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

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8.4 The specific unimolecular reaction rate constants () 191<br />

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

We may intuitively expect that the specific uinimolecular reaction rate constants ()<br />

depend on the energy content (i.e., the excitation energy ) of the energetically activated<br />

molecules molecules A ∗ . More precisely, we will also have to take into account<br />

the dependence of the specific rate constants on other conserved degrees of freedom,<br />

in particular total angular momentum (⇒ ()), and perhaps other quantities<br />

(symmetry, components of if -mixing is weak, (⇒ (; ; ))).<br />

8.4.1 Rice-Ramsperger-Kassel (RRK) theory<br />

I RRK model: In order to derive an expression for the specific rateconstants (),<br />

werealizethatitisnotenoughthatthemoleculesareenergizedtoabove 0 . Indeed,<br />

for the reaction to take place, the energy also has to be in the right oscillator, namely<br />

in the RC. In particular, for the reaction to take place, of the total excitation energy ,<br />

the amount † has to be concentrated in the RC such that † ≥ 0 . Thus, we can<br />

write the reaction scheme as<br />

∗ †<br />

→ † → (8.74)<br />

where † denotes those excited molecules that have enough energy in the RC to overcome<br />

0 . We assume that once this critical configuration ( † ) is reached, the molecules<br />

will immediately cross the TS and go to the product side.<br />

I Probabilities of A † and A ∗ : The probability of † compared to ∗ can be derived<br />

using statistical arguments by considering the ratio of the density of states. We consider<br />

amoleculewith<br />

• oscillators,<br />

• = quanta which have to be distributed over the oscillators,<br />

• a threshold energy of 0 such that a minimum of = 0 quanta have to be<br />

concentrated in the RC and only − quanta can be distributed freely,<br />

• À and − À .<br />

The probability of † relative to ∗ is given by<br />

¡ †¢<br />

( ∗ ) = ¡ †¢<br />

( ∗ )<br />

(8.75)<br />

where<br />

( ∗ ) ∝ ∗ () = 1 ( + − 1)!<br />

(8.76)<br />

!( − 1)!<br />

and, since in the critical configuration only − quanta can be distributed freely,<br />

¡ †¢ ∝ † () = 1 ( − + − 1)!<br />

( − )! ( − 1)!<br />

(8.77)

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