Page 126 - Distillation theory
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P1: FCH/FFX  P2: FCH/FFX  QC: FCH/FFX  T1: FCH
            0521832772c04  CB644-Petlyuk-v1                                                      June 11, 2004  17:49





                        100    Trajectories of Thermodynamically Reversible Distillation







                                                       Figure 4.20. Reversible section trajectories for acetone(1)-
                                                       water(2)-methanol(3) extractive distillation. Short segments
                                                       with arrows, liquid–vapor tie-lines in arbitrary cross-sections
                                                       of stripping and intermediate sections; little circles, composi-
                                                       tion in main and entrainer feed cross-section.







                               agent is water, and the top product is acetone, are shown in Fig. 4.20 and may be
                               briefly described as follows:
                                      (1)    (2)      t(2)      (3)        (3)      t(2)      (2)
                                     x    ← x   ⇓⇒ x rev,e ← x       ⇓⇒   x    ← x rev,s ← x
                                    (  D     e−1       t        f −1        f         t       B  ).
                                    Reg D           Reg rev,e  Reg rev,e  Reg rev,s  Reg rev,s  Reg B
                                 Trajectories are constructed for a fixed value of the parameter E/F. Let’s note
                               that, unless all sections of the column work reversibly, as a whole the process is
                               irreversible because irreversibility arises in the points where the entrainer and the
                               main feeding enter.
                                 As we see, in contrast to simple column, we succeeded in obtaining pure ace-
                               tone and binary zeotropic mixture methanol-water, which can be separated in the
                               second column.
                                 Let’s examine now the structure of trajectory bundles of sharp reversible distil-
                               lation for the intermediate (extractive) section of the column with two feedings at
                               separation of different types of azeotropic mixtures, the way we did it for the top
                               and the bottom sections (Fig. 4.21). While composing these diagrams, we used,
                               just as we did before, the data on the phase equilibrium coefficients of present
                               and absent components at the sides of the concentration triangle and the general
                               regularities of the location of the trajectory bundles of sharp reversible distillation.
                                 It is obvious that for the separation of three-component mixtures by means of
                               extractive distillation, the mixtures of the type 4a (according to the classification
                               given by Gurikov) that are widespread in practice are of the biggest interest. For
                               these mixtures, according to Fig. 4.21, one can get pure component 1 as top product
                               and zeotropic mixture 2,3 as bottom product. One can get the same result for the
                               mixtures of type 4b.


                        4.7.   Trajectory Bundles of Extractive Reversible Distillation for
                               Multicomponent Mixtures
                               Figures 4.22a, b show two different flowsheets of autoextractive distillation of
                               a four-component ideal mixture (K 1 > K 2 > K 3 > K 4 ). Both flowsheets ensure
                               sharp separation in intermediate extractive section, because for any inner point of
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