Page 139 - Distillation theory
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P1: JPJ/FFX  P2: FCH/FFX  QC: FCH/FFX  T1: FCH
            0521820928c05  CB644-Petlyuk-v1                                                      June 11, 2004  20:15





                                5.2 Calculation of Distillation at Minimum Reflux for Ideal Mixtures  113

                                of constant concentration to the output of top product, taking into consideration
                                the conditions of phase equilibrium between the incoming vapor flow and the
                                outgoing liquid flow in this zone:
                                    V r y i = α i d i /(α i − L/VK n )

                                  Designating ϕ = L/VK n and summing up by all the components, we obtain one
                                of the main equations of Underwood:

                                                       min
                                       α i d i /(α i − ϕ) = V r                                  (5.1)
                                     i
                                  The analogous equation for the bottom section is as follows:

                                                         min
                                       α i b i /(α i − ψ) =−V                                    (5.2)
                                                         s
                                     i
                                  The main achievement of Underwood consists in the proof of equality of pa-
                                rameters φ and ψ in Eqs. (5.1) and (5.2) in the mode of minimum reflux. Sum up
                                these equations is following main equation:

                                       α i f i /(α i − θ) = (1 − q)F                             (5.3)
                                     i
                                where q is a portion of liquid in the feed and θ is a common parameter (root) of
                                Eqs. (5.1) and (5.2).
                                  For the set composition of the top product and for the set reflux number, the
                                number of roots of Eq. (5.1) equals that of the components in top product (k):

                                    0 <ϕ 1 <α k <ϕ 2 <α k−1 < ··· <α 2 <ϕ k <α 1
                                  Similarly, the number of roots of Eq. (5.2) equals that of components in the
                                bottom product (m):

                                    α m <ψ 1 <α m−1 < ··· <α 2 <ψ m−1 <α 1 <ψ m
                                  Correspondingly, the number of roots of Eq. (5.3) is less by one than that of
                                the components, present in the top and in the bottom products (i.e., the number
                                of distributed components).
                                  The Underwood equation system determines separation product compositions
                                and internal liquid and vapor flows in the sections for the set values of two param-
                                eters, characterizing the separation process. The reflux number R and withdrawal
                                of one of the products D/F or recoveries of some two components into the top
                                product ξ i = d i /f i and ξ j = d j /f j , etc., can be chosen as such two parameters. For
                                example, at direct split of three-component ideal mixture 1(2) : (1)2,3 (here the
                                top product contains component 1 and small admixture of component 2 and the
                                bottom product contain components 2,3 and small admixture of component 1),
                                Eq. (5.3) has only one common for both section root α 2 <θ <α 1 .If ξ 1 and ξ 2
                                are set, then d 1 and d 2 can be defined and V min  can be obtained from Eq. (5.1).
                                                                      r
                                The rest of internal flows in the column section can be defined with the help of
                                the material balance equations.
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