Subsonic Aircraft Wing Conceptual Design Synthesis and Analysis
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5.2 Drag Reduction Through Higher Wing Loading David L. Kohlman
5.2 Drag Reduction Through Higher Wing Loading David L. Kohlman University of Kansas |ntroduction The wing typically accounts for almost half of the wetted area of today's production light airplanes and approximately one-third of the total zero-lift or parasite drag. Thus the wing should be a primary focal point of any attempts to reduce drag of light aircraft with the most obvious configuration change being a reduction in wing area. Other possibilities involve changes in thickness, planform, and airfoil section. This paper will briefly discuss the effects of reducing wing area of typical light airplanes, constraints involved, and related configuration changes which may be necessary. Constraints and Benefits The wing area of current light airplanes is determined primarily by stall speed and/or climb performance requirements. Table I summarizes the resulting wing loading for a representative spectrum of single-engine airplanes. The maximum lift coefficient with full flaps, a constraint on wing size, is also listed. Note that wing loading (at maximum gross weight) ranges between about 10 and 20 psf, with most 4-place models averaging between 13 and 17. Maximum lift coefficient with full flaps ranges from 1.49 to 2.15. Clearly if CLmax can be increased, a corresponding decrease in wing area can be permitted with no change in stall speed. If total drag is not increased at climb speed, the change in wing area will not adversely affect climb performance either and cruise drag will be reduced. Though not related to drag, it is worthy of comment that the range of wing loading in Table I tends to produce a rather uncomfortable ride in turbulent air, as every light-plane pilot is well aware. -
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 ................................................................................................... -
F—18 Navy Air Combat Fighter
74 /2 >Af ^y - Senate H e a r tn ^ f^ n 12]$ Before the Committee on Appro priations (,() \ ER WIIA Storage ime nts F EB 1 2 « T H e -,M<rUN‘U«sni KAN S A S S F—18 Na vy Air Com bat Fighter Fiscal Year 1976 th CONGRESS, FIRS T SES SION H .R . 986 1 SPECIAL HEARING F - 1 8 NA VY AIR CO MBA T FIG H TER HEARING BEFORE A SUBC OMMITTEE OF THE COMMITTEE ON APPROPRIATIONS UNITED STATES SENATE NIN ETY-FOURTH CONGRESS FIR ST SE SS IO N ON H .R . 9 8 6 1 AN ACT MAKIN G APP ROPR IA TIO NS FO R THE DEP ARTM EN T OF D EFEN SE FO R T H E FI SC AL YEA R EN DI NG JU N E 30, 1976, AND TH E PE RIO D BE GIN NIN G JU LY 1, 1976, AN D EN DI NG SEPT EM BER 30, 1976, AND FO R OTH ER PU RP OSE S P ri nte d fo r th e use of th e Com mittee on App ro pr ia tio ns SPECIAL HEARING U.S. GOVERNM ENT PRINT ING OFF ICE 60-913 O WASHINGTON : 1976 SUBCOMMITTEE OF THE COMMITTEE ON APPROPRIATIONS JOHN L. MCCLELLAN, Ark ans as, Chairman JOH N C. ST ENN IS, Mississippi MILTON R. YOUNG, No rth D ako ta JOH N O. P ASTORE, Rhode Island ROMAN L. HRUSKA, N ebraska WARREN G. MAGNUSON, Washin gton CLIFFORD I’. CASE, New Je rse y MIK E MANSFIEL D, Montana HIRAM L. -
The Influence of Wing Loading on Turbofan Powered Stol Transports with and Without Externally Blown Flaps
https://ntrs.nasa.gov/search.jsp?R=19740005605 2020-03-23T12:06:52+00:00Z NASA CONTRACTOR NASA CR-2320 REPORT CXI CO CNI THE INFLUENCE OF WING LOADING ON TURBOFAN POWERED STOL TRANSPORTS WITH AND WITHOUT EXTERNALLY BLOWN FLAPS by R. L. Morris, C. JR. Hanke, L. H. Pasley, and W. J. Rohling Prepared by THE BOEING COMPANY WICHITA DIVISION Wichita, Kans. 67210 for Langley Research Center NATIONAL AERONAUTICS AND SPACE ADMINISTRATION • WASHINGTON, D. C. • NOVEMBER 1973 1. Report No. 2. Government Accession No. 3. Recipient's Catalog No. NASA CR-2320 4. Title and Subtitle 5. Reoort Date November. 1973 The Influence of Wing Loading on Turbofan Powered STOL Transports 6. Performing Organization Code With and Without Externally Blown Flaps 7. Author(s) 8. Performing Organization Report No. R. L. Morris, C. R. Hanke, L. H. Pasley, and W. J. Rohling D3-8514-7 10. Work Unit No. 9. Performing Organization Name and Address The Boeing Company 741-86-03-03 Wichita Division 11. Contract or Grant No. Wichita, KS NAS1-11370 13. Type of Report and Period Covered 12. Sponsoring Agency Name and Address Contractor Report National Aeronautics and Space Administration Washington, D.C. 20546 14. Sponsoring Agency Code 15. Supplementary Notes This is a final report. 16. Abstract The effects of wing loading on the design of short takeoff and landing (STOL) transports using (1) mechanical flap systems, and (2) externally blown flap systems are determined. Aircraft incorporating each high-lift method are sized for Federal Aviation Regulation (F.A.R.) field lengths of 2,000 feet, 2,500 feet, and 3,500 feet, and for payloads of 40, 150, and 300 passengers, for a total of 18 point-design aircraft. -
Aircraft of Today. Aerospace Education I
DOCUMENT RESUME ED 068 287 SE 014 551 AUTHOR Sayler, D. S. TITLE Aircraft of Today. Aerospace EducationI. INSTITUTION Air Univ.,, Maxwell AFB, Ala. JuniorReserve Office Training Corps. SPONS AGENCY Department of Defense, Washington, D.C. PUB DATE 71 NOTE 179p. EDRS PRICE MF-$0.65 HC-$6.58 DESCRIPTORS *Aerospace Education; *Aerospace Technology; Instruction; National Defense; *PhysicalSciences; *Resource Materials; Supplementary Textbooks; *Textbooks ABSTRACT This textbook gives a brief idea aboutthe modern aircraft used in defense and forcommercial purposes. Aerospace technology in its present form has developedalong certain basic principles of aerodynamic forces. Differentparts in an airplane have different functions to balance theaircraft in air, provide a thrust, and control the general mechanisms.Profusely illustrated descriptions provide a picture of whatkinds of aircraft are used for cargo, passenger travel, bombing, and supersonicflights. Propulsion principles and descriptions of differentkinds of engines are quite helpful. At the end of each chapter,new terminology is listed. The book is not available on the market andis to be used only in the Air Force ROTC program. (PS) SC AEROSPACE EDUCATION I U S DEPARTMENT OF HEALTH. EDUCATION & WELFARE OFFICE OF EDUCATION THIS DOCUMENT HAS BEEN REPRO OUCH) EXACTLY AS RECEIVED FROM THE PERSON OR ORGANIZATION ORIG INATING IT POINTS OF VIEW OR OPIN 'IONS STATED 00 NOT NECESSARILY REPRESENT OFFICIAL OFFICE OF EOU CATION POSITION OR POLICY AIR FORCE JUNIOR ROTC MR,UNIVERS17/14AXWELL MR FORCEBASE, ALABAMA Aerospace Education I Aircraft of Today D. S. Sayler Academic Publications Division 3825th Support Group (Academic) AIR FORCE JUNIOR ROTC AIR UNIVERSITY MAXWELL AIR FORCE BASE, ALABAMA 2 1971 Thispublication has been reviewed and approvedby competent personnel of the preparing command in accordance with current directiveson doctrine, policy, essentiality, propriety, and quality. -
Redesign of the Gossamer Albatross Using a Boxwing Armando R
Redesign of the Gossamer Albatross using a Boxwing Armando R. Collazo Garcia III, Undergraduate Student-Aerospace Engineering, Embry-Riddle Aeronautical University, Daytona Beach, FL 32114, [email protected] April 12, 2017 ABSTRACT Historically, human powered aircraft (HPA) have been known to have very large wingspans; the main reason being for aerodynamic performance. During low speeds, the predominant type of drag is the induced drag which is a by-product of large wing tip vortices generated at higher lift coefficients. In order to reduce this phenomenon, higher aspect ratio wings are used which is the reason behind the very large wingspans for HPA. Due to its high Oswald efficiency factor, the boxwing configuration is presented as a possible solution to decrease the wingspan while not affecting the aerodynamic performance of the airplane. The new configuration is analyzed through the use of VLAERO+©. The parasitic drag was estimated using empirical methods based on the friction drag of a flat plate. The structural weight changes in the boxwing design were estimated using “area weights” derived from the original Gossamer Albatross. The two aircraft were compared at a cruise velocity of 22 ft./s where the boxwing configuration showed a net drag reduction of approximately 0.36 lb., which can be deduced from a decrease of 0.81 lb. of the induced drag plus an increase of the parasite drag of around 0.45 lb. Therefore, for an aircraft with approximately half the wingspan, easier to handle, and more practical, the drag is essentially reduced by 4.4%. INTRODUCTION METHODOLOGY RESULTS Because of the availability of information and data, the Gossamer A boxwing of roughly half the span of the Albatross with the same airfoil, root chord, fuselage and taper ratio was modeled in VLAERO+©. -
Introduction to Aerospace Engineering
Introduction to Aerospace Engineering Lecture slides Challenge the future 1 15-12-2012 Introduction to Aerospace Engineering 5 & 6: How aircraft fly J. Sinke Delft University of Technology Challenge the future 5 & 6. How aircraft fly Anderson 1, 2.1-2.6, 4.11- 4.11.1, 5.1-5.5, 5.17, 5.19 george caley; wilbur wright; orville wright; samuel langley, anthony fokker; albert plesman How aircraft fly 2 19th Century - unpowered Otto Lilienthal (1848 – 1896) Was fascinated with the flight of birds (Storks) Studied at Technical School in Potsdam Started experiment in 1867 Made more than 2000 flights Build more than a dozen gliders Build his own “hill” in Berlin Largest distance 250 meters Died after a crash in 1896. No filmed evidence: film invented in 1895 (Lumiere) How aircraft fly 3 Otto Lilienthal Few designs How aircraft fly 4 Hang gliders Derivatives of Lilienthal’s gliders Glide ratio E.g., a ratio of 12:1 means 12 m forward : 1 m of altitude. Typical performances (2006) Gliders (see picture): V= ~30 to >145 km/h Glide ratio = ~17:1 (Vopt = 45-60 km/h) Rigid wings: V = ~ 35 to > 130 km/h Glide ratio = ~20:1 (Vopt = 50-60 km/h) How aircraft fly 5 Question With Gliders you have to run to generate enough lift – often down hill to make it easier. Is the wind direction of any influence? How aircraft fly 6 Answer What matters is the Airspeed – Not the ground speed. The higher the Airspeed – the higher the lift. So if I run 15 km/h with head wind of 10 km/h, than I create a higher lift (airspeed of 25 km/h) than when I run at the same speed with a tail wind of 10 km/h (airspeed 5 km/h)!! That’s why aircraft: - Take of with head winds – than they need a shorter runway - Land with head winds – than the stopping distance is shorter too How aircraft fly 7 Beginning of 20th century: many pioneers Early Flight 1m12s Failed Pioneers of Flight 2m53s How aircraft fly 8 1903 – first powered HtA flight The Wright Brothers December 17, 1903 How aircraft fly 9 Wright Flyer take-off & demo flight Wright Brothers lift-off 0m33s How aircraft fly 10 Wright Brs. -
Introduction to Aerospace Engineering
Introduction to Aerospace Engineering Lecture slides Challenge the future 1 Introduction to Aerospace Engineering Aerodynamics 11&12 Prof. H. Bijl ir. N. Timmer 11 & 12. Airfoils and finite wings Anderson 5.9 – end of chapter 5 excl. 5.19 Topics lecture 11 & 12 • Pressure distributions and lift • Finite wings • Swept wings 3 Pressure coefficient Typical example Definition of pressure coefficient : p − p -Cp = ∞ Cp q∞ upper side lower side -1.0 Stagnation point: p=p t … p t-p∞=q ∞ => C p=1 4 Example 5.6 • The pressure on a point on the wing of an airplane is 7.58x10 4 N/m2. The airplane is flying with a velocity of 70 m/s at conditions associated with standard altitude of 2000m. Calculate the pressure coefficient at this point on the wing 4 2 3 2000 m: p ∞=7.95.10 N/m ρ∞=1.0066 kg/m − = p p ∞ = − C p Cp 1.50 q∞ 5 Obtaining lift from pressure distribution leading edge θ V∞ trailing edge s p ds dy θ dx = ds cos θ 6 Obtaining lift from pressure distribution TE TE Normal force per meter span: = θ − θ N ∫ pl cos ds ∫ pu cos ds LE LE c c θ = = − with ds cos dx N ∫ pl dx ∫ pu dx 0 0 NN Write dimensionless force coefficient : C = = n 1 ρ 2 2 Vc∞ qc ∞ 1 1 p − p x 1 p − p x x = l ∞ − u ∞ C = ()C −C d Cn d d n ∫ pl pu ∫ q c ∫ q c 0 ∞ 0 ∞ 0 c 7 T=Lsin α - Dcosα N=Lcos α + Dsinα L R N α T D V α = angle of attack 8 Obtaining lift from normal force coefficient =α − α =α − α L Ncos T sin cl c ncos c t sin L N T =cosα − sin α qc∞ qc ∞ qc ∞ For small angle of attack α≤5o : cos α ≈ 1, sin α ≈ 0 1 1 C≈() CCdx − () l∫ pl p u c 0 9 Example 5.11 Consider an airfoil with chord length c and the running distance x measured along the chord. -
A High-Fidelity Approach to Conceptual Design John Thomas Watson Iowa State University
Iowa State University Capstones, Theses and Graduate Theses and Dissertations Dissertations 2016 A high-fidelity approach to conceptual design John Thomas Watson Iowa State University Follow this and additional works at: https://lib.dr.iastate.edu/etd Part of the Aerospace Engineering Commons, and the Art and Design Commons Recommended Citation Watson, John Thomas, "A high-fidelity approach to conceptual design" (2016). Graduate Theses and Dissertations. 15183. https://lib.dr.iastate.edu/etd/15183 This Thesis is brought to you for free and open access by the Iowa State University Capstones, Theses and Dissertations at Iowa State University Digital Repository. It has been accepted for inclusion in Graduate Theses and Dissertations by an authorized administrator of Iowa State University Digital Repository. For more information, please contact [email protected]. A high-fidelity approach to conceptual design by John T. Watson A thesis submitted to the graduate faculty in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE Major: Aerospace Engineering Program of Study Committee: Richard Wlezien, Major Professor Thomas Gielda Leifur Leifsson Iowa State University Ames, Iowa 2016 Copyright © John T. Watson, 2016. All rights reserved. ii TABLE OF CONTENTS Page LIST OF FIGURES ................................................................................................... iii LIST OF TABLES ..................................................................................................... v NOMENCLATURE ................................................................................................. -
After Concorde, Who Will Manage to Revive Civilian Supersonic Aviation?
After Concorde, who will manage to revive civilian supersonic aviation? By François Sfarti and Sebastien Plessis December 2019 Commercial aircraft are flying at the same speed as 60 years ago. Since Concorde, which made possible to fly from Paris to New York in only 3h30, no civilian airplane has broken the sound barrier. The loudness of the sonic boom was a major technological lock to Concorde success, but 50 years after its first flight, an on-going project led by NASA is about to make supersonic flights over land possible. If successful, it will significantly increase the number of supersonic routes and increase the supersonic aircraft market size substantially. This technological improvement combined with R&D efforts on operational costs and a much larger addressable market than when Concorde flew may revive civilian supersonic aviation in the coming years. Who are the new players at the forefront and the early movers? What are the current investments in this field? What are the key success drivers and remaining technological and regulatory locks to revive supersonic aviation? EXECUTIVE SUMMARY Commercial aircraft are typically flying between 800 km/h and 900 km/h, which is between 75% and 85% of the speed of sound. It is the same speed as 60 years ago and since Concorde, which flew at twice the speed of sound, was retired in 2003, there has been no civilian supersonic aircraft in service. Due to a prohibition to fly supersonic over land and large operational costs, Concorde did not reach commercial success. Even if operational costs would remain larger than subsonic flights, current market environment seems much more favourable: since Concorde was retired in 2003, the air traffic has more than doubled and the willingness to pay can be supported by an increase in the number of high net worth individuals and the fact that business travellers value higher speed levels. -
Zap Flaps and Ailerons by TEMPLE N
AER-56-5 Zap Flaps and Ailerons By TEMPLE N. JOYCE,1 DUNDALK, BALTIMORE, MD. The early history of the Zap development is covered, in been looked upon with more or less contempt. This was par cluding work done on the Flettner rotor plane in 1928. ticularly true during the boom days when everybody was using Because of phenomenal lift obtained by changes in flow a new engine and when landing speeds were thought of only in around a cylinder, investigations were begun on improving terms of getting into recognized airports. Three things have existing airfoils. This led to preliminary work on flapped occurred since then, however, that have again brought to the airfoils in the tunnel of New York University, and later its front the importance of low landing speed: First, a very distinct application to an Aristocrat cabin monoplane presented to realization that the public was afraid of aviation because of high the B/J Aircraft Corporation early in 1932. A chronological stalling speeds and the frequent crack-ups with serious conse record of the reactions of the personnel of the B/J organi quences. Second, the fact that increased high speeds could not zation to the Zap development is set forth, particularly be obtained without increasing still further high landing speeds the questions regarding lift and drag coefficients, effect unless some new aerodynamic development was brought into upon stability and balance, and the operating forces neces existence. Third, as speed ranges and wing loadings went up, sary to get the flaps down. The effectiveness of lateral takeoff run was increased and angle of climb decreased alarm control, particularly with regard to hinge moments and ingly. -
Section 7, Lecture 3: Effects of Wing Sweep
Section 7, Lecture 3: Effects of Wing Sweep • All modern high-speed aircraft have swept wings: WHY? 1 MAE 5420 - Compressible Fluid Flow • Not in Anderson Supersonic Airfoils (revisited) • Normal Shock wave formed off the front of a blunt leading g=1.1 causes significant drag Detached shock waveg=1.3 Localized normal shock wave Credit: Selkirk College Professional Aviation Program 2 MAE 5420 - Compressible Fluid Flow Supersonic Airfoils (revisited, 2) • To eliminate this leading edge drag caused by detached bow wave Supersonic wings are typically quite sharp atg=1.1 the leading edge • Design feature allows oblique wave to attachg=1.3 to the leading edge eliminating the area of high pressure ahead of the wing. • Double wedge or “diamond” Airfoil section Credit: Selkirk College Professional Aviation Program 3 MAE 5420 - Compressible Fluid Flow Wing Design 101 • Subsonic Wing in Subsonic Flow • Subsonic Wing in Supersonic Flow • Supersonic Wing in Subsonic Flow A conundrum! • Supersonic Wing in Supersonic Flow • Wings that work well sub-sonically generally don’t work well supersonically, and vice-versa à Leading edge Wing-sweep can overcome problem with poor performance of sharp leading edge wing in subsonic flight. 4 MAE 5420 - Compressible Fluid Flow Wing Design 101 (2) • Compromise High-Sweep Delta design generates lift at low speeds • Highly-Swept Delta-Wing design … by increasing the angle-of-attack, works “pretty well” in both flow regimes but also has sufficient sweepback and slenderness to perform very Supersonic Subsonic efficiently at high speeds. • On a traditional aircraft wing a trailing vortex is formed only at the wing tips.