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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System Aero-Thermodynamic Design of a Scramjet Propulsion System: The graduate school GRK 1095/2 funded by the “Deutsche Forschungsgemeinschaft“ (DFG) B. Weigand Universität Stuttgart Institut für Thermodynamik der Luft- und Raumfahrt

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Page 1: Aero-Thermodynamic Design of a Scramjet Propulsion · PDF fileAero-Thermodynamic Design of a Scramjet Propulsion System: The graduate school ... Aero-Thermodynamic Design of a Scramjet

Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

Aero-Thermodynamic Design of a Scramjet Propulsion System:

The graduate school GRK 1095/2 funded by the “Deutsche Forschungsgemeinschaft“ (DFG)

B. Weigand

Universität Stuttgart

Institut für Thermodynamik der Luft- und Raumfahrt

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

1. Introduction2. Research Training Group - GRK 1095/2

- Basic concept- Structure of the GRK- Educational-program

3. Selected results- Project group A: “Aero-thermodynamical analysis”- Project group B: “Combustion”- Project group C: “Nozzle flow and system analysis”

4. Conclusion and Outlook

Contents

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

Startschub: ca. 12 MNNutzlast: 6,5 to Brennstoff: LH2 26 to, LOx 132 to

Startschub: ca. 12 MNNutzlast: 6,5 to Brennstoff: LH2 26 to, LOx 132 to

Startschub: ca. 29 MNStartgewicht: 2000 toNutzlast: 28 to Brennstoff: LH2 100 to, LOx 600 to

Startschub: ca. 29 MNStartgewicht: 2000 toNutzlast: 28 to Brennstoff: LH2 100 to, LOx 600 to

Ariane 5Ariane 5 Space ShuttleSpace Shuttle

Introduction

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

Ramjet: - No moving parts; ram compression- Compression of the soaked up mass flow by reducing the flow speed to subsonic velocity inside the intake → subsonic combustion

- Mach number range: 2 ÷ 6

But: Increase of airspeed M∞>6a) increasing shock losses inside the intakeb) increasing stagnation temperature at the entry of the combustionchamber → increasing dissociation

Way out: - Reducing the flow speed inside the inlet to 30 - 50 % of the airspeed- Supersonic flow inside combustion chamber

⇒ supersonic combustion- Mach number range: 5 ÷ ~25

Scramjet: Supersonic Combustion Ramjet

Introduction – What is a “Scramjet”?

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

Introduction – ExamplesHyper X-43

first stage

combinedengine, scramjet

second stage

Sänger*-concept

*germ. aerospace-engineer, 1905-1964

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

1. Introduction2. Research Training Group - GRK 1095/2

- Basic concept- Structure of the GRK- Educational-program

3. Selected results- Project group A: “Aero-thermodynamical analysis”- Project group B: “Combustion”- Project group C: “Nozzle flow and system analysis”

4. Conclusion and outlook

Contents

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

Ltot>1000 mmdm/dt: =1.45 kg/s

LF=450 ÷ 500 mmρ∞=1.801⋅10-2 kg/m3

h=228 mmT∞=226.7 K

b≈76 mmp∞=11.7 hPa

α2≈19°M=8

α1≈7,5°H=30 km

Geometry:Inflow data:

Topic: Aero-thermodynamic design of a scramjet propulsion system for future reusable space transportation systems and hypersonic flight

Basic Concept

2D / 3D-inlet

with double rampCombustion chamber

with strut Injector

SERN-Nozzle

Isolator

- Group A: Aero-thermodynamical analysis

- Group B: Combustion

- Group C: Nozzle flow and system analysis

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

Group A: Aero-thermodynamic investigations

A1: Experimental investigations of the boundary layer transition of a double ramp configuration.

A2: Experimental investigation of the shock boundary layer interaction of a double ramp configuration at different inflow conditions.

A3: Design and characterization of a 3D scramjet inlet.

A4: Experimental investigation of the internal flow conditions of a scramjet engine.

A5: Investigation of 3D flow structures caused by side wall effects of a scramjet engine.

A6: Numerical simulations of the unsteady effects in a scramjet intake.

A7: Computational analysis of the relaminarisation in hypersonic intake flows.

A8: Numerical investigation of the sensitivity on the design of a hypersonic intake.

Structure and sub-projects

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

Group B: Combustion

B1: Experimental investigations of the fuel injection and mixing and stability of a supersonic combustor.

B2: Numerical investigation of a supersonic combustion chamber for different flight conditions.

B3: Thermal and mechanical investigations of a central injector in a scramjet combustor.

B4: Numerical investigation of the turbulence-chemical reaction interaction and the emission production in a scramjet combustor.

B5: Unsteady simulations of supersonic combustion chambers.

B6: Development of a numerical efficient combustion model for the interaction between chemical reaction and turbulence for LES.

B7: Shock-boundary layer interaction for reactive flows.

B8: Prevention of thermal cocking in supersonic combustors by using staged injection..

Structure and sub-projects

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

Structure and sub-projectsGroup C: Nozzle flow and system analysis

C1: Aerodynamic design of a flight configuration and the related instrumentation.

C2: Numerical simulation of a nozzle flow with cooling.

C3: Experimental investigation of the expansion flow of an air breathing propulsion system under consideration of the temperature gradient between jet and outer flow.

C4: Multi-field formulation for functionally graded high-temperature materials.

C5: Coupled simulations for the systematic design optimization of scramjets.

C6: Investigation of the thermal loads of a hypersonic propulsion system.

C7: Modeling of a scramjet propulsion system.

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

Germany

Locations:

Stuttgart

Universität Stuttgart

Aachen

(Aix-la-Chapelle)

Köln

(Cologne)

München

(Munich)

Technische Universität München

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

Speaker of the GRK 1095/2:-Prof. Dr. B. Weigand, ITLR Stuttgart University

Project leaders:- Stuttgart: E. Krämer, C.D. Munz, B. Kröplin, S. Staudacher, J. von Wolfersdorf,

M. Aigner, P. Gerlinger, B. Weigand

- Aachen/DLR Köln: H. Olivier, W. Schröder, A. Gülhan, M. Behr

- München: H.P. Kau, T. Sattelmayer, N. Adams

Scholars and Postdocs:-Stuttgart (9): A.M. Schreyer, M. Banica, M. Staudenmaier, J. Vellaramkalayil, A. Hell,

B. Rust, C. Messe, J. Groß, V. Shevchuk-Aachen (4)/DLR Köln (2): O. Hohn, C. Fischer, T. Nguyen, J. Riehmer, M. Konapka,

F. Bramkamp - München (3): D. Bruno, O. Petrache, S. Kirstein

And a lot of Associated members: U. Gaisbauer, B. Reinartz, G. Lamanna, T. Scheuermann, T. Langener,…

Structure - Members

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

combustionaero-thermodynamicinvestigations

A1, A2

A6 A4, A5

A3

A7, A8

supersoniccombustion

B1

B2 B3

B4

B5

B6B7

B8

nozzle flow and total system analysis

C1, C2, C3 C4, C5 C6, C7

Structure - interactions

very strong interaction within thedifferent sub-projects

technical requirements of a

„scramjet“-propulsion system

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

Standard Elements:

• Individual training program with specific courses• Lectures by the involved scientists and guests• Courses and lectures by international specialists• Meetings and discussion forums• Regular internal conferences

Special Features:• A stay abroard for all members for 6 months• Self organised summer schools and workshops withinternational specialists (by the PhD-students)

• Discussion forums with partners from industry• Integration of an external patent agent

Structure - Educational-program

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

Educational-Program - Summer Schools

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

1. Introduction2. Research Training Group - GRK 1095/2

- Basic concept- Structure of the GRK- Educational-program

3. Selected results- Project group A: “Aero-thermodynamical analysis”- Project group B: “Combustion”- Project group C: “Nozzle flow and system analysis”

4. Conclusion and outlook

Content

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

static pressure field doubstatic pressure field double ramp configuration le ramp configuration M=2.5, Re/m=9.82M=2.5, Re/m=9.82··101066

A2: A2: NumericalNumerical investigationsinvestigations of a double of a double rampramp configurationconfiguration withwith different different initialinitialconditionsconditions (Dr. Irina Fedorchenko, Institut f(Dr. Irina Fedorchenko, Institut füür Aerodynamik und Gasdynamik, Universitr Aerodynamik und Gasdynamik, Universitäät t Stuttgart, Stuttgart, Khristianovich Institute of Theoretical and Applied Mechanics SB RAS, Novosibirsk, Russia))

Selected Results

M

Reattachmentwaves

First kinkshock

Secondkink shock

Slip line

Joinedshock

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

A7: Numerical investigation of the influence of laminar turbulent transition on hypersonic inlets (Martin Krause, Lehr- und Forschungsgebiet für Mechanik, RWTH Aachen)

Selected Results

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

Cooperation shown as an example for the Project A7

A7(Krause)

A3(Häberle)

A5(Neuenhahn)

AX(Bosco)

A2 und A8(PostDocs)

A6(Lörcher)

C2(Meiss)

C6(Fuhrmann)

C7(Schütte)

C4(Leetsch)

B1(Scheuermann)

B4(Rust)

B8(Maier)

B2(Rosenko)

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

B1: Experimental investigation of the design of a subersonic combustion chamber(Tobias Scheuermann, Institut für Thermodynamik der Luft- und Raumfahrt, Universität Stuttgart)

Selected Results

modified geometry of thecombustion chamber

Strong and weak combustion –normalized wall pressure distribution for different equivalence ratios (Φ)

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

Distribution of hydrogen

2.5 cm 5 cm10 cm

20 cmXH2

Lobed strut injector

B5: Numerical investigation of the turbulent chemistry interaction(B. Rust, Institut für Verbrennungstechnik der LRT, Universität Stuttgart)

Selected Results

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

Selected Results

B6: Turbulence-Chemistry Interaction (Henrik Förster, Lehrstuhl A für Thermodynamik, TU München)

Example of an in situ tabel for a 3D thermodynamic state variable. Betweenthe cells, the results can be interpoated.

Ignition delay time for a Hydrogen-airmixture, directly calculated and interpolatedfrom 36 cells.

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

C1: Experimental investigation of a scramjet nozzle (Christian Hirschen, DLR, Abteilung Windkanäle des Instituts für Aerodynamik und Strömungstechnik)

Selected Results

Schlieren picture with air (left) und argon (right) for p0,D = 3,2 bar→ Influence of the ratio of the specific heats

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

C2: Simulation of the interaction between nozzle flow and outside flow(Jan Hendrik Meiß, Aerodynamisches Institut, RWTH Aachen)

SERN (grid)

Single Expansion Ramp Nozzle

Mach number distribution, M=7 (left), M=4 (right)

Selected Results

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

C6 & C7: GRK-Design Tools (T. Fuhrmann, G. Schütte)

31~E

Inlet-2D Euler- Perfect gas

Combustor-1D Streamline- Chemical kinetics

Nozzle-2D Euler- Perfect gas

47~E

0~X

InletG

9~E

31X 47X 9X

CombustorGCombustorS~

NozzleG

9~X

C6

C7

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

B4

Düsendruckverhältnis Π, -

Schu

bbei

wer

tcfg

,-

Schu

bvek

torw

inke

lβf,

°

200 400 600 800 10000.9

0.92

0.94

0.96

0.98

3.5

4

4.5

5

cfg,xβf

Cooperation shown as an example for the Projects C6 & C7

C6 C7

A3

A7

B1B8

C1

C2C4

A6

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

• Research Training Group GRK 1095 – started April 2005

• Involved institutions: RWTH Aachen, DLR Köln, TU München and

Universität Stuttgart

• Comprehensive educational program

• Integration of international experts in scramjet technology / international

scientific exchange

• High level of integration and networking between all members and

institutions within Germany and with foreign partners

• First results demonstrate the efficiency of the philosophy

• Upgrading of the national know how and continuation of the long „scramjet

history“ in Germany

• Strict focus on hydrogen combustion with lobed strut injectors

Summary

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

• Aim for the first project stage (4.5 years): development of a successfull

design of a scramjet propulsion system with focus on a lobed strut injector

concept

• Verification of the functionality in tests associated project: wind tunnel test of

a scramjet propulsion system (GA1332/1, financed by DFG)

⇒ Project GRK 1095/1 has been evaluated by DFG in 2009.

Because of the very good achievements, the project got elongated by

another 4,5 years, starting from 1.10.2009

Summary - Outlook

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Research Training Group 1095/2: Aero-Thermodynamic Design of a Scramjet Propulsion System

All members of the Graduate School GRK

1095 would like to thank the Deutsche

Forschungsgemeinschaft (DFG) for the

support and the financing of the presented

scramjet research activities.

Acknowledgement