Page 55 - Adsorption Technology & Design, Elsevier (1998)
P. 55

52  Fundamentals of adsorption equilibria


            sum of coverages of the individual components. The resulting isotherm for
            component i is

              Oi(-qi    )=     bipin                                   (3.31)
                    qmi     1 + ~  bipi
                                1
            where  qm~  is  the  quantity  of  component  i  in  a  monolayer  of  mixed
            adsorbates.  It has been shown, by invoking thermodynamic principles, that,
            for consistency, the monolayer quantity or volume for each of the adsorbed
            components  must  be  identical.  This  means,  for  example,  that  qm~ =  qmj
            (Kemball  et al.  1948, Broughton  1948).  For  a  gas  mixture  containing
            adsorbate  molecules  which would  occupy  substantially  different  areas  on
            adsorption, such a constraint is unrealistic and so the monolayer capacities
            of each adsorbate are then regarded as empirical quantities, qm~ in equation
            (3.31)  would thus be  replaced  by an empirical  constant ai. However,  such
            empirical constants may not be applicable over an extended range of partial
            pressures  and  their  use  should  then  be  restricted  to  the  range  of partial
            pressures for which they are ostensibly constant.
              Indeed,  the  extended  Langmuir  equation  (3.31)  provides  a  satisfactory
            correlation  of single component  isotherm  data  for carbon  dioxide-carbon
            monoxide  mixtures  adsorbed  on  a  porous  activated  carbon  (Battrum  and
            Thomas 1991). From the single-component isotherm data for CO2 values of
            aco~ and bco~ may be obtained from the intercept and slope of a linear plot
            of 1/qco2 against 1/pco~. Similarly values of aco and bco are obtained from
            single component  isotherm  data  for CO.  The  values so obtained  are  then
            substituted  into  equation  (3.31)  to  obtain  the  isotherms  for  each  of  the
            components CO2 and CO in the mixture. On the other hand, for mixtures of
            benzene and toluene vapours,  the extended  Langmuir isotherm for binary
            mixture  adsorption  on  an  activated  charcoal  is  only  correlated  by  the
            constants obtained  from the single component  toluene  isotherm when the
            constant  bB  for  benzene  was  determined  empirically  by  linearizing  the
            extended  Langmuir  equation  for  the  component  toluene  (Thomas  and
            Lombardi 1971). Data relating to the adsorption of benzene-toluene vapour
            mixtures on charcoal do not conform with the condition that aT and aB are
            equal. This is demonstrated by defining a separation factor
                     q2[c2
                                                                        (3.32)
               K12  =
                     ql/cl
            by  analogy  with  the  definition  for  vapour-liquid  mixtures  in  which  a
            comparison is made of the relative volatilities of each component. If QT and
            CT represent total concentrations  of adsorbed  and gas (or vapour)  phases,
            respectively, then equation (3.32) may be written in the alternative form
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