1. Developing a Force Field Molecular Mechanics

2. Experimental One Dimensional PES Quantum mechanics tells us that vibrational energy levels are quantized, and that the energy separations between levels are dictated by the shape of the potential within which vibration takes place (i.e., the 1-D PES). By observing the allowed (above, with rotational information too) and forbidden (not shown) transitions of HCl and its isotopes of isomers (which have different vibrational energy levels by virtue of having different reduced masses) the shape of the PES can be deduced over a large range.

3. Result from lots of Experiments

4. Mathematically, how do we build the curve?

5. Additional things to think about Strain is a phenomenon associated with individual components of a molecular geometry. You can have many types of molecular strain, bond, angle, torsional strain Ideal values of bond lengths, angles and torsions depend on more that just the atomic number, there are more than one “type” of the same atom. Think sp3 C vs sp2 C A force field is defined by its atom types, its functions for computing strain and the ideal constraints that appear in those functions Force fields can get very complicated very quickly (even though the calculations are “easy” given that the classification of atoms becomes more and more complex

6. Constants Needed! The more atom types, the better the force field can predict reality. – MM4 force field has over --- atom types Every atom type requires the definition of a force constant, and an equilibrium length between it and every other atom defined in the force field. The number of bond stretch parameters goes up as N 2 where N is the number of atom types Assignment of parameters comes from experimental data or from high level QM calculations.

7. Bending

8. Torsion

9. Computer Power Rules Assign an atom type to all atoms Assign which atoms are bonded to each other (can be explicit, or based on some set distance algorithm) Look up force constants, equilibrium values, phase angles etc. for all bonds, angles and torsions (are we missing any?) Compute energy in a small fraction of a second on any decent computer

10. What about non-bonded interactions?

11. Electrostatics

12. Other Electrostatic Possibilities

13. Force Field Validation Collect experimental data (structural and energetic information is the more useful) Define an error function that balances what is tolerable for errors Vary the parameters and functional forms of the force field to minimize the error function Lock all the parameters and functional forms into stone (give it a name “MM3” “MMFF” and publish it (or sell it)

14. A word of Warning Selection of a force field should be made based on how similar your molecule is to those used to parameterize the force field. Force fields are bad for reactions and good for structures and energies – Once bonds are defined, they cannot break in a harmonic force field, nor can new ones form If you start with a bad guess structure, there is no guarantee that the nearest minimum will be a chemically meaningful one – You must be smarter than your computer All of these issues can be corrected, and thus new force fields are being developed as we speak