Page 87 - Bird R.B. Transport phenomena
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72   Chapter 2  Shell Momentum  Balances and Velocity Distributions in Laminar Flow

                           (a)  Begin by analyzing the system without the rotation  of the cone. Assume that it is possible
                           to apply the results  of Problem  2B.3 locally. That is, adapt the solution  for the mass flow  rate
                           from that problem by making the following replacements:
                           replace  (9> 0 -  SP L )/L by  -d<3>/dz
                           replace  W by        2rrr = 2TTZ sin /3
                           thereby obtaining





                           The mass flow rate w is a constant over the range  of z. Hence this equation can be integrated
                           to give

                                                                  ^     ln  ¥                  (2C.6-2)

                           (b)  Next, modify  the above result to account for the fact that the cone is rotating with angular
                           velocity П. The mean centrifugal force per unit volume acting on the fluid  in the slit will have
                           a  z-component approximately given by
                                                                     2
                                                                          2
                                                       (Fcentrif.) 2  = Kp^ z sin  p             (2C.6-3)
                           What  is  the value  of  K? Incorporate  this  as  an  additional  force  tending to  drive  the  fluid
                           through the channel. Show that this leads to the following expression for the mass rate of  flow:
                                                                                   2 L
                                                                                   l\
                                              4тгВ р sin p  [<9>i  "  9>) + <Щ1 2  sin 2  p)(L\  - L )
                                                  3
                                           w  =   *             2  1  n  /T \                  (2C.6-4)
                                                  Зд    |_         ln  (L /L )
                                                                       2  }
                           Here 9>j = p t  + pgL, cos p.
                      2C.7  A  simple rate-of-climb indicator (see Fig. 2C.7).  Under the proper circumstances the simple
                           apparatus  shown in the figure  can be used  to measure the rate  of  climb of an airplane. The
                           gauge pressure inside the Bourdon element is taken  as proportional  to the rate  of climb. For
                           the  purposes of this problem the apparatus may be assumed to have the following properties:
                           (i)  the capillary tube (of radius R and length L, with R «  L) is  of negligible volume but ap-
                           preciable  flow  resistance; (ii) the Bourdon element has a constant volume V and offers  negli-
                           gible resistance to flow;  and (iii) flow  in the capillary is laminar and incompressible, and the
                           volumetric flow  rate depends only on the conditions at the ends of the capillary.


                                       Rate of climb





                                                  • Bourdon
                           Capillary^,    ^   /    element
                             tube
                              Pressure        Pressure
                             outside = p 0   i n s i d e  "  Pi  Fig. 2C.7  A rate-of-climb indicator.


                           (a)  Develop an expression for  the change of  air pressure with  altitude, neglecting tempera-
                           ture changes, and considering air to be an ideal gas  of  constant  composition.  (Hint: Write a
                           shell balance in which the weight  of gas is balanced against the static pressure.)
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