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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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<strong>Helicopter</strong> performance 327<br />

Fig. 8.1 A density/altitude chart. This allows density altitude to be obtained from pressure altitude. <strong>The</strong> chart<br />

corrects for ISA standard lapse rate and allows compensation for non-ISA temperature. See text.<br />

subject to considerable variations. Sustained flight is not possible where demand<br />

exceeds available power. In <strong>the</strong> opposite case, flight in equilibrium is possible with<br />

a power surplus, usually called a power margin, which can be used for climbing or for<br />

manoeuvres.<br />

In general <strong>the</strong> engine(s) provide power which has a physical limit to <strong>the</strong> transmission<br />

which has a physical torque limit. For a constant RPM machine such as a helicopter<br />

rotor, power is proportional to torque and engines may be described in terms <strong>of</strong> torque<br />

available. <strong>The</strong> engine power/torque available will be a function <strong>of</strong> density altitude. <strong>The</strong><br />

rate at which fuel can be burned is limited primarily by <strong>the</strong> temperature that <strong>the</strong> power<br />

turbine blades can withstand. At low altitude, <strong>the</strong> compressor can produce plenty <strong>of</strong><br />

mass flow and <strong>the</strong> combustion takes place with excess air that limits <strong>the</strong> power turbine<br />

temperature. As altitude increases <strong>the</strong> air density falls and <strong>the</strong> mass flow reduces. At<br />

some point <strong>the</strong> amount <strong>of</strong> fuel burned must be reduced to prevent excessive turbine

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