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4.3.  COMBUSTION GAS  TURBINES AND  ENGINES  65



               EXAMPLE
                      41.1
               Steam Requirement of a Turbine Operation
            Steam is fed to a turbine at 414.7 psia and 825°F and is discharged at
            64.7 psia. (a) Find the theoretical steam rate, lb/kWh, by using the
            steam tables.  (lb)  If  the isentropic efficiency is 70%, find the outlet
            temperature.  (c) Find the theoretical steam rate if  the  behavior is
            ideal, with CJC,  = 1.33.                             1421
               (a)  The  expansion  is  isentropic.  The  initial  and  terminal
            conditions are  identified in  the  following table  and  on the  graph.
            The data are read off  a large Mollier diagram (Keenan et al., Steam
            Tables, Wiley, New York, 1969).
                        Point   P   TOF   N    s
                         1    614.7   825   1421.4  1.642
                         2     64.7   315   1183.0  1.642
                         3     64.7   445   1254.5  1.730       M
                                                                -1
                                                               \
                                                                3
               AHs = H2 -HI  = -238.4  Btu/lb                  +
                                                               M
                                                                >
            Theoretical  steam  rate = 3412i238.4 = 14.31 lb/kWh.  This value is   Q
            checked exactly with th'e data of  Table 4.3.       2 1255
                                                                I
                                                               k-
                                                               z
               (b)  E&  -HI  =0.7(H2 - HI) = -166.9  Btu/lb    W
               H3 = 1421.4 - 166.9 = 1254.5 Btu/lb
            The  corresponding  values  of  &  and  S,  are  read  off  the  Mollier   1783
            diagram, as tabulated.
               (c)  The isentropic relation for ideal gases is
                     k
               AH=-     Rq[(Pz/q)(k-')'k - 11
                    k-1
                  - 1.987(1285) [(64.7/614.7)0-25 - 11
                  -
                      0.25
                                                                                 1-64   1.73
                                                                                 ENTROPY , BTU/( LB) (F)


            combustion gases. The name turboexpander is  applied to machines   transmission  lines  where  the  low  thermal  efficiency  is  counter-
            whose objective is to reduce the energy content (and temperature)   balanced by  the  convenience and  economy of  having the  fuel on
            of  the stream, as for cryogenic purposes.         hand.  Offshore  drilling  rigs  also  employ  gas  turbines.  Any  hot
               Gas expanders are used  to recover energy from high  pressure   process gas at elevated pressure is a candidate for work recovery in
            process gas streams in a plant when the lower pressure is  adequate   a turbine.  Offgases of  catalytic cracker regenerators,  commonly at
            for further processing. Power calculations are made in the same way   45psig  and  as  high  as  1250"F,  are  often  charged  to  turbines  for
            as those for compressors. Usually several hundred horsepower must   partial recovery of  their energy contents. Plants for the manufacture
            be  involved for  economic justification of  an expander.  In smaller   of  nitric acid by oxidation of  ammonia at pressures of  100 psig or so
            plants,  pressures  are  simply  let  down  with  throttling  valves   utilize expanders on the  offgases from the  absorption towers,  and
            (Joule-Thomson)  without attempt at recovery of  energy.   the  recovered  energy  is  used  to  compress the  process  air  to  the
               The specification sheet  of  Table 4.4 has room for the process   reactors.
            conditions  and  some  of  the  many  mechanical  details  of  steam   Combustion gas  turbine  processes are  diagrammed on Figure
            turbines.                                          4.2  and in Example 4.2. In the basic process, a mixture of  air and
                                                               fuel (or air alone) is compressed to 5-10  atm, and then ignited and
                  MBUSTlON  GAS TURBINES  AND  ENGINES         burned and finally expanded through a turbine from which power is
                                                               recovered. The process follows essentially a Brayton cycle which is
            When  a  low  cost  fuel  is  available,  internal  combustion  drivers   shown in Figure 4.2 in idealized forms on TS and PV diagrams. The
            surpass all others in compactness and low  cost of  installation and   ideal process consists of  an isentropic compression, then heating at
            operation.  FOT example, gas compression on a large scale has long   constant pressure followed by  an  isentropic expansion and  finally
            been done with integral engine compressors. Reciprocating engines   cooling  at  the  starting  pressure.  In practice,  efficiencies  of  the
            also  are widelly  used with  centrifugal compressors in low pressure   individual steps are high:
            applications,  but  speed  increasing  gears  are  needed  to  up  the
            300-600  rpm  of  the  engines to  the  3000-10,000 rpm  or  so  of  the
            compressor.                                         Compressor isentropic efficiency, 85%
               Process  applications  of  combustioin  gas  turbines  are  chiefly   Expander isentropic efficiency, 85-90%
            to  driving  pumps  and  compressors,  particularly  on  gas  and  oil   Combustion efficiency, 98%
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