Page 129 - DJJ20063- Thermodynamics 1
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DJJ20063- Thermodynamics 1



                      The steady  flow energy equation gives



                                        C  2                 C  2
                              gZ +  h +   1  +  Q =  gZ +  h +  2  +  W
                                 1   1               2   2
                                         2                    2

                      and with the flow rate, m (kg/s) the equation may be written as


                                            C  2  −C 2            
                                           +
                       Q  −W  = m   (h  − h  )   2  1     ( + gZ  − gZ  )                                 3.28)
                                                                     
                                            
                                   2   1       2          2     1  
                                                                     
                                 

                              In applying this equation to the boiler, the following points should be noted :
                              i.     Q is the amount of heat energy passing into the fluid per second

                              ii.    W is zero since a boiler has no moving parts capable of affecting a work

                                     transfer

                              iii.   The  kinetic  energy  is  small  as  compared  to  the  other  terms  and  may

                                     usually be neglected
                              iv.    The potential energy is generally small enough to be neglected.

                              v.     m (kg/s) is the rate of the flow of fluid.



                              Hence the equation is reduced to


                                     Q =  m  (h −  h 1 )                                                           (3.29)
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