Simulation and Control Design of a Gliding Autogyro for Precision Airdrop by Joshua F

Total Page:16

File Type:pdf, Size:1020Kb

Simulation and Control Design of a Gliding Autogyro for Precision Airdrop by Joshua F Simulation and Control Design of a Gliding Autogyro for Precision Airdrop by Joshua F. Torgerson Submitted to the Department of Aeronautics and Astronautics in partial fulfillment of the requirements for the degree of Master of Science in Aeronautics and Astronautics at the MASSACHUSETTS INSTITUTE OF TECHNOLOGY June 2005 @ Joshua F. Torgerson, MMV. All rights reserved. The author hereby grants to MIT permission to reproduce and distribute publicly paper and electronic copies of this thesis document in whole or in part. MASSACHUSETTS INS E OF TECHNOLOGY JUN 2 3 2OO5 Author ...... IBRARIES Department of Aeronautics and Astronautics May 6, 2005 Certified by ........... ... ........ John J. Deyst Professor of Aeronautics and Astronautics Thesis Supervisor C ertified by ........... ................. Sean George Member Technical Staff, Draper Laboratory Thesis Supervisor A ccepted by .......................................... Jaime Peraire Chairman, Department Committee on Graduate Students AERO i [This page intentionally left blank.] Simulation and Control Design of a Gliding Autogyro for Precision Airdrop by Joshua F. Torgerson Submitted to the Department of Aeronautics and Astronautics on May 6, 2005, in partial fulfillment of the requirements for the degree of Master of Science in Aeronautics and Astronautics Abstract Precision airdrop is a technology whose required capabilities have become more exact- ing as combat situations necessitate greater degrees of accuracy. Ballistic and parafoil type delivery vehicles do not have the capacity to consistently deliver a payload on, for example, a particular rooftop in an urban combat situation. A gliding autogyro delivery platform has been investigated as a means of achieving greater airdrop performance. The autogyro has similar gliding characteristics to the parafoil, but has improved wind resilience and control authority. An initial simulation, based on momentum and blade element helicopter theory, has been constructed. A classical controller using a multiple loop closure strategy has been developed that uses a new nonlinear guidance law to follow paths generated by an algorithm considering initial conditions. An extended Kalman filter is used for state estimation. Results from simulations show consistent accuracy of about 5 feet, with the final position error rarely exceeding 10 feet. Thesis Supervisor: John J. Deyst Title: Professor of Aeronautics and Astronautics Thesis Supervisor: Sean George Title: Member Technical Staff, Draper Laboratory 3 [This page intentionally left blank.] Acknowledgments Acknowledgment May 6, 2005 This thesis was prepared at The Charles Stark Draper Laboratory, Inc., under Internal Company Sponsored Research in the Autonomous Vehicles Laboratory, Project Number 5042. Publication of this thesis does not constitute approval by Draper of the findings or conclusions contained herein. It is published for the exchange and stimulation of ideas. Joshua F. Torgerson 5 [This page intentionally left blank.] Contents 1 Introduction 19 2 Simulation Development 23 2.1 Equations of Motion ... .... ... .... ... .... ... ... 23 2.1.1 Quaternions ... ... .... .... .... .... .... .. 26 2.1.2 W ind .. ... .... ... ... .... ... ... .... ... 27 2.2 Forces and Moments ... .... ... ... ... ... ... ... .. 28 2.2.1 Rotor Forces and Moments .. ... .... ... ... ... .. 28 2.2.2 Induced Velocity Near Vertical Descent .. .... ... ... 32 2.2.3 Aerodynamic Forces and Moments . ... ... ... ... .. 33 2.3 Implementation .. .. ... ... ... .. ... ... ... .. ... 35 2.4 Validation . ... .... ... ... ... ... ... ... ... ... 36 3 Guidance Control Design 39 3.1 Linearization .. .... ... ... ... ... ... ... ... ... 39 3.2 Modal Analysis ... .... ... .... ... ... .... ... ... 40 3.3 Control Structure ... ... .. ... ... ... .. ... ... ... 43 3.4 Longitudinal Control Design ... ... ... ... ... ... ... .. 44 3.5 Lateral Control Design . ... .. ... .. ... .. ... .. ... .. 49 3.6 Path Planning .. .. ... .. ... .. ... .. ... .. ... .. .. 54 3.6.1 Steady Wind ... ... ... ... ... ... ... ... ... 57 3.7 Simulation Results . ... ... ... .. ... ... ... .. ... .. 58 7 4 Estimation 61 4.1 Extended Kalman Filter . ...... ...... ..... ...... 61 4.2 Filter Dynamics .............. ................ 61 4.3 Time Propagation. ....... ........ ....... ...... 63 4.4 Measurement Updates ..... ........ ....... ...... 64 4.4.1 G P S . ........... .......... ...... 65 4.4.2 Magnetometer. ..... ....... ....... ....... 65 4.4.3 Range Finder ... ..................... ... 66 4.4.4 Pixel Position ... ....... ....... ....... ... 66 4.5 Estimator Performance .. ....... ........ ........ 69 5 Results 73 5.1 Parameter Setup ........ ........ ....... ...... 73 5.2 Accuracy. ....... ........ ........ ....... ... 74 6 Conclusion 75 A Solutions for Thrust and Induced Velocity 77 A.1 Iterative Solution ....... ........... ........... 77 A.2 Quartic Solution .. ....... ........ ........ .... 79 B Simulation Details 81 B.1 Parameters ........ ....... ........ ........ 81 B.2 Trim Point ... ....... ........ ........ ....... 82 B.3 Linear Model .. ........ ........ ....... ...... 82 C Estimator Definition 85 C.1 Error Covariance Propagation .. .... ............... 85 C.2 Linearized Measurement Equations ........... ........ 88 C.2.1 G PS ....... ...... .............. ..... 89 C.2.2 Magnetometer ....... ..... .............. 89 C.2.3 Range Finder .... .... .......... ......... 89 8 C .2.4 C am era Im age .. .. .. ... .. .. .. .. .. .. .. .. .. 90 9 [This page intentionally left blank.] List of Figures 1-1 GyroBee model aircraft and coordinate system (reprinted with permis- sion from the Autogyro Company of Arizona) .... ........ 20 2-1 Comparison of theory and simulation trim response ...... .... 36 2-2 Trim forward rotor tilt input and glide slope ... ........ ... 37 3-1 Comparison of linear and nonlinear impulse responses ... ...... 40 3-2 Eigenvalues of the linear system on the imaginary plane .... .... 41 3-3 Modal response of linear system .. .... ..... ..... ..... 42 3-4 Nonlinear guidance diagram .. ..... .... ..... ..... .. 44 3-5 Control structure .... ...... ...... ....... ...... 45 3-6 Longitudinal glide slope controller .... ..... ..... ..... 45 3-7 Bode plots of successive longitudinal inner loop transfer functions, from 6f to the controlled variable ........ ........ ....... 46 3-8 Eigenvalues of inner-loop controlled longitudinal system ...... .. 47 3-9 Response of linear model to step in y . ....... ...... .. 48 3-10 Response of linear model to initial altitude offset . ..... ..... 49 3-11 Lateral bank controller ........ ........ ......... 50 3-12 Bode plots of successively closed lateral inner loop transfer functions, from 6, to the controlled variable .... ....... ....... .. 51 3-13 Eigenvalues of inner-loop controlled lateral system ..... ...... 52 3-14 Response of linear model to step in # ... ...... ...... .. 52 3-15 Response of linear model to various commanded paths .. ...... 53 3-16 Trajectory Setup . ..... ...... .... ..... ..... ... 54 11 3-17 Detailed geometry of the first turn in the commanded path .. .. 56 3-18 Path generation with and without wind U, = -2ft/s, W, = 10ft/s . 58 3-19 Controlled simulation result . .. .. .. .. .. .. 59 4-1 Geometry of camera showing vector relations . .. .. .. .. 68 4-2 Camera image details . .. .. .. .. .. .. .. .. .. 68 4-3 Results of baseline estimator simulation . .. .. .. .. .. 70 5-1 Final absolute position error of several simulation runs .. .. .. 74 A-1 Locus of roots of the induced velocity equation ((A.3)) with varying forward flight speeds .. .. .. .. .. .. .. .. .. .. 78 12 List of Tables 3.1 Eigenvalues of the linear system with their interpretations .. ... 43 3.2 Controller parameter summary .. ... ... .. ... .. ... .. 53 4.1 Root mean square values of estimation error during the entire and last ten seconds of the baseline estimator simulation .. .. ... .. .. 69 5.1 Variances of the normally distributed parameters for simulation trials 73 B.1 Simulation parameters ... .. .. ... .. .. ... .. .. ... .. 81 B.2 Simulation trim point . ... .. ... ... .. ... .. ... .. ... 82 13 [This page intentionally left blank.] List of Symbols C ............ direction cosine transformation matrix, body to local frames CDO .. .. .. .. zero lift drag coefficient of blades CT 2 ........... coefficient of thrust pwr,2 t~t tip F ............ force vector [X Y Z]T F ........... equivalent flat plate area of blades G............controller transfer function H ........... angular momentum vector I.............inertia matrix Ib... ......... inertia of rotor blade IX, I yI Izz . inertia KGE ......... ground effect constant L,M N..... torque around x, y, z axes Li.. ......... reference point distance in nonlinear lateral guidance law P, Q,R ...... body rotation rates about x, y, z axes Pi,P ...... .. induced and profile power of rotor T... ......... torque vector [L M N]T T... ......... thrust from rotor U, V, W ...... linear velocities in x, y, z directions Vi .. ......... induced velocity Vh .. ......... induced velocity in hover Vtip . ......... blade tip speed Qr Wb.. ......... aggregate velocity normal to blade W r .......... aggregate velocity normal to rotor disk X, Y, Z ...... forces in x, y, z directions X 0 s, Yv, Z., dimensional drag/lift coefficients Yuv, Zuw.. dimensional lift coefficient due to angle of attack 15 a ............ lift curve slope of rotor blade ao, ai, b1 ..... coning, forward, and side flapping angles of the rotor disk b.............number of blades c.............chord
Recommended publications
  • Real-Time Helicopter Flight Control: Modelling and Control by Linearization and Neural Networks
    Purdue University Purdue e-Pubs Department of Electrical and Computer Department of Electrical and Computer Engineering Technical Reports Engineering August 1991 Real-Time Helicopter Flight Control: Modelling and Control by Linearization and Neural Networks Tobias J. Pallett Purdue University School of Electrical Engineering Shaheen Ahmad Purdue University School of Electrical Engineering Follow this and additional works at: https://docs.lib.purdue.edu/ecetr Pallett, Tobias J. and Ahmad, Shaheen, "Real-Time Helicopter Flight Control: Modelling and Control by Linearization and Neural Networks" (1991). Department of Electrical and Computer Engineering Technical Reports. Paper 317. https://docs.lib.purdue.edu/ecetr/317 This document has been made available through Purdue e-Pubs, a service of the Purdue University Libraries. Please contact [email protected] for additional information. Real-Time Helicopter Flight Control: Modelling and Control by Linearization and Neural Networks Tobias J. Pallett Shaheen Ahmad TR-EE 91-35 August 1991 Real-Time Helicopter Flight Control: Modelling and Control by Lineal-ization and Neural Networks Tobias J. Pallett and Shaheen Ahmad Real-Time Robot Control Laboratory, School of Electrical Engineering, Purdue University West Lafayette, IN 47907 USA ABSTRACT In this report we determine the dynamic model of a miniature helicopter in hovering flight. Identification procedures for the nonlinear terms are also described. The model is then used to design several linearized control laws and a neural network controller. The controllers were then flight tested on a miniature helicopter flight control test bed the details of which are also presented in this report. Experimental performance of the linearized and neural network controllers are discussed.
    [Show full text]
  • Montgomerie-Bensen B8MR, G-BXDC
    Montgomerie-Bensen B8MR, G-BXDC AAIB Bulletin No: 1/2001 Ref: EW/C2000/04/03 - Category: 2.3 Aircraft Type and Registration: Montgomerie-Bensen B8MR, G-BXDC No & Type of Engines: 1 Rotax 582 piston engine Year of Manufacture: 1999 Date & Time (UTC): 16 April 2000 at 1411 hrs Location: Carlisle Airport, Cumbria Type of Flight: Private Persons on Board: Crew - 1 - Passengers - None Injuries: Crew - 1 - Passengers - N/A Nature of Damage: Aircraft destroyed Commander's Licence: Private Pilot's Licence (gyroplanes) Commander's Age: 51 years Commander's Flying Experience: 67 hours (of which 30 were on type) Last 90 days - 44 hours Last 28 days - 43 hours Information Source: AAIB Field Investigation Background information The pilot first showed an active interest in autogyros when in March 1999 he visited Carlisle Airport for a trial lesson. He had not flown before and enjoyed the experience so much that he flew again the same day and agreed to embark on a formal training programme with an instructor who was authorised by the CAA to conduct dual and single seat autogyro training as well as flight examinations. The instructor reported that his student approached all matters to do with his flying 'with a great deal of enthusiasm and a fair degree of ability'. From the start of his course until January 2000 the pilot undertook dual instruction, mainly at weekends, on a two seater VPM M16 autogyro. By March 2000 he was sufficiently experienced to transfer to the 'open frame' single-seat Benson autogyro. He flew this for approximately 20 hours, carrying out mainly short 'hops' along the length of the runway and practising balancing on the main wheels before progressing to flying the aircraft in the visual circuit and carrying out general handling exercises.
    [Show full text]
  • Book Reviews the SYCAMORE SEEDS
    Afterburner Book Reviews THE SYCAMORE SEEDS Early British Helicopter only to be smashed the following night in a gale. The book then covers the Cierva story in some detail, the Development chapter including, out of context, two paragraphs on By C E MacKay the Brennan propeller-driven rotor driven helicopter [helicogyro] fl own in 1924 at Farnborough but Distributed by A MacKay, 87 Knightscliffe Avenue, aborted by the Air Ministry the next year, stating that Netherton, Glasgow G13 2RX, UK (E charlese87@ there was no future for the helicopter and backing btinternet.com). 2014. 218pp. Illustrated. £12.95. Cierva’s autogyro programme contracting Avro to build ISBN 978-0-9573443-3-4. the fi rst British machines. Good coverage is given to the range of Cierva autogyros culminating in the Avro Given the paucity of coverage of British helicopter C30 Rota and its service use by the RAF. development I approached this slim (218 A5 pp) The heart of the book begins with a quotation: publication with interest. While autogyros have been “Morris, I want you to make me blades, helicopter well documented, Charnov and Ord-Hume giving blades,” with which William Weir, the fi rst Air Minister, exhaustive and well documented treatments of the founder of the RAF and supporter of Cierva, brought helicopter’s predecessor, the transition to the directly furniture maker H Morris & Co into the history of driven rotor of the helicopter is somewhat lacking. rotorcraft pulling in designers Bennett, Watson, Unfortunately MacKay’s book only contributes a Nisbet and Pullin with test pilots Marsh and Brie fi nal and short chapter to the ‘British Helicopter’ to form his team.
    [Show full text]
  • Adventures in Low Disk Loading VTOL Design
    NASA/TP—2018–219981 Adventures in Low Disk Loading VTOL Design Mike Scully Ames Research Center Moffett Field, California Click here: Press F1 key (Windows) or Help key (Mac) for help September 2018 This page is required and contains approved text that cannot be changed. NASA STI Program ... in Profile Since its founding, NASA has been dedicated • CONFERENCE PUBLICATION. to the advancement of aeronautics and space Collected papers from scientific and science. The NASA scientific and technical technical conferences, symposia, seminars, information (STI) program plays a key part in or other meetings sponsored or co- helping NASA maintain this important role. sponsored by NASA. The NASA STI program operates under the • SPECIAL PUBLICATION. Scientific, auspices of the Agency Chief Information technical, or historical information from Officer. It collects, organizes, provides for NASA programs, projects, and missions, archiving, and disseminates NASA’s STI. The often concerned with subjects having NASA STI program provides access to the NTRS substantial public interest. Registered and its public interface, the NASA Technical Reports Server, thus providing one of • TECHNICAL TRANSLATION. the largest collections of aeronautical and space English-language translations of foreign science STI in the world. Results are published in scientific and technical material pertinent to both non-NASA channels and by NASA in the NASA’s mission. NASA STI Report Series, which includes the following report types: Specialized services also include organizing and publishing research results, distributing • TECHNICAL PUBLICATION. Reports of specialized research announcements and feeds, completed research or a major significant providing information desk and personal search phase of research that present the results of support, and enabling data exchange services.
    [Show full text]
  • Helicopter Physics by Harm Frederik Althuisius López
    Helicopter Physics By Harm Frederik Althuisius López Lift Happens Lift Formula Torque % & Lift is a mechanical aerodynamic force produced by the Lift is calculated using the following formula: 2 = *4 '56 Torque is a measure of how much a force acting on an motion of an aircraft through the air, it generally opposes & object causes that object to rotate. As the blades of a Where * is the air density, 4 is the velocity, '5 is the lift coefficient and 6 is gravity as a means to fly. Lift is generated mainly by the the surface area of the wing. Even though most of these components are helicopter rotate against the air, the air pushes back on the rd wings due to their shape. An Airfoil is a cross-section of a relatively easy to measure, the lift coefficient is highly dependable on the blades following Newtons 3 Law of Motion: “To every wing, it is a streamlined shape that is capable of generating shape of the airfoil. Therefore it is usually calculated through the angle of action there is an equal and opposite reaction”. This significantly more lift than drag. Drag is the air resistance attack of a specific airfoil as portrayed in charts much like the following: reaction force is translated into the fuselage of the acting as a force opposing the motion of the aircraft. helicopter via torque, and can be measured for individual % & -/ 0 blades as follows: ! = #$ = '()*+ ∫ # 1# , where $ is the & -. Drag Force. As a result the fuselage tends to rotate in the Example of a Lift opposite direction of its main rotor spin.
    [Show full text]
  • Helicopter Flying Handbook (FAA-H-8083-21B) Chapter 8
    Chapter 8 Ground Procedures and Flight Preparations Introduction Once a pilot takes off, it is up to him or her to make sound, safe decisions throughout the flight. It is equally important for the pilot to use the same diligence when conducting a preflight inspection, making maintenance decisions, refueling, and conducting ground operations. This chapter discusses the responsibility of the pilot regarding ground safety in and around the helicopter and when preparing to fly. 8-1 Preflight There are two primary methods of deferring maintenance on rotorcraft operating under part 91. They are the deferral Before any flight, ensure the helicopter is airworthy by provision of 14 CFR part 91, section 91.213(d) and an FAA- inspecting it according to the rotorcraft flight manual (RFM), approved MEL. pilot’s operating handbook (POH), or other information supplied either by the operator or the manufacturer. The deferral provision of 14 CFR section 91.213(d) is Remember that it is the responsibility of the pilot in command widely used by most pilot/operators. Its popularity is due (PIC) to ensure the aircraft is in an airworthy condition. to simplicity and minimal paperwork. When inoperative equipment is found during preflight or prior to departure, the In preparation for flight, the use of a checklist is important decision should be to cancel the flight, obtain maintenance so that no item is overlooked. [Figure 8-1] Follow the prior to flight, determine if the flight can be made under the manufacturer’s suggested outline for both the inside and limitations imposed by the defective equipment, or to defer outside inspection.
    [Show full text]
  • Paper Helicopters Preparation
    Paper Helicopters Preparation CLASS LEVEL First – sixth class OBJECTIVES Content Strand and Strand Unit Energy & forces, Forces Through investigation the child should be enabled to come to appreciate that gravity is a force, SESE: Science Curriculum page 87. In this activity children explore how some things fall and how varying the size of the rotor blades, the shape of the rotor blades and the weight of a paper helicopter affect the way a helicopter spins. Skill development Through completing the strand units of the science curriculum the child should be enabled to design, plan and carry out simple experiments, having regard to one or two variables and the need to sequence tasks and tests, SESE: Science Curriculum page 79. This activity helps them understand fair testing by changing only one variable (i.e. shape only or length only) at a time. Investigating; experimenting; observing; analysing; measuring/timing; recording and communicating. CURRICULUM LINKS Mathematics Data / representing and interpreting data SESE: History Continuity and change over time/ technological and scientific developments over long periods BACKGROUND A previous activity on how things fall (i.e. the weight of the object is not a factor – Galileo and the Leaning Tower of Pisa) would help understanding of this activity, but not essential. MATERIALS/EQUIPMENT Paper, Ruler, Paper Clips, Scissors Templates of different sizes PREPARATION Test out a few thicknesses of paper/cardboard first to see that some of them spin. BACKGROUND The shape of the helicopter rotor blades make it spin INFORMATION when dropped from a height. Gravity pulls the helicopter down. The air resists the movement and pushes up each rotor separately, causing the helicopter to spin.
    [Show full text]
  • Over Thirty Years After the Wright Brothers
    ver thirty years after the Wright Brothers absolutely right in terms of a so-called “pure” helicop- attained powered, heavier-than-air, fixed-wing ter. However, the quest for speed in rotary-wing flight Oflight in the United States, Germany astounded drove designers to consider another option: the com- the world in 1936 with demonstrations of the vertical pound helicopter. flight capabilities of the side-by-side rotor Focke Fw 61, The definition of a “compound helicopter” is open to which eclipsed all previous attempts at controlled verti- debate (see sidebar). Although many contend that aug- cal flight. However, even its overall performance was mented forward propulsion is all that is necessary to modest, particularly with regards to forward speed. Even place a helicopter in the “compound” category, others after Igor Sikorsky perfected the now-classic configura- insist that it need only possess some form of augment- tion of a large single main rotor and a smaller anti- ed lift, or that it must have both. Focusing on what torque tail rotor a few years later, speed was still limited could be called “propulsive compounds,” the following in comparison to that of the helicopter’s fixed-wing pages provide a broad overview of the different helicop- brethren. Although Sikorsky’s basic design withstood ters that have been flown over the years with some sort the test of time and became the dominant helicopter of auxiliary propulsion unit: one or more propellers or configuration worldwide (approximately 95% today), jet engines. This survey also gives a brief look at the all helicopters currently in service suffer from one pri- ways in which different manufacturers have chosen to mary limitation: the inability to achieve forward speeds approach the problem of increased forward speed while much greater than 200 kt (230 mph).
    [Show full text]
  • Helicopter and Tiltrotor Noise Modeling Procedures Document
    ACRP Problem Statement: 89 Recommended Allocation: $250,000 Helicopter and Tiltrotor Noise Modeling Procedures Document Click here to see problem statement in IdeaHub: http://ideascale.com/t/UKsrZBVBS (Note: you must be a registered user in myACRP/IdeaHub.) TAGS: Airport Planning, Environment, Noise Impacts, Operations, Policy, Public Relations STAFF COMMENTS No comments. AVERAGE INDUSTRY RATING SUMMARY Committees1 Airport Community2 Achievable 3.00 3.50 Applicable 2.50 3.50 Implementable 2.00 3.50 Understandable 2.50 3.00 OVERALL 2.50 3.38 Notes: 1. Includes TRB aviation committees and committees from ACI-NA and AAAE. 2. Includes airport employees serving on active ACRP project panels. CLICK HERE TO SEE DETAILED INDUSTRY RATINGS CLICK HERE TO SEE DETAILED INDUSTRY COMMENTS ACRP OVERSIGHT COMMITTEE (AOC) DISPOSITION The average AOC rating among its voting members was 2.1 on a scale of 1 to 5. There was on discussion. The problem statement was not selected for ACRP funding and will be returned to the idea collection phase of ACRP’s IdeaHub. ACRP Problem Statement: 89 Helicopter and Tiltrotor Noise Modeling Procedures Document TAGS: Airport Planning, Environment, Noise Impacts, Operations, Policy, Public Relations OBJECTIVE The objective of this research effort is to develop written documentation on best available methods to model community noise generated from helicopter and tiltrotor operations. The document should address integrated and simulation modeling techniques, and methods for collecting and analyzing noise source data, and outline noise source development protocols. The language and format of the document shall be suitable for standards submission. BACKGROUND Existing noise modeling standards [SAE-AIR-1845; ICAO, Doc-29] for prediction of fixed wing community noise have been promulgated internationally and serve as the technical justification and defensible rationale upon which numerous noise models such as the Aviation Environmental Design Tool (AEDT) and the Integrated Noise Model (INM) rely.
    [Show full text]
  • Rotor Spring 2018
    Departments Features Index of Advertisers Spring 2018 rotor.org Serving the International BY THE INDUSTRY Helicopter Community FOR THE INDUSTRY Grand Canyon Helitack The Best Job in Aviation? What’s In Your Jet Fuel? p 58 Vietnam Pilots and Crew Members Honored p 28 Make the Connection March 4–7, 2019 • Atlanta Georgia World Congress Center Exhibits Open March 5–7 Apply for exhibit space at heliexpo.rotor.org LOTTERY 1* Open to HAI HELI-EXPO 2018 Exhibitors APPLY BY June 22, 2018 WITH PAYMENT LOTTERY 2 Open to All Companies APPLY BY Aug. 10, 2018 WITH PAYMENT heliexpo.rotor.org * For information on how to upgrade within Lottery 1, contact [email protected]. EXHIBIT NOW FALCON CREST AVIATION PROUDLY SUPPLIES & MAINTAINS AVIATION’S BEST SEALED LEAD ACID BATTERY RG-380E/44 RG-355 RG-214 RG-222 RG-390E RG-427 RG-407 RG-206 Bell Long Ranger Bell 212, 412, 412EP Bell 407 RG-222 (17 Ah) or RG-224 (24 Ah) RG-380E/44 (42 Ah) RG-407A1 (27 Ah) Falcon Crest STC No. SR09069RC Falcon Crest STC No. SR09053RC Falcon Crest STC No. SR09359RC Airbus Helicopters Bell 222U Airbus Helicopters AS355 E, F, F1, F2, N RG-380E/44 (42 Ah) BK 117, A-1, A-3, A-4, B-1, B-2, C-1 RG-355 (17 Ah) Falcon Crest STC No. SR09142RC RG-390E (28 Ah) Falcon Crest STC No. SR09186RC Falcon Crest STC No. SR09034RC Sikorsky S-76 A, C, C+ Airbus Helicopters RG-380E/44 (42 Ah) Airbus Helicopters AS350B, B1, B2, BA, C, D, D1 Falcon Crest STC No.
    [Show full text]
  • Helicopter Safety July-August 1991
    F L I G H T S A F E T Y F O U N D A T I O N HELICOPTER SAFETY Vol. 17 No. 4 For Everyone Concerned with the Safety of Flight July/August 1991 The Philosophy and Realities of Autorotations Like the power-off glide in a fixed-wing aircraft, the autorotation in a helicopter must be used properly if it is to be a successful safety maneuver. by Michael K. Hynes Aviation Consultant In all helicopter flying, there is no single event that has a In the early years of airplane flight, the fear of engine greater impact on safety than the autorotation maneuver. failure, or that the airplane might have structural prob- The mere mention of the word “autorotation” at any lems during flight, was very strong. If either of these gathering of helicopter pilots, especially flight instruc- events took place, the pilot’s ability to get the airplane tors, will guarantee a long and lively discussion. safely on the ground quickly was important. The time it took to get the airplane on the ground was directly in There are many misconceptions about autorotations and proportion to the altitude at which the airplane was being they contribute to the accident rate when an autorotation flown. It is therefore logical that all early flights were precedes a helicopter landing accident. One approach to flown at low altitudes, often at less than 500 feet above a discussion of autorotations is to look at the subject the ground (agl). from three views: first, the philosophy of the subject; second, the reality of the circumstances that require au- At these low altitudes, the pilot did not always have the torotations; and third, the execution of the maneuver.
    [Show full text]
  • DYNAMIC MODELING of AUTOROTATION for SIMULTANEOUS LIFT and WIND ENERGY EXTRACTION by SADAF MACKERTICH B.S. Rochester Institute O
    DYNAMIC MODELING OF AUTOROTATION FOR SIMULTANEOUS LIFT AND WIND ENERGY EXTRACTION by SADAF MACKERTICH B.S. Rochester Institute of Technology, 2012 A thesis submitted in partial fulfilment of the requirements for the degree of Master of Science in the Department of Mechanical and Aerospace Engineering in the College of Engineering and Computer Science at the University of Central Florida Orlando, Florida Spring Term 2016 Major Professor: Tuhin Das c 2016 Sadaf Mackertich ii ABSTRACT The goal of this thesis is to develop a multi-body dynamics model of autorotation with the objective of studying its application in energy harvesting. A rotor undergoing autorotation is termed an Autogyro. In the autorotation mode, the rotor is unpowered and its interaction with the wind causes an upward thrust force. The theory of an autorotating rotorcraft was originally studied for achieving safe flight at low speeds and later used for safe descent of helicopters under engine failure. The concept can potentially be used as a means to collect high-altitude wind energy. Autorotation is inherently a dynamic process and requires detailed models for characterization. Existing models of autorotation assume steady operating conditions with constant angu- lar velocity of the rotor. The models provide spatially averaged aerodynamic forces and torques. While these steady-autorotation models are used to create a basis for the dynamic model developed in this thesis, the latter uses a Lagrangian formulation to determine the equations of motion. The aerodynamic effects on the blades that produce thrust forces, in- plane torques, and out-of-plane torques, are modeled as non-conservative forces within the Lagrangian framework.
    [Show full text]