Page 225 - Modelling in Transport Phenomena A Conceptual Approach
P. 225

7.5.  CONSERVATION OF ENERGY                                        205


           Solution
           a) System:  Contents of  the tank

           Assumptions
             1.  Properties of  the tank contents are uniform, ie., Hout  = Hsys.

             2.  Heat  transfer between the system and  its surroundings  is almost  zero.  Note
                that the insulation around the tank does not necessarily  imply that Qint = 0.
                Since the tank wall is in the surroundings,  there will be heat transfer between
                the  tank  wall  and  air remaining  in the tank  during the evacuation process.
                Heat  transfer may be  considered negligible when  (i) the mass of  the wall is
                small,  (ii) process takes place rapidly  (remember that heat  transfer is a slow
                process).
           Analysis

           Since nin = nint  = 0 and there is no chemical  reaction, Eq.  (7.3-2) reduces to




           Integration  of Eq.  (1) yields
                                       nsYs = no - 12t                         (2)

           where no is the number of  moles of  air initially present in the tank, i.e.,

                        no=-- POV  -       (7)(0*5)       = 130.3mol
                             RT,    (8.314 x 10-5)(50 + 273)
           On the other hand,  the inventory  rate  equation for energy,  Eq.  (7.5-5), takes the
          form







           Substitution  of  Eqs.  (1) and  (2) into Eq.  (3)  gives
                                         -
                                                          fays
                             - 12 (flout - Us,,)  = (no - 12 t) -              (4)
                                   I
                                                           dt
           Since H  = U+Pv = O+RT, the use of  the first assumption enables us to express
           the left-hand  side of  Eq.  (4) as
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