Page 283 - Introduction to Colloid and Surface Chemistry
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272  Emulsions  and  foams


        Foam  drainage

        Initially,  the  liquid  films  of  a  foam  will  be  relatively  thick  and
        drainage will take  place  mainly by gravitational flow throughout  the
        whole of these films. The foaming agent plays an important role even
        at this stage in restricting  this flow to a level where local  disturbances
        and  consequent  film  rupture  is  minimised.  When  the  films  have
        attained  a  thickness of  the  order  of micrometres,  gravitational flow
        down  the  laminar regions  will become  extremely slow. The  predom-
        inant  drainage  mechanism  will  then  involve liquid being  discharged
        locally  at positions  of inter-film  contact (known as Plateau  borders),
        where the  liquid capacity is relatively high. Subsequent  drainage then
        takes  place  through  the  network  of  Plateau  borders  that  exists
        throughout  the  foam.












        Figure  10.2  Plateau  border at  a  line  of intersection  of three  bubbles.  Owing  to  the
        curvature of the liquid-gas interface  at  A,  the  pressure of liquid at  A is lower than at
        B,  thus causing capillary flow of  liquid  towards  A

          The  discharge  of  liquid  from  the  laminar  part  of  a  thin  film  is
        governed  by the  pressure  of the  liquid in this region  compared  with
        that  of  the  liquid in  the  Plateau  borders.  At  least  three  factors  are
        likely  to  be  involved,  van  der  Waals  attractive  forces  favour film
        thinning,  and  the  overlapping  of  similarly  charged  electric  double
        layers  opposes film thinning (see  Chapter  8).  The  other  important
        factor  is a capillary pressure,  which favours film thinning. This arises
        because  the  pressure  of  the  adjacent  gas  phase  is  uniform  and,
        therefore,  the  pressure  of  liquid  in  the  Plateau  borders,  where  the
        interface  is  curved,  is  less  than  that  of  liquid  in  the  laminar film.
        Depending  on  the  balance  of  these  forces,  a  film  may  either  thin
        continuously  and  eventually  rupture,  or  attain  an  equilibrium
        thickness. Any propagated  structure within the film may significantly
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