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

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5.4 Advanced collision theory 137<br />

• Withalong-rangeattractivetermoftheform− ¡ <br />

¢ <br />

<br />

, the intermolecular potential<br />

thus has the form<br />

µ 2<br />

() =− + (5.213)<br />

<br />

µ 2 <br />

= − + ~2 ( +1)<br />

(5.214)<br />

2 2<br />

i.e.,<br />

() ∝− − + −2 (5.215)<br />

<strong>—</strong> The −2 term is important in practice if 3. In effect, it leads to an<br />

effective energy barrier (“centrifigual” barrier).<br />

<strong>—</strong> The larger for a given , the larger the orbital angular momentum .<br />

I<br />

Figure 5.28: Potential energy curves with centrifugal barriers for a diatomic system.<br />

d) Langevin “capture” rate constant for ion-molecule reactions*<br />

An nice illustration of the above results is the rate constant for ion-molecule reactions.<br />

The intermolecular interaction is governed by the point charge-induced dipole interaction.<br />

40 In addition, the centrifugal barrier has to be taken into account, so that<br />

() =−<br />

µ 2 ()2 <br />

(4 0 ) 2 2 + 4 (5.216)<br />

<br />

The resulting expression for the rate constant is<br />

à !<br />

4 () 2 12 µ 1<br />

( )=<br />

(4 0 ) 2 × Γ<br />

(5.217)<br />

2<br />

Typical values of are 100 × <br />

40 () needs to be checked again!!

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