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Aviation and the Global Atmosphere

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<strong>Aviation</strong> <strong>and</strong> <strong>the</strong> <strong>Global</strong> <strong>Atmosphere</strong><br />

<strong>Aviation</strong> <strong>and</strong> <strong>the</strong> <strong>Global</strong> <strong>Atmosphere</strong><br />

Table of contents | Previous page | Next page<br />

7.4.1.2. Propulsive <strong>and</strong> Overall Efficiency<br />

O<strong>the</strong>r reports in this collection<br />

The power produced by engine thrust is <strong>the</strong> product of thrust <strong>and</strong> flight velocity (V). The ratio of this useful power to <strong>the</strong> increment in kinetic energy given to <strong>the</strong> flow in<br />

passing through <strong>the</strong> engine is <strong>the</strong> propulsive efficiency (h p ); a good approximation of this variable may written in <strong>the</strong> form h p = 2V/(V + V j ), where V j is <strong>the</strong> jet velocity.<br />

High levels of <strong>the</strong>rmal efficiency require <strong>the</strong> T 4 /T 2 ratio to be as high as possible with appropriate pressure ratio <strong>and</strong> component efficiencies. In <strong>the</strong> case of a simple<br />

turbojet gas turbine engine, this requirement would mean that <strong>the</strong> jet velocities are also relatively high. For example, for a ratio of T 4 /T 2 = 5.6 toge<strong>the</strong>r with an engine<br />

pressure ratio of 40, <strong>the</strong> jet velocity V j would be about 817 ms -1 , (Cumpsty, 1997). At Mach 0.85 at 10.7 km, when <strong>the</strong> flight velocity V is 252 ms -1 , <strong>the</strong> relationship<br />

shown above gives a propulsive efficiency of only about 47%. Thermal efficiency at this condition is about 48%, so h o = h p x h <strong>the</strong>rm = 0.48 x 0.47 = 23% for <strong>the</strong><br />

assumptions of this simplified example. For typical aircraft, overall efficiency ranges between 20 <strong>and</strong> 40%.<br />

The most practical method of raising overall efficiency is to lower <strong>the</strong> jet velocity <strong>and</strong> <strong>the</strong>reby increase propulsive efficiency; this approach has been adopted in <strong>the</strong><br />

bypass engine used so widely today. In this engine design, hot gases leaving <strong>the</strong> core turbine exp<strong>and</strong> through fur<strong>the</strong>r turbine stages, which drive <strong>the</strong> fan mounted in<br />

front of <strong>the</strong> core compressor. In most modern engines, <strong>the</strong> pressure ratio across <strong>the</strong> fan at cruise condition is about 1.6, giving a bypass ratio of about 6 <strong>and</strong> a jet<br />

velocity of about 400 ms -1 . At this jet velocity, propulsive efficiency is about 77% at a cruise speed of Mach 0.85 at 10.7 km. Unfortunately, losses associated with <strong>the</strong><br />

inefficiency of <strong>the</strong> fan <strong>and</strong> <strong>the</strong> turbine driving it inevitably reduce <strong>the</strong>se benefits somewhat, so a typical value for <strong>the</strong> overall efficiency of such an engine is currently<br />

about 30 to 37% at cruise. Increasing <strong>the</strong> bypass ratio clearly offers <strong>the</strong> prospect of fur<strong>the</strong>r increases in propulsive efficiency, but this approach has to be weighed<br />

against <strong>the</strong> penalties of increased size <strong>and</strong> weight of <strong>the</strong> installed engine <strong>and</strong> associated changes in drag (see Section 7.2 for fur<strong>the</strong>r discussion of airframe efficiency<br />

<strong>and</strong> installation effects). O<strong>the</strong>r prospects for increasing propulsive efficiency (e.g., propellers <strong>and</strong> unducted fans) are discussed in Section 7.4.3.<br />

http://www.ipcc.ch/ipccreports/sres/aviation/097.htm (1 von 3)08.05.2008 02:43:28

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