Rotorcraft Flying Handbook, FAA-H-8083-21
Rotorcraft Flying Handbook, FAA-H-8083-21
Rotorcraft Flying Handbook, FAA-H-8083-21
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VERTICAL AUTOROTATION<br />
HUB<br />
Resultant<br />
Relative Wind<br />
Upward Airflow<br />
(17 m.p.h. or 25 f.p.s.)<br />
Rotational Airflow<br />
(<strong>21</strong> m.p.h. or 31 f.p.s.)<br />
Rotor Speed: 300 r.p.m.<br />
Upward Airflow<br />
(17 m.p.h. or 25 f.p.s.)<br />
TIP<br />
Resultant Relative Wind<br />
Rotational Airflow (267 m.p.h. or 393 f.p.s.)<br />
Figure 16-3. Moving outboard on the rotor blade, the rotational velocity increasingly exceeds the upward component of airflow,<br />
resulting in a higher relative wind at a lower angle of attack.<br />
speed of 393 feet per second, or 267 m.p.h. The result<br />
is a higher total relative wind, striking the blades at a<br />
lower angle of attack. [Figure 16-3]<br />
F<br />
ROTOR DISC REGIONS<br />
As with any airfoil, the lift that is created by rotor<br />
blades is perpendicular to the relative wind. Because<br />
the relative wind on rotor blades in autorotation shifts<br />
from a high angle of attack inboard to a lower angle of<br />
attack outboard, the lift generated has a higher forward<br />
component closer to the hub and a higher vertical component<br />
toward the blade tips. This creates distinct<br />
regions of the rotor disc that create the forces necessary<br />
for flight in autorotation. [Figure 16-4] The<br />
autorotative region, or driving region, creates a total<br />
aerodynamic force with a forward component that<br />
exceeds all rearward drag forces and keeps the blades<br />
spinning. The propeller region, or driven region, generates<br />
a total aerodynamic force with a higher vertical<br />
component that allows the gyroplane to remain aloft.<br />
Near the center of the rotor disc is a stall region where<br />
the rotational component of the relative wind is so low<br />
that the resulting angle of attack is beyond the stall<br />
limit of the airfoil. The stall region creates drag against<br />
the direction of rotation that must be overcome by the<br />
forward acting forces generated by the driving region.<br />
AUTOROTATION IN FORWARD FLIGHT<br />
As discussed thus far, the aerodynamics of autorotation<br />
apply to a gyroplane in a vertical descent. Because<br />
gyroplanes are normally operated in forward flight, the<br />
component of relative wind striking the rotor blades as<br />
a result of forward speed must also be considered. This<br />
component has no effect on the aerodynamic principles<br />
that cause the blades to autorotate, but causes a shift in<br />
the zones of the rotor disc.<br />
Driven Region<br />
(Propeller)<br />
Lift<br />
Rotational<br />
Relative Wind<br />
Inflow Up<br />
Through Rotor<br />
TAF<br />
Axis of<br />
Rotation<br />
VERTICAL AUTOROTATION<br />
Total<br />
Aerodynamic<br />
Force Aft<br />
of Axis of<br />
Rotation<br />
Drag<br />
Chord Line<br />
Resultant<br />
Relative Wind<br />
Driven Region<br />
Driving Region<br />
Stall<br />
Region<br />
Driving Region<br />
(Autorotative)<br />
Total<br />
Aerodynamic<br />
Force<br />
TAF Forward<br />
Lift of Axis of<br />
Rotation<br />
Drag<br />
Inflow<br />
Axis of<br />
Rotation<br />
Stall Region<br />
(Blade is Stalled)<br />
Inflow<br />
TAF<br />
Drag<br />
Axis of<br />
Rotation<br />
Figure 16-4. The total aerodynamic force is aft of the axis of<br />
rotation in the driven region and forward of the axis of rotation<br />
in the driving region. Drag is the major aerodynamic<br />
force in the stall region. For a complete depiction of force<br />
vectors during a vertical autorotation, refer to Chapter 3—<br />
Aerodynamics of Flight (Helicopter), Figure 3-22.<br />
As a gyroplane moves forward through the air, the forward<br />
speed of the aircraft is effectively added to the<br />
Lift<br />
16-2