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17.2 SIMPLE GAS TURBINE CYCLE ANALYSIS          397




                                                    (b)
                                                                   Maximum        3    5
                                                      Temperature, T                        2
                    (a)                                            temperature             Q

                         Heater    Heater                                         4
                    23    Q 23      Q 45
                                                                                      6
                                                        Q
                                                         1
                                4                                                4’
                      2        3         5    Power
                     C         T         T
                                                                                           Q
                                                                                            3
                                              W net
                     1            4       6                2



                                                          p 1
                                                           i
                               Cooler
                                                                                    Entropy, S
               FIGURE 17.15
               (a) Schematic diagram of gas turbine with reheat, (b) T–s diagram for gas turbine with reheat.


                  The ‘reheat cycle’ has a lower pressure ratio but would again obey the same equation – hence it
               would have a lower efficiency. Hence the gas turbine cycle with reheat has a lower efficiency than a
               basic cycle even though the mean temperature of energy addition is higher.
                  The reason for this is that reheating has, in addition to increasing the mean temperature of energy
               addition, increased the mean temperature of energy rejection also. The latter effect is greater than the
               former. Hence, to regain any efficiency benefit from reheating it is necessary to attempt to lower the
               mean rejection temperature: this can be achieved by heat exchange. Such a cycle is shown in
               Fig. 17.13, and it can be seen that the mean temperature of energy addition is raised relative to a
               standard cycle while the mean temperature of energy rejection is reduced. This cycle is more efficient
               than the standard one, and it is also more efficient than the heat exchange cycle (Fig. 17.10).
                  A similar effect occurs with intercooling. Figure 17.16 shows a gas turbine cycle with intercooling
               between two stages of the compressor. The effect of intercooling is to increase the amount of energy
               rejected from the cycle but it is difficult to assess the actual effect on efficiency. The method of doing
               this is to subdivide the intercooled cycle into ‘two cycles’. It can then be seen that intercooling
               effectively adds a low-pressure ratio cycle of low efficiency to the original cycle without intercooling –
               hence the overall efficiency is lower but the total work output is greater.
                  If a heat exchanger is fitted then the raising of the mean temperature of energy addition coupled
               with the lowering of the mean temperature of energy rejection brought about with the intercooler will
               raise the efficiency.
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