
SENSITIVITY ANALYSIS
RATIO
RANGE
SUBSONIC COMBUSTION RAMJET
24
U3,¢1:
<
0m
.¢Cn.
<LUn-<
k-
XUJ
UJ-JNNOZ
2O
16
12
8
4
00
I0
_mlm
/\%
J,/4
/,
1 2 .3 4 5FLIGHT VELOCITY, I000 ft/sec
I I i0.5 1.0 1.5
FLIGHT VELOCITY, 1000 m/sec
6
I
2.0
VAN NUV'S, CALIFOIINiAu
Eeport 25,194Volume 7
Page 159
Eng. No. 22
Figure LINLET PRESSURE RECOVERY
SENSITIVITY ANALY SIS RANGE
SUPERSONIC COMBUSTION RAMJET
1.0
0I,--
t_
c_JI-.
O.
q,b
>.e,.IJJ
0f.J1.1.1e,-
UJe,-
u')u9I.tJn-IZ.
0.8
0.6
0.4
0.2
05
L
1.5
6
_._ _ _ _ '8 _h.. _
_KE -965 -'-' "
, I7 8 9 10 11 12
FLIGHT VELOCITY, 1000 fV_c
I I I I I
2.0 2.5 3.0 3.5
FLIGHT VELOCITY, 1000 m/sec
13
H
rquamz
Report 25,194Volume 7
Page 160
Eng. No. 22
SENSITIVITY ANALYSIS - RESULTS
For the reference conditions stated in the previous section, resulting
specific impulse and thrust perturbations are presented here. Performance
is normalized to the baseline trends given over the appropriate flight
velocity ranges.
The specific impulse and thrust data are both displayed on individual sheets
for each sensitivity variable. On the same sheet, a miniature plot of the
absolute specific impulse and thrust baseline characteristic is shown for
nominal reference purposes. For precise readings, the full-sized curve
appearing previously (its page number is indicated) should be referred to.
The section concludes with a plot reflecting subsystem weight variations
on uninstalled engine thrust/weight ratio.
m
_J
E.
Is1
Report 25 194rMt.4._ Volur_e 7
Page 161
INLET PRESSURE RECOVERY EFFECT
EJECTOR MODE
Page iI_5 _" _|ASILII[ SP[Ctf*¢ I_UL$[
CslCt_ _@D!
Eng. No.
-'_-I L I ! I i t 1 Z ! t i ] ; I l_z_J_I_:J] Baseline
-1i J
j l'iilJi!llh_l PT2/PTo:_1 1 I i I 1 I I I ! I I_t'l I I I-I 1 t I _ _ I 1 ! t I/l- ! I I I I
I _tt t I tl t t_ri it i _l I Figure EI11 I i I 1.14 _ E { I I 1 ti,.I I ! I 1 _ill {.t I ! I il (Page 152)
... ,1-'I'_! I I i I I I I I I T ! I 11I i *.* i.| iJ l._ I.* I.* I,e =,1
22
|,-
j_
I*
I
a i
:= !
I
r- i
I
A
Page lh6 " " "|_$$LII[ IH|U$1
#. 1.4o-, 1
'riKE = 0.92
u. 0.80P._. 0.60
0,401.60
F-u_
.-I-F-
I--{,o
e,,
1.40
1,20
1.00
0,80
0,60
0,40
!
0
am
'l
mm
,5
_---- _/KE = 0.92
, I
0.2
I
1.0 1.5 2.0
FLIGHT VELOCITY, 1000 ft,/sec
1 !0.4 0.6
m n
2.5
I
0.8
FLIGHT VELOCI' O0 m/sec
i i
EQU I VALENCE RAT I0
EJECTOR MODE
Report 25.194Volur6 e 7
Page 16Z
EFFECT
1.15
_ 1.10uJw i
_!_ 1.o5
__ 1.oo!
._..u._-o.951--I
o.9oi
o.8511.15
0.85
L0
Page IL_5 " " _IaSlL_umt SPt¢IFIC _nPU_S!
i Jl c'I@ll mOOl
]d +tm
| ,,,,,
i-
+,NI
J"F+ i
_+ =.+ 4.1 l.l
_m
i •
I.I0
m
m
1 .I0
0.5 1.0
FLIGHT
I
0.2
FLIGHT
Eng. No.
Baseline
9_ = 1.00
22
Page i£6 '_" °IA$_LIN[ I.|USr
(JlCtOl mOO1
i I II
0.90
_______.n
0.90
1.5 2.0
VELOCITY, I000 ft,/sec
1 I
0.4 0.6
VELOCITY 1000 m/see
mpmm
2.5 3.0
0.8
te
nluan#J JI.Y_'Ir_4F_
PRIMARY
VAN NU¥|, ¢&LIFOINI&
ROCKET
i
COMBUSTION EFFICIENCY
EJECTOR MODE
Report 25, 1 94Volume ?
Page 163i i
EFFECT
Page 145 _""IISILIII SIICIIIC IItVLS|
t Jl_tOl moll
i !!,+""I II i| ._J i i ;
I}. t l
r i j,..,.-
Eng. No. 22
I ] I_'I I
IY[ ili_ .X!!, !+-i ;iii',Is i" i ....
i
i i I I I, 1.1 i+I 31.1
vl&ll_, ;iiii l_m
1.06
o.+ 1uJIm 0.96Q.Q. -
0.94
Baseline
*= 0.975C
!,|,., .I =
. I
Page 146 _ " "Idllll.lll IIIIU It
IJl¢_Ol Hit
1.06
1.041.02
+ __0.98
= o.9a 1 -I n I L _,/
0.94 0.5 1.0 1.5 2.0 2.5 3.0
FLIGHT VELOCITY, 1000 if/see
I , I I I , I0 0.2 0.4 0.6 0.8
1000 m/sec
PRIMARYROCKETNOZZLEEJECTOR
EFFICIENCY
MODE
Page 1_5|ASlL_N! SPt¢4_tC impu_$!
lJ[¢_Qt MOO1
Eng. No. 22
Page 146IASILIN[ r_RUST
lllCtOl moa!
Report 25,194Volume ?
Page 164
EFFECT
1.03
1.02WI,,
1.OlIz._.
____ 1.oo
E:,'T 0.99
a,o. 0.98¢/I_U')
0.97
1.03
_: 1.02
I--_n 1.01
,w
= 1.00p.
p-_n 0.99
= 0.98p-
0.97
I0
Baseline
_N = 0.98
J
i
0,5
j_
1.0 1.5
FLIGHT VELOCITY,
I I
0.2 0.4
FLIGHT VELI
1.00
/_'- 0.95
/
1.00
.._a20.95
2.0 2.5 3.0
I000 ft,/sac
I0.6
000 m/sac
I
0.8
ugln_J_Jd=riO.
_m_m
f.)f.._
,r,rml i
(._uf.}Iiii
{hi cn
/
Report 25 194
_. Volun_e 7
/.4 mKlUOrdl .........,,,=.,. P_ge_6s
MIXING EFFICIENCY EFFECT
EJECTOR MODE
Page 145 _ ""I&sli, ll( $P|¢111c lifgksf
11|¢I01 moil
i ! i i ...r, _1
;-, t. _!!!!!ill_ j,=; ,:,. j,ij.iii2.iL.ii• Ii.I *.z
l,t,llm wl,lCl_. Iiii i_
A ,_, .t. ,L. .'., ,I,n_ll_ _, ,iiol,ii
Eng. No. 22
Baseline
19M = 0.80
Page i_,6|ASILOml lU|USTIJI¢I01 m@|[
!,I"--'.:=.r
;++l.l ,III
J.i.I • ..,.+
;_j
& ,4, ,., 4, ,.,_m,s w. m m
,,2
n,I--
,Y-r-F-
I--(/)
n,..i-
1.06
1.04
1.02
1.00
0.98
0.96
0.94
1.06
1.04
1.02
1.00
0.98
0.96
0.94
m
i
//
i i
--m
_,.,,i._ _
1.00
"-T-o.50
n"--
|
0
/f
i|
/i i
0.5 1.0 1.5 2.0
FLIGHT VELOCITY, 1000 ft,/sec
I I I ,
0.2 0.4 0.6
FLIGHT VELOCI I00 m/see
j,i
zoo__0.50 _.
w._i/"
2.5
I
0.8
m
3.0
HEAT EXCHANGER
EJECTOR
EQUIVALENCE
MODE
RATIO
Page 1_5IASlUlII SPI¢IFI¢ ImpULSl
{JtCt@l mO|l
Wiq
,=1!!Ii iii¸
Illl : : :
I ,
i "3t_l _,i_ p o.4 ' *i
Eng. No. 22
Baseline
4)HXFigure F
(Page 153)
Page 146IASlLSUl _wlust
(_fctom mop(
1.30
UJ
= ..j I.I0
__m 1.oo
°J°IT,;" 0.90
"'"' 0.80D.(_.
0.701.03
7
9
-- 1.02
p.u_ 1.01
= 1.00l--
P" 0.99
= 0.98
0.97
1
0
0.5
9
7-_
1.0 1.5
FLIGHT VELOCITY,
I0.2
I
0.4
I000
I000
/
2.0
ft/sec
0.6
m/see
/
Report Z5,194Volume 7
Page 166
EFFECT
2.5 3.0
I
0.8
_.I_Ir,_cj
,";"T_,.
AFTERBURNER COMBUSTIONii
EFFICIENCY
EJECTOR MOD E
Page 145 _"" °IIAS|LIm¢ SP(l_lfll_ IglPUL$|
I_IClO| moll
Eng. No. 22
Baseline
7/ =0.95C
z.;
i
e_ i l-
i
o., L
Page 146|AStLm! IMn$!
IJIC?OI ION
1.06
1.04
N 1.o21.00
0.98
0.96
0.94
1.06
.: 1.04
a-
P" 1.026")
= 1.00p-
_" 0.98
,w
::: 0.96p-
0,94
0
J_
I
0.5
f
I I
1.0 1.5 2.0
FLIGHT VELOCITY, 1000 ft,/sec
0.2 0.4 0.6
FLIGHT VELO( 1000 m/=ec
I
f
Report 25,194Volume 7
Page 167
EFFECT
1.00
1.00
1
0.85
2.5 S.O
I0.8
VAN NMY$. CAtlPOONM
EXIT NOZZLE EFFICIENCY
EJECTOR MODE
EFFECT
Report 25,194Volurne 7
Page 168
1.06
_|uJ
_.J 1.02
____ 1.oo
°t°,r_. 0.9
LUUJ_._. 0.9¢nu_
0.9
1.06
,c 1.04
F--u_ 1 02_ •
" 1 00
_" 0.98oo
"" 0.96I,-
Page 125 _" =IiilLim( $PI=i_I¢ tmpuis!
[Jiclon moo(
Eng. No. 22 ,.,
Page 126$ASlLbm! t.lU STlilC10e iOOÁ
1.00__
m
m_
1.00__
t.5 1.0 1.5 2.0 2.S
FLIGHT VELOCITY, 1000 ft/sec
i I I I
0 0.2 0.4 0.6
FL_G_T, ,000 m/sec
0.95-"T-"
B.O
I
0.8
/
AREA RATIO
MODEEJECTOR
EFFECT
Report 25_ 194Volur_e 7
Page 169
.J
E
1.06
1,04
..i 1,02
0.
__ l.oo
E 0.98
0.96on
0.94
1.06
1.04
1.o2
1.00
k-0.98
o¢= 0.96
0,94
I0
Page 1_5 _ ""IASILOlll SPECIFIC Im@_L$(
IJICIOI mill[
i -IIIl_1 I I i i [ i I l 1 _ vl I
i I I I !] I I _ _ i /_ i I: II_ till
l_t+ JillI _ i I + I i._ I I i t I i I
i I I i L,,_I t ] i I I i I i I
-r:_,_. i L ] ,!, L L,Ll l ,!.i,!
_, ,_, ,_. _,
Eng. No. 22
Baseline
A6/A5:
Figure J(Page 157)
z;,
0.75 B_,_ _-
1.25 BL /'v/
.5
Ol. 'sBL/f1.25 BL /
/
1.0 1.5
FLIGHT VELOCITY, 1000
I0.2 0.4
FLIGH" 000
2.0
ft/sec
i0.6
m/sec
Page i_6 _""las|Loml 1NIU|T
IJ1¢I_1 moll
2.5
I
0.8
3,0
INLET PRESSURE
RAMJET
RECOVERY
MODE
Report 25,194Volume 7
Page 170
EFFECT
Page 147|_SlLIm! splcJp,¢ i_pu_s!
sulsom_¢ ¢oml_tlOl i_mJHPage 148IASILim[ TWIUS!
_U$$_I¢ C@mO_|tlGI nA@J(r
1.30
F'.o
Ioo__I__ 0.90-l--
°J°uJ,,, 0,80Q,n
0.70
1.30
su_r _tucar,. L_ vm
Eng. No. 22
Baseline I
PT2/ : _-PT 0 i
Figure E _"_(Page 152) !
[
/J/
M IL-E-5OOSB --_ '_ /
KE
IXp-
IX
k-
k-
1.20
I.I0
1.00
0.90
0.80
0.700
L0
J
MIL-E-5OO8B -'_" / /
_KE
I1
= 0.92
0.5
2 3 4 5 6
FLIGHT VELOCITY, 1000 ft/secI I
1.0 1.5
FLIGHT VELOCITY 1000 m/see
7 8
2.0 2®5
COMBUSTOR EQUIVALENCE
RAMJET MODE
RATIO
Report 25 194J
Volu.n'_ e 7
Page 171
EFFECT
1.60
_="J'Ju_l_1.20:Era 1.00
0.80ElL
°F_ _ 0,60'
0.40
1,60
1.40
z.2o
l-¢n 0.80
= 0.60k-
0.40
PB ge 147 " " =
$_|somlc c|=|ust¢om |AmJlt
i i : ; !
i : "N
. i!! !__n,N ! }1,!._ ii
. . I I
'" I [ "
1_-: i i i ' , •
A ", _I, ,2, Z,
0 1 2
I
0I
0.5
Eng. No. 22
Baseline
= 1.00
Page i_ _ " =sal |LOmt tNmU|T
su|s_lc ¢oMlu$_lo_ mLmhll
Ii i i/kTi ] i
I I/i I I_L [ I !
,I vl ! I i'i,I _
] i/ [ I i i : i n i'!
/
i i III] Ii i ] I
_ 0.50
..j--
1.50
1.50
0.50
r.,,... ,.,.._ _. _
3 4 5
FLIGHT VELOCITY, 1000 ft,/secI I
6 7
I
2.01.0 1.5
FLIGHT VELOCITY, 1000 m/see
8
I
2.5
VAN NMY|. CALIFQINtA
COMBUSTOR COMBUSTION EFFICIENCY
RAMJET MODE
Page 147 _ " _lasl%pq! spq¢_i¢ AmP.LS(
su|som4c COMlUST_O_ aAMJlT
Eng. No. 22
Baseline i!
=o.95 j; I
,L
1.15
r 1.1oujluj_U_l_n 1.0 5
..i.Jl
rim..
____ _.oo
(-'__ 0.95u.tu-
uJ[_ o 900.85
i.I
1.00i
__ --" "-------_ _ 0.85
-.:I.I0
F--u', 1.05
" 1.00I,,-
I--u_ 0.95
O_"" 0.90F-
1.00i
_-_ .__ .... 0.85
0.850
I
0
i 2
I
0.5
3 4 5
FLIGHT VELOCITY, 1000I I
ft,/sec
m/sec
Report 25,194Volume 7
Page 17Zii
EFFECT
Page 114.8 ....IA s [L*m! i.llu_1
6 7 8
I
2.0I
2.5
Report 25 194
Volu_e 7
rquardt ....., ., ,.., page73I t,TJll_#Mtl_
EXIT NOZZLE EFFICIENCY EFFECT
RAMJET MODE
Page IL_V "-" "i_SliIIl $_IGlflC mPULSl
iUlSOql¢ COmIUiTIOU e_aill
Eng. No. 22|
1,. Baseline ! "i l"
I/N = 0.98 j.i
lloT mJc_v, ll_ lyre
r_ _ Im• wm
Page 148 ....
|A$|LIq| THinS1lll$OlllC lCIM|U$ltOi llIl[l
,.I I t I i # _ki 1 iI i i i [/! I_] i ' !
_Ill V Ii_, iI ! ] I.,4 ] : !"% i
] 1 _ _ ! ! i i : --i
_1 i I,"I, i i i : ;I!lI![ i Ii,'
.{i!,}_!,_Ji :
.: I.I0
1.05--
1.ooI,-.
0.95
=: 0.90k-
0.850
I
0
_I.00-
|i
___0.95_
_m
_mm_
1.00
.0.95
1 2
I
0.5
3 4 5
FLIGHT VELOCITY, 1000 ft,/se¢I l
1.0 1.5
FLIGHT I000 m/see
6 7 8
!
2.0• I
2.5
AREA RATIO
MODE
EFFECT
Report Z5,194Volume ?
Page 174
Page lit _ _ =|ASEtlml SPt¢IFOC tmPuL|l
SUgI$OIIC Comoustno0o llAmJ{f
• , , m
Eng. No. 22
Baseline
A6/A 5 •
Figure K(Page 158)
1.03
jj,o.(Z)o_..nJ_ 1.01
_o/
_ 0.99 BL //"_/-o981.25 BL
0.97 ' J
1.03
1.02
0¢k-
1.01
=: 1.00k-
k--¢n 0.99
"_ 0.98f-.
0.930
I
0
f
1 I
1 2
I0.5
5 4 5 6
FLIGHT VELOCITY, 1000 ft/secI I
1.0 1.5
FLIGHT 1000 m/sec
Page li8 '__ =
|ASILIN! l.lus_Sul$Omt_ CO_IuSlION IAM*£T
7 8
!
2.0I
2.5
/,, ......,..,,,..,.INLET PRESSURE
SCRAM JET
RECOVERY
MODE
EFFECT
pk
Keport 35 194Volun_e 7
Page 175n
Page ib-9
IalILI_E _Ptc,;l_ u_Pu_S!SuplISOml_ ¢OmIUSllON iAmji1 Eng. No. 22
Page 150 '':
IASILItl IWIUII_,uPtlsomlc ¢olleu$11OlO IAmjI1
,LW_' VtLIC.I,. *IO0 *..
:_+ l'o ZI +'.* ];_ ,,
Baseline
PT2/ :PT 0
Figure L(Page 159 )
ui_ _lUlO_ 10w ,n,
zl, _.i ,_e ,'i ,[.6
1.15
1.05 "-- I'/ = 0.985m KE
1.00 '--" -" " .....
l1.5
•r/KE- 0.985
6 7
I
2.0
965
___ _ I
.,._._,KE = 0.965
8 9 I0 ii
FLIGHT VELOCITY, I000 K/secI I
2.5 3.0
FLIGHT VEL _ITY, 1000 m/see
12
I3.5
13
14.0
%L
COMBUSTOR EQUIVALENCE
Report 25,194Volume 7
Page 176
RATIO EFFECT
SCRAM JET MODE
Page 149
IAS[Llml SPI¢_F_¢ hI*PU_S!SUP[ISOmI_ ¢OmlUST_Ot t*mJlt
[,4 'IL _
Eng. No. 22
Baseline
= io00
Page 150 ....
llSlLI_I twlU$+SU*IRSOmlC Comlustlom lJ_Jlt
I.I
+]+E E 0.9O
_"' 0.80O.Q..(,/)u'1
0
.1
O_i- 1.20u'1
-r 1.00k--
M- 0.80u")
o_ 0.60-v-p.
0.405
I1.5
6
I
2.0
7
I0.75
[0.50
8 9 I0 II
FLIGHT VELOCITY, I000 ft/sacI I 1
2.5 3.0 3.5
FLIGHT VELOCITY, 1000 m/see
12 13
I
4.0
z_eport 25 i94
rs_ Volu_e 7
:muv_ n ' , , Page 177/A mrquorm .....,,.,,,..,.
COMBUSTOR COMBUSTION EFFICIENCY EFFECT "_
SCRAM JET MODE
1.1
"_ I.I0
__ _.oo_1__--.i_
°1°I,.u I.uD,. O..u') (.f)
I,,,,-
I=:
).-
I-,.
:Z:I-,-
Page 149 " " _ Page 150 _"= *
IA$1LOII! "*IIv S_suplltsoui¢ ¢om_usllom t_lJ_oJ$Itl.[ s*,tc*Ft¢ I_puts¢
""'""" .......'..... Eng. No. 22
li { _til! il_ i!
"' ',t i _ ] ! i ' i I i
i i i "k _,,_jl t i } 1_ _ ,I( ] I ]l[I]!
J J , t t ] I I l '. _
0.90 --
0._
1.15
atom
m_ m
0.90
.0.85
-7-
I.I0
1.05
1.00
0.95
0.90
0.85
m m ----------/
5 6 7
1.5 2.0
m Imm_ _q
8 9 I0
FLIGHT VELOCITY, 1000 ft,/secI I
2.5 3.0
FLIGHT VELOCITY, 1000 m/sec
11
I0.90
I
12
I
3.5
13
1
4.0
_a
EX IT NOZ ZLE
Report 75 194Volu_n5 e 7
Page 178
EFFICIENCY EFFECT
SCRAM JET MODE
..I
m m
uJUJ
_¢,_
Page 149 .... Page 150 ....
|AS|LiN| $P_¢1_1C 4M@UL$|SWP[|SOnIC COU|USrlOR |auJH
m*S[L*N( r_quSlSup[wsoaL¢ coulu$¢*o. I*UJ[:
Eng. No. 22
,,u_,, vlu_'r,,. L_ .,.
Baseline
,!, •
1.30
"_ 1.20
_, 1.10--
1.00
_m
_Iv
II
Q.}e,.
b-
-r"
b-6"}
,v-v
0.90
0.80
0.70
1.30
0.96
1.00 _
I1.5
6 7
I
2.0
8
FLIGHT
I
0.96-
9
VELOCITY,
I0
I000
I
II
_4'sec
I
2.5FLIGHT
3.0
TY, i000 m/sec
3.5
12 13
i
4.0
• Report Z5,194
_ Volume ?#_ Page 179/,4 larquamz .....,..,,,..,,
lU_m4r/_
EXIT NOZZLE/INLET COWL AREA RATIO EFFECT
SCRAM JET MODE
1.30
I
1.5
,N
Page 14-9 _" = Page 150 _""
IASK&iI( leerS1I*Slllml $PICIpI_ I_wisi liPlIIN#¢ COIIlUITllt lil#_T
iuPi|sowlt tOmlUillom llaili
F_m. vlumT,, slee _m
ILl ' i!"- I_*_ W Lm
_:i 4,,
Eng. No, 22
Baseline
A6/Ac = 1.50
.. " I f_ L[L] l +ill _ ]II_.[ [ [ J ] [ ! I ! : I ! I I i , !
z L;I _xJ _llz!itl;l, l)l-r-.! M I : I" {i'l:!r,._ll II_,:!, _ !l-l-l.I I i I _ ! I t _ i I"- |; l _ I f I F'I_t ' f i I ' i ;-',-t-l.I i ] i I i I ?-,i...i I i i i ; i _' i I ! i I I i i I I V"r"4..J-I _ i l
.L .{_!1 {i!l!!{it_,j
C, ,}, i:, 3!* *_, 4.1
6
I
2.0
7 8 9 10 II
FLIGHT VELOCITY, 1000 _secI I
2.5 3.0
FLIGHT VELOCITY, 1000 m/sec
I3.5
I
4.0
r"t/i_
/,r/arTu L ivan NUI'$o CAtWFOINIA
Report 35,194Volume 7
Page 180
Eng. No. 22
EFFECT OF SUBSYSTEM WEIGHT VARIATION
ON ENGINE THRU ST/WEIGHT
+ 10 PER CENT WEIGHT VARIATIONn
17.2
17.00
_ 16.8 f DE IGN POINT/
7 _(D__, 56.4 SUBSYSTEM "N_ _,_--t ('_ LINES, CONTROLS , .
__L(_ EXIT NOZZLE SUBSYSTEM. •=_ 16.2_p I I I I I I
_z ---(,_) M IXER/DIFFUSER/AFTERBURN ER
,., 16.0 ---(_ PRIMARY ROCKET SUBSYSTEM_1 I I I \®_)HEAT EXCHANGER UNIT
15.80.90 1.00 1,10
NORMALIZED SUBSYSTEM WEIGHT
EFFECT OF SUBSYSTEM WEIGHT VARON ENGINE THRUST/WEIGHT
. eport Z5,194Volume 7
Eng.
IATION
Page 181tl
No. 22
+ 50 PER CENT WEIGHT VARIATION
21
20
0 19 ' •
=_ 18y DESIGN POINT
o _,,,_E,,,, ,,__
14 -
130.50 1.00 1.50
NORMALIZED SUBSYSTEM WEIGHT
UNCLASSIFIED
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