Supersonic Combustion Ramjet: Analysis on Fuel Options
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Brazilian 14-Xs Hypersonic Unpowered Scramjet Aerospace Vehicle
ISSN 2176-5480 22nd International Congress of Mechanical Engineering (COBEM 2013) November 3-7, 2013, Ribeirão Preto, SP, Brazil Copyright © 2013 by ABCM BRAZILIAN 14-X S HYPERSONIC UNPOWERED SCRAMJET AEROSPACE VEHICLE STRUCTURAL ANALYSIS AT MACH NUMBER 7 Álvaro Francisco Santos Pivetta Universidade do Vale do Paraíba/UNIVAP, Campus Urbanova Av. Shishima Hifumi, no 2911 Urbanova CEP. 12244-000 São José dos Campos, SP - Brasil [email protected] David Romanelli Pinto ETEP Faculdades, Av. Barão do Rio Branco, no 882 Jardim Esplanada CEP. 12.242-800 São José dos Campos, SP, Brasil [email protected] Giannino Ponchio Camillo Instituto de Estudos Avançados/IEAv - Trevo Coronel Aviador José Alberto Albano do Amarante, nº1 Putim CEP. 12.228-001 São José dos Campos, SP - Brasil. [email protected] Felipe Jean da Costa Instituto Tecnológico de Aeronáutica/ITA - Praça Marechal Eduardo Gomes, nº 50 Vila das Acácias CEP. 12.228-900 São José dos Campos, SP - Brasil [email protected] Paulo Gilberto de Paula Toro Instituto de Estudos Avançados/IEAv - Trevo Coronel Aviador José Alberto Albano do Amarante, nº1 Putim CEP. 12.228-001 São José dos Campos, SP - Brasil. [email protected] Abstract. The Brazilian VHA 14-X S is a technological demonstrator of a hypersonic airbreathing propulsion system based on supersonic combustion (scramjet) to fly at Earth’s atmosphere at 30km altitude at Mach number 7, designed at the Prof. Henry T. Nagamatsu Laboratory of Aerothermodynamics and Hypersonics, at the Institute for Advanced Studies. Basically, scramjet is a fully integrated airbreathing aeronautical engine that uses the oblique/conical shock waves generated during the hypersonic flight, to promote compression and deceleration of freestream atmospheric air at the inlet of the scramjet. -
The SKYLON Spaceplane
The SKYLON Spaceplane Borg K.⇤ and Matula E.⇤ University of Colorado, Boulder, CO, 80309, USA This report outlines the major technical aspects of the SKYLON spaceplane as a final project for the ASEN 5053 class. The SKYLON spaceplane is designed as a single stage to orbit vehicle capable of lifting 15 mT to LEO from a 5.5 km runway and returning to land at the same location. It is powered by a unique engine design that combines an air- breathing and rocket mode into a single engine. This is achieved through the use of a novel lightweight heat exchanger that has been demonstrated on a reduced scale. The program has received funding from the UK government and ESA to build a full scale prototype of the engine as it’s next step. The project is technically feasible but will need to overcome some manufacturing issues and high start-up costs. This report is not intended for publication or commercial use. Nomenclature SSTO Single Stage To Orbit REL Reaction Engines Ltd UK United Kingdom LEO Low Earth Orbit SABRE Synergetic Air-Breathing Rocket Engine SOMA SKYLON Orbital Maneuvering Assembly HOTOL Horizontal Take-O↵and Landing NASP National Aerospace Program GT OW Gross Take-O↵Weight MECO Main Engine Cut-O↵ LACE Liquid Air Cooled Engine RCS Reaction Control System MLI Multi-Layer Insulation mT Tonne I. Introduction The SKYLON spaceplane is a single stage to orbit concept vehicle being developed by Reaction Engines Ltd in the United Kingdom. It is designed to take o↵and land on a runway delivering 15 mT of payload into LEO, in the current D-1 configuration. -
Modelling a Hypersonic Single Expansion Ramp Nozzle of a Hypersonic Aircraft Through Parametric Studies
energies Article Modelling a Hypersonic Single Expansion Ramp Nozzle of a Hypersonic Aircraft through Parametric Studies Andrew Ridgway, Ashish Alex Sam * and Apostolos Pesyridis College of Engineering, Design and Physical Sciences, Brunel University London, London UB8 3PH, UK; [email protected] (A.R.); [email protected] (A.P.) * Correspondence: [email protected]; Tel.: +44-1895-267-901 Received: 26 September 2018; Accepted: 7 December 2018; Published: 10 December 2018 Abstract: This paper aims to contribute to developing a potential combined cycle air-breathing engine integrated into an aircraft design, capable of performing flight profiles on a commercial scale. This study specifically focuses on the single expansion ramp nozzle (SERN) and aircraft-engine integration with an emphasis on the combined cycle engine integration into the conceptual aircraft design. A parametric study using computational fluid dynamics (CFD) have been employed to analyze the sensitivity of the SERN’s performance parameters with changing geometry and operating conditions. The SERN adapted to the different operating conditions and was able to retain its performance throughout the altitude simulated. The expansion ramp shape, angle, exit area, and cowl shape influenced the thrust substantially. The internal nozzle expansion and expansion ramp had a significant effect on the lift and moment performance. An optimized SERN was assembled into a scramjet and was subject to various nozzle inflow conditions, to which combustion flow from twin strut injectors produced the best thrust performance. Side fence studies observed longer and diverging side fences to produce extra thrust compared to small and straight fences. Keywords: scramjet; single expansion ramp nozzle; hypersonic aircraft; combined cycle engines 1. -
2. Afterburners
2. AFTERBURNERS 2.1 Introduction The simple gas turbine cycle can be designed to have good performance characteristics at a particular operating or design point. However, a particu lar engine does not have the capability of producing a good performance for large ranges of thrust, an inflexibility that can lead to problems when the flight program for a particular vehicle is considered. For example, many airplanes require a larger thrust during takeoff and acceleration than they do at a cruise condition. Thus, if the engine is sized for takeoff and has its design point at this condition, the engine will be too large at cruise. The vehicle performance will be penalized at cruise for the poor off-design point operation of the engine components and for the larger weight of the engine. Similar problems arise when supersonic cruise vehicles are considered. The afterburning gas turbine cycle was an early attempt to avoid some of these problems. Afterburners or augmentation devices were first added to aircraft gas turbine engines to increase their thrust during takeoff or brief periods of acceleration and supersonic flight. The devices make use of the fact that, in a gas turbine engine, the maximum gas temperature at the turbine inlet is limited by structural considerations to values less than half the adiabatic flame temperature at the stoichiometric fuel-air ratio. As a result, the gas leaving the turbine contains most of its original concentration of oxygen. This oxygen can be burned with additional fuel in a secondary combustion chamber located downstream of the turbine where temperature constraints are relaxed. -
10. Supersonic Aerodynamics
Grumman Tribody Concept featured on the 1978 company calendar. The basis for this idea will be explained below. 10. Supersonic Aerodynamics 10.1 Introduction There have actually only been a few truly supersonic airplanes. This means airplanes that can cruise supersonically. Before the F-22, classic “supersonic” fighters used brute force (afterburners) and had extremely limited duration. As an example, consider the two defined supersonic missions for the F-14A: F-14A Supersonic Missions CAP (Combat Air Patrol) • 150 miles subsonic cruise to station • Loiter • Accel, M = 0.7 to 1.35, then dash 25 nm - 4 1/2 minutes and 50 nm total • Then, must head home, or to a tanker! DLI (Deck Launch Intercept) • Energy climb to 35K ft, M = 1.5 (4 minutes) • 6 minutes at M = 1.5 (out 125-130 nm) • 2 minutes Combat (slows down fast) After 12 minutes, must head home or to a tanker. In this chapter we will explain the key supersonic aerodynamics issues facing the configuration aerodynamicist. We will start by reviewing the most significant airplanes that had substantial sustained supersonic capability. We will then examine the key physical underpinnings of supersonic gas dynamics and their implications for configuration design. Examples are presented showing applications of modern CFD and the application of MDO. We will see that developing a practical supersonic airplane is extremely demanding and requires careful integration of the various contributing technologies. Finally we discuss contemporary efforts to develop new supersonic airplanes. 10.2 Supersonic “Cruise” Airplanes The supersonic capability described above is typical of most of the so-called supersonic fighters, and obviously the supersonic performance is limited. -
Flight Data Analysis of the HYSHOT Flight #2 Scramjet
13th AIAA/CIRA International Space Planes and Hypersonic Systems and Technologies Conference Flight Data Analysis of HyShot 2 Neal E. Hass*, Michael K. Smart+ NASA Langley Research Center, Hampton, Virginia Allan Paull! University of Queensland, Brisbane, Australia Abstract The development of scramjet propulsion for alternative launch and payload delivery capabilities has comprised largely of ground experiments for the last 40 years. With the goal of validating the use of short duration ground test facilities, the University of Queensland, supported by a large international contingency, devised a ballistic re-entry vehicle experiment called HyShot to achieve supersonic combustion in flight above Mach 7.5. It consisted of a double wedge intake and two back-to-back constant area combustors; one supplied with hydrogen fuel at an equivalence ratio of 0.33 and the other un-fueled. Following a first launch failure on October 30th 2001, the University of Queensland conducted a successful second launch on July 30th, 2002. Post-flight data analysis of the second launch confirmed the presence of supersonic combustion during the approximately 3 second test window at altitudes between 35 and 29 km. Reasonable correlation between flight and some pre-flight shock tunnel tests was observed. Nomenclature f aerodynamic factor h altitude M Mach number P pressure q dynamic pressure s seconds T temperature V velocity w mass flow X axial coordinate Y lateral coordinate Z normal coordinate α angle-of-attack ηc combustion efficiency γ ratio of specific heats φ equivelance ratio ω angular velocity about longitudinal body axis ζ angular velocity of longitudinal axis about velocity vector * Aerospace Engineer, Hypersonic Airbreathing Propulsion Branch + Research Scientist, Hypersonic Airbreathing Propulsion Branch ! Professor, Mechanical Engineering Department 1 Subscripts: 0 freestream c combustor entrance w wedge t2 Pitot Introduction The theoretical performance advantage of scramjets over rockets in hypersonic flight has been well known since the 1950’s. -
Ciam/Nasa Mach 6.5 Scramjet Flight and Ground Test
AIAA-99-4848 CIAM/NASA MACH 6.5 SCRAMJET FLIGHT AND GROUND TEST R. T. Voland* and A. H. Auslender** NASA Langley Research Center Hampton, VA M. K. Smart Lockheed Martin Engineering Sciences Hampton, VA A.S. Roudakovà, V.L. Semenov¤, and V. Kopchenov¤ Central Institute of Aviation Motors Moscow, Russia ABSTRACT NOMENCLATURE The Russian Central Institute of Aviation Motors (CIAM) performed a flight test of a CIAM-designed, C-16V/K Ð CIAM scramjet engine ground test facility, hydrogen-cooled/fueled dual-mode scramjet engine located in Tureavo, Russia (Figure 10) over a Mach number range of approximately 3.5 to 6.4 CIAM Ð Central Institute of Aviation Motors, Moscow, on February 12, 1998, at the Sary Shagan test range in Russia Kazakhstan. This rocket-boosted, captive-carry test of CO2 Ð Carbon dioxide the axisymmetric engine reached the highest Mach Cp Ð Pressure Coefficient number of any scramjet engine flight test to date. The H Ð Altitude (km, m, or ft) flight test and the accompanying ground test program, H2 Ð Hydrogen conducted in a CIAM test facility near Moscow, were H2O Ð Water performed under a NASA contract administered by the He Ð Helium Dryden Flight Research Center with technical HFL Ð Hypersonic Flying Laboratory assistance from the Langley Research Center. Analysis HRE Ð Hypersonic Research Engine of the flight and ground data by both CIAM and NASA HRE AIM Ð Hypersonic Research Engine, resulted in the following preliminary conclusions. An Aerothermodynamic Integration Model unexpected control sensor reading caused non-optimal Hyper-X Ð NASA airframe integrated scramjet- fueling of the engine, and flowpath modifications added powered vehicle flight test program to the engine inlet during manufacture caused markedly ht Ð Total enthalpy (MJ/kg or Btu/lbm) reduced inlet performance. -
Chemical Kinetics of SCRAMJET Propulsion by Rodger Joseph Biasca Master of Science Aeronautics and Astronautics at the Massachus
Chemical Kinetics of SCRAMJET Propulsion by Rodger Joseph Biasca S.B. Aeronautics and Astronautics, Massachusetts Institute of Technology, 1987 SUBMITTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF Master of Science in Aeronautics and Astronautics at the Massachusetts Institute of Technology July 1988 ©1988, Rodger J. Biasca The author hereby grants to MIT and the Charles Stark Draper Laboratory, Inc. permission to reproduce and distribute copies of this thesis document in whole or in part. Signature of Author Department of Aeronautics and Astronautics July 1988 Certified by Professor Jean F. Louis, Co- Thesis Supervisor Department of Aeronautics and Astronautics Professor Manuel Martinez-Sanchez, Co- Thesis Supervisor pepartment of Aeronautics and Astronautics nr Phillin T). Hattis, Technical Supervisor s Stark Draper Laboratory Accepted by xtew,Ex3.*sh \. Professor Harold Y. Wachman,Chairman Department Graduate Committee MAOHUSET1S r1nTSrn OF TEO LOGY TH DRWN SEP 07 1988 A MVrN UU. fl~ u<;HZSR3ES~!'-~' Chemical Kinetics of SCRAMJET Propulsion by Rodger Joseph Biasca Submitted to the Department of Aeronautics and Astronautics in partial fulfillment of the requirements for the degree of Master of Science in Aeronautics and Astronautics Recent interest in hypersonics has focused on the development of a single stage to orbit vehicle propelled by hydrogen fueled SCRAMJETs. Necessary for the design of such a vehicle is a thorough understanding of the chemical kinetic mechanism of hydrogen-air combustion and the possible effect this mechanism may have on the performance of the SCRAMJET propulsion system. This thesis investigates possible operational limits placed on a SCRAMJET powered vehicle by the chemical kinetics of the combustion mechanism and estimates the performance losses associated with chemical kinetic effects. -
Reaction Engines and High-Speed Propulsion
Reaction Engines and High-Speed Propulsion Future In-Space Operations Seminar – August 7, 2019 Adam F. Dissel, Ph.D. President, Reaction Engines Inc. 1 Copyright © 2019 Reaction Engines Inc. After 60 years of Space Access…. Copyright © 2019 Reaction Engines Inc. …Some amazing things have been achieved Tangible benefits to everyday life Expansion of our understanding 3 Copyright © 2019 Reaction Engines Inc. Accessing Space – The Rocket Launch Vehicle The rocket launch vehicle (LV) has carried us far…however current launchers still remain: • Expensive • Low-Operability • Low-Reliability …Which increases the cost of space assets themselves and restricts growth of space market …little change in launch vehicle technology in almost 60 years… 1957 Today 4 Copyright © 2019 Reaction Engines Inc. Why All-Rocket LV’s Could Use Help All-rocket launch vehicles (LVs) are challenged by the physics that dictate performance thresholds…little improvement in key performance metrics have been for decades Mass Fraction Propulsion Efficiency – LH2 Example Reliability 1400000 Stage 2 Propellant 500 1.000 Propellent 450 1200000 Vehicle Structure 0.950 236997 400 1000000 350 0.900 300 800000 0.850 250 Launches 0.800 600000 320863 200 906099 150 400000 Orbital Successful 0.750 100 Hydrogen Vehicle Weights (lbs) Weights Vehicle 0.700 LV Reliability 454137 (seconds)Impulse 200000 50 Rocket Engines Hydrogen Rocket Specific Specific Rocket Hydrogen 0 0.650 0 48943 Falcon 9 777-300ER 1950 1960 1970 1980 1990 2000 2010 2020 1950 1960 1970 1980 1990 2000 2010 2020 Air-breathing enables systems with increased Engine efficiency is paramount but rocket Launch vehicle reliability has reached a plateau mass margin which yields high operability, technology has not achieved a breakthrough in and is still too low to support our vision of the reusability, and affordability decades future in space 5 Copyright © 2019 Reaction Engines Inc. -
Aircraft of Today. Aerospace Education I
DOCUMENT RESUME ED 068 287 SE 014 551 AUTHOR Sayler, D. S. TITLE Aircraft of Today. Aerospace EducationI. INSTITUTION Air Univ.,, Maxwell AFB, Ala. JuniorReserve Office Training Corps. SPONS AGENCY Department of Defense, Washington, D.C. PUB DATE 71 NOTE 179p. EDRS PRICE MF-$0.65 HC-$6.58 DESCRIPTORS *Aerospace Education; *Aerospace Technology; Instruction; National Defense; *PhysicalSciences; *Resource Materials; Supplementary Textbooks; *Textbooks ABSTRACT This textbook gives a brief idea aboutthe modern aircraft used in defense and forcommercial purposes. Aerospace technology in its present form has developedalong certain basic principles of aerodynamic forces. Differentparts in an airplane have different functions to balance theaircraft in air, provide a thrust, and control the general mechanisms.Profusely illustrated descriptions provide a picture of whatkinds of aircraft are used for cargo, passenger travel, bombing, and supersonicflights. Propulsion principles and descriptions of differentkinds of engines are quite helpful. At the end of each chapter,new terminology is listed. The book is not available on the market andis to be used only in the Air Force ROTC program. (PS) SC AEROSPACE EDUCATION I U S DEPARTMENT OF HEALTH. EDUCATION & WELFARE OFFICE OF EDUCATION THIS DOCUMENT HAS BEEN REPRO OUCH) EXACTLY AS RECEIVED FROM THE PERSON OR ORGANIZATION ORIG INATING IT POINTS OF VIEW OR OPIN 'IONS STATED 00 NOT NECESSARILY REPRESENT OFFICIAL OFFICE OF EOU CATION POSITION OR POLICY AIR FORCE JUNIOR ROTC MR,UNIVERS17/14AXWELL MR FORCEBASE, ALABAMA Aerospace Education I Aircraft of Today D. S. Sayler Academic Publications Division 3825th Support Group (Academic) AIR FORCE JUNIOR ROTC AIR UNIVERSITY MAXWELL AIR FORCE BASE, ALABAMA 2 1971 Thispublication has been reviewed and approvedby competent personnel of the preparing command in accordance with current directiveson doctrine, policy, essentiality, propriety, and quality. -
7. Transonic Aerodynamics of Airfoils and Wings
W.H. Mason 7. Transonic Aerodynamics of Airfoils and Wings 7.1 Introduction Transonic flow occurs when there is mixed sub- and supersonic local flow in the same flowfield (typically with freestream Mach numbers from M = 0.6 or 0.7 to 1.2). Usually the supersonic region of the flow is terminated by a shock wave, allowing the flow to slow down to subsonic speeds. This complicates both computations and wind tunnel testing. It also means that there is very little analytic theory available for guidance in designing for transonic flow conditions. Importantly, not only is the outer inviscid portion of the flow governed by nonlinear flow equations, but the nonlinear flow features typically require that viscous effects be included immediately in the flowfield analysis for accurate design and analysis work. Note also that hypersonic vehicles with bow shocks necessarily have a region of subsonic flow behind the shock, so there is an element of transonic flow on those vehicles too. In the days of propeller airplanes the transonic flow limitations on the propeller mostly kept airplanes from flying fast enough to encounter transonic flow over the rest of the airplane. Here the propeller was moving much faster than the airplane, and adverse transonic aerodynamic problems appeared on the prop first, limiting the speed and thus transonic flow problems over the rest of the aircraft. However, WWII fighters could reach transonic speeds in a dive, and major problems often arose. One notable example was the Lockheed P-38 Lightning. Transonic effects prevented the airplane from readily recovering from dives, and during one flight test, Lockheed test pilot Ralph Virden had a fatal accident. -
EMISSION CALCULATIONS for a SCRAMJET POWERED HYPERSONIC TRANS PORT by Erwin A
NASA TECHNICAL NASA TM X-71464 MEMORANDUM (NASA-TM-X-71464) EMISSION CALCULATIONS N74- 1244 FOR A'SCRANJET POWERED HYPERSONIC TRANSPORT (NASA) 32 p HC $3.75 CSCL 21E Unclas G3/28 2277 1 Cc EMISSION CALCULATIONS FOR A SCRAMJET POWERED HYPERSONIC TRANS PORT by Erwin A. Lezberg Lewis Research Center Cleveland, Ohio 44135 November, 1973 EMISSION CALCULATIONS FOR A SCRAMJET POWERED HYPERSONIC TRANSPORT by Erwin A. Lezberg Lewis Research Center ABSTRACT Calculations of exhaust emissions from a scramjet powered hy- personic transport burning hydrogen fuel have been performed over a range of Mach numbers of 5 to 12 to provide input data for wake mixing calculations and forecasts of future levels of pollutants in the strato- sphere. The calculations were performed utilizing a one-dimensional chem- ical kinetics computer program for the combustor and exhaust nozzle of a fixed geometry dual-mode scramjet engine. Inlet conditions to the combustor and engine size was based on a vehicle of 2.27x10 5 kg (500 000 lb) gross take of weight with engines sized for Mach 8 cruise. Nitric oxide emissions were very high for stoichiometric engine operation but for Mach 6 cruise at reduced equivalence ratio are in the range predicted for an advanced supersonic transport. Combustor de- signs which utilize fuel staging and rapid expansion to minimize resi- dence time at high combustion temperatures were found to be effective in preventing nitric oxide formation from reaching equilibrium concen- trations. INTRODUCTION Calculations of exhaust emissions from a scramjet powered hyper- sonic transport burning hydrogen fuel have been performed over a range of Mach numbers to provide input data for wake mixing calculations and forecasts of future levels of pollutants in the stratosphere.