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Chapter 4. Binary Column Distillation: Internal Stage-by-Stage

                    Balances




                    4.1 Internal Balances

                    In Chapter 3 we introduced column distillation and developed the external balance equations. In this
                    chapter we start looking inside the column. For binary systems the number of stages required for the
                    separation can conveniently be obtained by use of stage-by-stage balances. We start at the top of the
                    column and write the balances and equilibrium relationship for the first stage, and then once we have
                    determined the unknown variables for the first stage we write balances for the second stage. Utilizing the
                    variables just calculated we can again calculate the unknowns. We can now proceed down the column in

                    this stage-by-stage fashion until we reach the bottom. We could also start at the bottom and proceed
                    upwards. This procedure assumes that each stage is an equilibrium stage, but this assumption may not be
                    true. Ways to handle nonequilibrium stages are discussed in Section 4.11.
                    In the enriching section of the column it is convenient to use a balance envelope that goes around the
                    desired stage and around the condenser. This is shown in Figure 4-1. For the first stage the balance

                    envelope is shown in Figure 4-1A. The overall mass balance is then



                                                                                                                        (4-1, stage 1)

                              Figure 4-1. Enriching section balance envelopes; (A) stage 1, (B) stage 2, (C) stage j








































                    The more volatile component mass balance is




                                                                                                                        (4-2, stage 1)
                    For a well-insulated, adiabatic column (Q       column  = 0), the energy balance is
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