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106    CHAPTER 5 RATIONAL EFFICIENCY OF POWER PLANT




                If the turbine and feed pump of the cycle are not isentropic then the work output will be less than
             that of the ideal Rankine cycle and it is possible to define the efficiency ratio as
                                                           h cycle
                                           Efficiency ratio ¼                             (5.27)
                                                          h Rankine
                Substituting from Eqns (5.23) and (5.26) gives
                                                    w net  h 3   h 2  w net
                                   Efficiency ratio ¼    $      ¼
                                                   h 3   h 2 b 3   b 2  b 3   b 2         (5.28)
                                                 ¼ rational efficiency; h R

                This means that a steam turbine which operates on a reversible Rankine cycle will have a rational
             efficiency of 100% because the condenser temperature is T 0 . If there are any irreversibilities then the
             rational efficiency will be less than 100%. Rational efficiency shows the scope for improving the
             device within the constraints of, say, peak pressure and temperature. If the rational efficiency is low
             then the efficiency can be improved significantly, whereas if it is high then not much improvement is
             possible.
                It has to be remembered that these definitions of rational efficiency for a steam plant cycle
             are based on the dead-state temperature being made equal to the condenser temperature. If
             another temperature is chosen then the rational efficiency will be reduced as shown in
             Eqn (5.22). It will be shown that this results in a rational efficiency of unity for an ideal (internally
             reversible) Rankine cycle, and such an approach can be used to indicate how far an actual
             (irreversible) steam plant cycle falls short of the yardstick set by the reversible one. However, this
             approach also masks the ‘cost’ of external irreversibilities between the working fluid in
             the condenser and the true dead state of environmental conditions. These effects are discussed in the
             examples.
                When the term rational efficiency is applied to an air-standard cycle it is never possible to achieve a
             value of unity because the temperature at which energy is rejected is not constant. This will also be
             considered in the examples by reference to the Joule cycle for a gas turbine.


             5.4 EXAMPLES
             5.4.1 STEAM TURBINE CYCLES
             Q1. A steam turbine operates on a basic Rankine cycle with a maximum pressure of 20 bar and a
                 condenser pressure of 0.5 bar. Evaluate the thermal efficiency of the plant. Calculate the
                 maximum net work available from the cycle, and evaluate the rational efficiency of the cycle.
                Solution
                The T–s diagram for the Rankine cycle is shown in Fig 5.4. The parameters for the state points on
             cycle 1-2-3-4-6-1 will now be evaluated.
                Conditions at 4
                                             p 4 ¼ 20 bar;  x 4 ¼ 1

                                t s ¼ 212:4 C; h g ¼ 2799 kJ=kg; s g ¼ 6:340 kJ=kg K
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