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The Art of the Helicopter John Watkinson - Karatunov.net

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

Fig. 4.32 A supercritical rotor has such a high dragging frequency that <strong>the</strong> rotor can never reverse it. No<br />

damping is <strong>the</strong>n needed.<br />

becomes progressive again. <strong>The</strong> frequency <strong>the</strong>n rises to become asymptotic to <strong>the</strong><br />

value determined by centrifugal stiffening. Point D in Figure 4.31corresponds to a<br />

coincidence between a hull frequency and a progressive backwards whirling frequency,<br />

at which ground resonance can occur. Consequently s<strong>of</strong>t-in-plane rotors still require<br />

damping.<br />

A ‘stiff-in-plane’ or ‘supercritical’ rotor has a powerful dragging restoring force due to<br />

its construction and so has a significant dragging resonant frequency, even at rest. When<br />

<strong>the</strong> rotor is turning, <strong>the</strong> dragging frequency increases even fur<strong>the</strong>r due to centrifugal<br />

stiffening. Figure 4.32 shows that, by definition, in <strong>the</strong> case <strong>of</strong> a ‘stiff-in-plane’ rotor,<br />

<strong>the</strong> whirling frequency is always higher than <strong>the</strong> rotor frequency. <strong>The</strong> behaviour <strong>of</strong> <strong>the</strong><br />

forward whirling is benign as before. However, as <strong>the</strong> backwards whirling frequency is<br />

so high, <strong>the</strong> rotor frequency can never reverse it and so backwards whirling is always<br />

regressive in <strong>the</strong> case <strong>of</strong> a stiff-in-plane rotor. In that case <strong>the</strong> unstable combination <strong>of</strong><br />

progressive backwards whirling can never occur and such a rotor can function with no<br />

damping at all. Two-bladed teetering rotors take advantage <strong>of</strong> this concept. <strong>The</strong>y are<br />

built without dragging hinges to obtain supercritical dragging behaviour.<br />

<strong>The</strong>re is a small possibility <strong>of</strong> a damper failure and so it is as well to know how to<br />

handle it. <strong>The</strong>re are two ways to recover from incipient ground resonance, depending<br />

on <strong>the</strong> rotor speed at <strong>the</strong> time it happens. If sufficient revs are available to permit flight,<br />

<strong>the</strong> answer is to take-<strong>of</strong>f immediately. With no ground reaction against <strong>the</strong> undercarriage,<br />

<strong>the</strong> hull rocking resonance cannot occur and <strong>the</strong> shaking stops immediately. An<br />

attempt at a gentle landing may succeed, but if not <strong>the</strong>n a landing should be attempted<br />

on a s<strong>of</strong>t or high friction surface which is more likely to absorb energy than tarmac.<br />

It is important that <strong>the</strong>re is no groundspeed whatsoever at <strong>the</strong> moment <strong>of</strong> touchdown.<br />

If insufficient rotor revs exist for flight, <strong>the</strong> solution is to change <strong>the</strong> frequency <strong>of</strong> <strong>the</strong><br />

excitation away from <strong>the</strong> hull/undercarriage resonance. This may be done by reducing<br />

rotor speed by cutting <strong>the</strong> throttle and using <strong>the</strong> rotor brake if fitted.<br />

4.18 Air resonance<br />

Air resonance is a condition primarily relevant to helicopters having hingeless rotors.<br />

In articulated rotors <strong>the</strong> natural frequency <strong>of</strong> <strong>the</strong> blade about <strong>the</strong> lagging hinge is low

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