Page 88 - Bird R.B. Transport phenomena
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Problems  73

                  (b)  By  making  a  mass  balance  over  the  gauge,  develop  an  approximate  relation  between
                  gauge pressure  /?, -  p 0 and  rate  of climb v z  for  a long continued  constant-rate  climb. Neglect
                  change  of air viscosity, and assume changes in air density to be small.
                  (c)  Develop an approximate expression  for  the "relaxation time" f rcl of the indicator—that is,
                  the time required  for  the gauge pressure  to drop  to 1 /e  of its initial value when  the external
                  pressure is suddenly  changed  from  zero (relative to the interior  of the gauge) to some  differ-
                  ent constant value, and maintained indefinitely  at this new value.
                  (d)  Discuss the usefulness  of this type of indicator  for small  aircraft.
                  (e)  Justify  the plus and minus signs in the figure.
                  Answers: (a) dp/dz  = -pg  =  -(pM/RT)g
                                             4
                          (b) pi -  p 0 ~  v z(8/xL/7rR )(MgV/R^T), where R ? is the gas constant and M is the mole-
                          cular weight.
                                            4
                              =  (m/7r)(/jiVL/7TD p),  where p  =  \(p,  +  p 0)
                          (c) t 0
             2D.1 Rolling-ball  viscometer.  An  approximate  analysis  of  the  rolling-ball  experiment  has  been
                                                             8
                  given, in which the results  of Problem  2B.3 are used.  Read the original paper and  verify  the
                  results.
                                  9
             2D.2 Drainage  of liquids  (see Fig. 2D.2).  How much liquid  clings to the inside surface  of a large
                  vessel when it is drained? As shown  in the figure there is a thin  film  of liquid  left  behind  on
                  the wall as the liquid  level  in the vessel  falls. The local  film  thickness  is a function  of both z
                  (the distance down  from  the initial liquid level) and t (the elapsed time).



                                Initial level of liquid










                               8(z, t) = thickness of film










                                  I Liquid level moving
                                  I  downward  with
                                  *     speed s
                                                      Fig. 2D.2  Clinging  of a viscous fluid  to wall of
                           Wall of containing vessel
                                                      vessel during draining.





                      s
                       H. W. Lewis, Anal.  Chem., 25, 507 (1953); R. B. Bird and  R. M. Turian, bid.  Eng. Chem.  Fundamentals,
                  3, 87 (1964); J. Sestak and  F. Ambros, Rheoi  Ada,  12, 70-76 (1973).
                      9
                       J. J. van Rossum, Appl.  Sci. Research, A7,121-144  (1958); see also V. G. Levich, Physicochemical
                  Hydrodynamics,  Prentice-Hall, Englewood  Cliffs, NJ.  (1962), Chapter  12.
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