Thursday, July 16, 2009

Flap

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Triple-slotted trailing-edge flaps and leading edge Krueger (unslotted and slotted) flaps (slats) fully extended on a Boeing 747 for landing.
Virgin Atlantic Airbus A340-600, landing with trailing-edge flaps extended.
An Air France jet with flaps fully extended as it reduces speed before landing at Paris
A British Airways Boeing 757-200 lands with flaps extended

Flaps are hinged surfaces on the trailing edge of the wings of a fixed-wing aircraft. As flaps are extended, the stalling speed of the aircraft is reduced. Flaps are also used on the leading edge of the wings of some high-speed jet aircraft, where they may be called Krueger flaps.

Flaps increase the camber of the wing airfoil, thus raising the lift coefficient. This increase in lift coefficient allows the aircraft to generate a given amount of lift with a slower speed. Therefore, extending the flaps will reduce the stalling speed of an aircraft. They also increase drag which helps to slow the aircraft. A useful side effect of flap deployment is a decrease in aircraft pitch angle resulting from the increase in angle of attack relative to the fuselage. This allows the pilot to lower the nose for better ground visibility.

Some trailing edge flap systems increase the planform area of the wing in addition to changing the camber. In turn, the larger lifting surface will allow the aircraft to generate a given amount of lift with a slower speed, thus further reducing stalling speed. Although this effect is very similar to increasing the lift coefficient, raising the planform area of the wing does not itself raise the lift coefficient. The Fowler flap is an example of a flap system that increases the planform area of the wing in addition to increasing the camber.

Contents


Physics Explanation

The general airplane lift equation demonstrates these relationships:

L = \tfrac12 \rho V^2 S C_L

where:

  • L is the lift,
  • ρ is the air density,
  • V is the true airspeed of the airplane
  • S is the planform area of the wing and
  • CL is the aircraft lift coefficient

Here, it can be seen that increasing the area (S) and lift coefficient (CL) will allow a similar amount of lift to be generated at a slower airspeed (V).

Extending the flaps also increases the drag coefficient of the aircraft. Therefore, for any given weight and airspeed, flaps increase the drag force. Flaps increase the drag coefficient of an aircraft because of higher induced drag caused by the distorted spanwise lift distribution on the wing with flaps extended. Some flaps increase the planform area of the wing and, for any given speed, this also increases the parasitic drag component of total drag.

Depending on the aircraft type, flaps may be partially extended for takeoff. Especially with general aviation aircraft, the use of flaps for takeoff may be optional. This will depend on the manufacturer's procedures in the Airplane Flight Manual for a specific takeoff method (e.g., short field, soft field, normal, etc.). Flaps may be partially extended on takeoff to increase the amount of lift generated at a given airspeed, as well as to reduce the stalling speed of the airplane. Together, these two effects will help an airplane lift off in a shorter distance at a lower drag penalty than that incurred by a full flap deflection.

Flaps are usually fully extended for landing to give the aircraft a slower stalling speed so the approach to landing can be flown more slowly, allowing the aircraft to land in a shorter distance. The higher lift and drag associated with fully extended flaps allows a steeper and slower approach to the landing site. This demonstrates the combined benefit of the higher lift and drag coefficients of fully extended flaps.

Some gliders not only use flaps when landing but also in flight to optimize the camber of the wing for the chosen speed. When thermalling, flaps may be partially extended to reduce the stalling speed so that the glider can be flown more slowly and thereby turn in a smaller circle to make best use of the core of the thermal. At higher speeds a negative flap setting is used to reduce the nose-down pitching moment. This reduces the balancing load required on the horizontal stabilizer which in turn reduces the trim drag associated with keeping the glider in longitudinal trim. Negative flap may also be used during the initial stage of an aerotow launch and at the end of the landing run in order to maintain better control by the ailerons.

Types

Four types of flaps

Types of flap systems include:

  • Krueger flap: hinged flap on the leading edge.[1] [2] Often called a "droop."
  • Plain flap: rotates on a simple hinge.
  • Split flap: upper and lower surfaces are separate, the lower surface operates like a plain flap, but the upper surface stays immobile or moves only slightly.
  • Fowler flap: slides backwards before hinging downwards, thereby increasing both camber and chord, creating a larger wing surface better tuned for lower speeds. The Fowler flap was invented by Harlan D. Fowler.
  • Fairey-Youngman flap: moves bodily down before moving aft and rotating.
  • Slotted flap: a slot (or gap) between the flap and the wing enables high pressure air from below the wing to re-energize the boundary layer over the flap. This helps the airflow to stay attached to the flap, delaying the stall.
  • Blown flaps: systems that blow engine air over the upper surface of the flap at certain angles to improve lift characteristics.

There are several technology development efforts to incorporate the function of the flaps into a flexible wing, so that the aerodynamic purpose is accomplished without the weight and mechanical complexity of a flap system. The X-53 Active Aeroelastic Wing is a NASA effort to incorporate this technology, and the Adaptive Compliant Wing is commercial development effort.

Slats, also known as leading-edge flaps, have a similar purpose to trailing-edge flaps, except that they are located on the leading edge of the wing. Note that a Krueger flap and a leading-edge slat differ in how they are extended (and retracted), but their aerodynamic function is the same.

References

  • Clancy, L.J. (1975), Aerodynamics, Chapter 6, Pitman Publishing Limited, London ISBN 0 273 01120 0

Notes

See also

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