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6



                                                 FLOW  OF  FLUIDS




                    he transfer of fluids through piping and equipment is   rates. In this chapter, the concepts and theory of fluid
                    accompanied by friction and may result in changes   mechanics bearing on these topics will be reviewed briefly
                    in pressure, velocity, and elevarion. These effects   and practical and empirical methods of sizing hes and
                    requ,ire input of energy to maintain flow at desired   auxiliary equipment will be emphasized.



             6.1.  PRQPERTES AND  UNITS                         For nonideal gases a general relation is
             The  basis  of  flow  relations  is  Newton’s relation  between  force,
             mass, and acceleration, which is                       p = MP/zRT,                              (6.4)
                                                                where the compressibility factor z is correlated empirically in terms
                F = (m/s,)a.                              (6.1)   of  reduced properties  TIT, and P/P, and the  acentric factor. This
                                                                 subject is treated for example by Reid et al. (1977, p. 26) and Walas
             When F and a are in lb units, the numerical value of the coefficient   (1985, pp.  17, 70). Many PVT equations of  state are available. That
             is gc = 32.174 Ib ft/’lbfsec2. In some other units,   of  Redlich and Kwong may be written in the form
                     kg m/sec”   g cm/sec*   kg m/sec*
                g  =I--= 1  ~-         -9.ao6-.                     V = b + RT/(P + a/fiV2),                 (6.5)
                       N          dw           kg,
                                                                which is suitable for solution by direct iteration as used in Example
             Since the  common engineering units  for  both  mass  and  force are   6.1.
             llb, it  is  essential  to  retain  g,  in  all  force-mass  relations.  The   Flow rates are expressible as linear velocities or in volumetric,
             interconversions may  be  illustrated with  the  example of  viscosity   mass,  or  weight  units.  Symbols  for  and  relations  between  the
             whose basic definition is force/(velocity)(distance).  Accordingly the   several modes are summarized in Table 6.1.
             viscosity in various units relative to that in SI units is   The  several  variables  on  which  fluid  fiow  depends  may  be
                                                                 gathered into  a smaller number of  dimensionless groups,  of  which
                         1
                1 Ws/mz = __ kg,  s/m2 = 10 g/(cm)(s)           the  Reynolds  number  and  friction  factor  are  of  particular
                        9.806                                    importance. They are defined and written in the common kinds of
                      = 10 P = 0.0672 lb/(ft)(sec)              units  also  in  Table  6.1.  Other  dimensionless groups  occur  less
                                                                frequently and will  be  mentioned as they occur in this  chapter;  a
                      -- 0‘0672 Ibf sec/ft’ = 0.0020189 lbf sec/ft2
                      -
                        32.174                                  long  list  is  given  in  Perry’s  Chemical  Engineers  Handbook
                                                                 (McGraw-Hill, New York, 1984, p. 5.62).
             In data  book’s, viscosity may  be  recorded  either in force or  mass
             units. The particular merit of SI units (kg, m, s, N) is that g, = 1 and
             much  confusion can be  avoided by  consistent use  of  that  system.
             Some numbeIs of  frequent use in fluid Wow  problems are
                                                                    EXAMPLE 6.1
             Viscosity:  1 cPoise = 0.001 N s/m2 = 0.41134 Ib/(ft)(hr).   Density of a Nonideal Gas from Its Equation of State
             Density:  1 g m/crn3 = 1000 kg/m3 = 62.43 lb/ft3.   The Redlich-Kwong  equation of  carbon dioxide is
             Specific weight:  62.43 Ibf/cuft = 1000 kg,/m3.
             Pressure:  1 afm = 0.10125 MPa = 0.10125(106) N/m2 = 1.0125 bar.   (P + 63.72(106)/fiV2)(V  - 29.664) = 82.05T
                Data  of  densities of  liquids are  empirical in  nature,  but  the   with P in atm, V in mL/g mol and Tin K. The density will be found
             effects of temperature, pressure, and composition can be estimated;   at P = 20 and T = 400.  Rearrange the equation to
             suitable methods are described by  Reid  et al.  (Properties of  Gases
             and  Liquids, McGraw  Hill, New  Yorlr,  1977),  the  APZ  Refining   V = 29.664 + (82.05)(400)/(20 + 63.72(1O6)/$$%V2).
             Data Book (American Petroleum Institute, Washington, DC, 1983),
             and the AlChE Data  Prediction Manual  (1984-date).  The densities   Substitute the ideal gas volume on the right, V = 1641; then find V
             of  gases are represented by equations of  state of  which the simplest   on the  left;  substitute that  value on the  right,  and  continue.  The
             is that of  ideal gases; from this the density is given by:   successive values of V are

                p = 1/V = MP/RT,  massfvolume             (6.2)    V = 1641, 1579, 1572.1, 1571.3, 1571.2, . . .  mL/g mol
             where A4  is  the molecular weight. For air, for example, with  P in   and converge at 1571.2. Therefore, the density is
             atm and T in “R,
                                                                   p = 1/V = 1/1571.2,  or  0.6365 g mol/L  or  28.00 g/L.
                   29p   Ib/cuft.                         (6.3)
                p=m’
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