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126     Chapter 7  Thermodynamics of the Binding of Ligands by  Proteins


                 Table 7.1   Standard Transformed Gibbs Energy of  Formation AfG'" and Standard Further Transformed Gibbs
                 Energies of  Formation A,G""  of  Hcinoglobin Tetramer at 21.5T, 1 bar, pH  7.4, [Cl-]  = 0.2 M, and 0.2 M
                 Ionic Strength
                                                                            A,G""/kJ  mol

                                        A,G'',kJ  mol-'   [Oz]=5 x 10-'  M   [O,]=lO-s  M   [O,]=~X 10-5M
                               ~     ~~      ~~
                 T                           0                 0                 0                0
                 PO,)                     - 10 092 2           3711 09           2 012 97         0 314 85
                 T(0,)2                   - 17 045 5          10561 10           7 164 84         3 768 59
                 T(02)j                   - 32 5768            8833 13           3 738 77       - 1 355 60
                 ~(0~4                    -49  3213            5891 89         -0  900 59       - 7 693 07
                 A,G"J(TotT)/kJ  mol  '    -0736  51         - 0 73651         -2814  90        - 8 069 06

                 Sourti..  Ikprintcd from K. A. Alberty, Biop/i).s. C/iei?i. 62,  141  159 (1996), with permission  from  Elsevier Science
                                                            ~
                 Norr:  See Problem  7.1.
                                       p"(T(O,),)  = p"(T(O,),)  = p"(T(0JJ.  Therefore equation 7.2-5 can be written

                                        dC" = -SdT+  VdP + p"(T)dnh(TotT) - n;(O,)dp'(O,)  + RTln(lO)n,(H)dpH
                                                                                                      (7.2-1  1)

                                       This shows that the natural variables for the further transformed Gibbs energy G"
                                       are 7:  P, n:(T),  p'(O,), and pH, and so the criterion for spontaneous change and
                                       equilibrium  is  dC" < 0  at constant  7:  P, nk(T), p"(02), pH.  There  are  D"  = 5
                                       natural variables and F"  = 4 independent intensive variables,  the same as for  G'.
                                           The  integrated form  of  equation  7.2-11  at constant  values  of  the  intensive
                                       variables is

                                                                 G" = p"(T)nk(TotT)                   (7.2- 12)
                                       so this system behaves like a one-component system. Under these conditions the
                                       entity TotT, which  is made up of  the various forms of  the tetramer, has a set  of
                                       further  transformed  thermodynamic  properties.  As  we  have  seen  before,  the
                                       standard  further  transformed  Gibbs  energy  of  formation  A,G""(TotT)  of  the
                                       tetramer  pseudoisomer  group  at  a  specified  concentration  of  molecular oxygen
                                       can be calculated by  using equation 4.5-1 for an isomer group.
                                           Derivations  are  carried  out  with  chemical  potentials,  but  calculations  are
                                       carried out with Gibbs energies of  formation, and so equation 7.2-2 is used in the
                                       form

                                                     Arc:" = AfCio + AJi(02)(AfCo(02) + RTln[O,])     (7.2-  13)
                                       where A,G"  values are given after equation 7.1-20. The values of A,C;" calculated
                                       using equation 7.2-13 for the five forms at three [O,]  are given in  Table 7.1. The
                                       ArGi") values for T are independent of [O,]  because T does not contain 0,. The
                                       other  AfG;"  values  decrease  as  [O,]  is  raised  because  the  oxygenated  forms
                                       become inore stable relative  to T. The value of  A,G""(TotT)  is calculated using
                                       the partition function in equation 4.5-1. A,G""(TotT)  is more negative than A,G;"
                                       for any of the pseudoisomers and becomes more negative as the concentration of
                                       oxygen is increased. The entries in Table 7.1 were calculated with  the Matlumut-
                                       icu program calctgfT (Alberty, 1996b).
                                           The equilibrium mole fractions of  the various forms of  the tetramer can  be
                                       calculated using the following analog of equation 4.5-2:
                                                                    A,G""(TotT)  - AfGa]
                                                           ri = exp                                   (7.2- 1 4)


                                       These equilibrium mole fractions are given in Table 7.2.
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