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The Art of the Helicopter John Watkinson - Karatunov.net

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

longer a dominant blade-passing frequency. Additionally with a carefully chosen skew<br />

angle and spacing between <strong>the</strong> two rotors a small gain in aerodynamic efficiency can<br />

be obtained because <strong>the</strong> axially spaced pairs <strong>of</strong> blades act to some extent like staggered<br />

biplane wings.<br />

As with <strong>the</strong> main rotor, airspeed alternately adds to and subtracts from <strong>the</strong> blade<br />

speed due to rotation. <strong>The</strong> resulting roll couple is subject to precession and <strong>the</strong> result<br />

will be flapback and dragging. As <strong>the</strong> tail rotor tip path axis is tilted backwards due<br />

to <strong>the</strong> flapping, <strong>the</strong> thrust has a rearward component acting as a drag which <strong>the</strong> main<br />

rotor has to overcome. However, <strong>the</strong> inflow has a small component along <strong>the</strong> tip path<br />

axis in forward flight reducing <strong>the</strong> angle <strong>of</strong> attack and <strong>the</strong> shaft power needed. <strong>The</strong><br />

power saved is <strong>the</strong>n available to <strong>the</strong> main rotor and is precisely <strong>the</strong> correct amount <strong>the</strong><br />

main rotor needs to overcome <strong>the</strong> drag. As a result tail rotor flapping is not detrimental<br />

to efficiency but it could lead to stress and/or wear.<br />

In very large helicopters <strong>the</strong> tail rotor will need both flapping and dragging articulation<br />

to contain <strong>the</strong> stresses and <strong>the</strong> dragging axis will need damping. In smaller<br />

machines it is enough to have flapping hinges. <strong>The</strong> hinge will <strong>of</strong>ten incorporate some<br />

delta-three effect (see section 4.7). <strong>The</strong> delta-three hinge has <strong>the</strong> effect that as <strong>the</strong> rotor<br />

flaps, some cyclic pitch change is applied. <strong>The</strong> rotor finds equilibrium with a smaller<br />

amount <strong>of</strong> flapping.<br />

<strong>The</strong> tail rotor counters <strong>the</strong> torque <strong>of</strong> <strong>the</strong> main rotor in <strong>the</strong> hover, but it also aids<br />

<strong>the</strong> directional stability <strong>of</strong> <strong>the</strong> machine in forward flight by acting as a fin. Figure 5.3<br />

shows how this happens. If <strong>the</strong> tail swings to one side or <strong>the</strong> o<strong>the</strong>r, a component <strong>of</strong><br />

<strong>the</strong> airspeed will change <strong>the</strong> inflow and with it <strong>the</strong> angle <strong>of</strong> attack. <strong>The</strong> result will be<br />

a change <strong>of</strong> thrust in such a sense as to return <strong>the</strong> tail to its original position. This<br />

is a highly desirable characteristic, except in rearward flight where <strong>the</strong> effect makes<br />

<strong>the</strong> machine unstable in yaw. An attempt to fly backwards at speed results in <strong>the</strong> tail<br />

swinging round, a phenomenon known as wea<strong>the</strong>rcocking.<br />

Fig. 5.3 <strong>The</strong> tail rotor acts like a fin in forward flight because if <strong>the</strong> machine yaws, <strong>the</strong> angle <strong>of</strong> attack <strong>of</strong> <strong>the</strong><br />

tail rotor blades will change in <strong>the</strong> sense that opposes <strong>the</strong> yaw.

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