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The Art of the Helicopter John Watkinson - Karatunov.net

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

Fig. 6.23 <strong>The</strong> duplex nozzle. (a)At idle <strong>the</strong> fuel flow is small and spring 2 forces <strong>the</strong> shuttle 1 to <strong>the</strong> right<br />

allowing fuel only through <strong>the</strong> idle nozzle. (b)As flow increases <strong>the</strong> shuttle admits fuel to <strong>the</strong> larger nozzle also.<br />

6.21 Power turbines<br />

<strong>The</strong> power turbine is <strong>the</strong> most highly stressed part <strong>of</strong> <strong>the</strong> engine as, like <strong>the</strong> compressor,<br />

it has to operate at high RPM but with <strong>the</strong> additional problems <strong>of</strong> working with high<br />

temperature gases and at higher power. Turbine inlet temperature may be between 700<br />

and 1200 ◦ C. As <strong>the</strong> temperature is so high, <strong>the</strong> speed <strong>of</strong> sound is correspondingly high<br />

and gas velocities in <strong>the</strong> turbine may reach 700 metres per second. <strong>The</strong> power turbines<br />

are almost always axial to provide sufficient flow. Like compressors, power turbines<br />

may have cascaded stages with stator vanes between. <strong>The</strong> power turbine extracts power<br />

from <strong>the</strong> gas flow by reducing its velocity, pressure and temperature. As <strong>the</strong> gases give<br />

up energy, <strong>the</strong>y expand and so <strong>the</strong> cross-sectional area <strong>of</strong> <strong>the</strong> turbine must increase<br />

towards <strong>the</strong> exhaust. As was seen in Chapter 3, a rotor is at its most efficient with<br />

uniform inflow. One <strong>of</strong> <strong>the</strong> functions <strong>of</strong> <strong>the</strong> stator is to modify <strong>the</strong> radial distribution<br />

<strong>of</strong> gas velocity and pressure so that <strong>the</strong> gas emerging from <strong>the</strong> adjacent rotor disc has<br />

uniform pressure and velocity from root to tip. <strong>The</strong> stator vanes also induce swirl in<br />

<strong>the</strong> direction <strong>of</strong> rotation. <strong>The</strong> rotor blades are not shaped like conventional airfoils, but<br />

have much deeper curvature or camber characteristic <strong>of</strong> reaction wheels.<br />

One <strong>of</strong> <strong>the</strong> greatest challenges in power turbine design is to control <strong>the</strong> temperature<br />

<strong>of</strong> parts exposed to <strong>the</strong> hot gas flow. In general oil cooling cannot be applied to <strong>the</strong><br />

rotating blades because <strong>of</strong> sealing difficulties and <strong>the</strong> extremely high oil pressure that<br />

would be built up due to <strong>the</strong> high rotational speed. Thus in practice <strong>the</strong> parts must be<br />

air cooled. Air from <strong>the</strong> compressor can be used for this purpose. Figure 6.24 shows<br />

that <strong>the</strong> stator vanes are hollow and can be fed with cooling air from both ends. <strong>The</strong> air<br />

can be arranged to exhaust into <strong>the</strong> gas flow via small drillings in <strong>the</strong> face <strong>of</strong> <strong>the</strong> vane. In<br />

this way an insulating boundary layer <strong>of</strong> air is provided which protects <strong>the</strong> thin trailing<br />

edge <strong>of</strong> <strong>the</strong> vane.<br />

<strong>The</strong> rotor blades are subject to extreme temperatures and extend in length considerably<br />

due to expansion. If sufficient tip clearance is provided for expansion, losses due

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