sition state, and rewrite the Eyring equation in terms of the Gibbs free energy.
We g e t
k
c
k
°
T
h
eG*/RT (20.80)
where kon the left is the rate constant, whereas kon the right is Boltzmann’s
constant. Since Gcan be written in terms ofHand S, we can rewrite equa-
tion 20.80 as
k
c
k
°
T
h
eH/RTeS*/R (20.81)
where now we are referring to an enthalpy change for the formation of the
transition state,H, and an entropy change for the formation of the transi-
tion state,S. Equation 20.81 is similar to the Arrhenius equation, but not
exactly. However, if we write the logarithm of the Arrhenius equation as
ln kln A
R
E
T
A
we differentiate with respect to temperature:
ln
T
k
ln
T
A
T
R
E
T
A
The term (ln A)/Tis zero (Ais a constant, so the derivative is zero), and we
can evaluate the derivative of the activation energy. We get
ln
T
k
R
E
T
A
(^2)
We can rearrange this to
EART^2
ln
T
k
RT^2
1
k
T
k
(20.82)
We can substitute the expression for kfrom equation 20.81 into equation 20.82
to find that
EAH* 2 RT or H* EA 2 RT (20.83)
In terms of the activation energy,kcan be written as
k
c
k
°
T
h
e(EA^2 RT)/RTeS*/R
c
k
°
T
h
eEA/RTe(^2 RT)/RTeS*/R
20.10 Transition-State Theory 723
Table 20.2 Experimental and calculated pre-exponential factors
A[cm^3 /(mols)]
Reaction Experimental Calculated
H H 2 →H 2 H 5.4 1013 7.4 1013
H 2 Br →HBr H 3 1013 1 1014
H CH 4 →H 2 CH 3 1 1013 2 1013
CH 3 H 2 →CH 4 H 2 1012 1 1012
ClO ClO →Cl 2 O 2 6 1010 1 1011
Source:J. Nicholas,Chemical Kinetics: A Modern Survey of Gas Reactions,Wiley, New York, 1976.