Page 80 - Packed bed columns for absorption, desorption, rectification and direct heat transfer
P. 80

75


                                        4L
                           where Re L =      is the Reynolds number for the liquid phase;
                                       a.v L
                                    :
                           Fr L = — — Froude number for the liquid phase;
                                   g

                           Ed=—*z— -EStvos number;
                               a a
                                                        3
                           p L - liquid phase density in kg/m ;
                                                                2
                           v h - liquid phase kinematic viscosity in m /s;
                                  In equation (262) the viscosities of both phases are omitted because at
                           developed turbulence the effect of the viscous forces is negligible.
                                  In case of a fully wetted packing, like some packings with vertical
                           walls, Ed can also be omitted.

                           1.6.2. Liquid holdup

                                  As already mentioned the value of A is closely connected with the
                           liquid holdup. The last can also be divided, some formally, into two parts;


                           H d=H d0+AH d,                                                  (263)



                           where Hat is the holdup under the loading point and AH d - its increase over this
                           point because of the forces between the gas and the liquid phase. The equations
                           for these two parts are similar to the equations for A and Ad, namely:


                           H d0 = f(Re L,Fr L.E6,e,l r.JJ,                                 (264)



                                 — f(     1     ~,——iEd,e,l,....L).                        (265)





                           1.6,3. Effective staface area

                                  The effective surface area a e is the surface of the interface between the
                                                          3
                           gas and the liquid phases per 1 m  of the packing volume. It is a sum of the
                           effective wetted surface of the packing and the surface of the jets and drops
   75   76   77   78   79   80   81   82   83   84   85