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

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5.1 Hardspherecollisiontheory 97<br />

<strong>—</strong> number density of B<br />

(5.15)<br />

<strong>—</strong> Number of collisions of a single A in time : ⇒ number of molecules B in<br />

that volume<br />

= 2 × × (5.16)<br />

• Number of all collisions between A and B:<br />

= 2 × × (5.17)<br />

• Modification for collisions between identical molecules (collisions must not be<br />

counted twice):<br />

= 1 2 × 2 × × (5.18)<br />

=<br />

√<br />

2<br />

2 × 2 × × (5.19)<br />

• Comparison with rate expression:<br />

y<br />

− <br />

<br />

= − <br />

<br />

= × = (5.20)<br />

• Expression for rate constant for collisions A + B:<br />

<br />

max = 2 × = × (5.21)<br />

y<br />

µ 12<br />

max = 2 8 <br />

×<br />

(5.22)<br />

<br />

• Modification for collisions between identical molecules (A + A):<br />

max = 1 2 2 × = √ 1 µ 12<br />

2 8 <br />

×<br />

(5.23)<br />

2 <br />

Theseexpressionsgivetheupper limits for the rate constants of bimolecular<br />

reactions. The upper limits are reached only if<br />

• there are no energetic restrictions (no energy barriers),<br />

• all collisions lead to reaction (no steric constraints),<br />

• molecules can be approximated as hard spheres (unrealistic, usually one has <br />

),<br />

• all molecules collide with the same relative speed (in reality there is a distribution<br />

of speeds).

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