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            0521820928c05  CB644-Petlyuk-v1                                                      June 11, 2004  20:15





                                5.4 Evolution of Section Trajectory Bundles for Three-Component Mixture  127


                                               2                             2
                                       a)                             b)








                                    1                    3        1                     3
                                       +                                     +
                                      N                             S      N
                                     x D       2                   x D      S 3  2
                                       c)                             d)
                                x                             x F
                                F                                         S 2
                                                                                  ( V)L  = 1
                                                                                     3
                                           S
                                    x B                            x B
                                                                               (L  V)
                                                                       S 1
                                                                                  2
                                                                          (L  V)
                                    x D                            x          1
                                                                   D
                                     1            +       3       1          +      +   3
                                        −       N                     −      1 N   2 N  +
                                      N                             N                 N
                                                                                       3
                                Figure 5.11. The evolution of trajectory (arrow-ended line) bundles of the rec-
                                tifying section for an ideal mixture with K 1 > K 2 > K 3 (component 1 is the
                                                                1
                                                      1
                                                1
                                                                           1
                                product): (a) L/V< K , (b) K < L/V < K , (c) L/V > K (the attraction re-
                                                3
                                                                2
                                                                           2
                                                     3
                                     2,3
                                                                                   1
                                                                                     1
                                      R
                                gion Reg w,r  ≡ Reg 1 att  shaded), (d) (L/V) 3 = 1, (L/V) 2 > (L/V) 1 > K . K and
                                                                                     2
                                                                                  2
                                     1
                                 1
                                K are the phase equilibrium coefficients at vertex 1 for components 2 and 3,
                                 3
                                respectively.
                                  At further increase of the parameter L/V, the points S and N move away from
                                                                                     +
                                vertex 1 (Fig. 5.11d) and reach vertexes 2 and 3 correspondingly at L/V = 1 (i.e.,
                                in the mode of infinite reflux).
                                  Let’s note that vertexes 2 and 3 cannot be top product points no matter what the
                                value of parameter L/V because for these vertexes Eq. (5.15) is not valid (i.e., x D 
=
                                                                                           2,3
                                [0,1,0] and x D 
= [0,0,1]). Let’s also note that section working region Reg R  at n =
                                                                                             w,r
                                                                                            1
                                                                                     1
                                3 and k = 1 is two dimensional (i.e., at each value of L/V > K in concentration
                                                                                     2
                                                                          2,3
                                triangle there is an attraction region Reg 1 att  ≡ Reg R  of point x D [1,0,0]). This
                                                                            w,r
                                                                           1
                                region is called the attraction region because a calculated trajectory springing
                                from any point of this region toward the product point is “attracted” to the product
                                point.
                                                                     −
                                  The trajectories touch on the segment N – S in the point N . One of these is
                                                                                      −
                                the distillation working trajectory at minimum reflux. It goes through the saddle
                                point S (see later in this Chapter).
                                  Let’s examine some deviations from the described evolution appearing at sep-
                                aration of nonideal zeotropic and azeotropic mixtures. One of such deviations
                                can be caused by nonmonotonous dependence of the function K 2 (x 2 ) at side 1-
                                2 and inside concentration triangle (Fig. 5.12a,b). Such nonmonotony leads in
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