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Air standard cycles

In their original air standard cycle analysis, using constant specific heats, Hawthorne and Davis 4 considered the dry [CBTIiXr cycle. They assumed a perfect heat exchanger, with the specific heats of gas and air constant and identical, so that Ty becomes equal to Tj in Fig. 6.6. From their examination of the enthalpy-entropy diagram of this... [Pg.91]

Note also that the heat rejected is equal to the compressor work in this case. For this air standard cycle with constant specific heats, Eq. (6.17) reduces simply to... [Pg.92]

The rea.son for this choice of low pressure ratio is illustrated by an approximate analysis [12], which extends the graphical method of calculating gas turbine pierformance described in Chapter 3. If the gas turbine higher plant is assumed to ojjerate on an air standard cycle (i.e. the working fluid is a perfect gas with a constant ratio of specific heats, y), then the compressor work, the turbine work, the net work output and the heat supplied may be written as... [Pg.123]

Here, we first discuss whether such semi-closure (which is introduced so that CO2 separation can be undertaken more easily) is likely to lead to higher or lower thermal efficiency, and in this discussion it is helpful to consider recirculation in relation to an air standard cycle (see Fig. 8.4). Fig. 8.4a shows a closed air standard cycle with unit air flow Fig. 8.4b shows an open cycle similarly with unit air flow and an air heater rather than a combustion chamber. The cycles are identical in every respect except that in the former the turbine exhaust air from the turbine is cooled before it re-enters the compressor. In the latter, the turbine exhaust air is discharged to atmosphere and a fresh charge of air is taken in by the compressor. The quantities of heat supplied and the work output are the same for each of the two cycles, so that the thermal efficiencies are identical. [Pg.139]

In contrast to the air-standard cycle, the fuel-air cycle is a cycle in the mechanical sense only. It is not... [Pg.563]

The effect of increasing the compression ratio, defined as the ratio of the volumes at the beginning and end of the compression stroke, is to increase the efficiency of the engine, i.e., to increase the work produced per unit quantity of fuel. We demonstrate this for an idealized cycle, called the air-standard cycle, shown in Fig. 8.9. It consists of two adiabatic and two constant-volume steps, which comprise a heat-engine cycle for which air is the working fluid. In step DA, sufficient heat is absorbed by the air at constant volume to raise its temperature and pressure to the values resulting from combustion in an actual Otto engine. Then the air is expanded adiabatically and reversibly (step AB), cooled... [Pg.141]

The thermal efficiency 17 of the air-standard cycle shown in Fig. 8.9 is simply... [Pg.142]

Consider an air-standard cycle for representing the turbojet power plant shown in Fig. 8.13. The temperature and pressure of the air entering the compressor are 1 bar and 30°C. The pressure ratio in the compressor is 6,5, and the temperature at the turbine inlet is l,I00°C. If expansion in the nozzle is isentropic and if the nozzle exhausts at 1 bar. what is the pressure at the nozzle inlet (turbine exhaust) and what is the velocity of the air leaving the nozzle ... [Pg.147]


See other pages where Air standard cycles is mentioned: [Pg.28]    [Pg.33]    [Pg.216]    [Pg.217]    [Pg.329]    [Pg.88]    [Pg.90]   
See also in sourсe #XX -- [ Pg.28 , Pg.33 , Pg.48 , Pg.68 ]




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