Tutorial Questions with Solutions Flight Mechanics
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Sept. 12, 1950 W
Sept. 12, 1950 W. ANGST 2,522,337 MACH METER Filed Dec. 9, 1944 2 Sheets-Sheet. INVENTOR. M/2 2.7aar alwg,57. A77OAMA). Sept. 12, 1950 W. ANGST 2,522,337 MACH METER Filed Dec. 9, 1944 2. Sheets-Sheet 2 N 2 2 %/ NYSASSESSN S2,222,W N N22N \ As I, mtRumaIII-m- III It's EARAs i RNSITIE, 2 72/ INVENTOR, M247 aeawosz. "/m2.ATTORNEY. Patented Sept. 12, 1950 2,522,337 UNITED STATES ; :PATENT OFFICE 2,522,337 MACH METER Walter Angst, Manhasset, N. Y., assignor to Square D Company, Detroit, Mich., a corpora tion of Michigan Application December 9, 1944, Serial No. 567,431 3 Claims. (Cl. 73-182). is 2 This invention relates to a Mach meter for air plurality of posts 8. Upon one of the posts 8 are craft for indicating the ratio of the true airspeed mounted a pair of serially connected aneroid cap of the craft to the speed of sound in the medium sules 9 and upon another of the posts 8 is in which the aircraft is traveling and the object mounted a diaphragm capsuler it. The aneroid of the invention is the provision of an instrument s: capsules 9 are sealed and the interior of the cas-l of this type for indicating the Mach number of an . ing is placed in communication with the static aircraft in fight. opening of a Pitot static tube through an opening The maximum safe Mach number of any air in the casing, not shown. The interior of the dia craft is the value of the ratio of true airspeed to phragm capsule is connected through the tub the speed of sound at which the laminar flow of ing 2 to the Pitot or pressure opening of the Pitot air over the wings fails and shock Waves are en static tube through the opening 3 in the back countered. -
E6bmanual2016.Pdf
® Electronic Flight Computer SPORTY’S E6B ELECTRONIC FLIGHT COMPUTER Sporty’s E6B Flight Computer is designed to perform 24 aviation functions and 20 standard conversions, and includes timer and clock functions. We hope that you enjoy your E6B Flight Computer. Its use has been made easy through direct path menu selection and calculation prompting. As you will soon learn, Sporty’s E6B is one of the most useful and versatile of all aviation computers. Copyright © 2016 by Sportsman’s Market, Inc. Version 13.16A page: 1 CONTENTS BEFORE USING YOUR E6B ...................................................... 3 DISPLAY SCREEN .................................................................... 4 PROMPTS AND LABELS ........................................................... 5 SPECIAL FUNCTION KEYS ....................................................... 7 FUNCTION MENU KEYS ........................................................... 8 ARITHMETIC FUNCTIONS ........................................................ 9 AVIATION FUNCTIONS ............................................................. 9 CONVERSIONS ....................................................................... 10 CLOCK FUNCTION .................................................................. 12 ADDING AND SUBTRACTING TIME ....................................... 13 TIMER FUNCTION ................................................................... 14 HEADING AND GROUND SPEED ........................................... 15 PRESSURE AND DENSITY ALTITUDE ................................... -
Circular Motion Dynamics
Problem Solving Circular Motion Dynamics Problem 1: Double Star System Consider a double star system under the influence of gravitational force between the stars. Star 1 has mass m1 and star 2 has mass m2 . Assume that each star undergoes uniform circular motion about the center of mass of the system. If the stars are always a fixed distance s apart, what is the period of the orbit? Solution: Choose radial coordinates for each star with origin at center of mass. Let rˆ1 be a unit vector at Star 1 pointing radially away from the center of mass. Let rˆ2 be a unit vector at Star 2 pointing radially away from the center of mass. The force diagrams on the two stars are shown in the figure below. ! ! From Newton’s Second Law, F1 = m 1a 1 , for Star 1 in the radial direction is m m ˆ 1 2 2 r1 : "G 2 = "m1 r 1 ! . s We can solve this for r1 , m r = G 2 . 1 ! 2s 2 ! ! Newton’s Second Law, F2 = m 2a 2 , for Star 2 in the radial direction is m m ˆ 1 2 2 r2 : "G 2 = "m2 r 2 ! . s We can solve this for r2 , m r = G 1 . 2 ! 2s 2 Since s , the distance between the stars, is constant m2 m1 (m2 + m1 ) s = r + r = G + G = G 1 2 ! 2s 2! 2s 2 ! 2s 2 . Thus the angular velocity is 1 2 " (m2 + m1 ) # ! = $G 3 % & s ' and the period is then 1 2 2! # 4! 2s 3 $ T = = % & . -
Assignment 2 Centripetal Force & Univ
LAST NAME______________________________ FIRST NAME_____________________DATE______ CJ - Assignment 2 Centripetal Force & Universal Gravitation, 5.4 Banked Curves Draw the vectors for a free body diagram of a car in an unbanked turn and a banked turn. For this situation assume the cars are turning to the left side of the drawing. Car in Unbanked Turn Car in Banked turn Is this car in Equilibrium? Is this car in Equilibrium? Do the same for the airplane. Airplane in Unbanked Turn Airplane in Banked turn Let’s be careful to fully understand what is going on with this one. We have made an assumption in doing this for the airplane which are not valid. THE BANKED TURN- car can make it a round a turn even if friction is not present (or friction is zero). In order for this to happen the curved road must be “banked”. In a non-banked turn the centripetal force is created by the friction of the road on the tires. What creates the centripetal force in a banked turn? Imagine looking at a banked turn as shown to the right. Draw the forces that act on the car on the diagram of the car. Is the car in Equilibrium? YES , NO The car which has a mass of m is travelling at a velocity (or speed) v around a turn of radius r. How do these variables relate to optimize the banked turn. If the mass of the car is greater is a larger or smaller angle required? LARGER, SMALLER, NO CHANGE NECESSARY If the VELOCITY of the car is greater is a larger or smaller angle required? LARGER, SMALLER, NO CHANGE NECESSARY If the RADUS OF THE TURN is greater is a larger or smaller angle required? LARGER, SMALLER, NO CHANGE NECESSARY To properly show the relationship an equation must be created. -
Air Data Computer 8EB3AAA1 DESCRIPTION AMETEK Has Designed a Compact, Solid State Air Data Computer for Military Applications
Air Data Computer 8EB3AAA1 DESCRIPTION AMETEK has designed a compact, solid state Air Data Computer for military applications. The Air Data Computer utilizes a digital signal processor for fast calculation and response of air data parameters. Silicon pressure transducers provide the static and Pitot pressure values and are easily replaced without calibration. The AMETEK Air Data Computer incorporates a unique power supply that allows the unit to operate through 5 second power interrupts when at any input voltage in its operating range. This ensures that critical air data parameters reach the cockpit and control systems under a FEATURES wide variety of conditions. 3 The MIL-STD-1553 interface 40 ms update rate Thirteen (13) different air data parameters are provided on the MIL-STD- 3 11-bit reported pressure 1553B interface and are calculated by the internal processor at a 40 ms rate. altitude interface 3 AOA and total temperature An 11-bit reported pressure altitude interface encoded per FAA order inputs 1010.51A is available for Identification Friend or Foe equipment. 3 Low weight: 2.29 lbs. 3 Small size: 6.81” x 6.0” x 2.5” 3 Low power: 1.5 watts 3 DO-178B level A software AEROSPACE & DEFENSE Air Data Computer 8EB3AAA1 SPECIFICATIONS PERFORMANCE CHARACTERISTICS Air Data Parameters Power: DO-160, Section 16 Cat Z or MIL-STD-704A-F • ADC Altitude Rate Output (Hpp or dHp/dt) 5 second power Interruption immunity at any • True Airspeed Output (Vt) input voltage • Calibrated Airspeed Output (Vc) Power Consumption: 1.5 watts • Indicated Airspeed Output (IAS) Operating Temperature: -55°C to +71°C; 1/2 hour at +90°C • Mach Number Output (Mt) Weight: 2.29 lbs. -
16.00 Introduction to Aerospace and Design Problem Set #3 AIRCRAFT
16.00 Introduction to Aerospace and Design Problem Set #3 AIRCRAFT PERFORMANCE FLIGHT SIMULATION LAB Note: You may work with one partner while actually flying the flight simulator and collecting data. Your write-up must be done individually. You can do this problem set at home or using one of the simulator computers. There are only a few simulator computers in the lab area, so not leave this problem to the last minute. To save time, please read through this handout completely before coming to the lab to fly the simulator. Objectives At the end of this problem set, you should be able to: • Take off and fly basic maneuvers using the flight simulator, and describe the relationships between the control yoke and the control surface movements on the aircraft. • Describe pitch - airspeed - vertical speed relationships in gliding performance. • Explain the difference between indicated and true airspeed. • Record and plot airspeed and vertical speed data from steady-state flight conditions. • Derive lift and drag coefficients based on empirical aircraft performance data. Discussion In this lab exercise, you will use Microsoft Flight Simulator 2000/2002 to become more familiar with aircraft control and performance. Also, you will use the flight simulator to collect aircraft performance data just as it is done for a real aircraft. From your data you will be able to deduce performance parameters such as the parasite drag coefficient and L/D ratio. Aircraft performance depends on the interplay of several variables: airspeed, power setting from the engine, pitch angle, vertical speed, angle of attack, and flight path angle. -
April 2018 the Privileged View Steve Beste, President
Volume 18 – 04 www.FlyingClub1.org April 2018 The Privileged View Steve Beste, President Maker Faire. When something breaks, who you gonna call? If it’s your car or your Cessna, you put it into the shop and get out your checkbook. But if you fly an experimental or Part 103 aircraft, it’s not so simple. That’s why - when newbies ask me about our sport - I find out if they’re tinkerers and do-it-yourselfers. If all they bring to a problem is their checkbook, then they’re better off going with the Cessna. The tinkerers and builders, though, they’re my kind of people. That’s why I went with Dick Martin to the annual Maker Faire at George Mason in mid-March. I thought we’d find a modest event that focused on 3D printing for adult hobbyists, but I was so wrong. They had 140 exhibitors filling three buildings. With several thousand visitors, there were lines outside the buildings by mid-afternoon. Yes, they had 3D printers, but so much more. And so many kids! The focus of the event was clearly on bringing young people into the world of making stuff. The cleverest exhibit was the one shown below. They set up four tables with junk computer gear and told kids to just take things apart. Don’t worry about putting anything back together again. It’s all junk! Rip it apart! See how it’s made! Do it! It looked like a destruction derby, with laptops and printers and even a sewing machine being reduced to screws and plates. -
Joint Aviation Requirements JAR–FCL 1 ЛИЦЕНЗИРОВАНИЕ ЛЕТНЫХ ЭКИПАЖЕЙ (САМОЛЕТЫ)
Joint Aviation Requirements JAR–FCL 1 ЛИЦЕНЗИРОВАНИЕ ЛЕТНЫХ ЭКИПАЖЕЙ (САМОЛЕТЫ) Joint Aviation Authorities 1 JAR-FCL 1 ЛИЦЕНЗИРОВАНИЕ ЛЕТНЫХ ЭКИПАЖЕЙ (САМОЛЕТЫ) Издано 14 февраля 1997 года ПРЕДИСЛОВИЕ ПРЕАМБУЛА ЧАСТЬ 1 - ТРЕБОВАНИЯ ПОДЧАСТЬ A – ОБЩИЕ ТРЕБОВАНИЯ JAR-FCL 1.001 Определения и Сокращения JAR-FCL 1.005 Применимость JAR-FCL 1.010 Основные полномочия членов летного экипажа JAR-FCL 1.015 Признание свидетельств, допусков, разрешений, одобрений или сер- тификатов JAR-FCL 1.016 Кредит, предоставляемый владельцу свидетельства, полученного в государстве не члене JAA JAR-FCL 1.017 Разрешения/квалификационные допуски для специальных целей JAR-FCL 1.020 Учет военной службы JAR-FCL 1.025 Действительность свидетельств и квалификационных допусков JAR-FCL 1.026 Свежий опыт для пилотов, не выполняющих полеты в соответствии с JAR-OPS 1 JAR-FCL 1.030 Порядок тестирования JAR-FCL 1.035 Годность по состоянию здоровья JAR-FCL 1.040 Ухудшение состояния здоровья JAR-FCL 1.045 Особые обстоятельства JAR-FCL 1.050 Кредитование летного времени и теоретических знаний JAR-FCL 1.055 Организации и зарегистрированные предприятия JAR-FCL 1.060 Ограничение прав владельцев свидетельств, достигших 60-летнего возраста и более JAR-FCL 1.065 Государство выдачи свидетельства 2 JAR-FCL 1.070 Место обычного проживания JAR-FCL 1.075 Формат и спецификации свидетельств членов летных экипажей JAR-FCL 1.080 Учет летного времени Приложение 1 к JAR-FCL 1.005 Минимальные требования для выдачи свиде- тельства/разрешения JAR-FCL на основе нацио- нального свидетельства/разрешения, выданного в государстве-члене JAA. Приложение 1 к JAR-FCL 1.015 Минимальные требования для признания дейст- вительности свидетельств пилотов, выданных государствами не членами JAA. -
Digital Air Data Computer Type Ac32
DIGITAL AIR DATA COMPUTER TYPE AC32 GENERAL THOMMEN is a leading manufacturer of Air Data Systems It also supports the Air Data for enhanced safety and aircraft instruments used worldwide on a full range infrastructure capabilities for Transponders and an ICAO aircraft types from helicopters to corporate turbine aircraft encoded altitude output is also available as an option. and commercial airliners. The AC32 measures barometric altitude, airspeed and temperature in the atmosphere with Its power supply is designed for 28 VDC. The low power integrated vibrating cylinder pressure sensors with high consumption of less than 7 Watts and its low weight of only accuracy and stability for both static and pitot ports. 2.2 Ibs (1000 grams) have been optimized for applications in state-of-the-art avionics suites. The extensive Built-in-Test The THOMMEN AC32 Digital Air Data Computer exceeds FAA capability guarantees safe operation. Technical Standard Order (TSO) and accuracy requirements. The computed air data parameters are transmitted via the The AC32 is designed to be modular which allows easy configurable ARINC 429 data bus. There are two ARINC 429 maintenance by the operator thanks to the RS232 transmit channels and two receive channels with which baro maintenance interface. The THOMMEN AC32 can be confi correction can be accomplished also. gured for different applications and has excellent hosting capabilities for supplying data to next generation equipment The AC32 meets the requirements for multiple platforms for without altering the system architecture. TAWS, ACAS/TCAS, EGPWS or FMS systems. For customized versions please contact THOMMEN AIRCRAFT EQUIPMENT AG sales department. -
Introduction
CHAPTER 1 Introduction "For some years I have been afflicted with the belief that flight is possible to man." Wilbur Wright, May 13, 1900 1.1 ATMOSPHERIC FLIGHT MECHANICS Atmospheric flight mechanics is a broad heading that encompasses three major disciplines; namely, performance, flight dynamics, and aeroelasticity. In the past each of these subjects was treated independently of the others. However, because of the structural flexibility of modern airplanes, the interplay among the disciplines no longer can be ignored. For example, if the flight loads cause significant structural deformation of the aircraft, one can expect changes in the airplane's aerodynamic and stability characteristics that will influence its performance and dynamic behavior. Airplane performance deals with the determination of performance character- istics such as range, endurance, rate of climb, and takeoff and landing distance as well as flight path optimization. To evaluate these performance characteristics, one normally treats the airplane as a point mass acted on by gravity, lift, drag, and thrust. The accuracy of the performance calculations depends on how accurately the lift, drag, and thrust can be determined. Flight dynamics is concerned with the motion of an airplane due to internally or externally generated disturbances. We particularly are interested in the vehicle's stability and control capabilities. To describe adequately the rigid-body motion of an airplane one needs to consider the complete equations of motion with six degrees of freedom. Again, this will require accurate estimates of the aerodynamic forces and moments acting on the airplane. The final subject included under the heading of atmospheric flight mechanics is aeroelasticity. -
Volume 2 – General Navigation (JAR Ref 061) Table of Contents
Volume 2 – General Navigation (JAR Ref 061) Table of Contents CHAPTER 1 The Form of the Earth Shape of the Earth ........................................................................................................................................1-1 The Poles......................................................................................................................................................1-2 East and West...............................................................................................................................................1-2 North Pole and South Pole ...........................................................................................................................1-2 Cardinal Directions........................................................................................................................................1-3 Great Circle...................................................................................................................................................1-3 Vertex of a Great Circle ................................................................................................................................1-4 Small Circle...................................................................................................................................................1-5 The Equator ..................................................................................................................................................1-5 Meridians ......................................................................................................................................................1-6 -
Unusual Attitudes and the Aerodynamics of Maneuvering Flight Author’S Note to Flightlab Students
Unusual Attitudes and the Aerodynamics of Maneuvering Flight Author’s Note to Flightlab Students The collection of documents assembled here, under the general title “Unusual Attitudes and the Aerodynamics of Maneuvering Flight,” covers a lot of ground. That’s because unusual-attitude training is the perfect occasion for aerodynamics training, and in turn depends on aerodynamics training for success. I don’t expect a pilot new to the subject to absorb everything here in one gulp. That’s not necessary; in fact, it would be beyond the call of duty for most—aspiring test pilots aside. But do give the contents a quick initial pass, if only to get the measure of what’s available and how it’s organized. Your flights will be more productive if you know where to go in the texts for additional background. Before we fly together, I suggest that you read the section called “Axes and Derivatives.” This will introduce you to the concept of the velocity vector and to the basic aircraft response modes. If you pick up a head of steam, go on to read “Two-Dimensional Aerodynamics.” This is mostly about how pressure patterns form over the surface of a wing during the generation of lift, and begins to suggest how changes in those patterns, visible to us through our wing tufts, affect control. If you catch any typos, or statements that you think are either unclear or simply preposterous, please let me know. Thanks. Bill Crawford ii Bill Crawford: WWW.FLIGHTLAB.NET Unusual Attitudes and the Aerodynamics of Maneuvering Flight © Flight Emergency & Advanced Maneuvers Training, Inc.