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

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3.5 Numerical integration 58<br />

I<br />

Survey of methods of numerical integration methods:<br />

• explicit methods (e.g., Runge-Kutta),<br />

• implicit methods (e.g., Gear),<br />

• extrapolation methods (e.g., Richardson, Bulirsch-Stoer, Deuflhard).<br />

In the following, we consider the basics of the most convenient methods.<br />

3.5.1 Taylor series expansions<br />

The Taylor expansion is the basis for all numerical integration methods. We start from<br />

the initial value of ( 0 ) at some time 0<br />

( 0 )= 0 (3.136)<br />

and want to determine the value ( 0 + ) at time 0 + . UsingtheDEfor <br />

we expand in a Taylor series around 0 :<br />

Recursion formula:<br />

·<br />

() =( ) (3.137)<br />

( 0 + ) = ( 0 )+ · · ( 0 0 )+ 2<br />

2! · ··<br />

( 0 0 )+ (3.138)<br />

= ( 0 )+ · ( 0 0 )+ 2<br />

2! · ·<br />

( 0 0 )+ (3.139)<br />

+1 = + · ( )+ 2<br />

2! · ·<br />

( )+ (3.140)<br />

The first-order term ( ) is given by the rate equation at , the second-order<br />

term ( ·<br />

) (which is taken into account for example by the 2 order Runge-Kutta<br />

method) and higher order terms (⇒ higher order Runge-Kutta methods) have to be<br />

evaluated numerically by finite differences.<br />

3.5.2 Euler method<br />

The Euler method is based on a 1 order Taylor expansion. If the step size is small<br />

enough, the higher order terms can be neglected:<br />

( 0 + ) = ( 0 )+ · ·<br />

( 0 )+O( 2 ) (3.141)<br />

Initial value problem:<br />

·<br />

= ( ) (3.142)

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