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The Art of the Helicopter John Watkinson - Karatunov.net

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

Fig. 3.33 A rotor is not an ideal actuator disc. <strong>The</strong> downwash velocity is not constant but increases as each<br />

blade passes and falls in between. A fixed point on a blade will cross its own path and <strong>the</strong> paths <strong>of</strong> o<strong>the</strong>r blades<br />

in forward flight.<br />

<strong>the</strong> point on <strong>the</strong> blade at which <strong>the</strong> lift dips is constantly changing in radius. However,<br />

it can be seen from Figure 3.33 that at about 60 ◦ <strong>of</strong> azimuth <strong>the</strong> blade is nearly parallel<br />

to <strong>the</strong> cycloid, meaning that a significant length <strong>of</strong> <strong>the</strong> blade is experiencing <strong>the</strong> effect<br />

at <strong>the</strong> same time.<br />

<strong>The</strong> non-uniformity <strong>of</strong> <strong>the</strong> downwash will also directly excite <strong>the</strong> hull and is commonly<br />

observed as flexing <strong>of</strong> <strong>the</strong> canopy at <strong>the</strong> blade passing frequency. In <strong>the</strong> absence<br />

<strong>of</strong> vibration structurally transmitted from <strong>the</strong> rotor, this mechanism will still vibrate<br />

<strong>the</strong> hull.<br />

In addition to <strong>the</strong> vibration sources noted above, in some flight regimes <strong>the</strong> rotor<br />

may ingest its own tip vortices. <strong>The</strong>se are mostly carried away by downwash in powered<br />

flight or upwash in autorotation, but in some conditions, such as <strong>the</strong> end <strong>of</strong> a landing<br />

approach or a roll manoeuvre, <strong>the</strong> vortex from one blade may hit <strong>the</strong> next blade headon.<br />

Figure 3.34(a) shows that <strong>the</strong> effect <strong>of</strong> a vortex approaching a blade is a local<br />

modulation <strong>of</strong> <strong>the</strong> RAFdirection causing a dip in <strong>the</strong> angle <strong>of</strong> attack. Figure 3.34(c)<br />

shows that as <strong>the</strong> vortex leaves <strong>the</strong> blade <strong>the</strong> angle <strong>of</strong> attack is increased. <strong>The</strong> time taken<br />

for <strong>the</strong> blade to transit <strong>the</strong> vortex is only a few milliseconds and so <strong>the</strong> resulting pressure<br />

dipulse shown at (c) produces audio frequencies. This is <strong>the</strong> origin <strong>of</strong> blade slap.<br />

In order to simplify study and to allow comparison between rotors turning at different<br />

speeds, <strong>the</strong> frequencies <strong>of</strong> vibration are always divided by <strong>the</strong> rotor frequency. Thus <strong>the</strong><br />

units <strong>of</strong> vibration are not cycles per second but cycles per revolution. An imbalanced<br />

rotor will cause a lateral vibration at <strong>the</strong> rotor frequency having a vibration frequency<br />

<strong>of</strong> one cycle per rev. This is usually abbreviated to ‘one-per’.<br />

In establishing <strong>the</strong> effect on <strong>the</strong> hull <strong>of</strong> vibrations created in <strong>the</strong> rotor, it is vital<br />

to appreciate that <strong>the</strong>re are two completely different mechanisms at work. Vibrations<br />

in <strong>the</strong> direction <strong>of</strong> <strong>the</strong> mast axis and torsional vibrations about <strong>the</strong> mast axis are<br />

directly transmitted and will be felt in <strong>the</strong> hull at <strong>the</strong> same frequency. However, <strong>the</strong><br />

rotor is turning with a frequency <strong>of</strong> its own and so vibrations in <strong>the</strong> plane <strong>of</strong> <strong>the</strong> rotor<br />

are taking place in a rotating frame <strong>of</strong> reference. When <strong>the</strong>se vibrations reach <strong>the</strong> hull,<br />

which is in a stationary frame <strong>of</strong> reference, <strong>the</strong> same frequency will not be felt. Instead,

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