Page 164 - Distillation theory
P. 164

P1: JPJ/FFX  P2: FCH/FFX  QC: FCH/FFX  T1: FCH
            0521820928c05  CB644-Petlyuk-v1                                                      June 11, 2004  20:15





                        138    Distillation Trajectories and Conditions of Mixture Separability

                                                        2
                                     x D
                                                           (L/V) 3
                                                            (L/V)
                               x F
                                                               2
                                                              (L/V)
                                                                 1
                                     x B
                                                  qS
                                                       +
                                                     N
                                                      1
                                              x D
                                                              +
                                                             N
                                                              2
                                         1                             3
                                                                   +
                                                                  N 3
                               Figure 5.20. The trajectories of rectifying section for
                               quasisharp separation of the ideal mixture. (L/V) 3 =
                               1, (L/V) 3 > (L/V) 2 > (L/V) 1 , the region between the
                               reversible-distillation trajectory and the distillation tra-
                               jectory under infinite reflux is shaded. qS, quasistationary
                               point.


                               small. In point qS, trajectory of quasisharp distillation changes its direction: be-
                               tween points x D and qS it is almost parallel to the side of concentration triangle
                                                                       (3)     (3)    +(3)
                                                        +
                               and between points qS and N it goes inside (x  → qS r  → N r  ).
                                                                       D
                                 Let’s note, that distillation trajectory of three-component mixture for the set
                               product point is located between trajectory at infinite reflux (i.e., at L/V = 1, and
                               reversible distillation trajectory) (Kiva, 1976; Petlyuk & Serafimov, 1983; Wahn-
                               schafft et al., 1992; Castillo, Thong, & Towler, 1998).
                                 The structure of the trajectory bundle has interesting peculiarities for qua-
                               sisharp distillation at non-monotonous change of the parameter L/V along re-
                               versible distillation trajectory (i.e., at “tangential pinch”). Figure 5.19 shows for
                               the mixture acetone(1)-benzene(2)-chloroform(3) dependence of the parameter
                               (L/V) rev on concentration of component 2 along the trajectory of reversible qua-
                               sisharp distillation (composition in the point x D : 0,699; 0,001; 0,300). This depen-
                               dence has two extremums – minimum and maximum. The point of maximum
                               (L/V = 0,758) corresponds to stationary saddle-node point SN inside concentra-
                               tion triangle (Fig. 5.18b). This stationary saddle-node point SN is a node point for
                               the trajectories, located closer than this point to the side of triangle, and a saddle
                               point for the rest of trajectories. The saddle-node point exists for the set product
                               composition x D at the unique value of the parameter L/V: (L/V) pinch  = 0,758. At
                               the smaller value, there is no trajectory tear-off from the side and at the bigger
                               value trajectory bundle has only node point N . The section’s trajectory can be
                                                                       +
                                                   (3)     (3)    +(3)
                               put in brief as follows: x  → SN r  → N r  .
                                                   D
                                 The structure of trajectory bundle also has interesting peculiarities at the best
                               nonsharp separation. In this case, trajectory bundle also has saddle-node and
                               node points (Shafir et al., 1984). Figure 5.21a shows for the azeotropic mixture
                               acetone(1)-benzene(2)-chloroform(3) the line of best bottom product (Poellmann
                                                                                 1
                               & Blass, 1994), connecting the end of possible segment Reg at side 2-3 at sharp
                                                                                  B
                                                                                2,3
   159   160   161   162   163   164   165   166   167   168   169