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    Acta Astronautica 63 (2008) 565574

    www.elsevier.com/locate/actaastro

    Recent progress in scramjet/combined cycle engines at JAXA,Kakuda space center

    Tetsuo Hiraiwa, Katsuhiro Ito, Shigeru Sato, Shuichi Ueda, Kouichiro Tani,Sadatake Tomioka, Takeshi Kanda

    Kakuda Space Center, Japan Aerospace Exploration Agency, 1 Kimigaya, Kakuda, Miyagi 981-1525, Japan

    Received 22 December 2006; received in revised form 6 February 2008; accepted 28 April 2008

    Abstract

    This report presents recent research activities of the Combined Propulsion Research Group of Japan Aerospace Exploration

    Agency. Aerodynamics and combustion of the scramjet engine and the rocketramjet combined-cycle engine, structure and

    material for the two engines and thermo-aerodynamic of a re-entry vehicle are major subjects. In Mach 6 condition tests, a

    scramjet engine model produced about 2000 N net thrust, whereas a model produced thrust almost equal to its drag in Mach 12

    condition. A flight test of a combustor model was conducted with Hyshot-IV. A rocketramjet combined-cycle engine model is

    under construction with validation of the rocket engine component. Studies of combustor models and aerodynamic component

    models were conducted for demonstration of the engine operation and improvement of its performances. Light-weight cooling

    panel by electrochemical etching examined and C/C composite structure was tested. Thermo-aerodynamics of re-entry vehicle

    was investigated and oxygen molecular density was measured also in high enthalpy flow.

    2008 Elsevier Ltd. All rights reserved.

    1. Introduction

    An orbital vehicle needs large kinetic energy. Con-

    ventional liquid rockets attain this speed with consump-

    tion of onboard oxidizer such as liquid oxygen, which is

    about 70% of initial weight of the rockets. Air-breathing

    engines use oxygen in air and implementation of the en-

    gine to a launch vehicle will cause larger payload to anorbit. The scramjet engine, a hypersonic air-breathing

    engine, has a high performance in hypersonic speed, and

    its application to a booster stage will increase payload

    to an orbit, comparing to that by the conventional space

    transportation systems. The Combined Propulsion Re-

    search Group of Japan Aerospace Exploration Agency

    Corresponding author.

    E-mail address: [email protected] (T. Hiraiwa).

    0094-5765/$ - see front matter 2008 Elsevier Ltd. All rights reserved.

    doi:10.1016/j.actaastro.2008.04.011

    (JAXA), Kakuda Space Center (KSC) has progressed

    research on a scramjet engine to establish its design

    technologies from 1980s [1]. In the present paper, re-

    cent progresses of scramjet and combined-cycle engine

    research works in JAXA are presented.

    2. Research history in KSC

    The scramjet engine can operate only in the hy-

    personic speed and needs other engines to flight in

    other conditions, such as taking-off and space flight.

    To obtain larger operability, the group has started to

    study a rocketramjet combined-cycle engine. The

    rocketramjet combined-cycle engine is a combination

    of the rocket engine and the ramjet engine [2]. This

    engine has rocket engines inside the ramjet engine duct

    and can operate from take-off to orbital flight.

    http://www.elsevier.com/locate/actaastromailto:[email protected]:[email protected]://www.elsevier.com/locate/actaastro
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    566 T. Hiraiwa et al. / Acta Astronautica 63 (2008) 565 574

    Fig. 1 shows an image of the engine and Fig. 2 shows

    a series of operating schematics of the engine. The en-

    gine operates in the ejector-jet mode in low speed. As

    flight speed increases, its operating mode changes to

    the ramjet, the scramjet and the rocket [3,4]. In order to

    Fig. 1. Image of rocketramjet combined-cycle engine.

    Fig. 2. Conceptual operating modes of rocketramjet combined-cycle engine.

    change these operating modes, the engine should be a

    variable geometry configuration. However, this compli-

    cated configuration will make many kinds of difficulties

    in its development, maintenance and cost. Fixed geom-

    etry engine is presumed in the research activities in this

    group.Fig. 3 shows the diagram of our research activities

    for the scram and combined-cycle engines. Prior to

    the activities listed in the figure, a study of the air-

    breathing rocket (ABR) started in 1975 [5]. Around

    1980s, component and system studies on the scramjet

    engine started. For further research activities in 1990s,

    three major facilities were constructed; the ramjet en-

    gine test facility (RJTF), the numerical space engine

    (NSE), and the high enthalpy shock tunnel (HIEST). At

    RJTF, sub-scale engine combustion tests can be con-

    ducted in hypersonic flight condition from Mach 4 to

    8. At HIEST, tests at higher Mach number flight con-ditions can be operated. The NSE, the supercomputer

    system for the combined-cycle engine, can simulate

    operating conditions of the engine models tested at

    RJTF, HIEST and other small facilities. Table 1 lists

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    Fig. 3. Research activities on scramjet and combined-cycle engines in JAXAKSC.

    Table 1

    Features of RJTF, HIEST and NSE

    RJTF M4 and 6 at dynamic pres. 50 kPa

    M8 at dynamic pres. 25 kPa

    HIEST Maximum stagnation enthalpy: 25 M J kg1

    Maximum stagnation pressure: 150 MPa

    NSE 512 GFlops, 512 GB memory, 64 CPU

    specifications of the facilities. RJTF was recently mod-

    ified to conduct Mach 0 condition test, that is, the sea-

    level still air condition test for the ejector-jet mode tests.

    The design technology of the ejector-jet mode can

    be applied to a booster engine of a rocket vehicle. The

    technologies of the scramjet engine and this mode of

    the combined-cycle engine can be also applied to a hy-

    personic flight vehicle [6].

    3. Scramjet engine studies

    Studies on the scramjet engine, preceding studies to

    those on the combined-cycle engine, have produced re-

    markable results in experimental, numerical and system

    Fig. 4. Thrust increment of scramjet model under Mach 6 condition

    at RJTF.

    investigations. Recent activities are introduced in this

    section.

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    Fig. 5. Schematic of scramjet engine model tested under Mach 6 condition at RJTF.

    Fig. 6. OH distributions in scramjet engine model at Mach 6 con-

    dition of RJTF.

    From March to April of 2005, a scramjet engine

    model was tested under Mach 6 condition at RJTF.

    Staged fuel injection was tried and an effect of in-

    flow boundary layer was investigated [7]. Fig. 4 shows

    thrust increment against an equivalence ratio, and Fig. 5

    shows a schematic of the model. Fuel was injected from

    a strut, and three positions on the sidewalls indicated

    with MV1, MV3 and MV4. The engine produced about1.9 kN net thrust and specific impulse of 9000 m s1.

    The net thrust doubled the previous value by the single

    fuel injection. Fig. 6 shows numerical simulation re-

    sults with NSE, showing OH distributions at fuel flow

    rates [8]. In HIEST, another scramjet engine model was

    tested under Mach 1015 conditions [9]. Fig. 7 shows a

    schematic of the engine model setup. The engine model

    succeeded to produce thrust almost equal to its drag. In

    the model, hydrogen fuel was injected from hypermixer

    injector, which enhanced mixing by streamwise vortices

    [10]. Fig. 8 shows distribution of H2O mole fraction by

    CFD simulation by NSE and Fig. 9 shows the injector.

    The engine model was modified, and recently another

    model was constructed.

    The effectiveness of the injector was tried to demon-

    strate in an actual flight condition with Hyshot-IV at

    Woomera, Australia, under contraction with University

    of Queensland. The test was also aimed to validatetest results produced at the wind tunnel of HIEST. Ac-

    cording to experimental results at HIEST, the injector

    showed higher mixing performance [10]. The flight test

    was operated on March 30 with a flight model with two

    combustors (Fig. 10). The nose cone did not open and

    the trial was failed. The cause of the failure is now un-

    der investigation.

    4. Rocketramjet combined cycle engine studies

    4.1. Engine model for RJTF tests

    A rocketramjet combined-cycle engine model

    shown in Fig. 11 is now under construction for tests

    at RJTF [2]. Operation of each mode will be demon-

    strated and design technologies of the engine will be

    validated. Propellants are gas hydrogen and gas oxy-

    gen. The choking condition with no geometrical throat

    at the engine exit requires a large equivalence ratio,

    especially in the ramjet mode. To compensate, this

    engine model has a throat at the exit for safety. First

    test is scheduled around November 2006 at a sea-level,still-air condition. This model will have additional fuel

    injection positions along the engine duct as well as in

    the downstream combustor section to study an effect of

    the fuel injection position on mixing and combustion

    condition. Geometry of the cowl leading edge is also

    exchangeable to study its effect on breathing ability

    in the ejector-jet mode and air-capture ability in the

    ramjet and scramjet modes.

    The rocket component was tested before integration

    [11,12]. It operated in wide ranges of chamber pressure

    and a mixture ratio, O/F. In an actual engine, number

    of combination of the pressure and the mixture ratio

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    Fig. 7. M12-02 scramjet model at HIEST.

    Fig. 8. H2O mole fraction in M12-02 model.

    Fig. 9. Hypermixer injector.

    will be limited. However, in the research process, lots

    of combinations should be examined to make clear the

    suitable operating condition and engine configuration.

    Fig. 12 shows C* efficiency against O/F. The rocket

    component showed sufficient efficiency. Durability of

    the face plate was enforced through the series of the

    combustion tests. Fig. 13 shows the damaged plate and

    the modified one after firing tests.

    4.2. Component studies

    Prior to the test in RJTF, component tests were con-

    ducted to demonstrate the operation of the combined-

    cycle engine and these experimental results were used

    to design the RJTF model. Fig. 14 shows an example of

    wall pressure distributions of a combustor model in the

    ejector-jet mode at sea-level-, still-air condition [13].

    Breathed air was choked at the exit of the throat sec-

    tion. Pressure became lower than the choking pressure

    of an atmospheric air around the entrance of the diver-

    gent section. The combustion gas choked at the exit of

    the model. Fig. 15 shows wall pressure distributions in

    the downstream-combustion ramjet mode [14]. In this

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    mode, fuel is injected into the downstream combustor.

    Subsonic combustion and subsequent choking at the exit

    are attained.

    The inlet section should satisfy contradicting require-

    ments; sufficient air capture in the subsonic and tran-

    sonic condition and sufficient compression in the su-personic and hypersonic condition. Experimental and

    Fig. 10. Scramjet combustor model test by Hyshot-IV.

    Fig. 11. Schematic of rocketramjet combined-cycle engine model.

    numerical investigations were conducted to design the

    engine model. Fig. 16 shows CFD results of the inlet

    sections at Mach 10 [15]. The shock waves from the side

    wall leading edges deformed the ramp shock around the

    symmetric plane, and this interaction increased spillage.

    The engine operation was examined in a transonicwind tunnel. Fig. 17 shows a wind tunnel model [16].

    Nitrogen gas was used to simulate rocket exhaust. The

    ejector-jet mode operation was demonstrated and aero-

    dynamic improvements were achieved.

    5. Fundamental research works

    5.1. Cooling structure and material

    As shown in Fig. 1, the scramjet engine and the

    combined-cycle engine have a large duct and the

    Fig. 12. C* efficiency of rocket component.

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    Fig. 13. Face plate of rocket component: (a) before improvementand (b) after improvement.

    structure. The engine requires the regenerative cool-

    ing system composed in the engine structure. There-

    fore, light-weight material and structure are requested.

    In KSC, production technique of the large cooling panel

    and light-weight material of C/C composite have been

    investigated.

    Machining to such a large panel will be difficult. Elec-trochemical etching was employed for creating cooling

    passages on the nickel alloy plate [17,18]. Fig. 18 shows

    a trial product of stainless steel panel with cooling pas-

    sages by chemical etching.

    Combination of the C/C material with metal cool-

    ing channel was proposed to prevent leakage of coolant

    through breathable C/C material [19]. Fig. 19 shows a

    picture of the model. Effectiveness of SiC coating to

    the C/C material against oxidization and mechanism of

    oxidizing erosion were also investigated [20]. Fig. 20

    shows damage of C/C composite piece after heating

    test.

    Fig. 14. Wall pressure distributions in ejector-jet mode combustor

    model.

    Fig. 15. Wall pressure distributions in a combustor model.

    Fig. 16. Isobars in inlet section.

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    Fig. 17. Engine model for transonic wind tunnel tests.

    Fig. 18. A stainless steel panel with cooling passages by chemical

    etching method.

    5.2. Thermo-aerodynamics for re-entry

    The re-entry technique is necessary to carry passen-

    gers or payload from the space station. Future space

    Fig. 19. C/C composite structure with metal cooling passage.

    transportation vehicle with the scramjet engine and the

    combined-cycle engine also have to re-enter the at-

    mosphere. Studies for re-entry vehicle are also being

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    Fig. 20. Damage of C/C composite piece after heating test: (a) surface of pinhole and (b) cross section of pinhole.

    Fig. 21. Schlieren image of flow field around a model with large

    cone angle.

    conducted in HIEST, which can simulate re-entry con-

    dition. A model with a large cone angle was used to

    investigate the real gas effect on pressure distribution

    [21]. Fig. 21 shows a schlieren image around the model.

    Recombination of dissociated air on surface of the re-

    entry vehicle affects heat flux. Oxygen molecular den-

    sity was measured on a flat plate model surface by

    laser absorption spectroscopy with measurement of heat

    flux [22].

    6. Summary

    The combined Propulsion Research Group of JAXA

    is conducting researches on the scramjet engine and the

    rocketramjet combined-cycle engine for wide applica-

    tions of space transportation. In the scramjet engine re-

    search, net thrust was attained in lower Mach numbers

    and is being tested in higher Mach numbers. The scram-jet is combined with the rocket engine to enlarge its

    operating range, and this rocketramjet combined-cycle

    engine is also studied. Based on results of component

    and system studies, sub-scale model is now under con-

    struction. Researches on cooling panel and light-weight

    material are being progressed, which will be useful for

    future air-breathing and combined-cycle engines. Ac-

    tivities of thermo-aerodynamics on the re-entry vehicle

    are also progressed.

    References

    [1] N. Chinzei, Research activities on scramjets at NAL-KRC

    in Japan, 15th ISABE Paper 2001-1075, Bangalore, India,

    September 2001.

    [2] T. Kanda, et al., Design of sub-scale rocketramjet combined-

    cycle engine model, in: 56th IAC Paper IAC-05-C4.5.03,

    Fukuoka, Japan, October 2005.

    [3] T. Kanda, et al., Conceptual study of a combined-cycle engine

    for an aerospace plane, Journal of Propulsion and Power 19

    (5) (2003) 544553.

    [4] T. Kanda, et al., Conceptual study of a rocketramjet combined-

    cycle engine for an aerospace plane, Journal of Propulsion and

    Power 23 (2) (2007) 301309.

    [5] G. Masuya, et al., A study of air breathing rocketssubsonicmode combustion, Acta Astronautica 1 (8) (1981) 643661.

    [6] T. Kanda, T. Hiraiwa, Evaluation of effectiveness of periodic

    flight by a hypersonic vehicle, Journal of Aircraft 44 (6) (2007)

    20762077.

    [7] S. Ueda, et al., Mach 6 test of a scramjet engine with multi-

    staged fuel injection, AIAA Paper 2005-1027, January 2006.

    [8] T. Kouchi, et al., Transition of combustion modes in a scramjet

    engine, in: 25th ISTS Paper ISTS-2006-a-46, Kanazawa, Japan,

    June 2006.

    [9] M. Takahashi, et al., Experimental study on scramjet engine

    performance at Mach 1015 flight condition, 17th ISABE Paper

    2005-1238, Munich, Germany, September 2005.

    [10] Sunami, et al., Effects of streamwise vortices on scramjet

    combustion at Mach 815 flight enthalpiesan experimental

  • 7/31/2019 1-s2.0-S0094576508001549-main

    10/10

    574 T. Hiraiwa et al. / Acta Astronautica 63 (2008) 565 574

    study in HIEST, in: 17th ISABE Paper 2005-1028, Munich,

    Germany, September 2005.

    [11] M. Takegoshi, et al., Firing tests of a rocket combustor for

    combined cycle engine at various conditions, AIAA Paper 2005-

    4286, July 2005.

    [12] M. Takegoshi, et al., Scramjet mode operation of the rocket

    engine for the combined cycle engine, AJCPP Paper 2006-22194, April, 2006.

    [13] T. Kanda, et al., Experimental study of a combined-cycle engine

    combustor in ejector-jet mode, Journal of Propulsion and Power

    23 (6) (2007) 11531159.

    [14] K. Kato, et al., Preliminary tests of downstream combustion

    ramjet-mode in a combined cycle engine combustor, in: 25th

    ISTS Paper ISTS-2006-a-53, Kanazawa, Japan, June 2006.

    [15] K. Tani, et al., Designing and aerodynamic performance of the

    combined-cycle engine inlet in a hypersonic flow, in: 56th IAC

    Paper IAC-05-C4.5.06, Fukuoka, Japan, October 2005.

    [16] K. Tani et al., Aerodynamic characteristics of the modified

    combined cycle engines in ejector-jet mode, AIAA Paper 2006-

    0224, January 2006.

    [17] T. Saito, et al., Heating evaluation test of a duct-shaped cooling

    structure simulating scramjet combustors, AIAA Paper 2004-

    2174, June 2004.

    [18] T. Saito, et al., Experimental study of an etching method as a

    fabrication technique of cooling passages for combined cycle

    engine wall structure, in: 25th ISTS Paper ISTS-2006-c-03,

    Kanazawa, Japan, June 2006.[19] M. Takegoshi, S. Ueda, Cooling characteristics of C/C

    composite material structure with a metallic tube fixed by

    elastic force of each material, Journal of the Japan Society for

    Aeronautical Space Science 54 (2006) 129135 (in Japanese).

    [20] F. Ono, et al., Durability of CVD-SiC layer on the isotropic

    graphite in high temperature air, AIAA Paper 2002-5134,

    October 2002.

    [21] K. Itoh, et al., Hypersonic aerothermodynamic and scramjet

    research using high enthalpy shock tunnel, Shock Waves 12

    (2002) 9398.

    [22] H. Tanno, et al., Laser absorption spectroscopy of oxygen

    molecule in free piston shock tunnels, in: 25th ISTS Paper

    ISTS-2006-e-11, Kanazawa, Japan, June 2006.