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The Art of the Helicopter John Watkinson - Karatunov.net

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

OP is an arbitrary hinge axis and could be a flapping or a lagging hinge. In <strong>the</strong> literature,<br />

<strong>the</strong> flapping hinge is called <strong>the</strong> δ hinge and <strong>the</strong> dragging hinge is called <strong>the</strong> α hinge.<br />

<strong>The</strong>se hinges can be turned away from <strong>the</strong> mutually orthogonal in three axes, 1, 2 and<br />

3. Only two <strong>of</strong> <strong>the</strong>se axes are shown in Figure 4.9(a); axis 2 is redundant. If OP is a<br />

flapping hinge and is projected into <strong>the</strong> plane <strong>of</strong> <strong>the</strong> rotor, OXY, <strong>the</strong> angle between <strong>the</strong><br />

projection and OY is called δ3 (delta-three). If OP is projected onto <strong>the</strong> plane OZY, <strong>the</strong><br />

angle between <strong>the</strong> projection and OY is δ1 (delta-one). In an orthogonal head <strong>the</strong>se<br />

angles are both zero.<br />

Figure 4.9(b) shows that to avoid coupling between flapping and fea<strong>the</strong>ring, <strong>the</strong><br />

spherical bearing between <strong>the</strong> pitch control rod and <strong>the</strong> pitch control arm must be on<br />

<strong>the</strong> axis <strong>of</strong> <strong>the</strong> flapping hinge which must also be at 90 ◦ to <strong>the</strong> fea<strong>the</strong>ring axis.<br />

<strong>The</strong> pitch control arm is generally on <strong>the</strong> leading edge <strong>of</strong> <strong>the</strong> blade. If <strong>the</strong> pitch control<br />

arm is made slightly shorter as in Figure 4.9(c), <strong>the</strong>re will be an interaction between<br />

flapping and fea<strong>the</strong>ring. Figure 4.9(d) reveals that upward flapping will reduce <strong>the</strong> pitch<br />

<strong>of</strong> <strong>the</strong> blade, tending to lower <strong>the</strong> blade, whereas downward flapping would have <strong>the</strong><br />

reverse effect. Effectively a positive δ3 hinge has been created. This is a stable condition,<br />

whereas <strong>the</strong> reverse relationship between <strong>the</strong> control rod joint and <strong>the</strong> flapping axis to<br />

give a negative δ3 hinge would be unstable.<br />

In some autogyros <strong>the</strong> dragging hinge was inclined to produce a δ1 hinge. This had <strong>the</strong><br />

effect <strong>of</strong> coupling <strong>the</strong> dragging and <strong>the</strong> blade pitch to allow jump take-<strong>of</strong>f. <strong>The</strong> blades<br />

would stay in fine pitch whilst being driven, but upon <strong>the</strong> drive being disconnected <strong>the</strong><br />

blades would swing forward, increasing <strong>the</strong> pitch.<br />

In some toy free-flying helicopters a reverse δ1 hinge is used which sets <strong>the</strong> machine<br />

automatically into autorotation when <strong>the</strong> fuel runs out.<br />

4.8 Types <strong>of</strong> rotor head<br />

For many years <strong>the</strong> designer was faced with a choice between a teetering two-bladed<br />

head and an articulated multi-bladed head. <strong>The</strong>se techniques were developed because<br />

<strong>the</strong>y greatly reduce bending loads on <strong>the</strong> blades. <strong>The</strong> teetering head imposes <strong>the</strong> least<br />

stress on <strong>the</strong> mast, but has some drawbacks as will be seen in section 4.10. In <strong>the</strong><br />

early years <strong>of</strong> helicopter design, available blade materials and designs precluded <strong>the</strong><br />

use <strong>of</strong> o<strong>the</strong>r types <strong>of</strong> rotor head and <strong>the</strong> drawbacks had to be accepted. Although<br />

it is less demanding on <strong>the</strong> blades and <strong>the</strong> fea<strong>the</strong>ring bearings, <strong>the</strong> articulated rotor<br />

head contains a mass <strong>of</strong> bearings subject to oscillating motion that causes wear. <strong>The</strong>se<br />

bearings require frequent replacement. Large machines may require continuous oil feed<br />

to <strong>the</strong> bearings, whereas smaller machines require <strong>the</strong> periodic application <strong>of</strong> a grease<br />

gun. <strong>The</strong> hingeless rotor head is a desirable goal if only because it reduces <strong>the</strong> amount<br />

<strong>of</strong> maintenance required.<br />

<strong>The</strong> effect <strong>of</strong> blade flapping in articulated and teetering heads is also used to prevent<br />

excessively rapid response to cyclic control inputs. This will be made clear in<br />

section 4.11.<br />

<strong>The</strong> stress due to coning can be relieved by fitting <strong>the</strong> blades at a preset coning angle.<br />

In practice, <strong>the</strong> disc and shaft axes will be slightly different since <strong>the</strong> hull blowback will<br />

never be perfectly balanced by <strong>the</strong> tail plane, particularly if <strong>the</strong> CM is displaced. As<br />

<strong>the</strong> hinges are only resolving a small geometric problem, it is clear that a rotor strong<br />

enough or flexible enough to accommodate <strong>the</strong> geometric conflict can dispense with<br />

actual flapping and dragging hinges. <strong>The</strong> result is a hingeless rotor. <strong>The</strong> term ‘rigid<br />

rotor’ is sometimes used to describe such a system, but clearly it is a misnomer and <strong>the</strong><br />

term hingeless is to be preferred.

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