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Gas Turbine Handbook : Principles and Practices

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<strong>Gas</strong> <strong>Turbine</strong> Systems Theory 45<br />

Chapter 4<br />

<strong>Gas</strong> <strong>Turbine</strong> Systems Theory<br />

GAS TURBINE OPERATING CYCLE<br />

The gas turbine cycle is best depicted by the Brayton Cycle.<br />

The characteristics of the operating cycle are shown on the<br />

pressure-temperature map, the pressure-specific volume map,<br />

<strong>and</strong> the temperature-entropy map (Figure 4-1a to 4-1c).<br />

The gas turbine, as a continuous flow machine, is best described<br />

by the first law of thermodynamics.<br />

where<br />

1 W 2<br />

W ( 1<br />

Q 2<br />

) ≡ W (h 2<br />

– h 1<br />

+ KE 2<br />

– KE 1<br />

+ PE 2<br />

– PE 1<br />

+ ——)<br />

J (4-1)<br />

W* = Mass flow rate, lb m<br />

/sec<br />

1 Q 2<br />

= H eat transferred to or from the system, Btu/lb m<br />

h 2<br />

= enthalpy of the fluid leaving, Btu/lb m<br />

h 1<br />

= enthalpy of the fluid entering, Btu/lb m<br />

KE 2<br />

= kinetic energy of the fluid leaving, Btu/lb m<br />

KE 1<br />

= kinetic energy of the fluid entering, Btu/lb m<br />

PE 2<br />

= potential energy of the fluid leaving, Btu/lb m<br />

PE 1<br />

= potential energy of the fluid entering, Btu/lb m<br />

1 W 2 = Work per unit mass on or by the system, ft-lb f /lb m<br />

J = Ratio of work unit to heat unit, 778.2 ft lb f<br />

/Btu<br />

1 W 2 /J = Work, Btu/lb m<br />

*Here mass flow is designated by W to distinguish it from 1<br />

W 2<br />

, which is used<br />

to designate work. Later in this text W a<br />

<strong>and</strong> W f<br />

(which are industry st<strong>and</strong>ards)<br />

are used to designate air flow <strong>and</strong> fuel flow.<br />

45

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