Page 181 - Thermodynamics of Biochemical Reactions
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11.2 Transformed Gibbs Energy for a System Containing a Weak  Acid   181


             When a system at specified T and P contains  two species and one of them is
         in  equilibrium  with  that  species in  a  reservoir  through  a  semipermeable  mem-
         brane,  the  transformed  Gibbs  energy  of  the  system  is  calculated  from  the
         semigrand partition function r’(T, P, pl, N,)  by  use of
                          G’(T P, p,,  N,)  = -kTInI-’(T,  P, p,, N2)   (1 1.1-4)
             Statistical  mechanics  is  often  thought  of  as  a  way  to  predict  the  ther-
         modynamic properties  of  molecules from their microscopic properties,  but statis-
         tical  mechnics  is  more  than  that  because  it  provides  a  complementary  way  of
         looking at thermodynamics. The transformed  Gibbs energy G‘ for a biochemical
         reaction  system at specified pH is given by

                                     G‘ = - kTln I-’                    ( 1 1.1 -5)
         The  semigrand  partition  function  r’ corresponds  with  a  system  of  enzyme-
         catalyzed reactions in contact with a reservoir of hydrogen ions at a specified pH.
         The  semigrand  partition  function  can  be  written  for  an  aqueous solution  of  a
         biochemical  reactant  at  specified  pH  or  a  system  involving  many  biochemical
         reations.  The other  thermodynamic  properties  of  the  system  can  be  calculated
         from r‘.
             The further transformed Gibbs energy G” for a biochemical rection system at
         specified pH and specified concentrations  of  certain coenzymes is given by
                                     G“ = - kTln I-’’                   ( 1 1.1 -6)
         where  r” is  the  corresponding  semigrand  partition function.  All  the  remaining
         thermodynamic  properties  of  the  system  can  be  calculated  by  taking  partial
         derivatives of  G“ or r”.
             This is not the place to discuss the partition functions E, Y, A, and   in detail,
         but it is important to point out that B and Y differ by the factor exp(fiN,p,) and
         A  and r differ by the same factor. Thus holding the chemical potential  of  species
         1 constant has the effect of introducing an exponential factor that depends on the
         number  of  molecules of species 1 and the chemical potential  of  species 1.


         H  11.2  TRANSFORMED GIBBS ENERGY FOR A SYSTEM
                   CONTAINING A WEAK ACID AND ITS BASIC
                   FORM AT A SPECIFIED pH

         The forms of  semigrand partition functions for biochemical  rection  systems can
         be illustrated, starting with an aqueous solution of a weak acid and its basic form
         at a  specified pH  (Alberty, 2001~). The semigrand  partition  function r’ for  this
         system is given by
         I-’(T P, PH, KO)

              = (exp( -[lp,)exp(   - N,,  In(l0)pH) + exp( -Pp2)exp(-  N,,  In(10)pH}N~50

              = {exp( - bpi) + exp( - [jpi)}Niso                         (1 1.2- 1)
         where  ,LL~ and p2 are the chemical potentials  of  species 1 and 2 (i.e., A-  and HA)
          and  11: = p, - N,,p(H+).  N,,  and  N,,  are  the  numbers  of  hydrogen  atoms  in
          these  two  species  N:so is  the  number  of  molecules  in  the  pseudoisomer  group,
          N, + N,.  Equation  11.2-1 has been  given  in  the  form  of  the  partition  function
          that applies at zero ionic strength  in order to keep it simpler, but this complica-
          tion can be  taken into account by  using

                                                   2.91482(zj - NH(j))I”2
                  p\ = pj(Z = 0) + N,(j)RTIn(lO)pH  -                    (1 1.2-2)
                                                         1 + 1.61”2
          Note that the exp( -Bpi)  terms for species are weighted  according to the number
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