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

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8.4 The specific unimolecular reaction rate constants () 198<br />

b) Density of states:<br />

() = ( + () ) −1<br />

( − 1)! Q <br />

=1 <br />

(8.106)<br />

c) Specific rate constant:<br />

³<br />

() = 1 − 0 + ‡ ( − 0 ) ‡ ´−1<br />

() + <br />

()( − 1)! Q −<br />

−1<br />

=1 ‡ <br />

(4) For energies sufficiently above 0 , we can use the expressions<br />

and<br />

to obtain<br />

y<br />

‡ ( − 0 )=<br />

() = ‡ ( − 0 )<br />

()<br />

() =<br />

() =<br />

=<br />

³<br />

− 0 + ‡ ´−1<br />

<br />

( − 1)! Q −1<br />

=1 ‡ <br />

( + ) −1<br />

( − 1)! Q <br />

=1 <br />

³<br />

‡ (0) ‡ ´−1<br />

<br />

()( − 1)! Q −1<br />

=1 ‡ <br />

(8.107)<br />

(8.108)<br />

(8.109)<br />

³<br />

Q <br />

=1 − 0 + ‡ ´−1<br />

<br />

<br />

Q −1<br />

=1 ‡ <br />

( + ) −1 (8.110)<br />

Q <br />

=1 <br />

Q −1<br />

=1 ‡ <br />

The resemblence to the Kassel formula is obvious.<br />

Ã<br />

− 0 + ‡ <br />

+ <br />

! −1<br />

(8.111)<br />

8.4.3 The SACM and VRRKM model<br />

More advanced models allow for the tightening of the TS with increasing (variational<br />

RRKM theory = VRRKM theory) or even for individual adiabatic channel potential<br />

curves (statistical adiabatic channel model = SACM). The latter model has to be used<br />

for reactions with loose transition states.

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