c21 JWBS043-Rogers September 13, 2010 11:30 Printer Name: Yet to Come
354 PHOTOCHEMISTRY AND THE THEORY OF CHEMICAL REACTIONS
reacting because each one-cycle vibration leads to products. Thusk 1 isν(notice that
both are frequencies) and
−
d[A]
dt
=
RT
NAh
K∗[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
=κ
RT
NAh
K∗[A][B]
or
kobserved=κ
RT
NAh
K∗
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 write
G◦∗=−RTlnK◦∗
where the superscript designates the standard state of the Gibbs free energy for the
activation pseudo-equilibrium. The equivalent form forK◦∗is
K◦∗=e−G
◦∗/RT
By analogy to a true equilibrium, for which
G◦=H◦−TS◦
we write
K◦∗=eS
∗/R
e−H
∗/RT
The observed rate constant is
kobserved=κ
RT
NAh
eS
∗/R
e−H
∗/RT