Performance. 12. Gliding Flight (Steady State)

Similar documents
Performance. 13. Climbing Flight

Performance. Power Plant Output in Terms of Thrust - General - Arbitrary Drag Polar

When the fluid velocity is zero, called the hydrostatic condition, the pressure variation is due only to the weight of the fluid.

Understanding Drag, Thrust, and Airspeed relationships

CHAPTER 7 CLIMB PERFORMANCE

AOE 3104 Aircraft Performance Problem Sheet 2 (ans) Find the Pressure ratio in a constant temperature atmosphere:

Gliding, Climbing, and Turning Flight Performance! Robert Stengel, Aircraft Flight Dynamics, MAE 331, 2014!

AIRCRAFT PERFORMANCE Pressure Altitude And Density Altitude

Lecture L5 - Other Coordinate Systems

Behavioral Animation Simulation of Flocking Birds

The aerodynamic center

Astromechanics Two-Body Problem (Cont)

WEIGHTLESS WONDER Reduced Gravity Flight

G U I D E T O A P P L I E D O R B I T A L M E C H A N I C S F O R K E R B A L S P A C E P R O G R A M

Mechanics 1: Conservation of Energy and Momentum

AE Stability and Control of Aerospace Vehicles

NIFA NATIONAL SAFECON

Exam questions for obtaining aircraft licenses and ratings

Flight path optimization for an airplane

Free fall from SPACE!

Flight Operations Briefing Notes

Lecture L14 - Variable Mass Systems: The Rocket Equation

Chapter 4 Atmospheric Pressure and Wind

Section 4: The Basics of Satellite Orbits

Project: OUTFIELD FENCES

Cessna Skyhawk II / 100. Performance Assessment

Physics of the Atmosphere I

Flight Safety Foundation. Approach-and-landing Accident Reduction. Tool Kit. FSF ALAR Briefing Note 4.2 Energy Management

SIX DEGREE-OF-FREEDOM MODELING OF AN UNINHABITED AERIAL VEHICLE. A thesis presented to. the faculty of

Lecture L6 - Intrinsic Coordinates

TOTAL ENERGY COMPENSATION IN PRACTICE

DIRECCION DE PERSONAL AERONAUTICO DPTO. DE INSTRUCCION PREGUNTAS Y OPCIONES POR TEMA

Chapter 3: Weather Map. Weather Maps. The Station Model. Weather Map on 7/7/2005 4/29/2011

Differential Relations for Fluid Flow. Acceleration field of a fluid. The differential equation of mass conservation

Aircraft Trajectory Optimization. Aircraft Trajectory Optimization. Motivation. Motivation

In order to describe motion you need to describe the following properties.

Lecture L2 - Degrees of Freedom and Constraints, Rectilinear Motion

Turbulence: The Invisible Hazard presented by Scott Miller PIA Symposium 2005 Jacksonville, Florida, USA

5. Forces and Motion-I. Force is an interaction that causes the acceleration of a body. A vector quantity.

Turn off all electronic devices

APPENDIX 3-B Airplane Upset Recovery Briefing. Briefing. Figure 3-B.1

State Newton's second law of motion for a particle, defining carefully each term used.

Shear Force and Moment Diagrams

Aerospace Engineering 3521: Flight Dynamics. Prof. Eric Feron Homework 6 due October 20, 2014

Projectile motion simulator.

Chapter 3: Weather Map. Station Model and Weather Maps Pressure as a Vertical Coordinate Constant Pressure Maps Cross Sections

Newton s Law of Gravity

Lecture L9 - Linear Impulse and Momentum. Collisions

Lab 8 Notes Basic Aircraft Design Rules 6 Apr 06

Propeller Efficiency. Rule of Thumb. David F. Rogers, PhD, ATP

Certification Specifications for Large Rotorcraft CS-29

This file contains the full script of the corresponding video, published on YouTube. November 2014:

Flight crew awareness and alertness are key factors in the

Chapter 10: Linear Kinematics of Human Movement

Dipl. Ing. Falk Pätzold Technische Universität Braunschweig, Institut für Flugführung February 21 st 2014

SIMPLIFIED METHOD FOR ESTIMATING THE FLIGHT PERFORMANCE OF A HOBBY ROCKET

Acceleration Introduction: Objectives: Methods:

oil liquid water water liquid Answer, Key Homework 2 David McIntyre 1

Introduction to Flight

Uniformly Accelerated Motion

Solutions to Homework 5

Torque Analyses of a Sliding Ladder

In-flight Evaluation of Avionic Systems

Trigonometry Hard Problems

Air Data Computers. The Beginning

CHAPTER 6 WORK AND ENERGY

Journal of Engineering Science and Technology Review 2 (1) (2009) Lecture Note

Exam 1 Review Questions PHY Exam 1

Temperature. PJ Brucat

Flightlab Ground School 5. Longitudinal Static Stability

FUNDAMENTALS OF ENGINEERING THERMODYNAMICS

Lecture L29-3D Rigid Body Dynamics

Preliminary Analysis of an Aircraft Capable of Deploying and Retracting a

39th International Physics Olympiad - Hanoi - Vietnam Theoretical Problem No. 3

ACCELERATION OF HEAVY TRUCKS Woodrow M. Poplin, P.E.

Worksheet to Review Vector and Scalar Properties

Lecture L17 - Orbit Transfers and Interplanetary Trajectories

ESTIMATING R/C MODEL AERODYNAMICS AND PERFORMANCE

OPERATING MINIMA FOR AEROPLANES AND HELICOPTER OPERATIONS PURPOSE REFERENCE 4.0 DEFINITION

Rotation: Moment of Inertia and Torque

1 of 7 9/5/2009 6:12 PM

Penn State University Physics 211 ORBITAL MECHANICS 1

Section 10.4 Vectors

2 Newton s First Law of Motion Inertia

2008 FXA DERIVING THE EQUATIONS OF MOTION 1. Candidates should be able to :

Fundamentals of Airplane Flight Mechanics

Fluid Dynamics Basics

UAS Control From a Moving Platform - A Preliminary Simulator Study

THE FLIGHT COMPUTER TRUE AIRSPEED (TAS)

Lecture 3 Fluid Dynamics and Balance Equa6ons for Reac6ng Flows

Fluid Mechanics Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

General aviation & Business System Level Applications and Requirements Electrical Technologies for the Aviation of the Future Europe-Japan Symposium

Chapter 15 Collision Theory

Chapter 11 Equilibrium

W i f(x i ) x. i=1. f(x i ) x = i=1

3. FLYING TECHNIQUES. 3.1 Speed Management. 3.2 Attitude Management. 3.3 Height Management. 3.4 Transit Flying

= 800 kg/m 3 (note that old units cancel out) J 1000 g = 4184 J/kg o C

Lecture L22-2D Rigid Body Dynamics: Work and Energy

Chapter 28 Fluid Dynamics

Transcription:

Performance 12. Gliding Flight (Steady State) If the engine is turned off, (T = 0), and one desires to maintain airspeed, it is necessary to put the vehicle at such an attitude that the component of the gravity force in the direction of the velcocity vector balances the drag. The equations of motion are given by: (1) where is the flight path angle (the angle the velocity makes with the horizontal). If we divide one equation by the other, we get: (2) We see from Eq. (2) that the flight path angle is negative, as expected! We can then define the glide angle as the negative of the flight path angle and write: where 1 = glide angle (and is positive). We can observe the following: 1) the glide angle depends only on L/D and is independent of the weight of the vehicle!, 2) the flattest glide angle occurs at the maximum L/D. Glide Range The glide range is how far it travels along the ground during the glide descent. It is easy to see from the figure that (3) or 1

(4) Hence the range for gliding flight depends on the L/D and h. It is clear that the maximum range occurs when L/D is maximum. Therefore the maximum range glide is flown at the minimum drag airspeed, V md. Small Glide Angle Assumption In most cases, the glide angle will be small for an equilibrium glide. Under these circumstances, we can make the following approximations : The most important result of this assumption is that we can make the approximation that (5) Hence we can use the weight in order to compute the airspeed. Without this assumption the calculations can become more difficult. Rate of Climb (Sink) The rate of climb is given by (6) From Eq. (1) we can eliminate to get or (7) 2

We can note the rate of climb is negative (hence a sink rate), and that it is directly related to the quantity. Therefore, if we want to minimize the sink rate, we must minimize the quantity. Recall, however that this is the same requirement that we had for minimizing the power required. Note that if we minimize the sink rate, we maximize the time to descend or maximize the time aloft, or endurance. Summary 1) For maximum range, we must operate at the maximum L/D condition (minimum drag) 2) For maximum endurance (minimum sink rate) we must operate at the minimum power require condition. Time to descend From Eq. (7) we can see that the rate of descent depends on the altitude (through the density,,). So to get an exact solution for the time to descend we would need to include density variations in our calculations. However, if the change in altitude is relatively small (whatever that means?) we can approximate the time to descend by assuming the density is constant and, in addition, assume we fly at constant angle-of-attack (constant C L and C D ). Under these circumstances and assumptions the rate of descent is constant. Thus we have: where is assumed constant. Generally the value of used is that calculated for an altitude halfway between the initial and final altitudes. If large altitude changes are involved, the above equation can be used for several smaller increments in altitude and the results summed. Example: A sailplane weighs 1000 lbs with a wing loading W/S = 12.5 lbs/ft 2. The drag polar is given by C L = 0.010 + 0.022 C L2. Find the time to glide from 1000 ft to sea-level flying at minimum sink rate conditions. Minimum sink rate occurs at the minimum power required flight condition. (8) 3

Note that L/D) max = 33.7 Therangeoftheglideis: Example Consider our executive jet that has a weight of 10,000 lbs, a wing area of 200 ft 2, and a parabolic drag polar. We would like to calculate the glide range and endurance from 20,000 ft. We would like to compare the range and endurance for a max range flight condition with that for a max endurance flight condtion. Max Range Flight Condition The max range condition occurs at max L/D or the min drag condition: and 4

Range (max) The endurance for this flight is given by:, where (Couldalsouse ) then (Endurance for max range conditions) Max Endurance Flight Condition Maximum endurance glide occurs at the minimum power required flight condition. (Less than L/D max ) Range: Glide range: Endurance; 5

Summary: Flight condition Max Range Max Endurance Range 59.9 mi 51.87 mi Endurance (TOF) 17.55 min 20.0 min As expected, max range conditions give biggest range, and max endurance conditions give max TOF. In addition we could have selected a specified L/D. For the case of L/D = 10 we obtain the following results: L/D = 10, Range = 37.88 mi Endurance: TOF 1 = 6.63 min, or TOF 2 = 18.60 min Note that there are two flight conditions at L/D = 10! The range is the same, but the endurance is not. An Exact Solution for Glide Endurance It turns out that we can get an exact solution for the glide time if we assume a standard atmosphere. The equation we developed for sink rate is: Or In the troposphere: where is the temperature gradient in the troposphere, and R is the gas constant. If we integrate the time equation above from altitude to sea-level, we get: 6

(9) If we substitute minimum power conditions into Eq. (9), with h = 20,000 ft, for the same aircraft as in the example problems, we get the time of flight, TOF = 20.0 min! For other altitudes to sea-level: h(ft) 0 5K 10K 15K 20K 25K 30K 35K 40K TOF(sec) 0 337 649 938 1203 1448 1671 1875 2061 7