The Modelling and Optimisation of High Performance Internal Combustion Engines

Total Page:16

File Type:pdf, Size:1020Kb

The Modelling and Optimisation of High Performance Internal Combustion Engines The Modelling and Optimisation of High Performance Internal Combustion Engines by Julian Ross Panting A thesis submitted for the degree of Doctor of Philosophy of the Faculty of Engineering, University of London, and the Diploma of Imperial College July 1993 Department of Mechanical Engineering Imperial College of Science, Technology and Medicine University of London 1 Abstract The project described addresses the numerical modelling of two types of small, novel internal combustion engines of unusually high power/weight ratio in order to obtain data upon their suitability for automotive application. The particular data sought are reliable estimates of the part and full load thermal efficiencies and the maximum specific power output level. The engine types studied are an unusual form of two shaft gas turbine with and without a heat exchanger, and a compound highly turbocharged, spark ignition, high speed, four stroke piston engine. The latter may be considered a hybrid of gas turbine and spark ignition piston engines. Maximum specific power output projections are based upon the assumption of high turbine entry temperatures of the order of 1600K. This in turn would require future use of ceramics technology if an uncooled turbine were to be used. It is assumed the engine is coupled with a continuously variable transmission, which permits greater flexibility in engine operation and hence enhanced performance levels. The numerical models used are of well known types - iterative matching calculations based on turbomachinery maps for the gas turbine simulations and the filling and emptying model type for the compound turbocharged engine calculations. A feature of the studies as applied to the latter engine type is the use of a sophisticated multi - dimensional optimisation algorithm to maximise simulated engine performance. The particular algorithm used is of the well known conjugate - gradient type. With this algorithm, the value of a number of independent input parameters can each be chosen to obtain the best engine performance, with this being defined, for the purposes of this work, as the specific power output. 2 Acknowledgements My thanks go to the following people. To my supervisor, Dr. N.Baines for providing support and encouragement and for arranging a special grant which enabled my third year studies to continue. To my parents and sister for also providing support and encouragement and to my parents for providing considerable financial assistance. To Rev. W.Raines for arranging my student accommodation. To Dr. S.Etemad for permitting me to use his section's computing facilities. Finally to the Imperial College Computer Centre help desk for providing much helpful advice. 3 CONTENTS Chapter (1) Considerations for the Optimum Design of a High Specific Output, High Thermal Efficiency Powertrain (1.1) Overview 23 (1.2) Continuously Variable Transmission Design 27 (1.3) Hybrid Vehicles- 31 (1.4) Compact, High Efficiency Engines - the Gas Turbine verses the Compound Highly Turbocharged Engine 34 (1.5) Simultaneously Optimising Many Design Parameters and the use of Continuously Variable Mechanisms 36 (1.6) Emissions Considerations 39 (1.7) Turbine Entry Temperature Limits 40 (1.8) The Structure of this Thesis 41 (1.9) References 43 4 Chapter (2) The Determination of Fluid Properties (2.1) Overview 57 (2.2) The Calculation of Fluid Properties for 'Low' Temperatures 59 (2.3) The Calculation of Fluid Properties for 'High' Temperatures 62 (2.3.1) Burnt Fuel/Air Mixture Properties 62 (2.3.2) Concerning the Calculation of the Specific Gas Constant 66 (2.3.3) Unburnt Fuel Vapour Properties 67 (2.3.4) Combining Burnt and Unburnt Gas Mixture Properties 68 (2.3.5) The Fuel Heat Content Value 69 (2.4) Summary 70 (2.5) References 71 5 Chapter (3) Automotive Gas Turbine Studies (3.1) Overview 90 (3.2) Basic Gas Turbine Performance Analysis 92 (3.3) The use of Turbomachinery Characteristics 97 (3.4) The General Calculation Procedure Invoking the use of Turbomachinery Characteristics and Variable Properties 99 (3.5) Modelling a Single Shaft, Constant Speed Gas Turbine without Variable Geometry 102 (3.6) Modelling the Twin Shaft Differential Gas Turbine without Variable Geometry 105 (3.7) A Note Concerning the Differential Gas Turbine Operating Schedule 107 (3.8) Alternative Gas Turbine Concepts which were not Modelled 107 (3.9) Summary 109 (3.10)References 110 6 Chapter (4) The Compound Highly Turbocharged Engine (4.1) Overview 129 (4.2) The Theoretical Advantages of the Compound Turbocharged Engine 131 (4.2.1) The Efficiency of the Compound Turbocharged Engine in a Limiting Case 131 (4.2.2) Consideration of the Optimum Pressure Ratio for Efficiency for the Gas Turbine 133 (4.2.3) The Compound Turbocharged Engine Considered as a High Pressure Ratio Unit 135 (4.2.4) The Specific Power Outputs of Various Engine Types Compared 139 (4.2.5) Further Considerations 141 (4.3) A Brief Review of Past Compound Turbocharged Engine Designs 142 (4.4) Justifying Further Research into the Compound Turbocharged Engine 143 (4.5) The Proposed Design Layout 144 (4.5.1) Four Cylinder Layout 145 (4.5.2) Four Stroke, Spark Ignition, High Speed Cycle 145 (4.5.3) Hybrid Sleeve/Aspin Valves 145 (4.5.4) Swash Plate Crank Mechanism 147 (4.5.5) Variable Cylinder Compression Ratio 148 (4.5.6) Throttleless Concept 149 (4.5.7) High TET Operation 150 (4.5.8) The Overall Concept 150 (4.6) The Turbine Entry Temperature Limit 152 (4.7) Transient Response 154 (4.8) A Simple Quasi-Steady Compound Turbocharged Engine Model 154 (4.9) Summary 157 (4.10)References 158 7 Chapter (5) Time - Marching Numerical Models of Naturally Aspirated and Compound Turbocharged Spark Ignition Piston Engines (5.1) Overview 175 (5.2) A Comparison of Modelling Strategies 176 (5.3) The Filling and Emptying Model 178 (5.3.1) The Governing Ordinary Differential Equations 178 (5.3.2) The Mass Flow Differential Equation 180 (5.3.2.1) The Basic Mass Flow Rate Equation 180 (5.3.2.2) Determination of the Flow Coefficient and Port Area 182 (5.3.3) The Energy Flow Rate Differential Equation 184 (5.3.3.1) Combustion Simulation 184 (5.3.3.2) The Heat Transfer Rate 187 (5.3.3.3) Modelling Direct Fuel Injection 188 (5.3.3.4) Cylinder Volume Calculation 189 (5.3.3.5) Frictional Loss Calculations 190 (5.3.4) Convergence of the Solution 191 (5.3.5) The Order of Integration 192 (5.4) Modifications to Produce a Compound Turbocharged Filling and Emptying Model 192 (5.4.1) The use of Turbomachinery Characteristics 192 (5.4.2) Modelling an Aftercooler 197 (5.4.3) The use of a Variable Cylinder Volumetric Compression Ratio 198 (5.4.4) Estimating the Turbine Entry Temperature 199 (5.5) Determining the Power Output and Brake Thermal Efficiency 199 (5.6) Summary 200 (5.7) References 201 8 Chapter (6) Ensuring the Stability of the Integration of the Mass Balance O.D.E. (6.1) Overview 215 (6.2) An Example of the Mass Flow Rate Calculation Instability Problem 216 (6.3) Analytic Stability of Integration of an O.D.E. 217 (6.4) The Numerical Stability of the First Order Euler Scheme 221 (6.5) Applying the Stability Condition 222 (6.6) Numerical Integration and Ill - Conditioned Problems 223 (6.7) Controlling the Ill - Conditioned Problem 226 (6.8) The Complete Algorithm 229 (6.9) Summary 229 (6.10)References 231 9 Chapter (7) Minimisation of a Function of a Vector - and the Application of this Technique to Powertrain Design Optimisation (7.1) Overview 236 (7.2) Multi - Dimensional Optimisation Methods Employing Line Minimisations 239 (7.2.1) The Orthogonal Directions Method 240 (7.2.2) The Method of Steepest Descent 241 (7.2.3) The use of Conjugate Directions 241 (7.2.3.1) The Conjugate Directions Method 244 (7.2.3.2) The Conjugate Gradient Method 245 (7.2.4) Quasi - Newton or Variable Metric Methods 246 (7.3) Multi - Dimensional Optimisation Employing the 'Monte-Carlo' Technique 247 (7.4) The Choice of Multi - Dimensional Optimisation Method 248 (7.5) Bracketing the Minimum and Employing a Line Minimisation Technique 249 (7.6) Calculating the Distances to the Input Vector Boundaries 253 (7.7) Evaluating the Gradient Vector 256 (7.8) Convergence of the Solution 257 (7.9) Applying the Multi - Dimensional Minimisation Technique to Powertrain Design Optimisation 257 (7.10)Summary 259 (7.11)References 260 10 Chapter (8) Numerical Results (8.1) The Gas Turbine Models 262 (8.2) Validation of the Piston Engine Models 265 (8.3) Optimisation Results 267 (8.3.1) Employing Test Mathematical Functions 267 (8.3.2) Employing the Quasi-Steady Piston Engine Models 267 (8.3.3) Employing the Filling and Emptying Piston Engine Models 269 (8.3.4) Part Validation of the Optimisation Results 272 (8.4) Further Aspects of the Filling and Emptying Piston Engine Modelling 274 (8.4.1) Increasing the Bore/Stroke Ratio of the Naturally Aspirated Engine 274 (8.4.2) Some Adjustments to the Compound Turbocharged Engine Model Input Parameters 274 (8.4.3) Part Load Efficiency Contours 276 (8.4.4) Further Data from the Compound Turbocharged Engine Model 278 (8.5) Comparing the Gas Turbine and Piston Engines' Specific Power Output Figures 278 (8.6) References 280 11 Chapter (9) Conclusions and Suggestions for Further Work (9.1) Conclusions 320 (9.1.1) The Gas Turbine Simulations 320 (9.1.2) The Compound Turbocharged Engine Simulations 321 (9.1.3) Comparisons Between the Gas Turbine and Compound Turbocharged Engine Simulations 323 (9.1.4) The Optimisation Procedure 325 (9.2) Suggestions for Further Work 326 (9.2.1) Modifications to the Filling and Emptying Method 326
Recommended publications
  • Turbocompound Reheat Gas Turbine Combined Cycle 2015
    INFRASTRUCTURE MINING & METALS NUCLEAR, SECURITY & ENVIRONMENTAL OIL, GAS & CHEMICALS Turbocompound Reheat Gas Turbine Combined Cycle 2015 Turbocompound Reheat Gas Turbine Combined Cycle S. Can Gülen Mark S. Boulden Bechtel Infrastructure Power POWER-GEN INTERNATIONAL 2015 December 8 - 10, 2015 Las Vegas Convention Center Las Vegas, NV USA ABSTRACT This paper discusses a new power generation cycle based on the fundamental thermodynamic concepts of constant volume combustion and reheat. The turbo- compound reheat gas turbine combined cycle (TC-RHT GTCC) comprises three pieces of rotating equipment: A turbo-compressor and two prime movers, i.e., a reciprocating gas engine and an industrial (heavy duty) gas turbine. Ideally, the cycle is proposed as the foundation of a customized power plant design of a given size and performance by combining different prime movers with new "from the blank sheet" designs. Nevertheless, a compact power plant based on the TC-RHT cycle can also be constructed by combining off-the-shelf equipment with modifications for immediate implementation. The paper describes the underlying thermodynamic principles, representative cycle calculations and value proposition as well as requisite modifications to the existing hardware. The operational philosophy governing plant start-up, shut-down and loading is described in detail. Also included in the paper is a 110 MW reference power block concept with 57+% net efficiency. The concept has been developed using a pre-engineered standard block approach and is amenable to simple “module-by-module” construction including easy shipment of individual components. POWER-GEN INTERNATIONAL 2015 Page 1 OF 26 INTRODUCTION Brief History Internal combustion engines can be classified into two major categories based on the heat addition portion of their respective thermodynamic cycles: “constant volume” and “constant pressure” heat addition engines (cycles) [1].
    [Show full text]
  • The TSR-2: a BRITISH STORY with an AUSTRALIAN CHAPTER
    RAAF Radschool Association Magazine – Vol 32 Page 15 The TSR-2: A BRITISH STORY WITH AN AUSTRALIAN CHAPTER With the era of the F-111 coming to a close, it is timely to reflect on the development of this aircraft and the rivals that existed at the time of its selection. The principal competitor was the British Aircraft Corporation’s Tactical Strike and Reconnaissance (TSR-2) aircraft. However, as indicated by Sir Sydney Camm’s comment, the development and subsequent abrupt cancellation of the project in 1965 was politically charged. While it was suggested at the time that Australia played a key role in the demise of the TSR-2, there appears to have been many other contributors to its downfall. From the mid 1950s, the RAF and subsequently the RAAF identified the need to replace the Canberra bomber, focusing on a nuclear-capable aircraft. Given the rapid advances in anti-aircraft weaponry capability, having supersonic strike aircraft that could slip under radar surveillance was seen as a priority. The development of the TSR-2 was also the result of the British Government’s focus in the late 1950s on rationalising the eight main British aircraft manufacturers that then existed. On New Year’s Day 1959, Vickers-Armstrong and English Electric, amalgamated as the new British Aircraft Corporation (BAC), were awarded the contract to combine their earlier individual designs into the TSR-2. Later that year Bristol- Siddeley were awarded the contract for development of the Olympus engines which were to power the aircraft. Like the development of any aircraft, the TSR-2 had its technical problems.
    [Show full text]
  • Los Motores Aeroespaciales, A-Z
    Sponsored by L’Aeroteca - BARCELONA ISBN 978-84-608-7523-9 < aeroteca.com > Depósito Legal B 9066-2016 Título: Los Motores Aeroespaciales A-Z. © Parte/Vers: 1/12 Página: 1 Autor: Ricardo Miguel Vidal Edición 2018-V12 = Rev. 01 Los Motores Aeroespaciales, A-Z (The Aerospace En- gines, A-Z) Versión 12 2018 por Ricardo Miguel Vidal * * * -MOTOR: Máquina que transforma en movimiento la energía que recibe. (sea química, eléctrica, vapor...) Sponsored by L’Aeroteca - BARCELONA ISBN 978-84-608-7523-9 Este facsímil es < aeroteca.com > Depósito Legal B 9066-2016 ORIGINAL si la Título: Los Motores Aeroespaciales A-Z. © página anterior tiene Parte/Vers: 1/12 Página: 2 el sello con tinta Autor: Ricardo Miguel Vidal VERDE Edición: 2018-V12 = Rev. 01 Presentación de la edición 2018-V12 (Incluye todas las anteriores versiones y sus Apéndices) La edición 2003 era una publicación en partes que se archiva en Binders por el propio lector (2,3,4 anillas, etc), anchos o estrechos y del color que desease durante el acopio parcial de la edición. Se entregaba por grupos de hojas impresas a una cara (edición 2003), a incluir en los Binders (archivadores). Cada hoja era sustituíble en el futuro si aparecía una nueva misma hoja ampliada o corregida. Este sistema de anillas admitia nuevas páginas con información adicional. Una hoja con adhesivos para portada y lomo identifi caba cada volumen provisional. Las tapas defi nitivas fueron metálicas, y se entregaraban con el 4 º volumen. O con la publicación completa desde el año 2005 en adelante. -Las Publicaciones -parcial y completa- están protegidas legalmente y mediante un sello de tinta especial color VERDE se identifi can los originales.
    [Show full text]
  • US5507253.Pdf
    |||||||||| USO05507253A United States Patent (19) 11 Patent Number: 5,507,253 Lowi, Jr. (45) Date of Patent: Apr. 16, 1996 54 ADABATIC, TWO-STROKECYCLE ENGINE ing,” SAE Paper 650007. HAVING PSTON-PHASING AND John C. Basiletti and Edward F. Blackburne, Dec. 1966, COMPRESSION RATO CONTROL SYSTEM "Recent Developments in Variable Compression Ratio Engines.” SAE Paper 660344. 76 Inventor: Alvin Lowi, Jr., 2146 Toscanini Dr., L. J. K. Setright, "Some Unusual Engines,” Dec. 1975, pp. Rancho Palos Verde, Calif. 90732 99-105, 109-111. R. Kamo, W. Bryzik and P. Glance Dec. 1987, "Adiabatic (21) Appl. No.: 311,348 Engine Trends-Worldwide,” SAE Paper 870018. (22 Filed: Sep. 23, 1994 S. G. Timony, M. H. Farmer and D. A. Parker, Dec. 1987, "Preliminary Experiences with a Ceramics Evaluation Related U.S. Application Data Engine Rig.” SAE Paper 870021. Paul and Humphrheys, Dec. 1952, SAE Transactions No. 6, 63 Continuation of Ser. No. 112,887, Aug. 27, 1993, Pat. No. 5,375,567. p. 259. (51) Int. Cl." ......................................... FO2B 75/26 Primary Examiner-Marguerite Macy I52 U.S. Cl. .................................... 123/S6.9 Attorney, Agent, or Firm-Bruce M. Canter 58) Field of Search .................................. 123/55.7, 56.1, 123/56.2, 56.8, 56.9, 51 B, 193.6 57) ABSTRACT An engine structure and mechanism that operates on various 56) References Cited combustion processes in a two-stroke-cycle without supple U.S. PATENT DOCUMENTS mental cooling or lubrication comprises an axial assembly of cylindrical modules and twin, double-harmonic cams that 1,127,267 2/1915 McElwain .............................. 123/56.8 operate with opposed pistons in each cylinder through fully 1,339,276 5/1920 Murphy .................................
    [Show full text]
  • Principles of an Internal Combustion Engine
    Principles of an Internal Combustion Engine Course No: M03-046 Credit: 3 PDH Elie Tawil, P.E., LEED AP Continuing Education and Development, Inc. 22 Stonewall Court Woodcliff Lake, NJ 076 77 P: (877) 322-5800 [email protected] Chapter 2 Principles of an Internal Combustion Engine Topics 1.0.0 Internal Combustion Engine 2.0.0 Engines Classification 3.0.0 Engine Measurements and Performance Overview As a Construction Mechanic (CM), you are concerned with conducting various adjustments to vehicles and equipment, repairing and replacing their worn out broken parts, and ensuring that they are serviced properly and inspected regularly. To perform these duties competently, you must fully understand the operation and function of the various components of an internal combustion engine. This makes your job of diagnosing and correcting troubles much easier, which in turn saves time, effort, and money. This chapter discusses the theory and operation of an internal combustion engine and the various terms associated with them. Objectives When you have completed this chapter, you will be able to do the following: 1. Understand the principles of operation, the different classifications, and the measurements and performance standards of an internal combustion engine. 2. Identify the series of events, as they occur, in a gasoline engine. 3. Identify the series of events, as they occur in a diesel engine. 4. Understand the differences between a four-stroke cycle engine and a two-stroke cycle engine. 5. Recognize the differences in the types, cylinder arrangements, and valve arrangements of internal combustion engines. 6. Identify the terms, engine measurements, and performance standards of an internal combustion engine.
    [Show full text]
  • Electric Boosting and Energy Recovery Systems for Engine Downsizing
    energies Review Electric Boosting and Energy Recovery Systems for Engine Downsizing Mamdouh Alshammari 1,2, Fuhaid Alshammari 2 and Apostolos Pesyridis 1,* 1 Centre of Advanced Powertrain and Fuels (CAPF), Department of Mechanical, Aerospace and Civil Engineering, Brunel University London, Middlesex UB8 3PH, UK; [email protected] 2 Department of Mechanical Engineering, University of Hai’l, Hail 55476, Saudi Arabia; [email protected] * Correspondence: [email protected] Received: 31 October 2019; Accepted: 4 December 2019; Published: 6 December 2019 Abstract: Due to the increasing demand for better fuel economy and increasingly stringent emissions regulations, engine manufacturers have paid attention towards engine downsizing as the most suitable technology to meet these requirements. This study sheds light on the technology currently available or under development that enables engine downsizing in passenger cars. Pros and cons, and any recently published literature of these systems, will be considered. The study clearly shows that no certain boosting method is superior. Selection of the best boosting method depends largely on the application and complexity of the system. Keywords: engine downsizing; electrically assisted turbocharger; electric supercharger; e-turbo; waste heat recovery; turbocharging; supercharging; turbocompounding; organic Rankine cycle 1. Introduction Although internal combustion engines are getting more efficient nowadays, still the major part of fuel energy is transformed into wasted heat. In terms of harmful exhaust emissions, the transportation sector is responsible for the one-third of CO2 emissions worldwide and approximately 15% of the overall greenhouse gas emissions [1]. Moreover, owing to the limited amount of fossil fuels, prices fluctuate significantly, with consistent general rising trends, resulting in economic issues in non-oil-producing countries.
    [Show full text]
  • Mathematical Modeling and Analysis of Gas Torque in Twinrotor Piston
    J. Cent. South Univ. (2013) 20: 3536−3544 DOI: 10.1007/s11771­013­1879­y Mathematical modeling and analysis of gas torque in twin­rotor piston engine DENG Hao(邓豪) 1, 2, PAN Cun­yun(潘存云) 1, XU Xiao­jun(徐小军) 1, ZHANG Xiang(张湘) 1 1. College of Mechatronic Engineering and Automation, National University of Defense Technology, Changsha 410073, China; 2. Naval Aeronautical Engineering Institute, Qingdao Branch, Qingdao 266041, China © Central South University Press and Springer­Verlag Berlin Heidelberg 2013 Abstract: The gas torque in a twin­rotor piston engine (TRPE) was modeled using adiabatic approximation with instantaneous combustion. The first prototype of TRPE was manufactured. This prototype is intended for high power density engines and can produce 36 power strokes per shaft revolution. Compared with the conventional engines, the vector sum of combustion gas forces acting on each rotor piston in TRPE is a pure torque, and the combustion gas rotates the rotors while compresses the gas in the compression chamber at the same time. Mathematical modeling of gas force transmission was built. Expression for gas torque on each rotor was derived. Different variation patterns of the volume change of working chamber were introduced. The analytical and numerical results is presented to demonstrate the main characteristics of gas torque. The results show that the value of gas torque in TRPE falls to be less than zero before the combustion phase is finished; the time for one stroke is 30° in terms of the rotating angle of the output shaft; gas torque in one complete revolution of the output shaft has a period which is equal to 60° and it is necessary to put off the moment when gas torque becomes zero in order to export the maximum energy.
    [Show full text]
  • 19FFL-0023 2-Stroke Engine Options for Automotive Use: a Fundamental Comparison of Different Potential Scavenging Arrangements for Medium-Duty Truck Applications
    Citation for published version: Turner, J, Head, RA, Chang, J, Engineer, N, Wijetunge, RS, Blundell, DW & Burke, P 2019, '2-Stroke Engine Options for Automotive Use: A Fundamental Comparison of Different Potential Scavenging Arrangements for Medium-Duty Truck Applications', SAE Technical Paper Series, pp. 1-21. https://doi.org/10.4271/2019-01-0071 DOI: 10.4271/2019-01-0071 Publication date: 2019 Document Version Peer reviewed version Link to publication The final publication is available at SAE Mobilus via https://doi.org/10.4271/2019-01-0071 University of Bath Alternative formats If you require this document in an alternative format, please contact: [email protected] General rights Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. Take down policy If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim. Download date: 27. Sep. 2021 Paper Offer 19FFL-0023 2-Stroke Engine Options for Automotive Use: A Fundamental Comparison of Different Potential Scavenging Arrangements for Medium-Duty Truck Applications Author, co-author (Do NOT enter this information. It will be pulled from participant tab in MyTechZone) Affiliation (Do NOT enter this information. It will be pulled from participant tab in MyTechZone) Abstract For the opposed-piston engine, once the port timing obtained by the optimizer had been established, a supplementary study was conducted looking at the effect of relative phasing of the crankshafts The work presented here seeks to compare different means of on performance and economy.
    [Show full text]
  • ENRESO WORLD - Ilab
    ENRESO WORLD - ILab Different Car Engine Types Istas René Graduated in Automotive Technologies 1-1-2019 1 4 - STROKE ENGINE A four-stroke (also four-cycle) engine is an internal combustion (IC) engine in which the piston completes four separate strokes while turning the crankshaft. A stroke refers to the full travel of the piston along the cylinder, in either direction. The four separate strokes are termed: 1. Intake: Also known as induction or suction. This stroke of the piston begins at top dead center (T.D.C.) and ends at bottom dead center (B.D.C.). In this stroke the intake valve must be in the open position while the piston pulls an air-fuel mixture into the cylinder by producing vacuum pressure into the cylinder through its downward motion. The piston is moving down as air is being sucked in by the downward motion against the piston. 2. Compression: This stroke begins at B.D.C, or just at the end of the suction stroke, and ends at T.D.C. In this stroke the piston compresses the air-fuel mixture in preparation for ignition during the power stroke (below). Both the intake and exhaust valves are closed during this stage. 3. Combustion: Also known as power or ignition. This is the start of the second revolution of the four stroke cycle. At this point the crankshaft has completed a full 360 degree revolution. While the piston is at T.D.C. (the end of the compression stroke) the compressed air-fuel mixture is ignited by a spark plug (in a gasoline engine) or by heat generated by high compression (diesel engines), forcefully returning the piston to B.D.C.
    [Show full text]
  • Constant Volume Combustion: the Ultimate Gas Turbine Cycle
    INFRASTRUCTURE MINING & METALS NUCLEAR, SECURITY & ENVIRONMENTAL OIL, GAS & CHEMICALS Constant volume combustion: the ultimate gas turbine cycle About Bechtel Bechtel is among the most respected engineering, project management, and construction companies in the world. We stand apart for our ability to get the job done right—no matter how big, how complex, or how remote. Bechtel operates through four global business units that specialize in infrastructure; mining and metals; nuclear, security and environmental; and oil, gas, and chemicals. Since its founding in 1898, Bechtel has worked on more than 25,000 projects in 160 countries on all seven continents. Today, our 58,000 colleagues team with customers, partners, and suppliers on diverse projects in nearly 40 countries. Guest Feature Also in this section Constant volume combustion: 00 DARPA-funded CVC projects the ultimate gas turbine cycle 00 Power cycle thermodynamics 00 History of CVC engineering By S. C. Gülen, PhD, PE; Principal Engineer, Bechtel Power Pulse detonation combustion holds the key to 45% simple cycle and close to 65% combined cycle efficiencies at today’s 1400-1500°C gas turbine firing temperatures. The Kelvin-Planck statement of the Second Law of Thermo- Why constant volume combustion? dynamics leaves no room for doubt: the maximum efficiency In a modern gas turbine with an approximately constant pres- of a heat engine operating in a thermodynamic cycle cannot sure combustor, the compressor section consumes close to exceed the efficiency of a Carnot cycle operating between 50% of gas turbine power output. the same hot and cold temperature reservoirs. Assume one could devise a combustion system where All practical heat engine cycles are attempts to approxi- energy added to the working fluid (i.e.
    [Show full text]
  • N O T I C E This Document Has Been Reproduced From
    N O T I C E THIS DOCUMENT HAS BEEN REPRODUCED FROM MICROFICHE. ALTHOUGH IT IS RECOGNIZED THAT CERTAIN PORTIONS ARE ILLEGIBLE, IT IS BEING RELEASED IN THE INTEREST OF MAKING AVAILABLE AS MUCH INFORMATION AS POSSIBLE CONTRACTORS REPORT NO. 995 NASA CR•165,170 LIGHTWEIGHT DIESEL ENGINE DESIGNS FOR COMMUTER TYPE AIRCRAFT (NASA-C8-165470) LIG BINEIGHT DIESEL ENGINE DiS1VNS FOR C ONMUTEi T y kE N82-11066 Coatiuenta^ AIRCRAFT (TelEdyne 10t0rs, nuskeyon, Micu^) 7U P hC: A04/&F A01 CSCL 21c Uncla., G3/J7 u8165 Alex P. Brouwers Teledyne Continental Motors General Products Division 76 Getty Street Muskegon, Michigan 49442 JULY 1981 ^^ NGV1S81 RECEIVED NASA Sn FACSftx Acm 01 PREPARED FOR: AMM NATIONAL AERONAUTICS AND SPACE ADMINISTRATION LEWIS RESEARCH CENTER 21000 BROOKPARK ROAD CLEVELAND, OHIO 44135 CONTRACT NAS3.22149 CONTRACTORS REPORT NO. 995 NASA CR•165470 LIGHTWEIGHT DIESEL ENGINE DESIGNS FOR COMMUTER TYPE AIRCRAFT Alex P. Bromers Teledyne Continental Motors General Products Division 76 Getty Street Muskegon, Michigan 49442 JULY 1981 PREPARED FOR: NATIONAL AERONAUTICS AND SPACE ADMINISTRATION LEWIS RESEARCH CENTER 21000 BROOKPARK ROAD CLEVELAND, OHIO 44135 CONTRACT NAS3.22149 .xTELEDYNE C *ff1NEN1AL Mc7 M. General Products Wslon 4244J7-81 U, TABLE OF CONTENTS Papa No. 1.0 Summary ................................................................1 2.0 Introduction .............................................................3 2.1 Purpose of the Study ..................................................3 2.2 Previous Large Aircraft Diesel Engines
    [Show full text]
  • Aircraft Propulsion C Fayette Taylor
    SMITHSONIAN ANNALS OF FLIGHT AIRCRAFT PROPULSION C FAYETTE TAYLOR %L~^» ^ 0 *.». "itfnm^t.P *7 "•SI if' 9 #s$j?M | _•*• *• r " 12 H' .—• K- ZZZT "^ '! « 1 OOKfc —•II • • ~ Ifrfil K. • ««• ••arTT ' ,^IfimmP\ IS T A Review of the Evolution of Aircraft Piston Engines Volume 1, Number 4 (End of Volume) NATIONAL AIR AND SPACE MUSEUM 0/\ SMITHSONIAN INSTITUTION SMITHSONIAN INSTITUTION NATIONAL AIR AND SPACE MUSEUM SMITHSONIAN ANNALS OF FLIGHT VOLUME 1 . NUMBER 4 . (END OF VOLUME) AIRCRAFT PROPULSION A Review of the Evolution 0£ Aircraft Piston Engines C. FAYETTE TAYLOR Professor of Automotive Engineering Emeritus Massachusetts Institute of Technology SMITHSONIAN INSTITUTION PRESS CITY OF WASHINGTON • 1971 Smithsonian Annals of Flight Numbers 1-4 constitute volume one of Smithsonian Annals of Flight. Subsequent numbers will not bear a volume designation, which has been dropped. The following earlier numbers of Smithsonian Annals of Flight are available from the Superintendent of Documents as indicated below: 1. The First Nonstop Coast-to-Coast Flight and the Historic T-2 Airplane, by Louis S. Casey, 1964. 90 pages, 43 figures, appendix, bibliography. Price 60ff. 2. The First Airplane Diesel Engine: Packard Model DR-980 of 1928, by Robert B. Meyer. 1964. 48 pages, 37 figures, appendix, bibliography. Price 60^. 3. The Liberty Engine 1918-1942, by Philip S. Dickey. 1968. 110 pages, 20 figures, appendix, bibliography. Price 75jf. The following numbers are in press: 5. The Wright Brothers Engines and Their Design, by Leonard S. Hobbs. 6. Langley's Aero Engine of 1903, by Robert B. Meyer. 7. The Curtiss D-12 Aero Engine, by Hugo Byttebier.
    [Show full text]