Page 73 - Gas Adsorption Equilibria
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1. Basic Concepts                                                 59


          Likewise we have from Eqs. (1.31) combined with (1.27)






          From equations (1.34), (1.35) the total mass adsorbed   can be calculated
          from density  measurements and calculations of the  sorptive gas   and
          given  data of  the  corresponding  helium  experiments      and  after
          choosing or calculating the reference density  of the sorbate phase.


             It should  be  noted  that according to  Eq.  (1.30) at  low gas densities,
                    or, equivalently  low  gas  pressures,          the absolute
          mass adsorbed     and the Gibbs surface excess     are nearly equal





          However, for high  gas  densities           or,  equivalently, high  gas
          pressures both  quantities are  becoming  different.  Consequences of this  are
          demonstrated in Figure  1.22  below showing                of  nitrogen
          adsorbed on activated carbon Norit R1 Extra [1.50].

             Both  concepts of masses of  an  adsorbate discussed  so far  –  the Gibbs
          surface excess      based on proposition (P1) and calculated by Eq. (1.27)
          and the absolute mass adsorbed   based on proposition (P2) and calculated
          by either Eq. (1.34) or (1.35) – do have their physical limitations. Hence it is
          desirable to  mention other possibilities to  define and to measure masses of
          adsorbates in gas adsorption systems.

             A fairly simple possibility to do this is to realize that contrary to a PSSS,
          Fig.  1.20, the volume  of  an  irregular  porous  sorbent being impenetrable
          for molecules of a sorptive gas, generally will depend on the size of the gas
          molecules, cp. Figs.  1.1, 1.21. This is well known in the mathematical theory
          of fractal surfaces  [1.67] and  thermodynamic phases  of fractal  dimension
          [1.68].  Also the range  of surface forces      cp.  (1.14), of a  sorbent
                                   )
          material is limited in space  but also depend on the sorptive  gas molecules.
                                  *
          Hence one may consider the volume of the joint sorbent/sorbate phase  as

          * )
            The boundaries of the region (A) of surface forces of the sorbent can be defined as surface
            on which the potential energy of the surface forces is equal to the (average) energy of the
            thermal fluctuations of a sorptive gas molecule. Naturally these boundaries will depend on
            the type of sorptive gas considered and – predominantly – on its temperature.
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