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                       destroyed by irreversibilities within the system or control volume. Exergy balances can be written in
                       various forms, depending on whether a closed system or control volume is under consideration and
                       whether steady-state or transient operation is of interest. Owing to its importance for a wide range of
                       applications, an exergy rate balance for control volumes at steady state is presented alternatively as
                       Eqs. (12.12a) and (12.12b).

                                                            ˙
                                                                        ˙
                                                                           ˙
                                               0 =  ∑ E q, j –  W + ∑ E i – ∑ E e –  E D       (12.12a)
                                                      ˙
                                                                  ˙
                                                    j           i     e
                                                   ------------------------------- ---
                                                           rates of        rate of
                                                           exergy          exergy
                                                           transfer        destruction
                                                            ˙
                                          0 =  ∑   1 –  T 0 ˙  W + ∑ m ˙ i e i ∑ m ˙ e e e –  E D  (12.12b)
                                                                                ˙
                                                     ----- Q j –
                                                                      –
                                                       
                                               j     T j        i       e
                                                                                       ˙
                       ˙
                      W   has the same significance as in Eq. (12.7a): the work rate excluding the flow work. Q j   is the time rate of
                       heat transfer at the location on the boundary of the control volume where the instantaneous temperature
                       is T j  . The associated rate of exergy transfer is
                                                       E q, j =    1 –  T 0 ˙                (12.13)
                                                       ˙
                                                                  
                                                                 ----- Q j
                                                                 T j
                       As for other control volume rate balances, the subscripts i and e denote inlets and exits, respectively. The
                       exergy transfer rates at control volume inlets and exits are denoted, respectively, as  E i =  m ˙ ie i   and
                                                                                          ˙
                       E e =  m ˙ e e  . Finally,  E D   accounts for the time rate of exergy destruction due to irreversibilities within
                                       ˙
                       ˙
                             e
                       the control volume. The exergy destruction rate is related to the entropy generation rate by
                                                         E D =  T 0 S gen                       (12.14)
                                                          ˙
                                                                 ˙
                         The specific exergy transfer terms e i  and e e  are expressible in terms of four components: physical exergy
                       PH
                                                                         CH
                                      KN
                                                      PT
                       e , kinetic exergy e , potential exergy e , and chemical exergy e :
                                                    e =  e PH +  e KN  +  e PT  +  e CH        (12.15a)
                       The first three components are evaluated as follows:
                                                    PH
                                                                   (
                                                   e   =  ( hh 0 ) T 0 ss 0 )                 (12.15b)
                                                           –
                                                                     –
                                                                –
                                                           KN   1 2
                                                          e  =  --v                            (12.15c)
                                                                2
                                                           PT
                                                           e  =  gz                           (12.15d)
                       In Eq. (12.15b), h 0  and s 0  denote, respectively, the specific enthalpy and specific entropy at the restricted
                       dead state. In Eqs. (12.15c) and (12.15d), v and z denote velocity and elevation relative to coordinates
                       in the environment, respectively.
                         To evaluate the chemical exergy (the exergy component associated with the departure of the chemical
                       composition of a system from that of the environment), alternative models of the environment can be
                       employed depending on the application; see for example Moran (1989) and Kotas (1995). Exergy analysis
                       is facilitated, however, by employing a  standard environment and a corresponding table of  standard


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