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

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Appendix E 286<br />

Appendix E: Laplace transforms<br />

The concept of Laplace and inverse Laplace transforms is extremely useful in chemical<br />

kinetics for two reasons:<br />

(1) They connect microscopic molecular properties and statistically averaged quantities:<br />

a) () ↔ ( ): Collision cross section vs. thermal rate constant for bimolecular<br />

reactions (section ??),<br />

b) () ↔ ( ): Specific rateconstantvs. thermal rate constant for unimolecular<br />

reactions (section 8),<br />

c) () ↔ ( ): Density of states vs. partition function in statistical rate<br />

theories 8).<br />

(2) They provide a convenient method for solving of differential equations (section<br />

3.4.2).<br />

I<br />

Definition E.1: The Laplace transform L [ ()] of a function () is defined as the<br />

integral<br />

Z ∞<br />

() =L [ ()] = () − <br />

(E.1)<br />

where<br />

0<br />

• is a real variable,<br />

• () is a real function of the variable with the property () =0for 0,<br />

• is a complex variable,<br />

• () =L [ ()] is a function of the variable .<br />

I<br />

Definition E.2: The inverse Laplace transform L −1 [ ()] of the function () is<br />

defined as the integral<br />

() =L −1 [ ()] = 1 Z<br />

2<br />

+∞<br />

−∞<br />

() <br />

(E.2)<br />

where<br />

• is an arbitrary real constant.

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