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Sustaining Operational Ef ficiency of a CHP System     279


             constant value for the heat capacity, c   can be evaluated at the average of the HRU
                                             p,ex
             inlet and outlet temperatures.
                Using Eqs. (17-12) and (17-13), Eq. (17-11) can be rewritten as

                                        ρ (   vc  )  (T  − T    )
                                 ε   =     p  HRU,w  HRU, ,w o  HRU, ,w i       (17-14)
                                  HRU                    −
                                       ρ (   vc  )  (T     T     )
                                                               w
                                          p HHRU,min  HRU,ex,i  HRU, ,i
             Similarly, if hot air is generated instead of hot water, Eq. (17-14) can be rewritten as
                                         ρ (   vc  )  (T  − T   )
                                 ε   =      p  HRU,a  HRU, ,a o  HRU, ,a i      (17-15)
                                  HRU                     −
                                        ρ (   vc  )  (T    T     )
                                            H
                                           p HRU,min  HRU,ex,i  HRU, ,i
                                                               a
                One of the flow rates appearing in Eq. (17-14) can be eliminated using a heat bal-
             ance on the HRU, that is, the heat loss by the exhaust gas as it passes through the HRU
             (Q     ) is equal to the sum of the heat gain by the water as it passes through the HRU
               HRU,ex
             (Q    ) and heat losses through the walls of the HRU (L  ):
               HRU,w                                         HRU
                                        Q     = Q     + L                       (17-16)
                                         HRU,ex  HRU,w  HRU
             Here,
                                 Q     = (ρ   vc )  T (   −  T    )             (17-17)
                                  HRU,ex    p HRU,ex  HRU,ex,  i  HRU,ex, o
             and
                                 Q     = (ρ   vc )  T (  − T     )              (17-18)
                                   HRU, w   p HRU,  w  HRU,,  HRU,,
                                                               w i
                                                       w o
                The rate of heat loss through the walls will generally be very small compared to
             both Q     and Q     [approximately 1.5 percent of Q  for a heat recovery steam
                   HRU, ex   HRU,w                          HRU,ex
             generator (HRSG) according to Kovacik (1982), p. 213)]. Therefore, L   can be neglected
                                                                     HRU
             without introducing significant errors, and   v  can be obtained as a function of
                                                       ,
                                                    HRU ex
               v   from Eq. (17-16) as
              HRU, w
                                      (ρ c )    T (    −  T   )
                                 v  =    p HRU, w  HRU, w o ,  HRU , w i ,  v   (17-19)
                               HRU,ex  (ρ c )  (T     −  T    )  HRU,w
                                                            ,
                                         p HHRU,ex  HRU ex,i  HRU ex,o
                                                   ,
             Substituting this expression for   v  into Eq. (17-14), we obtain
                                         HRU,ex
                                            (T      − T     )
                                      ε   =   HRU,ex,i  HRU,ex,o                (17-20)
                                       HRU   (T     − T     )
                                              HRU,ex,i  HRU,w,,i
             for an HRU that uses exhaust gases from a prime mover to produce hot water, when
             (ρ   vc  )  = (ρ   vc  )  , which will ordinarily be true.
                 p HRU,  min  p HRU, ex
                Following similar logic for an HRU that uses exhaust from a prime mover to heat
             air, from Eq. (17-15),
                                             (T     − T     )
                                      ε   =   HRU,ex,i  HRU,ex,o                (17-21)
                                       HRU   (T     − T     )
                                               HRU,ex,i  HRU,a,,i
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