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

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8.2 Lindemann mechanism 180<br />

I Half-pressure: We have found the following results:<br />

=<br />

2 1 [M]<br />

−1 [M] + 2<br />

(8.17)<br />

Thus, if −1 [M] = 2 ,wehave<br />

1<br />

∞ = 2<br />

−1<br />

(8.18)<br />

0 = 1 [M] (8.19)<br />

=<br />

2 1 [M]<br />

= 2 1 [M]<br />

−1 [M] + 2 2 −1 [M] = 1 2 1<br />

= 1 2 −1 2 ∞ (8.20)<br />

Half “pressure”:<br />

[M] 12<br />

= 2<br />

−1<br />

(8.21)<br />

I Lifetimes of energized molecules: It is instructive to look at the reciprocal values:<br />

1<br />

−1 [M] = 1 2<br />

(8.22)<br />

1<br />

• is the time between two collisions. This is, in fact, the lifetime of the<br />

−1 [M]<br />

energized molecules with respect to collisional deactivation.<br />

• 1 is the lifetime of the excited molecules with respect to reaction.<br />

2<br />

Thus, at the half pressure, we have<br />

Collisional Deactivation = Unimolecular Decay (8.23)<br />

I Determination of k ∞ :<br />

y<br />

=<br />

2 1 [M]<br />

−1 [M] + 2<br />

(8.24)<br />

1<br />

= −1<br />

+ 1 1<br />

1 2 1 [M]<br />

(8.25)<br />

= 1 + 1 1<br />

∞ 1 [M]<br />

(8.26)<br />

= 1 + 1 ∞ 0<br />

(8.27)<br />

y Plot of −1 vs. [M] −1 should give a straight line with slope 1 −1 and intercept<br />

∞ −1 .

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