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                                  Ramm [96, p.446] proposed the expression:


                                 AL
                           a.- —      .                                                     000)



                           where A and B are experimental constants. For Raschig rings and saddles 25-50
                           mm, A=%5 and 5=0.00125. The accuracy of the equation is ±25%. For 50 mm
                           Raschig rings, it is better to use .4=83.5 and ,6=0.00067. It is surprising that the
                           influence of the specific surface area of the packing is not taken into account in
                           this equation. This can be explained only with the small interval of changing of
                           this value.
                                  Using data obtained with the method described in 2.1.2.5.7., Hikita,
                           Kataoka and Nakanishi [99] obtained the equation:



                                      l a  m  ,                                             (101)
                            a

                           where m = bd" . The value of a in this equation is in mN/m. d is the packing
                           element diameter, m.
                                  The values of the constants A, bandp are as follows:
                                             A                 B                 P
                           Rings             2.26              1.83              0.48
                           Saddles           0.707             0.495             0.98

                                  Because of some shortcomings of the method for obtaining the
                           experimental constants, discussed in 2.1.2.5.7., this equation is not to be
                           recommended.
                                  Another equation for calculation of the effective surface area of random
                           packings is suggested by Onda et al. [92]:


                                                         0M
                                                75
                                                      0J
                                                             OJ
                                               f-  Re L Ff We J,                            (102)
                                          L
                           where Re L = '  is the Reynolds number; Fr = —— - Froude number; We
                                        o-Mi                               8
                              3
                           = L fi/(er.a)- Weber number; a- surface tension in N/m; and a^ critical surface
                           tension at which the wettabiliry angel is zero. Principally this equation is unable
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