ME6604 Gas Dynamics and Jet Propulsion
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Fluid Mechanics
cen72367_fm.qxd 11/23/04 11:22 AM Page i FLUID MECHANICS FUNDAMENTALS AND APPLICATIONS cen72367_fm.qxd 11/23/04 11:22 AM Page ii McGRAW-HILL SERIES IN MECHANICAL ENGINEERING Alciatore and Histand: Introduction to Mechatronics and Measurement Systems Anderson: Computational Fluid Dynamics: The Basics with Applications Anderson: Fundamentals of Aerodynamics Anderson: Introduction to Flight Anderson: Modern Compressible Flow Barber: Intermediate Mechanics of Materials Beer/Johnston: Vector Mechanics for Engineers Beer/Johnston/DeWolf: Mechanics of Materials Borman and Ragland: Combustion Engineering Budynas: Advanced Strength and Applied Stress Analysis Çengel and Boles: Thermodynamics: An Engineering Approach Çengel and Cimbala: Fluid Mechanics: Fundamentals and Applications Çengel and Turner: Fundamentals of Thermal-Fluid Sciences Çengel: Heat Transfer: A Practical Approach Crespo da Silva: Intermediate Dynamics Dieter: Engineering Design: A Materials & Processing Approach Dieter: Mechanical Metallurgy Doebelin: Measurement Systems: Application & Design Dunn: Measurement & Data Analysis for Engineering & Science EDS, Inc.: I-DEAS Student Guide Hamrock/Jacobson/Schmid: Fundamentals of Machine Elements Henkel and Pense: Structure and Properties of Engineering Material Heywood: Internal Combustion Engine Fundamentals Holman: Experimental Methods for Engineers Holman: Heat Transfer Hsu: MEMS & Microsystems: Manufacture & Design Hutton: Fundamentals of Finite Element Analysis Kays/Crawford/Weigand: Convective Heat and Mass Transfer Kelly: Fundamentals -
Introduction to Gas Dynamics All Lecture Slides
Introduction to Gas Dynamics AERODYNAMICS - II All Lecture Slides N. Venkata Raghavendra Farheen Sana Autumn 2009 Gasdynamics — Lecture Slides 1 Compressible flow 2 Zeroth law of thermodynamics 3 First law of thermodynamics 4 Equation of state — ideal gas 5 Specific heats 6 The “perfect” gas 7 Second law of thermodynamics 8 Adiabatic, reversible process 9 The free energy and free enthalpy 10 Entropy and real gas flows 11 One-dimensional gas dynamics 12 Conservation of mass — continuity equation 13 Conservation of energy — energy equation 14 Reservoir conditions 15 On isentropic flows Gasdynamics — Lecture Slides 16 Euler’s equation 17 Momentum equation 18 A review of equations of conservation 19 Isentropic condition 20 Speed of sound — Mach number 21 Results from the energy equation 22 The area-velocity relationship 23 On the equations of state 24 Bernoulli equation — dynamic pressure 25 Constant area flows 26 Shock relations for perfect gas — Part I 27 Shock relations for perfect gas — Part II 28 Shock relations for perfect gas — Part III 29 The area-velocity relationship — revisited 30 Nozzle flow — converging nozzle Gasdynamics — Lecture Slides 31 Nozzle flow — converging-diverging nozzle 32 Normal shock recovery — diffuser 33 Flow with wall roughness — Fanno flow 34 Flow with heat addition — Rayleigh flow 35 Normal shock, Fanno flow and Rayleigh flow 36 Waves in supersonic flow 37 Multi-dimensional equations of the flow 38 Oblique shocks 39 Relationship between wedge angle and wave angle 40 Small angle approximation 41 Mach lines 42 Weak oblique -
Chapter Sixteen / Plug, Underexpanded and Overexpanded Supersonic Nozzles ------Chapter Sixteen / Plug, Underexpanded and Overexpanded Supersonic Nozzles
UOT Mechanical Department / Aeronautical Branch Gas Dynamics Chapter Sixteen / Plug, Underexpanded and Overexpanded Supersonic Nozzles -------------------------------------------------------------------------------------------------------------------------------------------- Chapter Sixteen / Plug, Underexpanded and Overexpanded Supersonic Nozzles 16.1 Exit Flow for Underexpanded and Overexpanded Supersonic Nozzles The variation in flow patterns inside the nozzle obtained by changing the back pressure, with a constant reservoir pressure, was discussed early. It was shown that, over a certain range of back pressures, the flow was unable to adjust to the prescribed back pressure inside the nozzle, but rather adjusted externally in the form of compression waves or expansion waves. We can now discuss in detail the wave pattern occurring at the exit of an underexpanded or overexpanded nozzle. Consider first, flow at the exit plane of an underexpanded, two-dimensional nozzle (see Figure 16.1). Since the expansion inside the nozzle was insufficient to reach the back pressure, expansion fans form at the nozzle exit plane. As is shown in Figure (16.1), flow at the exit plane is assumed to be uniform and parallel, with . For this case, from symmetry, there can be no flow across the centerline of the jet. Thus the boundary conditions along the centerline are the same as those at a plane wall in nonviscous flow, and the normal velocity component must be equal to zero. The pressure is reduced to the prescribed value of back pressure in region 2 by the expansion fans. However, the flow in region 2 is turned away from the exhaust-jet centerline. To maintain the zero normal-velocity components along the centerline, the flow must be turned back toward the horizontal. -
Normal and Oblique Shocks, Prandtl Meyer Expansion
Aerothermodynamics of high speed flows AERO 0033{1 Lecture 3: Normal and oblique shocks, Prandtl Meyer expansion Thierry Magin, Greg Dimitriadis, and Adrien Crovato [email protected] Aeronautics and Aerospace Department von Karman Institute for Fluid Dynamics Aerospace and Mechanical Engineering Department Faculty of Applied Sciences, University of Li`ege Wednesday 9am { 12:15pm February { May 2021 1 / 36 Outline Normal shock Total and critical quantities Oblique shock Prandtl-Meyer expansion Shock reflection and shock interaction 2 / 36 Outline Normal shock Total and critical quantities Oblique shock Prandtl-Meyer expansion Shock reflection and shock interaction 2 / 36 Normal shock relations (inviscid flow) Rankine-Hugoniot relations for steady normal shock σ = 0; v = u ex ; n = ex ! σn(U2 − U1) = (F · n)2 − (F · n)1 ρ2u2 = ρ1u1 2 2 ρ2u2 + p2 = ρ1u1 + p1 ρ2u2H2 = ρ1u1H1 I Eqs. also valid for non calorically perfect gases I Contact discontinuity when u2 = u1 = 0 ! p2 = p1 I Otherwise, the total enthalpy conservation can be expressed as 2 2 2 u cp p γ p2 u2 γ p1 u1 H2 = H1 with H = h+ ; h = ! + = + 2 R ρ γ − 1 ρ2 2 γ − 1 ρ1 2 I Non-linear algebraic system of 3 eqs. in 3 unknowns ρ2, u2, and p2 with closed solution expressed in function of dimensionless parameters: Machp number M1 = u1=a1 and specific heat ratio γ, with a1 = γRT1 3 / 36 Normal shock relations for calorically perfect gases For M1 > 1 (derivation given further in this section) 2 ρ2 u1 (γ+1)M1 I ρ = u = 2 > 1 1 2 2+(γ−1)M1 p2 = 1 + 2γ (M2 − 1) > 1 I p1 γ+1 1 γ−1 2 2 1+ 2 -
Introduction
CHAPTER 1 Introduction "For some years I have been afflicted with the belief that flight is possible to man." Wilbur Wright, May 13, 1900 1.1 ATMOSPHERIC FLIGHT MECHANICS Atmospheric flight mechanics is a broad heading that encompasses three major disciplines; namely, performance, flight dynamics, and aeroelasticity. In the past each of these subjects was treated independently of the others. However, because of the structural flexibility of modern airplanes, the interplay among the disciplines no longer can be ignored. For example, if the flight loads cause significant structural deformation of the aircraft, one can expect changes in the airplane's aerodynamic and stability characteristics that will influence its performance and dynamic behavior. Airplane performance deals with the determination of performance character- istics such as range, endurance, rate of climb, and takeoff and landing distance as well as flight path optimization. To evaluate these performance characteristics, one normally treats the airplane as a point mass acted on by gravity, lift, drag, and thrust. The accuracy of the performance calculations depends on how accurately the lift, drag, and thrust can be determined. Flight dynamics is concerned with the motion of an airplane due to internally or externally generated disturbances. We particularly are interested in the vehicle's stability and control capabilities. To describe adequately the rigid-body motion of an airplane one needs to consider the complete equations of motion with six degrees of freedom. Again, this will require accurate estimates of the aerodynamic forces and moments acting on the airplane. The final subject included under the heading of atmospheric flight mechanics is aeroelasticity. -
Nozzle Aerodynamics Baseline Design
Preliminary Design Review Supersonic Air-Breathing Redesigned Engine Nozzle Customer: Air Force Research Lab Advisor: Brian Argrow Team Members: Corrina Briggs, Jared Cuteri, Tucker Emmett, Alexander Muller, Jack Oblack, Andrew Quinn, Andrew Sanchez, Grant Vincent, Nathaniel Voth Project Description Model, manufacture, and verify an integrated nozzle capable of accelerating subsonic exhaust to supersonic exhaust produced from a P90-RXi JetCat engine for increased thrust and efficiency from its stock configuration. Stock Nozzle Vs. Supersonic Nozzle Inlet Compressor Combustor Turbine Project Baseline Nozzle Nozzle Test Nozzle Project Description Design Aerodynamics Bed Integration Summary Objectives/Requirements •FR 1: The Nozzle Shall accelerate the flow from subsonic to supersonic conditions. •FR 2: The Nozzle shall not decrease the Thrust-to-Weight Ratio. •FR 3: The Nozzle shall be designed and manufactured such that it will integrate with the JetCat Engine. •DR 3.1: The Nozzle shall be manufactured using additive manufacturing. •DR 3.4: Successful integration of the nozzle shall be reversible such that the engine is operable in its stock configuration after the new nozzle has been attached, tested, and detached. •FR4: The Nozzle shall be able to withstand engine operation for at least 30 seconds. Project Baseline Nozzle Nozzle Test Nozzle Project Description Design Aerodynamics Bed Integration Summary Concept of Operations JetCat P90-SE Subsonic Supersonic Engine Flow Flow 1. Remove Stock Nozzle 2. Additive Manufactured 3-D Nozzle -
Gas Dynamics and Jet Propulsion
A Course Material on GAS DYNAMICS AND JET PROPULSION By Mr. C.RAVINDIRAN. ASSISTANT PROFESSOR DEPARTMENT OF MECHANICAL ENGINEERING SASURIE COLLEGE OF ENGINEERING VIJAYAMANGALAM – 638 056 QUALITY CERTIFICATE This is to certify that the e-course material Subject Code : ME2351 Subject : GAS DYNAMICS AND JET PROPULSION Class : III Year MECHANICAL ENGINEERING being prepared by me and it meets the knowledge requirement of the university curriculum. Signature of the Author Name : C. Ravindiran Designation: Assistant Professor This is to certify that the course material being prepared by Mr. C. Ravindiran is of adequate quality. He has referred more than five books amount them minimum one is from abroad author. Signature of HD Name: Mr. E.R.Sivakumar SEAL CONTENTS S.NO TOPIC PAGE NO UNIT-1 BASIC CONCEPTS AND ISENTROPIC 1.1 Concept of Gas Dynamics 1 1.1.1 Significance with Applications 1 1.2 Compressible Flows 1 1.2.1 Compressible vs. Incompressible Flow 2 1.2.2 Compressibility 2 1.2.3. Compressibility and Incompressibility 3 1.3 Steady Flow Energy Equation 5 1.4 Momentum Principle for a Control Volume 5 1.5 Stagnation Enthalpy 5 1.6 Stagnation Temperature 7 1.7 Stagnation Pressure 8 1.8 Stagnation velocity of sound 9 1.9 Various regions of flow 9 1.10 Flow Regime Classification 11 1.11 Reference Velocities 12 1.11.1 Maximum velocity of fluid 12 1.11.2 Critical velocity of sound 13 1.12 Mach number 16 1.13 Mach Cone 16 1.14 Reference Mach number 16 1.15 Crocco number 19 1.16 Isothermal Flow 19 1.17 Law of conservation of momentum 19 1.17.1 Assumptions -
Surface Pressure Fluctuations Near an Axisymmetric Stagnation Point
KM m Vk I •/•*.*.•* .^ >.,*.' . i • I H H '**<J2 MITED STATES \RTMENT OF 1MERCE NBS TECHNICAL NOTE 563 JUCATION If"' Surface Pressure Fluctuations Near an Axisymmetric Stagnation Point U.S. VRTMENT OF MMERCE National Bureau of -. ndards Lz UI — NATIONAL BUREAU OF STANDARDS 1 The National Bureau of Standards was established by an act of Congress March 3, 1901. The Bureau's overall goal is to strengthen and advance the Nation's science and technology and facilitate their effective application for public benefit. To this end, the Bureau conducts research and provides: (1) a basis for the Nation's physical measure- ment system, (2) scientific and technological services for industry and government, (3) a technical basis for equity in trade, and (4) technical services to promote public safety. The Bureau consists of the Institute for Basic Standards, the Institute for Materials Research, the Institute for Applied Technology, the Center for Computer Sciences and Technology, and the Office for Information Programs. THE INSTITUTE FOR BASIC STANDARDS provides the central basis within the United States of a complete and consistent system of physical measurement; coordinates that system with measurement systems of other nations; and furnishes essential services leading to accurate and uniform physical measurements throughout the Nation's scien- tific community, industry, and commerce. The Institute consists of a Center for Radia- tion Research, an Office of Measurement Services and the following divisions: Applied Mathematics—Electricity—Heat—Mechanics—Optical Physics—Linac Radiation2—Nuclear Radiation 2—Applied Radiation 2—Quantum Electronics 3— Electromagnetics 3—Time and Frequency 3—Laboratory Astrophysics 3—Cryo- 3 genics . -
Model-Based Stagnation Pressure Control in a Supersonic Wind Tunnel
Model-Based Stagnation Pressure Control in a Supersonic Wind Tunnel Biljana Ilić Lead Research Engineer The flow parameters control in wind tunnels is an area of intense research Experimental Aerodynamics Department in recent years, with the aim of improving quality and efficiency of the Military Technical Institute Belgrade wind tunnel operation. In this paper, an attempt is made to contribute to a Marko Miloš better understanding of the stagnation pressure control in supersonic Professor blowdown-type facilities. The stagnation pressure control strategy in the University of Belgrade VTI Belgrade T-38 wind tunnel is discussed. An improved mathematical Faculty of Mechanical Engineering model for a supersonic wind tunnel is suggested and applied to the T-38 Mirko Milosavljević facility. Comparisons of simulation and experimental data are made to Lead Research Engineer demonstrate accurate prediction of the facility response in supersonic flow Experimental Aerodynamics Department conditions by the mathematical model. The model is used to incorporate a Military Technical Institute Belgrade modified feedforward control in the original T-38 wind tunnel control Jovan Isaković system. The actual wind tunnel tests confirm model-predicted decrease of flow stabilization time and increase of available measurement time, Professor Tehnikum Taurunum - College of Applied bringing significant improvement in the wind tunnel operation efficiency. Engineering Studies Belgrade Keywords: supersonic flow, mathematical model, blowdown wind tunnel, stagnation -
Copyrighted Material
BBMIndx.inddMIndx.indd PPageage I-1I-1 111/10/181/10/18 6:536:53 PMPM f-389f-389 //208/WB02304_EVALCS/9781119469582/bmmatter/text_s208/WB02304_EVALCS/9781119469582/bmmatter/text_s Index Absolute pressure, 13, 41 Angular momentum flow, 174, video V5.12 restrictions on use of, 106–110, 222, Absolute temperature Annulus, flow in, 257–258 video V3.12 in British Gravitational (BG) System, 7 Apparent viscosity, 16 unsteady flow, 107–108 in English Engineering (EE) System, 8 Aqueducts, 454 use of, video V3.2 in ideal gas law, 12 Archimedes, 27, 28, 62 Best efficiency points, 564 in International System (SI), 7 Archimedes’ principle, 61–64, video V2.7 Best hydraulic cross section, 460–461 Absolute velocity Area BG units. see British Gravitational (BG) System in centrifugal pumps, 558–561 centroid, 51–53 of units defined, 154, 551 compressible flow with change in, 507–522 Bingham plastic, 16–17 in rotating sprinkler example, 176–177 isentropic flow of ideal gas with change in, Birds, wings of, 429 in turbo machine example, 551–554 510–516 Blades vs. relative velocity, 141–142 and Mach number, 511–513 curved and radia, 561, 562 Absolute viscosity moment of inertia, 52 radial, 561 of air, 620–621 Aspect ratio rotor, 575, 591 of common gases, 617 air foil, 435 stator, 575, 591 of common liquids, 617 plate, 271 turbo machine, 549 defined, 15 Assemblies, 603 Blade velocity, 551–554, 558–559 of U.S. Standard Atmosphere, 622–623 Atmosphere, standard. see Standard Blasius, H., 29, 285, 389 of water, 619 atmosphere Blasius formula, 285, 339 Acceleration -
Cold Flow Performance of a Ramjet Engine
COLD FLOW PERFORMANCE OF A RAMJET ENGINE A Thesis Presented to the Faculty of California Polytechnic State University San Luis Obispo In Partial Fulfillment of the Requirements for the Degree Master of Science in Aerospace Engineering by Harrison G. Sykes December 2014 ©2014 Harrison G. Sykes ALL RIGHTS RESERVED ii COMMITTEE MEMBERSHIP TITLE: Cold Flow Performance of a Ramjet Engine AUTHOR: Harrison G. Sykes DATE SUBMITTED: December 2014 COMMITTEE CHAIR: Eric Mehiel, Ph.D. Associate Professor Aerospace Engineering Department COMMITTEE MEMBER: Patrick Lemieux, Ph.D. Associate Professor, Mechanical Engineering Department COMMITTEE MEMBER: Daniel J. Wait, M.S. Systems Engineer, Tyvak Nano-Satelite Systems LLC iii ABSTRACT Cold Flow Performance of a Ramjet Engine Harrison G. Sykes The design process and construction of the initial modular ramjet attachment to the Cal Poly supersonic wind tunnel is presented. The design of a modular inlet, combustor, and nozzle are studied in depth with the intentions of testing in the modular ramjet. The efforts undertaken to characterize the Cal Poly supersonic wind tunnel and the individual component testing of this attachment are also discussed. The data gathered will be used as a base model for future expansion of the ramjet facility and eventual hot fire testing of the initial components. Modularity of the inlet, combustion chamber, and nozzle will allow for easier modification of the initial design and the designs ability to incorporate clear walls will allow for flow and combustion visualization once the performance of the hot flow ramjet is determined. The testing of the blank ramjet duct resulted in an error of less than 10% from predicted results. -
2006-709: a Web-Based Solver for Compressible Flow Calculations
2006-709: A WEB-BASED SOLVER FOR COMPRESSIBLE FLOW CALCULATIONS Harish Eletem, Lamar University HARISH ELETEM was a graduate student in the Department of Mechanical Engineering at Lamar University. He received his M.S. degree in Mechanical Engineering from Lamar University in 2005. Fred Young, Lamar University FRED YOUNG is a professor in the Department of Mechanical Engineering at Lamar University. He received his Ph.D. degree in Mechanical Engineering from Southern Methodist University. He has published many technical papers and presented several papers at international conferences. Kendrick Aung, Lamar University KENDRICK AUNG is an associate professor in the Department of Mechanical Engineering at Lamar University. He received his Ph.D. degree in Aerospace Engineering from University of Michigan in 1996. He is an active member of ASEE, ASME, AIAA and Combustion Institute. He has published over 50 technical papers and presented several papers at national and international conferences. Page 11.144.1 Page © American Society for Engineering Education, 2006 A Web-based Solver for Compressible Flow Calculations Abstract Compressible flow is an important subject in aerospace and mechanical engineering disciplines. This paper describes a web-base solver for carrying out compressible flow calculations. The main objective of the solver is to provide students with a software tool than can be used in the compressible flow course offered in the Department of Mechanical Engineering at Lamar University. The solver has a graphical user interface (GUI) for ease of use and interactivity. The solver is capable of solving typical compressible flows such as isentropic flows, Rayleigh and Fanno flows, normal and oblique shock flows, and Prandtl-Myer expansion waves.