Topic 2
S01:E02

Topic 2

Episode description

Topic 2

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0:00

if

0:18

so from what we

0:20

discussed

0:23

up to this point

0:26

flying for range and flocking for endurance are two

0:30

completely separate arguments.

0:33

And so we'll be coming back to that. By the

0:36

way, you're going to hear it over and over again is the

0:39

as the course progresses

0:41

It's time down to move on to another concept which

0:44

is a lot easier to get your head around.

0:47

All over the terminology might be something we need to.

0:51

Clear up.

0:54

We call it kinetic energy.

0:58

now let's start with the

1:00

the simple formula

1:03

That allows us to calculate.

1:06

kinetic energy

1:09

but before we do

1:12

I just want to put it in the most simple terms because as

1:15

we've seen since so far whatever can

1:18

be done with formulas and graphs and

1:21

things can be said in civil words.

1:24

Now if you ask me.

1:27

What do you mean by kinetic energy? What what the

1:30

hell is it?

1:32

It's one very simple answer to that that any school

1:35

child knows.

1:38

How hard would it be to stop?

1:43

full stop

1:45

that tells you all you need to know about kinetic energy kinetic

1:48

energy if you want to see how much

1:51

kinetic energy and object possesses.

1:54

Ask yourself how hard it would be to stop

1:57

it.

1:58

Because kinetic energy is the energy you possess

2:01

because of your motion.

2:04

And so to find out how much kinetic energy you have

2:07

you take the motion away.

2:09

You stop it.

2:11

And so the formula is

2:14

very simple in.

2:16

Kinetic energy is one half.

2:19

times the mass

2:21

by the speed of velocity

2:24

But the velocity notices squared.

2:28

That that square tells us something.

2:31

It means that if you double the speed.

2:34

You'll get four times the kinetic energy.

2:37

The the relationship is not linear.

2:40

It's

2:42

it's exponential.

2:44

And so by the way, don't let the half bother you

2:47

that's put in a math as purely as a mathematical convenience. So

2:50

it doesn't concern us right now,

2:53

but the formula does say one half times the

2:56

mass.

2:57

by the speed squared

3:00

and when I look at that it means because the

3:03

mass

3:05

the mass does not have a squared on it.

3:08

Say that's a straight direct proportion.

3:12

That means double the mass you get double the kinetic

3:15

energy.

3:16

Double the speed and you get four

3:19

times the kinetic energy.

3:23

And so that's a very rapid increase.

3:26

And the question and the way to think about it is simply.

3:30

m stands for the mass of the object

3:34

and v stands for the speed that

3:37

it's traveling at.

3:42

And the speed is squared.

3:46

And so that means if you

3:48

approach your airplane just a little bit faster.

3:53

What you think is only a little bit faster.

3:56

You'll be surprised at how much more room you need

3:59

to pull up in?

4:00

Because for an airplane, that's a perfect example of kinetic energy

4:03

how far how much runway do

4:06

you need to stop?

4:08

How hard would it be to stop that's that's just

4:11

the unscientific way of talking about

4:14

kinetic energy.

4:18

If I travel if I approach a bit faster than I should.

4:22

I find that I have a

4:24

Very big difference in the distance there to stop by the

4:28

way. I'd luckily it works the other way if I can reduce my speed over

4:31

the fence.

4:33

I have a surprisingly big Improvement in landing

4:36

distance. I'll need a lot shorter Landing distance.

4:39

And so that's why airplanes and

4:42

we'll deal with this later in the course.

4:45

Big jet airplanes have got a hell of a lot of mass.

4:50

A very very large, Mass.

4:53

hundreds of tons

4:56

They can't help that because that's where we build them. We build

4:59

them to carry weight.

5:01

And so the only way to have a sensible Landing distance

5:04

is to have less speed over the

5:07

fence bit of a dilemma, isn't it for the for the

5:10

designer I wanted to go fast, but

5:13

I wanted to go slow when I needed to.

5:17

And so that's why the Jets have all those lift augmentation

5:20

devices on the wings. That's another

5:23

day. We'll be discussing that quite simple. We can

5:26

we can actually create a whole new wing for landing.

5:30

So that I can now fly a jumbo

5:33

jet can cross the fence with something like 130 knots.

5:38

Which is really slow when you consider its weight.

5:43

And so we'll be talking a lot more about that'll still that

5:46

when the time comes.

5:48

and so

5:50

if I double the mass I double the kinetic energy.

5:53

If I double the speed I get four times the kinetic

5:57

energy.

5:59

It's the energy and object has because

6:02

it is moving.

6:05

So the question to ask is

6:08

how hard would it be to stop it?

6:12

And the rest of that, of course the relates to motorbikes and semi-trailers and

6:15

it's as clear as can be.

6:19

and

6:21

Landing distance

6:24

if I

6:25

the distance I need to land.

6:27

In depends under the kinetic energy

6:30

that I possess when I touch down.

6:35

The if I touch down slower.

6:38

Then I can pull up shorter.

6:42

Almost embarrassing and have to say that I

6:45

think I think most people would say. Yeah, that's but the interesting

6:48

that there's always a formula that says that in a

6:51

way that can't be argued. It's precise.

6:56

And the distance required to

6:59

stop now. That means two ways

7:02

to kinetic energy can be created.

7:04

I can have a heavy object traveling

7:07

slowly.

7:09

It can still have a hell of a lot of kinetic energy a perfect

7:12

example would be an ocean liner.

7:15

100,000 tons ship

7:17

traveling at three knots

7:20

Is bloody hard to stop?

7:23

It's not going very fast.

7:25

But try stopping it.

7:27

All right, that's why they have to be so careful when they dock it

7:30

now. They got all those propellers that work sideways. But

7:33

in the olden days they had to have tug boats that

7:36

gently gently nudge it until it's

7:39

up against the jetty.

7:41

If it's doing one knot and it hits the jetty and it

7:44

weighs 100,000 tons good boy, Jenny.

7:48

It just continues to travel.

7:52

On the other hand, of course a lighter object traveling fast

7:55

can end up with a lot of kinetic energy.

7:59

a bullet

8:00

is a light object.

8:02

But it travels at something like 2000 kilometers an

8:05

hour when it leaves them a gun.

8:09

And so it's it's equally difficult to stop.

8:12

Some people have discovered that for themselves. It's hard

8:15

to stop a bullet.

8:17

and

8:19

but this leads us to an interesting discussion.

8:23

Because it's one of the most important instruments in our cockpit and

8:26

it's vital that we understand it.

8:29

And that is a thing we call the indicated airspeed.

8:34

airspeed indicator

8:37

it's very

8:39

it's very poorly understood quite often.

8:43

In fact, I find the best way to understand it clearly is

8:46

to take a trip down memory lane years

8:49

and years ago at the earliest.

8:53

ESPN indicators, by the way, did you realize the Wright

8:56

brothers didn't have one?

8:58

We put so much importance now on AirSpeed your

9:01

instructor jumps up and down saying look at what's your SB

9:04

does this is as and and I can imagine some students

9:07

thinking they must have adverted AirSpeed

9:10

indicators first before they had airplanes because no

9:13

one could fly without one you'd die for sure.

9:16

No, we flew our Appliance without spit

9:19

indicators for a long time, but then we discovered you

9:22

can't fly it accurately.

9:24

You can't get the best out of it. Unless you have

9:27

a good Espin indicator, but when it

9:30

comes to being safe that must have been the good old days,

9:33

you know, you you open the throttle and you sort of feel the wind, you

9:36

know, that feels about right. I reckon she'll go now and

9:39

so off you go and fly away.

9:41

all right, and

9:43

yeah, there's been Dakota was what you felt.

9:47

But here when they started introducing AirSpeed

9:50

indicators, this is one of the earliest and

9:53

I love this one because it shows you really clearly.

9:57

What it is?

9:59

Remember we had that discussion about molecules.

10:03

And we said here is that is actually made up of molecules.

10:07

And each molecule has got weight a tiny tiny

10:10

weight, but each one has weight.

10:13

And and the pressure it exerts as due purely to the

10:16

impact of those molecules.

10:19

And so they invented this gadget which

10:22

explains it so clearly

10:24

we have a flat plate.

10:27

and a spring

10:30

All right a flat plate.

10:32

down there and a spring

10:35

and as I fly the air.

10:38

slams into that plate

10:41

and molecules slam into that plate.

10:44

And that applies a force to that plate?

10:48

But that Force depends on two things it depends

10:51

on how fast each molecule is moving when

10:54

it hits.

10:56

But don't forget it also depends on how many molecules hit.

11:00

How close together are they?

11:03

That's what we call a density.

11:06

if the air is

11:08

it isn't just the speed that matters.

11:11

if the molecules hit at a certain speed

11:14

They'll apply a certain Force.

11:16

But if a lot more molecules hit at the

11:19

same speed then they'll apply a bigger Force.

11:22

And so what happens now is as the airplane

11:25

flies.

11:27

it

11:28

the molecules hitting that plate move it

11:31

across the dial.

11:34

And this airplane above the door?

11:37

Was built by a very good made of iron laying kidbe.

11:43

who is a

11:44

most amazing gentleman die

11:46

I'll tell you more about him at the bar one day but a

11:49

fascinating man, but he built that airplane to

11:52

commemorate bertinklers flight from England to

11:55

Australia.

11:56

And he built it in Australia took it to England.

11:59

And then flew it out on the same route

12:02

that Burt Heckler took.

12:04

as a commemoration of Burt angle's flight

12:08

And it was originally built.

12:10

With one of these aspid indicators. In fact, he

12:13

left it on.

12:15

He left it on there, but he still had to have a proper one, of course

12:18

for Casa to be registered.

12:21

But he still had the old one.

12:23

And when he came in from England, he landed at archerfield.

12:27

and

12:29

the front cockpit was actually all fuel tank. So it's

12:32

only had one seat.

12:34

And he was doing a channel 9 interview.

12:37

I mean said to me.

12:39

Plans there they can't have floors. See what you reckon.

12:43

That's how I jumped off at all. I want to haven't had burrow

12:46

in my log book. So and so I jumped

12:49

in it and did a couple of circuits.

12:52

and

12:55

the interesting thing was

12:57

this was mounted on the interplan strut.

13:01

It's mounted on those struts between the wings those way

13:04

outside the cockpit.

13:06

And but you you can compare it with the real airspeed

13:09

indicator that was in the cockpit and it was

13:12

spot on.

13:14

So it was a lot I love the way.

13:17

I love the way that shows you so clearly.

13:20

Just what's going on? And it's so

13:23

obvious now that if if the air

13:26

is thin?

13:27

Then the speed.

13:31

The speed and if the speed stays the

13:34

same in the air is thin.

13:36

Then the indication will be less.

13:39

And so the speed of each molecule is really your

13:42

true speed.

13:44

But then you've got to consider how many molecules are hitting the

13:47

plate and that's that's the

13:50

density of the air.

13:53

So it's a beautiful.

13:55

Way to introduce the argument nowadays, of

13:59

course, we use a far more sophisticated idea.

14:03

and we use

14:06

a

14:07

capsule that can expand like the Bellows of

14:10

a piano accordion

14:12

and I pedo tube.

14:16

That that reminds us by the way the French had a

14:19

lot to do with early flight.

14:21

They still I reckon that they did it first before the Wright

14:24

brothers.

14:25

and

14:27

the pedo

14:28

Is an open tube that faces forward?

14:31

And so there ear molecules that go

14:34

in there are traveling at the speed of the aircraft.

14:38

And they go up into the capsule and flood into

14:41

the inside.

14:43

But the outside of the capsule is connected to

14:46

a static vent.

14:48

And it's a range so that the air doesn't blow in there. The

14:51

air goes straight past it, but it doesn't actually blow

14:54

in.

14:56

And so it doesn't record the speed of the

14:59

year. It just records the pressure of the air if

15:02

it wasn't moving.

15:05

And we call it the static Source or static

15:08

vent.

15:10

And so as I as I it does the same job as that

15:13

old one. It measures the force of

15:16

the wind now, of course that's already got static

15:19

pressure in there.

15:21

But the extra force is called Dynamic pressure the force

15:24

of motion.

15:26

And it goes in and builds up what we're called total pressure

15:29

inside the capsule.

15:32

But the pressure here is just the static pressure of the air.

15:35

And so that the capsule starts to expand.

15:40

Due to the difference between the total

15:43

pressure and the static pressure.

15:46

And we call that difference the dynamic pressure

15:49

the instrument measures the dynamic

15:52

pressure of the air.

15:56

And so this is basically what happens as my speed increases

15:59

the capsule expands.

16:02

And the moving capsule drives the hand drives the

16:05

pointer.

16:06

It's responding that is not to speed.

16:10

It's the responding not to speed at all. It's responding

16:13

to pressure.

16:17

So I don't know why it's actually.

16:20

a bit of a fiber

16:21

it's not really a speed indicator.

16:29

It's a pressure indicator. It's the dynamic pressure indicator.

16:36

the molecules enter at the speed of

16:39

the true speed of the airplane

16:41

But then the number of molecules matters as

16:44

well.

16:45

When it comes to the pressure that's built up.

16:50

the mass now I hope that might

16:54

I hope that might remind you of something we said before we

16:57

had that short break.

17:00

and that is

17:02

it responds to the kinetic energy of the

17:06

air because that's the mass and the speed.

17:09

half MV squared

17:12

right notice what this is really doing. It's catching

17:15

some of the air and bringing it to

17:18

a stop in a dead end.

17:21

Well, isn't that what we just said if you want to know how

17:24

much kinetic energy it has then stop it and

17:27

see how hard it is to stop.

17:29

By catching that air and stopping it. We're

17:32

releasing its kinetic energy.

17:35

And this instrument is measuring the kinetic energy of the

17:38

air.

17:41

the mass

17:42

And the speed together.

17:46

Is what it's reacting to.

17:50

Okay, and therefore because it's

17:53

a pressure that we're talking about.

17:56

Remember when pressures act on surfaces they create forces?

18:01

We all know that When Storms hit.

18:03

The moving air hitting an object

18:06

will apply a force to the object.

18:10

And the roof blows off the house.

18:13

and so

18:14

therefore that's got that's got implications for

18:17

aircraft.

18:19

Because of that Force gets big enough for women or two

18:22

the force increases with the square of the speed. You

18:25

don't have to go much faster to get a lot

18:28

more force and when we build airplanes we can't

18:31

make it out of angle iron.

18:33

Our big concern is wait.

18:36

And so most airplanes are only just strong enough to do the

18:39

job.

18:41

And therefore it's up to us to be careful that we don't

18:44

apply too much force. That is too much

18:47

kinetic energy too much indicated airspeed.

18:51

And so the espion indicator has the following.

18:57

limiting air speeds

19:00

right firstly they have a color the white Arc the

19:03

beginning of the white Arc.

19:06

Is the stalling speed?

19:10

with flaps and undercarriage down

19:14

the Air Force call it the dirty.

19:17

stalling speed

19:19

I mean everything's hanging out of aircraft.

19:22

flaps them undercarriage down

19:25

if you go, but if you go slower than that, there's not enough

19:28

kinetic energy in the air to make the lift you

19:31

want.

19:32

So flight is impossible.

19:36

The green Arc is the stalling speed vsi.

19:40

Usually I use the Roman letter i for one.

19:45

and

19:47

that's the green Arc and that's the stalling speed clean.

19:51

That's the stalling speed with the flaps up and the gear up.

19:56

And then over here, we have the end of the white Arc called

19:59

vfe flap extended speed.

20:03

That is the greatest speed I can fly out.

20:06

Before I start to damage the flaps if they're

20:09

down. So any any speed

20:12

above vfe.

20:14

Means the flaps must be retracted.

20:18

Don't forget by the way, not only may you not only may you

20:21

damage the flap?

20:23

but clearly

20:25

if I've got my flaps down.

20:28

It could damage the flap itself, but it's also applying a

20:31

strong force on the back of the wing.

20:34

And that's trying to twist the wing.

20:36

So we can actually distort the whole wing.

20:39

If we go fast enough with the flaps down that'll apply

20:42

a torsion load on the wing a

20:45

twisting word.

20:47

And so

20:50

vfe

20:53

It's all about forces.

20:56

As I said, it's not it's not speed at all.

20:59

It's pressure.

21:01

And and then we have v&o.

21:05

Which is where the green arcans?

21:08

And that's called normal operating.

21:11

speed

21:13

and it means if you're above that speed.

21:17

Then don't allow any

21:20

turbulence.

21:23

Turbulence can impose those forces as well.

21:27

By changing the angle of attack on the wing when

21:30

air hits it from underneath.

21:32

and so

21:34

you can fly that you can still fly up here.

21:38

But you must not allow the airplane to be

21:41

to encounter turbulence.

21:44

And then finally have a red line.

21:47

Covey and a which stands for never exceed

21:52

and that's the speed.

21:53

That even if the air is calm and even

21:56

if the flaps are up.

21:58

you can still cause damage to the

22:02

aircraft structure

22:04

We've got a lot more to say about that. Later.

22:07

but

22:09

every pilot should be aware that they speeds exist.

22:12

Some of them are actually color-coded as

22:15

you can see.

22:17

But there are other speed limits that are not color coded.

22:21

But they are still important ones.

22:24

for example

22:26

There's a speed call maneuvering speed or VA.

22:32

maneuvering speed

22:35

means

22:36

do not apply full control deflection if

22:39

you're above that speed.

22:45

So mostly it's the elevator we're interested.

22:48

In that don't pull the elevator all the way back to the

22:51

stopper.

22:53

If you're above that speed and that mainly and I think

22:56

you'd agree would have to be due to.

23:00

Pilots

23:02

Doing aerobatics because it's not likely that a

23:05

pilot would be flying along and then go

23:08

I think I'll pull the elevator all the way back, right? Normally.

23:11

We don't do that unless this

23:14

something seriously wrong, so

23:18

so

23:19

that's more mostly an aerobatic issue.

23:22

VA don't don't have the

23:25

elevator fully extended above that speed.

23:30

and

23:32

then we have another one called turbulence penetration speed.

23:36

and turbulence penetration speed

23:39

basically works like this.

23:43

if

23:46

this represents the wing

23:49

and this represents my forward speed.

23:54

then if

23:56

tabulence is basically vertical movement of

23:59

the air.

24:00

And so if the air comes up from underneath like that.

24:05

That it means the effectively the angle of

24:08

attack.

24:10

The air is now coming from this direction instead of

24:13

that direction.

24:14

So effectively the angle of attack has

24:17

been increased. So hitting hitting turbulence

24:20

as much the same as pulling a stick back.

24:24

The airplane can't tell the difference.

24:26

The airplane can't tell the difference between you pulling

24:29

the stick back.

24:30

And you hitting an updraft?

24:33

It does has the same effect on the wing.

24:37

And so nice many airplanes have

24:40

a turbulence penetration speed if you

24:43

in Canada severe turbulence.

24:46

And slow down below that speed.

24:49

by the way

24:51

You're more likely to be very concerned about that when

24:54

you do your instrument rating.

24:56

because an IFR pilot a vfi pilot

25:00

can see

25:03

it's not often a vfi pilot's going to encounter severe

25:06

to turbulence.

25:09

But in our five Paul is flying in Cloud.

25:12

Now imagine this problem. I'm flying in Cloud. I can't

25:15

see so how do I there's not a thunderstorm in the

25:18

cloud?

25:20

a thunderstorm embedded in the cloud

25:23

and so one thing that haunts all of our

25:26

Pilots is I'm flying along one day and suddenly found

25:29

myself in accumulated numbers, and I couldn't see

25:32

it coming.

25:34

And so if I

25:37

Pilots are much more interested in turbulence penetration speed.

25:43

Okay. Now this leads us to a related

25:46

argument in fact

25:48

the idea

25:50

of vectors

25:52

So let's look at it. I said we're going to talk about

25:55

vectors. They're those arrows that people like to

25:58

draw all over the board when they're

26:01

giving you a briefing.

26:03

Imagine I've got a weight and a rope

26:06

attached to the weight that I'm trying to drag it along.

26:09

And so the real force is acting on the Rope.

26:14

That's what I'm really doing.

26:16

But it's possible to break that up into two imaginary

26:19

forces. They would have the same effect.

26:23

And so what I can do is draw

26:26

a line along horizontally and another

26:29

one vertically.

26:32

and if I drop

26:34

a perpendicular down

26:36

Under the horizontal line and a cross under

26:39

the vertical line.

26:40

I could create two separate arrows.

26:44

To represent two separate forces which would

26:47

have exactly the same effect as this one.

26:52

Now, sometimes it's convenient to do that.

26:55

Sometimes it's handy.

26:57

To take one big force and think

27:00

of it as though it was two forces acting separately.

27:04

the beauty of a vector is

27:07

the direction of the arrow represents the direction of the

27:10

force.

27:11

And the length of the arrow represents the strength

27:14

of the force.

27:16

How strong it is?

27:19

So those two black forces if they

27:22

acted simultaneously.

27:24

Would have exactly the same effect.

27:27

as the real force that is acting

27:33

now this happens on the wing.

27:35

because when the wing is

27:38

Is flying and the air is flying over it?

27:42

What really happens is there's a total reaction.

27:46

And the total reaction is the caused by

27:49

all of the molecules of air.

27:52

flowing over the entire Wing surface

27:56

Now, of course that would drive us nuts if we try to imagine that is

27:59

separate each separate individual molecule. That's what's

28:02

really happening. Each molecule is contributing

28:05

but we think of it as though one force acted.

28:09

And we represent it as a single Force.

28:12

That doesn't only lift up but pulls back as well.

28:17

that single Force represents

28:19

the total reaction of the wing to the airflow.

28:23

Now we can split that up into two separate forces.

28:27

And we split it this way. We take

28:30

one force.

28:32

And right angles to the direction of travel.

28:36

This one is always at right angles.

28:39

to the direction of travel

28:42

and we call that one lift.

28:45

And then we take another Force.

28:48

Which is parallel to the direction of travel.

28:52

And we call that one drag.

28:54

Now one point I always like to try to make to people

28:57

here is we talk so much about lift and

29:00

drag.

29:02

But isn't it interesting to know that they don't exist?

29:07

All right, you'll never understand lift and

29:10

drag.

29:11

Unless you realize they don't exist. They're not real.

29:15

They're imaginary. They certainly handy Way To

29:18

Think.

29:19

But and that's this by the way explains a

29:22

few other things for example.

29:26

If you try to change lift.

29:29

It's almost impossible.

29:31

to change lift without changing drag

29:36

because the two are not really separate they really

29:39

sides of the same coin

29:43

lift and drag

29:45

are inseparable

29:48

because they really components what we call components

29:51

of the total reaction.

29:56

And so there's an airplane is in a climb for example.

30:00

Then two forces two types of forces are

30:03

trying to pull it down.

30:05

the weight

30:06

and the drag

30:08

erecting together

30:11

now we can now use another technique with vectors.

30:15

With two separate forces we can caught we can turn

30:18

them into one.

30:21

That that has the same we call it

30:24

a resultant a resultant Force. So those

30:27

two forces are really separate drag and wait.

30:32

but if we then

30:34

Do this.

30:36

I move weight down to the end of the drag Arrow.

30:40

And then I joined that join them with a line.

30:46

from the beginning of drag to the end of weight

30:50

and that dotted line is actually called a resultant.

30:54

Now then I can now forget about dragon and wait.

30:59

I can ignore them and I think of it as one

31:02

force.

31:03

dragonwade acting together

31:06

and therefore lift and lift

31:09

and thrust also.

31:12

Are acting that way and that way.

31:16

And I can do the same with that. I can add thrust

31:19

and lift together.

31:21

And I get a result now. Here's where

31:24

you take some advantage.

31:26

And what we said earlier.

31:28

We now have equilibrium in a climb.

31:32

this resultant of dragon White

31:37

is

31:38

is also

31:43

is also

31:45

balanced exactly balanced

31:47

by the result of lift and thrust

31:51

so that that line is the same length as that line.

31:55

And they and together they are one straight line.

31:58

So they are exactly balancing out.

32:01

and so equilibrium now exists

32:04

four forces are acting

32:06

lift weight thrust and drag

32:08

But they combined effectors balanced.

32:12

and so equilibrium exists

32:16

and the airplane continues to climb in a

32:19

straight line at a constant speed.

32:24

Now money using that now we're going to

32:27

talk about climbing in a lot more detail. Later.

32:30

But only using it now as an example of vectors

32:33

how a vector can be used to prove a

32:36

point.

32:39

I can use vectors to prove a point.

32:43

The results are equal and opposite so there's no

32:46

net force acting.

32:48

on the aircraft

32:51

and so it'll keep doing what it's doing.

32:54

Now this one I'll just go through quickly because I'm sure you

32:57

would have done this in PPL.

33:00

But let's say a little bit about motion what types of

33:03

motion can the airplane perform?

33:07

It can do three types of motion.

33:10

Now this is going back to baby.

33:13

stuff on the beginning of everything the airplane

33:16

can pitch

33:18

that means it can move and that fashion.

33:21

It can roll.

33:23

So it can move in this fashion.

33:28

and it can your

33:30

so it can move in this fashion.

33:33

Now we don't need to say that I'm sure to you as you got a private

33:36

license, but one thing that is interesting though,

33:39

and a lot of people miss this

33:42

point.

33:43

often cease to say this to instructors that I trained we

33:46

tell all the students the airplane can pitch and

33:49

role in your

33:50

but we often don't say the most important thing.

33:53

And that is it can't do anything else.

33:57

It can't do anything but pitch role in

34:00

you the most complicated aerobatic maneuver.

34:04

There was ever devised.

34:06

this picture role in your

34:08

Okay, they might be all simultaneous but the airplane

34:11

can only do three things.

34:14

And that's that's reassuring because it means if

34:17

I've got three controls.

34:20

I can control each of those three motions. There's nothing

34:23

the airplane can ever do providing the controls

34:26

remain effective.

34:28

There's nothing the airplane can ever do that. I can't control.

34:32

And so these are important things

34:35

but here's another point. I'd just like you to think about

34:38

briefly.

34:39

when an airplane pictures

34:41

then the nose comes up we'll know that the nose

34:44

comes up in the tail goes down.

34:48

like that

34:50

and that means everything neither the nose goes up.

34:54

And everything near the tile goes down.

34:58

but he's a point that often we don't stop and think

35:01

about

35:02

if the tail is going downwards and the nose

35:05

is going upwards.

35:08

What there must be a place somewhere where it swaps

35:11

were changes?

35:13

There must be a point where everything ahead of

35:16

that point.

35:17

Is traveling up.

35:19

And everything behind that point is traveling down.

35:22

That's the axle or axis of

35:25

rotation.

35:26

right and

35:29

That's the point about which the rotation does occur and

35:32

for every object in the universe not just airplanes.

35:36

That are free and spiced to rotate and

35:39

they're not attached to something.

35:41

everything that rotates and moves

35:44

the point about which it rotates is the

35:47

center of gravity.

35:48

Of that airplane. That's what Senator gravity is. It's

35:51

the point about which the rotation occurs will

35:54

be coming back to that. Of course when we do performance.

35:59

It's called the center of gravity. It's the

36:02

point about which the rotation occurs

36:05

and it rotates about an imaginary axis.

36:09

which can be thought of as a

36:12

as a wire that goes through the airplane from wingtip

36:15

to wingtip.

36:16

If we held it by that wire the only

36:19

motion it could do would be to pitch.

36:27

It's called the lateral axis. We'll be

36:30

dealing with this and much more detail too. Later.

36:34

Now rolling is a similar argument if the

36:37

airplane rolls then everything on one side goes up

36:40

and everything on the other side goes down.

36:45

So there must be a changeover.

36:48

There must be a point.

36:50

About which it will about which it rolls.

36:54

And again, that's the center of gravity.

36:56

The center of gravity is again the

36:59

Pivot Point.

37:01

And we can imagine an axis.

37:04

Now that passes through the airplane longitudinally from

37:07

the nose to the tail.

37:10

And if I held the airplane by that axis.

37:13

Then the animation possible.

37:16

Will be role.

37:20

And finally if they are applying yours.

37:23

Same argument part of it goes one way to the

37:26

right and part of it goes to the left. There's again,

37:30

there's a changeover.

37:32

Which is the center of gravity?

37:36

Okay.

37:38

And the center of gravity in this case when it comes

37:41

to your ring. The axis is a vertical axis that

37:44

passes through the airplane

37:47

from roof to floor.

37:50

It's proper name is normal.

37:53

It's called the normal axis if I

37:56

hold the airplane by that axis the only motion possible.

38:00

is your

38:04

and the whole three axes

38:08

all go through the center of gravity.

38:11

So the center of gravity is actually the

38:14

center of it all that's the point where all three

38:17

axes meet. In fact.

38:22

and

38:24

pitching about the lateral axis

38:27

rolling about the longitudinal axis

38:30

and urine about the normal axis.

38:34

Now sometimes it is an examiner. I talk

38:37

about a plane of motion.

38:39

It's really same argument that I'd like to just mention it

38:42

in passing.

38:44

The plan of motion is an imaginary sheet

38:47

of glass.

38:49

And this guy says it's the pitching plane.

38:52

That passes through the airplane from spinner to tile.

38:56

when the airplane pitches

38:58

it is moving in the pitching plane. It's

39:01

just another way saying the same thing.

39:04

Also, we have a plane that moves.

39:07

That vertical plane that goes across the wings.

39:12

And when it moves in that plane that's rolling the rolling

39:15

plan.

39:16

And then it has a horizontal plane that passes

39:19

that way.

39:20

and when it moves in that plant

39:23

it's urine.

39:25

We call it the urine plan now, they're just

39:28

definition so I won't dwell on them.

39:32

And of course, we all know this.

39:34

We have three controls elevators the control pitch.

39:38

They are notice that it control doesn't only prevent doesn't

39:41

only cause motion a control

39:44

is often used to prevent motion.

39:47

If you do if you do a loop in an

39:50

airplane, if I fly around a loop,

39:53

then the only motion is pitching but that

39:56

doesn't mean there's only using the elevator.

40:00

Because while you're doing that you don't

40:03

want that to happen either.

40:06

And so if you do a loop, especially in a high

40:09

powered aerobatic airplane, you're going to have to use the rudder.

40:12

to prevent motion

40:16

Okay, and you'll have to use the Allen's because

40:19

you don't want this to happen either.

40:22

I want to go around the lip. And so even though you're

40:25

only the only emotion is

40:28

Is pitch it doesn't mean the only control?

40:32

is elevator

40:34

Controls are used to prevent as well as to initiate motion.

40:41

And so

40:45

so we've said all this this morning so I won't I'll just

40:48

go through the quick as a quick revision.

40:51

State of motion speed and direction is what

40:54

motions all about.

40:56

A force is a pusher or pull that attempts to change motion.

41:00

and forces that act on aircraft lift drag

41:03

thrust

41:06

and white

41:09

Okay and a little bit more to say about

41:12

lift and drag.

41:14

as the air flows across the wing

41:16

we get a total reaction.

41:19

Which can be then resolved into two separate forces

41:22

or imaginary forces.

41:26

called

41:28

and right angles to the role of air flow lift parallel

41:31

to the relative air flow.

41:34

drag

41:35

infectious shooting me once

41:38

white is lifted right angles to the relative air

41:41

flow.

41:43

And I said because I said so.

41:47

Why why because it

41:50

don't lift doesn't exist.

41:53

I just decided that that part of it that does

41:56

act it right angles.

41:58

I will call that lift.

42:00

We chose we chose to do that. That's that's not a

42:03

law of nature.

42:05

And so

42:10

we've already once once I've established lift

42:13

and drag then I can forget about the total reaction.

42:18

So we'll be doing that a lot.

42:21

now

42:23

for people

42:25

watching this video

42:28

will now on suggesting that you should stop hit the

42:31

pause button.

42:33

And try exercise A1 on page 17 of their

42:36

Dynamics book, you'll find the answers are fully

42:39

explained on page 17.

42:46

So now we'll move on to the next part of

42:49

what we want to say.

42:51

and that is

42:55

how does lift get made in the first place?

42:58

What what causes lift to be generated?

43:02

So there are a number of different ways we

43:05

can consider it.

43:08

for example

43:11

Isaac Newton said

43:13

For every action, there's always an opposite reaction Philly

43:16

well known statement.

43:19

Which originally was Isaac's contribution?

43:23

so when the air before the air hits the wing

43:26

it's traveling in the direction indicated.

43:30

by that Arrow

43:32

and the end result

43:35

when the air leaves the wing it's been deflected.

43:38

And it's now changed its direction

43:41

and its speed.

43:45

Now that that's the action the action is the air before

43:48

the wing was traveling and that direction and after

43:51

the wing it's traveling in that direction.

43:55

Now Isaac said you can't have an action without a

43:58

reaction.

44:00

So if you've deflected the air downwards.

44:03

Then you'll deflect the wing up and back.

44:07

So most of this again has gut feeling it's

44:10

like it makes common sense to say that.

44:14

There that's called the total reaction. It pulls

44:17

the wing both up and back.

44:21

But one thing that that Casa say

44:24

because you're here to try to pass an

44:27

exam.

44:28

And Casa syllabus is clearly that you

44:31

should be able to explain lift production.

44:35

By referring to a man called Mr. Benealy.

44:40

And talk about his contribution.

44:46

So

44:48

Mr. Benealy said

44:52

that

44:55

pressure

44:57

The pressure in a gas we've already said this now we can start taking

45:00

some advantage of what we said earlier.

45:03

The pressure in a gas is due to molecules that hit

45:06

the surface.

45:09

And so he's one individual molecule it

45:12

hits the surface and when it hits

45:15

the surface it applies.

45:17

a pressure on that surface

45:20

But manually also said something else.

45:24

He said if the molecule hits the surface and the

45:27

air isn't isn't actually traveling anywhere. It's

45:30

staying still.

45:32

Then the molecules are hitting the surface.

45:35

And that way and that fashion.

45:38

but if the air starts to move

45:41

then the molecule while it's coming down is also going forward.

45:45

And so it hits the surface like that.

45:49

It comes down hits the surface and goes up now that

45:52

means

45:54

That if it hits the surface and a glancing Blow instead

45:57

of straight down it won't push

46:00

so hard.

46:02

So what ultimately what he said was if it

46:05

starts to move across the surface?

46:08

Then the pressure it exerts on that surface will be

46:11

reduced.

46:13

because the molecules of air are now hitting

46:16

at an angle instead of straight down because of

46:19

the forward motion.

46:21

of the air

46:23

and so

46:25

an interesting principle is

46:28

this

46:30

so here it is just as a bit of a

46:32

a simple animation

46:35

stationary air

46:36

means the molecules doing that.

46:41

And so they're applying a fairly strong force on the surface.

46:46

but moving air

46:48

the molecules are doing this.

46:52

And so they don't press down so hard.

46:55

But it reduces the force pushing downwards.

46:59

So it basically said if you travel if you start

47:02

to speed the air up.

47:04

Then it will have less pressure. It will exert less pressure.

47:08

And we can prove that and Engadget called a

47:11

Venturi.

47:13

A Venturi is nothing more than I Hollow pipe

47:16

with a narrow neck in the

47:19

middle.

47:21

and as the air flows through that Venturi

47:25

the air has to speed up to get through that narrow

47:28

Gap.

47:29

In the same way that a river has to speed up when

47:32

the banks come closer together and the Rapids form.

47:37

and so

47:39

when air flows through the Venturi it flows

47:42

in that fashion.

47:44

faster in the middle

47:48

and this area where the air is traveling faster means it

47:51

doesn't have enough time to press sideways. It's

47:54

too it's too much

47:57

of its energy is going into forward motion.

48:00

And I can't press sideways as hard.

48:03

so if I turn to this Blackboard

48:06

and I say I'm going to push on the Blackboard like that.

48:10

Then I can push pretty hard.

48:13

But if you change the rules and say I've got to walk past

48:16

and push.

48:18

Then I can't push this hard anymore because some

48:21

of my energy is going into forward motion.

48:24

and therefore the pressure

48:27

in the narrow part of the Venturi B

48:31

drops

48:35

and then an increases again as the air comes out the other end.

48:39

now if we connect a pipe to that and that

48:42

point

48:43

That will produce.

48:45

a suction

48:47

that low pressure will produce a suction exactly

48:50

the same effect as if you put a

48:53

drinking straw in your milkshake and suck on

48:56

it and you suck the the liquid up.

49:01

in fact carburetors use this

49:03

as a means of sucking the fuel into the engine.

49:08

And so that's the Venturi.

49:12

if speed increases

49:15

then pressure will decrease and I can

49:18

use that a little illustration again.

49:21

If that string represents the total energy that the

49:24

air has.

49:27

Then some of it is speed.

49:31

And some of it is pressure.

49:34

But if you the length of a string

49:37

doesn't change the total energy doesn't change. So

49:40

if speed increases the pressure has

49:43

to decrease.

49:45

and speed decreases

49:47

The pressure has to increase.

49:49

That's what you know, Mr. B nearly was saying

49:52

by the way, I might add that must have been nearly.

49:56

was

49:57

was born and lived and died long before airplanes ever

50:00

flew. He wasn't trying to build an airplane.

50:04

He was mainly interested in the flow of water.

50:07

And he's interested in rivers and dams and

50:10

things like that, but his rules

50:13

still apply to subsonic air.

50:18

And here's an example. Otherwise, this

50:21

is a target moth and out

50:24

on the side. We see.

50:27

a beautiful example

50:29

of a Venturi

50:33

and through that

50:35

through that little pipe coming in from the side to the

50:38

narrowest part.

50:41

That's causing a suction, which is sucking air.

50:46

And that's sucking air out of a gyro.

50:50

So what what it does by the by the way is something like this?

50:54

Imagine we have a wheel.

50:58

Imagine we have a wheel.

51:03

And it has a little buckets cut in it.

51:07

that

51:12

and we put that in our case.

51:17

And we put a little jet here.

51:23

That's a little nozzle.

51:25

And a filter to keep everything clean.

51:30

And then we connect this to a Venturi.

51:35

And his egg goes through the Venturi.

51:38

It creates a low.

51:40

pressure

51:41

and it sucks air out.

51:44

And that means fresh air.

51:46

Gets pulled in.

51:49

Through the through this.

51:53

And it comes out and hits the buckets.

51:56

And that makes the jurors spin.

51:59

So by the this in in a

52:02

tiger moth, which is what that airplane is.

52:05

And that I don't have a vacuum pump. We have

52:08

a vacuum pump. That's run by the engine.

52:12

But eventually works perfectly. Well, it

52:15

sucks the air out of that case and makes the door

52:18

spin.

52:20

And that's the instrument that it runs.

52:24

the turn and Bank indicator

52:30

okay, and so

52:33

what what?

52:36

Benue's theorem says is as the

52:39

air flows over the top of the wing it travels faster.

52:43

And as it flies underneath the wing if anything

52:46

it slowed down a little.

52:48

And so we get a low pressure area above the wing.

52:53

And that means there'll be a force acting up.

52:58

The total reaction now. I'm sure in your

53:01

life as you progress. You're going to

53:04

hear instructors.

53:06

Who challenge that and say

53:09

that being really fear and can't be

53:12

used to explain to fully explain lift.

53:15

We're not here to get involved in philosophical arguments. We're

53:18

here to pass an exam and so it cast

53:21

aside that that's how it works.

53:23

So at least we should be able to we should at

53:26

least be able to say how the newly's theorem

53:29

could be applied.

53:30

But there's a strong argument among people

53:33

now that

53:34

that it isn't really a full explanation.

53:37

of lift generation

53:42

However, you should know the principle behind.

53:45

the newly's lift Theory

53:50

So anyway, whatever whatever

53:53

the magic is that causes lifts to be

53:56

made.

53:57

There are some basic things that we need to know.

54:01

Anything any shape that's designed to

54:04

make lift.

54:06

It's called an aerofoil. So you'll hear

54:09

that phrase used a lot from now on.

54:12

The airfoil has got some names that we need to be sure of.

54:16

The front of the era foil is called the Leading Edge.

54:20

The back is called the trailing Edge.

54:23

The straight line that joins the trailing Edge to the

54:26

leading to the center of curvature of the Leading Edge.

54:30

It's called the chord line.

54:34

But his very interesting point most people know

54:37

that already.

54:39

The chord line is used by the way to measure the angles.

54:42

like angle of attack

54:45

because the wing is curved.

54:48

generally

54:49

And so that we need a straight line to measure an angle.

54:53

So the cord line is Handy.

54:56

If you want to be accurate and measure angles.

55:00

Now if you draw this is interesting, right if

55:03

you draw a whole lot of lines across the cord and

55:06

they're all at right angles to the cord.

55:11

And then I find the midpoint.

55:14

of each one of those short lines

55:17

each one of those lines going across

55:21

I find the exact middle of them.

55:25

And so I do that put a little dots there all those dots

55:28

are exactly halfway along the line.

55:32

and so those dots

55:34

is why join them?

55:36

I get a line like that. Call the main Campbell line.

55:41

and that

55:43

that line that line always remains the

55:46

same distance.

55:48

Between the top and bottom of the wing at any

55:51

given point that line is the same distance from

55:54

the top and the bottom.

55:57

It's called the candle on.

56:00

and

56:02

when we

56:05

talk about a wing having camber.

56:08

we talk about

56:10

the separation

56:12

between the chord line

56:14

and the cameline

56:18

and we've if we find the point where that separation

56:21

is that it's greatest.

56:24

So let's say let's say it's about

56:27

there.

56:28

backs maximum separation occurs

56:31

at that point

56:36

then that's what we mean by kamba.

56:39

Kamba is telling us.

56:42

How far what is the greatest distance or separation?

56:47

between the Campbell line and the chord line

56:52

now another thing that designers do

56:55

and have done for many years.

56:57

We like to put Wings in Wind tunnels and test

57:00

them.

57:01

But that's a very expensive business big wind

57:04

tunnels. Don't come cheap.

57:07

And so

57:09

What are we discovered was?

57:11

If you make an exact model of your wing.

57:14

And keep all those proportions the same.

57:18

If you keep all those distances exactly the same

57:21

you can build a smaller version of the wing.

57:25

And you can put it in the Wind Tunnel.

57:27

And you can get valid results about how

57:30

it's going to behave have a real Wing will

57:33

be Hive in other words what you're

57:36

really saying is you can test this shape.

57:39

With any size and then you

57:42

can scale it up or down and you'll all the data will

57:45

be valid.

57:46

It'll still be correct.

57:49

And so when they build a wing they

57:52

made this rule up years ago.

57:55

The chord the red line there the chord

57:58

line.

58:00

becomes

58:02

the basic

58:03

basic measurement of everything the cord

58:06

everything else is expressed.

58:09

As a percentage of the chord instead

58:12

of a number of millimeters.

58:16

Because by expressing it as a percentage of the chord.

58:19

Then I can if I keep those percentages the same

58:22

I can make the wing bigger and smaller and

58:25

be the same shape.

58:27

It'll always be the same shape even though it's bigger or smaller.

58:31

And so they express everything as a

58:34

percentage.

58:35

That means that a designer if we

58:38

could leave drop on a all the designers

58:41

having a coffee break.

58:43

That'd be talking about I'm working on a wing

58:46

that's 12% thick.

58:50

What do I mean by 12% think?

58:53

They mean the thickest part of the wing is 12% of the cord.

58:59

All right, and I'm working on a wing that's 12% thick

59:02

at 30%

59:07

if it's 12% thick at 30%

59:10

then it's 12%

59:12

The maximum thickness is 12% and it

59:15

occurs 30% down the cord.

59:18

So it's a really cool way to explain everything you want to

59:21

say about that wing.

59:23

And more importantly, it'll say what's this distance here?

59:30

and he might say

59:32

This ring has got a 4% camber.

59:37

A 4% camber would mean that that distance had separation

59:40

is 4% of the total chord.

59:45

And it's 4% camber at?

59:47

40%

59:50

telling you where it is as well.

59:52

So it's a really clever way to fully describe

59:55

the wing.

59:57

And then if someone wants to build it.

59:59

All I have to do is get all those percentages.

1:00:03

and I might get any Source they like

1:00:07

And they don't have to go they don't have to put it in the Wind Tunnel

1:00:10

again.

1:00:11

The wind tunnel tests are valid.

1:00:15

and so

1:00:18

we'll hear a lot more about percentages of chord.

1:00:21

as we go into performance ladder

1:00:24

and discuss that

1:00:26

but

1:00:31

so if you wanted to build a wing

1:00:33

they keep all these wind tunnel tests and NASA did

1:00:37

them all they keep all these wind tunnel tests in big

1:00:40

computer.

1:00:42

So I could write a letter and say I guys

1:00:45

I want to Wing that'll do this.

1:00:48

And I'll tell them how I want my wing to behave.

1:00:51

And they gave such the database and they

1:00:54

find the wing that's close. Most closely resembles

1:00:57

the one I want.

1:00:59

And they say railroad we found your

1:01:02

wing.

1:01:03

Do you want it and you say yeah, please

1:01:06

I'll have it and they say enter your bank

1:01:09

card details.

1:01:12

and all I send you

1:01:14

Is all the percentages?

1:01:18

All right, and then you go down the backyard and build that wing.

1:01:21

according to those percentages

1:01:24

and you've got a wing now that you know how

1:01:27

it's going to behave it's been tested.

1:01:30

That particular shape has been tested.

1:01:33

So it's really smart idea.

1:01:37

So don't be frightened. By the way. Those numbers are just gave you

1:01:40

with a fairly typical of most general aviation Wings.

1:01:43

They're mostly about 12% thick and

1:01:46

they mostly about 4% camber. They're very

1:01:49

a bit but

1:01:51

That's pretty close.

1:01:54

Except there are some special.

1:01:58

Wings, for example, I can build a wing

1:02:01

with no camber.

1:02:03

Now a lot of people think camber is

1:02:06

like thickness.

1:02:07

But that's that's not true Fitness isn't

1:02:10

Canberra. I can have a thick wing with no camber.

1:02:14

Because this is how I build a wing without camber.

1:02:17

I simply make.

1:02:20

The top and bottom a mirror image of each other.

1:02:25

and so the now

1:02:27

the chord line is the candle line.

1:02:30

Because the chord line is equal distance from the top and

1:02:33

bottom surface.

1:02:35

as well

1:02:36

so that Wing has zero can but doesn't have zero thickness.

1:02:40

It is there a canva?

1:02:44

We call it a symmetrical airfoil.

1:02:48

It would have some serious disadvantages.

1:02:51

because without camber

1:02:53

the only way it can make lift.

1:02:56

Is by having an angle of attack a fairly big angle of attack?

1:03:00

Whereas a candid Wing can make lift it

1:03:03

no angle of attack because it's got that shape over

1:03:06

the top.

1:03:08

But but some airplanes do use symmetrical aerofoils.

1:03:13

Some aerobatic airplanes. I spent a lot of my time flowing

1:03:16

a pit special and that aerobatics

1:03:19

and things and their foil

1:03:23

is

1:03:24

In the case of the pit special. It's pretty much exactly

1:03:27

symmetrical.

1:03:29

and the idea of a symmetrical aerofoil of

1:03:32

course means

1:03:33

if you want to fly upside down.

1:03:36

Then a cambod Aero foil is a disadvantage because it's

1:03:39

making lift the wrong direction.

1:03:42

You need a very big angle of attack to fly upside down.

1:03:46

And so there are many

1:03:49

aerobatic airplanes have

1:03:51

symmetrical or very nearly symmetrical

1:03:55

wings and of course, don't forget there are

1:03:58

some aerofoils their aerofoils beside Wings. What about

1:04:01

Rutters and elevators?

1:04:04

an irons

1:04:06

well

1:04:08

It would make sense that they should be symmetrical.

1:04:11

Because sometimes I go one way sometimes they

1:04:14

go the other we don't want to have it favoring one myth One

1:04:17

Direction.

1:04:19

and so

1:04:21

symmetricular foils are effective life

1:04:24

and they do exist.

1:04:30

in the case of the symmetrical aerofoil

1:04:33

the cordliners the candle line

1:04:40

a sign

1:04:45

so no angle of attack. It makes no lift.

1:04:55

I was decided aerobatic students.

1:04:58

A symmetrical aerofoil Works equally

1:05:01

badly on the way.

1:05:04

It doesn't allow you to fly upside down.

1:05:07

But you pay the price when you want to fly the right way up.

1:05:10

So it works equally badly.

1:05:16

Okay.

1:05:18

Now another thing we need to say a little bit about

1:05:22

and this is really important area actually.

1:05:26

and that is

1:05:28

as the air flows across the wing

1:05:32

air has another property by the way that we often forget about.

1:05:36

We call it viscosity.

1:05:38

now a lot of people would be surprised if I

1:05:41

had me say

1:05:42

that they're a sticky.

1:05:46

But again, that's because we live here.

1:05:48

And we're used to it. There is sticky stuff.

1:05:51

If you've got a ceiling fan.

1:05:54

the ceiling fan spins around

1:05:57

and it drags here with it.

1:05:59

But pretty soon all the air in the whole room is moving around

1:06:02

and the fans not doing it the fans

1:06:05

Not hitting all the air.

1:06:07

It's stirring it up and the rest and the air is

1:06:10

dragging the rest of it with it. It's sticky like, honey.

1:06:14

On not as bad as that, but it's the concept

1:06:17

it has viscosity.

1:06:20

And so when the air flows across the wing the air

1:06:23

at the very very surface if we

1:06:26

get right down to the scale of a molecule.

1:06:29

The air at the surface of the wing actually sticks

1:06:32

to the wind.

1:06:35

And then the air above that.

1:06:37

if this represents the wing

1:06:42

the air right at the bottom of the wing is actually

1:06:45

stuck to the wind

1:06:47

at the scale of a molecule is actually stationary.

1:06:52

And then the air above that is moving a little bit.

1:06:56

And the air above that a bit faster.

1:06:59

And so that happens until they get

1:07:02

far enough away for the wing to have no effect.

1:07:06

But you have this region in here.

1:07:09

Where the air is?

1:07:11

Actually, it's flowing in layers.

1:07:14

The bottom layer is still the layer above

1:07:17

that is moving slowly the layer above that

1:07:20

a bit faster a bit faster a bit faster. And then finally

1:07:23

it's too far away to be affected.

1:07:26

Now I'm gracefully exaggerating that.

1:07:29

The thickness of that we're talking about is like a

1:07:32

couple of millimeters.

1:07:35

It's not nothing like what I've drawn.

1:07:38

And we call that laminar flow.

1:07:48

So it's very orderly.

1:07:50

There's no mixing.

1:07:52

the air at the bottom

1:07:55

So if you are a molecule.

1:07:58

And you were down on the bottom.

1:08:00

There'd be no wind.

1:08:02

They could have a barbecue.

1:08:05

All right, the wind is all happening above your head.

1:08:09

And so

1:08:12

However, the laminar flow doesn't persist.

1:08:15

for the whole length of the journey

1:08:18

the laminar flow tends to stay laminar

1:08:21

while the wing is getting thicker.

1:08:24

In other words well over the air is going uphill.

1:08:29

Here it's there's going uphill.

1:08:32

Whether it's going uphill the rest of the air is trying to push

1:08:35

down on it.

1:08:36

So it stays lamina.

1:08:39

But as soon as the air tries to go downhill.

1:08:44

Then it doesn't stay laminar. It starts

1:08:47

to Tumble.

1:08:49

Now don't confuse that with stalling.

1:08:52

It doesn't leave the wing.

1:08:54

It just rolls the rest of the way Lord ball

1:08:57

bearings.

1:08:59

If you want to see laminar Flow, by the way.

1:09:02

Don't get in the kitchen and turn the tap on

1:09:05

if you turn the tap on just a tiny bit. The water

1:09:08

comes out is a beautiful clean strain.

1:09:11

If you keep turning it suddenly it'll

1:09:14

break up into rum into rumbling water.

1:09:17

into sort of frothy water

1:09:19

if the first little bit of turning on

1:09:22

a tap the water comes out as laminar flow and

1:09:25

when you turn it a bit further, it becomes turbulent changes

1:09:28

this whole appearance.

1:09:31

and

1:09:32

this becomes

1:09:34

turbulent flow

1:09:44

turbulent flow

1:09:47

and this point here where the changes it changes

1:09:50

quite suddenly usually

1:09:53

from laminar to turbulent

1:09:55

That point is called transition point.

1:10:12

Now turns out.

1:10:14

As you can see from this drawing.

1:10:17

that the lamina flow

1:10:19

the flow stays laminar

1:10:22

Whatever the airfoil is getting thicker.

1:10:25

While over the air is going uphill.

1:10:28

As soon as the air starts to go downhill.

1:10:31

it tumbles and

1:10:33

it stays on the wing so it's not stalling. This is

1:10:36

only happening in a couple of millimeters.

1:10:38

And it becomes turbulent for the rest of the journey.

1:10:43

Ultimately, of course to the whole airflow will separate

1:10:46

completely off the wing. That's a stall

1:10:49

that's the turbulent flow isn't

1:10:52

a still it's just a different way of

1:10:54

moving across the wing

1:11:01

Okay, don't confuse it.

1:11:04

with stalling

1:11:08

now

1:11:09

there are some Advantage for high-speed flight.

1:11:14

There are some advantage.

1:11:16

in

1:11:20

Keeping the airflow laminar.

1:11:23

for a longer time

1:11:25

because that actually creates less drag.

1:11:28

You can probably but you can see that if there's

1:11:31

turbulence there's got to be more energy being used up and so

1:11:34

drag if you could keep the airflow laminar.

1:11:38

Then it will.

1:11:40

It will reduce the total drag and we already

1:11:43

saw that that's pretty important.

1:11:45

If you can reduce drag.

1:11:48

and so

1:11:50

we can build a wing that is designed to

1:11:53

keep the airflow laminar.

1:11:56

And we do it like this.

1:11:58

We the flow will stay laminar

1:12:01

while over the aerofoil is getting thicker.

1:12:04

So why don't we put the thickest part further back?

1:12:09

Why don't we have the point of Maximum camber at

1:12:12

about 50% of the cord?

1:12:15

And so that means it'll stay on

1:12:18

her longer.

1:12:22

And so that's called a laminar air flow

1:12:25

aerofoil.

1:12:27

A normal cambered aerofoil looks like that.

1:12:32

That's the typical general purpose thereofoil.

1:12:36

A laminate floor will look like that.

1:12:45

And also it makes some sense.

1:12:48

To keep this part of where wallet is going uphill.

1:12:53

That means more of the wing will have lamina flow.

1:12:58

And it makes some sense to keep that really smooth and clean.

1:13:02

Because that'll help it style lamina.

1:13:05

So usually the wing will be flush riveted.

1:13:08

For that part of the Winking will be flush riveted and

1:13:11

the nice smooth polished surface.

1:13:14

And then down the back here. They often go back to roundhead rivets

1:13:17

because they don't care anymore.

1:13:23

And of course the symmetrical airflow we know

1:13:26

about now, here's a case of a lamina error foil.

1:13:30

And this is Papa. I'm sorry. This is a Mooney.

1:13:35

And if you look at that airport, you see

1:13:38

where's the thickest part?

1:13:40

Well, it is it's probably half. It's probably halfway down.

1:13:44

And and also when you look up close.

1:13:48

The all the front part of smooth and the

1:13:51

back part has got the roundhead rivets.

1:13:55

But the front part is kept very smooth and Polished.

1:13:59

Here's a Cherokee 140.

1:14:02

notices laminar flow

1:14:05

You can see that really clearly. The thickest part

1:14:08

of the wing is at least halfway down.

1:14:11

That's a fairly unusual Wing show.

1:14:18

and

1:14:19

Interesting, by the way that Piper ended up

1:14:22

going back to normal aerofoles.

1:14:27

So he tried he tried lemon a flow.

1:14:30

as a sort of fashion statement

1:14:34

and then he found that it doesn't

1:14:37

make that much difference. You know, why because lemon flow

1:14:40

doesn't really have any big effect until you

1:14:43

start talking about 300 knots or faster.

1:14:47

You can bet every year or every airliner will have

1:14:50

lemon flow.

1:14:52

but Lord aircraft

1:14:54

blood aircraft that is more of a fashion statement. Oh look

1:14:57

at me. I've got a lemon flow wing.

1:15:00

But so what it's probably

1:15:03

not much better than any other wing.

1:15:11

So there's the thickest part of the chord.

1:15:14

halfway down the wing

1:15:18

so you can tell you can pick a line on the floorboard looking at it. You

1:15:21

can tell what sort of wing it is.

1:15:28

Okay. Now a few other little things I hear about angle

1:15:31

of attack.

1:15:34

You know this from PPL.

1:15:37

the angle of attack is defined as

1:15:41

the angle between the chord

1:15:44

line

1:15:45

and the direction of the role of airflow

1:15:49

most light aircraft when they're in Cruise

1:15:52

would have an angle of attack of something like two degrees.

1:15:55

Not much.

1:15:57

Just a little tiny angle of attack.

1:16:00

Because the speed is making the lift. You don't

1:16:03

need a lot of angle of attack.

1:16:07

if I

1:16:08

if I present the wing at a bigger angle to the

1:16:11

airflow.

1:16:13

Then the angle of attack.

1:16:15

has increased

1:16:20

and if I presented an even bigger

1:16:23

angle of attack.

1:16:28

So the that's what we mean by angle of attack.

1:16:31

the angle of attack

1:16:33

Is the angle between the direction and by

1:16:36

the way, the direction of the role of airflow is really the direction you're

1:16:39

flying.

1:16:41

It's the direction you're flying compared to.

1:16:45

the code line of the wing

1:16:50

sometimes if you want to sound really cool.

1:16:53

And impress the girls.

1:16:55

Then scientists talk about Alpha.

1:16:59

All right. So that's a always make sure

1:17:02

I say that if I'm at a conference or

1:17:06

I had a pretty high alpha.

1:17:08

today

1:17:09

All right, and I increased Alpha is

1:17:12

just a flash drive saying angle of attack.

1:17:15

People like to say it if they want to impress everybody is to

1:17:18

how clever they are.

1:17:22

Okay.

1:17:24

Now the next thing we want to look at.

1:17:26

Is again very simple.

1:17:29

It's angle of attack and inertia.

1:17:33

for example

1:17:34

Here is a way now. What's this carefully? It's and

1:17:37

it's an animation.

1:17:38

But you need to look carefully to notice.

1:17:41

If the wing is moving through the

1:17:44

air and the pilot now pulls back

1:17:47

on the elevator.

1:17:49

And that makes their airplane pitch nose up, but

1:17:52

here's the important thing even though the airplane

1:17:55

pitched nose up.

1:17:58

For a little while. It keeps flying.

1:18:00

down the same path

1:18:03

that's called inertia.

1:18:05

every object in the universe

1:18:08

takes a while before it changes.

1:18:11

And so if I'm flying like that might be better

1:18:14

than you put it on this side.

1:18:16

If I'm flying like that, and I suddenly

1:18:19

pull the nose up.

1:18:22

I'm exaggerating it. Now then for a

1:18:25

few seconds, you're a plane keeps going on that same path.

1:18:30

And therefore you get a big increase in angle of attack, especially

1:18:33

if you do it suddenly if the airplanes

1:18:36

flying like this and I pull back on the controls the

1:18:39

nose comes up, but initially it

1:18:42

keeps going but then of course it'll get more lift.

1:18:45

And So eventually it'll start to

1:18:48

climb.

1:18:49

But this little period is what we're interested in this period

1:18:52

where I pull the nose up.

1:18:55

And for a little while, it doesn't do anything except keep going.

1:18:59

That's a natural consequence because of

1:19:02

the problem of inertia.

1:19:06

And so

1:19:08

That's got some interesting effects. There's with we'll talk

1:19:11

more about later.

1:19:13

So this happens the airplane is going to fly.

1:19:18

along that direction of flight

1:19:22

and if you looked at that carefully, I'll just do it again.

1:19:25

You'll notice that even though the nose even though

1:19:28

the airplane pitched those up.

1:19:30

It still kept going on the same path.

1:19:33

And so it ends up.

1:19:37

That's an important point.

1:19:40

It keeps going on the same path briefly.

1:19:45

angle of attack

1:19:47

increases

1:19:54

so the angle of attack gets greater.

1:19:57

because of inertia

1:20:01

now important another important point

1:20:04

don't confuse angle of attack with nose attitude.

1:20:10

The nose attitude of an airplane is the

1:20:13

relationship between the nose and the Horizon outside.

1:20:20

So the angle of attack

1:20:23

is the angle between the chord line and the

1:20:26

relative air flow so in level float, of

1:20:29

course.

1:20:30

The Horizon would give you a pretty good idea of the angle of

1:20:33

attack because you're going level anyway

1:20:37

however, if I'm climbing

1:20:40

it's possible to have a high nose attitude.

1:20:45

and a small angle of attack

1:20:50

pretty obvious, right? Just because the noses High

1:20:53

doesn't mean you've got a high angle of

1:20:56

attack.

1:20:58

Of course.

1:21:00

If you're flying level in the nose is high then you

1:21:03

have a high angle of attack.

1:21:06

But it's possible to have.

1:21:09

a high nose attitude and a low

1:21:12

angle of attack

1:21:14

because the angle of attack is not interested in the horizon.

1:21:18

It's just it's working on which way you're flying.

1:21:22

and the same thing for a descent

1:21:26

If I'm descending, I have a low nose attitude.

1:21:29

But that doesn't always mean I've got a low angle

1:21:32

of attack.

1:21:34

In fact, we could talk about this briefly in a minute.

1:21:37

It's possible for that to be a dangerous thing.

1:21:42

because if I

1:21:44

just because the noses below the Horizon doesn't mean you don't have

1:21:47

a high angle of attack.

1:21:49

And we all know that an angle of attack is what causes the stall we

1:21:52

certainly got a lot more to say about that as we

1:21:55

progress.

1:21:57

But you should know that from people.

1:22:00

And so therefore don't confuse

1:22:03

those attitude.

1:22:05

with angle of attack

1:22:08

Now there's a very interesting way that we can study this

1:22:11

in great detail.

1:22:13

And we do it by creating a thing called a

1:22:16

wind tunnel.

1:22:19

A wind tunnel allows you as we said

1:22:22

earlier.

1:22:23

It allows them to test the model of the airplane.

1:22:27

And therefore predict exactly how the real airplane will

1:22:30

behave.

1:22:33

And so we put the airplane in the wind tunnel and we

1:22:36

blow the air on it.

1:22:38

And then we change the angle of attack notice by

1:22:41

the way.

1:22:42

This is going to become important.

1:22:45

That can only be done in the Wind Tunnel.

1:22:49

The only way I can I can check the angle of

1:22:52

attack alone.

1:22:54

Just the angle of attack changing.

1:22:57

because if I try to change the angle of attack in Flight, I'll

1:23:00

change the flight path and everything goes

1:23:03

ape s*** as they say right if I

1:23:06

try to change the angle attack in level flight everything go

1:23:09

everything else changes the only one way

1:23:12

for a designer.

1:23:15

to study angle of attack alone

1:23:19

And that's put it in the Wind Tunnel turn the wind on at a

1:23:22

certain speed and then rotate the airplane in that

1:23:25

wind.

1:23:27

You can't do that in a rural airplane the moment you try.

1:23:30

You're going to change the speed and direction and

1:23:33

so it's very hard to know what the hell's going

1:23:36

on.

1:23:37

So that's the beauty of a wind

1:23:40

tunnel. It allows me to do what I can't do in a

1:23:43

real airplane.

1:23:44

It allows me to watch how the angle of attack is behaving

1:23:47

and what effect it's having alone with

1:23:50

everything else constant.

1:23:54

and

1:23:56

that's a smaller cheaper version.

1:24:00

For testing notice, by the

1:24:03

way, they actually in the Wind Tunnel actually suck the air out

1:24:06

of the tunnel.

1:24:08

And the ear that comes in and is nice and smooth.

1:24:11

If you have the propeller up the front the air

1:24:14

coming in would be spiraling and that it

1:24:17

spoil it all.

1:24:18

So they actually suck the air out of the back and then

1:24:21

pull nice smooth there.

1:24:23

to pass over the wing

1:24:27

Now here are some actual wind tunnel tests.

1:24:29

And the beauty of it is we can now see

1:24:32

very clearly What's Happening by introducing

1:24:35

smoke?

1:24:37

With little nozzles in the Wind Tunnel they can

1:24:40

introduce smoke into the wind.

1:24:42

And then we then it all becomes visible. These are

1:24:45

actual movies of actual wind tunnels.

1:24:48

And so we see this happening.

1:24:52

We rotate the wing.

1:24:58

Only the angle of attack is changing.

1:25:01

You see how the air now is separating?

1:25:04

The stall is occurring.

1:25:11

That's not laminar and turbulent flow. That's there is

1:25:14

actually completely breaking away from the wind.

1:25:20

Now here's a big danger.

1:25:23

And this is where it becomes a safety issue.

1:25:27

I'm diving down on the ground at the ground.

1:25:31

And then I pull the nose up.

1:25:34

Now I'll do that again so you can watch it again slot carefully.

1:25:39

What happens to this guy? He's diving at the ground. Now, this

1:25:42

is something that's really important. We call it

1:25:45

ground Rush.

1:25:46

and for many years I was the

1:25:49

test officer for low level aerobatic training

1:25:52

and so when people wanted low level

1:25:55

aerobatic approval to do air shows and

1:25:58

things

1:25:59

On tests are appointed me as the guy who does

1:26:02

the test and but one of the things you check is.

1:26:06

This idea of grand now doesn't happen up high if

1:26:09

you're at 3,000 feet and you're diving

1:26:12

at the ground.

1:26:13

you can't even see the grounds too far away to take

1:26:16

much notice of

1:26:18

but if you're at 300 feet and you're

1:26:21

diving at the ground all of a sudden the

1:26:24

ground starts to expand in the windscreen.

1:26:27

now if you haven't had that experience that can

1:26:30

be really bad news because people

1:26:33

People overreact they see the ground

1:26:36

expanding.

1:26:37

The ground expands in all directions are

1:26:40

about the point where you're going to hit.

1:26:43

So you're looking through the windscreen and everything looks good

1:26:46

for a while and then all of a sudden the ground goes.

1:26:49

And and what and someone who hasn't

1:26:52

been trained says oh s***, and he pulls like

1:26:55

mad on the control column. That's exactly what it's just

1:26:58

talking about the airplane pictures up, but it keeps

1:27:01

going

1:27:02

and all he's done is increase the angle of attack and if

1:27:05

he happens to go through the stalling angle.

1:27:08

Then he's going to end up with less lift.

1:27:11

Instead of more and he's made it

1:27:14

worse not better.

1:27:16

They call it ground Rush. It's a psychological effect.

1:27:20

It's an optical illusion really but it's

1:27:23

a very powerful one if you haven't experienced it.

1:27:26

It'll only happen if you diving deeply at the

1:27:29

ground and also very low, so hopefully you won't be

1:27:32

doing it for a little while. But if you do yeah a low

1:27:35

level neurobatic rating one day.

1:27:37

It's a real thing. I've got some movies later. I'll show you of doing

1:27:40

a loop at 300 feet instead of

1:27:43

at 3,000 feet.

1:27:46

And so this is what happens. I pulled back why it gets

1:27:49

the angle of attack increase now if that

1:27:52

angle of attack goes beyond the stalling angle.

1:27:55

Then he goes.

1:27:57

He's got a problem.

1:28:01

And so we can now check this.

1:28:05

And I'll just finish we'll just get this in before we

1:28:08

have a short break.

1:28:09

as a result of the Wind

1:28:12

Tunnel tests

1:28:14

I can draw a graph.

1:28:17

And in this exam by the

1:28:20

way, the examiner is going to give you graphs.

1:28:22

And he's going to ask you to interpret the graph very simply.

1:28:26

But for example along here

1:28:29

we put angle of attack.

1:28:32

increasing

1:28:33

and up here. We put lift increasing.

1:28:37

Right and then in the wind tile now, this is important. We

1:28:40

keep the speed the same now, you

1:28:43

can't do this in a real airplane.

1:28:45

We have the speed on the same speed and we

1:28:48

just rotate the wing.

1:28:50

and say the lift does this

1:28:53

It goes up and as angle of attack increases.

1:28:57

the lifting creases

1:28:59

and then it reaches a peak.

1:29:03

And that Peak is called seal Max the maximum

1:29:06

lift coefficient. The wing

1:29:09

is now making the greatest possible amount of

1:29:12

lifted leather make

1:29:14

at that speed