Page 138 - Distillation theory
P. 138

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





                        112    Distillation Trajectories and Conditions of Mixture Separability

                                          y f
                               a)     x F






                                                       Figure 5.1. (a) Stripping section. (b) Stripping trajectory (liq-
                                                x B
                                                       uid compostion profile) for a ideal mixture; dashes, tray com-
                                                       positions.
                                            2
                               b)




                                                  x B
                                        y f  x F
                                   1                3

                               located at the boundary elements of concentration simplex and partially located
                               inside it, where they are joined with each other. Another common regularity is
                               availability of constant concentration zones, to which stationary points at each
                               section trajectory correspond. It is expedient to begin the analysis of distillation
                               regularities at minimum reflux with the ideal mixtures, for which the whole con-
                                                                            1,2...n
                               centration simplex is one component-order region Reg  (K 1 > K 2 > ··· > K n ).
                                                                              ord
                               In a more particular case, we understand as the ideal mixtures those for which,
                               besides that, relative volatilities of the components in all points of concentration
                               simplex are the same (i.e., α i = K i /K h = const), and latent heats of evaporation
                               of the components are the same (i.e., at distillations, molar vapor and liquid flow
                               rates do not change along the section height V r = const, V s = const, L r = const,
                               L s = const).
                                 Availability of these conditions allowed Underwood (1948) to obtain general
                               solution, connecting separation product compositions at minimum reflux with
                               the mode parameters (e.g., with V r and V s ). Even before (Hausen, 1934, 1935),
                               distillation trajectories of the ideal mixtures in the one-section columns (Fig. 5.1a)
                               were investigated by means of calculation, and it was shown that the part of
                               distillation trajectory located inside the concentration triangle is rectilinear for
                               the ideal mixture (Fig. 5.1b). Later, linearity of distillation trajectories of three-
                               component ideal mixtures at sharp separation was rigorously proved (Levy et al.,
                               1985).


                        5.2.1. Underwood System of Equations

                               The Underwood system of equations can be obtained from the conditions of
                               componentwise material balance and of phase equilibrium in the cross-section of
                               constant concentration zones of each section. For example, the following expres-
                               sion can be obtained from the equation of componentwise material balance at
                               the contour, embracing the part of top section from the cross-section in the zone
   133   134   135   136   137   138   139   140   141   142   143