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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 />

7.4.1. Fundamental Thermodynamics<br />

The core of <strong>the</strong> basic gas turbine consists of three essential elements: The compressor, which<br />

mechanically increases <strong>the</strong> energy of <strong>the</strong> air (raising <strong>the</strong> pressure <strong>and</strong> temperature); <strong>the</strong><br />

combustor, in which fuel is burned (fur<strong>the</strong>r raising <strong>the</strong> temperature of <strong>the</strong> pressurized air); <strong>and</strong><br />

<strong>the</strong> turbine, which mechanically extracts enough energy from <strong>the</strong> hot compressed gas to drive<br />

<strong>the</strong> compressor (<strong>the</strong>reby reducing <strong>the</strong> pressure <strong>and</strong> temperature of <strong>the</strong> gas). A fraction of <strong>the</strong> net<br />

energy remaining in <strong>the</strong> gas after it leaves <strong>the</strong> turbine is <strong>the</strong>n available to be used in different<br />

ways, as shown in Figure 7-7. Case (a) uses an additional turbine stage to mechanically convert<br />

<strong>the</strong> energy to shaft work (such as might be required to drive a propeller or electric generator);<br />

case (b) is <strong>the</strong> turbojet, in which a nozzle is used to accelerate <strong>the</strong> gas (converting some of <strong>the</strong><br />

energy into kinetic energy), producing a high-speed jet that can be used to propel <strong>the</strong> vehicle;<br />

<strong>and</strong> case (c) is <strong>the</strong> turbofan, in which a fur<strong>the</strong>r turbine converts most of <strong>the</strong> energy of <strong>the</strong> gas into<br />

shaft work to drive <strong>the</strong> bypass air compressor, <strong>the</strong>reby producing <strong>the</strong> bypass jet that propels <strong>the</strong><br />

vehicle. For aircraft applications, <strong>the</strong> weight of <strong>the</strong> engine must be low in relation to <strong>the</strong> power<br />

output. This constraint has kept <strong>the</strong> aircraft type of gas turbine simple-much simpler than those<br />

now being built for l<strong>and</strong>-based power generation. (The implications of going to more complicated<br />

configurations are considered briefly in Section 7.4.4.)<br />

Figure 7-8: Gas turbine <strong>the</strong>rmal efficiency.<br />

The overall efficiency of an aircraft engine, h0 , is <strong>the</strong> mechanical power created by <strong>the</strong> thrust<br />

divided by <strong>the</strong> energy input rate of <strong>the</strong> fuel flow. It is convenient to express overall efficiencies by h0 = h<strong>the</strong>rm x hp , where h<strong>the</strong>rm is <strong>the</strong> <strong>the</strong>rmal efficiency <strong>and</strong> hp is <strong>the</strong><br />

propulsion efficiency; <strong>the</strong>se terms are considered below.<br />

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

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

http://www.ipcc.ch/ipccreports/sres/aviation/095.htm (2 von 2)08.05.2008 02:43:26<br />

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