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70  TRANSFER  OF  SOLIDS



                   EXAMPLE 5.1
                   Conditions of a Coal Slurry Pipeline
               Data of  a pulverized coal slurry are

                   C, = 0.4,
                   D = 0.333 ft,
                    f= 0.0045 (Blasius’ eq. at N,  = lo5),
                    s = 1.5.

                     Mesh size         24   48   100   Mixture
                     d(rnrn)          0.707  0.297  0.125   0.321
                     Weight fraction   0.1   0.8   0.1   1
                     u, (ft/sec)      0.164  0.050  0.010   0.0574
                The terminal velocities are read off Figure 5.1, and the values of the
                mixture are weight averages.
                   The following results are found with the indicated equations:
                       Item       Eq.   24   48   100  Mixture
                       “c        5.1   7.94  5.45  3.02
                       k         5.8   1.36  2.89  9.38   3.39
                                  5.6  20.6
                                          6.27  1.25
                       AEIAPL    5.1 1             1.539
                       AEI4      5.13              1.296
                   Eq. (5.1):   up = 34.6(0.4)(0.333)vwF7304.8
                                                     mrn

                                 8.41~~
                   Eq. (5.6):   u =--
                                Vmm - 125u,,
                                4 32.2(1.5 - 1) d,,   - 0.0704drnrn
                   Eq. (5.8):   CD =-     --
                                3    u:   304.8    u;   ’
                                    069 [ - JTZ@~~BE-J~~
                                           i
                             Ae
                   Eq. (5.11):  --l+-
                                -
                            APL     0.4°.3  0.0574   304.8(3.39)’                       Sphere  diameter.  ern
                                = 1.5391,                          Figure 5.1. Settling velocities of  spheres as a function of  the ratio 01
                                               (0.0574)’(3.39)  1
                   Eq.  (5.13):   ~  A&  -   0.0045(0.333)32.2(0.5)   densities of  the two phases.  Stokes law applies at diameters below
                                - 1 + 0.272(0.4)[
                                                                    approximately 0.01 cm (based on a chart of Lupple et ul.,  Chemical
                            APL                                     Engineering Handbook, McGruw-Hill, New York, 1984, p. 5.67).
                                = 1.296.
                With  coal  of  sp gr = 1.5,  a  slurry  of  40~01% has  a  sp gr = 1.2.
                Accordingly the rule,  AelAP, = sp gr, is not confirmed accurately
                by these results.                                  For particles of  one size, Eqs. (5.7) and (5.8) combine to
                                                                       APs/APL = 1 + ~OOC,[(U,D/U’)~~~~.~,
                                                                                                  consistent units.  (5.10)
                The drag coefficient is                            The pressure drop relation at the critical velocity given by Eq. (5.1)
                                                                   is found by substitution into Eq. (5.7) with the result


                                                                       Ae/APL = 1 + 0 L[(l/ut)qgd(s   - 1)/CDJ’3.   (5.11)
                                                                                   69
                                                                                  c:3
                For mixtures, a number of  rules has been proposed for evaluating
                the  drag  coefficient,  of  which  a  weighted  average  seems  to  be   With Eq. (5.10) the result is
                favored.
                                                                       Ae/APL = 1 + 1/C:3.                      (5.12)
                                                                    With the velocity from Eq. (5.6),  Eq. (5.7) becomes
                where the wi are the weight fractions of  particles with diameters di.   Ae/APL = 1 + 0.272Cu[fgD(s - ~)/u:G]’.~   (5.13)
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