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

Similar documents
CHAPTER 7 CLIMB PERFORMANCE

Performance. 13. Climbing Flight

TOP VIEW. FBD s TOP VIEW. Examination No. 2 PROBLEM NO. 1. Given:

C B A T 3 T 2 T What is the magnitude of the force T 1? A) 37.5 N B) 75.0 N C) 113 N D) 157 N E) 192 N

Understanding Drag, Thrust, and Airspeed relationships

AE Stability and Control of Aerospace Vehicles

Displacement (x) Velocity (v) Acceleration (a) x = f(t) differentiate v = dx Acceleration Velocity (v) Displacement x

Cessna Skyhawk II / 100. Performance Assessment

Chapter 4. Forces and Newton s Laws of Motion. continued

Behavioral Animation Simulation of Flocking Birds

APP Aircraft Performance Program Demo Notes Using Cessna 172 as an Example

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

Lecture L5 - Other Coordinate Systems

Work, Power, Energy Multiple Choice. PSI Physics. Multiple Choice Questions

Aircraft Trajectory Optimization. Aircraft Trajectory Optimization. Motivation. Motivation

Lab 8 Notes Basic Aircraft Design Rules 6 Apr 06

SIMPLIFIED METHOD FOR ESTIMATING THE FLIGHT PERFORMANCE OF A HOBBY ROCKET

Lecture L14 - Variable Mass Systems: The Rocket Equation

The aerodynamic center

Problem Set 5 Work and Kinetic Energy Solutions

VELOCITY, ACCELERATION, FORCE

Lecture 8 : Dynamic Stability

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

WEIGHTLESS WONDER Reduced Gravity Flight

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

Introduction to Flight

EDUH SPORTS MECHANICS

Wing Design: Major Decisions. Wing Area / Wing Loading Span / Aspect Ratio Planform Shape Airfoils Flaps and Other High Lift Devices Twist

Lecture L9 - Linear Impulse and Momentum. Collisions

NIFA NATIONAL SAFECON

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

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

JET ENGINE PERFORMANCE. Charles Robert O Neill. School of Mechanical and Aerospace Engineering. Oklahoma State University. Stillwater, OK 74078

HW Set II page 1 of 9 PHYSICS 1401 (1) homework solutions

Uniform Circular Motion III. Homework: Assignment (1-35) Read 5.4, Do CONCEPT QUEST #(8), Do PROBS (20, 21) Ch. 5 + AP 1997 #2 (handout)

Notice numbers may change randomly in your assignments and you may have to recalculate solutions for your specific case.

Ch 7 Kinetic Energy and Work. Question: 7 Problems: 3, 7, 11, 17, 23, 27, 35, 37, 41, 43

Work. Work = Force x parallel distance (parallel component of displacement) F v

Chapter 6. Work and Energy

WORK DONE BY A CONSTANT FORCE

Projectile motion simulator.

There are four types of friction, they are 1).Static friction 2) Dynamic friction 3) Sliding friction 4) Rolling friction

Chapter 9. particle is increased.

Difference between a vector and a scalar quantity. N or 90 o. S or 270 o

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

HSC Mathematics - Extension 1. Workshop E4

Physics 1A Lecture 10C

Computational Aerodynamic Analysis on Store Separation from Aircraft using Pylon

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

Lesson 3 - Understanding Energy (with a Pendulum)

Forces on the Rocket. Rocket Dynamics. Equation of Motion: F = Ma

8. Potential Energy and Conservation of Energy Potential Energy: When an object has potential to have work done on it, it is said to have potential

v v ax v a x a v a v = = = Since F = ma, it follows that a = F/m. The mass of the arrow is unchanged, and ( )

SOLUTIONS TO CONCEPTS CHAPTER 15

Mechanics 1: Conservation of Energy and Momentum

Chapter 11. h = 5m. = mgh mv Iω 2. E f. = E i. v = 4 3 g(h h) = m / s2 (8m 5m) = 6.26m / s. ω = v r = 6.

Problem 15.1 In Active Example 15.1, what is the velocity of the container when it has reached the position s = 2m?

CHAPTER 15 FORCE, MASS AND ACCELERATION

PHY231 Section 1, Form B March 22, 2012

Physics 590 Homework, Week 6 Week 6, Homework 1

Lesson 11. Luis Anchordoqui. Physics 168. Tuesday, December 8, 15

Summary of Aerodynamics A Formulas

Physics 201 Homework 8

1. Mass, Force and Gravity

Midterm Solutions. mvr = ω f (I wheel + I bullet ) = ω f 2 MR2 + mr 2 ) ω f = v R. 1 + M 2m

WORKSHEET: KINETIC AND POTENTIAL ENERGY PROBLEMS

Lift and Drag on an Airfoil ME 123: Mechanical Engineering Laboratory II: Fluids

Chapter 6 Work and Energy

F f v 1 = c100(10 3 ) m h da 1h 3600 s b =

Newton s Laws of Motion

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

AIRCRAFT PERFORMANCE Pressure Altitude And Density Altitude

Here the units used are radians and sin x = sin(x radians). Recall that sin x and cos x are defined and continuous everywhere and

AIRCRAFT GENERAL GTM CONTENTS

while the force of kinetic friction is fk = µ

Project: OUTFIELD FENCES

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

CHAPTER 6 WORK AND ENERGY

Work Energy & Power. September 2000 Number Work If a force acts on a body and causes it to move, then the force is doing work.

Exam questions for obtaining aircraft licenses and ratings

AP1 Oscillations. 1. Which of the following statements about a spring-block oscillator in simple harmonic motion about its equilibrium point is false?

Physics 1120: Simple Harmonic Motion Solutions

NIFA REGIONAL SAFECON 2006 Manual Flight Computer Accuracy Explanations

AP Calculus AB 2003 Scoring Guidelines

Introduction and Mathematical Concepts

PHY231 Section 2, Form A March 22, Which one of the following statements concerning kinetic energy is true?

Physics Notes Class 11 CHAPTER 6 WORK, ENERGY AND POWER

TOTAL ENERGY COMPENSATION IN PRACTICE

AP Calculus AB 2006 Scoring Guidelines

Chapter 8: Potential Energy and Conservation of Energy. Work and kinetic energy are energies of motion.

AP Physics C. Oscillations/SHM Review Packet

Recitation Week 4 Chapter 5

Flight path optimization for an airplane

Solution Derivations for Capa #11

FRICTION, WORK, AND THE INCLINED PLANE

APPLIED MATHEMATICS ADVANCED LEVEL

Parachute Jumping, Falling, and Landing David C. Arney, Barbra S. Melendez, Debra Schnelle 1

Simple Harmonic Motion(SHM) Period and Frequency. Period and Frequency. Cosines and Sines

AP PHYSICS C Mechanics - SUMMER ASSIGNMENT FOR

Transcription:

Gliding, Climbing, and Turning Flight Performance! Robert Stengel, Aircraft Flight Dynamics, MAE 331, 2014! Learning Objectives! Conditions for gliding flight" Parameters for maximizing climb angle and rate" Review the V-n diagram" Energy height and specific excess power" Alternative expressions for steady turning flight" The Herbst maneuver! Reading:! Flight Dynamics! Aerodynamic Coefficients, 130-141! Copyright 2014 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! Gliding Flight! 2!

Equilibrium Gliding Flight" D C D 1 2!V 2 S " sin# 1 2!V 2 S cos#!h V sin#!r V cos# 3! Gliding Flight" Thrust 0" Flight path angle < 0 in gliding flight" Altitude is decreasing" Airspeed ~ constant" Air density ~ constant " Gliding flight path angle " tan! " D L " C D h!!r dh dr ;! # D "tan"1 % $ L Corresponding airspeed " & # L & ( "cot "1 % ( ' $ D ' V glide 2!S C D 2 + 2 4!

Maximum Steady Gliding Range" Glide range is maximum when! is least negative, i.e., most positive" This occurs at (L/D) max " 5! Maximum Steady Gliding Range" Glide range is maximum when! is least negative, i.e., most positive" This occurs at (L/D) max " # D &! max "tan "1 % ( $ L ' min # L & "cot "1 % ( $ D ' max h tan!!!r negative constant h " h o r " r o #r #h tan! "#h "tan! maximum when L D maximum 6!

Sink Rate, m/s " Lift and drag define! and V in gliding equilibrium" D C D 1 2!V 2 S " sin# sin# " D!h V sin! L 1 2!V 2 S cos" V 2 cos"!s Sink rate altitude rate, dh/dt (negative)" " 2 cos! #S $ D ' & ) " % ( 2 cos! #S $ L & % ' ( ) $ D ' & % L ) ( " 2 cos! #S cos! $ 1 ' & ) % L D ( 7! Conditions for Minimum Steady Sink Rate" Minimum sink rate provides maximum endurance" Minimize sink rate by setting "(dh/dt)/" 0 (cos! ~1)"!h! 2 cos" #S! 2 cos3 " $ & #S % cos" $ C ' D & ) % ( C D 3/2 ' ) *! 2 $ & ( # % S ' $ )& (% C D 3/2 ' ) ( ME 3C D o! and C DME 4C Do 8!

L/D and V ME for Minimum Sink Rate" ( L D ) 1 ME 4 3 3!C Do 2 ( L D ) " 0.86 L max ( D) max V ME 2!S C 2 DME + C " 2 S 2 LME! # 3C Do " 0.76V L Dmax 9! L/D for Minimum Sink Rate" For L/D < L/D max, there are two solutions" hich one produces minimum sink rate?" ( L D )! 0.86 L ME ( D) max V ME! 0.76V L Dmax 10!

Climbing Flight! 11! Climbing Flight" Flight path angle " Required lift" ( T! D! sin" )!V 0 m ( sin" T! D ) ; " T! D sin!1!! 0 L cos! ( L " cos! ) mv Rate of climb, dh/dt Specific Excess Power "!h V sin! V ( T " D) ( P " P ) thrust drag Specific Excess Power (SEP) Excess Power Unit eight ( # P thrust " P drag ) 12!

Steady Rate of Climb" Climb rate " *"!h V sin! V, $ T +,# % '( C 2 ( D o +) )q - / & ( S)./ L q S cos" # & % ( cos" $ S ' q # V 2 & % ( cos" $ S ' ) Note significance of thrust-to-weight ratio and wing loading" *!!h V T $ # &' C D o q " % ( S) ' ( S )cos 2 ) -, / + q.! V T ( h ) $ # &' C D o 0 ( h)v 3 ' 2( ( S )cos 2 ) " % 2( S) 0 ( h)v 13! Condition for Maximum Steady Rate of Climb"!!h V T $ # &' C D o (V 3 " % 2 S ' 2) S cos 2 * (V Necessary condition for a maximum with respect to airspeed"! h!!v 0 (" T % "!T /!V * $ '+V $ )# & # % + '-. 3C D o /V 2 &, 2 S + 20 S cos 2 1 /V 2 14!

Maximum Steady" Rate of Climb: " Propeller-Driven Aircraft" At constant power"! P thrust!v 0 (" T % "!T /!V * $ '+V $ )# & # ith cos 2! ~ 1, optimality condition reduces to"! h!!v 0 " 3C D o #V 2 2 S + 2$ ( S ) #V 2 % + '- &, Airspeed for maximum rate of climb at maximum power, P max " 2! V 4 4 $ # & ' S ; V 2 S " 3% C Do ( 2 ( ' 3C Do V ME 15! Maximum Steady Rate of Climb: " Jet-Driven Aircraft" Condition for a maximum at constant thrust and cos 2! ~ 1"!! h!v 0! 3C D o " 2 S V 4 + T $! 3C D o " 2( S) V 2 Airspeed for maximum rate of climb at maximum thrust, T max " # % 2 + % T $ & (V 2 + 2) S ' " 0 ax 2 + bx + c and V + x # & (( V 2 )+ 2) S ' " 16!

Optimal Climbing Flight! 17! hat is the Fastest ay to Climb from One Flight Condition to Another?" 18!

Energy Height" Specific Energy " (Potential + Kinetic Energy) per Unit eight" Energy Height" Total Energy Unit eight! Specific Energy mgh + mv 2 2 mg! Energy Height, E h, ft or m h + V 2 2g Could trade altitude with airspeed with no change in energy height if thrust and drag were zero" 19! Specific Excess Power" Rate of change of Specific Energy " de h dt d! h + V 2 $ # & dh dt " 2g % dt +! V $ # & dv " g % dt " V sin! + V % # $ g & ' " # $ T ( D ( mgsin! m % & ' V T ( D Specific Excess Power (SEP) Excess Power Unit eight! P thrust " P drag ( C V T ( C D ) 1 2 )(h)v 2 S 20!

Contours of Constant Specific Excess Power" Specific Excess Power is a function of altitude and airspeed" SEP is maximized at each altitude, h, when" d SEP(h) 0 [ ] dv 21! Subsonic Energy Climb" Objective: Minimize time or fuel to climb to desired altitude and airspeed" 22!

Supersonic Energy Climb" Objective: Minimize time or fuel to climb to desired altitude and airspeed" 23! The Maneuvering Envelope! 24!

Typical Maneuvering Envelope: V-n Diagram" Maneuvering envelope: limits on normal load factor and allowable equivalent airspeed"! Structural factors"! Maximum and minimum achievable lift coefficients"! Maximum and minimum airspeeds"! Protection against overstressing due to gusts"! Corner Velocity: Intersection of maximum lift coefficient and maximum load factor" Typical positive load factor limits"! Transport: > 2.5"! Utility: > 4.4"! Aerobatic: > 6.3"! Fighter: > 9" Typical negative load factor limits"! Transport: < 1"! Others: < 1 to 3" C-130 exceeds maneuvering envelope! http://www.youtube.com/watch?v4bdncac2n1o&featurerelated! 25! Maneuvering Envelopes (V-n Diagrams) for Three Fighters of the Korean ar Era" Republic F-84! Lockheed F-94! North American F-86! 26!

Turning Flight! 27! Level Turning Flight" Level flight constant altitude" Sideslip angle 0" Vertical force equilibrium" L cos µ Load factor" µ : Bank Angle n L L mg sec µ,"g"s Thrust required to maintain level flight" 2 T req ( C Do +! ) 1 2 "V 2 S D o + 2! "V 2 S D o + 2! ( "V 2 S n )2 # & $ % cos µ ' ( 2 28!

Maximum Bank Angle in Level Flight" µ : Bank Angle Bank angle" cosµ qs 1 n 2! ( T req " D o )#V 2 S $ ' $ 1 µ cos "1 & ) cos "1 & ' * % qs ( % n cos"1, +, 2! - / ( T req " D o )#V 2 S./ Bank angle is limited by " max or T max or n max 29! Turning Rate and Radius in Level Flight" Turning rate"!! qssin µ mv tan µ n2 " 1 mv Turning rate is limited by " mv g tan µ L2 " 2 V mv ( T req " D o )#V 2 S 2$ " 2 mv max or T max or n max Turning radius " V 2 R turn V! g n 2 " 1 30!

Maximum Turn Rates" ind-up turns! 31! Corner Velocity Turn" Corner velocity" V corner 2n max mas!s For steady climbing or diving flight" sin! T max " D Turning radius " R turn V 2 cos 2! g n 2 max " cos 2! 32!

Corner Velocity Turn" Turning rate "! g n 2 max " cos 2 # V cos# Time to complete a full circle " t 2! V cos" g n 2 max # cos 2 " Altitude gain/loss "!h 2" t 2" V sin# 33! Herbst Maneuver" Minimum-time reversal of direction" Kinetic-/potential-energy exchange" Yaw maneuver at low airspeed" X-31 performing the maneuver" 34!

Next Time:! Aircraft Equations of Motion! Reading:! Flight Dynamics,! Section 3.1, 3.2, pp. 155-161! Airplane Stability and Control! Chapter 5! 35!!upplemental Ma"rial # 36!

Gliding Flight of the P-51 Mustang" Loaded eight 9,200 lb (3,465 kg) ( L / D) max $ L ' " MR #cot #1 & ) % D ( C D Maximum Range Glide! 1 2!C Do 16.31 max L/Dmax 2C Do 0.0326 ( ) L/Dmax C D o 0.531! V L/Dmax 76.49 * m / s!h L/Dmax V sin" # 4.68 * m / s #cot #1 (16.31) #3.51 R ho 10km ( 16.31) ( 10) 163.1 km Maximum Endurance Glide! Loaded eight 9,200 lb (3, 465 kg) S 21.83 m 2 C DME 4C Do 4 0.0163 ME 3C D o! L D ME 14.13 0.0652 3 ( 0.0163 ) 0.0576 0.921!h ME " 2 $ ' $ & ) C ' D ME 3/2 # % S (& % C ) " 4.11 LME ( # m / s * ME "4.05 V ME 58.12 # m / s 37!