Page 66 - Gas Adsorption Equilibria
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52                                                         Chapter 1

             Consequently, the temperature of the gas remained nearly constant and a
          monotonous increase of the mass  of   adsorbed  could be observed. More
          examples of gas adsorption processes are given in Chaps. 3, 4 and 6.


             In concluding this section  we  want to  emphasize  that  gas  adsorption
          experiments also  can  be  done at  elevated  temperatures.  Preferently  they
          should be  carried out gravimetrically using  a highly  sensitive microbalance.
          These  so-called  thermogravimetric measurements can  be used  to monitor
          surface and  structural changes of the sorbent material  caused by physical or
          chemical modifications [1.3].


          5.       MASS AND VOLUME OF ADSORBED PHASES


             The set of molecules of a fluid phase, i. e. a gas or a liquid, which is within
          the field of forces of the atoms or molecules of the external or internal surface
          of a solid sorbent is called the adsorbate of the fluid on this sorbent material.
          This set may be considered as a thermodynamic system or phase in the sense
          of W. Schottky [1.63].  Such a system is defined as set of bodies or molecules
          divided from its surroundings by clearly defined boundaries and exchanging
                                                                * )
          with its surroundings only mechanical work, heat and mass.  Obviously, any
          adsorbate is  an inhomogeneous phase as – by definition – its molecules are
          subject to the surface forces of the sorbent atoms.  Hence the conditions for
          local                thermodynamic  equilibrium conditions, derived  from
          the Second Law of thermodynamics, are [1.64]













          Here p,   T,  indicate the pressure, mass density, temperature and chemical
          potential of the  adsorbate at location           is the temperature of
          the sorptive fluid. The quantity     is  the  potential energy per unit mass
          at location (x) of the  surface  forces of the  sorbent atoms.  As  this quantity
          normally is  an unknown  function of space  coordinates (x),  so are  the local
          thermodynamic quantities (p,  T,  For given model function of the surface


          *) This definition may  be  extended to  include  also electric loads,  electromagnetic work,
            radiation energy and information [1.64, 1.65].
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