Parametric Scramjet Analysis

Total Page:16

File Type:pdf, Size:1020Kb

Parametric Scramjet Analysis University of Mississippi eGrove Electronic Theses and Dissertations Graduate School 2014 Parametric Scramjet Analysis Jongseong Choi University of Mississippi Follow this and additional works at: https://egrove.olemiss.edu/etd Part of the Aerospace Engineering Commons Recommended Citation Choi, Jongseong, "Parametric Scramjet Analysis" (2014). Electronic Theses and Dissertations. 535. https://egrove.olemiss.edu/etd/535 This Thesis is brought to you for free and open access by the Graduate School at eGrove. It has been accepted for inclusion in Electronic Theses and Dissertations by an authorized administrator of eGrove. For more information, please contact [email protected]. PARAMETRIC SCRAMJET ANALYSIS A Thesis presented in partial fulfillment of requirements for the degree of Master of Science in the Department of Mechanical Engineering The University of Mississippi by JONGSEONG CHOI May 2014 Copyright Jongseong Choi 2014 ALL RIGHT RESERVED ABSTRACT The performance of a hypersonic flight vehicle will depend on existing materials and fuels; this work presents the performance of the ideal scramjet engine for three different combustion chamber materials and three different candidate fuels. Engine performance is explored by parametric cycle analysis for the ideal scramjet as a function of material maximum service temperature and the lower heating value of jet engine fuels. The thermodynamic analysis is based on the Brayton cycle as similarly employed in describing the performance of the ramjet, turbojet, and fanjet ideal engines. The objective of this work is to explore material operating temperatures and fuel possibilities for the combustion chamber of a scramjet propulsion system to show how they relate to scramjet performance and the seven scramjet engine parameters: specific thrust, fuel-to-air ratio, thrust-specific fuel consumption, thermal efficiency, propulsive efficiency, overall efficiency, and thrust flux. The information presented in this work has not been done by others in the scientific literature. This work yields simple algebraic equations for scramjet performance which are similar to that of the ideal ramjet, ideal turbojet and ideal turbofan engines. ii LIST OF SYMBOLS ao = freestream speed of sound, m/s 2 A2 = diffuser (engine inlet) exit area (Ae =A2), cm ; combustor entrance area A*/A = area ratio . cp = specific heat at constant pressure, kJ / (kg K) F = thrust, N F m o = specific thrust, N / (kg / s) . 2 gc = Newton’s constant, (kg m) / (N s ) h PR = fuel lower heating value, kJ / kg h o = freestream ambient enthalphy, kJ / kg h 9 = enthalphy at engine nozzle exit, kJ / kg h t2 = total enthalphy at combustor entrance, kJ / kg h t4 = total enthalphy at combustor exit, kJ / kg Mc = combustion Mach number Mo = Mach number at freestream flight conditions * Mo = freestream Mach number for maximum F m o ** Mo = freestream Mach number for minimum S *** M o = freestream Mach number for maximum F / A2 M9 = Mach number at engine nozzle exit (M9’ = M9’’ = M9 = Mo) iii m o = mass flow rate of air, kg / s m f = mass flow rate of fuel, kg / s Po = freestream static pressure, Pa P9 = static pressure at engine nozzle exit (Pe =P9), Pa (also P9’ and P9’’) Pto = freestream total pressure, Pa Pt2 = total pressure at combustor entrance, Pa (also P’’2) Pt4 = total pressure at combustor exit, Pa Pt9 = total pressure at engine nozzle inlet, Pa (also Pt9’ and Pt9’’) R = gas constant for air, kJ / (kg . K) s = entropy, (J / K) S = thrust-specific fuel consumption, mg / (N . s) T = temperature, K Tmax = material temperature limit, K T'max = burner exit total temperature, Mc < Mo, K T''max = burner exit total temperature, Mc ≥ Mo, K To = freestream ambient temperature, K Tto = freestream total temperature, K T2 = temperature at combustor entrance, K (also T’2) Tt2 = total temperature at combustor entrance, K (also T’’2) Tt4 = total temperature at combustor exit, K iv T9 = temperature at engine nozzle exit, K (also T9’ and T9’’) Tt9 = total temperature at engine nozzle inlet, K (also Tt9’ and Tt9’’) Vo = freestream velocity V9 = engine nozzle exit velocity (Ve = V9), m / s (also V9’ and V9’’) Wnetout = amount of work per unit time through the net area from T-s diagram, J / s Qin = heat flow rate by combustion, J / s γ = ratio of specific heats f = fuel-to-air ratio τ = total temperature ratio across burner, T / T , τ /τ b t4 t2 λ r τ d = total temperature ratio across diffuser, Tt2 / Tto τ n = total temperature ratio across nozzle, Tt9 / Tt4 2 τr = inlet temperature ratio, Tto / To = [1 + ( γ - 1) Mo / 2] τ = total temperature to freestream temperature ratio, Tt4 / To Tmax / To b = total pressure ratio across burner, Pt4 / Pt2 d = total pressure ratio across diffuser, Pt2 / Pto n = total pressure ratio across nozzle, Pt9 / Pt4 2 / 1 r = inlet pressure ratio, Pto / Po = [1 + (γ - 1) Mo / 2] T = thermal efficiency v P = propulsive efficiency o = overall efficiency vi ACKOWLEDGEMENTS I would like to gratefully acknowledge the enthusiastic supervision of Dr. Jeffrey A. Roux during this research. There has been his great contribution toward this thesis, which has yielded three journal publications in the past two years. I offer my sincerest appreciation for the learning opportunities and support provided by Dr. Arunachalam M. Rajendran. His guidance has provided me a thoughtful and rewarding journey. I would like to thank to Dr. Chung Song for general advice concerning scholastic life besides my research. While data collecting and researching, Kiyun Kim spent countless hours listening to me talk about my thoughts on my research. I am grateful to all my friends from KSA and OKCC. I have received support and encouragement from my friend group named Sekye from Korea. Finally, I am forever indebted to my parents for their understanding, endless patience, and encouragement when it was most required. vii TABLE OF CONTENTS ABSTRACT ........................................................................................................................... ii LIST OF SYMBOLS ............................................................................................................... iii ACKOWLEDGEMENTS ...................................................................................................... vii TABLE OF CONTENTS ...................................................................................................... viii LIST OF TABLES .................................................................................................................. xi LIST OF FIGURES ................................................................................................................ xv INTRODUCTION .....................................................................................................................1 1.1 Hypersonic Propulsion .............................................................................................1 1.2 Parametric Thermodynamic Cycle Analysis for Ideal Engines .................................2 1.3 Definition .................................................................................................................3 1.3.1 Ramjet ...................................................................................................................3 1.3.2 Scramjet ................................................................................................................5 1.4 Scramjet Components ...............................................................................................8 1.5 Historical Development ............................................................................................9 1.6 Materials and Fuels Candidates .............................................................................. 13 1.6.1 Materials ............................................................................................................. 14 viii 1.6.2 Fuels ................................................................................................................... 15 1.7 This Work .............................................................................................................. 17 STATEMENT OF THE PROBLEM...................................................................................... 19 2.1 Definition of the Problem ....................................................................................... 19 2.2 T-s Diagram .......................................................................................................... 20 2.2.1 Situations for Mc < Mo ......................................................................................... 21 2.2.2 Situations for Mc ≥ Mo ......................................................................................... 24 2.3 Materials and Fuels Selection ................................................................................. 25 ANALYSIS .......................................................................................................................... 27 3.1 Fundamental Assumptions for Parametric Analysis ................................................ 27 3.2 Parametric Analysis for Ideal Mass Flow Scramjet ................................................. 28 3.2.1 Summary of Equations – Ideal Mass Flow Scramjet ............................................ 36 3.3 Parametric Analysis for Non-Ideal Mass Flow Scramjet ......................................... 37 3.3.1 Summary of Equations – Non-Ideal Mass Flow Scramjet .................................... 43 * 3.4 Optimum Freestream Mach Number
Recommended publications
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • Supersonic Combustion in Air-Breathing Propulsion Systems for Hypersonic Flight
    FL50CH23_Urzay ARI 22 November 2017 21:18 Annual Review of Fluid Mechanics Supersonic Combustion in Air-Breathing Propulsion Systems for Hypersonic Flight Javier Urzay Center for Turbulence Research, Stanford University, Stanford, California 94305-3024; email: [email protected] Annu. Rev. Fluid Mech. 2018. 50:593–627 Keywords The Annual Review of Fluid Mechanics is online at hypersonics, compressible flows, turbulent combustion, scramjets, fluid.annualreviews.org high-speed chemical propulsion, sound barrier https://doi.org/10.1146/annurev-fluid-122316- 045217 Abstract Copyright c 2018 by Annual Reviews. Annu. Rev. Fluid Mech. 2018.50:593-627. Downloaded from www.annualreviews.org Great efforts have been dedicated during the last decades to the research and All rights reserved development of hypersonic aircrafts that can fly at several times the speed of sound. These aerospace vehicles have revolutionary applications in national security as advanced hypersonic weapons, in space exploration as reusable ANNUAL stages for access to low Earth orbit, and in commercial aviation as fast long- REVIEWS Further Access provided by Stanford University - Main Campus Robert Crown Law Library on 01/05/18. For personal use only. Click here to view this article's range methods for air transportation of passengers around the globe. This online features: review addresses the topic of supersonic combustion, which represents the • Download figures as PPT slides • Navigate linked references central physical process that enables scramjet hypersonic propulsion systems • Download citations • Explore related articles to accelerate aircrafts to ultra-high speeds. The description focuses on recent • Search keywords experimental flights and ground-based research programs and highlights associated fundamental flow physics, subgrid-scale model development, and full-system numerical simulations.
    [Show full text]
  • A Parametric Analysis on the Performance of Ideal Scramjets Dan Londrico Cleveland State University
    A Parametric Analysis on the Performance of Ideal Scramjets Dan Londrico Cleveland State University Abstract and Background Results Supersonic combustion ramjets, known as The plots show specific thrust, fuel-air ratio, and thrust scramjets, are useful for applications where specific fuel consumption for the three combustor hypersonic flight is desired. Main areas of materials, and fuel-air ratio for the four fuels. research include the use of alternative fuels to reduce system weight and increase performance, and suitable combustor materials to allow for the high temperatures occurring in scramjets, and improve performance. While the research is promising, physical testing in scramjet engines can be expensive. Numerical models offer a good alternative to physical testing, and can be used to analyze trends, and to help direct physical models. The purpose of this research is to analyze the performance of a scramjet numerically using an ideal, one-dimensional thermodynamic model. Methods Conclusion • An ideal system was setup for the analysis • The data from this analysis shows: using these assumptions: • the three alternative fuels used can produce a lower • Isentropic diffuser and exhaust fuel air ratio than JP-7. • Combustion treated as constant heat • increasing the maximum allowable temperature of the addition process combustor increases thrust output, but also increases • Combustion occurs under constant Mach fuel consumption. number • Inlet and outlet pressures are equal • Calorically perfect air as operating fluid Future Work • Combustor materials were varied, and were modelled using their maximum allowable • Future work on this includes: temperature (T): • Performing the analysis using combustion conditions • Inconel, T = 1700K other than constant Mach number, such as constant • C-SiC, T = 1900K velocity, area, or pressure.
    [Show full text]
  • Supersonic Combustion Ramjet: Analysis on Fuel Options
    SUPERSONIC COMBUSTION RAMJET: ANALYSIS ON FUEL OPTIONS by Stephanie W. Barone A thesis submitted to the faculty of The University of Mississippi in partial fulfillment of the requirements of the Sally McDonnell Barksdale Honors College. Oxford May 2004 Approved by ___________________________________ Advisor: Dr. Jeffrey Roux ___________________________________ Reader: Dr. Erik Hurlen ___________________________________ Reader: Dr. John O’Haver 1 © 2016 STEPHANIE BARONE ALL RIGHTS RESERVED 2 ABSTRACT STEPHANIE BARONE: Supersonic Combustion Ramjet: Analysis on Fuel Options This report focuses on different fuel options available to use for scramjet engines. The advantages and disadvantages of JP-7, JP-8, and hydrogen fuels are covered, also the effectiveness and requirements for each fuel are discussed. The recent history of the scramjet engine is included as well as its advantages and disadvantages. An explanation of what each fuel option encompasses and engineering analysis for each fuel are shown. The equations presented for the parametric analysis are shown as functions of the freestream Mach number, with the combustion Mach number as a parameter. The results can be seen for the theoretical possibilities of the scramjet engine and the most likely operating situations. Hydrogen has the highest lower heating value which makes it very appealing to use as a fuel, but it is not very dense so more volume of it is needed to create enough energy. The hydrocarbon fuels, JP-7 and JP-8, have half the value of hydrogen for the lower heating value
    [Show full text]
  • Scramjet Inlets
    Scramjet Inlets Professor Michael K. Smart Chair of Hypersonic Propulsion Centre for Hypersonics The University of Queensland Brisbane 4072 AUSTRALIA [email protected] ABSTRACT The supersonic combustion ramjet, or scramjet, is the engine cycle most suitable for sustained hypersonic flight in the atmosphere. This article describes some challenges in the design of the inlet or intake of these hypersonic air-breathing engines. Scramjet inlets are a critical component and their design has important effects on the overall performance of the engine. The role of the inlet is first described, followed by a description of inlet types and some past examples. Recommendations on the level of compression needed in scramjets are then made, followed by a design example of a three-dimensional scramjet inlet for use in an access-to-space system that must operate between Mach 6 and 12. NOMENCLATURE A area (m2) x axial distance (m) Cf skin friction coefficient φ equivalence ratio D diameter (m); Drag (N) ϑ constant in mixing curve fst stoichiometric ratio ηc combustion efficiency F stream thrust (N) ηKE kinetic energy efficiency Fadd additive drag (N) ηKE_AD adiabatic kinetic energy efficiency Fun uninstalled thrust (N) ηo overall scramjet efficiency h enthalpy (289K basis) (J/kg) ηn nozzle efficiency h heat of combustion (J/kg of fuel) pr H total enthalpy (298K basis) (J/kg) t Subscript L length (m) c cowl m mass capture ratio c comb combustor m& mass flow rate (kg/s) f fuel M Mach number in inflow P pressure (Pa) out outflow Q heat loss (kJ) q dynamic pressure (Pa) isol isolator T temperature (K); thrust (N) n,N nozzle u,V velocity (m/s) SEP separation RTO-EN-AVT-185 9 - 1 Scramjet Inlets 1.0 INTRODUCTION The desire for hypersonic flight within the atmosphere has motivated multiple generations of aerodynamicists, scientists and engineers.
    [Show full text]
  • Jet Propulsion Engines
    JET PROPULSION ENGINES 5.1 Introduction Jet propulsion, similar to all means of propulsion, is based on Newton’s Second and Third laws of motion. The jet propulsion engine is used for the propulsion of aircraft, m issile and submarine (for vehicles operating entirely in a fluid) by the reaction of jet of gases which are discharged rearw ard (behind) with a high velocity. A s applied to vehicles operating entirely in a fluid, a momentum is imparted to a mass of fluid in such a manner that the reaction of the imparted momentum furnishes a propulsive force. The magnitude of this propulsive force is termed as thrust. For efficient production of large power, fuel is burnt in an atmosphere of compressed air (combustion chamber), the products of combustion expanding first in a gas turbine which drives the air compressor and then in a nozzle from which the thrust is derived. Paraffin is usually adopted as the fuel because of its ease of atomisation and its low freezing point. Jet propulsion was utilized in the flying Bomb, the initial compression of the air being due to a divergent inlet duct in which a sm all increase in pressure energy w as obtained at the expense of kinetic energy of the air. Because of this very limited compression, the thermal efficiency of the unit was low, although huge power was obtained. In the normal type of jet propulsion unit a considerable improvement in efficiency is obtained by fitting a turbo-com pressor which w ill give a com pression ratio of at least 4:1.
    [Show full text]
  • 04 Propulsion
    Aircraft Design Lecture 2: Aircraft Propulsion G. Dimitriadis and O. Léonard APRI0004-­1, Aerospace Design Project, Lecture 4 1 Introduction • A large variety of propulsion methods have been used from the very start of the aerospace era: – No propulsion (balloons, gliders) – Muscle (mostly failed) – Steam power (mostly failed) – Piston engines and propellers – Rocket engines – Jet engines – Pulse jet engines – Ramjet – Scramjet APRI0004-­1, Aerospace Design Project, Lecture 4 2 Gliding flight • People have been gliding from the-­ mid 18th century. The Albatross II by Jean Marie Le Bris-­ 1849 Otto Lillienthal , 1895 APRI0004-­1, Aerospace Design Project, Lecture 4 3 Human-­powered flight • Early attempts were less than successful but better results were obtained from the 1960s onwards. Gerhardt Cycleplane (1923) MIT Daedalus (1988) APRI0004-­1, Aerospace Design Project, Lecture 4 4 Steam powered aircraft • Mostly dirigibles, unpiloted flying models and early aircraft Clément Ader Avion III (two 30hp steam engines, 1897) Giffard dirigible (1852) APRI0004-­1, Aerospace Design Project, Lecture 4 5 Engine requirements • A good aircraft engine is characterized by: – Enough power to fulfill the mission • Take-­off, climb, cruise etc. – Low weight • High weight increases the necessary lift and therefore the drag. – High efficiency • Low efficiency increases the amount fuel required and therefore the weight and therefore the drag. – High reliability – Ease of maintenance APRI0004-­1, Aerospace Design Project, Lecture 4 6 Piston engines • Wright Flyer: One engine driving two counter-­ rotating propellers (one port one starboard) via chains. – Four in-­line cylinders – Power: 12hp – Weight: 77 kg APRI0004-­1, Aerospace Design Project, Lecture 4 7 Piston engine development • During the first half of the 20th century there was considerable development of piston engines.
    [Show full text]