Page 59 - Gas Adsorption Equilibria
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1. Basic Concepts                                                  45


          use to  calculate the  pore  spectrum  of  the  sorbent  from a  measured gas
          adsorption isotherm.  Naturally,  they  often  will  lead to  different  results.
          Examples for  these  methods are  the  t-plot  method, the         the
          Horvath-Kavazoe procedure,  the density  functional  theory (DFT)  procedure
          and also its non-local generalization (NLDFT). All of these are presented and
          discussed in today’s  literature  [1.2, 1.42].  Actually, the  above mentioned
          difficulties with gas adsorption measurements are condensed in two important
          draft  documents of  the International Standardization  Organization  (ISO),
          Geneva [1.55,  1.56]  providing recommendations  for both the  experimental
          procedure of measuring gas adsorption isotherms and to calculate from these
          data the macro-,  meso-, and  micropore spectrum  of  the  solid  material
          considered, However, it  must  be  emphasized that these documents  today
          (2004) are still drafts and do not provide international standards. Even though,
          it can be expected that they sometime will be promoted, probably in an only
          slightly different  form.


             A characteristic parameter  of  a  porous  material  is its so-called  BET-
          surface. This  is the  surface of a monolayer  adsorbate of         at
          boiling temperature  of   at        namely 77.3 K [1.3]. It is determined
          by nitrogen  adsorption  experiments  at  this temperature  for pressures
                    The mass of the monolayer load    is determined by fitting data
              to the adsorption isotherm equation developed by Brunauer, Emmett and
          Teller in 1938, originally designed for multilayer adsorbates [1.1-1.3, 1.57].







          Here  (C,   )  are parameters  to be determined by a data  fitting procedure,
          preferably restricted  to  the region         A theoretical  analysis  of
          Eq. (1.9) is presented in brief in Sect. 3.4 of Chap. 7.

             Assuming a cross section of                per            [1.3], the
          BET-surface      of  the monolayer simply can be calculated as





                         being the molar  mass of nitrogen. An  example  for such
          measurements is given in Figure 1.12, [1.36]. It presents Gibbs excess masses
          of nitrogen  adsorbed  on  reference material  CRM  BAM-PM-104 at  77 K
                      determined by  the  volumetric/manometric method in  a  closed
          system and without carrier gas. Data show hysteresis between the adsorption-
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