Page 84 - Handbook of Energy Engineering Calculations
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gives 1443.05 + 327.5 = 1770.55 Btu (1867.9 J) as the heat input per pound
               (kg) of steam.
                  The work done per pound (kg) of steam is: For mercury = (lb Hg/lb steam)
               (h  − H ) = 11.23(151.1 − 120.7) = 341.4 Btu (360.2 J). For steam = H  −
                  m1
                          me
                                                                                                        c1
               H  = 1499.2 − 909.1 = 590.1 Btu (622.6 J). Summing, as before, the total
                  se
               work done per pound (kg) of steam = 931.5 Btu (982.7 J).


               6. Compute the binary cycle efficiency
               The  binary  cycle  efficiency  =  [work  done  per  pound  (kg)  of  steam]/[heat
               input per pound (kg) of steam]. Or binary cycle efficiency = 931.5/1770.55 =
               0.526, or 52.6 percent.


               7. Calculate the steam cycle efficiency without the mercury topping turbine

               The steam cycle efficiency without the mercury topping turbine = [work done
               per pound (kg) of steam]/(H  − H ) = 590.1/(1499.2 − 69.7) = 0.4128, or
                                                           sf
                                                   s1
               41.3 percent.


               Related Calculations. Any binary cycle being considered for an installation
               depends on the effects of the difference in thermodynamic properties of the
               two  pure  fluids  involved.  For  example,  steam  works  under  relatively  high
               pressures  with  an  attendant  relatively  low  temperature.  Mercury,  by

               comparison,  has  the  vapor  characteristic  of  operating  under  low  pressures
               with attendant high temperature.
                  In a mercury-vapor binary cycle, the pressures are selected so the mercury

               vapor condenses at a temperature higher than that at which steam evaporates.
               The  processes  of  mercury  vapor  condensation  and  steam  evaporation  take
               place in a common vessel called the condenser-boiler, which is the heart of
               the cycle.
                  In the steam portion of this cycle, condenser water carries away the heat of

               steam condensation; in the mercury portion of the cycle it is the steam that
               picks  up  the  heat  of  condensation  of  the  mercury  vapor.  Hence,  there  is  a
               great  saving  in  heat  and  the  economies  effected  reflect  the  consequent

               improvement in cycle efficiency.
                  The  same  furnace  serves  the  mercury  boiler  and  the  steam  superheater.
               Mercury  vapor  is  only  condensed,  not  superheated.  And  if  the  condenser-
               boiler  is  physically  high  enough  above  the  mercury  boiler,  the  head  of
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