Page 53 - Thermodynamics of Biochemical Reactions
P. 53

3.7 Effect of  Temperature on Thermodynamic Properties   47


         to  provide  activity  coefficients  in  the  physiological  range  by  introducing  an
         empirical term  to form the extended Debye-Huckel  equation.

                                             cx.;   Ill2
                                   lny, = -                              (3.6-1)
                                            1 + BPI~
         where B is 1.6 L1'2 mol-'".  This equation works quite well in the 0.05 to 0.25 M
         range of ionic strengths for a number of electrolytes for which activity coefficients
         have been  determined  accurately.  It is evident  from this equation  that the effect
         of ionic strength on the thermodynamic  properties of ionic species of biochemical
         interest  are  significant  in  the  0.05  to  0.25  M  range.  The effects  are  especially
         significant  when  ions  have  charges  of  2,  3,  or  4.  The  treatments  of  the  ther-
         modynamics  of  electrolyte  solutions  at  higher  concentrations  require  more
         complicated  equations  with  more  empirical  parameters  (Pitzer,  1991,  1995).
         However,  there  is  insufficient  data  on  the  specific  effects  of  various  ions  in
         biochemical buffers to go beyond  equation 3.6-1 at present.
            Thus the standard enthalpy of formation AfHY(I) and standard Gibbs energy
         of formation AfG:(I)  of an ionic species at 298.15 K in kJ mol- ' can be calculated
         using (Clark and Glew, 1980; Goldberg and Tewari,  1991)
                           A,HP(I) = A,HP(I = 0) +  1.4775~?1"~          (3.6-2)
                                                   1 + BP

                                                  2.91482221 'I2
                            A, GP(I) = A, Gp(Z  = 0) -                   (3.6-3)
                                                   1 + BP
         These equations will be very useful in the next chapter.
             The  standard  thermodynamic  properties  of  ions  are  given  in  tables  of
         standard thermodynamic properties at I  = 0. The effect of ionic strength on Arc"
         for  a  chemical  reaction  is  obtained  by  substituting  equation  3.6-3  in  equation
         3.1- 12:
                                               2.91482I1I2  E viz;
                         A,G"(I) = A,G"(I = 0) -                         (3.6-4)
                                                   1 + BI'I~
         where  E:viz? is the change in  z;  in  the reaction.  The effect of ionic  strength  on
         ArH'(I)  for  a  chemical  reaction  is  obtained  by  using  the  Gibbs-Helmholtz
         equation  (2.5-18 and 3.2-12):
                          A,HP(I) = A,Hp(I  = 0) +  1.47751'/2Evi~f      (3.6-5)
                                                   1 + BI"~
         The effect of ionic strength on the equilibrium constant for a chemical reaction at
         25"C is obtained  by substituting equation 3.6-4 in equation 3.1-2:
                          In  K(I) = In K(I  = 0) +  1.1 75821112Cviz2   (3.6-6)
                                                   1 + BI'I2


            3.7  EFFECT OF TEMPERATURE ON
                  THERMODYNAMIC PROPERTIES

         In  order  to  discuss  thermodynamic  properties  in  dilute  aqueous  solutions  at
         temperatures  other than 298.15 K, it is necessary  to have the standard enthalpies
         of  the species involved. Over narrow ranges  of  temperature,  calculations can be
         based  on the assumption  that A,HP  values  are independent  of  temperature,  but
         more accurate calculations can be made when C&i)  values are known. It is also
         necessary  to  take  into  account  the temperature dependencies  of  the  numerical
         coefficients in  equations 3.6-4 to  3.6-6. Clarke and  Glew  (1980)  calculated  the
         Debye-Huckel  slopes  for  water  between  0  and  150'C.  They  were  primarily
         concerned  with  electrostatic  deviations  from  ideality  of  the  solvent  osmotic
   48   49   50   51   52   53   54   55   56   57   58