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PHASE EQUILIBRIA INVOLVING TWO-COMPONENT SYSTEMS: PARTITION     205

     5.4     Phase equilibria involving two-component
             systems: partition


              Why does a fizzy drink lose its fizz and go flat?

             Equilibrium constants of partition

             Drinks such as lemonade, orangeade or coke contain dissolved CO 2 gas. As soon as
             the drink enters the warm interior of the mouth, CO 2 comes out of solution, imparting
             a sensation we say is ‘fizzy’.
               The CO 2 is pumped into the drink at the relatively high pressure of about 3 bar.
             After sealing the bottle, equilibrium soon forms between the gaseous CO 2 in the space
             above the drink and the CO 2 dissolved in the liquid drink (Figure 5.14). We say the
             CO 2 is partitioned between the gas and liquid phases.
               The proportions of CO 2 in the space above the liquid and in the liquid are fixed
             according to an equilibrium constant, which we call the partition constant:
                                            amount of CO 2 in phase 1
                                 K (partition) =                                   (5.8)
                                            amount of CO 2 in phase 2

             We need to note how the identities of phases 1 and 2 must be
                                                                          This equilibrium con-
             defined before K can be cited. We need to be aware that K (partition)
             is only ever useful if the identities of phases 1 and 2 are defined.  stant is often incor-
               On opening the drink bottle we hear a hissing sound, which  rectly called a ‘partition
                                                                          function’ – which is in
             occurs because the pressure of the escaping CO 2 gas above the
                                                                          fact a term from statis-
             liquid is greater than the atmospheric pressure. We saw in Chapter 4
                                                                          tical mechanics.
             that the molar change in Gibbs function for movement of a gas is
             given by

                                                     p (final)
                                        G = RT ln                                  (5.9)
                                                     p (initial)





                                                     Carbon dioxide
                                                     in the gas phase


                                                    Carbon dioxide
                                                    dissolved in solution






             Figure 5.14 In a bottle of fizzy drink, carbon dioxide is partitioned between the gas and the
             solution phases
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