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Rotorcraft Flying Handbook, FAA-H-8083-21

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Resultant<br />

Lift<br />

Lift<br />

Resultant<br />

Thrust<br />

Rotor<br />

Drag<br />

Thrust<br />

Fuselage<br />

Drag<br />

Drag<br />

Weight<br />

Resultant<br />

Resultant<br />

Weight<br />

Figure 16-7. Unlike a helicopter, in forward powered flight the resultant rotor force of a gyroplane acts in a rearward direction.<br />

thrust directly from the engine through a propeller.<br />

[Figure 16-7]<br />

The force produced by the gyroplane rotor may be<br />

divided into two components; rotor lift and rotor drag.<br />

The component of rotor force perpendicular to the<br />

flight path is rotor lift, and the component of rotor force<br />

parallel to the flight path is rotor drag. To derive the<br />

total aircraft drag reaction, you must also add the drag<br />

of the fuselage to that of the rotor.<br />

ROTOR LIFT<br />

Rotor lift can most easily be visualized as the lift<br />

required to support the weight of the aircraft. When an<br />

airfoil produces lift, induced drag is produced. The<br />

most efficient angle of attack for a given airfoil produces<br />

the most lift for the least drag. However, the airfoil<br />

of a rotor blade does not operate at this efficient<br />

angle throughout the many changes that occur in each<br />

revolution. Also, the rotor system must remain in the<br />

autorotative (low) pitch range to continue turning in<br />

order to generate lift.<br />

Some gyroplanes use small wings for creating lift when<br />

operating at higher cruise speeds. The lift provided by<br />

the wings can either supplement or entirely replace<br />

rotor lift while creating much less induced drag.<br />

ROTOR DRAG<br />

Total rotor drag is the summation of all the drag forces<br />

acting on the airfoil at each blade position. Each blade<br />

position contributes to the total drag according to the<br />

speed and angle of the airfoil at that position. As the<br />

rotor blades turn, rapid changes occur on the airfoils<br />

depending on position, rotor speed, and aircraft speed.<br />

A change in the angle of attack of the rotor disc can<br />

effect a rapid and substantial change in total rotor drag.<br />

Rotor drag can be divided into components of induced<br />

drag and profile drag. The induced drag is a product of<br />

lift, while the profile drag is a function of rotor r.p.m.<br />

Because induced drag is a result of the rotor providing<br />

lift, profile drag can be considered the drag of the rotor<br />

when it is not producing lift. To visualize profile drag,<br />

consider the drag that must be overcome to prerotate<br />

the rotor system to flight r.p.m. while the blades are<br />

producing no lift. This can be achieved with a rotor system<br />

having a symmetrical airfoil and a pitch change<br />

capability by setting the blades to a 0° angle of attack.<br />

A rotor system with an asymmetrical airfoil and a built<br />

in pitch angle, which includes most amateur-built<br />

teeter-head rotor systems, cannot be prerotated without<br />

having to overcome the induced drag created as well.<br />

THRUST<br />

Thrust in a gyroplane is defined as the component of<br />

total propeller force parallel to the relative wind. As<br />

with any force applied to an aircraft, thrust acts around<br />

the center of gravity. Based upon where the thrust is<br />

applied in relation to the aircraft center of gravity, a relatively<br />

small component may be perpendicular to the<br />

relative wind and can be considered to be additive to<br />

lift or weight.<br />

In flight, the fuselage of a gyroplane essentially acts as<br />

a plumb suspended from the rotor, and as such, it is<br />

16-4

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