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The Art of the Helicopter John Watkinson - Karatunov.net

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Introduction to rotorcraft 19<br />

wings is that <strong>the</strong> former are in comparison very thin and flexible, and <strong>the</strong> forces acting<br />

upon <strong>the</strong>m are greater and more rapidly varying. <strong>The</strong> rotors have more to do than an<br />

aeroplane wing, because <strong>the</strong>y are also <strong>the</strong> control system. Chapter 3 explains how <strong>the</strong><br />

rotors produce lift and introduces <strong>the</strong> control <strong>of</strong> <strong>the</strong> machine.<br />

1.12 <strong>The</strong> control system<br />

<strong>The</strong> control system cannot be treated in isolation, but must be integrated into <strong>the</strong> design<br />

<strong>of</strong> a machine from <strong>the</strong> outset. In <strong>the</strong> pure helicopter, control <strong>of</strong> <strong>the</strong> machine is achieved<br />

entirely by changing <strong>the</strong> pitch <strong>of</strong> <strong>the</strong> main and tail rotor blades in various ways. This will<br />

<strong>the</strong>n determine <strong>the</strong> amount <strong>of</strong> engine power needed. <strong>The</strong> rotors are generally designed<br />

to turn at constant speed and <strong>the</strong> throttle setting will have to be modified whenever <strong>the</strong><br />

rotor power demand changes so that <strong>the</strong> speed does not change. Chapter 6 considers<br />

engines and power control.<br />

<strong>The</strong>re are two main forces acting on a helicopter, <strong>the</strong> force due to gravity, which is<br />

always downwards, and <strong>the</strong> rotor thrust vector, which is always at right angles to <strong>the</strong><br />

tip path plane, o<strong>the</strong>rwise called <strong>the</strong> rotor disc. Chapter 2 explains how <strong>the</strong> result <strong>of</strong><br />

forces acting in various ways can be predicted and Chapter 3 shows how rotors develop<br />

thrust. <strong>The</strong> pilot can control <strong>the</strong> magnitude <strong>of</strong> <strong>the</strong> rotor thrust with <strong>the</strong> collective pitch<br />

lever held in his left hand, and <strong>the</strong> direction <strong>of</strong> <strong>the</strong> rotor thrust with <strong>the</strong> cyclic stick<br />

held in his right hand. <strong>The</strong> cyclic stick works in two dimensions: if <strong>the</strong> stick is pushed<br />

in any direction, <strong>the</strong> rotor thrust tilts <strong>the</strong> same way. <strong>The</strong>se two fundamental controls<br />

are illustrated in Figure 1.21.<br />

<strong>The</strong> blade movements necessary to produce lift and to achieve control will be outlined<br />

in Chapter 3, whereas Chapter 4 treats <strong>the</strong> construction and dynamics <strong>of</strong> <strong>the</strong> blades<br />

Fig. 1.21 <strong>The</strong> fundamental rotor controls.<strong>The</strong> cyclic stick tilts <strong>the</strong> rotor in <strong>the</strong> direction it is moved, whereas<br />

<strong>the</strong> collective lever changes <strong>the</strong> magnitude <strong>of</strong> <strong>the</strong> thrust.

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