Page 152 - Advanced Gas Turbine Cycles
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Chapter 7.  The combined cycle gas turbine (CCGT)   123

                                 Exhaust           DtFH






















      Fig. 7.8.  Single pressure steam cycle system with LP evaporator in a pre-heating  loop, as  alternative to feed
                                 heating (after Wunsch [I 11).
         Kehlhofer regards the two pressure system as a natural extension of the single pressure
      cycle with a low pressure evaporator acting as a pre-heater. Under some conditions more
      steam could be produced in the LP evaporator than is required to pre-heat the feed water
      and this can be used by admitting it to the turbine at a low pressure. For a fuel with high
      sulphur content (requiring high feed water temperature (Tb) at entry to the HRSG), a dual
      pressure  system  with  no  low pressure  water  economiser  may  have  two  regenerative
      surface feed heaters and a pre-heating loop. For a sulphur free fuel (with a lower Tb), a
      dual  pressure  system  with  a  low  pressure  economiser  may  have  a  single-stage
      deaeratoddirect contact feed heater using bled steam.



      7.6.  The optimum pressure ratio for a CCGT plant
        Rufli’s calculations (Fig. 7.7a, b), indicated that the optimum pressure ratio for a CCGT
      plant is relatively low compared with that of a simple gas turbine (CBT) plant. In both
      cases, the optimum pressure ratio increases with maximum temperature. Davidson and
      Keeley [6] have given a comparative plot of the efficiencies of the two plants (Fig. 7.9),
      showing that the optimum pressure ratio for a CCGT plant is about the same as that giving
      maximum specific work for a CBT plant.
        The reason for this choice of low pressure ratio is illustrated by an approximate analysis
      [ 121,  which  extends  the  graphical  method  of  calculating  gas  turbine  performance
      described in Chapter 3. If  the gas turbine higher plant is assumed to operate on an air
      standard cycle (Le. 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

           mw w:: = (x - l)/q(-(O - I),                                   (7.27)
                  =
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