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Untitled - Aerobib - Universidad Politécnica de Madrid

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32 CHAPTER 1. THERMOCHEMISTRY<br />

which can be i<strong>de</strong>ntified with Eq. (1.122) by making<br />

√ ( )<br />

k = Nσ12<br />

2 M1 + M 2<br />

8πRT<br />

e −E/RT , (1.130)<br />

M 1 M 2<br />

that is, from Eq. (1.124),<br />

α = 1 2<br />

(1.131)<br />

and<br />

B = Nσ 2 12<br />

√<br />

8πR<br />

( )<br />

M1 + M 2<br />

. (1.132)<br />

M 1 M 2<br />

When comparing Collisions Theory with experimental results, an exact numerical<br />

agreement between the reaction rates predicted and observed is not to be expected,<br />

but an agreement of the or<strong>de</strong>rs of magnitu<strong>de</strong>. In fact, Collisions Theory does not inclu<strong>de</strong>,<br />

among others, the influence of the relative orientation of the molecules as they<br />

colli<strong>de</strong> which can <strong>de</strong>ci<strong>de</strong> the success of the collision. Such an effect can be of importance<br />

specially in molecules of complicated structure. It is taken into consi<strong>de</strong>ration<br />

by including in Eq. (1.129) a numerical factor P of orientation equal or smaller than<br />

unity<br />

dc 1<br />

dt = dc 2<br />

dt = − dc 3<br />

dt =<br />

− P<br />

√<br />

ρ2<br />

Nσ 2<br />

M 1 M<br />

12Y 1 Y 2 8πRT<br />

2<br />

( )<br />

M1 + M 2<br />

e −E/RT .<br />

M 1 M 2<br />

(1.133)<br />

Experimental reaction rates agree, fairly, with those predicted by Collision Theory<br />

only for a short number of reactions, yet in other cases experimental rates are as much<br />

as 10 8 times larger or smaller than those predicted by theory. Such a discrepancy can<br />

not be justified within the theory. These results that in the best cases Collision Theory<br />

represents approximately the actual facts only for a short number of reactions. A more<br />

correct formulation is provi<strong>de</strong>d by the so-called Theory of Absolute Reaction Rates.<br />

In this theory it is assumed that the passing of the reacting species to the products<br />

takes place through the formation of an activated complex resulting from the<br />

assembly of the reacting species. This complex is consi<strong>de</strong>red as located at the top of<br />

an energy barrier which separates the species from the products. The reaction rate<br />

is <strong>de</strong>termined by the velocity at which the activated complex crosses the barrier. It<br />

is, furthermore, assumed that such complex stands in equilibrium with the reacting<br />

species and that its dissociation in products is due to the action of one of the vibrational<br />

<strong>de</strong>gree of freedom. Then, by applying the laws of Statistical Mechanics the<br />

reaction rate can be computed when the structure of the activated complex is known.

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