Physical Chemistry 3: — Chemical Kinetics — - Christian-Albrechts ...

Physical Chemistry 3: — Chemical Kinetics — - Christian-Albrechts ... Physical Chemistry 3: — Chemical Kinetics — - Christian-Albrechts ...

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7.1 Foundations of transition state theory 151 • −→ ‡ = −→ ‡ is the mean speed of the molecules crossing the DS in the forward direction. (6) We now use the equilibrium constant to determine ‡ via ‡ = ‡ ABC A BC (7.18) y ‡ = ‡ ABC = ‡ A BC (7.19) y −→ −→ ‡ ‡ = ‡ A BC = A BC (7.20) with −→ ‡ = ‡ (7.21) (7) From statistical thermodynamics (see Appendix G), we have the following expression for the equilibrium constant ‡ ( ) in terms of the molecular partition functions: ‡ ( )= ∗ = µ exp − ∆ 0 (7.22) • The ’s are the respective molecular partition functions (per unit volume). • ∗ is written with respect to the zero-point level of the reactants. • The exp (−∆ 0 ) factor arises subsequently, because we now express the value of partition function for the TS relative to the zero-point level of the TS ( ∗ = exp (−∆ 0 )). (8) Separating the motion along the reaction coordinate ‡ from the other degrees of freedom, we write = ‡ ‡ (7.23) where ‡ is the 1-D (translational) partition function describing the translational motion of the molecules along ‡ across the TS and ‡ is the partition function for all 3 − 7 other (rotational-vibrational-electronic) degrees of freedom. Here, • the 1-D translational partition function is ‡ = µ 2 2 12 × (7.24) • the mean speed along ‡ for crossing the DS in the forward direction is given by R −→ ∞ ‡ −2 2 µ 12 0 = R ∞ −∞ −2 2 = (7.25) 2

7.1 Foundations of transition state theory 152 (9) Collecting and inserting the results into −→ ‡ ( )= ( ) (7.26) we obtain ( )= 1 µ 12 µ 12 µ 2 × × ‡ exp − ∆ 0 (7.27) 2 2 y ( )= ‡ µ exp − ∆ 0 (7.28) I Result: In order to account () forsomerecrossingoftheTSand() for quantum mechanical tunneling, we add an additional factor called the transmission coefficient. For well-behaved reactions, ≈ 1. Thus, we end up with the fundamental equation of TST in the form: ( )= ‡ µ exp − ∆ 0 Note that ‡ is the partition function of the TS excluding the RC. Equation 7.29 allows us to calculate ( ) using the following data: (7.29) • The threshold energy for the reaction ∆ 0 (or, per mol, ∆ 0 ). ∆ 0 has to be obtained from ab initio quantum chemistry calculations, and • structural information on the reactants and the TS (i.e., bond lengths and angles, vibrational frequencies). I Figure 7.4: Illustration of ∆ ‡ , ∆ 0 ,and .

7.1 Foundations of transition state theory 152<br />

(9) Collecting and inserting the results into<br />

−→<br />

<br />

‡<br />

( )=<br />

( ) (7.26)<br />

we obtain<br />

( )= 1 µ 12 µ 12 µ<br />

2 <br />

×<br />

× ‡ <br />

exp − ∆ <br />

0<br />

(7.27)<br />

2<br />

2<br />

<br />

y<br />

( )= ‡ µ<br />

<br />

exp − ∆ <br />

0<br />

(7.28)<br />

<br />

I Result: In order to account () forsomerecrossingoftheTSand() for quantum<br />

mechanical tunneling, we add an additional factor called the transmission coefficient.<br />

For well-behaved reactions, ≈ 1. Thus, we end up with the fundamental equation<br />

of TST in the form:<br />

( )= <br />

<br />

‡ µ<br />

<br />

exp − ∆ <br />

0<br />

<br />

Note that ‡ <br />

is the partition function of the TS excluding the RC.<br />

Equation 7.29 allows us to calculate ( ) using the following data:<br />

(7.29)<br />

• The threshold energy for the reaction ∆ 0 (or, per mol, ∆ 0 ). ∆ 0 has to be<br />

obtained from ab initio quantum chemistry calculations, and<br />

• structural information on the reactants and the TS (i.e., bond lengths and angles,<br />

vibrational frequencies).<br />

I Figure 7.4: Illustration of ∆ ‡ , ∆ 0 ,and .

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