Page 271 - Gas Adsorption Equilibria
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5. Oscillometry                                                  257


          since the  volume of  the material needed for  buoyancy or  dead space
          corrections respectively, depends not only on pressure and temperature of the
          sorptive gas but also on the amount of gas absorbed. Today there are several
          techniques described  in  literature for measuring  polymeric  swelling
          phenomena  [5.21-23],  usually  determining the change  in one  or two
          dimensions of a polymer sample. However, these methods require a specific
          shape or state of the polymeric material, i. e. a thin film or a liquid drop and,
          despite the geometry, often assume isotropic swelling of the polymer sample.

             By combining oscillometric and gravimetric measurements it is possible to
          simultaneously determine the mass  of  gas    absorbed in a  polymeric
          material of  mass     and  the  volume  (V)  of the  sample material  in the
          absorption state thus providing together with (p) and (T) the basic data for the
          thermal equation of state of the polymer loaded with gas  [5.8],  [5.26]. The
          polymer samples which can be investigated in this way can be either highly
          viscous liquids or dense solid materials formed as cylindrical rings, pulverous
          flakes or  pellets.  Isotropic swelling is  not mandatory for the  method to be
          applied.

             In this  section we  first will  describe the experimental  device,  Sect.  3.2,
          then  provide  formulas to  calculate  and  of  a  polymer sample  from
          measured data  Sect. 3.3,  and  finally present an example namely  sorption of
              in (swelling) polycarbonate (Makrolon 2400), Sect. 3.4.

          3.2      Experimental


             An  instrument for combined oscillometric-gravimetric  measurements  of
          sorption equilibria in  swelling (polymeric)  materials has  been designed and
          built at IFT during  1997-2000, [5.2,  5.7, 5.8]. It  mainly consists of  the
          rotational pendulum already  described in  Sect. 2.1  and  a  microbalance
          installation as presented in Chap.  3,  Sect.  2.1.1. A schematic diagram of the
          instrument is  given in Figure  5.9  followed by photos  of the  ring slit of the
          pendulum filled with polycarbonate pellets, Fig. 5.10 and a front view of the
          installation in  our laboratory  (PB-A  0126/1) in  1998,  Fig. 5.11.  Detailed
          information of  the  instrument  including specifications of  vessels,  tubes,
          valves, and materials are given in the literature [5.2, 5.7] and references cited,
          cp. [Tom94],  [Sch99a].
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