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

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7.3 Thermodynamic interpretation of transition state theory 160<br />

7.3 Thermodynamic interpretation of transition state theory<br />

7.3.1 Fundamental equation of thermodynamic transition state theory<br />

As shown above,<br />

( )= <br />

‡ (7.59)<br />

<br />

‡ can often be interpreted using thermodynamic arguments, i.e., ∆ ‡ , ∆ ‡ ,and<br />

∆ ‡ . For liquid phase reactions, this is straightforward. For gas phase reactions, we<br />

have to take into account the difference between ‡ and .<br />

‡<br />

a) Thermodynamic transition state theory for unimolecular gas phase reactions<br />

For unimolecular isomerization and dissociation reactions of the type<br />

or<br />

we have<br />

ABC → ABC ‡ → ACB ‡ (7.60)<br />

ABC → ABC ‡ → A+BC ‡ , (7.61)<br />

£ ¤<br />

ABC<br />

‡<br />

‡ ( )=<br />

[ABC]<br />

= ABC ‡<br />

ABC<br />

= ‡ ( ) (7.62)<br />

‡ ( )= ‡ ( )= ‡ ( ) is dimensionless (∆ ‡ =0) and we do not have to worry<br />

about a difference between ‡ ( )= ‡ ( ) and about units or different standard<br />

states.<br />

I Results: Eq. 7.59 thus gives the following results:<br />

• Rate constant:<br />

y<br />

( )= <br />

‡ ( )= µ <br />

<br />

exp − ∆‡<br />

<br />

( )= µ <br />

<br />

∆<br />

‡<br />

exp exp<br />

µ− ∆‡<br />

<br />

<br />

(7.63)<br />

(7.64)<br />

• Arrhenius activation energy:<br />

y<br />

= 2 ln <br />

<br />

= 2 ∙ µ<br />

ln ∆<br />

‡<br />

exp <br />

<br />

exp<br />

¸<br />

µ− ∆‡<br />

<br />

(7.65)<br />

<br />

= ∆ ‡ + + 2 ∆‡<br />

<br />

= ∆ ‡ + + ∆‡ <br />

<br />

(7.66)<br />

(7.67)<br />

If ∆ ‡ 6= ( ) in the temperature range of interest, we obtain<br />

= ∆ ‡ + (7.68)

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