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7.4 Experimental Determination  of  Seven Apparent  Equilibrium Constants   129


             The values of A,G"'(TotT)  in Table 7.1 and AfG"'(TotD)  in Table 7.2 make
         it possible  to calculate the apparent equilibrium  constant for the reaction
                                     2TotD = TotT                        (7.3-7)
         at three concentrations  of molecular  oxygen. The apparent equilibrium  constant
         K", which is a function  of  [O,],  is defined by
                                            [TotT]
                                      K" =                               (7.3-8)
                                           [Tot D]
         This  apparent  equilibrium  constant  can  be  written  in  terms  of  the  binding
         polynomials  of tetramer  and dimer and "K';:

                                                                         (7.3-9)

         As  [O,]  approaches  infinity,  this  apparent  equilibrium  constant  approaches a
         limiting value because the reaction becomes

                                    2D(02)2  = T(02)4                   (7.3- 10)
         in the limit  of  infinite  [O,].  The value  of  this  apparent equilibrium constant at
         very high  oxygen concentrations  is given by




                                                                        (7.3-1 1)
         Note that this equilibrium constant is 5 x lo4 times smaller than for 2D = T (see
         Problem  7.3). This  is  not  unexpected  because  of  the  cooperative  effect  in  the
         tetramer.



         rn  7.4  EXPERIMENTAL DETERMINATION OF SEVEN
                  APPARENT EQUILIBRIUM CONSTANTS

         The fractional saturation of tetramer  Y, and the fractional saturation of dimer  YD
         are functions only of [O,]  at specified 7; P, pH, etc., as shown by equations 7.1-18
         and 7.3-6. However, since the tetramer  form is partially  dissociated  into dimers,
          the fractional saturation of heme Y is a function of both [O,]  and [heme].  Ackers
          and  Halvorson  (1974)  derived  an expression  for  the function  Y([O,],  [heme]).
          When Legendre transforms are used, a simpler form of  this function is obtained,
          and it can be used to derive limiting forms at high and low [heme].  These limiting
          forms are of  interest  because they  show that if  data can  be  obtained in regions
         where  Y  is  linear  in  some  function  of  [heme],  extrapolations  can  be  made  to
          obtain  Y,  and  Y,.  These  fractional  saturations can  be  analyzed  separately  to
          obtain the Adair constants  for the tetramer  and the dimmer (Alberty, 1997a).
             When the tetramer  and dimer are in equilibrium, the fractional saturation of
          heme is given by

                                      Y=fD%   +fTYT                       (7.4-1)
          where  fD  = 2[TotD]/[heme]   is  the  fraction  of  the  heme  in  the  dimer  and
          fT  = 4[TotT]/[heme]   is  the  fraction  of  the  heme  in  the  tetramer.  Since
         fT  = 1 - f,, equation 7.4-1 can be written
                                   Y = YT  + fD(  YD  - YT)               (7.4-2)
          The concentration  of  heme in the solution is given by

                    [heme]  = 2[TotD]  + 4[TotT]  = 2[TotD]  + 4K"[TotDI2   (7.4-3)
          where  equation  7.3-8  has  been  used  in  writing  the  last  form.  Applying  the
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