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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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<strong>Helicopter</strong> performance 345<br />

moment from <strong>the</strong> main rotor. <strong>The</strong> helicopter may enter a spiral dive if disturbed in roll.<br />

Spiral instability may be remedied by lowering <strong>the</strong> CM, reducing fin area or by moving<br />

it upwards or forwards or by adding side area to <strong>the</strong> hull high up ahead <strong>of</strong> <strong>the</strong> mast.<br />

Upward relocation <strong>of</strong> <strong>the</strong> tail rotor and/or increasing <strong>the</strong> main rotor flapping <strong>of</strong>fset<br />

will also be beneficial.<br />

On <strong>the</strong> o<strong>the</strong>r hand if <strong>the</strong> fin and tail rotor are high mounted, <strong>the</strong>y may hardly oppose<br />

<strong>the</strong> dihedral effect <strong>of</strong> <strong>the</strong> main rotor at all and <strong>the</strong> helicopter may have too much lateral<br />

stability such that if disturbed it suffers a phenomenon called a dutch roll.<br />

Dutch roll describes a flight path like a corkscrew. Following a slip, excessive lateral<br />

stability creates a restoring roll couple so powerful that <strong>the</strong>re is insufficient momentum<br />

for <strong>the</strong> helicopter to overshoot <strong>the</strong> correct attitude. <strong>The</strong> helicopter <strong>the</strong>n oscillates about<br />

its path near-sinusoidally in pitch, roll and yaw but with phase differences between <strong>the</strong><br />

motions. <strong>The</strong> motion may be damped heavily, so that it dies out or it may stabilize with<br />

certain amplitude. In some cases <strong>the</strong> amplitude will grow indefinitely. In most cases<br />

pilot intervention prevents such a divergence. However, for IFR operation, Dutch roll<br />

is considered as detrimental as spiral instability. Dutch roll may be remedied by raising<br />

<strong>the</strong> CM, by lowering <strong>the</strong> tail rotor, by reducing <strong>the</strong> main rotor flapping <strong>of</strong>fset, by<br />

increasing fin area, by moving <strong>the</strong> fin back and/or down or by adding side area to <strong>the</strong><br />

hull low down. Fences may be seen on <strong>the</strong> bottom <strong>of</strong> <strong>the</strong> hull for this purpose.<br />

Hover stability is marginal in most helicopters because <strong>the</strong> hull mass is located<br />

below <strong>the</strong> rotor. It might be thought that this would act like a pendulum and give<br />

stability but this is not what happens. <strong>The</strong> hull has mass and is more or less flexibly<br />

suspended from <strong>the</strong> rotor according to <strong>the</strong> type <strong>of</strong> rotor head. As a result <strong>the</strong> attitude<br />

<strong>of</strong> <strong>the</strong> hull will always lag <strong>the</strong> attitude <strong>of</strong> <strong>the</strong> rotor. Figure 8.16 shows that if a helicopter<br />

is trimmed to stationary hover and <strong>the</strong>n <strong>the</strong> controls are locked, it will begin<br />

a divergent oscillation. <strong>The</strong> rotor on its own is stable in <strong>the</strong> hover because if it moves<br />

in any horizontal direction, flapback will tend to arrest <strong>the</strong> motion. However, it can be<br />

seen from <strong>the</strong> figure that <strong>the</strong> hull swings from side to side under <strong>the</strong> rotor, but because<br />

<strong>the</strong> swashplate is referenced to <strong>the</strong> hull, that swinging causes cyclic inputs. <strong>The</strong>se are<br />

not phased to damp <strong>the</strong> motion, but in fact augment <strong>the</strong> motion.<br />

Fig. 8.16 <strong>Helicopter</strong>s are unstable in hover and, without pilot intervention, will wander to and fro as<br />

shown here.

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