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ID: 3658

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

CHAPTER 13: THE STALL AND SPIN

TAS always represents the actual speed of the aircraft through the air.

On the other hand, as you learnt in Chapter 4, Airspeed Indicators (ASI) ftted to aircraft are calibrated to read TAS in ICAO Standard Atmosphere sea-level conditions only, where the air density, ρ, is 1.225 kg/m³.

For any given TAS, if ρ decreases below 1.225 kg/m³, the corresponding Indicated

Airspeed (IAS), the speed that a pilot reads from the ASI, will decease too.

Consequently, because ρ decreases with increasing altitude (mostly because pressure also decreases with altitude), we may deduce that, in general, for any given TAS, the corresponding IAS will decrease, the higher an aircraft climbs.

What we can state with absolute confdence is that IAS is equal to TAS only when ρ

= 1.225 kg/m³; and it is a sound general assumption that, at altitude, IAS will always be less than TAS.

So, if the Pilot’s Operating Handbook for a particular aircraft tells us that the aircraft stalls at an IAS of 60 knots, what happens to the indicated stall speed that the pilot reads from the ASI, as the aircraft changes altitude?

The question is not diffcult to answer. All you have to remember is that the IAS is read from the ASI and that the ASI is actually reading the dynamic pressure, Q, that the airfow is exerting on the aircraft as it advances through that air. If you need to refresh your memory on this topic, take another look at Chapter 4.

You may recall, though, that the expression for dynamic pressure, Q, is:

Q = ½ ρ

If we examine the lift equation, we see that the expression for dynamic pressure, Q, is part of that equation. We see that:

Lift = CL½ ρv²S

and Q = ½ ρ

So, Lift = CLQS

We can also see that, at the point of stall, the dynamic pressure, Qstall, acting on the aircraft is given by the expression:

Qstall = ½ ρ(vstall

It is, of course, Qstall which determines the IAS at the stall.

So, at the point of stall,

Lift = CL MAX Qstall S

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Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

CHAPTER 13: THE STALL AND SPIN

The stalling IAS for a given

aircraft and a given weight or load factor will be the same

at all altitudes.

And because, right up to the moment the aircraft stalls, lift must equal the aircraft’s weight, we may write, for the stall:

Weight = Lift = CL MAX Qstall S

Now, an aircraft’s straight-fight stall speed is always quoted in the Pilot’s Operating

Handbook for a given all-up weight. We may deduce, then, that:

Weight is a constant, at the point of stall.

And, as Weight = Lift

Lift is also a constant, at the point of stall

Likewise, as Weight = Lift = CL MAX Qstall S

The expression, CL MAX Qstall S must be a constant, at the stall:

Finally, CL MAX is, by defnition, a constant, and, likewise, if the pilot does not alter his fap setting, wing area, S, is also a constant. It follows then that:

Qstall is a constant

And Qstall is the Indicated Air Speed (IAS) at the stall.

We may conclude, then, that an aircraft always stalls at the same IAS from straight and level fight, whatever the altitude the aircraft is fying at, even though the stalling

IAS will represent different values of True Airspeed (TAS), depending on the prevailing value of air density, ρ.

By looking again at the original lift equation for the point of stall,

Lift = CL MAX ½ ρ(vstall)² S

Where vstall is the TAS at the stall, we can see that as ρ decreases with increasing altitude, vstall (the TAS) must increase to make the lift equation balance.

However, the IAS at the stall is an indication of the term ½ ρ(vstall)² (i.e. Qstall) and the value of this term remains constant at all altitudes. Therefore the indicated stalling speed at a given weight or load factor remains constant at all altitudes.

The Effect of Aerofoil Section on the Stall.

The shape of a wing’s aerofoil section will affect the aircraft’s behaviour at the stall.

Some aerofoil sections have benign stall characteristics. With these sections the approach to the stall is gradual and undramatic, leading to little height loss and rapid recovery. Aircraft used for elementary fying training generally have wings with benign stall characteristics. With other types of aerofoil section, however, the stall can be quite vicious. Aircraft ftted with this type of aerofoil may stall abruptly, lose signifcant height and require a very positive application of the stall recovery procedure.

298

ID: 3658

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

CHAPTER 13: THE STALL AND SPIN

Figure 13.10 Some aerofoil characteristics which affect behaviour at the stall.

 

Among the aerofoil features which determine its behavioural characteristics at the

 

stall, are: leading-edge radius, degree of camber, particularly near the leading-edge,

 

thickness-chord ratio, point of maximum thickness and maximum camber. (See

 

Figure 13.10).

 

Generally speaking, the stall will be more abrupt the thinner the aerofoil section, and

A thick, highly

the further back the positions of maximum camber and maximum thickness. Figure

cambered wing

13.11 depicts graphs of CL against angle of attack for two aerofoils, the graph on the

will stall more

left representing an aerofoil with more benign stall characteristics than the graph on

gently than a

the right.

thin wing.

Figure 13.11 Graphs of CL against angle of attack. The graph on the left depicts an aerofoil of benign stall characteristics. The graph on the right depicts an aerofoil of less benign stall characteristics.

Variations of Aerofoil Section.

The aircraft designer may opt to use a wing section, at the root, which has a sharper leading edge and less pronounced camber than the section at the wing tip. The stall characteristics of such a wing would help ensure that the stall occurred at the root frst (See Figure 13.12 overleaf).

299

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Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

CHAPTER 13: THE STALL AND SPIN

Figure 13.12 Variation in aerofoil section along the wing.

Stall Strips.

You have just learnt that an aerofoil with a sharper leading-edge radius will stall before one with a more rounded, leading-edge. Consequently, some aircraft have small triangular stall strips attached to the wing leading-edge in the region of the wing root. At high angles of attack, these stall strips promote separation of the airfow, helping to ensure that the wing root stalls before the wing tip. (See Figure 13.13 )

Vortex generators

increase the kinetic energy

within the boundary layer.

Figure 13.13 Stall strips help to ensure that the wing root stalls first.

Vortex Generators.

Vortex generators are small aerofoil-shaped blades, normally attached in rows as depicted in Figure 13.14, which project about 2.5cms (1 inch) vertically from the upper surface of the wing. These devices are designed to generate a small vortex within the boundary layer.

Vortex generators cause swirling motions in the boundary layer. This greater turbulence energises the boundary layer and delays separation, thus increasing control effectiveness, especially at the ailerons.

300

ID: 3658

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

CHAPTER 13: THE STALL AND SPIN

Figure 13.14 Vortex generators delay separation of the boundary layer.

Leading Edge Slots.

Slots and slats

You have already learnt how slots and slats energise the boundary layer, retard the

cause the

 

 

onset of turbulent fow and delay separation (See Figure 13.15). Generally, then,

 

 

stalling angle

slots and slats will cause the wing to stall at a higher angle of attack. Their use on

of attack to

the outboard leading-edge gives rise to a local increase in CL which helps delay

increase because they retard

separation at the wing tip and retains aileron effectiveness.

the onset of turbulence in the

 

airflow and delay separation.

 

The stall

 

speed quoted

 

 

 

 

 

in the Pilot’s

 

Operating

 

Handbook refers to Maximum

Figure 13.15 Slots/slats on the leading-edge of a wing energise the boundary layer and

Take-Off Weight with the most

forward C of G position.

delay the onset of the stall.

 

 

 

The Effect of the Position of Centre of Gravity on the Stall.

You learnt in the Mass and Balance section of this series of text books that if the aircraft’s centre of gravity (C of G) is at its most forward limit, the tailplane or stabilator has to produce a greater downforce in order to balance the lift-weight couple (See Figure 13.16 overleaf). This greater tailplane force acting in the same direction as weight, effectively increases the weight of the aircraft. Consequently, for the reasons you have already learnt, the stalling speed increases. As the C of G moves aft, less tailplane downforce is required. This condition reduces the lift requirement for level fight, since lift must balance weight plus downforce, and consequently also decreases the stalling speed. (See Figure 13.17 overleaf). During fight testing, the stalling speed is calculated for the worst case scenario, i.e. maximum weight, with the C of G at its most forward position.

The downforce produced by the tailplane influences the stall speed.

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Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

CHAPTER 13: THE STALL AND SPIN

The stall speed will

increase as the C of G

moves forward and decrease as it moves aft.

When flaps are deployed

CL increases and stalling

speed will decrease.

Figure 13.16 A forward C of G position requires an increased tailplane down-force, leading to an increase in stall speed.

Figure 13.17 Stall speed decreases as the C of G moves aft, because the required tailplane down-force is less.

The Effect of Flaps on the Stall .

Chapter 10, Lift Augmentation, considers in detail the effect which the deployment of faps has on the stall. As you have learnt from Chapter 10, deploying faps alters the shape and camber of the wing’s aerofoil section and increases CL MAX. So, from the lift equation for the point of stall, we see that (vstall) must decrease to keep the equation balanced.

Weight = Lift = CL MAX ½ ρ (vstall)² S

You have also learnt that lowering faps, while increasing CL MAX, not only reduces the angle of attack at which the aircraft stalls, but also increases the angle of incidence of the wing by increasing its camber. This means that if the aircraft stalls from straight and level fight, the nose attitude, with faps down, will be lower than for an equivalent stall exercise with faps up.

The fact that lowering faps reduces the aircraft’s stalling speed is, of course, one of the main advantages of faps, allowing shorter take-off and landing distances to

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ID: 3658

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

CHAPTER 13: THE STALL AND SPIN

be achieved, as well as low-speed cruising fight, should a pilot become lost or fnd himself in deteriorating weather conditions such as a lowering cloudbase.

Note, however, that if the aircraft stalls when faps are down, wing drop at the stall may be more marked than with faps up, because the inboard section of the wing will have a higher local CL than the outer section.

Wing Contamination.

Stalling speed may be increased signifcantlyifthewingiscontaminated

(See Figure 13.18). Snow, frost, and ice deposits on the wing, and even heavy rain, can reduce the value of CL MAX by as much as 30% because of their modifying effect on wing profle. Deposits on the airframe will also increase aircraft weight, causing a further increase in stalling speed. Any contamination (ice, raindrops, squashed insects, etc.) must be removed from the wings before fight,

especially from the leading edge.

Figure 13.18 Frost, snow and ice on the wings increase stall speed.

The Effect of Power on the Stall.

Figure 13.19 When stalling under power, thrust contributes to the Lift, and so the wing can fulfil the smaller lift requirement at a lower speed; stall speed is thus reduced.

When the propeller is producing signifcant thrust, the aircraft’s stalling speed will be lower than with the engine throttled back. The reasons for this are twofold:

The propeller slipstream energises the airfow over the inner region of the wings and, thereby delays separation. This action increases the value of CL MAX and, thus, decreases the stalling speed.

Prior to flight, always ensure that the wing

is free of all contaminants, especially at the leading edge.

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Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

CHAPTER 13: THE STALL AND SPIN

The nose high attitude required to induce a stall under power means that the thrust force has a vertical component which helps to balance the aircraft’s weight. Consequently, the lift force which must be generated by the wing to support the aircraft’s weight is now less than the weight, and it will reach its critical angle of attack at a lower speed. The high nose attitude is a result of the change in relative airfow and downwash due to the slipstream; the greater the power, the higher the nose will be at the stall, and the lower the stall speed. (See Figure 13.19 overleaf).

The Effect of Wing Plan Form on the Stall.

Rectangular Wings.

The separation of the airfow over a wing, which is the essential cause of the stall, does not necessarily occur simultaneously across the whole span of the wing. With a wing of rectangular planform (see Figure 13.20), separation tends to occur near the wing root and then progress outwards towards the wing tips.

The wing of rectangular planform can possess quite benign stall characteristics. The wing stalls frst at its root, while the wing outer section is still effective. So, an aircraft with a rectangular wing is less prone to wing-drop at the stall.

With a wing of rectangular planform, the wing vortices cause high levels of induced drag near the stalling angle of attack. This increases downwash at the wing outer section, reducing the local angle of attack below that at the wing root. It is this situation which leads to the wing root stalling frst. (See Figure 13.20).

Figure 13.20 With rectangular wings, wing tip vortices reduce the angle of attack and ensure that the wing root stalls first.

Tapered Wings.

With wings of tapered planform, separation tends to occur frst of all at the wing tips, and then spreads inboard. It follows, then, that if one wing stalls before the other, there will be pronounced wing drop at the stall.

The reason why the wing tips stall frst with wings of tapered planform is, again, the nature of the wing-tip vortices. As you learnt in the chapter on drag, wing tip vortices for tapered wings are weak. Downwash at the tips is, therefore, less than at the root, resulting in a greater local angle of attack at the wing tip (See Figure 13.21).

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ID: 3658

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

CHAPTER 13: THE STALL AND SPIN

Figure 13.21 Wing tip vortices on tapered wings are weak, causing the wing tips to stall first.

WING CHARACTERISTICS WHICH DELAY WING TIP STALL.

The list below contains some of the most common wing design features which are used to delay the stall and to prevent the wing tips stalling frst.

Stall strips.

Variations of aerofoil section.

Vortex generators.

Leading edge slots.

Washout.

Washout.

We have already examined how most of these features help to delay wing-tip stall, but we have not yet, however, mentioned washout.

Figure 13.22 Washout is the name given to the reduction in a wing’s angle of incidence towards the wing tip.

Washout is the term used to describe the reduction in angle of incidence of the wing from root to tip. This feature helps ensure that the stall occurs at the wing root frst

(See Figure 13.22). (NB. The angle of incidence is the angle between the wing chord line and the aircraft’s longitudinal axis.)

Washout ensures that the wing root stalls first.

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Order: 6026

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

Customer: Oleg Ostapenko E-mail: ostapenko2002@yahoo.com

CHAPTER 13: THE STALL AND SPIN

You must know

the signs of the approaching

stall so that your aircraft never stalls inadvertently.

SIGNS OF THE APPROACHING STALL.

During your PPL flying training, your instructor will demonstrate fully developed stalls to you, and teach you how to recover from the stall, using the standard stall recovery procedure. But while it is instructive to carry out stalls in the upper air under your instructor’s supervision, and to practise stall recovery, you must never allow your aircraft to stall unintentionally or inadvertently. Several hundred feet can be lost while recovering from the stall, so, if your aircraft were to stall inadvertently at low height, on the approach, say, you may not have time to recover before the aircraft hits the ground.

It is, therefore, of vital importance for the pilot that he should be able to recognise the signs and symptoms of an approaching stall so that he can intervene early to prevent the stall from occurring. By learning the symptoms of the approaching stall, you are unlikely to allow your aircraft to stall inadvertently.

If you bear in mind all you have learnt about the stall in this chapter, you should have little difficulty in recognising the warning signs that the aircraft is in danger of stalling. Those warning signs are listed below. They may be present individually or in combination.

Possibly, a high nose attitude, though this is not an essential sign because, as you have learnt, a stall can occur at any attitude and at any speed. The stall occurs when the wing reaches the stalling angle of attack. The stalling speed will vary, among other things, with the load factor acting on the aircraft. If the stall occurs from straight and level flight, however, nose attitude will be high.

Low and decreasing airspeed. When the stall is approached from level flight or the glide, the higher-than-normal nose attitude will be accompanied by low and decreasing airspeed.

Sloppiness and decreasing effectiveness of the controls. Again, if the stall is approached from level flight, nose attitude will be high, speed will be decreasing and, consequently, the controls become noticeably less effective, feeling sloppy instead of firm.

Stall warning device. At the point of the stall (at CL MAX) airframe buffeting becomes more severe. On some aircraft, such as the PA28 Warrior, a stall warning horn operates at a preset angle of attack, just before the onset of the stall, typically sounding 5-10 kts above the stall speed.

Airframe buffeting. As you have learnt, as the angle of attack increases in the approach to the stall, the airflow begins to separate and break away from the wing surface. Airflow in this condition is turbulent and gives rise to airframe buffeting. As the turbulence strikes the elevator, it is felt through the control column as vibration.

Your flying instructor will teach you how to react to the signs of the approaching stall in order to prevent the stall from occurring. If you are operating normally in the climb, cruise or descent, in order to prevent the stall from occurring it will, generally, be sufficient for you to reselect the correct attitude for the phase of flight that you are in, and to confirm that you have the appropriate power setting.

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