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

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5.4 Advanced collision theory 129<br />

y<br />

⎧<br />

⎨<br />

( )=<br />

⎩<br />

2 µ<br />

1 − 0<br />

<br />

<br />

0<br />

(5.187)<br />

0 0<br />

( ) is shown as function of in Fig. 5.22. Crossed molecular beam experiments<br />

have indeed shown similar dependencies for a number of reactions.<br />

I<br />

Figure 5.22: Reactive cross section for the line-of-centers model.<br />

(3) Result for ( ) from Eq. 5.162:<br />

y<br />

µ 1<br />

( )=<br />

<br />

Z ∞ µ<br />

× 2<br />

0<br />

=<br />

µ 1<br />

<br />

×<br />

Z ∞<br />

0<br />

( )=<br />

12 µ 2<br />

<br />

32<br />

1 − <br />

0<br />

<br />

12 µ 2<br />

32<br />

<br />

2 ( − 0 )exp<br />

µ 8 <br />

<br />

µ<br />

exp − <br />

<br />

(5.188)<br />

<br />

µ<br />

− <br />

<br />

(5.189)<br />

<br />

12 µ<br />

2 exp − <br />

0<br />

<br />

(5.190)<br />

This result is identical to that of our primitive “hard sphere-fixedmeanrelative<br />

speed” model from Section 5.1!

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