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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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Introduction to helicopter dynamics 77<br />

needed in <strong>the</strong> real helicopter where <strong>the</strong> actuator has <strong>the</strong> same diameter as <strong>the</strong> rotor.<br />

This is <strong>the</strong> origin <strong>of</strong> <strong>the</strong> figure <strong>of</strong> merit.<br />

3.13 Blade twist and taper<br />

<strong>The</strong> forward velocity <strong>of</strong> <strong>the</strong> rotating blade increases linearly from zero at <strong>the</strong> shaft<br />

to a maximum at <strong>the</strong> tip. This is not a good starting point from which to obtain<br />

uniform inflow, but <strong>the</strong> rotor is <strong>the</strong> only practical approximation to an actuator disc that<br />

anyone has devised. <strong>The</strong> figure <strong>of</strong> merit may be improved by twisting and tapering<br />

<strong>the</strong> rotor blades. Figure 3.12(a) shows that in untwisted, untapered blades, <strong>the</strong> lift<br />

will be produced increasingly toward <strong>the</strong> tips as a parabolic function, until tip loss<br />

dominates.<br />

Given <strong>the</strong> induced velocity is required to be uniform, it is easy to calculate <strong>the</strong> pitch<br />

required at any radius to make <strong>the</strong> angle <strong>of</strong> attack constant along <strong>the</strong> blade so that<br />

<strong>the</strong> whole blade operates at an efficient L/D ratio. However, in practice <strong>the</strong> induced<br />

velocity will be a function <strong>of</strong> radius and such a twist will not be optimal. Twist that<br />

takes account <strong>of</strong> induced velocity distribution is known as ideal twist. In fact ideal<br />

twist is academic because <strong>the</strong> amount <strong>of</strong> twist would have to change as a function <strong>of</strong><br />

induced velocity and clearly it does not in any practical blade.<br />

Ideal twist does not achieve uniform inflow, because <strong>of</strong> <strong>the</strong> reduced effectiveness <strong>of</strong> <strong>the</strong><br />

inner slow-moving parts <strong>of</strong> <strong>the</strong> blade. Tapering <strong>the</strong> blade as well as twisting it removes<br />

area at <strong>the</strong> fast moving tips and places it in <strong>the</strong> slower moving areas where induced<br />

velocity is ordinarily lower. Ideally, <strong>the</strong> rotor chord needs to be inversely proportional<br />

to <strong>the</strong> radius. This results in an impractical rotor for a helicopter, but <strong>the</strong> technique<br />

Fig. 3.12 (a) An untwisted, untapered blade has a parabolic lift distribution and far from uniform inflow.<br />

(b) Taper and twist improve <strong>the</strong> uniformity <strong>of</strong> inflow.

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