Page 159 - Gas Adsorption Equilibria
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3. Gravimetry                                                    145































          Figure 3.14. Adsorption  isotherms of oxygen   on zeolite Köstrolith SX6 without and with
                    pre-sorbed water of (0.89, 1.86, 3.79) mmol  at 313.35K.

          The Gibbs  excess  amounts  of   and   adsorbed  on the  zeolite SX6  have
          been calculated  from the microbalance recordings  following eq.  (3.34). For
          data referring to the dry zeolite, the helium volume
          measured  in  the  dry zeolite has been used.  For  data  referring to the  “wet
          zeolite” including presorbed water, the helium volume corrected by the bulk
          volume  of the adsorbed water, i. e.                    has been  used,
                being the density of liquid water at T = 313.15K and p =  1.013 bar. As
          can be seen from the figures, the adsorption capacity of the zeolite due to the
          presorbed water is reduced much more for nitrogen than for oxygen. Hence it
          can be  argued that the  selectivity  of the zeolite for  air  separation  processes
          based on quadrupole  induced adsorption of   will be considerably reduced
          due to  the  presence of water.  Indeed this has been experienced  for various
          types of zeolites [3.37].  Actually, not only equilibria  of   on SX6 are
          changed by presorbed  water but  also the kinetics of the  adsorption process.
          This can be seen from Figure 3.15  showing uptake curves of nitrogen on dry
          and wet  SX6  taken at 313.6 K.  The  adsorption process  was  initiated by
          increasing the  gas  pressure of   (5.0)  from 0.5  MPa to  0.7  MPa.
          Corresponding desorption  curves  were  identical within experimental
          uncertainties, i. e. no hysteresis was found for this system and experiment.
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