Page 8 - AN INTRODUCTION TO SURFACE CHEMISTRY By ERIC KEIGHTLEY RIDEAL
P. 8

EXISTENCE  OF SURFACE  PHASES             3

       Surface  tension  is  thus exactly  analogous  to  pressure  in  three
     dimensions except  that the sign is reversed.  By taking into considera-
     tion the thickness of the surface film we can imagine surface tension
     as a  negative pressure, averaged over the thickness of the film but it
     is seldom convenient to  do so,  partly because the  thickness of the
     film  is not  usually  known  with  certainty,  and  partly because  the
     calculated  mean  pressure  has  no  very clear  physical  significance.
     We  may  however,  if  we  choose, regard  the  surface  tension  as  an
     integrated   value  of the  tangential  pressure  over  the  thickness of
     the film.
       There  is another point of view .from  which  it is often  useful to
     regard  surface  phenomena.  If the surface of a soap-film  in a wire
     frame is  increased by moving outwards against the tension one side
     of the frame,  a quantity  of work must be done against the surface
     tension  equal  to the  product  of the surface tension and the increase
     of area.  A definite  quantity  of potential  energy is thus bound up
     with  each  unit of  surface,  The  numerical  value  of  the  surface
     energy  defined  as  energy  per  unit surface  is  clearly  the  same  as
     that  of  the  surface  tension.  The  dimensions  in  each  case  are
     l,"}    see  he  potential  energy  of  the or»tom  tends  to


     minimum,  the  surface  must contract  to a  minimum  area:  we  are
     thus led to the same result as before,
       It is  important to observe that the surface energy a is a quantity
     of the kind called "free energy" by Gibbs, and  Helmholtz.  It does
     not  represent  the  whole  of  the  energy  expended  when  a  fresh
     surface is formed.  If the extension of surface  takes place adiabati-
     cally, a quantity of heat - T � ;,  is absorbed from the interior, which

     is  thereby  somewhat cooled.  Allowing  for  the additional  energy,
     which may be called the latent heat of surface formation, introduced
     to compensate for this  cooling  effect, the  total  energy per  unit of

     fresh  surface is u -T  :;,:   this quantity is known at the Total Sur-
                                                                          \
     face Energy:  (w),  We are  as  a rule more  concerned with  the free
     surface energy,  and the  latter  quantity will be understood when for
     shortness the term  surface energy  is  used.
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