Page 494 - Bird R.B. Transport phenomena
P. 494

474   Chapter 15  Macroscopic Balances  for Nonisothermal Systems

                              Now we  use  Eq. 15.5-39  to eliminate р л  from  Eq. 15.5-41. Then we  have a first-order dif-
                           ferential  equation for p v  which may be integrated to give
                                                                         * " ?                П5.5-42»
                                         V2(p / )ly/(y  -                              •1>/y
                                            o Po
                           From  this  equation we can  obtain  the  time required  to discharge  any  given  fraction  of the
                           original  gas.
                              At  low  flow  rates the pressure p  at the nozzle opening is equal  to the ambient  pressure.
                                                        2
                           However,  examination of Eq. 15.5-41  shows  that, as the ambient pressure is reduced, the cal-
                           culated mass rate of flow reaches a maximum at a critical pressure  ratio

                                                                                              (15.5-43)

                           For air  (y  =  1.4), this critical pressure  ratio is 0.53. If the ambient pressure is further  reduced,
                           the pressure  just  inside  the nozzle will remain at the value  of p  calculated  from  Eq. 15.5-43,
                                                                              2
                           and  the mass  rate of flow  will become independent of ambient pressure  p . Under these con-
                                                                                      0
                           ditions, the discharge  rate is
                                                        V          9  \(y+D/(y-l)


                           Then, for p /p\ < r, we may write  Eq. 15.5-42 more simply:
                                   a

                                                 V( /p )y(2/(y  •
                                                      o
                                                   Po
                           or
                                            v/s
                                               2                                         r
                                                                                  tyJV\ < )   (15.5-46)

                           If p lp\  is initially  less than  r, both Eqs.  15.5-46  and  42 will be useful  for  calculating  the total
                             a
                           discharge time.


                           QUESTIONS FOR DISCUSSION

                        1.  Give the physical  significance  of each term in the five macroscopic balances.
                        2.  How are the equations  of change related to the macroscopic balances?
                        3.  Does each of the four  terms within  the parentheses  in  Eq. 15.1-2 represent a form  of energy?
                           Explain.
                        4.  How is the macroscopic (total) energy  balance related to the first law  of thermodynamics, ALJ =
                           Q+  W?
                                                       3
                        5.  Explain how the averages  (v) and (v ) arise in Eq. 15.1-1.
                        6.  What is the physical  significance  of E  and E ? What  sign  do they  have?  How are they related
                                                              v
                                                         c
                           to the velocity  distribution? How can they be estimated?
                        7.  How is the macroscopic balance for internal energy  derived?
                        8.  What  information can be obtained from  Eq. 15.2-2 about a fluid  at rest?

     PROBLEMS       15A.1.  Rates of heat transfer in a double-pipe heat exchanger.
                           (a)  Hot oil entering the heat exchanger  in Example  15.4-1 at surface  2 is to be cooled by  water
                           entering at surface  1. That is, the exchanger is being operated in countercurrent flow. Compute
                                                                                             2
                           the required  exchanger  area A, if the heat transfer  coefficient  U is 200 Btu/hr • ft  •  F and the
                           fluid  streams have the following  properties:
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