Page 213 - Packed bed columns for absorption, desorption, rectification and direct heat transfer
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                                  The mean relative deviation of the equation is about 15%. About 91%
                           of the used experimental data are within a 30% band. It is to be expected that
                           the great difference between the experimental and predicted data is connected
                           with the great variety of packmgs for which the constants in the equation are
                           determined.
                                  For calculation of H, under the loading point, Billet and Schultes [316]
                           proposed the equation:


                                                      3/3
                                                                                             (83)



                           Here the hydraulic surface area Of, under the loading point is calculated by the
                           equations:

                           for Re L<5

                                      ls
                                          J
                           — = Cf,Rel Frl ;                                                  (84)
                            a

                           forRep-5

                                          3S
                                              J
                           ^- = 0,85C hRe° L Frl .                                           (85)
                            a
                           The experimental constant Q, for different types and dimensions of packings is
                           given in Table 10.

                           3.2.1.2.1.3.2. Liquid holdup over the loading point
                                  With increasing of the friction forces between the gas and the liquid
                           phases in the area of the loading point, their influence on the liquid holdup can
                           be neglect no more. Typical curves for the influence of the gas phase on the
                           liquid holdup, in case of metal Bialecki ring, taken from Billet [177], are
                           presented in Fig. 17.
                                  For determination of the liquid holdup over the loading point Otake and
                           Kimura [81] presented a graphical method in coordinates:


                           for    5<^<
                                   L
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