Mach Number, Relative Thickness, Sweep and Lift Coefficient of the Wing - an Empirical Investigation of Parameters and Equations

Total Page:16

File Type:pdf, Size:1020Kb

Mach Number, Relative Thickness, Sweep and Lift Coefficient of the Wing - an Empirical Investigation of Parameters and Equations Project Department of Automotive and Aeronautical Engineering Mach number, relative thickness, sweep and lift coefficient of the wing - An empirical investigation of parameters and equations Author: Simona Ciornei Examiner: Prof. Dr.-Ing. Dieter Scholz, MSME Delivered: 31.05.2005 2 Abstract 12 equations were investigated to calculate the relative thickness t/c of the wing of an aircraft. The calculated relative thickness was taken as the average relative thickness of the wing. The data obtained from these 12 equations was checked against the given average relative thickness of 29 carefully selected aircraft, spanning a space of the parameters Mach number, lift coefficient, sweep, and type of airfoil. Some equations selected are empirical in their nature (partly based on aerodynamic derivation) other equations are purely statistical. Whenever equations had free parameters, these were optimized against the aircraft data. The best equation turned out to be an equation based on nonlinear regression. It achieved a Standard Error of Estimate of only 0.75 % for the average relative thickness of the wing. Torenbeek’s equation will probably be preferred by those that like to see an equation that is based on aerodynamic considerations. It achieved a Standard Error of Estimate of 0.80 % when all its free parameters were considered for optimization. The worst equation produced an Standard Error of Estimate of 8 %. For an airfoil with 10 % relative thickness this would give an unacceptable 10 % +/- 8 % band of values for t/c which renders equations like this quite useless. 1 FACHBEREICH FAHRZEUGTECHNIK UND FLUGZEUGBAU Mach number, relative thickness, sweep and lift coefficient of the wing - an empirical investigation of parameters and equations Aufgabenstellung zum Projekt gemäß Prüfungsordnung Background In aircraft design, the wing parameters "relative thickness" and "sweep" follow from a demand for a certain cruise Mach number at low wave drag. In addition, the cruise lift coefficient and the type of airfoil have an influence on the aerodynamics of the wing. If there is a demand for a higher cruise Mach number during aircraft design, the sweep has to be increased or the rela- tive thickness has to be decreased. The transonic flow around a wing can not be described with simple equations. For this reason, the relationship between the parameters as given above will be based in preliminary aircraft design on statistics of known aircrafts. Task Equations based on statistical data relating Mach number, relative thickness, sweep and lift coefficient of the wing have to be investigated, checked and improved for their suitability in preliminary aircraft design. The project's task includes these subtasks: • Introduction to transonic flow around wings. • Literature search for equations dealing with the relationship of named parameters. • Theoretical substantiation of the empirical equations as far as possible. • Investigation of aircraft parameters for sample calculations with equations form the litera- ture. • Comparison of equations based on sample calculations. Selection of the most suitable equation. • Adaptation of this equation to further improve the accuracy based on given aircraft pa- rameters. The report has to be written according to German DIN standards on report writing! 4 Table of Contents page List of Figures ........................................................................................................................... 8 List of Tables .......................................................................................................................... 10 List of Symbols ....................................................................................................................... 11 List of Key Words and Definitions ......................................................................................... 13 1 Introduction ........................................................................................................ 15 1.1 Motivation ............................................................................................................ 15 1.2 Definitions ............................................................................................................ 15 1.3 Task ...................................................................................................................... 18 1.4 Literature .............................................................................................................. 19 1.5 Structure of Work ................................................................................................ 19 2 Transonic Flow ................................................................................................... 21 2.1 Transonic Flow Phenomena ................................................................................. 21 2.2 Compressibility Corrections ................................................................................ 23 2.3 Critical Mach Number and Critical Pressure Coefficient .................................... 24 2.4 Drag –Divergence Mach Number ........................................................................ 28 2.5 Development of the Supercritical Airfoil ............................................................. 31 2.6. Swept Wings ........................................................................................................ 34 2.7 Relative Thickness ............................................................................................... 37 3 Equations for the Calculation of Relative Thickness ..................................... 38 3.1 Equation based on Torenbeek .............................................................................. 38 3.2 Equations from Aerodynamic Similarity based on Anderson .............................. 40 3.3 Equation based on Shevell ................................................................................... 41 3.4 Equation based on Kroo ....................................................................................... 44 3.5 Equation from Howe ............................................................................................ 47 3.6 Equation from Jenkinson ..................................................................................... 48 3.7 Equation from Weisshaar ..................................................................................... 49 3.8 Equation based on Böttger ................................................................................... 50 3.9 Equation based on Raymer ................................................................................... 54 3.10 Equation based on Linear Regression .................................................................. 59 3.11 Equation based on Nonlinear Regression ............................................................ 60 3.12 Substantiation of the Equation from Torenbeek .................................................. 61 4 Investigation Comparison and Adaptation of Equations ............................... 65 4.1 Input from Aircraft Data ...................................................................................... 65 4.2 Calculation, Optimization and Results ................................................................ 66 5 5 Conclusions ......................................................................................................... 70 6 Recommendations ............................................................................................... 71 List of References................................................................................................................... 72 Appendix A Three-View Drawings .................................................................................... 77 Appendix B Investigation of Aircraft Parameters from Different Sources ................. 107 Appendix C Summary of Aircraft Parameters .............................................................. 137 Appendix D Calculation of Relative Thickness / Optimization of Equations ............. 142 Appendix E Schaufele’s Method .......................................................................................151 6 List of Figures Figure 1.1 Definition of sweep angles on a tapered inner and outer wing .........................17 Figure 2.1 Physical mechanism of drag divergence ...........................................................22 Figure 2.2 Variation of (a) lift coefficient and (b) drag coefficient versus Mach number with angle of attack as a parameter for an NACA 2315 airfoil............22 Figure 2.3 Several compressibility corrections compared with experimental results for an NACA 4412 airfoil at an angle of attack α = 1°53’ ...............................24 Figure 2.4 Illustration of critical Mach number..................................................................25 Figure 2.5 Illustration of critical pressure coefficient.........................................................26 Figure 2.6 Critical pressure coefficient and critical Mach numbers for airfoils of different thickness.........................................................................................26 Figure 2.7 Sketch of the variation of profile drag coefficient with freestream Mach number, illustrating the critical and drag-divergence Mach number and showing the large drag rise near Mach 1.............................29 Figure 2.8 Definition of critical Mach number...................................................................30 Figure 2.9 Peaky
Recommended publications
  • Aerodynamics Material - Taylor & Francis
    CopyrightAerodynamics material - Taylor & Francis ______________________________________________________________________ 257 Aerodynamics Symbol List Symbol Definition Units a speed of sound ⁄ a speed of sound at sea level ⁄ A area aspect ratio ‐‐‐‐‐‐‐‐ b wing span c chord length c Copyrightmean aerodynamic material chord- Taylor & Francis specific heat at constant pressure of air · root chord tip chord specific heat at constant volume of air · / quarter chord total drag coefficient ‐‐‐‐‐‐‐‐ , induced drag coefficient ‐‐‐‐‐‐‐‐ , parasite drag coefficient ‐‐‐‐‐‐‐‐ , wave drag coefficient ‐‐‐‐‐‐‐‐ local skin friction coefficient ‐‐‐‐‐‐‐‐ lift coefficient ‐‐‐‐‐‐‐‐ , compressible lift coefficient ‐‐‐‐‐‐‐‐ compressible moment ‐‐‐‐‐‐‐‐ , coefficient , pitching moment coefficient ‐‐‐‐‐‐‐‐ , rolling moment coefficient ‐‐‐‐‐‐‐‐ , yawing moment coefficient ‐‐‐‐‐‐‐‐ ______________________________________________________________________ 258 Aerodynamics Aerodynamics Symbol List (cont.) Symbol Definition Units pressure coefficient ‐‐‐‐‐‐‐‐ compressible pressure ‐‐‐‐‐‐‐‐ , coefficient , critical pressure coefficient ‐‐‐‐‐‐‐‐ , supersonic pressure coefficient ‐‐‐‐‐‐‐‐ D total drag induced drag Copyright material - Taylor & Francis parasite drag e span efficiency factor ‐‐‐‐‐‐‐‐ L lift pitching moment · rolling moment · yawing moment · M mach number ‐‐‐‐‐‐‐‐ critical mach number ‐‐‐‐‐‐‐‐ free stream mach number ‐‐‐‐‐‐‐‐ P static pressure ⁄ total pressure ⁄ free stream pressure ⁄ q dynamic pressure ⁄ R
    [Show full text]
  • Concorde Is a Museum Piece, but the Allure of Speed Could Spell Success
    CIVIL SUPERSONIC Concorde is a museum piece, but the allure Aerion continues to be the most enduring player, of speed could spell success for one or more and the company’s AS2 design now has three of these projects. engines (originally two), the involvement of Air- bus and an agreement (loose and non-exclusive, by Nigel Moll but signed) with GE Aviation to explore the supply Fourteen years have passed since British Airways of those engines. Spike Aerospace expects to fly a and Air France retired their 13 Concordes, and for subsonic scale model of the design for the S-512 the first time in the history of human flight, air trav- Mach 1.5 business jet this summer, to explore low- elers have had to settle for flying more slowly than speed handling, followed by a manned two-thirds- they used to. But now, more so than at any time scale supersonic demonstrator “one-and-a-half to since Concorde’s thunderous Olympus afterburn- two years from now.” Boom Technology is working ing turbojets fell silent, there are multiple indi- on a 55-seat Mach 2.2 airliner that it plans also to cations of a supersonic revival, and the activity offer as a private SSBJ. NASA and Lockheed Martin appears to be more advanced in the field of busi- are encouraged by their research into reducing the ness jets than in the airliner sector. severity of sonic booms on the surface of the planet. www.ainonline.com © 2017 AIN Publications. All Rights Reserved. For Reprints go to Shaping the boom create what is called an N-wave sonic boom: if The sonic boom produced by a supersonic air- you plot the pressure distribution that you mea- craft has long shaped regulations that prohibit sure on the ground, it looks like the letter N.
    [Show full text]
  • 8. Level, Non-Accelerated Flight
    Performance 8. Level, Non-Accelerated Flight For non-accelerated flight, the tangential acceleration, , and normal acceleration, . As a result, the governing equations become: (1) If we add the additional assumptions of level flight, , and that the thrust is aligned with the velocity vector, , then Eq. (1) reduces to the simple form: (2) The last two equations tell us that the altitude is a constant, and the velocity is the range rate. For now, however, we are interested in the first two equations that can be rewritten as: (3) The key thing to remember about these equations is that the weight,W,isagivenand it is equal to the Lift. Consequently, lift is not at our disposal, it must equal the given weight! Thus for a given aircraft and any given altitude, we can determine the required lift coefficient (and hence angle-of-attack) for any given airspeed. (4) Therefore at a given weight and altitude, the lift coefficient varies as 1 over V2. A sketch of lift coefficient vs. speed looks as follows: 1 It is clear from the figure that as the vehicle slows down, in order to remain in level flight, the lift coefficient (and hence angle-of-attack) must increase. [You can think of it in terms of the momentum flux. The momentum flux (the mass flow rate time the velocity out in the z direction) creates the lift force. Since the mass flow rate is directional proportional to the velocity, then the slower we go, the more the air must be deflected downward. We do this by increasing the angle-of-attack!].
    [Show full text]
  • NASA Supercritical Airfoils
    NASA Technical Paper 2969 1990 NASA Supercritical Airfoils A Matrix of Family-Related Airfoils Charles D. Harris Langley Research Center Hampton, Virginia National Aeronautics-and Space Administration Office of Management Scientific and Technical Information Division Summary wind-tunnel testing. The process consisted of eval- A concerted effort within the National Aero- uating experimental pressure distributions at design and off-design conditions and physically altering the nautics and Space Administration (NASA) during airfoil profiles to yield the best drag characteristics the 1960's and 1970's was directed toward develop- over a range of experimental test conditions. ing practical two-dimensional turbulent airfoils with The insight gained and the design guidelines that good transonic behavior while retaining acceptable were recognized during these early phase 1 investiga- low-speed characteristics and focused on a concept tions, together with transonic, viscous, airfoil anal- referred to as the supercritical airfoil. This dis- ysis codes developed during the same time period, tinctive airfoil shape, based on the concept of local resulted in the design of a matrix of family-related supersonic flow with isentropic recompression, was supercritical airfoils (denoted by the SC(phase 2) characterized by a large leading-edge radius, reduced prefix). curvature over the middle region of the upper surface, and substantial aft camber. The purpose of this report is to summarize the This report summarizes the supercritical airfoil background of the NASA supercritical airfoil devel- development program in a chronological fashion, dis- opment, to discuss some of the airfoil design guide- lines, and to present coordinates of a matrix of cusses some of the design guidelines, and presents family-related supercritical airfoils with thicknesses coordinates of a matrix of family-related super- critical airfoils with thicknesses from 2 to 18 percent from 2 to 18 percent and design lift coefficients from and design lift coefficients from 0 to 1.0.
    [Show full text]
  • Critical Mach Number, Transonic Area Rule
    Critical Mach number - Compressibility Effects on Lift The design parameter that influences compressibility effects on lift is the Critical Mach number (Mcr). This is the free stream Mach number when sonic conditions (M = 1) is reached at some point on the airfoil surface The figure illustrates the same airfoil, at the same angle of attack at different free stream Mach numbers leading to the definition of the critical Mach number The critical Mach number can be obtained through the curve for the minimum pressure coefficient as a function of Mach number. It can be determined through the intersection of the two equations The lift coefficient correction for compressibility is The figure above illustrates that If you plan to fly at high free stream Mach number, you airfoil should be thin to (a) increase your critical Mach number as this will keep your drag rise small This will also result in lower minimum pressure: Therefore your lift coefficient will decrease Note that the minimum pressure coefficient on thick airfoil is high; this means that the velocity is also correspondingly high. Therefore the critical Mach number is reached for lower value of the free stream Mach number. Swept wing A B-52 Stratofortress showing wing with a large sweepback angle. A swept wing is a wing planform favored for high subsonic jet speeds first investigated in Germany from 1935 onwards until the end of the Second World War. Since the introduction of the MiG-15 and North American F-86 which demonstrated a decisive superiority over the slower first generation of straight-wing jet fighters during the Korean War, swept wings have become almost universal on all but the slowest jets (such as the A- 10).
    [Show full text]
  • 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.
    [Show full text]
  • No Acoustical Change” for Propeller-Driven Small Airplanes and Commuter Category Airplanes
    4/15/03 AC 36-4C Appendix 4 Appendix 4 EQUIVALENT PROCEDURES AND DEMONSTRATING "NO ACOUSTICAL CHANGE” FOR PROPELLER-DRIVEN SMALL AIRPLANES AND COMMUTER CATEGORY AIRPLANES 1. Equivalent Procedures Equivalent Procedures, as referred to in this AC, are aircraft measurement, flight test, analytical or evaluation methods that differ from the methods specified in the text of part 36 Appendices A and B, but yield essentially the same noise levels. Equivalent procedures must be approved by the FAA. Equivalent procedures provide some flexibility for the applicant in conducting noise certification, and may be approved for the convenience of an applicant in conducting measurements that are not strictly in accordance with the 14 CFR part 36 procedures, or when a departure from the specifics of part 36 is necessitated by field conditions. The FAA’s Office of Environment and Energy (AEE) must approve all new equivalent procedures. Subsequent use of previously approved equivalent procedures such as flight intercept typically do not need FAA approval. 2. Acoustical Changes An acoustical change in the type design of an airplane is defined in 14 CFR section 21.93(b) as any voluntary change in the type design of an airplane which may increase its noise level; note that a change in design that decreases its noise level is not an acoustical change in terms of the rule. This definition in section 21.93(b) differs from an earlier definition that applied to propeller-driven small airplanes certificated under 14 CFR part 36 Appendix F. In the earlier definition, acoustical changes were restricted to (i) any change or removal of a muffler or other component of an exhaust system designed for noise control, or (ii) any change to an engine or propeller installation which would increase maximum continuous power or propeller tip speed.
    [Show full text]
  • Experimental and Numerical Investigations of a 2D Aeroelastic Arifoil Encountering a Gust in Transonic Conditions Fabien Huvelin, Arnaud Lepage, Sylvie Dequand
    Experimental and numerical investigations of a 2D aeroelastic arifoil encountering a gust in transonic conditions Fabien Huvelin, Arnaud Lepage, Sylvie Dequand To cite this version: Fabien Huvelin, Arnaud Lepage, Sylvie Dequand. Experimental and numerical investigations of a 2D aeroelastic arifoil encountering a gust in transonic conditions. CEAS Aeronautical Journal, Springer, In press, 10.1007/s13272-018-00358-x. hal-02027968 HAL Id: hal-02027968 https://hal.archives-ouvertes.fr/hal-02027968 Submitted on 22 Feb 2019 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. 1 EXPERIMENTAL AND NUMERICAL INVESTIGATIONS OF A 2D 2 AEROELASTIC AIRFOIL ENCOUNTERING A GUST IN TRANSONIC 3 CONDITIONS 4 Fabien HUVELIN1, Arnaud LEPAGE, Sylvie DEQUAND 5 6 ONERA-The French Aerospace Lab 7 Aerodynamics, Aeroelasticity, Acoustics Department 8 Châtillon, 92320 FRANCE 9 10 KEYWORDS: Aeroelasticity, Wind Tunnel Test, CFD, Gust response, Unsteady coupled 11 simulations 12 ABSTRACT: 13 In order to make substantial progress in reducing the environmental impact of aircraft, a key 14 technology is the reduction of aircraft weight. This challenge requires the development and 15 the assessment of new technologies and methodologies of load prediction and control. To 16 achieve the investigation of the specific case of gust load, ONERA defined a dedicated 17 research program based on both wind tunnel test campaigns and high fidelity simulations.
    [Show full text]
  • Drag Bookkeeping
    Drag Drag Bookkeeping Drag may be divided into components in several ways: To highlight the change in drag with lift: Drag = Zero-Lift Drag + Lift-Dependent Drag + Compressibility Drag To emphasize the physical origins of the drag components: Drag = Skin Friction Drag + Viscous Pressure Drag + Inviscid (Vortex) Drag + Wave Drag The latter decomposition is stressed in these notes. There is sometimes some confusion in the terminology since several effects contribute to each of these terms. The definitions used here are as follows: Compressibility drag is the increment in drag associated with increases in Mach number from some reference condition. Generally, the reference condition is taken to be M = 0.5 since the effects of compressibility are known to be small here at typical conditions. Thus, compressibility drag contains a component at zero-lift and a lift-dependent component but includes only the increments due to Mach number (CL and Re are assumed to be constant.) Zero-lift drag is the drag at M=0.5 and CL = 0. It consists of several components, discussed on the following pages. These include viscous skin friction, vortex drag due to twist, added drag due to fuselage upsweep, control surface gaps, nacelle base drag, and miscellaneous items. The Lift-Dependent drag, sometimes called induced drag, includes the usual lift- dependent vortex drag together with lift-dependent components of skin friction and pressure drag. For the second method: Skin Friction drag arises from the shearing stresses at the surface of a body due to viscosity. It accounts for most of the drag of a transport aircraft in cruise.
    [Show full text]
  • CHAPTER 11 Subsonic and Supersonic Aircraft Emissions
    CHAPTER 11 Subsonic and Supersonic Aircraft Emissions Lead Authors: A. Wahner M.A. Geller Co-authors: F. Arnold W.H. Brune D.A. Cariolle A.R. Douglass C. Johnson D.H. Lister J.A. Pyle R. Ramaroson D. Rind F. Rohrer U. Schumann A.M. Thompson CHAPTER 11 SUBSONIC AND SUPERSONIC AIRCRAFT EMISSIONS Contents SCIENTIFIC SUMMARY ......................................................................................................................................... 11.1 11.1 INTRODUCTION ............................................................................................................................................ 11.3 11.2 AIRCRAFT EMISSIONS ................................................................................................................................. 11.4 11.2.1 Subsonic Aircraft .................................................................................................................................. 11.5 11.2.2 Supersonic Aircraft ............................................................................................................................... 11.6 11.2.3 Military Aircraft .................................................................................................................................... 11.6 11.2.4 Emissions at Altitude ............................................................................................................................ 11.6 11.2.5 Scenarios and Emissions Data Bases ...................................................................................................
    [Show full text]
  • Aerospace Facts and Figures 1983/84
    Aerospace Facts and Figures 1983/84 AEROSPACE INDUSTRIES ASSOCIATION OF AMERICA, INC. 1725 DeSales Street, N.W., Washington, D.C. 20036 Published by Aviation Week & Space Technology A MCGRAW-HILL PUBLICATION 1221 Avenue of the Americas New York, N.Y. 10020 (212) 997-3289 $9.95 Per Copy Copyright, July 1983 by Aerospace Industries Association o' \merica, Inc. · Library of Congress Catalog No. 46-25007 2 Compiled by Economic Data Service Aerospace Research Center Aerospace Industries Association of America, Inc. 1725 DeSales Street, N.W., Washington, D.C. 20036 (202) 429-4600 Director Research Center Virginia C. Lopez Manager Economic Data Service Janet Martinusen Editorial Consultant James J. Haggerty 3 ,- Acknowledgments Air Transport Association of America Battelle Memorial Institute Civil Aeronautics Board Council of Economic Advisers Export-Import Bank of the United States Exxon International Company Federal Trade Commission General Aviation Manufacturers Association International Civil Aviation Organization McGraw-Hill Publications Company National Aer~mautics and Space Administration National Science Foundation Office of Management and Budget U.S. Departments of Commerce (Bureau of the Census, Bureau of Economic Analysis, Bureau of Industrial Economics) Defense (Comptroller; Directorate for Information, Operations and Reports; Army, Navy, Air Force) Labor (Bureau of Labor Statistics) Transportation (Federal Aviation Administration The cover and chapter art throughout this edition of Aerospace Facts and Figures feature computer-inspired graphics-hot an original theme in the contemporary business environment, but one particularly relevant to the aerospace industry, which spawned the large-scale development and application of computers, and conti.nues to incorpora~e computer advances in all aspects of its design and manufacture of aircraft, mis­ siles, and space products.
    [Show full text]
  • Some Supersonic Aerodynamics
    Some Supersonic Aerodynamics W.H. Mason Configuration Aerodynamics Class Grumman Tribody Concept – from 1978 Company Calendar The Key Topics • Brief history of serious supersonic airplanes – There aren’t many! • The Challenge – L/D, CD0 trends, the sonic boom • Linear theory as a starting point: – Volumetric Drag – Drag Due to Lift • The ac shift and cg control • The Oblique Wing • Aero/Propulsion integration • Some nonlinear aero considerations • The SST development work • Brief review of computational methods • Possible future developments Are “Supersonic Fighters” Really Supersonic? • If your car’s speedometer goes to 120 mph, do you actually go that fast? • The official F-14A supersonic missions (max Mach 2.4) – CAP (Combat Air Patrol) • 150 miles subsonic cruise to station • Loiter • Accel, M = 0.7 to 1.35, then dash 25nm – 4 ½ minutes and 50nm total • Then, head home or to a tanker – DLI (Deck Launch Intercept) • Energy climb to 35K ft., M = 1.5 (4 minutes) • 6 minutes at 1.5 (out 125-130nm) • 2 minutes combat (slows down fast) After 12 minutes, must head home or to a tanker Very few real supersonic airplanes • 1956: the B-58 (L/Dmax = 4.5) – In 1962: Mach 2 for 30 minutes • 1962: the A-12 (SR-71 in ’64) (L/Dmax = 6.6) – 1st supersonic flight, May 4, 1962 – 1st flight to exceed Mach 3, July 20, 1963 • 1964: the XB-70 (L/Dmax = 7.2) – In 1966: flew Mach 3 for 33 minutes • 1968: the TU-144 – 1st flight: Dec. 31, 1968 • 1969: the Concorde (L/Dmax = 7.4) – 1st flight, March 2, 1969 • 1990: the YF-22 and YF-23 (supercruisers) – YF-22: 1st flt.
    [Show full text]