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              Physical Organic Chemistry                                                                  223

              the reaction of Eq. (19) an appropriate reaction coordinate  with nuclei fixed at the particular value of  Q where the
              Q is given as follows since the distance between B and  energy is maximum.
              C is long in reactants and short in products, whereas the
              A B distance increases as reaction proceeds:
                             Q = d A B  − d B C  .      (22)
                                                                  That maximum energy of the transition state lies above
              Therefore  Q is a large negative number in the reactants  that of the reactants by an amount  G , equal to G ‡ −
                                                                                                ‡
              and rises to a large positive number in the products.  G reactants , as shown in Fig. 11. This energy difference is
                The key to understanding reaction rates is the depen-  calledtheactivationenergyorthefreeenergyofactivation.
              dence of energy upon Q. As C approaches A B, the en-  The rate constant of Eq. (21) can be related to this energy
              ergy must increase, from two sources: van der Waals re-  difference through the following equation, where k B is
              pulsion arising from overlap of the electron clouds, and  Boltzmann’s constant (1.381 × 10 −23   J/K), h is Planck’s
              an endothermicity from starting to break the A B bond.  constant (6.626 × 10 −33  J-sec), R is the gas constant, and
              This energy continues to increase until eventually, at large  T is the absolute temperature:
              Q, the energy will decrease as the B C bond develops
                                                                                             ‡
              and as the van der Waals repulsion between B C and A is     k = (k B T/h) exp(− G /RT ).    (23)
              relieved. Somewhere, in between, near Q = 0, when both                      ‡
                                                                This equation arises because  G is the amount of energy
              bonds are stretched about equally, the energy reaches a
                                                                that the reacting molecules must acquire in addition to that
              maximum, as sketched in Fig. 11.
                                                                of the reactants. It is the barrier that must be overcome.
                The position of the maximum is called the transition
                                                                This energy is used to push C into A B and to break the
              state, symbolized with a double dagger, ‡. This is the key
                                                                A B bond sufficiently for the B C bond to start forming.
              concept for understanding chemical reactivity. It is a spe-
                                                                That energy is derived from the accumulation of random
              cific point along the reaction coordinate  Q, or a unique
                                                                thermal motions. The average thermal energy is RT ,or
              geometry, with particular values of d A  B  and d B  C . It is  about 0.6 kcal/mole at room temperature. Some molecules
              the geometry at which the energy is maximum.
                                                                have less than average and some have more. Very few have
                The structure of the transition state cannot be described   ‡
                                                                as much as  G , but those that do will react. Conversion
              using simple Lewis structures since there are delocalized
                                                                of Eq. (23) into Table II shows how sensitive the rate of
              electrons. A pair of electrons is not localized in either the        ‡
                                                                reaction is to both  G and to T . A low barrier corre-
              A B bond, which is being broken, or in the B C bond,
                                                                sponds to a reaction that is very fast. A reaction with a
              which is being formed. The transition state can be de-
                                                                high barrier is very slow, but increasing the temperature
              scribed as a resonance hybrid of two resonance forms,  makes it go faster.
              60 and 61. Alternatively, in the shorthand form of 22–24  Much of our understanding of chemical reactivity
              it can be symbolized as 62, where the dotted lines sym-  comes from reasoning by analogy. If the rate constant k
              bolize the partial bonds that are breaking or forming. Yet  is known for some standard reaction, it is often possible
              according to the rules of resonance, only the electrons are  to predict, at least qualitatively, the rate constant k for a

              delocalized. The transition state has its unique geometry,  related reaction involving some modification of molecular
                                                                TABLE II Rate Constants and Activation Energy at Different
                                                                Temperatures
                                                                               At 25 ◦ ◦          At 100 ◦ ◦
                                                                  ∆G ‡ ‡
                                                                (kcal/mole)  k (sec −1 )  Half-life  k (sec −1 )  Half-life

                                                                    0     6.21 × 10 12  0.112 psec  7.78 × 10 12  0.089 psec
                                                                    5     1.34 × 10 9  516 psec  9.17 × 10 9  75.6 psec
                                                                   10     2.91 × 10 5  2.39 µsec  1.08 × 10 7  64.1 nsec
                                                                   15     6.28 × 10 1  11.0 msec  1.28 × 10 4  54.4 µsec
                                                                   20     1.36 × 10 −2  51.0 sec  1.50 × 10 1  46.1 msec
                                                                   25     2.94 × 10 −6  65.5 hr  1.77 × 10 −2  39.1 sec
                                                                   30     6.35 × 10 −10  34.5 years  2.09 × 10 −5  9.21 hr
                                                                   35     1.37 × 10 −13  160 kyears  2.47 × 10 −8  325 days
              FIGURE 11  Variation of energy along reaction coordinate Q for    −17                −11
                                                                   40     2.97 × 10  739 Myears  2.91 × 10  755 years
              the reaction A B + C → A + B C.
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