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Lecture 1

Lift and Drag

Aspects of Aircraft Design and Control Olivier Cleynen – February 2014 – v1.4

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~ foreword ~

The present notes serve as a support for in-class work, not the opposite!

Refer to the introductory course notes for explanations.

These notes are used as a succinct introduction to selected topics. They are purposefully

incomplete and must not be used for real-life

applications.

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Feedback is always appreciated:

olivier.cleynen ariadacapo.net

These course documents can be found at:

http://aircraft.ariadacapo.net/

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This document is published

under a Creative Commons license.

Some photos and illustrations have their author and specific license indicated on the bottom of the page.

All other content is © 2011-2013 CC by-sa Olivier Cleynen.

You are encouraged to copy, modify,

and re-use this content under specific conditions:

http://creativecommons.org/licenses/by-sa/3.0/

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1. Basic concepts in mechanics

(6)

energy time force distance

t F

d

(7)

Weight

m g

(8)

Work

F × d

[J]

(9)

Power

t

[W] or [hp]

F × d

(10)

Power

Power and fuel economy are two different things!

A more powerful car usually raises your fuel consumption

A more powerful aircraft usually does not

Aircraft are usually extremely powerful (×100)

(11)

~ 50 khp machine

(12)

Work

The work spent and the work received are often very different

P

received

= F × V

aircraft

P

spent

= F × V

air

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(14)

2. Power and speed

on the ground

(15)
(16)

Forces on a train

CC-0 Olivier Cleynen

(17)
(18)

No friction

F = 0

(19)

Voyager

(20)

Solid Friction

(rolling friction/resistance) (dry metal friction)

F = k

(21)
(22)

CC-0 Olivier Cleynen

(23)

If F = k

(24)

Friction with flexible materials

F = k × V

(25)
(26)

If F = k × V

(27)

Fluid Friction

F = k × V²

(28)

CC by-sa W:MorganaF1

(29)

If F = k × V²

(30)

If F = k × F²

(31)

Power spent to drive a train

No friction?

→ infinite max. speed

Solid friction?

→ there exists a max. speed

→ Fuel burn per km does not depend on speed

Fluid friction?

→ Any 40% speed increase doubles fuel burn per km

(32)

Power and fuel economy are determined

by the speed dependence of drag

D = f ( V )

(33)
(34)

CC-0 Olivier Cleynen

(35)
(36)

CC by-sa Vincent Edlinger

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(38)

3. Aircraft forces

(39)

Aircraft forces

(40)

Weight

CC by-sa Vincent Edlinger

(41)

Weight

MTOW MLW OWE

(42)

Aerodynamic reaction force

depends on a very large number of factors!

(43)
(44)

Thrust

≠ power

≠ energy expense

...but related to both

(45)

Lift and Drag

~ blessing and curse ~

(46)

Lift and Drag

Directions relative to speed, not fuselage An arbitrary (not “physical”) distinction

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Finesse [the lift-to-drag ratio]

measures how “vertical” the reaction force is varies according to flight conditions...

fL

D

(49)

Finesse (the “lift-to-drag ratio”)

“finesse” is often used to mean “maximum finesse”

Finesse varies extensively during a flight, and aircraft rarely fly at fmax

fmax is usually 10 on a jet fighter, 20 on a modern airliner or private aircraft, 40 for a competition sailplane

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4. Quantifying aircraft forces

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Experimenting: measuring lift

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Experimenting: measuring lift

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Experimenting: measuring lift

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Experimenting: measuring lift

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Lift

Increases with speed squared

Varies linearly with angle of attack (only in a certain range!)

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Experimenting: measuring drag

(57)

Experimenting: measuring drag

(58)

Drag

A strange behavior indeed!

Increases with speed squared

Increases with inverse of speed squared, too...

At a given lift and altitude, drag will increase if you fly too slow. (≠ train!)

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5. Lift and drag coefficients

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How can we compare the ability to generate lift

for two wings of different shape and size ?

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Wings generate lift

by imparting downward velocity on the air

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A crude description of lift generation

CC-0 Olivier Cleynen

(63)

A crude description of lift generation

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An idealized description of downwash

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A crude description of lift generation

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A crude description of lift generation

CC-0 Olivier Cleynen

(67)

An idealized description of downwash

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How does an aircraft generate a force on air ?

Given a steady mass flow:

F

net

= d

d t ( mv ) = ˙ mv

mass flux × change in velocity

(69)

What flight parameters affect mass flux ?

Proportional to air density

Proportional to aircraft size (surface)

Proportional to aircraft speed

Depends on aircraft geometry

m ˙

m ˙ = ρ 1

S V g

(70)

What flight parameters

affect downwash velocity ?

Proportional aircraft speed

Depends on aircraft geometry

Depends on aircraft attitude

v

d

v

d

= V

aircraft

g

geometry(2)

g

angle

(71)

Quantifying lift:

= ρ 1

2 S V

aircraft2

g

geometry

g

geometry(2)

g

angle

L = ˙ m v

d

g

geometry& angle

C

L

(72)

The lift coefficient

The wing’s figure of merit

“influence of the wing geometry”

C

L

L 1

2 ρ S V

2

(73)

And thus:

L = 1

2  S V

2

C

L

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For a given C

L

(given flow pattern):

Double the density?

→ lift doubled

Double the wing surface?

→ lift doubled

Double the velocity?

→ lift quadrupled

C

L

L 1

2 ρ S V

2

(75)

For a given L (given aircraft)

High speed, high density, high surface?

→ you want low CL

Low speed, low density, low surface?

→ you want high CL

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CC by-sa Vincent Edlinger

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(78)

CC by-sa Vincent Edlinger

(79)
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CL L 1

2 S V2

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The lift coefficient

“Wing capability” for generating lift, independently of main conditions

Controlled mainly with two parameters:

Angle of attack

Wing shape (esp. camber)

Defined arbitrarily (but meaningfully) Dimensionless number (has no units)

(82)

Predicting the lift coefficient on a given wing

Extraordinary wing shapes have different behavior Linear aerodynamics: CL,α is constant

Only true when the wing isn’t stalled!

C

L

= C

L ,

 − 

0

C

L

= k

1

  k

2

(83)

The drag coefficient

C

D

D 1

2  S V

2

(84)

Predicting the drag coefficient on a given wing

Lift-independent drag (“viscous”)

Induced drag (“lift-induced”)

This equation only works in ideal conditions, i.e. high Re, low M, linear aerodynamics

C

D

= C

D0

K C

L2

C

D0

K C

L2

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(90)

6. Basic flight mechanics

(91)
(92)

CD D 1

2 S V 2

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Lift and Drag

The equations we wrote have amazing consequences.

Small wings, low density will increase your speed without an energy cost...

… but you need higher power.

Play around with the above notions and equations...

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Beware:

The equations we wrote have limited validity...

Mach number dependence

Reynolds number dependence

No account for stall

Never trust equations that “fall from the sky”.

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Project 1

Flight speed range

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(98)

Eclipse 500: the “$1,5m” jet

CC by-sa Alan Radecki

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CC by-sa Josh Hallett

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(102)

CC by-sa Josh Hallett

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Pratt & Whitney Canada PW610F (Eclipse 500)

$150k D=37cm W= 120kg BPR=1,8 T=4kN

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Project 1

… is about putting together the concepts we explored today (in particular, drag)

You are working for an aircraft manufacturer

Data from a wind tunnel model series of tests is passed on to you – what do you think?

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Project 1: tasks

Choose a wing area that meets the design specifications ;

Calculate the minimum and maximum flight speeds at low altitude ;

Calculate the aircraft’s finesse and its optimal flight conditions.

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Tools and help

Use whatever software you wish (or none)

Books, websites etc. in English are okay, but must be quoted.

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Length

Reports: 8 pages max (no longer!)

Presentations: 15 minutes max, plus questions

(108)

How to Get the Project Done

This is not a riddle that must be solved...

→ the solution is not hidden in the appendix

Try to imagine the result first...

Think about the data you need, then look for it

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Key to a successful project:

Get a rough idea

of what the result looks like

as early as you can

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