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

Fig. 8.10 Minimum and maximum airspeed as a function <strong>of</strong> density altitude. Note that at <strong>the</strong> operational<br />

ceiling <strong>the</strong>re is only one airspeed available.<br />

can increase rotor efficiency by reducing RRPM. This will reduce pr<strong>of</strong>ile drag and<br />

require a larger angle <strong>of</strong> attack so that <strong>the</strong> lift to drag ratio will improve. Whilst very<br />

low RRPM is dangerous because it may not be possible to recover, a reduction <strong>of</strong> 10%<br />

is quite safe and has a dramatic effect on autorotation range. Prior to landing RRPM<br />

can be recovered by gradual application <strong>of</strong> back cyclic. In some machines <strong>the</strong> use <strong>of</strong><br />

low RRPM may result in increased vibration if <strong>the</strong> rotor detuning has been optimized<br />

for a narrow RRPM range.<br />

Figure 8.9 applies at one density altitude only and obviously climb or descent will<br />

change that. Figure 8.10 shows an alternative way <strong>of</strong> depicting <strong>the</strong> performance. This is<br />

a chart <strong>of</strong> minimum and maximum airspeed as a function <strong>of</strong> density altitude. Minimum<br />

power and maximum range speeds may also be shown as a function <strong>of</strong> density altitude.<br />

At sea level minimum airspeed is zero showing that vertical climb is possible. At some<br />

density altitude <strong>the</strong> HOGE power will exceed available power and <strong>the</strong>n <strong>the</strong> minimum<br />

speed becomes non-zero. At sea level <strong>the</strong> maximum airspeed is power limited but may<br />

peak at some density altitude where reduced air density is reducing pr<strong>of</strong>ile drag and<br />

improving rotor L/D. At higher density altitude maximum airspeed will fall again. As<br />

density altitude increases, <strong>the</strong> available power falls down into <strong>the</strong> power-required curve<br />

and <strong>the</strong> differences between minimum power speed, minimum airspeed and maximum<br />

airspeed become smaller. Where <strong>the</strong>se speeds coincide, <strong>the</strong> absolute ceiling has been<br />

reached. As <strong>the</strong> absolute ceiling can only be reached asymptotically, <strong>the</strong> service ceiling<br />

is <strong>of</strong>ten taken to be a slightly lower density altitude at which a rate <strong>of</strong> climb <strong>of</strong> 100 fpm<br />

remains.<br />

Given <strong>the</strong> existence <strong>of</strong> a minimum airspeed, potentially a helicopter could take <strong>of</strong>f<br />

vertically at sea level with a full load and fly to some high altitude destination at best<br />

rate <strong>of</strong> climb speed where an attempted vertical landing would result in a crash. <strong>The</strong><br />

fact that this does not happen in practice is due to a combination <strong>of</strong> <strong>the</strong> availability<br />

<strong>of</strong> power curves in <strong>the</strong> flight manual and piloting techniques that establish what <strong>the</strong><br />

power margin is before attempting a landing.

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