The Philosophy of Airplane Design
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CHAPTER TWO - Static Aeroelasticity – Unswept Wing Structural Loads and Performance 21 2.1 Background
Static aeroelasticity – structural loads and performance CHAPTER TWO - Static Aeroelasticity – Unswept wing structural loads and performance 21 2.1 Background ........................................................................................................................... 21 2.1.2 Scope and purpose ....................................................................................................................... 21 2.1.2 The structures enterprise and its relation to aeroelasticity ............................................................ 22 2.1.3 The evolution of aircraft wing structures-form follows function ................................................ 24 2.2 Analytical modeling............................................................................................................... 30 2.2.1 The typical section, the flying door and Rayleigh-Ritz idealizations ................................................ 31 2.2.2 – Functional diagrams and operators – modeling the aeroelastic feedback process ....................... 33 2.3 Matrix structural analysis – stiffness matrices and strain energy .......................................... 34 2.4 An example - Construction of a structural stiffness matrix – the shear center concept ........ 38 2.5 Subsonic aerodynamics - fundamentals ................................................................................ 40 2.5.1 Reference points – the center of pressure..................................................................................... 44 2.5.2 A different -
Design of a Transonic Wing with an Adaptive Morphing Trailing Edge Via Aerostructural Optimization
Design of a Transonic Wing with an Adaptive Morphing Trailing Edge via Aerostructural Optimization David A. Burdettea, Joaquim R. R. A. Martinsa,∗ a University of Michigan, Department of Aerospace Engineering Abstract Novel aircraft configurations and technologies like adaptive morphing trailing edges offer the potential to improve the fuel efficiency of commercial transport aircraft. To accurately quantify the benefits of morphing wing technology for commercial transport aircraft, high-fidelity design optimization that considers both aerodynamic and structural design with a large number of design vari- ables is required. To address this need, we use high-fidelity aerostructural that enables the detailed optimization of wing shape and sizing using hundreds of de- sign variables. We perform a number of multipoint aerostructural optimizations to demonstrate the performance benefits offered by morphing technology and identify how those benefits are enabled. In a comparison of optimizations con- sidering seven flight conditions, the addition of a morphing trailing edge device along the aft 40% of the wing can reduce cruise fuel burn by more than 5%. A large portion of fuel burn reduction due to morphing trailing edges results from a significant reduction in structural weight, enabled by adaptive maneuver load alleviation. We also show that a smaller morphing device along the aft 30% of the wing produces nearly as much fuel burn reduction as the larger morphing device, and that morphing technology is particularly effective for high aspect ratio wings. Keywords: Morphing, Adaptive compliant trailing edge, Wing design, Aerostructural optimization, Common Research Model ∗Corresponding author Preprint submitted to Elsevier August 8, 2018 1. Introduction Increased awareness of environmental concerns and fluctuations in fuel prices in recent years have led the aircraft manufacturing industry to push for improved aircraft fuel efficiency. -
Low-Speed Aerodynamics Robert Stengel, Aircraft Flight Dynamics, MAE 331, 2018 Learning Objectives
Low-Speed Aerodynamics Robert Stengel, Aircraft Flight Dynamics, MAE 331, 2018 Learning Objectives • 2D lift and drag • Reynolds number effects • Relationships between airplane shape and aerodynamic characteristics • 2D and 3D lift and drag • Static and dynamic effects of aerodynamic control surfaces Reading: Flight Dynamics Aerodynamic Coefficients, 65-84 Copyright 2018 by Robert Stengel. All rights reserved. For educational use only. http://www.princeton.edu/~stengel/MAE331.html http://www.princeton.edu/~stengel/FlightDynamics.html 1 2-Dimensional Aerodynamic Lift and Drag 2 1 Wing Lift and Drag • Lift: Perpendicular to free-stream airflow • Drag: Parallel to the free-stream airflow 3 Longitudinal Aerodynamic Forces Non-dimensional force coefficients, CL and CD, are dimensionalized by dynamic pressure, q, N/m2 or lb/sq ft reference area, S, m2 of ft2 ⎛ 1 2 ⎞ Lift = C q S = C ρV S L L ⎝⎜ 2 ⎠⎟ ⎛ 1 2 ⎞ Drag = C q S = C ρV S D D ⎝⎜ 2 ⎠⎟ 4 2 Circulation of Incompressible Air Flow About a 2-D Airfoil Bernoullis equation (inviscid, incompressible flow) (Motivational, but not the whole story of lift) 1 p + ρV 2 = constant along streamline = p static 2 stagnation Vorticity at point x Vupper (x) = V∞ + ΔV(x) 2 ΔV(x) γ (x) = V (x) V V(x) 2 2−D lower = ∞ − Δ Δz(x) Circulation about airfoil Lower pressure on upper surface c c ΔV(x) Γ = γ (x)dx = dx 2−D ∫ 2−D ∫ 0 0 Δz(x) 5 Relationship Between Circulation and Lift Differential pressure along chord section ⎡ 1 2 ⎤ ⎡ 1 2 ⎤ Δp(x) = pstatic + ρ∞ (V∞ + ΔV (x) 2) − pstatic + ρ∞ (V∞ − ΔV (x) 2) ⎣⎢ 2 ⎦⎥ ⎣⎢ 2 ⎦⎥ 1 ⎡ 2 2 ⎤ = ρ∞ (V∞ + ΔV (x) 2) − (V∞ − ΔV (x) 2) 2 ⎣ ⎦ = ρ∞V∞ΔV (x) = ρ∞V∞Δz(x)γ 2−D (x) 2-D Lift (inviscid, incompressible flow) c c Lift = Δp x dx = ρ V γ (x)dx = ρ V Γ ( )2−D ∫ ( ) ∞ ∞ ∫ 2−D ∞ ∞ ( )2−D 0 0 1 2 ! ρ∞V∞ c(2πα ) thin, symmetric airfoil + ρ∞V∞ (Γcamber ) 2 [ ] 2−D 1 2 ! ρ V c C α + ρ V Γ 6 ∞ ∞ ( Lα ) ∞ ∞ ( camber )2−D 2 2−D 3 Lift vs. -
Flexible Wing Structure and Variable-Sweep Wing Mechanism
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 08 Issue: 03 | Mar 2021 www.irjet.net p-ISSN: 2395-0072 FLEXIBLE WING STRUCTURE AND VARIABLE-SWEEP WING MECHANISM Advait Inamdar1, Narayan Thakur2, Deepak Pal3, Akshat Mohite4 1Advait Inamdar, Mechanical Engineer, A. P. Shah Institute of Technology, Thane, Maharashtra, India 2Narayan Thakur, Mechanical Engineer, A. P. Shah Institute of Technology, Thane, Maharashtra, India 3Deepak Pal, Mechanical Engineer. Rajendra Mane College of Engineering and Technology, Ratnagiri, Maharashtra, India 4Akshat Mohite, Mechanical Engineer, A. P. Shah Institute of Technology, Thane, Maharashtra, India ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - Aircraft Wings use aerofoil design to create a lift reduce the fuel burn of the aircraft. This has a huge impact force that leads to flight. Ailerons are used to stabilize the on today’s world where rising environmental concerns rule flight and control pitch motion. These are flap-like mechanical the industry. However, to utilize this technology and benefit devices with lots of components which leads to increased from its gains, further design studies are required. weight and a higher chance of failure. Using flexible wing systems can increase the manoeuvrability of the aircraft Swept wing designs are commonly used today in commercial significantly. Using compliant mechanisms is the next step as aircraft due to their various advantages like a higher Critical they do not require hinges, bolts, etc., weight can be reduced Mach Number which results in a delay to the onset of wave significantly. Due to the aerofoil design, at higher speeds, the wind over the leading edge may go supersonic. This occurs due drag. -
11 Empennage Sizing
11 - 1 11 Empennage Sizing In Section Empennage General Design, the areas of the horizontal and vertical tailplanes were calculated merely with the aid of tail volume coefficients. The tail lever arms were estimated as a percentage of the length of the fuselage. This initial estimate was necessary as a starting value for the iteration to be carried out here and in order to have tail parameters available for calculating mass and center of gravity. In this Section Empennage Sizing, the tail parameters will be calculated from stability and control requirements. 11.1 Horizontal Tailplane Sizing Horizontal tailplane sizing according to control requirement The horizontal tailplane sizing is based on the moment equilibrium around the lateral axis. The sum of the moments around the center of gravity gives =+⋅ +++−⋅−() + MMLxMMMLlxCG W W CG−− AC F E N H H CG AC M H . (11.1) Designations from equation (11.1) are explained in Fig. 11.1 in connection with Fig. 11.2. In addition: M F : The pitching moment of the fuselage (F) can be estimated according to DATCOM 1978 (4.2.2). The DATCOM method is comparatively time-consuming and is not presented here. M F is positive. For control, disregarding M F is a conser- vative estimate. M E : The pitching moment through the engines (E) is caused: 1. by the fact that the thrust vector does not go through the center of gravity; 2. by a propeller force perpendicular to the propeller shaft upward or downward, caused when the flow against the propeller is not directly from the front, but at an angle to the propeller shaft; 3. -
Matamorph 2: a New Experimental UAV with Twist-Morphing Wings and Camber-Morphing Tail Stabilizers
AIAA SciTech Forum 10.2514/6.2021-0584 11–15 & 19–21 January 2021, VIRTUAL EVENT AIAA Scitech 2021 Forum MataMorph 2: A new experimental UAV with twist-morphing wings and camber-morphing tail stabilizers Adam E. Schlup1, Tommy L. MacLennan1, Cristobal Barajas1, Bianca L. Talebian1, Gregory C. Thatcher1, Richard B. Flores1, Justin D. Perez-Norwood1, Christian L. Torres1, Kebron B. Kibret1, Edgar E. Guzman1 and Dr. Peter L. Bishay2 California State University, Northridge, Northridge, CA, 91330, United States Morphing technology aims to improve both aerodynamic and power efficiency of aircrafts by eliminating traditional control surfaces and implementing uniform wings with seamless shape- changing ability. A lot of research has focused on proposing new designs for morphing wings, without implementation in a flying aircraft. Only few papers reported the design and flight- testing of unmanned aerial vehicles (UAVs) with morphing surfaces. Most of such designs focused only on wings, while the tail stabilizers are conventionally designed. This paper presents Matamorph-2 (XM-2), a fully morphing UAV with twisting wings and variable- camber tail stabilizers. XM-2 can perform all required maneuvers without any discrete control surfaces. The wings feature balsa wood structure, wing-root and wing-tip laminated composite skin sections and a twisting section made of polyurethane foam covered by a smooth flexible skin. With a ±15° range of twisting motion, XM-2 wings do not need flaps, slats or ailerons to control lift and roll generated by the UAV. Each tail stabilizer consists of a rigid leading-edge section connected to a camber-morphing corrugated trailing edge section. -
Chapter 5 Wing Design
CHAPTER 5 WING DESIGN Mohammad Sadraey Daniel Webster College Table of Contents Chapter 5 ................................................................................................................................................... 1 Wing Design ............................................................................................................................................. 1 5.1. Introduction ................................................................................................................................ 1 5.2. Number of Wings ...................................................................................................................... 4 5.3. Wing Vertical Location ............................................................................................................ 5 5.3.1. High Wing............................................................................................................................. 7 5.3.2. Low Wing .............................................................................................................................. 9 5.3.3. Mid Wing ............................................................................................................................. 10 5.3.4. Parasol Wing ..................................................................................................................... 10 5.3.5. The Selection Process ................................................................................................... 11 5.4. Airfoil .......................................................................................................................................... -
Computational Fluid Dynamics Simulations of Oscillating Wings and Comparison to Lifting-Line Theory
Utah State University DigitalCommons@USU All Graduate Theses and Dissertations Graduate Studies 5-2015 Computational Fluid Dynamics Simulations of Oscillating Wings and Comparison to Lifting-Line Theory Megan Keddington Utah State University Follow this and additional works at: https://digitalcommons.usu.edu/etd Part of the Aerospace Engineering Commons Recommended Citation Keddington, Megan, "Computational Fluid Dynamics Simulations of Oscillating Wings and Comparison to Lifting-Line Theory" (2015). All Graduate Theses and Dissertations. 4473. https://digitalcommons.usu.edu/etd/4473 This Thesis is brought to you for free and open access by the Graduate Studies at DigitalCommons@USU. It has been accepted for inclusion in All Graduate Theses and Dissertations by an authorized administrator of DigitalCommons@USU. For more information, please contact [email protected]. COMPUTATIONAL FLUID DYNAMICS SIMULATIONS OF OSCILLATING WINGS AND COMPARISON TO LIFTING-LINE THEORY by Megan Keddington A thesis submitted in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE in Aerospace Engineering Approved: ____________________ ____________________ Warren F. Phillips Steven L. Folkman Major Professor Committee Member ____________________ ____________________ Douglas F. Hunsaker Mark R. McLellan Committee Member Vice President for Research and Dean of the School of Graduate Studies UTAH STATE UNIVERSITY Logan, Utah 2015 ii Copyright © Megan Keddington 2015 All Rights Reserved iii ABSTRACT Computational Fluid Dynamics Simulations of Oscillating Wings and Comparison to Lifting-Line Solution by Megan Keddington Utah State University, 2015 Major Professor: Dr. Warren F. Phillips Department: Mechanical and Aerospace Engineering Computational fluid dynamics (CFD) analysis was performed in order to compare the solutions of oscillating wings with Prandtl’s lifting-line theory. -
Exploitation of a Multifunctional Twistable Wing Trailing-Edge for Performance Improvement of a Turboprop 90-Seats Regional Aircraft
aerospace Article Exploitation of a Multifunctional Twistable Wing Trailing-Edge for Performance Improvement of a Turboprop 90-Seats Regional Aircraft Francesco Rea 1,* , Francesco Amoroso 1, Rosario Pecora 1 and Frederic Moens 2 1 Department of Industrial Engineering (Aerospace Division), University of Naples “Federico II”, Via Claudio 21, 80125 Naples, Italy; [email protected] (F.A.); [email protected] (R.P.) 2 ONERA, The French Aerospace Lab, Aerodynamic Aeroelasticity and Acoustics Department, 92190 Meudon, France; [email protected] * Correspondence: [email protected]; Tel.: +39-081-768-3573 Received: 4 October 2018; Accepted: 9 November 2018; Published: 16 November 2018 Abstract: Modern transport aircraft wings have reached near-peak levels of energy-efficiency and there is still margin for further relevant improvements. A promising strategy for improving aircraft efficiency is to change the shape of the aircraft wing in flight in order to maximize its aerodynamic performance under all operative conditions. In the present work, this has been developed in the framework of the Clean Sky 2 (REG-IADP) European research project, where the authors focused on the design of a multifunctional twistable trailing-edge for a Natural Laminar Flow (NLF) wing. A multifunctional wing trailing-edge is used to improve aircraft performance during climb and off-design cruise conditions in response to variations in speed, altitude and other flight parameters. The investigation domain of the novel full-scale device covers 5.15 m along the wing span and the 10% of the local wing chord. Concerning the wing trailing-edge, the preliminary structural and kinematic design process of the actuation system is completely addressed: three rotary brushless motors (placed in root, central and tip sections) are required to activate the inner mechanisms enabling different trailing-edge morphing modes. -
2013. Preliminary Airfoil Design of an Innovative Adaptive Variable Camber Compliant Wing
2013. Preliminary airfoil design of an innovative adaptive variable camber compliant wing Hongda Li1, Haisong Ang2 Ministerial Key Discipline Laboratory of Advanced Design Technology of Aircraft, College of Aerospace Engineering, Nanjing University of Aeronautics and Astronautics, Nanjing, China 2Corresponding author E-mail: [email protected], [email protected] Received 6 December 2015; received in revised form 25 February 2016; accepted 11 April 2016 DOI http://dx.doi.org/10.21595/jve.2016.16705 Abstract. In this study, an innovative adaptive variable camber compliant wing, with skin that can change thickness and tailing edge morphing mechanism that is designed based on a new kind of artificial muscles, is designed. Consisted of a compliant base plate and seamless and continuous compliant skin with the artificial muscles embedded in, this trailing edge morphing mechanism is extremely light in weight and efficient in reconfiguration of the wing sectional profile. To demonstrate the feasibility of this design, a simulative experiment of this kind of artificial muscles was designed and carried out. A demonstrative wing section with simulative driving skin mechanism and the compliant skin was manufactured. The demonstration wing section shows that the trailing edge morphing mechanism designed and simulative driving skin work good, with a –30°/+30° trailing edge morphing achieved. Targeting this innovative design, an airfoil design approach, employing CST parametric methodology, XFOIL and Multi-Objective Particle Swarm (MOPS) optimizer, is developed for the preliminary design of this innovative wing. A new selector is introduced to facilitate the searching process and improve the robustness of this method. The results show that this method is capable of designing airfoils for this special wing in a quick and effective way. -
A Review of Modelling and Analysis of Morphing Wings
A Review of Modelling and Analysis of Morphing Wings Daochun Lia, Shiwei Zhaoa, Andrea Da Ronchb*, Jinwu Xianga*, Jernej Drofelnikb, Yongchao Lia, Lu Zhanga, Yining Wua, Markus Kintscherc, Hans Peter Monnerc, Anton Rudenkoc, Shijun Guod, Weilong Yine, Johannes Kirnf, Stefan Stormf, Roeland De Breukerg, a School of Aeronautic Science and Engineering Beihang University, Beijing, China b Faculty of Engineering and the Environment University of Southampton, Southampton, SO17 1BJ, UK c Institute of Composite Structures and Adaptive Systems German Aerospace Centre, Braunschweig, Germany d Aerospace Engineering, School of Engineering Cranfield University, Bedford, UK e College of Aeronautics Harbin Institute of Technology, Harbin, China f IC3 - Energy, Propulsion & Aerodynamics, Airbus Group Innovations Munich, Germany g Aerospace Structures and Computational Mechanics, Delft University of Technology Delft, The Netherlands Abstract Morphing wings have a large potential to improve the overall aircraft performances, in a way like natural flyers do. By adapting or optimising dynamically the shape to various flight conditions, there are yet many unexplored opportunities beyond current proof-of-concept demonstrations. This review discusses the most prominent examples of morphing concepts with applications to two and three- dimensional wing models. Methods and tools commonly deployed for the design and analysis of these concepts are discussed, ranging from structural to aerodynamic analyses, and from control to optimisation aspects. Throughout the review process, it became apparent that the adoption of morphing concepts for routine use on aerial vehicles is still scarce, and some reasons holding back their integration for industrial use are given. Finally, promising concepts for future use are identified. Keywords: morphing wings; unmanned aerial vehicles; concepts; demonstrators; methods 1 Table of Contents 1. -
Aerodynamics of 3D Lifting Surfaces Through Vortex Lattice Methods
Aerodynamics of 3D Lifting Surfaces through Vortex Lattice Methods Wing and Wing-canard Aerodynamics Outline • Basic Concepts – Boundary conditions on the mean surface – Vortex Theorems, Biot-Savart Law – The Horseshoe Vortex – Selection of Control Point and Vortex Location • The Classical Vortex Lattice Method • Two implementations of the VLM – VLM program –TORNADO • Application Examples of VLM • Insights into wing and wing-canard aerodynamics Aerodynamics of Wings • Analysis Method – Lifting line theory • It is essentially correct for unswept wings, but is completely erroneous for swept wings. – Vortex lattice method • Be able to treat swept wings – Other advanced numerical methods Basic Concepts Design requirements Aero. characteristics Aerodynamic center stability and handling ¾ stability and handling low drag Spanload high maximum lift coef. ¾ location of the max. section lift coefficient field performance ¾ induced drag maneuver requirements ¾ root bending moment Wing shape Aspect ratio Taper Sweep Twist Design of Wing Shape • Aspect ratio, AR – From the view of aerodynamics • High values of AR for low induce drag – From the view of structure • Low values of AR for light structural weight Design of Wing Shape • Taper, λ – From the view of aerodynamics • For a straight untwisted, unswept wing, the min. induced drag corresponds to a taper ratio of about 0.4. • When highly tapered wings are selected, the section lift coefficient near the tip may become high. – From the view of structure • To reduce structural weight the wing should be highly tapered, with λ < 0.4. – From the view of manufacture • A tapered wing is more difficult and hence expensive to build than an untapered wing. Design of Wing Shape • Sweep, Λ – From the view of aerodynamics • Sweep is used primarily to delay the effects of compressibility and increase the drag divergence Mach number.