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4. Volumetric – Gravimetric Measurements                         185

          likewise  step  down) procedure more  often  than 3 – 4  times, cp.  remarks  in
          Chaps. 2 and 3.

             The instrument Figs. 4.1, 4.2 is subject to several severe restrictions which
          we would like to discuss in brief. First, all two beam balances commercially
          available today [2.3, 4.5], are designed such that the sorptive gas contacts the
          inner region  of the balance including parts  like electromagnetic  coils which
          are highly sensitive to corrosion. Hence these balances  only can be used for
          non-corrosive sorptive  gas mixtures including  components like  (He,  Ar,
               (CO)). Of course a permanent flow of inert gas could be used to cover
          and thus  to protect the microbalance  region. But  this  technique,  though in
          former  days  having  often  been used in  traditional  thermogravimetric
          experiments, has not proved to lead to reproducible and accurate results as it
          seems to  be  difficult to  attain stable equilibrium  conditions in systems
          including a permanent gas flow contacting a microbalance [2.3, 2.4, 4.5]. Also
          traditional  microbalances normally  can operate  in  fairly  narrow  ranges  of
          temperature and pressure – usually about ambient conditions – only. Hence it
          would  be desirable to  extend  these  ranges  of temperature and  pressure and
          also to  allow corrosive gases like                     An  instrument
          which can do  this  is provided  by the magnetic suspension  microbalance
                                          *)
          already mentioned in Chap. 3 (2.2).   We will give more details about this in
          Sect. 2.4 and Sect. 3 of this chapter.

          2.2      Theory


             The masses  of a two  component adsorbate        can  be determined
          from the  results of  a  volumetric-gravimetric experiment, namely  the  gas
          pressure (p) in  the  system, the  temperature (T),  and the  microbalance
          recording    as  follows: We first denote the mass balance equations for each
          component





          the thermal  equation of state  (EOS) of the sorptive gas mixture with masses
                i = l,2)






          * )  Manufacturer:  RUBOTHERM Praezisionsmesstechnik  GmbH, Universitätsstr.  142,
            D-44799 Bochum, Germany, www.rubotherm.de
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