20.01.2013 Views

The Art of the Helicopter John Watkinson - Karatunov.net

The Art of the Helicopter John Watkinson - Karatunov.net

The Art of the Helicopter John Watkinson - Karatunov.net

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

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

temperature. From <strong>the</strong>n on available power must fall. However, <strong>the</strong> fall in power is not<br />

as steep as might be expected because intake air temperature falls with altitude and<br />

this <strong>of</strong>fsets <strong>the</strong> loss <strong>of</strong> density due to reduced pressure to some extent. As a result <strong>the</strong><br />

engine power/torque available curve may show <strong>the</strong> characteristic knee <strong>of</strong> Figure 8.2.<br />

At low density altitudes <strong>the</strong> torque must be kept within <strong>the</strong> constant transmission limit<br />

whereas above a certain density altitude <strong>the</strong> available torque falls.<br />

<strong>The</strong> rotors in turn require power that is a complex function <strong>of</strong> density altitude and<br />

airspeed. <strong>The</strong> power will be delivered to <strong>the</strong> main and tail rotors and will be absorbed<br />

by various forms <strong>of</strong> drag. Power required to hover is clearly important and <strong>the</strong> worst<br />

case will be at zero airspeed. Figure 8.3 shows a typical chart relating hover power<br />

Fig. 8.2 Power available may be constant at low altitude owing to a transmission limit until turbine temperature<br />

limits dominate at higher density altitude.<br />

Fig. 8.3 Simple hover power chart.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!