c21 JWBS043-Rogers September 13, 2010 11:30 Printer Name: Yet to Come
354 PHOTOCHEMISTRY AND THE THEORY OF CHEMICAL REACTIONSreacting because each one-cycle vibration leads to products. Thusk 1 isν(notice that
both are frequencies) and−
d[A]
dt=
RT
NAhK∗[A][B]
If the assumption that all vibrations lead to products does not hold, one includes a
transmission coefficientκ, which is that fraction of activated complexes that break
up to give products. Now,−
d[A]
dt=κRT
NAhK∗[A][B]
orkobserved=κRT
NAhK∗
21.9 ENTROPIES OF ACTIVATION
In general, the free energy change of a reaction varies as the natural logarithm of its
equilibrium constant, so for the steady-state activation equilibrium we writeG◦∗=−RTlnK◦∗where the superscript designates the standard state of the Gibbs free energy for the
activation pseudo-equilibrium. The equivalent form forK◦∗isK◦∗=e−G◦∗/RTBy analogy to a true equilibrium, for whichG◦=H◦−TS◦
we writeK◦∗=eS
∗/R
e−H
∗/RTThe observed rate constant iskobserved=κRT
NAheS
∗/R
e−H
∗/RT