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The Art of the Helicopter John Watkinson - Karatunov.net

The Art of the Helicopter John Watkinson - Karatunov.net

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92 <strong>The</strong> <strong>Art</strong> <strong>of</strong> <strong>the</strong> <strong>Helicopter</strong><br />

(a)<br />

(b)<br />

(c)<br />

Fig. 3.24 (a) Given <strong>the</strong> pressure difference across a rotor in <strong>the</strong> hover, surrounding air will tend to move<br />

upwards. In translational flight <strong>the</strong> edge <strong>of</strong> <strong>the</strong> rotor may actually encounter upwash. (b) In forward flight <strong>the</strong><br />

rotor acts like a low aspect ratio wing. Vortices curl over <strong>the</strong> tips and down through <strong>the</strong> rear <strong>of</strong> <strong>the</strong> disc, reducing<br />

<strong>the</strong> angle <strong>of</strong> attack <strong>the</strong>re. Loss <strong>of</strong> lift at <strong>the</strong> rear precesses into inflow roll. (c) As <strong>the</strong> rotor blades are coned, in<br />

forward flight <strong>the</strong> air approaches at a different angle as shown here. <strong>The</strong> component perpendicular to <strong>the</strong> blade<br />

is greater for blades at <strong>the</strong> rear, where <strong>the</strong> angle <strong>of</strong> attack is reduced.<br />

Whilst coning causes no undue aerodynamic problems to a hovering helicopter, it<br />

has an unwanted effect in forward flight. Figure 3.24(c) shows that <strong>the</strong> effect <strong>of</strong> coning<br />

is to reduce <strong>the</strong> angle <strong>of</strong> attack <strong>of</strong> <strong>the</strong> blade passing across <strong>the</strong> tail compared with<br />

that <strong>of</strong> <strong>the</strong> blade passing across <strong>the</strong> nose. As for <strong>the</strong> inflow roll, this results in a taildown<br />

moment applied to <strong>the</strong> disc, which likewise manifests itself as a roll towards <strong>the</strong><br />

advancing side because <strong>of</strong> <strong>the</strong> phase lag <strong>of</strong> <strong>the</strong> rotor. <strong>The</strong> two effects take place in<br />

parallel, but as different functions <strong>of</strong> airspeed. Inflow roll commences on leaving <strong>the</strong><br />

hover but reduces significantly as speed increases, whereas coning roll slightly increases

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