Page 144 - Introduction to Colloid and Surface Chemistry
P. 144

134  The solid-gas  interface
        (Figure  5.6)  shows at  least  two distinct steps, each  corresponding  to
         the  formation  of an adsorbed  monomolecular layer. In most cases of
        multilayer physical gas adsorption, however, the adsorption  energies
        are  such  that  there  is  a  greater  or  lesser  tendency  for  .the  first
        monomolecular   adsorbed  layer  to  be  completed  prior  to  any
        adsorption  into  the  second  monolayer,  but  little  tendency  for  the
        second monolayer to be completed prior to adsorption into the third
        and  subsequent  monolayers.

        Surface  areas

        The  monolayer  capacity,  F m,  is a  parameter  of  particular  interest,
        since it can  be  used for calculating the  surface  area of an adsorbent if
        the  effective  area  occupied  by each adsorbate  molecule is known.
          If  the  BET  equation  is  applicable  to  a  multilayer  physical
        adsorption isotherm, a plot ofp/V(p Q-p)  versus p/p 0  gives a straight
        line of slope  (c— l)/V mc  and  an intercept of  l/V mc  on  the  p/V(pQ—p)
        axis - i.e.


             V
              m =        i                                     (5.13)
                  slope  +  intercept
        Using the  appropriate  gas equation,  the  monolayer  capacity  can  be
        calculated in terms of adsorbed molecules per unit mass of adsorbent.
          Although  the  BET  equation  is open  to  a  great  deal  of criticism,
        because  of  the  simplified  adsorption  model upon which it is based, it
        nevertheless fits many experimental multilayer adsorption  isotherms
                                                         a
        particularly  well  at  pressures  between  about  0.05  p 0 °d  0-35  p 0
        (within  which  range  the  monolayer  capacity  is  usually  reached).
        However,  with  porous  solids  (for  which  adsorption  hysteresis  is
        characteristic), or  when  point  B on  the  isotherm  (Figure  5.5)  is not
        very  well  defined,  the  validity  of  values of  V m  calculated  using  the
        BET  equation is  doubtful.
          With  a  small  loss  of  accuracy,  the  straight-line  BET  plot  (Figure
        5.13)  can  be  assumed  to  pass  through  the  origin  and  V m  can  be
        calculated  on  the  basis  of  a  single  gas-adsorption  measurement
                        between 0.2 and 0.3).  This procedure is frequently
        (usually with p/p 0
        adopted  for routine surface area  measurements.
          The  adsorbate  most  commonly  used  for  BET  surface  area
        determinations is nitrogen at 77 K (liquid nitrogen temperature). The
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