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P1: FCH/FFX  P2: FCH/FFX  QC: FCH/FFX  T1: FCH
            0521820928c06  CB644-Petlyuk-v1                                                      June 11, 2004  20:17





                                6.7 Distillation Complexes with Thermal Coupling Flows            195

                                equilibrium coefficients of components 1 ÷ 3 on the concentration of component 1
                                is shown in Fig. 6.11a, dependence of the concentration of component 1 in pseudo-
                                product point x on its concentration in reversible distillation trajectory tear-off

                                             D
                                point x t  , according to Eq. (6.13), is shown in Fig. 6.11b and the dependence of
                                      rev,e
                                the relative rate of the entrainer E/D on this concentration x t  , according to Eq.
                                                                                   rev,e
                                (6.16), is shown in Fig. 6.11c.
                                  It is seen from Fig. 6.11a that K 3 = 1 in points x 1 = 0.35 and x 1 = 0.85 and that
                                K 3 = K 1 in point x 1 = 0.9. In accordance with this (see Eq. 6.13) in point x t  =
                                                                                                rev,1
                                0.35 x    =±∞, in point x t  = 0.85 x     =+∞, and in point x t  = 0.9 x    = 0
                                     D,i              rev,1     D,i                  rev,1     D,i
                                (Fig. 6.11b). Along with that, in the segment [0; 0.35] x     < 0 (i.e., point x lies

                                                                               D,i              D
                                on the continuation of side 1-2 behind vertex 2) in the segment [0.35; 0.85] x    D,i  >
                                1 (i.e., point x lies on the continuation of side 1-2 behind vertex 1) and in the

                                            D
                                segment [0.9; 1.0] 0 < x D,i  < 1 (i.e., point x lies on side 1-2) (Fig. 6.8).


                                                                    D
                                  According to Fig. 6.11c, the parameter E/D →∞ at x t  → 0 and (E/D) min =
                                                                                rev,1
                                0.5 at x t  = 0.75.
                                      rev,1
                                  As it becomes evident from this example, to determine (E/D) min at m m = 2
                                it is sufficient to scan the values of phase equilibrium coefficients of the com-
                                                                                          t
                                ponents in the intermediate section trajectory tear-off segment Reg and to use
                                                                                          e
                                Eq. (6.16).
                                  Inamoregeneralcaseatm m >2insteadofthetrajectorytear-offsegment,there
                                is a tear-off region, in points of which it is necessary to determine the phase equi-
                                librium coefficients and then to determine the values of the parameter (E/D) min .
                                For example, for the split at Fig. 6.9c the parameter (E/D) min depends on composi-
                                tion of entrainer (i.e., on location of point x E at side 3-4). Therefore, to determine
                                (E/D) min it necessary to scan the phase equilibrium coefficients of the components
                                in all the points of face 1-3-4. As a result, the value (E/D) min and the optimal
                                composition of the entrainer x E (i.e., optimal correlation in it of concentrations of
                                components 3 and 4) will be found.
                                  For the split in Fig. 6.9b, the composition of the top product x D , as a rule, is
                                fixed because it is conditioned by the correlation of components 1 and 2 in the
                                mixture under separation. Therefore, to determine (E/D) min it is sufficient to scan
                                                                                             t
                                the phase equilibrium coefficients of the components in tear-off points x rev  for the
                                pseudoproduct points x on continuation of line x D − x E .

                                                    D


                        6.7.    Distillation Complexes with Thermal Coupling Flows

                        6.7.1. Kinds of Distillation Complexes with Thermal Coupling Flows
                                Three kinds of distillation complexes with thermal coupling flows (with branching
                                of liquid and/or vapor flows) – columns with side stripping, columns with side
                                rectifiers and complexes with full thermal coupling flows, called Petlyuk column –
                                are used in industry at present.
                                  For three-component mixtures, these kinds of complexes can be easily obtained
                                from three splits of three-component mixture in the first in motion column of the
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