Page 258 - Introduction to Colloid and Surface Chemistry
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Rheology  247
         might  block  the  capillary, must be  removed  from  the  liquid prior  to
         its  introduction  into  the  viscometer.  A  viscometer  is selected  which
        gives  a  flow  time  in  excess  of  c.  100 s;  otherwise  a  kinetic energy
        correction  is  necessary.
          The capillary method  is simple to operate  and precise (c. 0.01-0.1
        per cent) in its results, but suffers  from  the disadvantage that the rate
        of shear  varies from  zero at  the centre  of the capillary to a maximum
         (which  decreases  throughout  the  determination)  at  the  wall.  Thus,
        with  asymmetric particles  a  viscosity  determination  in  an  Ostwald
        viscometer  could  cover  various  states  of orientation  and  the  measured
         viscosity,  although  reproducible,  would  have  little  theoretical  sig-
         nificance.

         Rotational methods

        Concentric  cylinder and  cone  and  plate  instruments are  particularly
        useful  for  studying the flow behaviour  of non-Newtonian liquids.
          In the first of these techniques an approximation  to uniform rate of
        shear throughout  the sample  is achieved by shearing a thin film of the
        liquid  between  concentric  cylinders.  The  outer  cylinder  can  be
        rotated  (or  oscillated)  at  a  constant  rate  and  the  shear  stress
        measured  in  terms  of  the  deflection  of  the  inner cylinder,  which  is
        suspended  by a torsion wire (Figure 9.2); or the inner cylinder can be
        rotated  (or  oscillated)  with  the  outer  cylinder  stationary  and  the
        resistance  offered  to  the  motor  measured.
          If  (a is the  angular velocity  of the  outer  cylinder and  6 the angular
        deflection  of  the  inner  cylinder,  the  coefficient  of  viscosity  of  the
        liquid  is given by

             „-*?                                               (9.4)
                 at
        where k is an apparatus constant (usually obtained  by calibration with
        a liquid of known viscosity). The  necessity for  an end-correction  can
        be  avoided  if  the  inner  cylinder  is appropriately  cone-shaped  at  its
        end,  or  if air  is entrapped  in a  hollowed-out  inner cylinder base.
          Cone  and  plate  instruments  (see  Figure  9.3)  permit  the  velocity
        gradient  to  be  kept  constant  throughout  the  sample,  and  are
        particularly  useful  for  studying  highly  viscous  materials.  A  very
        versatile  cone  and plate rheometer, known as a rheogoniometer, has
        been  developed  by  Weissenberg,  which  enables  both  tangential
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