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92  CHAPTER 2

           2.12.2.  How Does One Measure the Dielectric Constant of Ionic
                   Solutions?
               There is much to think about here. If one wishes to measure the dielectric constant
           of a liquid, not a conducting ionic solution, one simply uses an alternating current (ac)
           bridge containing a capacitor in one of the arms. Then the capacitance is measured in
           the presence of the liquid, the dielectric constant of which is to be measured, and then
           without it, i.e., in the presence of air. Since the dielectric constant is near to unity in
           the latter case, this gives rise to knowledge of the dielectric constant of the liquid
           because the capacitance of the cell in the bridge arm increases as the dielectric constant
           increases.
               However, when the liquid is a conducting solution, this approach breaks down.
           The conductance of the  solution  contributes to the impedance of the  cell,  which
           (depending on frequency) may no longer be overwhelmingly capacitative. Hence, the
           dielectric constant of a conducting liquid cannot be simply measured, because of the
           conductive components of the impedance.
               Two approaches can be used to avoid this difficulty. In the one, which is best used
           for frequencies well below the relaxation frequency of water, one measures the  force
           between two plates  that have  the conducting  liquid between  them. This  force is
           independent of the conductance of the liquid or the direction of the field.  If d is the
           distance between the plates, it is easy to show that the force is






           where E is the potential difference between the plates, A is their area, and  is the
           dielectric  constant (Fig.  2.26). To  obtain measurements  that  avoid  significantly
           changing the temperature of the solution, d should be minimal. The field between the
           two plates is small        Vibrations must also be minimized (e.g., by placing
           the apparatus on a stone slab supported on an inflated inner tube). An optical lever
                                                  25
           magnifies the very small movement of the plates.  Because everything is known in
           Eq. (2.28) except , the latter can be measured.
               If it is desired to measure the dielectric constant at high frequencies
           Hz), a different technique is necessary, partly because one may be working in the range
           of the relaxation time of water. The measurement of this, and the degree to which it is
           affected by  the  presence of ions, provides yet another way  of finding how  many
           molecules of water are bound to cation and to anion. The technique involves the use
           of a wave guide consisting of a coaxial liquid-filled cell, containing a probe that is
           moved about until the interference signal between it and an alternator is found to be


           25
             A movement of  0.1 mm in the plate can be magnified mote than 100 times by projecting a beam of light
            reflected from a mirror attached to the plate over a distance of 25 m.
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