Page 45 - Handbook of Electrical Engineering
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24    HANDBOOK OF ELECTRICAL ENGINEERING


























                            Figure 2.5 Gas turbine thermodynamic cycle. Simple-cycle gas turbine.

              ‘simple-cycle’ version of the Joule cycle. The main components of the gas turbine are shown in
              Figure 2.5.
                    The thermodynamic relationships used to describe the operation of the gas turbine are the
              pressure (P ) versus volume (V ) characteristic in Figure 2.6 and the temperature (T ) versus entropy
              (S) characteristic in Figure 2.7. These figures also show the effect of practical inefficiencies that
              occur both in the air compressor and the turbine.

                    Air is drawn into the compressor at atmospheric pressure P 1 (in practice slightly lower due to
              the inlet silencer, filter and ducting) and atmospheric temperature T 1 , and compressed adiabatically
              to a higher pressure P 2 to reduce its volume to V 2 and raise its temperature to T 2 . The adiabatic
              compression is given by the following equations; see standard textbooks e.g. References 1 to 5.

                                              P 2 V 2  P 1 V 1
                                                   =      = constant                          (2.1)
                                               T 2    T 1
                                                         γ
                                                 γ
                                             P 2 V 2 = P 1 V 1 = constant                     (2.2)
              The work done in the compressor per kg of fluid U c is,

                                                    γ
                                             U c =     (P 2 V 2 − P 1 V 1 )                   (2.3)
                                                  γ − 1
              The following standard relationships apply,

                                                    P 1 V 1 = RT 1                            (2.4)
                                                    P 2 V 2 = RT 2                            (2.5)
                                                 C p − C v = R                                (2.6)

                                                      C p
                                                         = γ                                  (2.7)
                                                      C v
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