|
|
Line 12: |
Line 12: |
| Bond sequence: 1-2-3: | | Bond sequence: 1-2-3: |
|
| |
|
| Bond Angle: <math> \theta </math> | | Bond Angle: <math> \left. \theta \right. </math> |
|
| |
|
| <math> \cos \theta = \frac{ \vec{r}_{21} \cdot \vec{r}_{23} } {|\vec{r}_{21}| |\vec{r}_{23}|} | | <math> \cos \theta = \frac{ \vec{r}_{21} \cdot \vec{r}_{23} } {|\vec{r}_{21}| |\vec{r}_{23}|} |
Revision as of 13:51, 22 February 2007
Modelling of internal degrees of freedom, usual techniques:
Bond distances
- Atoms linked by a chemical bond (stretching):
However, this internal coordinates are very often kept constrained (fixed bond distances)
Bond Angles
Bond sequence: 1-2-3:
Bond Angle:
Two typical forms are used to model the bending potential:
Dihedral angles. Internal Rotation
Bond sequence: 1-2-3-4
Dihedral angle (
) definition:
Consider the following vectors:
; Unit vector in the direction of the 2-3 bond
; normalized component of
ortogonal to 
; normalized component of
ortogonal to 


For molecules with internal rotation degrees of freedom (e.g. n-alkanes), a torsional potential is
usually modelled as:

or

Van der Waals intramolecular interactions
For pairs of atoms (or sites) which are separated by a certain number of chemical bonds,
pair interaction models similar to the typical intermolecular potentials are frequently
used (e.g. Lennard-Jones potentials)