TY - JOUR
T1 - Free energy of activation. Definition, properties, and dependent variables with special reference to "linear" free energy relations
AU - Levine, R. D.
PY - 1979
Y1 - 1979
N2 - The reaction rate constant is expressed as Z exp(-Ga/RT). Z is the binary collision frequency. Ga, the free energy of activation, is shown to be the difference between the free energy of the reactive reactants and the free energy of all reactants. The results are derived from both a statistical mechanical and a collision theoretic point of view. While the later is more suitable for an ab-initio computation of the reaction rate, it is the former that lends itself to the search of systematics and of correlations and to compaction of data. Different thermodynamic-like routes to the characterization of Ga are thus explored. The two most promising ones appear to be the use of thermodynamic type cycles and the changes of dependent variables using the Legendre transform technique. The dependence of Ga on ΔG°, the standard free energy change in the reaction, is examined from the later point of view. It is shown that one can rigorously express this dependence as Ga = αΔG° + Ga°M(α). Here α is the Brønsted slope, α = -∂ ln k(T)/∂(ΔG°/RT), Ga° is independent of ΔG° and M(α), the Legendre transform of Ga, is a function only of α. For small changes in ΔG°, the general result reduces to the familiar "linear" free energy relation δGa = αδΔG°. It is concluded from general considerations that M(α) is a symmetric, convex function of α and hence that α is a monotonically increasing function of ΔG°. Experimental data appear to conform well to the form α = 1/[1 + exp(-ΔG°/Ga°)]. A simple interpretation of the ΔG° dependence of Ga, based on an interpolation of the free energy from that of the reagents to that of the products, is offered.
AB - The reaction rate constant is expressed as Z exp(-Ga/RT). Z is the binary collision frequency. Ga, the free energy of activation, is shown to be the difference between the free energy of the reactive reactants and the free energy of all reactants. The results are derived from both a statistical mechanical and a collision theoretic point of view. While the later is more suitable for an ab-initio computation of the reaction rate, it is the former that lends itself to the search of systematics and of correlations and to compaction of data. Different thermodynamic-like routes to the characterization of Ga are thus explored. The two most promising ones appear to be the use of thermodynamic type cycles and the changes of dependent variables using the Legendre transform technique. The dependence of Ga on ΔG°, the standard free energy change in the reaction, is examined from the later point of view. It is shown that one can rigorously express this dependence as Ga = αΔG° + Ga°M(α). Here α is the Brønsted slope, α = -∂ ln k(T)/∂(ΔG°/RT), Ga° is independent of ΔG° and M(α), the Legendre transform of Ga, is a function only of α. For small changes in ΔG°, the general result reduces to the familiar "linear" free energy relation δGa = αδΔG°. It is concluded from general considerations that M(α) is a symmetric, convex function of α and hence that α is a monotonically increasing function of ΔG°. Experimental data appear to conform well to the form α = 1/[1 + exp(-ΔG°/Ga°)]. A simple interpretation of the ΔG° dependence of Ga, based on an interpolation of the free energy from that of the reagents to that of the products, is offered.
UR - http://www.scopus.com/inward/record.url?scp=0009797946&partnerID=8YFLogxK
U2 - 10.1021/j100464a023
DO - 10.1021/j100464a023
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AN - SCOPUS:0009797946
SN - 0022-3654
VL - 83
SP - 159
EP - 170
JO - Journal of Physical Chemistry
JF - Journal of Physical Chemistry
IS - 1
ER -