Physical Chemistry 3: — Chemical Kinetics — - Christian-Albrechts ...
Physical Chemistry 3: — Chemical Kinetics — - Christian-Albrechts ... Physical Chemistry 3: — Chemical Kinetics — - Christian-Albrechts ...
6.3 Trajectory Calculations 143 6.3 Trajectory Calculations The “exact” dynamics of the molecules on a potential energy hypersurface can be followed by classical trajectory calculations. I Phase Space: 6-dimensional space spanned by the spatial coordinates ( )and the conjugated momenta ( ): ↔ (6.12) where = = · (6.13) I I Hamilton function: = + = 2 + () (6.14) 2 Note that depends only on and depends only on . Equations of motion: • for a 1 particle system: (1) = = = − () y · = − = − since contains only not . (2) y y • for an atomic system: = + = (6.15) (6.16) = 2 2 + (6.17) = 1 × = 1 µ × · 3X =1 · = = · (6.18) (6.19) 2 2 + ( 1 2 3−6 ) (6.20) · = − (6.21) · = (6.22) Thus we obtain a set of coupled differential equations which can be solved using the Runge-Kutta or Gear methods.
6.3 Trajectory Calculations 144 • Thermal rate constants ( ) follow by suitable averaging over the initial conditions ( vibrational states, rotational states, angles, ...). • Major problems: Zero-point energy? Tunneling? Surface crossings? I Figure 6.6: Trajectory calculations. I Figure 6.7: Trajectory calculations.
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6.3 Trajectory Calculations 143<br />
6.3 Trajectory Calculations<br />
The “exact” dynamics of the molecules on a potential energy hypersurface can be<br />
followed by classical trajectory calculations.<br />
I Phase Space: 6-dimensional space spanned by the spatial coordinates ( )and<br />
the conjugated momenta ( ):<br />
↔ (6.12)<br />
where<br />
= <br />
<br />
<br />
= <br />
·<br />
(6.13)<br />
I<br />
I<br />
Hamilton function:<br />
= + = 2<br />
+ () (6.14)<br />
2<br />
Note that depends only on and depends only on .<br />
Equations of motion:<br />
• for a 1 particle system:<br />
(1)<br />
= = <br />
<br />
= −<br />
()<br />
<br />
y<br />
·<br />
= − <br />
= − <br />
since contains only not .<br />
(2)<br />
y<br />
y<br />
• for an atomic system:<br />
= + =<br />
(6.15)<br />
(6.16)<br />
= 2<br />
2 + (6.17)<br />
<br />
<br />
= 1 × = 1 µ<br />
× <br />
·<br />
3X<br />
=1<br />
·<br />
= <br />
<br />
= ·<br />
(6.18)<br />
(6.19)<br />
<br />
2 2 + ( 1 2 3−6 ) (6.20)<br />
·<br />
= − <br />
(6.21)<br />
<br />
·<br />
= <br />
(6.22)<br />
<br />
Thus we obtain a set of coupled differential equations which can be solved using<br />
the Runge-Kutta or Gear methods.