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Solubility: absorption and stripping
               Solubility data of a gaseous component in the liquid phase needs to be known for absorber and stripper
               design. Equilibrium solubility of components of a gas mixture over a liquid is often expressed in terms
               of partial pressure of the component (Table 9.3). An ideal dilute solution is described by Henry’s law:
               p i ¼ H i   x i , for components in minute quantities (x i /0). H i , the Henry’s law constant for
               component i depends on temperature but is relatively independent of system pressure at moderate
               pressure levels. x i   0:1 is considered as the upper limit for applicability of Henry’s law within en-
               gineering accuracy.
                  The solubility of gas decreases with increasing temperature, and hence, the equilibrium (solubility)
               curves are steeper at higher temperatures, as is evident from Fig. 9.1F. Gas solubility increases with
               pressure, and it is possible to produce any gas concentration in the liquid by applying sufficient
               pressure as long as the liquefied form of the gas is completely soluble in the liquid. Solubility of a gas
               is affected by presence of other gases in the system and also by the presence of nonvolatile solute.
                  The aforementioned relationships are applicable to nonreactive systems only and cannot be used
               for systems where the absorbed gas reacts with the solvent.
                  Considering the advantages of linear interpolation/extrapolation, experimental solubility data
                                         are often presented as a reference substance plot. These are plotted
                                         with the pure solvent boiling point along the x-axis and the partial
                                         pressure of the solute gas along the y-axis; each line on the graph
                    Linear equilibrium plots
                                         corresponds to a specific solute concentration. At times, the vapor
                                         pressure of pure liquid is also marked in lieu of its boiling point.
               This representation connects x i , T,and p i . Fig. 9.2 shows the reference substance plot for the
               ammoniaewater system.
                                  100
                                  80
                                  60


                                  40
                                Partial pressure ammonia, mmHg  20 8  H O in liquid = 1.0  0.75  0.60

                                            Mole fraction
                                           2

                                                0.90

                                  10





                                   4 6




                                   2
                                    4     6   8 10       20        40   60     100
                                                              O, mmHg
                                                Vapor pressure H 2
               FIGURE 9.2
                                     Reference substance plot for NH 3 eH 2 O system.
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