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P1: JPJ/FFX  P2: FCH/FFX  QC: VINOD/IYP  T1: FCH
            0521820928c03  CB644-Petlyuk-v1                                                      June 11, 2004  20:12





                                3.2 Analogy Between Residue Curves and Distillation Trajectories   41

                                  Themodeofinfiniterefluxisinterestingforusnotonlyasoneoflimitdistillation
                                conditions, but also mainly as a mode to which splits achievable in real columns
                                at finite but quite big reflux correspond. These splits are ones of distillation for
                                border mode between the second and third classes of fractioning.
                                  The question of the reflux at which these splits are achievable in real columns
                                and of how, along with that, the distillation trajectory is located in the concentra-
                                tion space is discussed in Chapter 5. Here, we investigate only the splits themselves.
                                  Often the splits for zeotropic mixtures are ones of sharp separation without
                                distributed components. At practice, these splits are the most widespread because
                                they are the sequences with the smallest number of columns (n − 1 column for
                                n-component mixture, if each component is a purpose product) that correspond
                                to them.
                                  For azeotropic mixtures, not all the practically interesting splits are feasible at
                                the infinite reflux. However, the sequencing should have the infinite reflux mode as
                                its starting point because these splits are the easiest to realize at finite reflux. That
                                is why we start systematic examination of distillation trajectories with the infinite
                                reflux rate. It is also proved to be correct because the regularities of trajectories’
                                locations for this mode are the simplest.
                                  The analogy with the process of open evaporation favored the fact that this
                                mode was investigated earlier than the others. Systematic examination of distilla-
                                tion at the infinite reflux was initially carried out in works (Zharov & Serafimov,
                                1975; Balashov & Serafimov, 1984). The analysis of infinite reflux mode in the
                                infinite columns was made (Petlyuk, 1979; Petlyuk, Kievskii, & Serafimov, 1977;
                                Petlyuk & Serafimov, 1983) that allowed general regularities of separation to be
                                defined for the mixtures with any number of components and azeotropes. A num-
                                ber of important investigations was realized (Doherty, 1985; Doherty & Caldarola,
                                1985; Laroche et al., 1992; Bekiaris et al., 1993; Safrit & Westerberg, 1997; Rooks
                                et al., 1998) and others.

                        3.2.    Analogy Between Residue Curves and Distillation Trajectories
                                Under Infinite Reflux

                                Investigations of residue curves have been conducted for over 100 years, begin-
                                ning Ostwald (1900) and Schreinemakers (1901). Later, close correspondence
                                between residue curves (i.e., curves of mixture composition change in time at the
                                open evaporation) and distillation trajectories at infinite reflux (i.e., lines of mix-
                                ture composition change at the plates of the column from top to bottom) was
                                ascertained.
                                  The similarity and the difference of these lines are defined by their equations:

                                    dx i /dt = y i − x i = x i (K i − 1)                         (3.1)
                                (For residue curves, see Chapter 1.)
                                     (k+1)   (k)     (k)
                                    x     = y  = K i x                                           (3.2)
                                     i       i       i
                                [For distillation trajectories at the infinite reflux, see Chapter 2 Thormann (1928).]
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