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

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7.2 Applications of transition state theory 157<br />

7.2.3 Example 2: The reaction F + H 2 → F···H···H ‡ → FH + H<br />

I<br />

Exercise 7.1: Evaluatetherateconstantforthereaction<br />

F+H 2 → F ···H ···H ‡ → FH + H (7.47)<br />

using the data in Table 7.2 at =200, 300, 500, 1000 and 2000 K, determinethe<br />

Arrhenius parameters, and compare the results with the experimental value of<br />

=2× 10 14 exp (−800 )cm 3 mol s (7.48)<br />

¤<br />

I Table 7.2: Properties of the reactants and transition state of the reaction F + H 2 .<br />

parameter F ···H ···H ‡ a F H 2<br />

2 (F ···H) ( Å) 1602<br />

1 (H ···H) ( Å) 0756<br />

07417 b<br />

1 (cm −1 ) 40076 43952<br />

2 (cm −1 ) 3979<br />

3 (cm −1 ) 3979<br />

4 (cm −1 ) 3108 c<br />

³ (u) 21014 189984 2016<br />

u Å 7433<br />

0277<br />

1 2<br />

<br />

d<br />

4 4 1<br />

0 ¡ kJ mol −1¢ 657 000<br />

a The transition state FHH ‡ is assumed to be linear.<br />

b = (H-H).<br />

c One imaginary frequency describes the TS along the RC.<br />

d The electronic ground state of F is 2 32 . We neglect the 2 12 spin-orbit component at ( 2 12 )=<br />

404 cm −1 because it does not correlate with the products H + HF. The electronic state of linear<br />

FHH ‡ is 2 Π. The ground state of H 2 is 2 Σ + .<br />

I Solution 7.1:<br />

( )= ‡ µ<br />

<br />

exp − ∆ <br />

0<br />

2 <br />

Ã<br />

!<br />

= ‡ <br />

( )( 2 )<br />

µ<br />

× exp − ∆ <br />

0<br />

<br />

<br />

à !<br />

‡ <br />

2<br />

<br />

à !<br />

‡ <br />

2<br />

<br />

(7.49)<br />

à !<br />

‡ <br />

2<br />

<br />

(7.50)

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