Page 251 - Gas Adsorption Equilibria
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5. Oscillometry                                                  237


          2.       MEASUREMENT OF PURE GAS ADSORPTION
                   EQUILIBRIA (N=1) BY SLOW OSCILLATIONS OF
                   A ROTATIONAL PENDULUM



          2.1      Experimental


             Pure gas  adsorption  equilibria can  be  measured  by observing slow
          oscillations of  a  rotational  pendulum bearing the  sorbent  material. An
          instrument of this  type  has been designed  and built at the  author’s institute
                                    *)
          during (1995-1997), Fig. 5.1.  It basically consists of a disk bearing a ring slit
          filled with homogeneously distributed sorbent material (pellets, powder etc.),
          fixed to a torsional wire and stabilized by a stem bearing a small mirror to
          reflect a laser beam, Fig. 5.2. The pendulum is placed in a vessel (adsorption
          chamber) which can  be  filled  with  sorptive  gas. The  adsorption chamber
          should be placed within a  thermostat and  equipped with manometer(s) and
          thermometer(s).


             To observe the motion of the pendulum a laser beam is sent to the mirror,
          the  reflected  beam  crossing  during its  motion in  radial direction within a
          horizontal plane 2 diodes placed at known angles    Fig.  5.2. The diodes
          of a couple produce by photo effect electric signals of opposite signs, hence
          the time when the reflected beam is crossing the area between the two diodes
          can be detected very accurately, cp. signal sample given in Fig. 5.3. The series
          of time  signals  produced in  this way  by a  slow damped oscillation  of the
          pendulum in the  gas  provides the  basis to fit an  ideal damped  harmonic
          motion, Eq. (5.7) to it and to calculate the respective angular frequency and
          logarithmic decrement by a Gaussian minimization procedure. To start  the
          motion of the pendulum, the instrument is based on a ball bearing allowing to
          rotate it by an arbitrary angle, cp. Fig. 5.1. Choosing this at about 90 ° and
                                                       **)
          keeping the instrument in this position for a while , the pendulum inside the
          instrument starts to move due to the retarding moment of the torsional wire.
          Returning then the whole  instrument to  its  original  position will maintain
          motion of the pendulum, this procedure resulting now in an oscillation. This
          however will fade away slowly due to internal  friction of the wire and the
          flow of gas surrounding the pendulum.


          * )   The instrument meanwhile has been transferred to the Institute of Thermodynamics, Dept.
            Chem. Engineering, University of Dortmund, Dortmund (2003).
          ** )
             The time  interval to be chosen for this distorted position of the pendulum depends on  its
            design parameters, especially its mass and may vary from a few seconds up to a minute.
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