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100                                                    Carraher’s Polymer Chemistry


                    While more complicated situations can occur, we will consider only the kinetics of simple polyes-
                 terification. The kinetics of most other common polycondensations follows an analogous pathway.

                    For uncatalyzed reactions where the diacid and diol are present in equimolar amounts, one dia-
                 cid is experimentally found to act as a catalyst. The experimental expression dependencies are
                 described in the usual manner as follows:
                                                                A
                                       Rate of polycondensation =−  d[ ]  =  [ ] [ ]        (4.14)
                                                                         D
                                                                    kA
                                                                        2
                                                               dt
                    where [A] is the concentration of diacid and [D] is the diol concentration. Since [A] = [D], we can
                 write
                                                      A
                                                   −  d[ ]  =  kA  3                        (4.15)
                                                           []
                                                      dt
                    Rearrangement gives
                                                       A
                                                    −  d[ ]  =  kt                          (4.16)
                                                            d
                                                      A 3
                    Integration of Equation 4.16 over the limits of A = A  to A = A  and t = 0 to t = t gives
                                                              o      t
                                         2kt =−  1  −  1   =   1    +   constant            (4.17)
                                                            A
                                               [A  ] 2  [A  ] 2  [ ] 2
                                                 0     0     t
                    It is usual to express Equation 4.17 in terms of the extent of reaction, p, where p is defi ned as the
                 fraction of functional groups that have reacted at time t. Thus, 1 − p is the fraction of groups unre-
                 acted. A  is in turn A  (1 − p), that is,
                        t         o
                                                   A  = A  (1 − p)                          (4.18)
                                                     t  o
                    Substitution of the expression for A  from Equation 4.18 into Equation 4.17 and rearrangement
                                                 t
                 gives

                                              2Akt =   1   +  constant                      (4.19)
                                                 2
                                                      −
                                                 0   (1 p ) 2

                 which is the equation of a straight line, that is,
                                                     mx = y + b

                                             −
                    Where m =  2A k x =  , t y =  1/(1 p ) , and b is the constant. A plot of 1/(1 − p)  as a function of
                                                2
                                2
                                                                                   2
                                 ,
                                0
                                                2
                 time should be linear with a slope 2A  k from which k is determined. Determination of k at differ-
                                               o

                 ent temperatures allows the calculation of activation energy. Thus, one definition of the specifi c rate
                                 a/
                               –
                 constant is k = Ae E kt. The log of both sides gives log k = log A –E /kt, which again is the equation
                                                                       a
                 of a straight line where y = log k, b = log A, m = −E /k and x = 1/t, where E  is the activation energy,
                                                          a                  a
                 A is a constant, k is the specific rate constant, and t is the temperature.

                    The number-average DP can be expressed as
                                     DP n  =  number of original molecules  =  N 0  =  A 0  (4.20)
                                           number of molecules at time t  N  A t
                                                                                              9/14/2010   3:38:07 PM
         K10478.indb   100                                                                    9/14/2010   3:38:07 PM
         K10478.indb   100
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