Page 40 - Distillation theory
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            0521820928c01  CB644-Petlyuk-v1                                                      June 11, 2004  17:45





                        14     Phase Equilibrium and Its Geometric Presentation

                                   K
                               a)
                                      K 2
                                         K 3
                                   1
                                           K 1
                                                    x 2
                                    0              1
                                   K
                               b)     K 2               Figure 1.11. Dependences K − x on the sides of the concen-
                                                        tration triangle for mixture in Fig. 1.9a: (a) side 1–2, (b) side
                                   1                    2–3, (c) side 1–3. Thick lines, K − x for present on side com-
                                             α
                                        K 3
                                              13        ponents; dotted lines, K − x for absent on side components
                                      K 1
                                                    x 2  (K ∞  − x).
                                    0              1
                                   K
                               c)
                                      K 2
                                       K 3     K 1
                                   1
                                       K 1 13  K 3
                                                    x 1
                                    0              1


                               Indeed, if α ij = K i /K j = 1, then y i /y j = x i /x j (i.e., points [x i , x j ] and [y i , y j ] lie
                               on the straight line that passes through vertex k [k  = i, k  = j]). For example,
                               in the points of α 13 -line in Fig. 1.9a, the liquid–vapor tie-lines are directed to
                               vertex 2.
                                 In the concentration tetrahedron, all points of α-surfaces are characterized by
                               the property that the liquid–vapor tie-lines in these points are directed along the
                               straight lines passing through that edge of the concentration tetrahedron, which
                               connects the vertexes whose numbers are missing in the index of α-surface. For
                               example, in the points of α 13 -surface in Fig. 1.9b, the liquid–vapor tie-lines are
                               directed to edge 2–4.
                                 In the concentration tetrahedron, the ternary azeotrope gives rise not only to
                               three α-surfaces, but also to one specific α-line in the points of which not two but
                               three components of the phase equilibrium coefficients are equal to each other.
                               We will call the line a three-index α-line. For example, in Fig. 1.10b, the ternary
                               azeotrope 123 gives rise to the α 123 -line, which crosses the face 1–3–4 in the α 123 -
                               point (it isn’t shown).
                                 It is characteristic of all points of the three-index α-line that the liquid–vapor
                               tie-lines in these points are directed along the straight lines passing through that
                               vertex of the concentration tetrahedron, the number of which is missing in the
                               index of α-line.
                                 For example, in Fig. 1.10a in the points of the α 123 -line, the liquid–vapor tie-lines
                               are directed to vertex 4. Let’s note that the α 123 -line is a line of intersection of all
                               three α-surfaces (α 12 , α 13 , and α 23 ).
                                 The quaternary azeotrope gives rise to six α-surfaces in the concentration tetra-
                               hedron (the number of combinations is every two from four). Each α-surface gives
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