Concise Physical Chemistry

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c10 JWBS043-Rogers September 13, 2010 11:26 Printer Name: Yet to Come


158 CHEMICAL KINETICS

0.541

0

(.9⋅r)^2 ⋅e−.9⋅r

r^2 ⋅e−r

[1.1⋅(r)]^2 ⋅e−1.1⋅r

0 r 10
FIGURE 10.6 A Boltzmann distribution of molecular speeds. The area under the tail of the
curve beyondrincreases exponentially.

The quantitative relationship between the reaction rate constant and temperature is

k=ae−aH/RT

This can be appreciated by looking at a Boltzmann distribution of reactant molecules.
The area under the Boltzmann curve that surpasses the activation barrier atrincreases
sharply (exponentially) with temperature, leading to the observed exponential in-
crease ink(Fig. 10.6). The exponential relationship betweenkandTis called the
Arrhenius rate law.

10.7 COLLISION THEORY


One can calculate the number of molecules colliding with one another in a gaseous
sample at a specified temperature. SupposeZABis the collision frequency for a
collection of gas molecules capable of undergoing a bimolecular reaction. If all the
molecules were activated, the rate would be directly determined by the number of
collisions per unit time of molecules of kind A with those of kind B. Not all molecules
will be activated, however, and we must multiplyZABby the fraction that are. This
is the Boltzmann factore−aH/RT.
For a gas reaction taking place between molecules that are structurally compli-
cated, a probability factorPis introduced to account for collisions between activated
molecules that are not oriented toward each other in the proper way for reaction to
occur. Now

k=PZABe−aH/RT

where the integration factorais included in the empirical probability factorP.
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