Flexible molecules: Difference between revisions

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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 11:51, 22 February 2007

Modelling of internal degrees of freedom, usual techniques:

Bond distances

  • Atoms linked by a chemical bond (stretching):

Vstr(r12)=12Kstr(r12−b0)2

However, this internal coordinates are very often kept constrained (fixed bond distances)

Bond Angles

Bond sequence: 1-2-3:

Bond Angle: θ

cosθ=r→21⋅r→23|r→21||r→23|

Two typical forms are used to model the bending potential:

Vbend(θ)=12kθ(θ−θ0)2

Vbend(cosθ)=12kc(cosθ−c0)2

Dihedral angles. Internal Rotation

Bond sequence: 1-2-3-4 Dihedral angle (ϕ) definition:

Consider the following vectors:

  • a→≡r→3−r→2|r→3−r→2|; Unit vector in the direction of the 2-3 bond
  • b→≡r→21−(r→21⋅a→)a→|r→21−(r→21⋅a→)a→|; normalized component of r→21 ortogonal to a→
  • e→34≡r→34−(r→34⋅a→)a→|r→34−(r→34⋅a→)a→|; normalized component of r→34 ortogonal to a→
  • c→=a→×b→
  • e34=(cosϕ)a→+(sinϕ)c→

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

  • Vtors(ϕ)=∑i=0nai(cosϕ)i

or

  • Vtors(ϕ)=∑i=0nbicos(iϕ)

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)